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6a4ea4ad783d82ffa221ec2839dc7b9d2af21295307e9fd47c16935af4b5b185 | """Simple Harmonic Oscillator 1-Dimension"""
from __future__ import print_function, division
from sympy import sqrt, I, Symbol, Integer, S
from sympy.core.compatibility import range
from sympy.physics.quantum.constants import hbar
from sympy.physics.quantum.operator import Operator
from sympy.physics.quantum.state import Bra, Ket, State
from sympy.physics.quantum.qexpr import QExpr
from sympy.physics.quantum.cartesian import X, Px
from sympy.functions.special.tensor_functions import KroneckerDelta
from sympy.physics.quantum.hilbert import ComplexSpace
from sympy.physics.quantum.matrixutils import matrix_zeros
#------------------------------------------------------------------------------
class SHOOp(Operator):
"""A base class for the SHO Operators.
We are limiting the number of arguments to be 1.
"""
@classmethod
def _eval_args(cls, args):
args = QExpr._eval_args(args)
if len(args) == 1:
return args
else:
raise ValueError("Too many arguments")
@classmethod
def _eval_hilbert_space(cls, label):
return ComplexSpace(S.Infinity)
class RaisingOp(SHOOp):
"""The Raising Operator or a^dagger.
When a^dagger acts on a state it raises the state up by one. Taking
the adjoint of a^dagger returns 'a', the Lowering Operator. a^dagger
can be rewritten in terms of position and momentum. We can represent
a^dagger as a matrix, which will be its default basis.
Parameters
==========
args : tuple
The list of numbers or parameters that uniquely specify the
operator.
Examples
========
Create a Raising Operator and rewrite it in terms of position and
momentum, and show that taking its adjoint returns 'a':
>>> from sympy.physics.quantum.sho1d import RaisingOp
>>> from sympy.physics.quantum import Dagger
>>> ad = RaisingOp('a')
>>> ad.rewrite('xp').doit()
sqrt(2)*(m*omega*X - I*Px)/(2*sqrt(hbar)*sqrt(m*omega))
>>> Dagger(ad)
a
Taking the commutator of a^dagger with other Operators:
>>> from sympy.physics.quantum import Commutator
>>> from sympy.physics.quantum.sho1d import RaisingOp, LoweringOp
>>> from sympy.physics.quantum.sho1d import NumberOp
>>> ad = RaisingOp('a')
>>> a = LoweringOp('a')
>>> N = NumberOp('N')
>>> Commutator(ad, a).doit()
-1
>>> Commutator(ad, N).doit()
-RaisingOp(a)
Apply a^dagger to a state:
>>> from sympy.physics.quantum import qapply
>>> from sympy.physics.quantum.sho1d import RaisingOp, SHOKet
>>> ad = RaisingOp('a')
>>> k = SHOKet('k')
>>> qapply(ad*k)
sqrt(k + 1)*|k + 1>
Matrix Representation
>>> from sympy.physics.quantum.sho1d import RaisingOp
>>> from sympy.physics.quantum.represent import represent
>>> ad = RaisingOp('a')
>>> represent(ad, basis=N, ndim=4, format='sympy')
Matrix([
[0, 0, 0, 0],
[1, 0, 0, 0],
[0, sqrt(2), 0, 0],
[0, 0, sqrt(3), 0]])
"""
def _eval_rewrite_as_xp(self, *args, **kwargs):
return (Integer(1)/sqrt(Integer(2)*hbar*m*omega))*(
Integer(-1)*I*Px + m*omega*X)
def _eval_adjoint(self):
return LoweringOp(*self.args)
def _eval_commutator_LoweringOp(self, other):
return Integer(-1)
def _eval_commutator_NumberOp(self, other):
return Integer(-1)*self
def _apply_operator_SHOKet(self, ket):
temp = ket.n + Integer(1)
return sqrt(temp)*SHOKet(temp)
def _represent_default_basis(self, **options):
return self._represent_NumberOp(None, **options)
def _represent_XOp(self, basis, **options):
# This logic is good but the underlying position
# representation logic is broken.
# temp = self.rewrite('xp').doit()
# result = represent(temp, basis=X)
# return result
raise NotImplementedError('Position representation is not implemented')
def _represent_NumberOp(self, basis, **options):
ndim_info = options.get('ndim', 4)
format = options.get('format','sympy')
matrix = matrix_zeros(ndim_info, ndim_info, **options)
for i in range(ndim_info - 1):
value = sqrt(i + 1)
if format == 'scipy.sparse':
value = float(value)
matrix[i + 1, i] = value
if format == 'scipy.sparse':
matrix = matrix.tocsr()
return matrix
#--------------------------------------------------------------------------
# Printing Methods
#--------------------------------------------------------------------------
def _print_contents(self, printer, *args):
arg0 = printer._print(self.args[0], *args)
return '%s(%s)' % (self.__class__.__name__, arg0)
def _print_contents_pretty(self, printer, *args):
from sympy.printing.pretty.stringpict import prettyForm
pform = printer._print(self.args[0], *args)
pform = pform**prettyForm(u'\N{DAGGER}')
return pform
def _print_contents_latex(self, printer, *args):
arg = printer._print(self.args[0])
return '%s^{\\dagger}' % arg
class LoweringOp(SHOOp):
"""The Lowering Operator or 'a'.
When 'a' acts on a state it lowers the state up by one. Taking
the adjoint of 'a' returns a^dagger, the Raising Operator. 'a'
can be rewritten in terms of position and momentum. We can
represent 'a' as a matrix, which will be its default basis.
Parameters
==========
args : tuple
The list of numbers or parameters that uniquely specify the
operator.
Examples
========
Create a Lowering Operator and rewrite it in terms of position and
momentum, and show that taking its adjoint returns a^dagger:
>>> from sympy.physics.quantum.sho1d import LoweringOp
>>> from sympy.physics.quantum import Dagger
>>> a = LoweringOp('a')
>>> a.rewrite('xp').doit()
sqrt(2)*(m*omega*X + I*Px)/(2*sqrt(hbar)*sqrt(m*omega))
>>> Dagger(a)
RaisingOp(a)
Taking the commutator of 'a' with other Operators:
>>> from sympy.physics.quantum import Commutator
>>> from sympy.physics.quantum.sho1d import LoweringOp, RaisingOp
>>> from sympy.physics.quantum.sho1d import NumberOp
>>> a = LoweringOp('a')
>>> ad = RaisingOp('a')
>>> N = NumberOp('N')
>>> Commutator(a, ad).doit()
1
>>> Commutator(a, N).doit()
a
Apply 'a' to a state:
>>> from sympy.physics.quantum import qapply
>>> from sympy.physics.quantum.sho1d import LoweringOp, SHOKet
>>> a = LoweringOp('a')
>>> k = SHOKet('k')
>>> qapply(a*k)
sqrt(k)*|k - 1>
Taking 'a' of the lowest state will return 0:
>>> from sympy.physics.quantum import qapply
>>> from sympy.physics.quantum.sho1d import LoweringOp, SHOKet
>>> a = LoweringOp('a')
>>> k = SHOKet(0)
>>> qapply(a*k)
0
Matrix Representation
>>> from sympy.physics.quantum.sho1d import LoweringOp
>>> from sympy.physics.quantum.represent import represent
>>> a = LoweringOp('a')
>>> represent(a, basis=N, ndim=4, format='sympy')
Matrix([
[0, 1, 0, 0],
[0, 0, sqrt(2), 0],
[0, 0, 0, sqrt(3)],
[0, 0, 0, 0]])
"""
def _eval_rewrite_as_xp(self, *args, **kwargs):
return (Integer(1)/sqrt(Integer(2)*hbar*m*omega))*(
I*Px + m*omega*X)
def _eval_adjoint(self):
return RaisingOp(*self.args)
def _eval_commutator_RaisingOp(self, other):
return Integer(1)
def _eval_commutator_NumberOp(self, other):
return Integer(1)*self
def _apply_operator_SHOKet(self, ket):
temp = ket.n - Integer(1)
if ket.n == Integer(0):
return Integer(0)
else:
return sqrt(ket.n)*SHOKet(temp)
def _represent_default_basis(self, **options):
return self._represent_NumberOp(None, **options)
def _represent_XOp(self, basis, **options):
# This logic is good but the underlying position
# representation logic is broken.
# temp = self.rewrite('xp').doit()
# result = represent(temp, basis=X)
# return result
raise NotImplementedError('Position representation is not implemented')
def _represent_NumberOp(self, basis, **options):
ndim_info = options.get('ndim', 4)
format = options.get('format', 'sympy')
matrix = matrix_zeros(ndim_info, ndim_info, **options)
for i in range(ndim_info - 1):
value = sqrt(i + 1)
if format == 'scipy.sparse':
value = float(value)
matrix[i,i + 1] = value
if format == 'scipy.sparse':
matrix = matrix.tocsr()
return matrix
class NumberOp(SHOOp):
"""The Number Operator is simply a^dagger*a
It is often useful to write a^dagger*a as simply the Number Operator
because the Number Operator commutes with the Hamiltonian. And can be
expressed using the Number Operator. Also the Number Operator can be
applied to states. We can represent the Number Operator as a matrix,
which will be its default basis.
Parameters
==========
args : tuple
The list of numbers or parameters that uniquely specify the
operator.
Examples
========
Create a Number Operator and rewrite it in terms of the ladder
operators, position and momentum operators, and Hamiltonian:
>>> from sympy.physics.quantum.sho1d import NumberOp
>>> N = NumberOp('N')
>>> N.rewrite('a').doit()
RaisingOp(a)*a
>>> N.rewrite('xp').doit()
-1/2 + (m**2*omega**2*X**2 + Px**2)/(2*hbar*m*omega)
>>> N.rewrite('H').doit()
-1/2 + H/(hbar*omega)
Take the Commutator of the Number Operator with other Operators:
>>> from sympy.physics.quantum import Commutator
>>> from sympy.physics.quantum.sho1d import NumberOp, Hamiltonian
>>> from sympy.physics.quantum.sho1d import RaisingOp, LoweringOp
>>> N = NumberOp('N')
>>> H = Hamiltonian('H')
>>> ad = RaisingOp('a')
>>> a = LoweringOp('a')
>>> Commutator(N,H).doit()
0
>>> Commutator(N,ad).doit()
RaisingOp(a)
>>> Commutator(N,a).doit()
-a
Apply the Number Operator to a state:
>>> from sympy.physics.quantum import qapply
>>> from sympy.physics.quantum.sho1d import NumberOp, SHOKet
>>> N = NumberOp('N')
>>> k = SHOKet('k')
>>> qapply(N*k)
k*|k>
Matrix Representation
>>> from sympy.physics.quantum.sho1d import NumberOp
>>> from sympy.physics.quantum.represent import represent
>>> N = NumberOp('N')
>>> represent(N, basis=N, ndim=4, format='sympy')
Matrix([
[0, 0, 0, 0],
[0, 1, 0, 0],
[0, 0, 2, 0],
[0, 0, 0, 3]])
"""
def _eval_rewrite_as_a(self, *args, **kwargs):
return ad*a
def _eval_rewrite_as_xp(self, *args, **kwargs):
return (Integer(1)/(Integer(2)*m*hbar*omega))*(Px**2 + (
m*omega*X)**2) - Integer(1)/Integer(2)
def _eval_rewrite_as_H(self, *args, **kwargs):
return H/(hbar*omega) - Integer(1)/Integer(2)
def _apply_operator_SHOKet(self, ket):
return ket.n*ket
def _eval_commutator_Hamiltonian(self, other):
return Integer(0)
def _eval_commutator_RaisingOp(self, other):
return other
def _eval_commutator_LoweringOp(self, other):
return Integer(-1)*other
def _represent_default_basis(self, **options):
return self._represent_NumberOp(None, **options)
def _represent_XOp(self, basis, **options):
# This logic is good but the underlying position
# representation logic is broken.
# temp = self.rewrite('xp').doit()
# result = represent(temp, basis=X)
# return result
raise NotImplementedError('Position representation is not implemented')
def _represent_NumberOp(self, basis, **options):
ndim_info = options.get('ndim', 4)
format = options.get('format', 'sympy')
matrix = matrix_zeros(ndim_info, ndim_info, **options)
for i in range(ndim_info):
value = i
if format == 'scipy.sparse':
value = float(value)
matrix[i,i] = value
if format == 'scipy.sparse':
matrix = matrix.tocsr()
return matrix
class Hamiltonian(SHOOp):
"""The Hamiltonian Operator.
The Hamiltonian is used to solve the time-independent Schrodinger
equation. The Hamiltonian can be expressed using the ladder operators,
as well as by position and momentum. We can represent the Hamiltonian
Operator as a matrix, which will be its default basis.
Parameters
==========
args : tuple
The list of numbers or parameters that uniquely specify the
operator.
Examples
========
Create a Hamiltonian Operator and rewrite it in terms of the ladder
operators, position and momentum, and the Number Operator:
>>> from sympy.physics.quantum.sho1d import Hamiltonian
>>> H = Hamiltonian('H')
>>> H.rewrite('a').doit()
hbar*omega*(1/2 + RaisingOp(a)*a)
>>> H.rewrite('xp').doit()
(m**2*omega**2*X**2 + Px**2)/(2*m)
>>> H.rewrite('N').doit()
hbar*omega*(1/2 + N)
Take the Commutator of the Hamiltonian and the Number Operator:
>>> from sympy.physics.quantum import Commutator
>>> from sympy.physics.quantum.sho1d import Hamiltonian, NumberOp
>>> H = Hamiltonian('H')
>>> N = NumberOp('N')
>>> Commutator(H,N).doit()
0
Apply the Hamiltonian Operator to a state:
>>> from sympy.physics.quantum import qapply
>>> from sympy.physics.quantum.sho1d import Hamiltonian, SHOKet
>>> H = Hamiltonian('H')
>>> k = SHOKet('k')
>>> qapply(H*k)
hbar*k*omega*|k> + hbar*omega*|k>/2
Matrix Representation
>>> from sympy.physics.quantum.sho1d import Hamiltonian
>>> from sympy.physics.quantum.represent import represent
>>> H = Hamiltonian('H')
>>> represent(H, basis=N, ndim=4, format='sympy')
Matrix([
[hbar*omega/2, 0, 0, 0],
[ 0, 3*hbar*omega/2, 0, 0],
[ 0, 0, 5*hbar*omega/2, 0],
[ 0, 0, 0, 7*hbar*omega/2]])
"""
def _eval_rewrite_as_a(self, *args, **kwargs):
return hbar*omega*(ad*a + Integer(1)/Integer(2))
def _eval_rewrite_as_xp(self, *args, **kwargs):
return (Integer(1)/(Integer(2)*m))*(Px**2 + (m*omega*X)**2)
def _eval_rewrite_as_N(self, *args, **kwargs):
return hbar*omega*(N + Integer(1)/Integer(2))
def _apply_operator_SHOKet(self, ket):
return (hbar*omega*(ket.n + Integer(1)/Integer(2)))*ket
def _eval_commutator_NumberOp(self, other):
return Integer(0)
def _represent_default_basis(self, **options):
return self._represent_NumberOp(None, **options)
def _represent_XOp(self, basis, **options):
# This logic is good but the underlying position
# representation logic is broken.
# temp = self.rewrite('xp').doit()
# result = represent(temp, basis=X)
# return result
raise NotImplementedError('Position representation is not implemented')
def _represent_NumberOp(self, basis, **options):
ndim_info = options.get('ndim', 4)
format = options.get('format', 'sympy')
matrix = matrix_zeros(ndim_info, ndim_info, **options)
for i in range(ndim_info):
value = i + Integer(1)/Integer(2)
if format == 'scipy.sparse':
value = float(value)
matrix[i,i] = value
if format == 'scipy.sparse':
matrix = matrix.tocsr()
return hbar*omega*matrix
#------------------------------------------------------------------------------
class SHOState(State):
"""State class for SHO states"""
@classmethod
def _eval_hilbert_space(cls, label):
return ComplexSpace(S.Infinity)
@property
def n(self):
return self.args[0]
class SHOKet(SHOState, Ket):
"""1D eigenket.
Inherits from SHOState and Ket.
Parameters
==========
args : tuple
The list of numbers or parameters that uniquely specify the ket
This is usually its quantum numbers or its symbol.
Examples
========
Ket's know about their associated bra:
>>> from sympy.physics.quantum.sho1d import SHOKet
>>> k = SHOKet('k')
>>> k.dual
<k|
>>> k.dual_class()
<class 'sympy.physics.quantum.sho1d.SHOBra'>
Take the Inner Product with a bra:
>>> from sympy.physics.quantum import InnerProduct
>>> from sympy.physics.quantum.sho1d import SHOKet, SHOBra
>>> k = SHOKet('k')
>>> b = SHOBra('b')
>>> InnerProduct(b,k).doit()
KroneckerDelta(b, k)
Vector representation of a numerical state ket:
>>> from sympy.physics.quantum.sho1d import SHOKet, NumberOp
>>> from sympy.physics.quantum.represent import represent
>>> k = SHOKet(3)
>>> N = NumberOp('N')
>>> represent(k, basis=N, ndim=4)
Matrix([
[0],
[0],
[0],
[1]])
"""
@classmethod
def dual_class(self):
return SHOBra
def _eval_innerproduct_SHOBra(self, bra, **hints):
result = KroneckerDelta(self.n, bra.n)
return result
def _represent_default_basis(self, **options):
return self._represent_NumberOp(None, **options)
def _represent_NumberOp(self, basis, **options):
ndim_info = options.get('ndim', 4)
format = options.get('format', 'sympy')
options['spmatrix'] = 'lil'
vector = matrix_zeros(ndim_info, 1, **options)
if isinstance(self.n, Integer):
if self.n >= ndim_info:
return ValueError("N-Dimension too small")
if format == 'scipy.sparse':
vector[int(self.n), 0] = 1.0
vector = vector.tocsr()
elif format == 'numpy':
vector[int(self.n), 0] = 1.0
else:
vector[self.n, 0] = Integer(1)
return vector
else:
return ValueError("Not Numerical State")
class SHOBra(SHOState, Bra):
"""A time-independent Bra in SHO.
Inherits from SHOState and Bra.
Parameters
==========
args : tuple
The list of numbers or parameters that uniquely specify the ket
This is usually its quantum numbers or its symbol.
Examples
========
Bra's know about their associated ket:
>>> from sympy.physics.quantum.sho1d import SHOBra
>>> b = SHOBra('b')
>>> b.dual
|b>
>>> b.dual_class()
<class 'sympy.physics.quantum.sho1d.SHOKet'>
Vector representation of a numerical state bra:
>>> from sympy.physics.quantum.sho1d import SHOBra, NumberOp
>>> from sympy.physics.quantum.represent import represent
>>> b = SHOBra(3)
>>> N = NumberOp('N')
>>> represent(b, basis=N, ndim=4)
Matrix([[0, 0, 0, 1]])
"""
@classmethod
def dual_class(self):
return SHOKet
def _represent_default_basis(self, **options):
return self._represent_NumberOp(None, **options)
def _represent_NumberOp(self, basis, **options):
ndim_info = options.get('ndim', 4)
format = options.get('format', 'sympy')
options['spmatrix'] = 'lil'
vector = matrix_zeros(1, ndim_info, **options)
if isinstance(self.n, Integer):
if self.n >= ndim_info:
return ValueError("N-Dimension too small")
if format == 'scipy.sparse':
vector[0, int(self.n)] = 1.0
vector = vector.tocsr()
elif format == 'numpy':
vector[0, int(self.n)] = 1.0
else:
vector[0, self.n] = Integer(1)
return vector
else:
return ValueError("Not Numerical State")
ad = RaisingOp('a')
a = LoweringOp('a')
H = Hamiltonian('H')
N = NumberOp('N')
omega = Symbol('omega')
m = Symbol('m')
|
99b0e605f87f8f7fc187e78813600644c3cc41f881b02546ae05a420bc584500 | from sympy import Rational, pi, sqrt, S
from sympy.physics.units.quantities import Quantity
from sympy.physics.units.dimensions import (dimsys_default, Dimension,
acceleration, action, amount_of_substance, capacitance, charge,
conductance, current, energy, force, frequency, information, impedance,
inductance, length, luminous_intensity, magnetic_density, magnetic_flux,
mass, power, pressure, temperature, time, velocity, voltage)
from sympy.physics.units.prefixes import (
centi, deci, kilo, micro, milli, nano, pico,
kibi, mebi, gibi, tebi, pebi, exbi)
One = S.One
#### UNITS ####
# Dimensionless:
percent = percents = Quantity("percent", latex_repr=r"\%")
percent.set_dimension(One)
percent.set_scale_factor(Rational(1, 100))
permille = Quantity("permille")
permille.set_dimension(One)
permille.set_scale_factor(Rational(1, 1000))
# Angular units (dimensionless)
rad = radian = radians = Quantity("radian", abbrev="rad")
radian.set_dimension(One)
radian.set_scale_factor(One)
deg = degree = degrees = Quantity("degree", abbrev="deg", latex_repr=r"^\circ")
degree.set_dimension(One)
degree.set_scale_factor(pi/180)
sr = steradian = steradians = Quantity("steradian", abbrev="sr")
steradian.set_dimension(One)
steradian.set_scale_factor(One)
mil = angular_mil = angular_mils = Quantity("angular_mil", abbrev="mil")
angular_mil.set_dimension(One)
angular_mil.set_scale_factor(2*pi/6400)
# Base units:
m = meter = meters = Quantity("meter", abbrev="m")
meter.set_dimension(length)
meter.set_scale_factor(One)
# gram; used to define its prefixed units
g = gram = grams = Quantity("gram", abbrev="g")
gram.set_dimension(mass)
gram.set_scale_factor(One)
# NOTE: the `kilogram` has scale factor 1000. In SI, kg is a base unit, but
# nonetheless we are trying to be compatible with the `kilo` prefix. In a
# similar manner, people using CGS or gaussian units could argue that the
# `centimeter` rather than `meter` is the fundamental unit for length, but the
# scale factor of `centimeter` will be kept as 1/100 to be compatible with the
# `centi` prefix. The current state of the code assumes SI unit dimensions, in
# the future this module will be modified in order to be unit system-neutral
# (that is, support all kinds of unit systems).
kg = kilogram = kilograms = Quantity("kilogram", abbrev="kg")
kilogram.set_dimension(mass)
kilogram.set_scale_factor(kilo*gram)
s = second = seconds = Quantity("second", abbrev="s")
second.set_dimension(time)
second.set_scale_factor(One)
A = ampere = amperes = Quantity("ampere", abbrev='A')
ampere.set_dimension(current)
ampere.set_scale_factor(One)
K = kelvin = kelvins = Quantity("kelvin", abbrev='K')
kelvin.set_dimension(temperature)
kelvin.set_scale_factor(One)
mol = mole = moles = Quantity("mole", abbrev="mol")
mole.set_dimension(amount_of_substance)
mole.set_scale_factor(One)
cd = candela = candelas = Quantity("candela", abbrev="cd")
candela.set_dimension(luminous_intensity)
candela.set_scale_factor(One)
mg = milligram = milligrams = Quantity("milligram", abbrev="mg")
milligram.set_dimension(mass)
milligram.set_scale_factor(milli*gram)
ug = microgram = micrograms = Quantity("microgram", abbrev="ug", latex_repr=r"\mu\text{g}")
microgram.set_dimension(mass)
microgram.set_scale_factor(micro*gram)
# derived units
newton = newtons = N = Quantity("newton", abbrev="N")
newton.set_dimension(force)
newton.set_scale_factor(kilogram*meter/second**2)
joule = joules = J = Quantity("joule", abbrev="J")
joule.set_dimension(energy)
joule.set_scale_factor(newton*meter)
watt = watts = W = Quantity("watt", abbrev="W")
watt.set_dimension(power)
watt.set_scale_factor(joule/second)
pascal = pascals = Pa = pa = Quantity("pascal", abbrev="Pa")
pascal.set_dimension(pressure)
pascal.set_scale_factor(newton/meter**2)
hertz = hz = Hz = Quantity("hertz", abbrev="Hz")
hertz.set_dimension(frequency)
hertz.set_scale_factor(One)
# MKSA extension to MKS: derived units
coulomb = coulombs = C = Quantity("coulomb", abbrev='C')
coulomb.set_dimension(charge)
coulomb.set_scale_factor(One)
volt = volts = v = V = Quantity("volt", abbrev='V')
volt.set_dimension(voltage)
volt.set_scale_factor(joule/coulomb)
ohm = ohms = Quantity("ohm", abbrev='ohm', latex_repr=r"\Omega")
ohm.set_dimension(impedance)
ohm.set_scale_factor(volt/ampere)
siemens = S = mho = mhos = Quantity("siemens", abbrev='S')
siemens.set_dimension(conductance)
siemens.set_scale_factor(ampere/volt)
farad = farads = F = Quantity("farad", abbrev='F')
farad.set_dimension(capacitance)
farad.set_scale_factor(coulomb/volt)
henry = henrys = H = Quantity("henry", abbrev='H')
henry.set_dimension(inductance)
henry.set_scale_factor(volt*second/ampere)
tesla = teslas = T = Quantity("tesla", abbrev='T')
tesla.set_dimension(magnetic_density)
tesla.set_scale_factor(volt*second/meter**2)
weber = webers = Wb = wb = Quantity("weber", abbrev='Wb')
weber.set_dimension(magnetic_flux)
weber.set_scale_factor(joule/ampere)
# Other derived units:
optical_power = dioptre = diopter = D = Quantity("dioptre")
dioptre.set_dimension(1/length)
dioptre.set_scale_factor(1/meter)
lux = lx = Quantity("lux", abbrev="lx")
lux.set_dimension(luminous_intensity/length**2)
lux.set_scale_factor(steradian*candela/meter**2)
# katal is the SI unit of catalytic activity
katal = kat = Quantity("katal", abbrev="kat")
katal.set_dimension(amount_of_substance/time)
katal.set_scale_factor(mol/second)
# gray is the SI unit of absorbed dose
gray = Gy = Quantity("gray")
gray.set_dimension(energy/mass)
gray.set_scale_factor(meter**2/second**2)
# becquerel is the SI unit of radioactivity
becquerel = Bq = Quantity("becquerel", abbrev="Bq")
becquerel.set_dimension(1/time)
becquerel.set_scale_factor(1/second)
# Common length units
km = kilometer = kilometers = Quantity("kilometer", abbrev="km")
kilometer.set_dimension(length)
kilometer.set_scale_factor(kilo*meter)
dm = decimeter = decimeters = Quantity("decimeter", abbrev="dm")
decimeter.set_dimension(length)
decimeter.set_scale_factor(deci*meter)
cm = centimeter = centimeters = Quantity("centimeter", abbrev="cm")
centimeter.set_dimension(length)
centimeter.set_scale_factor(centi*meter)
mm = millimeter = millimeters = Quantity("millimeter", abbrev="mm")
millimeter.set_dimension(length)
millimeter.set_scale_factor(milli*meter)
um = micrometer = micrometers = micron = microns = \
Quantity("micrometer", abbrev="um", latex_repr=r'\mu\text{m}')
micrometer.set_dimension(length)
micrometer.set_scale_factor(micro*meter)
nm = nanometer = nanometers = Quantity("nanometer", abbrev="nm")
nanometer.set_dimension(length)
nanometer.set_scale_factor(nano*meter)
pm = picometer = picometers = Quantity("picometer", abbrev="pm")
picometer.set_dimension(length)
picometer.set_scale_factor(pico*meter)
ft = foot = feet = Quantity("foot", abbrev="ft")
foot.set_dimension(length)
foot.set_scale_factor(Rational(3048, 10000)*meter)
inch = inches = Quantity("inch")
inch.set_dimension(length)
inch.set_scale_factor(foot/12)
yd = yard = yards = Quantity("yard", abbrev="yd")
yard.set_dimension(length)
yard.set_scale_factor(3*feet)
mi = mile = miles = Quantity("mile")
mile.set_dimension(length)
mile.set_scale_factor(5280*feet)
nmi = nautical_mile = nautical_miles = Quantity("nautical_mile")
nautical_mile.set_dimension(length)
nautical_mile.set_scale_factor(6076*feet)
# Common volume and area units
l = liter = liters = Quantity("liter")
liter.set_dimension(length**3)
liter.set_scale_factor(meter**3 / 1000)
dl = deciliter = deciliters = Quantity("deciliter")
deciliter.set_dimension(length**3)
deciliter.set_scale_factor(liter / 10)
cl = centiliter = centiliters = Quantity("centiliter")
centiliter.set_dimension(length**3)
centiliter.set_scale_factor(liter / 100)
ml = milliliter = milliliters = Quantity("milliliter")
milliliter.set_dimension(length**3)
milliliter.set_scale_factor(liter / 1000)
# Common time units
ms = millisecond = milliseconds = Quantity("millisecond", abbrev="ms")
millisecond.set_dimension(time)
millisecond.set_scale_factor(milli*second)
us = microsecond = microseconds = Quantity("microsecond", abbrev="us", latex_repr=r'\mu\text{s}')
microsecond.set_dimension(time)
microsecond.set_scale_factor(micro*second)
ns = nanosecond = nanoseconds = Quantity("nanosecond", abbrev="ns")
nanosecond.set_dimension(time)
nanosecond.set_scale_factor(nano*second)
ps = picosecond = picoseconds = Quantity("picosecond", abbrev="ps")
picosecond.set_dimension(time)
picosecond.set_scale_factor(pico*second)
minute = minutes = Quantity("minute")
minute.set_dimension(time)
minute.set_scale_factor(60*second)
h = hour = hours = Quantity("hour")
hour.set_dimension(time)
hour.set_scale_factor(60*minute)
day = days = Quantity("day")
day.set_dimension(time)
day.set_scale_factor(24*hour)
anomalistic_year = anomalistic_years = Quantity("anomalistic_year")
anomalistic_year.set_dimension(time)
anomalistic_year.set_scale_factor(365.259636*day)
sidereal_year = sidereal_years = Quantity("sidereal_year")
sidereal_year.set_dimension(time)
sidereal_year.set_scale_factor(31558149.540)
tropical_year = tropical_years = Quantity("tropical_year")
tropical_year.set_dimension(time)
tropical_year.set_scale_factor(365.24219*day)
common_year = common_years = Quantity("common_year")
common_year.set_dimension(time)
common_year.set_scale_factor(365*day)
julian_year = julian_years = Quantity("julian_year")
julian_year.set_dimension(time)
julian_year.set_scale_factor((365 + One/4)*day)
draconic_year = draconic_years = Quantity("draconic_year")
draconic_year.set_dimension(time)
draconic_year.set_scale_factor(346.62*day)
gaussian_year = gaussian_years = Quantity("gaussian_year")
gaussian_year.set_dimension(time)
gaussian_year.set_scale_factor(365.2568983*day)
full_moon_cycle = full_moon_cycles = Quantity("full_moon_cycle")
full_moon_cycle.set_dimension(time)
full_moon_cycle.set_scale_factor(411.78443029*day)
year = years = tropical_year
#### CONSTANTS ####
# Newton constant
# REF: NIST SP 959 (June 2019)
G = gravitational_constant = Quantity("gravitational_constant", abbrev="G")
gravitational_constant.set_dimension(length**3*mass**-1*time**-2)
gravitational_constant.set_scale_factor(6.67430e-11*m**3/(kg*s**2))
# speed of light
c = speed_of_light = Quantity("speed_of_light", abbrev="c")
speed_of_light.set_dimension(velocity)
speed_of_light.set_scale_factor(299792458*meter/second)
# elementary charge
# REF: NIST SP 959 (June 2019)
elementary_charge = Quantity("elementary_charge", abbrev="e")
elementary_charge.set_dimension(charge)
elementary_charge.set_scale_factor(1.602176634e-19*coulomb)
# Planck constant
# REF: NIST SP 959 (June 2019)
planck = Quantity("planck", abbrev="h")
planck.set_dimension(action)
planck.set_scale_factor(6.62607015e-34*joule*second)
# Reduced Planck constant
# REF: NIST SP 959 (June 2019)
hbar = Quantity("hbar", abbrev="hbar")
hbar.set_dimension(action)
hbar.set_scale_factor(planck / (2 * pi))
# Electronvolt
# REF: NIST SP 959 (June 2019)
eV = electronvolt = electronvolts = Quantity("electronvolt", abbrev="eV")
electronvolt.set_dimension(energy)
electronvolt.set_scale_factor(1.602176634e-19*joule)
# Avogadro number
# REF: NIST SP 959 (June 2019)
avogadro_number = Quantity("avogadro_number")
avogadro_number.set_dimension(One)
avogadro_number.set_scale_factor(6.02214076e23)
# Avogadro constant
avogadro = avogadro_constant = Quantity("avogadro_constant")
avogadro_constant.set_dimension(amount_of_substance**-1)
avogadro_constant.set_scale_factor(avogadro_number / mol)
# Boltzmann constant
# REF: NIST SP 959 (June 2019)
boltzmann = boltzmann_constant = Quantity("boltzmann_constant")
boltzmann_constant.set_dimension(energy/temperature)
boltzmann_constant.set_scale_factor(1.380649e-23*joule/kelvin)
# Stefan-Boltzmann constant
# REF: NIST SP 959 (June 2019)
stefan = stefan_boltzmann_constant = Quantity("stefan_boltzmann_constant")
stefan_boltzmann_constant.set_dimension(energy*time**-1*length**-2*temperature**-4)
stefan_boltzmann_constant.set_scale_factor(pi**2 * boltzmann_constant**4 / (60 * hbar**3 * speed_of_light ** 2))
# Atomic mass
# REF: NIST SP 959 (June 2019)
amu = amus = atomic_mass_unit = atomic_mass_constant = Quantity("atomic_mass_constant")
atomic_mass_constant.set_dimension(mass)
atomic_mass_constant.set_scale_factor(1.66053906660e-24*gram)
# Molar gas constant
# REF: NIST SP 959 (June 2019)
R = molar_gas_constant = Quantity("molar_gas_constant", abbrev="R")
molar_gas_constant.set_dimension(energy/(temperature * amount_of_substance))
molar_gas_constant.set_scale_factor(boltzmann_constant * avogadro_constant)
# Faraday constant
faraday_constant = Quantity("faraday_constant")
faraday_constant.set_dimension(charge/amount_of_substance)
faraday_constant.set_scale_factor(elementary_charge * avogadro_constant)
# Josephson constant
josephson_constant = Quantity("josephson_constant", abbrev="K_j")
josephson_constant.set_dimension(frequency/voltage)
josephson_constant.set_scale_factor(0.5 * planck / elementary_charge)
# Von Klitzing constant
von_klitzing_constant = Quantity("von_klitzing_constant", abbrev="R_k")
von_klitzing_constant.set_dimension(voltage/current)
von_klitzing_constant.set_scale_factor(hbar / elementary_charge ** 2)
# Acceleration due to gravity (on the Earth surface)
gee = gees = acceleration_due_to_gravity = Quantity("acceleration_due_to_gravity", abbrev="g")
acceleration_due_to_gravity.set_dimension(acceleration)
acceleration_due_to_gravity.set_scale_factor(9.80665*meter/second**2)
# magnetic constant:
u0 = magnetic_constant = vacuum_permeability = Quantity("magnetic_constant")
magnetic_constant.set_dimension(force/current**2)
magnetic_constant.set_scale_factor(4*pi/10**7 * newton/ampere**2)
# electric constat:
e0 = electric_constant = vacuum_permittivity = Quantity("vacuum_permittivity")
vacuum_permittivity.set_dimension(capacitance/length)
vacuum_permittivity.set_scale_factor(1/(u0 * c**2))
# vacuum impedance:
Z0 = vacuum_impedance = Quantity("vacuum_impedance", abbrev='Z_0', latex_repr=r'Z_{0}')
vacuum_impedance.set_dimension(impedance)
vacuum_impedance.set_scale_factor(u0 * c)
# Coulomb's constant:
coulomb_constant = coulombs_constant = electric_force_constant = \
Quantity("coulomb_constant", abbrev="k_e")
coulomb_constant.set_dimension(force*length**2/charge**2)
coulomb_constant.set_scale_factor(1/(4*pi*vacuum_permittivity))
atmosphere = atmospheres = atm = Quantity("atmosphere", abbrev="atm")
atmosphere.set_dimension(pressure)
atmosphere.set_scale_factor(101325 * pascal)
kPa = kilopascal = Quantity("kilopascal", abbrev="kPa")
kilopascal.set_dimension(pressure)
kilopascal.set_scale_factor(kilo*Pa)
bar = bars = Quantity("bar", abbrev="bar")
bar.set_dimension(pressure)
bar.set_scale_factor(100*kPa)
pound = pounds = Quantity("pound") # exact
pound.set_dimension(mass)
pound.set_scale_factor(Rational(45359237, 100000000) * kg)
psi = Quantity("psi")
psi.set_dimension(pressure)
psi.set_scale_factor(pound * gee / inch ** 2)
dHg0 = 13.5951 # approx value at 0 C
mmHg = torr = Quantity("mmHg")
mmHg.set_dimension(pressure)
mmHg.set_scale_factor(dHg0 * acceleration_due_to_gravity * kilogram / meter**2)
mmu = mmus = milli_mass_unit = Quantity("milli_mass_unit")
milli_mass_unit.set_dimension(mass)
milli_mass_unit.set_scale_factor(atomic_mass_unit/1000)
quart = quarts = Quantity("quart")
quart.set_dimension(length**3)
quart.set_scale_factor(Rational(231, 4) * inch**3)
# Other convenient units and magnitudes
ly = lightyear = lightyears = Quantity("lightyear", abbrev="ly")
lightyear.set_dimension(length)
lightyear.set_scale_factor(speed_of_light*julian_year)
au = astronomical_unit = astronomical_units = Quantity("astronomical_unit", abbrev="AU")
astronomical_unit.set_dimension(length)
astronomical_unit.set_scale_factor(149597870691*meter)
# Fundamental Planck units:
planck_mass = Quantity("planck_mass", abbrev="m_P", latex_repr=r'm_\text{P}')
planck_mass.set_dimension(mass)
planck_mass.set_scale_factor(sqrt(hbar*speed_of_light/G))
planck_time = Quantity("planck_time", abbrev="t_P", latex_repr=r't_\text{P}')
planck_time.set_dimension(time)
planck_time.set_scale_factor(sqrt(hbar*G/speed_of_light**5))
planck_temperature = Quantity("planck_temperature", abbrev="T_P",
latex_repr=r'T_\text{P}')
planck_temperature.set_dimension(temperature)
planck_temperature.set_scale_factor(sqrt(hbar*speed_of_light**5/G/boltzmann**2))
planck_length = Quantity("planck_length", abbrev="l_P", latex_repr=r'l_\text{P}')
planck_length.set_dimension(length)
planck_length.set_scale_factor(sqrt(hbar*G/speed_of_light**3))
planck_charge = Quantity("planck_charge", abbrev="q_P", latex_repr=r'q_\text{P}')
planck_charge.set_dimension(charge)
planck_charge.set_scale_factor(sqrt(4*pi*electric_constant*hbar*speed_of_light))
# Derived Planck units:
planck_area = Quantity("planck_area")
planck_area.set_dimension(length**2)
planck_area.set_scale_factor(planck_length**2)
planck_volume = Quantity("planck_volume")
planck_volume.set_dimension(length**3)
planck_volume.set_scale_factor(planck_length**3)
planck_momentum = Quantity("planck_momentum")
planck_momentum.set_dimension(mass*velocity)
planck_momentum.set_scale_factor(planck_mass * speed_of_light)
planck_energy = Quantity("planck_energy", abbrev="E_P", latex_repr=r'E_\text{P}')
planck_energy.set_dimension(energy)
planck_energy.set_scale_factor(planck_mass * speed_of_light**2)
planck_force = Quantity("planck_force", abbrev="F_P", latex_repr=r'F_\text{P}')
planck_force.set_dimension(force)
planck_force.set_scale_factor(planck_energy / planck_length)
planck_power = Quantity("planck_power", abbrev="P_P", latex_repr=r'P_\text{P}')
planck_power.set_dimension(power)
planck_power.set_scale_factor(planck_energy / planck_time)
planck_density = Quantity("planck_density", abbrev="rho_P", latex_repr=r'\rho_\text{P}')
planck_density.set_dimension(mass/length**3)
planck_density.set_scale_factor(planck_mass / planck_length**3)
planck_energy_density = Quantity("planck_energy_density", abbrev="rho^E_P")
planck_energy_density.set_dimension(energy / length**3)
planck_energy_density.set_scale_factor(planck_energy / planck_length**3)
planck_intensity = Quantity("planck_intensity", abbrev="I_P", latex_repr=r'I_\text{P}')
planck_intensity.set_dimension(mass * time**(-3))
planck_intensity.set_scale_factor(planck_energy_density * speed_of_light)
planck_angular_frequency = Quantity("planck_angular_frequency", abbrev="omega_P",
latex_repr=r'\omega_\text{P}')
planck_angular_frequency.set_dimension(1 / time)
planck_angular_frequency.set_scale_factor(1 / planck_time)
planck_pressure = Quantity("planck_pressure", abbrev="p_P", latex_repr=r'p_\text{P}')
planck_pressure.set_dimension(pressure)
planck_pressure.set_scale_factor(planck_force / planck_length**2)
planck_current = Quantity("planck_current", abbrev="I_P", latex_repr=r'I_\text{P}')
planck_current.set_dimension(current)
planck_current.set_scale_factor(planck_charge / planck_time)
planck_voltage = Quantity("planck_voltage", abbrev="V_P", latex_repr=r'V_\text{P}')
planck_voltage.set_dimension(voltage)
planck_voltage.set_scale_factor(planck_energy / planck_charge)
planck_impedance = Quantity("planck_impedance", abbrev="Z_P", latex_repr=r'Z_\text{P}')
planck_impedance.set_dimension(impedance)
planck_impedance.set_scale_factor(planck_voltage / planck_current)
planck_acceleration = Quantity("planck_acceleration", abbrev="a_P",
latex_repr=r'a_\text{P}')
planck_acceleration.set_dimension(acceleration)
planck_acceleration.set_scale_factor(speed_of_light / planck_time)
# Information theory units:
bit = bits = Quantity("bit")
bit.set_dimension(information)
bit.set_scale_factor(One)
byte = bytes = Quantity("byte")
byte.set_dimension(information)
byte.set_scale_factor(8*bit)
kibibyte = kibibytes = Quantity("kibibyte")
kibibyte.set_dimension(information)
kibibyte.set_scale_factor(kibi*byte)
mebibyte = mebibytes = Quantity("mebibyte")
mebibyte.set_dimension(information)
mebibyte.set_scale_factor(mebi*byte)
gibibyte = gibibytes = Quantity("gibibyte")
gibibyte.set_dimension(information)
gibibyte.set_scale_factor(gibi*byte)
tebibyte = tebibytes = Quantity("tebibyte")
tebibyte.set_dimension(information)
tebibyte.set_scale_factor(tebi*byte)
pebibyte = pebibytes = Quantity("pebibyte")
pebibyte.set_dimension(information)
pebibyte.set_scale_factor(pebi*byte)
exbibyte = exbibytes = Quantity("exbibyte")
exbibyte.set_dimension(information)
exbibyte.set_scale_factor(exbi*byte)
# Older units for radioactivity
curie = Ci = Quantity("curie", abbrev="Ci")
curie.set_dimension(1/time)
curie.set_scale_factor(37000000000*becquerel)
rutherford = Rd = Quantity("rutherford", abbrev="Rd")
rutherford.set_dimension(1/time)
rutherford.set_scale_factor(1000000*becquerel)
# check that scale factors are the right SI dimensions:
for _scale_factor, _dimension in zip(
Quantity.SI_quantity_scale_factors.values(),
Quantity.SI_quantity_dimension_map.values()):
dimex = Quantity.get_dimensional_expr(_scale_factor)
if dimex != 1:
if not dimsys_default.equivalent_dims(_dimension, Dimension(dimex)):
raise ValueError("quantity value and dimension mismatch")
del _scale_factor, _dimension
|
4cb223cc8f51ad0234f13290e3f09bf092b6753d77f86ba22e27f978869f9a38 | # isort:skip_file
"""
Dimensional analysis and unit systems.
This module defines dimension/unit systems and physical quantities. It is
based on a group-theoretical construction where dimensions are represented as
vectors (coefficients being the exponents), and units are defined as a dimension
to which we added a scale.
Quantities are built from a factor and a unit, and are the basic objects that
one will use when doing computations.
All objects except systems and prefixes can be used in sympy expressions.
Note that as part of a CAS, various objects do not combine automatically
under operations.
Details about the implementation can be found in the documentation, and we
will not repeat all the explanations we gave there concerning our approach.
Ideas about future developments can be found on the `Github wiki
<https://github.com/sympy/sympy/wiki/Unit-systems>`_, and you should consult
this page if you are willing to help.
Useful functions:
- ``find_unit``: easily lookup pre-defined units.
- ``convert_to(expr, newunit)``: converts an expression into the same
expression expressed in another unit.
"""
from sympy.core.compatibility import string_types
from .dimensions import Dimension, DimensionSystem
from .unitsystem import UnitSystem
from .util import convert_to
from .quantities import Quantity
from .dimensions import (
amount_of_substance, acceleration, action,
capacitance, charge, conductance, current, energy,
force, frequency, impedance, inductance, length,
luminous_intensity, magnetic_density,
magnetic_flux, mass, momentum, power, pressure, temperature, time,
velocity, voltage, volume
)
Unit = Quantity
speed = velocity
luminosity = luminous_intensity
magnetic_flux_density = magnetic_density
amount = amount_of_substance
from .prefixes import (
# 10-power based:
yotta,
zetta,
exa,
peta,
tera,
giga,
mega,
kilo,
hecto,
deca,
deci,
centi,
milli,
micro,
nano,
pico,
femto,
atto,
zepto,
yocto,
# 2-power based:
kibi,
mebi,
gibi,
tebi,
pebi,
exbi,
)
from .definitions import (
percent, percents,
permille,
rad, radian, radians,
deg, degree, degrees,
sr, steradian, steradians,
mil, angular_mil, angular_mils,
m, meter, meters,
kg, kilogram, kilograms,
s, second, seconds,
A, ampere, amperes,
K, kelvin, kelvins,
mol, mole, moles,
cd, candela, candelas,
g, gram, grams,
mg, milligram, milligrams,
ug, microgram, micrograms,
newton, newtons, N,
joule, joules, J,
watt, watts, W,
pascal, pascals, Pa, pa,
hertz, hz, Hz,
coulomb, coulombs, C,
volt, volts, v, V,
ohm, ohms,
siemens, S, mho, mhos,
farad, farads, F,
henry, henrys, H,
tesla, teslas, T,
weber, webers, Wb, wb,
optical_power, dioptre, D,
lux, lx,
katal, kat,
gray, Gy,
becquerel, Bq,
km, kilometer, kilometers,
dm, decimeter, decimeters,
cm, centimeter, centimeters,
mm, millimeter, millimeters,
um, micrometer, micrometers, micron, microns,
nm, nanometer, nanometers,
pm, picometer, picometers,
ft, foot, feet,
inch, inches,
yd, yard, yards,
mi, mile, miles,
nmi, nautical_mile, nautical_miles,
l, liter, liters,
dl, deciliter, deciliters,
cl, centiliter, centiliters,
ml, milliliter, milliliters,
ms, millisecond, milliseconds,
us, microsecond, microseconds,
ns, nanosecond, nanoseconds,
ps, picosecond, picoseconds,
minute, minutes,
h, hour, hours,
day, days,
anomalistic_year, anomalistic_years,
sidereal_year, sidereal_years,
tropical_year, tropical_years,
common_year, common_years,
julian_year, julian_years,
draconic_year, draconic_years,
gaussian_year, gaussian_years,
full_moon_cycle, full_moon_cycles,
year, years, tropical_year,
G, gravitational_constant,
c, speed_of_light,
elementary_charge,
Z0,
hbar,
planck,
eV, electronvolt, electronvolts,
avogadro_number,
avogadro, avogadro_constant,
boltzmann, boltzmann_constant,
stefan, stefan_boltzmann_constant,
R, molar_gas_constant,
faraday_constant,
josephson_constant,
von_klitzing_constant,
amu, amus, atomic_mass_unit, atomic_mass_constant,
gee, gees, acceleration_due_to_gravity,
u0, magnetic_constant, vacuum_permeability,
e0, electric_constant, vacuum_permittivity,
Z0, vacuum_impedance,
coulomb_constant, electric_force_constant,
atmosphere, atmospheres, atm,
kPa,
bar, bars,
pound, pounds,
psi,
dHg0,
mmHg, torr,
mmu, mmus, milli_mass_unit,
quart, quarts,
ly, lightyear, lightyears,
au, astronomical_unit, astronomical_units,
planck_mass,
planck_time,
planck_temperature,
planck_length,
planck_charge,
planck_area,
planck_volume,
planck_momentum,
planck_energy,
planck_force,
planck_power,
planck_density,
planck_energy_density,
planck_intensity,
planck_angular_frequency,
planck_pressure,
planck_current,
planck_voltage,
planck_impedance,
planck_acceleration,
bit, bits,
byte,
kibibyte, kibibytes,
mebibyte, mebibytes,
gibibyte, gibibytes,
tebibyte, tebibytes,
pebibyte, pebibytes,
exbibyte, exbibytes,
)
def find_unit(quantity):
"""
Return a list of matching units or dimension names.
- If ``quantity`` is a string -- units/dimensions containing the string
`quantity`.
- If ``quantity`` is a unit or dimension -- units having matching base
units or dimensions.
Examples
========
>>> from sympy.physics import units as u
>>> u.find_unit('charge')
['C', 'coulomb', 'coulombs', 'planck_charge', 'elementary_charge']
>>> u.find_unit(u.charge)
['C', 'coulomb', 'coulombs', 'planck_charge', 'elementary_charge']
>>> u.find_unit("ampere")
['ampere', 'amperes']
>>> u.find_unit('volt')
['volt', 'volts', 'electronvolt', 'electronvolts', 'planck_voltage']
>>> u.find_unit(u.inch**3)[:5]
['l', 'cl', 'dl', 'ml', 'liter']
"""
import sympy.physics.units as u
rv = []
if isinstance(quantity, string_types):
rv = [i for i in dir(u) if quantity in i and isinstance(getattr(u, i), Quantity)]
dim = getattr(u, quantity)
if isinstance(dim, Dimension):
rv.extend(find_unit(dim))
else:
for i in sorted(dir(u)):
other = getattr(u, i)
if not isinstance(other, Quantity):
continue
if isinstance(quantity, Quantity):
if quantity.dimension == other.dimension:
rv.append(str(i))
elif isinstance(quantity, Dimension):
if other.dimension == quantity:
rv.append(str(i))
elif other.dimension == Dimension(Quantity.get_dimensional_expr(quantity)):
rv.append(str(i))
return sorted(set(rv), key=lambda x: (len(x), x))
# NOTE: the old units module had additional variables:
# 'density', 'illuminance', 'resistance'.
# They were not dimensions, but units (old Unit class).
|
a2663363ffec5675f8372d874eb939a057fde3c0ad2d4d73c9fef0475a4c10b0 | """
Module defining unit prefixe class and some constants.
Constant dict for SI and binary prefixes are defined as PREFIXES and
BIN_PREFIXES.
"""
from sympy import Expr, sympify
class Prefix(Expr):
"""
This class represent prefixes, with their name, symbol and factor.
Prefixes are used to create derived units from a given unit. They should
always be encapsulated into units.
The factor is constructed from a base (default is 10) to some power, and
it gives the total multiple or fraction. For example the kilometer km
is constructed from the meter (factor 1) and the kilo (10 to the power 3,
i.e. 1000). The base can be changed to allow e.g. binary prefixes.
A prefix multiplied by something will always return the product of this
other object times the factor, except if the other object:
- is a prefix and they can be combined into a new prefix;
- defines multiplication with prefixes (which is the case for the Unit
class).
"""
_op_priority = 13.0
is_commutative = True
def __new__(cls, name, abbrev, exponent, base=sympify(10)):
name = sympify(name)
abbrev = sympify(abbrev)
exponent = sympify(exponent)
base = sympify(base)
obj = Expr.__new__(cls, name, abbrev, exponent, base)
obj._name = name
obj._abbrev = abbrev
obj._scale_factor = base**exponent
obj._exponent = exponent
obj._base = base
return obj
@property
def name(self):
return self._name
@property
def abbrev(self):
return self._abbrev
@property
def scale_factor(self):
return self._scale_factor
@property
def base(self):
return self._base
def __str__(self):
# TODO: add proper printers and tests:
if self.base == 10:
return "Prefix(%r, %r, %r)" % (
str(self.name), str(self.abbrev), self._exponent)
else:
return "Prefix(%r, %r, %r, %r)" % (
str(self.name), str(self.abbrev), self._exponent, self.base)
__repr__ = __str__
def __mul__(self, other):
if not hasattr(other, "scale_factor"):
return super(Prefix, self).__mul__(other)
fact = self.scale_factor * other.scale_factor
if fact == 1:
return 1
elif isinstance(other, Prefix):
# simplify prefix
for p in PREFIXES:
if PREFIXES[p].scale_factor == fact:
return PREFIXES[p]
return fact
return self.scale_factor * other
def __div__(self, other):
if not hasattr(other, "scale_factor"):
return super(Prefix, self).__div__(other)
fact = self.scale_factor / other.scale_factor
if fact == 1:
return 1
elif isinstance(other, Prefix):
for p in PREFIXES:
if PREFIXES[p].scale_factor == fact:
return PREFIXES[p]
return fact
return self.scale_factor / other
__truediv__ = __div__
def __rdiv__(self, other):
if other == 1:
for p in PREFIXES:
if PREFIXES[p].scale_factor == 1 / self.scale_factor:
return PREFIXES[p]
return other / self.scale_factor
__rtruediv__ = __rdiv__
def prefix_unit(unit, prefixes):
"""
Return a list of all units formed by unit and the given prefixes.
You can use the predefined PREFIXES or BIN_PREFIXES, but you can also
pass as argument a subdict of them if you don't want all prefixed units.
>>> from sympy.physics.units.prefixes import (PREFIXES,
... prefix_unit)
>>> from sympy.physics.units.systems import MKS
>>> from sympy.physics.units import m
>>> pref = {"m": PREFIXES["m"], "c": PREFIXES["c"], "d": PREFIXES["d"]}
>>> prefix_unit(m, pref) # doctest: +SKIP
[millimeter, centimeter, decimeter]
"""
from sympy.physics.units.quantities import Quantity
prefixed_units = []
for prefix_abbr, prefix in prefixes.items():
quantity = Quantity(
"%s%s" % (prefix.name, unit.name),
abbrev=("%s%s" % (prefix.abbrev, unit.abbrev))
)
quantity.set_dimension(unit.dimension)
quantity.set_scale_factor(unit.scale_factor*prefix)
prefixed_units.append(quantity)
return prefixed_units
yotta = Prefix('yotta', 'Y', 24)
zetta = Prefix('zetta', 'Z', 21)
exa = Prefix('exa', 'E', 18)
peta = Prefix('peta', 'P', 15)
tera = Prefix('tera', 'T', 12)
giga = Prefix('giga', 'G', 9)
mega = Prefix('mega', 'M', 6)
kilo = Prefix('kilo', 'k', 3)
hecto = Prefix('hecto', 'h', 2)
deca = Prefix('deca', 'da', 1)
deci = Prefix('deci', 'd', -1)
centi = Prefix('centi', 'c', -2)
milli = Prefix('milli', 'm', -3)
micro = Prefix('micro', 'mu', -6)
nano = Prefix('nano', 'n', -9)
pico = Prefix('pico', 'p', -12)
femto = Prefix('femto', 'f', -15)
atto = Prefix('atto', 'a', -18)
zepto = Prefix('zepto', 'z', -21)
yocto = Prefix('yocto', 'y', -24)
# http://physics.nist.gov/cuu/Units/prefixes.html
PREFIXES = {
'Y': yotta,
'Z': zetta,
'E': exa,
'P': peta,
'T': tera,
'G': giga,
'M': mega,
'k': kilo,
'h': hecto,
'da': deca,
'd': deci,
'c': centi,
'm': milli,
'mu': micro,
'n': nano,
'p': pico,
'f': femto,
'a': atto,
'z': zepto,
'y': yocto,
}
kibi = Prefix('kibi', 'Y', 10, 2)
mebi = Prefix('mebi', 'Y', 20, 2)
gibi = Prefix('gibi', 'Y', 30, 2)
tebi = Prefix('tebi', 'Y', 40, 2)
pebi = Prefix('pebi', 'Y', 50, 2)
exbi = Prefix('exbi', 'Y', 60, 2)
# http://physics.nist.gov/cuu/Units/binary.html
BIN_PREFIXES = {
'Ki': kibi,
'Mi': mebi,
'Gi': gibi,
'Ti': tebi,
'Pi': pebi,
'Ei': exbi,
}
|
821ebbbb29969b373c85f4f0ebc39df10ad7cfdb028e7536f13ff1f8bb67cbd5 | """
Several methods to simplify expressions involving unit objects.
"""
from __future__ import division
from sympy.utilities.exceptions import SymPyDeprecationWarning
from sympy import Add, Mul, Pow, Tuple, sympify
from sympy.core.compatibility import reduce, Iterable, ordered
from sympy.physics.units.dimensions import Dimension, dimsys_default
from sympy.physics.units.prefixes import Prefix
from sympy.physics.units.quantities import Quantity
from sympy.utilities.iterables import sift
def dim_simplify(expr):
"""
NOTE: this function could be deprecated in the future.
Simplify expression by recursively evaluating the dimension arguments.
This function proceeds to a very rough dimensional analysis. It tries to
simplify expression with dimensions, and it deletes all what multiplies a
dimension without being a dimension. This is necessary to avoid strange
behavior when Add(L, L) be transformed into Mul(2, L).
"""
SymPyDeprecationWarning(
deprecated_since_version="1.2",
feature="dimensional simplification function",
issue=13336,
useinstead="don't use",
).warn()
_, expr = Quantity._collect_factor_and_dimension(expr)
return expr
def _get_conversion_matrix_for_expr(expr, target_units):
from sympy import Matrix
expr_dim = Dimension(Quantity.get_dimensional_expr(expr))
dim_dependencies = dimsys_default.get_dimensional_dependencies(expr_dim, mark_dimensionless=True)
target_dims = [Dimension(Quantity.get_dimensional_expr(x)) for x in target_units]
canon_dim_units = {i for x in target_dims for i in dimsys_default.get_dimensional_dependencies(x, mark_dimensionless=True)}
canon_expr_units = {i for i in dim_dependencies}
if not canon_expr_units.issubset(canon_dim_units):
return None
canon_dim_units = sorted(canon_dim_units)
camat = Matrix([[dimsys_default.get_dimensional_dependencies(i, mark_dimensionless=True).get(j, 0) for i in target_dims] for j in canon_dim_units])
exprmat = Matrix([dim_dependencies.get(k, 0) for k in canon_dim_units])
res_exponents = camat.solve_least_squares(exprmat, method=None)
return res_exponents
def convert_to(expr, target_units):
"""
Convert ``expr`` to the same expression with all of its units and quantities
represented as factors of ``target_units``, whenever the dimension is compatible.
``target_units`` may be a single unit/quantity, or a collection of
units/quantities.
Examples
========
>>> from sympy.physics.units import speed_of_light, meter, gram, second, day
>>> from sympy.physics.units import mile, newton, kilogram, atomic_mass_constant
>>> from sympy.physics.units import kilometer, centimeter
>>> from sympy.physics.units import gravitational_constant, hbar
>>> from sympy.physics.units import convert_to
>>> convert_to(mile, kilometer)
25146*kilometer/15625
>>> convert_to(mile, kilometer).n()
1.609344*kilometer
>>> convert_to(speed_of_light, meter/second)
299792458*meter/second
>>> convert_to(day, second)
86400*second
>>> 3*newton
3*newton
>>> convert_to(3*newton, kilogram*meter/second**2)
3*kilogram*meter/second**2
>>> convert_to(atomic_mass_constant, gram)
1.660539060e-24*gram
Conversion to multiple units:
>>> convert_to(speed_of_light, [meter, second])
299792458*meter/second
>>> convert_to(3*newton, [centimeter, gram, second])
300000*centimeter*gram/second**2
Conversion to Planck units:
>>> from sympy.physics.units import gravitational_constant, hbar
>>> convert_to(atomic_mass_constant, [gravitational_constant, speed_of_light, hbar]).n()
7.62963085040767e-20*gravitational_constant**(-0.5)*hbar**0.5*speed_of_light**0.5
"""
if not isinstance(target_units, (Iterable, Tuple)):
target_units = [target_units]
if isinstance(expr, Add):
return Add.fromiter(convert_to(i, target_units) for i in expr.args)
expr = sympify(expr)
if not isinstance(expr, Quantity) and expr.has(Quantity):
expr = expr.replace(lambda x: isinstance(x, Quantity), lambda x: x.convert_to(target_units))
def get_total_scale_factor(expr):
if isinstance(expr, Mul):
return reduce(lambda x, y: x * y, [get_total_scale_factor(i) for i in expr.args])
elif isinstance(expr, Pow):
return get_total_scale_factor(expr.base) ** expr.exp
elif isinstance(expr, Quantity):
return expr.scale_factor
return expr
depmat = _get_conversion_matrix_for_expr(expr, target_units)
if depmat is None:
return expr
expr_scale_factor = get_total_scale_factor(expr)
return expr_scale_factor * Mul.fromiter((1/get_total_scale_factor(u) * u) ** p for u, p in zip(target_units, depmat))
def quantity_simplify(expr):
"""Return an equivalent expression in which prefixes are replaced
with numerical values and all units of a given dimension are the
unified in a canonical manner.
Examples
========
>>> from sympy.physics.units.util import quantity_simplify
>>> from sympy.physics.units.prefixes import kilo
>>> from sympy.physics.units import foot, inch
>>> quantity_simplify(kilo*foot*inch)
250*foot**2/3
>>> quantity_simplify(foot - 6*inch)
foot/2
"""
if expr.is_Atom or not expr.has(Prefix, Quantity):
return expr
# replace all prefixes with numerical values
p = expr.atoms(Prefix)
expr = expr.xreplace({p: p.scale_factor for p in p})
# replace all quantities of given dimension with a canonical
# quantity, chosen from those in the expression
d = sift(expr.atoms(Quantity), lambda i: i.dimension)
for k in d:
if len(d[k]) == 1:
continue
v = list(ordered(d[k]))
ref = v[0]/v[0].scale_factor
expr = expr.xreplace({vi: ref*vi.scale_factor for vi in v[1:]})
return expr
def check_dimensions(expr):
"""Return expr if there are not unitless values added to
dimensional quantities, else raise a ValueError."""
from sympy.solvers.solveset import _term_factors
# the case of adding a number to a dimensional quantity
# is ignored for the sake of SymPy core routines, so this
# function will raise an error now if such an addend is
# found.
# Also, when doing substitutions, multiplicative constants
# might be introduced, so remove those now
adds = expr.atoms(Add)
DIM_OF = dimsys_default.get_dimensional_dependencies
for a in adds:
deset = set()
for ai in a.args:
if ai.is_number:
deset.add(())
continue
dims = []
skip = False
for i in Mul.make_args(ai):
if i.has(Quantity):
i = Dimension(Quantity.get_dimensional_expr(i))
if i.has(Dimension):
dims.extend(DIM_OF(i).items())
elif i.free_symbols:
skip = True
break
if not skip:
deset.add(tuple(sorted(dims)))
if len(deset) > 1:
raise ValueError(
"addends have incompatible dimensions")
# clear multiplicative constants on Dimensions which may be
# left after substitution
reps = {}
for m in expr.atoms(Mul):
if any(isinstance(i, Dimension) for i in m.args):
reps[m] = m.func(*[
i for i in m.args if not i.is_number])
return expr.xreplace(reps)
|
549c74d1915158843b69264fde0f7e454f1a19b61c3c36ae104c4c3ed6de4420 | """
Physical quantities.
"""
from __future__ import division
from sympy import (Abs, Add, AtomicExpr, Derivative, Function, Mul,
Pow, S, Symbol, sympify)
from sympy.core.compatibility import string_types
from sympy.physics.units import Dimension, dimensions
from sympy.physics.units.prefixes import Prefix
from sympy.utilities.exceptions import SymPyDeprecationWarning
class Quantity(AtomicExpr):
"""
Physical quantity: can be a unit of measure, a constant or a generic quantity.
"""
is_commutative = True
is_real = True
is_number = False
is_nonzero = True
_diff_wrt = True
def __new__(cls, name, abbrev=None, dimension=None, scale_factor=None,
latex_repr=None, pretty_unicode_repr=None,
pretty_ascii_repr=None, mathml_presentation_repr=None,
**assumptions):
if not isinstance(name, Symbol):
name = Symbol(name)
# For Quantity(name, dim, scale, abbrev) to work like in the
# old version of Sympy:
if not isinstance(abbrev, string_types) and not \
isinstance(abbrev, Symbol):
dimension, scale_factor, abbrev = abbrev, dimension, scale_factor
if dimension is not None:
SymPyDeprecationWarning(
deprecated_since_version="1.3",
issue=14319,
feature="Quantity arguments",
useinstead="SI_quantity_dimension_map",
).warn()
if scale_factor is not None:
SymPyDeprecationWarning(
deprecated_since_version="1.3",
issue=14319,
feature="Quantity arguments",
useinstead="SI_quantity_scale_factors",
).warn()
if abbrev is None:
abbrev = name
elif isinstance(abbrev, string_types):
abbrev = Symbol(abbrev)
obj = AtomicExpr.__new__(cls, name, abbrev)
obj._name = name
obj._abbrev = abbrev
obj._latex_repr = latex_repr
obj._unicode_repr = pretty_unicode_repr
obj._ascii_repr = pretty_ascii_repr
obj._mathml_repr = mathml_presentation_repr
if dimension is not None:
# TODO: remove after deprecation:
obj.set_dimension(dimension)
if scale_factor is not None:
# TODO: remove after deprecation:
obj.set_scale_factor(scale_factor)
return obj
### Currently only SI is supported: ###
# Dimensional representations for the SI units:
SI_quantity_dimension_map = {}
# Scale factors in SI units:
SI_quantity_scale_factors = {}
def set_dimension(self, dimension, unit_system="SI"):
from sympy.physics.units.dimensions import dimsys_default, DimensionSystem
if unit_system != "SI":
# TODO: add support for more units and dimension systems:
raise NotImplementedError("Currently only SI is supported")
dim_sys = dimsys_default
if not isinstance(dimension, dimensions.Dimension):
if dimension == 1:
dimension = Dimension(1)
else:
raise ValueError("expected dimension or 1")
else:
for dim_sym in dimension.name.atoms(Dimension):
if dim_sym not in [i.name for i in dim_sys._dimensional_dependencies]:
raise ValueError("Dimension %s is not registered in the "
"dimensional dependency tree." % dim_sym)
Quantity.SI_quantity_dimension_map[self] = dimension
def set_scale_factor(self, scale_factor, unit_system="SI"):
if unit_system != "SI":
# TODO: add support for more units and dimension systems:
raise NotImplementedError("Currently only SI is supported")
scale_factor = sympify(scale_factor)
# replace all prefixes by their ratio to canonical units:
scale_factor = scale_factor.replace(lambda x: isinstance(x, Prefix), lambda x: x.scale_factor)
# replace all quantities by their ratio to canonical units:
scale_factor = scale_factor.replace(lambda x: isinstance(x, Quantity), lambda x: x.scale_factor)
Quantity.SI_quantity_scale_factors[self] = scale_factor
@property
def name(self):
return self._name
@property
def dimension(self):
# TODO: add support for units other than SI:
return Quantity.SI_quantity_dimension_map[self]
@property
def abbrev(self):
"""
Symbol representing the unit name.
Prepend the abbreviation with the prefix symbol if it is defines.
"""
return self._abbrev
@property
def scale_factor(self):
"""
Overall magnitude of the quantity as compared to the canonical units.
"""
return Quantity.SI_quantity_scale_factors.get(self, S.One)
def _eval_is_positive(self):
return self.scale_factor.is_positive
def _eval_is_constant(self):
return self.scale_factor.is_constant()
def _eval_Abs(self):
scale_factor = Abs(self.scale_factor)
if scale_factor == self.scale_factor:
return self
return None
def _eval_subs(self, old, new):
if isinstance(new, Quantity) and self != old:
return self
@staticmethod
def get_dimensional_expr(expr):
if isinstance(expr, Mul):
return Mul(*[Quantity.get_dimensional_expr(i) for i in expr.args])
elif isinstance(expr, Pow):
return Quantity.get_dimensional_expr(expr.base) ** expr.exp
elif isinstance(expr, Add):
return Quantity.get_dimensional_expr(expr.args[0])
elif isinstance(expr, Derivative):
dim = Quantity.get_dimensional_expr(expr.expr)
for independent, count in expr.variable_count:
dim /= Quantity.get_dimensional_expr(independent)**count
return dim
elif isinstance(expr, Function):
args = [Quantity.get_dimensional_expr(arg) for arg in expr.args]
if all(i == 1 for i in args):
return S.One
return expr.func(*args)
elif isinstance(expr, Quantity):
return expr.dimension.name
return S.One
@staticmethod
def _collect_factor_and_dimension(expr):
"""Return tuple with factor expression and dimension expression."""
if isinstance(expr, Quantity):
return expr.scale_factor, expr.dimension
elif isinstance(expr, Mul):
factor = 1
dimension = Dimension(1)
for arg in expr.args:
arg_factor, arg_dim = Quantity._collect_factor_and_dimension(arg)
factor *= arg_factor
dimension *= arg_dim
return factor, dimension
elif isinstance(expr, Pow):
factor, dim = Quantity._collect_factor_and_dimension(expr.base)
exp_factor, exp_dim = Quantity._collect_factor_and_dimension(expr.exp)
if exp_dim.is_dimensionless:
exp_dim = 1
return factor ** exp_factor, dim ** (exp_factor * exp_dim)
elif isinstance(expr, Add):
factor, dim = Quantity._collect_factor_and_dimension(expr.args[0])
for addend in expr.args[1:]:
addend_factor, addend_dim = \
Quantity._collect_factor_and_dimension(addend)
if dim != addend_dim:
raise ValueError(
'Dimension of "{0}" is {1}, '
'but it should be {2}'.format(
addend, addend_dim, dim))
factor += addend_factor
return factor, dim
elif isinstance(expr, Derivative):
factor, dim = Quantity._collect_factor_and_dimension(expr.args[0])
for independent, count in expr.variable_count:
ifactor, idim = Quantity._collect_factor_and_dimension(independent)
factor /= ifactor**count
dim /= idim**count
return factor, dim
elif isinstance(expr, Function):
fds = [Quantity._collect_factor_and_dimension(
arg) for arg in expr.args]
return (expr.func(*(f[0] for f in fds)),
expr.func(*(d[1] for d in fds)))
elif isinstance(expr, Dimension):
return 1, expr
else:
return expr, Dimension(1)
def _latex(self, printer):
if self._latex_repr:
return self._latex_repr
else:
return r'\text{{{}}}'.format(self.args[1] \
if len(self.args) >= 2 else self.args[0])
def convert_to(self, other):
"""
Convert the quantity to another quantity of same dimensions.
Examples
========
>>> from sympy.physics.units import speed_of_light, meter, second
>>> speed_of_light
speed_of_light
>>> speed_of_light.convert_to(meter/second)
299792458*meter/second
>>> from sympy.physics.units import liter
>>> liter.convert_to(meter**3)
meter**3/1000
"""
from .util import convert_to
return convert_to(self, other)
@property
def free_symbols(self):
"""Return free symbols from quantity."""
return self.scale_factor.free_symbols
|
380c249b9ecd4cad012234659cb07ed332d7b7c2891158beb5f5e874f3a3033d | """
Module to handle gamma matrices expressed as tensor objects.
Examples
========
>>> from sympy.physics.hep.gamma_matrices import GammaMatrix as G, LorentzIndex
>>> from sympy.tensor.tensor import tensor_indices
>>> i = tensor_indices('i', LorentzIndex)
>>> G(i)
GammaMatrix(i)
Note that there is already an instance of GammaMatrixHead in four dimensions:
GammaMatrix, which is simply declare as
>>> from sympy.physics.hep.gamma_matrices import GammaMatrix
>>> from sympy.tensor.tensor import tensor_indices
>>> i = tensor_indices('i', LorentzIndex)
>>> GammaMatrix(i)
GammaMatrix(i)
To access the metric tensor
>>> LorentzIndex.metric
metric(LorentzIndex,LorentzIndex)
"""
from sympy import S, Mul, eye, trace
from sympy.tensor.tensor import TensorIndexType, TensorIndex,\
TensMul, TensAdd, tensor_mul, Tensor, TensorHead, TensorSymmetry
from sympy.core.compatibility import range
# DiracSpinorIndex = TensorIndexType('DiracSpinorIndex', dim=4, dummy_fmt="S")
LorentzIndex = TensorIndexType('LorentzIndex', dim=4, dummy_fmt="L")
GammaMatrix = TensorHead("GammaMatrix", [LorentzIndex],
TensorSymmetry.no_symmetry(1), comm=None)
def extract_type_tens(expression, component):
"""
Extract from a ``TensExpr`` all tensors with `component`.
Returns two tensor expressions:
* the first contains all ``Tensor`` of having `component`.
* the second contains all remaining.
"""
if isinstance(expression, Tensor):
sp = [expression]
elif isinstance(expression, TensMul):
sp = expression.args
else:
raise ValueError('wrong type')
# Collect all gamma matrices of the same dimension
new_expr = S.One
residual_expr = S.One
for i in sp:
if isinstance(i, Tensor) and i.component == component:
new_expr *= i
else:
residual_expr *= i
return new_expr, residual_expr
def simplify_gamma_expression(expression):
extracted_expr, residual_expr = extract_type_tens(expression, GammaMatrix)
res_expr = _simplify_single_line(extracted_expr)
return res_expr * residual_expr
def simplify_gpgp(ex, sort=True):
"""
simplify products ``G(i)*p(-i)*G(j)*p(-j) -> p(i)*p(-i)``
Examples
========
>>> from sympy.physics.hep.gamma_matrices import GammaMatrix as G, \
LorentzIndex, simplify_gpgp
>>> from sympy.tensor.tensor import tensor_indices, tensor_heads
>>> p, q = tensor_heads('p, q', [LorentzIndex])
>>> i0,i1,i2,i3,i4,i5 = tensor_indices('i0:6', LorentzIndex)
>>> ps = p(i0)*G(-i0)
>>> qs = q(i0)*G(-i0)
>>> simplify_gpgp(ps*qs*qs)
GammaMatrix(-L_0)*p(L_0)*q(L_1)*q(-L_1)
"""
def _simplify_gpgp(ex):
components = ex.components
a = []
comp_map = []
for i, comp in enumerate(components):
comp_map.extend([i]*comp.rank)
dum = [(i[0], i[1], comp_map[i[0]], comp_map[i[1]]) for i in ex.dum]
for i in range(len(components)):
if components[i] != GammaMatrix:
continue
for dx in dum:
if dx[2] == i:
p_pos1 = dx[3]
elif dx[3] == i:
p_pos1 = dx[2]
else:
continue
comp1 = components[p_pos1]
if comp1.comm == 0 and comp1.rank == 1:
a.append((i, p_pos1))
if not a:
return ex
elim = set()
tv = []
hit = True
coeff = S.One
ta = None
while hit:
hit = False
for i, ai in enumerate(a[:-1]):
if ai[0] in elim:
continue
if ai[0] != a[i + 1][0] - 1:
continue
if components[ai[1]] != components[a[i + 1][1]]:
continue
elim.add(ai[0])
elim.add(ai[1])
elim.add(a[i + 1][0])
elim.add(a[i + 1][1])
if not ta:
ta = ex.split()
mu = TensorIndex('mu', LorentzIndex)
hit = True
if i == 0:
coeff = ex.coeff
tx = components[ai[1]](mu)*components[ai[1]](-mu)
if len(a) == 2:
tx *= 4 # eye(4)
tv.append(tx)
break
if tv:
a = [x for j, x in enumerate(ta) if j not in elim]
a.extend(tv)
t = tensor_mul(*a)*coeff
# t = t.replace(lambda x: x.is_Matrix, lambda x: 1)
return t
else:
return ex
if sort:
ex = ex.sorted_components()
# this would be better off with pattern matching
while 1:
t = _simplify_gpgp(ex)
if t != ex:
ex = t
else:
return t
def gamma_trace(t):
"""
trace of a single line of gamma matrices
Examples
========
>>> from sympy.physics.hep.gamma_matrices import GammaMatrix as G, \
gamma_trace, LorentzIndex
>>> from sympy.tensor.tensor import tensor_indices, tensor_heads
>>> p, q = tensor_heads('p, q', [LorentzIndex])
>>> i0,i1,i2,i3,i4,i5 = tensor_indices('i0:6', LorentzIndex)
>>> ps = p(i0)*G(-i0)
>>> qs = q(i0)*G(-i0)
>>> gamma_trace(G(i0)*G(i1))
4*metric(i0, i1)
>>> gamma_trace(ps*ps) - 4*p(i0)*p(-i0)
0
>>> gamma_trace(ps*qs + ps*ps) - 4*p(i0)*p(-i0) - 4*p(i0)*q(-i0)
0
"""
if isinstance(t, TensAdd):
res = TensAdd(*[_trace_single_line(x) for x in t.args])
return res
t = _simplify_single_line(t)
res = _trace_single_line(t)
return res
def _simplify_single_line(expression):
"""
Simplify single-line product of gamma matrices.
Examples
========
>>> from sympy.physics.hep.gamma_matrices import GammaMatrix as G, \
LorentzIndex, _simplify_single_line
>>> from sympy.tensor.tensor import tensor_indices, TensorHead
>>> p = TensorHead('p', [LorentzIndex])
>>> i0,i1 = tensor_indices('i0:2', LorentzIndex)
>>> _simplify_single_line(G(i0)*G(i1)*p(-i1)*G(-i0)) + 2*G(i0)*p(-i0)
0
"""
t1, t2 = extract_type_tens(expression, GammaMatrix)
if t1 != 1:
t1 = kahane_simplify(t1)
res = t1*t2
return res
def _trace_single_line(t):
"""
Evaluate the trace of a single gamma matrix line inside a ``TensExpr``.
Notes
=====
If there are ``DiracSpinorIndex.auto_left`` and ``DiracSpinorIndex.auto_right``
indices trace over them; otherwise traces are not implied (explain)
Examples
========
>>> from sympy.physics.hep.gamma_matrices import GammaMatrix as G, \
LorentzIndex, _trace_single_line
>>> from sympy.tensor.tensor import tensor_indices, TensorHead
>>> p = TensorHead('p', [LorentzIndex])
>>> i0,i1,i2,i3,i4,i5 = tensor_indices('i0:6', LorentzIndex)
>>> _trace_single_line(G(i0)*G(i1))
4*metric(i0, i1)
>>> _trace_single_line(G(i0)*p(-i0)*G(i1)*p(-i1)) - 4*p(i0)*p(-i0)
0
"""
def _trace_single_line1(t):
t = t.sorted_components()
components = t.components
ncomps = len(components)
g = LorentzIndex.metric
# gamma matirices are in a[i:j]
hit = 0
for i in range(ncomps):
if components[i] == GammaMatrix:
hit = 1
break
for j in range(i + hit, ncomps):
if components[j] != GammaMatrix:
break
else:
j = ncomps
numG = j - i
if numG == 0:
tcoeff = t.coeff
return t.nocoeff if tcoeff else t
if numG % 2 == 1:
return TensMul.from_data(S.Zero, [], [], [])
elif numG > 4:
# find the open matrix indices and connect them:
a = t.split()
ind1 = a[i].get_indices()[0]
ind2 = a[i + 1].get_indices()[0]
aa = a[:i] + a[i + 2:]
t1 = tensor_mul(*aa)*g(ind1, ind2)
t1 = t1.contract_metric(g)
args = [t1]
sign = 1
for k in range(i + 2, j):
sign = -sign
ind2 = a[k].get_indices()[0]
aa = a[:i] + a[i + 1:k] + a[k + 1:]
t2 = sign*tensor_mul(*aa)*g(ind1, ind2)
t2 = t2.contract_metric(g)
t2 = simplify_gpgp(t2, False)
args.append(t2)
t3 = TensAdd(*args)
t3 = _trace_single_line(t3)
return t3
else:
a = t.split()
t1 = _gamma_trace1(*a[i:j])
a2 = a[:i] + a[j:]
t2 = tensor_mul(*a2)
t3 = t1*t2
if not t3:
return t3
t3 = t3.contract_metric(g)
return t3
t = t.expand()
if isinstance(t, TensAdd):
a = [_trace_single_line1(x)*x.coeff for x in t.args]
return TensAdd(*a)
elif isinstance(t, (Tensor, TensMul)):
r = t.coeff*_trace_single_line1(t)
return r
else:
return trace(t)
def _gamma_trace1(*a):
gctr = 4 # FIXME specific for d=4
g = LorentzIndex.metric
if not a:
return gctr
n = len(a)
if n%2 == 1:
#return TensMul.from_data(S.Zero, [], [], [])
return S.Zero
if n == 2:
ind0 = a[0].get_indices()[0]
ind1 = a[1].get_indices()[0]
return gctr*g(ind0, ind1)
if n == 4:
ind0 = a[0].get_indices()[0]
ind1 = a[1].get_indices()[0]
ind2 = a[2].get_indices()[0]
ind3 = a[3].get_indices()[0]
return gctr*(g(ind0, ind1)*g(ind2, ind3) - \
g(ind0, ind2)*g(ind1, ind3) + g(ind0, ind3)*g(ind1, ind2))
def kahane_simplify(expression):
r"""
This function cancels contracted elements in a product of four
dimensional gamma matrices, resulting in an expression equal to the given
one, without the contracted gamma matrices.
Parameters
==========
`expression` the tensor expression containing the gamma matrices to simplify.
Notes
=====
If spinor indices are given, the matrices must be given in
the order given in the product.
Algorithm
=========
The idea behind the algorithm is to use some well-known identities,
i.e., for contractions enclosing an even number of `\gamma` matrices
`\gamma^\mu \gamma_{a_1} \cdots \gamma_{a_{2N}} \gamma_\mu = 2 (\gamma_{a_{2N}} \gamma_{a_1} \cdots \gamma_{a_{2N-1}} + \gamma_{a_{2N-1}} \cdots \gamma_{a_1} \gamma_{a_{2N}} )`
for an odd number of `\gamma` matrices
`\gamma^\mu \gamma_{a_1} \cdots \gamma_{a_{2N+1}} \gamma_\mu = -2 \gamma_{a_{2N+1}} \gamma_{a_{2N}} \cdots \gamma_{a_{1}}`
Instead of repeatedly applying these identities to cancel out all contracted indices,
it is possible to recognize the links that would result from such an operation,
the problem is thus reduced to a simple rearrangement of free gamma matrices.
Examples
========
When using, always remember that the original expression coefficient
has to be handled separately
>>> from sympy.physics.hep.gamma_matrices import GammaMatrix as G, LorentzIndex
>>> from sympy.physics.hep.gamma_matrices import kahane_simplify
>>> from sympy.tensor.tensor import tensor_indices
>>> i0, i1, i2 = tensor_indices('i0:3', LorentzIndex)
>>> ta = G(i0)*G(-i0)
>>> kahane_simplify(ta)
Matrix([
[4, 0, 0, 0],
[0, 4, 0, 0],
[0, 0, 4, 0],
[0, 0, 0, 4]])
>>> tb = G(i0)*G(i1)*G(-i0)
>>> kahane_simplify(tb)
-2*GammaMatrix(i1)
>>> t = G(i0)*G(-i0)
>>> kahane_simplify(t)
Matrix([
[4, 0, 0, 0],
[0, 4, 0, 0],
[0, 0, 4, 0],
[0, 0, 0, 4]])
>>> t = G(i0)*G(-i0)
>>> kahane_simplify(t)
Matrix([
[4, 0, 0, 0],
[0, 4, 0, 0],
[0, 0, 4, 0],
[0, 0, 0, 4]])
If there are no contractions, the same expression is returned
>>> tc = G(i0)*G(i1)
>>> kahane_simplify(tc)
GammaMatrix(i0)*GammaMatrix(i1)
References
==========
[1] Algorithm for Reducing Contracted Products of gamma Matrices,
Joseph Kahane, Journal of Mathematical Physics, Vol. 9, No. 10, October 1968.
"""
if isinstance(expression, Mul):
return expression
if isinstance(expression, TensAdd):
return TensAdd(*[kahane_simplify(arg) for arg in expression.args])
if isinstance(expression, Tensor):
return expression
assert isinstance(expression, TensMul)
gammas = expression.args
for gamma in gammas:
assert gamma.component == GammaMatrix
free = expression.free
# spinor_free = [_ for _ in expression.free_in_args if _[1] != 0]
# if len(spinor_free) == 2:
# spinor_free.sort(key=lambda x: x[2])
# assert spinor_free[0][1] == 1 and spinor_free[-1][1] == 2
# assert spinor_free[0][2] == 0
# elif spinor_free:
# raise ValueError('spinor indices do not match')
dum = []
for dum_pair in expression.dum:
if expression.index_types[dum_pair[0]] == LorentzIndex:
dum.append((dum_pair[0], dum_pair[1]))
dum = sorted(dum)
if len(dum) == 0: # or GammaMatrixHead:
# no contractions in `expression`, just return it.
return expression
# find the `first_dum_pos`, i.e. the position of the first contracted
# gamma matrix, Kahane's algorithm as described in his paper requires the
# gamma matrix expression to start with a contracted gamma matrix, this is
# a workaround which ignores possible initial free indices, and re-adds
# them later.
first_dum_pos = min(map(min, dum))
# for p1, p2, a1, a2 in expression.dum_in_args:
# if p1 != 0 or p2 != 0:
# # only Lorentz indices, skip Dirac indices:
# continue
# first_dum_pos = min(p1, p2)
# break
total_number = len(free) + len(dum)*2
number_of_contractions = len(dum)
free_pos = [None]*total_number
for i in free:
free_pos[i[1]] = i[0]
# `index_is_free` is a list of booleans, to identify index position
# and whether that index is free or dummy.
index_is_free = [False]*total_number
for i, indx in enumerate(free):
index_is_free[indx[1]] = True
# `links` is a dictionary containing the graph described in Kahane's paper,
# to every key correspond one or two values, representing the linked indices.
# All values in `links` are integers, negative numbers are used in the case
# where it is necessary to insert gamma matrices between free indices, in
# order to make Kahane's algorithm work (see paper).
links = dict()
for i in range(first_dum_pos, total_number):
links[i] = []
# `cum_sign` is a step variable to mark the sign of every index, see paper.
cum_sign = -1
# `cum_sign_list` keeps storage for all `cum_sign` (every index).
cum_sign_list = [None]*total_number
block_free_count = 0
# multiply `resulting_coeff` by the coefficient parameter, the rest
# of the algorithm ignores a scalar coefficient.
resulting_coeff = S.One
# initialize a list of lists of indices. The outer list will contain all
# additive tensor expressions, while the inner list will contain the
# free indices (rearranged according to the algorithm).
resulting_indices = [[]]
# start to count the `connected_components`, which together with the number
# of contractions, determines a -1 or +1 factor to be multiplied.
connected_components = 1
# First loop: here we fill `cum_sign_list`, and draw the links
# among consecutive indices (they are stored in `links`). Links among
# non-consecutive indices will be drawn later.
for i, is_free in enumerate(index_is_free):
# if `expression` starts with free indices, they are ignored here;
# they are later added as they are to the beginning of all
# `resulting_indices` list of lists of indices.
if i < first_dum_pos:
continue
if is_free:
block_free_count += 1
# if previous index was free as well, draw an arch in `links`.
if block_free_count > 1:
links[i - 1].append(i)
links[i].append(i - 1)
else:
# Change the sign of the index (`cum_sign`) if the number of free
# indices preceding it is even.
cum_sign *= 1 if (block_free_count % 2) else -1
if block_free_count == 0 and i != first_dum_pos:
# check if there are two consecutive dummy indices:
# in this case create virtual indices with negative position,
# these "virtual" indices represent the insertion of two
# gamma^0 matrices to separate consecutive dummy indices, as
# Kahane's algorithm requires dummy indices to be separated by
# free indices. The product of two gamma^0 matrices is unity,
# so the new expression being examined is the same as the
# original one.
if cum_sign == -1:
links[-1-i] = [-1-i+1]
links[-1-i+1] = [-1-i]
if (i - cum_sign) in links:
if i != first_dum_pos:
links[i].append(i - cum_sign)
if block_free_count != 0:
if i - cum_sign < len(index_is_free):
if index_is_free[i - cum_sign]:
links[i - cum_sign].append(i)
block_free_count = 0
cum_sign_list[i] = cum_sign
# The previous loop has only created links between consecutive free indices,
# it is necessary to properly create links among dummy (contracted) indices,
# according to the rules described in Kahane's paper. There is only one exception
# to Kahane's rules: the negative indices, which handle the case of some
# consecutive free indices (Kahane's paper just describes dummy indices
# separated by free indices, hinting that free indices can be added without
# altering the expression result).
for i in dum:
# get the positions of the two contracted indices:
pos1 = i[0]
pos2 = i[1]
# create Kahane's upper links, i.e. the upper arcs between dummy
# (i.e. contracted) indices:
links[pos1].append(pos2)
links[pos2].append(pos1)
# create Kahane's lower links, this corresponds to the arcs below
# the line described in the paper:
# first we move `pos1` and `pos2` according to the sign of the indices:
linkpos1 = pos1 + cum_sign_list[pos1]
linkpos2 = pos2 + cum_sign_list[pos2]
# otherwise, perform some checks before creating the lower arcs:
# make sure we are not exceeding the total number of indices:
if linkpos1 >= total_number:
continue
if linkpos2 >= total_number:
continue
# make sure we are not below the first dummy index in `expression`:
if linkpos1 < first_dum_pos:
continue
if linkpos2 < first_dum_pos:
continue
# check if the previous loop created "virtual" indices between dummy
# indices, in such a case relink `linkpos1` and `linkpos2`:
if (-1-linkpos1) in links:
linkpos1 = -1-linkpos1
if (-1-linkpos2) in links:
linkpos2 = -1-linkpos2
# move only if not next to free index:
if linkpos1 >= 0 and not index_is_free[linkpos1]:
linkpos1 = pos1
if linkpos2 >=0 and not index_is_free[linkpos2]:
linkpos2 = pos2
# create the lower arcs:
if linkpos2 not in links[linkpos1]:
links[linkpos1].append(linkpos2)
if linkpos1 not in links[linkpos2]:
links[linkpos2].append(linkpos1)
# This loop starts from the `first_dum_pos` index (first dummy index)
# walks through the graph deleting the visited indices from `links`,
# it adds a gamma matrix for every free index in encounters, while it
# completely ignores dummy indices and virtual indices.
pointer = first_dum_pos
previous_pointer = 0
while True:
if pointer in links:
next_ones = links.pop(pointer)
else:
break
if previous_pointer in next_ones:
next_ones.remove(previous_pointer)
previous_pointer = pointer
if next_ones:
pointer = next_ones[0]
else:
break
if pointer == previous_pointer:
break
if pointer >=0 and free_pos[pointer] is not None:
for ri in resulting_indices:
ri.append(free_pos[pointer])
# The following loop removes the remaining connected components in `links`.
# If there are free indices inside a connected component, it gives a
# contribution to the resulting expression given by the factor
# `gamma_a gamma_b ... gamma_z + gamma_z ... gamma_b gamma_a`, in Kahanes's
# paper represented as {gamma_a, gamma_b, ... , gamma_z},
# virtual indices are ignored. The variable `connected_components` is
# increased by one for every connected component this loop encounters.
# If the connected component has virtual and dummy indices only
# (no free indices), it contributes to `resulting_indices` by a factor of two.
# The multiplication by two is a result of the
# factor {gamma^0, gamma^0} = 2 I, as it appears in Kahane's paper.
# Note: curly brackets are meant as in the paper, as a generalized
# multi-element anticommutator!
while links:
connected_components += 1
pointer = min(links.keys())
previous_pointer = pointer
# the inner loop erases the visited indices from `links`, and it adds
# all free indices to `prepend_indices` list, virtual indices are
# ignored.
prepend_indices = []
while True:
if pointer in links:
next_ones = links.pop(pointer)
else:
break
if previous_pointer in next_ones:
if len(next_ones) > 1:
next_ones.remove(previous_pointer)
previous_pointer = pointer
if next_ones:
pointer = next_ones[0]
if pointer >= first_dum_pos and free_pos[pointer] is not None:
prepend_indices.insert(0, free_pos[pointer])
# if `prepend_indices` is void, it means there are no free indices
# in the loop (and it can be shown that there must be a virtual index),
# loops of virtual indices only contribute by a factor of two:
if len(prepend_indices) == 0:
resulting_coeff *= 2
# otherwise, add the free indices in `prepend_indices` to
# the `resulting_indices`:
else:
expr1 = prepend_indices
expr2 = list(reversed(prepend_indices))
resulting_indices = [expri + ri for ri in resulting_indices for expri in (expr1, expr2)]
# sign correction, as described in Kahane's paper:
resulting_coeff *= -1 if (number_of_contractions - connected_components + 1) % 2 else 1
# power of two factor, as described in Kahane's paper:
resulting_coeff *= 2**(number_of_contractions)
# If `first_dum_pos` is not zero, it means that there are trailing free gamma
# matrices in front of `expression`, so multiply by them:
for i in range(0, first_dum_pos):
[ri.insert(0, free_pos[i]) for ri in resulting_indices]
resulting_expr = S.Zero
for i in resulting_indices:
temp_expr = S.One
for j in i:
temp_expr *= GammaMatrix(j)
resulting_expr += temp_expr
t = resulting_coeff * resulting_expr
t1 = None
if isinstance(t, TensAdd):
t1 = t.args[0]
elif isinstance(t, TensMul):
t1 = t
if t1:
pass
else:
t = eye(4)*t
return t
|
c38e2fd1e0486e28dacc88ca51cedac6f04f36624f743544396f6811ee94eff7 | from sympy import S, sqrt, pi, Dummy, Sum, Ynm, symbols
from sympy.physics.wigner import (clebsch_gordan, wigner_9j, wigner_6j, gaunt,
racah, dot_rot_grad_Ynm, Wigner3j, wigner_3j)
from sympy.core.numbers import Rational
# for test cases, refer : https://en.wikipedia.org/wiki/Table_of_Clebsch%E2%80%93Gordan_coefficients
def test_clebsch_gordan_docs():
assert clebsch_gordan(S(3)/2, S(1)/2, 2, S(3)/2, S(1)/2, 2) == 1
assert clebsch_gordan(S(3)/2, S(1)/2, 1, S(3)/2, -S(1)/2, 1) == sqrt(3)/2
assert clebsch_gordan(S(3)/2, S(1)/2, 1, -S(1)/2, S(1)/2, 0) == -sqrt(2)/2
def test_clebsch_gordan1():
j_1 = S(1)/2
j_2 = S(1)/2
m = 1
j = 1
m_1 = S(1)/2
m_2 = S(1)/2
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == 1
j_1 = S(1)/2
j_2 = S(1)/2
m = -1
j = 1
m_1 = -S(1)/2
m_2 = -S(1)/2
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == 1
j_1 = S(1)/2
j_2 = S(1)/2
m = 0
j = 1
m_1 = S(1)/2
m_2 = S(1)/2
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == 0
j_1 = S(1)/2
j_2 = S(1)/2
m = 0
j = 1
m_1 = S(1)/2
m_2 = -S(1)/2
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == sqrt(2)/2
j_1 = S(1)/2
j_2 = S(1)/2
m = 0
j = 0
m_1 = S(1)/2
m_2 = -S(1)/2
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == sqrt(2)/2
j_1 = S(1)/2
j_2 = S(1)/2
m = 0
j = 1
m_1 = -S(1)/2
m_2 = S(1)/2
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == sqrt(2)/2
j_1 = S(1)/2
j_2 = S(1)/2
m = 0
j = 0
m_1 = -S(1)/2
m_2 = S(1)/2
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == -sqrt(2)/2
def test_clebsch_gordan2():
j_1 = S(1)
j_2 = S(1)/2
m = S(3)/2
j = S(3)/2
m_1 = 1
m_2 = S(1)/2
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == 1
j_1 = S(1)
j_2 = S(1)/2
m = S(1)/2
j = S(3)/2
m_1 = 1
m_2 = -S(1)/2
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == 1/sqrt(3)
j_1 = S(1)
j_2 = S(1)/2
m = S(1)/2
j = S(1)/2
m_1 = 1
m_2 = -S(1)/2
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == sqrt(2)/sqrt(3)
j_1 = S(1)
j_2 = S(1)/2
m = S(1)/2
j = S(1)/2
m_1 = 0
m_2 = S(1)/2
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == -1/sqrt(3)
j_1 = S(1)
j_2 = S(1)/2
m = S(1)/2
j = S(3)/2
m_1 = 0
m_2 = S(1)/2
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == sqrt(2)/sqrt(3)
j_1 = S(1)
j_2 = S(1)
m = S(2)
j = S(2)
m_1 = 1
m_2 = 1
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == 1
j_1 = S(1)
j_2 = S(1)
m = 1
j = S(2)
m_1 = 1
m_2 = 0
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == 1/sqrt(2)
j_1 = S(1)
j_2 = S(1)
m = 1
j = S(2)
m_1 = 0
m_2 = 1
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == 1/sqrt(2)
j_1 = S(1)
j_2 = S(1)
m = 1
j = 1
m_1 = 1
m_2 = 0
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == 1/sqrt(2)
j_1 = S(1)
j_2 = S(1)
m = 1
j = 1
m_1 = 0
m_2 = 1
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == -1/sqrt(2)
def test_clebsch_gordan3():
j_1 = S(3)/2
j_2 = S(3)/2
m = S(3)
j = S(3)
m_1 = S(3)/2
m_2 = S(3)/2
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == 1
j_1 = S(3)/2
j_2 = S(3)/2
m = S(2)
j = S(2)
m_1 = S(3)/2
m_2 = S(1)/2
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == 1/sqrt(2)
j_1 = S(3)/2
j_2 = S(3)/2
m = S(2)
j = S(3)
m_1 = S(3)/2
m_2 = S(1)/2
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == 1/sqrt(2)
def test_clebsch_gordan4():
j_1 = S(2)
j_2 = S(2)
m = S(4)
j = S(4)
m_1 = S(2)
m_2 = S(2)
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == 1
j_1 = S(2)
j_2 = S(2)
m = S(3)
j = S(3)
m_1 = S(2)
m_2 = 1
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == 1/sqrt(2)
j_1 = S(2)
j_2 = S(2)
m = S(2)
j = S(3)
m_1 = 1
m_2 = 1
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == 0
def test_clebsch_gordan5():
j_1 = S(5)/2
j_2 = S(1)
m = S(7)/2
j = S(7)/2
m_1 = S(5)/2
m_2 = 1
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == 1
j_1 = S(5)/2
j_2 = S(1)
m = S(5)/2
j = S(5)/2
m_1 = S(5)/2
m_2 = 0
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == sqrt(5)/sqrt(7)
j_1 = S(5)/2
j_2 = S(1)
m = S(3)/2
j = S(3)/2
m_1 = S(1)/2
m_2 = 1
assert clebsch_gordan(j_1, j_2, j, m_1, m_2, m) == 1/sqrt(15)
def test_wigner():
def tn(a, b):
return (a - b).n(64) < S('1e-64')
assert tn(wigner_9j(1, 1, 1, 1, 1, 1, 1, 1, 0, prec=64), S(1)/18)
assert wigner_9j(3, 3, 2, 3, 3, 2, 3, 3, 2) == 3221*sqrt(
70)/(246960*sqrt(105)) - 365/(3528*sqrt(70)*sqrt(105))
assert wigner_6j(5, 5, 5, 5, 5, 5) == Rational(1, 52)
assert tn(wigner_6j(8, 8, 8, 8, 8, 8, prec=64), -S(12219)/965770)
# regression test for #8747
half = Rational(1, 2)
assert wigner_9j(0, 0, 0, 0, half, half, 0, half, half) == half
assert (wigner_9j(3, 5, 4,
7 * half, 5 * half, 4,
9 * half, 9 * half, 0)
== -sqrt(Rational(361, 205821000)))
assert (wigner_9j(1, 4, 3,
5 * half, 4, 5 * half,
5 * half, 2, 7 * half)
== -sqrt(Rational(3971, 373403520)))
assert (wigner_9j(4, 9 * half, 5 * half,
2, 4, 4,
5, 7 * half, 7 * half)
== -sqrt(Rational(3481, 5042614500)))
def test_gaunt():
def tn(a, b):
return (a - b).n(64) < S('1e-64')
assert gaunt(1, 0, 1, 1, 0, -1) == -1/(2*sqrt(pi))
assert isinstance(gaunt(1, 1, 0, -1, 1, 0).args[0], Rational)
assert isinstance(gaunt(0, 1, 1, 0, -1, 1).args[0], Rational)
assert tn(gaunt(
10, 10, 12, 9, 3, -12, prec=64), (-S(98)/62031) * sqrt(6279)/sqrt(pi))
def gaunt_ref(l1, l2, l3, m1, m2, m3):
return (
sqrt((2 * l1 + 1) * (2 * l2 + 1) * (2 * l3 + 1) / (4 * pi)) *
wigner_3j(l1, l2, l3, 0, 0, 0) *
wigner_3j(l1, l2, l3, m1, m2, m3)
)
threshold = 1e-10
l_max = 3
l3_max = 24
for l1 in range(l_max + 1):
for l2 in range(l_max + 1):
for l3 in range(l3_max + 1):
for m1 in range(-l1, l1 + 1):
for m2 in range(-l2, l2 + 1):
for m3 in range(-l3, l3 + 1):
args = l1, l2, l3, m1, m2, m3
g = gaunt(*args)
g0 = gaunt_ref(*args)
assert abs(g - g0) < threshold
if m1 + m2 + m3 != 0:
assert abs(g) < threshold
if (l1 + l2 + l3) % 2:
assert abs(g) < threshold
def test_racah():
assert racah(3,3,3,3,3,3) == Rational(-1,14)
assert racah(2,2,2,2,2,2) == Rational(-3,70)
assert racah(7,8,7,1,7,7, prec=4).is_Float
assert racah(5.5,7.5,9.5,6.5,8,9) == -719*sqrt(598)/1158924
assert abs(racah(5.5,7.5,9.5,6.5,8,9, prec=4) - (-0.01517)) < S('1e-4')
def test_dot_rota_grad_SH():
theta, phi = symbols("theta phi")
assert dot_rot_grad_Ynm(1, 1, 1, 1, 1, 0) != \
sqrt(30)*Ynm(2, 2, 1, 0)/(10*sqrt(pi))
assert dot_rot_grad_Ynm(1, 1, 1, 1, 1, 0).doit() == \
sqrt(30)*Ynm(2, 2, 1, 0)/(10*sqrt(pi))
assert dot_rot_grad_Ynm(1, 5, 1, 1, 1, 2) != \
0
assert dot_rot_grad_Ynm(1, 5, 1, 1, 1, 2).doit() == \
0
assert dot_rot_grad_Ynm(3, 3, 3, 3, theta, phi).doit() == \
15*sqrt(3003)*Ynm(6, 6, theta, phi)/(143*sqrt(pi))
assert dot_rot_grad_Ynm(3, 3, 1, 1, theta, phi).doit() == \
sqrt(3)*Ynm(4, 4, theta, phi)/sqrt(pi)
assert dot_rot_grad_Ynm(3, 2, 2, 0, theta, phi).doit() == \
3*sqrt(55)*Ynm(5, 2, theta, phi)/(11*sqrt(pi))
assert dot_rot_grad_Ynm(3, 2, 3, 2, theta, phi).doit().expand() == \
-sqrt(70)*Ynm(4, 4, theta, phi)/(11*sqrt(pi)) + \
45*sqrt(182)*Ynm(6, 4, theta, phi)/(143*sqrt(pi))
|
7ac290fa96672b96da32eb1c36db4af717cb252832653a1e81a2a5763e8318ab | from sympy.physics.secondquant import (
Dagger, Bd, VarBosonicBasis, BBra, B, BKet, FixedBosonicBasis,
matrix_rep, apply_operators, InnerProduct, Commutator, KroneckerDelta,
AnnihilateBoson, CreateBoson, BosonicOperator,
F, Fd, FKet, BosonState, CreateFermion, AnnihilateFermion,
evaluate_deltas, AntiSymmetricTensor, contraction, NO, wicks,
PermutationOperator, simplify_index_permutations,
_sort_anticommuting_fermions, _get_ordered_dummies,
substitute_dummies, FockState, FockStateBosonKet,
ContractionAppliesOnlyToFermions
)
from sympy import (Dummy, expand, Function, I, Rational, simplify, sqrt, Sum,
Symbol, symbols, srepr)
from sympy.core.compatibility import range
from sympy.utilities.pytest import XFAIL, slow, raises
from sympy.printing.latex import latex
def test_PermutationOperator():
p, q, r, s = symbols('p,q,r,s')
f, g, h, i = map(Function, 'fghi')
P = PermutationOperator
assert P(p, q).get_permuted(f(p)*g(q)) == -f(q)*g(p)
assert P(p, q).get_permuted(f(p, q)) == -f(q, p)
assert P(p, q).get_permuted(f(p)) == f(p)
expr = (f(p)*g(q)*h(r)*i(s)
- f(q)*g(p)*h(r)*i(s)
- f(p)*g(q)*h(s)*i(r)
+ f(q)*g(p)*h(s)*i(r))
perms = [P(p, q), P(r, s)]
assert (simplify_index_permutations(expr, perms) ==
P(p, q)*P(r, s)*f(p)*g(q)*h(r)*i(s))
assert latex(P(p, q)) == 'P(pq)'
def test_index_permutations_with_dummies():
a, b, c, d = symbols('a b c d')
p, q, r, s = symbols('p q r s', cls=Dummy)
f, g = map(Function, 'fg')
P = PermutationOperator
# No dummy substitution necessary
expr = f(a, b, p, q) - f(b, a, p, q)
assert simplify_index_permutations(
expr, [P(a, b)]) == P(a, b)*f(a, b, p, q)
# Cases where dummy substitution is needed
expected = P(a, b)*substitute_dummies(f(a, b, p, q))
expr = f(a, b, p, q) - f(b, a, q, p)
result = simplify_index_permutations(expr, [P(a, b)])
assert expected == substitute_dummies(result)
expr = f(a, b, q, p) - f(b, a, p, q)
result = simplify_index_permutations(expr, [P(a, b)])
assert expected == substitute_dummies(result)
# A case where nothing can be done
expr = f(a, b, q, p) - g(b, a, p, q)
result = simplify_index_permutations(expr, [P(a, b)])
assert expr == result
def test_dagger():
i, j, n, m = symbols('i,j,n,m')
assert Dagger(1) == 1
assert Dagger(1.0) == 1.0
assert Dagger(2*I) == -2*I
assert Dagger(Rational(1, 2)*I/3.0) == -Rational(1, 2)*I/3.0
assert Dagger(BKet([n])) == BBra([n])
assert Dagger(B(0)) == Bd(0)
assert Dagger(Bd(0)) == B(0)
assert Dagger(B(n)) == Bd(n)
assert Dagger(Bd(n)) == B(n)
assert Dagger(B(0) + B(1)) == Bd(0) + Bd(1)
assert Dagger(n*m) == Dagger(n)*Dagger(m) # n, m commute
assert Dagger(B(n)*B(m)) == Bd(m)*Bd(n)
assert Dagger(B(n)**10) == Dagger(B(n))**10
assert Dagger('a') == Dagger(Symbol('a'))
assert Dagger(Dagger('a')) == Symbol('a')
def test_operator():
i, j = symbols('i,j')
o = BosonicOperator(i)
assert o.state == i
assert o.is_symbolic
o = BosonicOperator(1)
assert o.state == 1
assert not o.is_symbolic
def test_create():
i, j, n, m = symbols('i,j,n,m')
o = Bd(i)
assert latex(o) == "b^\\dagger_{i}"
assert isinstance(o, CreateBoson)
o = o.subs(i, j)
assert o.atoms(Symbol) == {j}
o = Bd(0)
assert o.apply_operator(BKet([n])) == sqrt(n + 1)*BKet([n + 1])
o = Bd(n)
assert o.apply_operator(BKet([n])) == o*BKet([n])
def test_annihilate():
i, j, n, m = symbols('i,j,n,m')
o = B(i)
assert latex(o) == "b_{i}"
assert isinstance(o, AnnihilateBoson)
o = o.subs(i, j)
assert o.atoms(Symbol) == {j}
o = B(0)
assert o.apply_operator(BKet([n])) == sqrt(n)*BKet([n - 1])
o = B(n)
assert o.apply_operator(BKet([n])) == o*BKet([n])
def test_basic_state():
i, j, n, m = symbols('i,j,n,m')
s = BosonState([0, 1, 2, 3, 4])
assert len(s) == 5
assert s.args[0] == tuple(range(5))
assert s.up(0) == BosonState([1, 1, 2, 3, 4])
assert s.down(4) == BosonState([0, 1, 2, 3, 3])
for i in range(5):
assert s.up(i).down(i) == s
assert s.down(0) == 0
for i in range(5):
assert s[i] == i
s = BosonState([n, m])
assert s.down(0) == BosonState([n - 1, m])
assert s.up(0) == BosonState([n + 1, m])
# 2019-07-24: No method move in the whole of SymPy
@XFAIL
def test_move1():
i, j = symbols('i,j')
A, C = symbols('A,C', cls=Function)
o = A(i)*C(j)
# This almost works, but has a minus sign wrong
assert move(o, 0, 1) == KroneckerDelta(i, j) + C(j)*A(i)
# 2019-07-24: No method move in the whole of SymPy
@XFAIL
def test_move2():
i, j = symbols('i,j')
A, C = symbols('A,C', cls=Function)
o = C(j)*A(i)
# This almost works, but has a minus sign wrong
assert move(o, 0, 1) == -KroneckerDelta(i, j) + A(i)*C(j)
def test_basic_apply():
n = symbols("n")
e = B(0)*BKet([n])
assert apply_operators(e) == sqrt(n)*BKet([n - 1])
e = Bd(0)*BKet([n])
assert apply_operators(e) == sqrt(n + 1)*BKet([n + 1])
def test_complex_apply():
n, m = symbols("n,m")
o = Bd(0)*B(0)*Bd(1)*B(0)
e = apply_operators(o*BKet([n, m]))
answer = sqrt(n)*sqrt(m + 1)*(-1 + n)*BKet([-1 + n, 1 + m])
assert expand(e) == expand(answer)
def test_number_operator():
n = symbols("n")
o = Bd(0)*B(0)
e = apply_operators(o*BKet([n]))
assert e == n*BKet([n])
def test_inner_product():
i, j, k, l = symbols('i,j,k,l')
s1 = BBra([0])
s2 = BKet([1])
assert InnerProduct(s1, Dagger(s1)) == 1
assert InnerProduct(s1, s2) == 0
s1 = BBra([i, j])
s2 = BKet([k, l])
r = InnerProduct(s1, s2)
assert r == KroneckerDelta(i, k)*KroneckerDelta(j, l)
def test_symbolic_matrix_elements():
n, m = symbols('n,m')
s1 = BBra([n])
s2 = BKet([m])
o = B(0)
e = apply_operators(s1*o*s2)
assert e == sqrt(m)*KroneckerDelta(n, m - 1)
def test_matrix_elements():
b = VarBosonicBasis(5)
o = B(0)
m = matrix_rep(o, b)
for i in range(4):
assert m[i, i + 1] == sqrt(i + 1)
o = Bd(0)
m = matrix_rep(o, b)
for i in range(4):
assert m[i + 1, i] == sqrt(i + 1)
def test_fixed_bosonic_basis():
b = FixedBosonicBasis(2, 2)
# assert b == [FockState((2, 0)), FockState((1, 1)), FockState((0, 2))]
state = b.state(1)
assert state == FockStateBosonKet((1, 1))
assert b.index(state) == 1
assert b.state(1) == b[1]
assert len(b) == 3
assert str(b) == '[FockState((2, 0)), FockState((1, 1)), FockState((0, 2))]'
assert repr(b) == '[FockState((2, 0)), FockState((1, 1)), FockState((0, 2))]'
assert srepr(b) == '[FockState((2, 0)), FockState((1, 1)), FockState((0, 2))]'
@slow
def test_sho():
n, m = symbols('n,m')
h_n = Bd(n)*B(n)*(n + Rational(1, 2))
H = Sum(h_n, (n, 0, 5))
o = H.doit(deep=False)
b = FixedBosonicBasis(2, 6)
m = matrix_rep(o, b)
# We need to double check these energy values to make sure that they
# are correct and have the proper degeneracies!
diag = [1, 2, 3, 3, 4, 5, 4, 5, 6, 7, 5, 6, 7, 8, 9, 6, 7, 8, 9, 10, 11]
for i in range(len(diag)):
assert diag[i] == m[i, i]
def test_commutation():
n, m = symbols("n,m", above_fermi=True)
c = Commutator(B(0), Bd(0))
assert c == 1
c = Commutator(Bd(0), B(0))
assert c == -1
c = Commutator(B(n), Bd(0))
assert c == KroneckerDelta(n, 0)
c = Commutator(B(0), B(0))
assert c == 0
c = Commutator(B(0), Bd(0))
e = simplify(apply_operators(c*BKet([n])))
assert e == BKet([n])
c = Commutator(B(0), B(1))
e = simplify(apply_operators(c*BKet([n, m])))
assert e == 0
c = Commutator(F(m), Fd(m))
assert c == +1 - 2*NO(Fd(m)*F(m))
c = Commutator(Fd(m), F(m))
assert c.expand() == -1 + 2*NO(Fd(m)*F(m))
C = Commutator
X, Y, Z = symbols('X,Y,Z', commutative=False)
assert C(C(X, Y), Z) != 0
assert C(C(X, Z), Y) != 0
assert C(Y, C(X, Z)) != 0
i, j, k, l = symbols('i,j,k,l', below_fermi=True)
a, b, c, d = symbols('a,b,c,d', above_fermi=True)
p, q, r, s = symbols('p,q,r,s')
D = KroneckerDelta
assert C(Fd(a), F(i)) == -2*NO(F(i)*Fd(a))
assert C(Fd(j), NO(Fd(a)*F(i))).doit(wicks=True) == -D(j, i)*Fd(a)
assert C(Fd(a)*F(i), Fd(b)*F(j)).doit(wicks=True) == 0
c1 = Commutator(F(a), Fd(a))
assert Commutator.eval(c1, c1) == 0
c = Commutator(Fd(a)*F(i),Fd(b)*F(j))
assert latex(c) == r'\left[a^\dagger_{a} a_{i},a^\dagger_{b} a_{j}\right]'
assert repr(c) == 'Commutator(CreateFermion(a)*AnnihilateFermion(i),CreateFermion(b)*AnnihilateFermion(j))'
assert str(c) == '[CreateFermion(a)*AnnihilateFermion(i),CreateFermion(b)*AnnihilateFermion(j)]'
def test_create_f():
i, j, n, m = symbols('i,j,n,m')
o = Fd(i)
assert isinstance(o, CreateFermion)
o = o.subs(i, j)
assert o.atoms(Symbol) == {j}
o = Fd(1)
assert o.apply_operator(FKet([n])) == FKet([1, n])
assert o.apply_operator(FKet([n])) == -FKet([n, 1])
o = Fd(n)
assert o.apply_operator(FKet([])) == FKet([n])
vacuum = FKet([], fermi_level=4)
assert vacuum == FKet([], fermi_level=4)
i, j, k, l = symbols('i,j,k,l', below_fermi=True)
a, b, c, d = symbols('a,b,c,d', above_fermi=True)
p, q, r, s = symbols('p,q,r,s')
assert Fd(i).apply_operator(FKet([i, j, k], 4)) == FKet([j, k], 4)
assert Fd(a).apply_operator(FKet([i, b, k], 4)) == FKet([a, i, b, k], 4)
assert Dagger(B(p)).apply_operator(q) == q*CreateBoson(p)
assert repr(Fd(p)) == 'CreateFermion(p)'
assert srepr(Fd(p)) == "CreateFermion(Symbol('p'))"
assert latex(Fd(p)) == r'a^\dagger_{p}'
def test_annihilate_f():
i, j, n, m = symbols('i,j,n,m')
o = F(i)
assert isinstance(o, AnnihilateFermion)
o = o.subs(i, j)
assert o.atoms(Symbol) == {j}
o = F(1)
assert o.apply_operator(FKet([1, n])) == FKet([n])
assert o.apply_operator(FKet([n, 1])) == -FKet([n])
o = F(n)
assert o.apply_operator(FKet([n])) == FKet([])
i, j, k, l = symbols('i,j,k,l', below_fermi=True)
a, b, c, d = symbols('a,b,c,d', above_fermi=True)
p, q, r, s = symbols('p,q,r,s')
assert F(i).apply_operator(FKet([i, j, k], 4)) == 0
assert F(a).apply_operator(FKet([i, b, k], 4)) == 0
assert F(l).apply_operator(FKet([i, j, k], 3)) == 0
assert F(l).apply_operator(FKet([i, j, k], 4)) == FKet([l, i, j, k], 4)
assert str(F(p)) == 'f(p)'
assert repr(F(p)) == 'AnnihilateFermion(p)'
assert srepr(F(p)) == "AnnihilateFermion(Symbol('p'))"
assert latex(F(p)) == 'a_{p}'
def test_create_b():
i, j, n, m = symbols('i,j,n,m')
o = Bd(i)
assert isinstance(o, CreateBoson)
o = o.subs(i, j)
assert o.atoms(Symbol) == {j}
o = Bd(0)
assert o.apply_operator(BKet([n])) == sqrt(n + 1)*BKet([n + 1])
o = Bd(n)
assert o.apply_operator(BKet([n])) == o*BKet([n])
def test_annihilate_b():
i, j, n, m = symbols('i,j,n,m')
o = B(i)
assert isinstance(o, AnnihilateBoson)
o = o.subs(i, j)
assert o.atoms(Symbol) == {j}
o = B(0)
def test_wicks():
p, q, r, s = symbols('p,q,r,s', above_fermi=True)
# Testing for particles only
str = F(p)*Fd(q)
assert wicks(str) == NO(F(p)*Fd(q)) + KroneckerDelta(p, q)
str = Fd(p)*F(q)
assert wicks(str) == NO(Fd(p)*F(q))
str = F(p)*Fd(q)*F(r)*Fd(s)
nstr = wicks(str)
fasit = NO(
KroneckerDelta(p, q)*KroneckerDelta(r, s)
+ KroneckerDelta(p, q)*AnnihilateFermion(r)*CreateFermion(s)
+ KroneckerDelta(r, s)*AnnihilateFermion(p)*CreateFermion(q)
- KroneckerDelta(p, s)*AnnihilateFermion(r)*CreateFermion(q)
- AnnihilateFermion(p)*AnnihilateFermion(r)*CreateFermion(q)*CreateFermion(s))
assert nstr == fasit
assert (p*q*nstr).expand() == wicks(p*q*str)
assert (nstr*p*q*2).expand() == wicks(str*p*q*2)
# Testing CC equations particles and holes
i, j, k, l = symbols('i j k l', below_fermi=True, cls=Dummy)
a, b, c, d = symbols('a b c d', above_fermi=True, cls=Dummy)
p, q, r, s = symbols('p q r s', cls=Dummy)
assert (wicks(F(a)*NO(F(i)*F(j))*Fd(b)) ==
NO(F(a)*F(i)*F(j)*Fd(b)) +
KroneckerDelta(a, b)*NO(F(i)*F(j)))
assert (wicks(F(a)*NO(F(i)*F(j)*F(k))*Fd(b)) ==
NO(F(a)*F(i)*F(j)*F(k)*Fd(b)) -
KroneckerDelta(a, b)*NO(F(i)*F(j)*F(k)))
expr = wicks(Fd(i)*NO(Fd(j)*F(k))*F(l))
assert (expr ==
-KroneckerDelta(i, k)*NO(Fd(j)*F(l)) -
KroneckerDelta(j, l)*NO(Fd(i)*F(k)) -
KroneckerDelta(i, k)*KroneckerDelta(j, l) +
KroneckerDelta(i, l)*NO(Fd(j)*F(k)) +
NO(Fd(i)*Fd(j)*F(k)*F(l)))
expr = wicks(F(a)*NO(F(b)*Fd(c))*Fd(d))
assert (expr ==
-KroneckerDelta(a, c)*NO(F(b)*Fd(d)) -
KroneckerDelta(b, d)*NO(F(a)*Fd(c)) -
KroneckerDelta(a, c)*KroneckerDelta(b, d) +
KroneckerDelta(a, d)*NO(F(b)*Fd(c)) +
NO(F(a)*F(b)*Fd(c)*Fd(d)))
def test_NO():
i, j, k, l = symbols('i j k l', below_fermi=True)
a, b, c, d = symbols('a b c d', above_fermi=True)
p, q, r, s = symbols('p q r s', cls=Dummy)
assert (NO(Fd(p)*F(q) + Fd(a)*F(b)) ==
NO(Fd(p)*F(q)) + NO(Fd(a)*F(b)))
assert (NO(Fd(i)*NO(F(j)*Fd(a))) ==
NO(Fd(i)*F(j)*Fd(a)))
assert NO(1) == 1
assert NO(i) == i
assert (NO(Fd(a)*Fd(b)*(F(c) + F(d))) ==
NO(Fd(a)*Fd(b)*F(c)) +
NO(Fd(a)*Fd(b)*F(d)))
assert NO(Fd(a)*F(b))._remove_brackets() == Fd(a)*F(b)
assert NO(F(j)*Fd(i))._remove_brackets() == F(j)*Fd(i)
assert (NO(Fd(p)*F(q)).subs(Fd(p), Fd(a) + Fd(i)) ==
NO(Fd(a)*F(q)) + NO(Fd(i)*F(q)))
assert (NO(Fd(p)*F(q)).subs(F(q), F(a) + F(i)) ==
NO(Fd(p)*F(a)) + NO(Fd(p)*F(i)))
expr = NO(Fd(p)*F(q))._remove_brackets()
assert wicks(expr) == NO(expr)
assert NO(Fd(a)*F(b)) == - NO(F(b)*Fd(a))
no = NO(Fd(a)*F(i)*F(b)*Fd(j))
l1 = [ ind for ind in no.iter_q_creators() ]
assert l1 == [0, 1]
l2 = [ ind for ind in no.iter_q_annihilators() ]
assert l2 == [3, 2]
no = NO(Fd(a)*Fd(i))
assert no.has_q_creators == 1
assert no.has_q_annihilators == -1
assert str(no) == ':CreateFermion(a)*CreateFermion(i):'
assert repr(no) == 'NO(CreateFermion(a)*CreateFermion(i))'
assert latex(no) == r'\left\{a^\dagger_{a} a^\dagger_{i}\right\}'
raises(NotImplementedError, lambda: NO(Bd(p)*F(q)))
def test_sorting():
i, j = symbols('i,j', below_fermi=True)
a, b = symbols('a,b', above_fermi=True)
p, q = symbols('p,q')
# p, q
assert _sort_anticommuting_fermions([Fd(p), F(q)]) == ([Fd(p), F(q)], 0)
assert _sort_anticommuting_fermions([F(p), Fd(q)]) == ([Fd(q), F(p)], 1)
# i, p
assert _sort_anticommuting_fermions([F(p), Fd(i)]) == ([F(p), Fd(i)], 0)
assert _sort_anticommuting_fermions([Fd(i), F(p)]) == ([F(p), Fd(i)], 1)
assert _sort_anticommuting_fermions([Fd(p), Fd(i)]) == ([Fd(p), Fd(i)], 0)
assert _sort_anticommuting_fermions([Fd(i), Fd(p)]) == ([Fd(p), Fd(i)], 1)
assert _sort_anticommuting_fermions([F(p), F(i)]) == ([F(i), F(p)], 1)
assert _sort_anticommuting_fermions([F(i), F(p)]) == ([F(i), F(p)], 0)
assert _sort_anticommuting_fermions([Fd(p), F(i)]) == ([F(i), Fd(p)], 1)
assert _sort_anticommuting_fermions([F(i), Fd(p)]) == ([F(i), Fd(p)], 0)
# a, p
assert _sort_anticommuting_fermions([F(p), Fd(a)]) == ([Fd(a), F(p)], 1)
assert _sort_anticommuting_fermions([Fd(a), F(p)]) == ([Fd(a), F(p)], 0)
assert _sort_anticommuting_fermions([Fd(p), Fd(a)]) == ([Fd(a), Fd(p)], 1)
assert _sort_anticommuting_fermions([Fd(a), Fd(p)]) == ([Fd(a), Fd(p)], 0)
assert _sort_anticommuting_fermions([F(p), F(a)]) == ([F(p), F(a)], 0)
assert _sort_anticommuting_fermions([F(a), F(p)]) == ([F(p), F(a)], 1)
assert _sort_anticommuting_fermions([Fd(p), F(a)]) == ([Fd(p), F(a)], 0)
assert _sort_anticommuting_fermions([F(a), Fd(p)]) == ([Fd(p), F(a)], 1)
# i, a
assert _sort_anticommuting_fermions([F(i), Fd(j)]) == ([F(i), Fd(j)], 0)
assert _sort_anticommuting_fermions([Fd(j), F(i)]) == ([F(i), Fd(j)], 1)
assert _sort_anticommuting_fermions([Fd(a), Fd(i)]) == ([Fd(a), Fd(i)], 0)
assert _sort_anticommuting_fermions([Fd(i), Fd(a)]) == ([Fd(a), Fd(i)], 1)
assert _sort_anticommuting_fermions([F(a), F(i)]) == ([F(i), F(a)], 1)
assert _sort_anticommuting_fermions([F(i), F(a)]) == ([F(i), F(a)], 0)
def test_contraction():
i, j, k, l = symbols('i,j,k,l', below_fermi=True)
a, b, c, d = symbols('a,b,c,d', above_fermi=True)
p, q, r, s = symbols('p,q,r,s')
assert contraction(Fd(i), F(j)) == KroneckerDelta(i, j)
assert contraction(F(a), Fd(b)) == KroneckerDelta(a, b)
assert contraction(F(a), Fd(i)) == 0
assert contraction(Fd(a), F(i)) == 0
assert contraction(F(i), Fd(a)) == 0
assert contraction(Fd(i), F(a)) == 0
assert contraction(Fd(i), F(p)) == KroneckerDelta(i, p)
restr = evaluate_deltas(contraction(Fd(p), F(q)))
assert restr.is_only_below_fermi
restr = evaluate_deltas(contraction(F(p), Fd(q)))
assert restr.is_only_above_fermi
raises(ContractionAppliesOnlyToFermions, lambda: contraction(B(a), Fd(b)))
def test_evaluate_deltas():
i, j, k = symbols('i,j,k')
r = KroneckerDelta(i, j) * KroneckerDelta(j, k)
assert evaluate_deltas(r) == KroneckerDelta(i, k)
r = KroneckerDelta(i, 0) * KroneckerDelta(j, k)
assert evaluate_deltas(r) == KroneckerDelta(i, 0) * KroneckerDelta(j, k)
r = KroneckerDelta(1, j) * KroneckerDelta(j, k)
assert evaluate_deltas(r) == KroneckerDelta(1, k)
r = KroneckerDelta(j, 2) * KroneckerDelta(k, j)
assert evaluate_deltas(r) == KroneckerDelta(2, k)
r = KroneckerDelta(i, 0) * KroneckerDelta(i, j) * KroneckerDelta(j, 1)
assert evaluate_deltas(r) == 0
r = (KroneckerDelta(0, i) * KroneckerDelta(0, j)
* KroneckerDelta(1, j) * KroneckerDelta(1, j))
assert evaluate_deltas(r) == 0
def test_Tensors():
i, j, k, l = symbols('i j k l', below_fermi=True, cls=Dummy)
a, b, c, d = symbols('a b c d', above_fermi=True, cls=Dummy)
p, q, r, s = symbols('p q r s')
AT = AntiSymmetricTensor
assert AT('t', (a, b), (i, j)) == -AT('t', (b, a), (i, j))
assert AT('t', (a, b), (i, j)) == AT('t', (b, a), (j, i))
assert AT('t', (a, b), (i, j)) == -AT('t', (a, b), (j, i))
assert AT('t', (a, a), (i, j)) == 0
assert AT('t', (a, b), (i, i)) == 0
assert AT('t', (a, b, c), (i, j)) == -AT('t', (b, a, c), (i, j))
assert AT('t', (a, b, c), (i, j, k)) == AT('t', (b, a, c), (i, k, j))
tabij = AT('t', (a, b), (i, j))
assert tabij.has(a)
assert tabij.has(b)
assert tabij.has(i)
assert tabij.has(j)
assert tabij.subs(b, c) == AT('t', (a, c), (i, j))
assert (2*tabij).subs(i, c) == 2*AT('t', (a, b), (c, j))
assert tabij.symbol == Symbol('t')
assert latex(tabij) == 't^{ab}_{ij}'
assert str(tabij) == 't((_a, _b),(_i, _j))'
assert AT('t', (a, a), (i, j)).subs(a, b) == AT('t', (b, b), (i, j))
assert AT('t', (a, i), (a, j)).subs(a, b) == AT('t', (b, i), (b, j))
def test_fully_contracted():
i, j, k, l = symbols('i j k l', below_fermi=True)
a, b, c, d = symbols('a b c d', above_fermi=True)
p, q, r, s = symbols('p q r s', cls=Dummy)
Fock = (AntiSymmetricTensor('f', (p,), (q,))*
NO(Fd(p)*F(q)))
V = (AntiSymmetricTensor('v', (p, q), (r, s))*
NO(Fd(p)*Fd(q)*F(s)*F(r)))/4
Fai = wicks(NO(Fd(i)*F(a))*Fock,
keep_only_fully_contracted=True,
simplify_kronecker_deltas=True)
assert Fai == AntiSymmetricTensor('f', (a,), (i,))
Vabij = wicks(NO(Fd(i)*Fd(j)*F(b)*F(a))*V,
keep_only_fully_contracted=True,
simplify_kronecker_deltas=True)
assert Vabij == AntiSymmetricTensor('v', (a, b), (i, j))
def test_substitute_dummies_without_dummies():
i, j = symbols('i,j')
assert substitute_dummies(att(i, j) + 2) == att(i, j) + 2
assert substitute_dummies(att(i, j) + 1) == att(i, j) + 1
def test_substitute_dummies_NO_operator():
i, j = symbols('i j', cls=Dummy)
assert substitute_dummies(att(i, j)*NO(Fd(i)*F(j))
- att(j, i)*NO(Fd(j)*F(i))) == 0
def test_substitute_dummies_SQ_operator():
i, j = symbols('i j', cls=Dummy)
assert substitute_dummies(att(i, j)*Fd(i)*F(j)
- att(j, i)*Fd(j)*F(i)) == 0
def test_substitute_dummies_new_indices():
i, j = symbols('i j', below_fermi=True, cls=Dummy)
a, b = symbols('a b', above_fermi=True, cls=Dummy)
p, q = symbols('p q', cls=Dummy)
f = Function('f')
assert substitute_dummies(f(i, a, p) - f(j, b, q), new_indices=True) == 0
def test_substitute_dummies_substitution_order():
i, j, k, l = symbols('i j k l', below_fermi=True, cls=Dummy)
f = Function('f')
from sympy.utilities.iterables import variations
for permut in variations([i, j, k, l], 4):
assert substitute_dummies(f(*permut) - f(i, j, k, l)) == 0
def test_dummy_order_inner_outer_lines_VT1T1T1():
ii = symbols('i', below_fermi=True)
aa = symbols('a', above_fermi=True)
k, l = symbols('k l', below_fermi=True, cls=Dummy)
c, d = symbols('c d', above_fermi=True, cls=Dummy)
v = Function('v')
t = Function('t')
dums = _get_ordered_dummies
# Coupled-Cluster T1 terms with V*T1*T1*T1
# t^{a}_{k} t^{c}_{i} t^{d}_{l} v^{lk}_{dc}
exprs = [
# permut v and t <=> swapping internal lines, equivalent
# irrespective of symmetries in v
v(k, l, c, d)*t(c, ii)*t(d, l)*t(aa, k),
v(l, k, c, d)*t(c, ii)*t(d, k)*t(aa, l),
v(k, l, d, c)*t(d, ii)*t(c, l)*t(aa, k),
v(l, k, d, c)*t(d, ii)*t(c, k)*t(aa, l),
]
for permut in exprs[1:]:
assert dums(exprs[0]) != dums(permut)
assert substitute_dummies(exprs[0]) == substitute_dummies(permut)
def test_dummy_order_inner_outer_lines_VT1T1T1T1():
ii, jj = symbols('i j', below_fermi=True)
aa, bb = symbols('a b', above_fermi=True)
k, l = symbols('k l', below_fermi=True, cls=Dummy)
c, d = symbols('c d', above_fermi=True, cls=Dummy)
v = Function('v')
t = Function('t')
dums = _get_ordered_dummies
# Coupled-Cluster T2 terms with V*T1*T1*T1*T1
exprs = [
# permut t <=> swapping external lines, not equivalent
# except if v has certain symmetries.
v(k, l, c, d)*t(c, ii)*t(d, jj)*t(aa, k)*t(bb, l),
v(k, l, c, d)*t(c, jj)*t(d, ii)*t(aa, k)*t(bb, l),
v(k, l, c, d)*t(c, ii)*t(d, jj)*t(bb, k)*t(aa, l),
v(k, l, c, d)*t(c, jj)*t(d, ii)*t(bb, k)*t(aa, l),
]
for permut in exprs[1:]:
assert dums(exprs[0]) != dums(permut)
assert substitute_dummies(exprs[0]) != substitute_dummies(permut)
exprs = [
# permut v <=> swapping external lines, not equivalent
# except if v has certain symmetries.
#
# Note that in contrast to above, these permutations have identical
# dummy order. That is because the proximity to external indices
# has higher influence on the canonical dummy ordering than the
# position of a dummy on the factors. In fact, the terms here are
# similar in structure as the result of the dummy substitutions above.
v(k, l, c, d)*t(c, ii)*t(d, jj)*t(aa, k)*t(bb, l),
v(l, k, c, d)*t(c, ii)*t(d, jj)*t(aa, k)*t(bb, l),
v(k, l, d, c)*t(c, ii)*t(d, jj)*t(aa, k)*t(bb, l),
v(l, k, d, c)*t(c, ii)*t(d, jj)*t(aa, k)*t(bb, l),
]
for permut in exprs[1:]:
assert dums(exprs[0]) == dums(permut)
assert substitute_dummies(exprs[0]) != substitute_dummies(permut)
exprs = [
# permut t and v <=> swapping internal lines, equivalent.
# Canonical dummy order is different, and a consistent
# substitution reveals the equivalence.
v(k, l, c, d)*t(c, ii)*t(d, jj)*t(aa, k)*t(bb, l),
v(k, l, d, c)*t(c, jj)*t(d, ii)*t(aa, k)*t(bb, l),
v(l, k, c, d)*t(c, ii)*t(d, jj)*t(bb, k)*t(aa, l),
v(l, k, d, c)*t(c, jj)*t(d, ii)*t(bb, k)*t(aa, l),
]
for permut in exprs[1:]:
assert dums(exprs[0]) != dums(permut)
assert substitute_dummies(exprs[0]) == substitute_dummies(permut)
def test_get_subNO():
p, q, r = symbols('p,q,r')
assert NO(F(p)*F(q)*F(r)).get_subNO(1) == NO(F(p)*F(r))
assert NO(F(p)*F(q)*F(r)).get_subNO(0) == NO(F(q)*F(r))
assert NO(F(p)*F(q)*F(r)).get_subNO(2) == NO(F(p)*F(q))
def test_equivalent_internal_lines_VT1T1():
i, j, k, l = symbols('i j k l', below_fermi=True, cls=Dummy)
a, b, c, d = symbols('a b c d', above_fermi=True, cls=Dummy)
v = Function('v')
t = Function('t')
dums = _get_ordered_dummies
exprs = [ # permute v. Different dummy order. Not equivalent.
v(i, j, a, b)*t(a, i)*t(b, j),
v(j, i, a, b)*t(a, i)*t(b, j),
v(i, j, b, a)*t(a, i)*t(b, j),
]
for permut in exprs[1:]:
assert dums(exprs[0]) != dums(permut)
assert substitute_dummies(exprs[0]) != substitute_dummies(permut)
exprs = [ # permute v. Different dummy order. Equivalent
v(i, j, a, b)*t(a, i)*t(b, j),
v(j, i, b, a)*t(a, i)*t(b, j),
]
for permut in exprs[1:]:
assert dums(exprs[0]) != dums(permut)
assert substitute_dummies(exprs[0]) == substitute_dummies(permut)
exprs = [ # permute t. Same dummy order, not equivalent.
v(i, j, a, b)*t(a, i)*t(b, j),
v(i, j, a, b)*t(b, i)*t(a, j),
]
for permut in exprs[1:]:
assert dums(exprs[0]) == dums(permut)
assert substitute_dummies(exprs[0]) != substitute_dummies(permut)
exprs = [ # permute v and t. Different dummy order, equivalent
v(i, j, a, b)*t(a, i)*t(b, j),
v(j, i, a, b)*t(a, j)*t(b, i),
v(i, j, b, a)*t(b, i)*t(a, j),
v(j, i, b, a)*t(b, j)*t(a, i),
]
for permut in exprs[1:]:
assert dums(exprs[0]) != dums(permut)
assert substitute_dummies(exprs[0]) == substitute_dummies(permut)
def test_equivalent_internal_lines_VT2conjT2():
# this diagram requires special handling in TCE
i, j, k, l, m, n = symbols('i j k l m n', below_fermi=True, cls=Dummy)
a, b, c, d, e, f = symbols('a b c d e f', above_fermi=True, cls=Dummy)
p1, p2, p3, p4 = symbols('p1 p2 p3 p4', above_fermi=True, cls=Dummy)
h1, h2, h3, h4 = symbols('h1 h2 h3 h4', below_fermi=True, cls=Dummy)
from sympy.utilities.iterables import variations
v = Function('v')
t = Function('t')
dums = _get_ordered_dummies
# v(abcd)t(abij)t(ijcd)
template = v(p1, p2, p3, p4)*t(p1, p2, i, j)*t(i, j, p3, p4)
permutator = variations([a, b, c, d], 4)
base = template.subs(zip([p1, p2, p3, p4], next(permutator)))
for permut in permutator:
subslist = zip([p1, p2, p3, p4], permut)
expr = template.subs(subslist)
assert dums(base) != dums(expr)
assert substitute_dummies(expr) == substitute_dummies(base)
template = v(p1, p2, p3, p4)*t(p1, p2, j, i)*t(j, i, p3, p4)
permutator = variations([a, b, c, d], 4)
base = template.subs(zip([p1, p2, p3, p4], next(permutator)))
for permut in permutator:
subslist = zip([p1, p2, p3, p4], permut)
expr = template.subs(subslist)
assert dums(base) != dums(expr)
assert substitute_dummies(expr) == substitute_dummies(base)
# v(abcd)t(abij)t(jicd)
template = v(p1, p2, p3, p4)*t(p1, p2, i, j)*t(j, i, p3, p4)
permutator = variations([a, b, c, d], 4)
base = template.subs(zip([p1, p2, p3, p4], next(permutator)))
for permut in permutator:
subslist = zip([p1, p2, p3, p4], permut)
expr = template.subs(subslist)
assert dums(base) != dums(expr)
assert substitute_dummies(expr) == substitute_dummies(base)
template = v(p1, p2, p3, p4)*t(p1, p2, j, i)*t(i, j, p3, p4)
permutator = variations([a, b, c, d], 4)
base = template.subs(zip([p1, p2, p3, p4], next(permutator)))
for permut in permutator:
subslist = zip([p1, p2, p3, p4], permut)
expr = template.subs(subslist)
assert dums(base) != dums(expr)
assert substitute_dummies(expr) == substitute_dummies(base)
def test_equivalent_internal_lines_VT2conjT2_ambiguous_order():
# These diagrams invokes _determine_ambiguous() because the
# dummies can not be ordered unambiguously by the key alone
i, j, k, l, m, n = symbols('i j k l m n', below_fermi=True, cls=Dummy)
a, b, c, d, e, f = symbols('a b c d e f', above_fermi=True, cls=Dummy)
p1, p2, p3, p4 = symbols('p1 p2 p3 p4', above_fermi=True, cls=Dummy)
h1, h2, h3, h4 = symbols('h1 h2 h3 h4', below_fermi=True, cls=Dummy)
from sympy.utilities.iterables import variations
v = Function('v')
t = Function('t')
dums = _get_ordered_dummies
# v(abcd)t(abij)t(cdij)
template = v(p1, p2, p3, p4)*t(p1, p2, i, j)*t(p3, p4, i, j)
permutator = variations([a, b, c, d], 4)
base = template.subs(zip([p1, p2, p3, p4], next(permutator)))
for permut in permutator:
subslist = zip([p1, p2, p3, p4], permut)
expr = template.subs(subslist)
assert dums(base) != dums(expr)
assert substitute_dummies(expr) == substitute_dummies(base)
template = v(p1, p2, p3, p4)*t(p1, p2, j, i)*t(p3, p4, i, j)
permutator = variations([a, b, c, d], 4)
base = template.subs(zip([p1, p2, p3, p4], next(permutator)))
for permut in permutator:
subslist = zip([p1, p2, p3, p4], permut)
expr = template.subs(subslist)
assert dums(base) != dums(expr)
assert substitute_dummies(expr) == substitute_dummies(base)
def test_equivalent_internal_lines_VT2():
i, j, k, l = symbols('i j k l', below_fermi=True, cls=Dummy)
a, b, c, d = symbols('a b c d', above_fermi=True, cls=Dummy)
v = Function('v')
t = Function('t')
dums = _get_ordered_dummies
exprs = [
# permute v. Same dummy order, not equivalent.
#
# This test show that the dummy order may not be sensitive to all
# index permutations. The following expressions have identical
# structure as the resulting terms from of the dummy substitutions
# in the test above. Here, all expressions have the same dummy
# order, so they cannot be simplified by means of dummy
# substitution. In order to simplify further, it is necessary to
# exploit symmetries in the objects, for instance if t or v is
# antisymmetric.
v(i, j, a, b)*t(a, b, i, j),
v(j, i, a, b)*t(a, b, i, j),
v(i, j, b, a)*t(a, b, i, j),
v(j, i, b, a)*t(a, b, i, j),
]
for permut in exprs[1:]:
assert dums(exprs[0]) == dums(permut)
assert substitute_dummies(exprs[0]) != substitute_dummies(permut)
exprs = [
# permute t.
v(i, j, a, b)*t(a, b, i, j),
v(i, j, a, b)*t(b, a, i, j),
v(i, j, a, b)*t(a, b, j, i),
v(i, j, a, b)*t(b, a, j, i),
]
for permut in exprs[1:]:
assert dums(exprs[0]) != dums(permut)
assert substitute_dummies(exprs[0]) != substitute_dummies(permut)
exprs = [ # permute v and t. Relabelling of dummies should be equivalent.
v(i, j, a, b)*t(a, b, i, j),
v(j, i, a, b)*t(a, b, j, i),
v(i, j, b, a)*t(b, a, i, j),
v(j, i, b, a)*t(b, a, j, i),
]
for permut in exprs[1:]:
assert dums(exprs[0]) != dums(permut)
assert substitute_dummies(exprs[0]) == substitute_dummies(permut)
def test_internal_external_VT2T2():
ii, jj = symbols('i j', below_fermi=True)
aa, bb = symbols('a b', above_fermi=True)
k, l = symbols('k l', below_fermi=True, cls=Dummy)
c, d = symbols('c d', above_fermi=True, cls=Dummy)
v = Function('v')
t = Function('t')
dums = _get_ordered_dummies
exprs = [
v(k, l, c, d)*t(aa, c, ii, k)*t(bb, d, jj, l),
v(l, k, c, d)*t(aa, c, ii, l)*t(bb, d, jj, k),
v(k, l, d, c)*t(aa, d, ii, k)*t(bb, c, jj, l),
v(l, k, d, c)*t(aa, d, ii, l)*t(bb, c, jj, k),
]
for permut in exprs[1:]:
assert dums(exprs[0]) != dums(permut)
assert substitute_dummies(exprs[0]) == substitute_dummies(permut)
exprs = [
v(k, l, c, d)*t(aa, c, ii, k)*t(d, bb, jj, l),
v(l, k, c, d)*t(aa, c, ii, l)*t(d, bb, jj, k),
v(k, l, d, c)*t(aa, d, ii, k)*t(c, bb, jj, l),
v(l, k, d, c)*t(aa, d, ii, l)*t(c, bb, jj, k),
]
for permut in exprs[1:]:
assert dums(exprs[0]) != dums(permut)
assert substitute_dummies(exprs[0]) == substitute_dummies(permut)
exprs = [
v(k, l, c, d)*t(c, aa, ii, k)*t(bb, d, jj, l),
v(l, k, c, d)*t(c, aa, ii, l)*t(bb, d, jj, k),
v(k, l, d, c)*t(d, aa, ii, k)*t(bb, c, jj, l),
v(l, k, d, c)*t(d, aa, ii, l)*t(bb, c, jj, k),
]
for permut in exprs[1:]:
assert dums(exprs[0]) != dums(permut)
assert substitute_dummies(exprs[0]) == substitute_dummies(permut)
def test_internal_external_pqrs():
ii, jj = symbols('i j')
aa, bb = symbols('a b')
k, l = symbols('k l', cls=Dummy)
c, d = symbols('c d', cls=Dummy)
v = Function('v')
t = Function('t')
dums = _get_ordered_dummies
exprs = [
v(k, l, c, d)*t(aa, c, ii, k)*t(bb, d, jj, l),
v(l, k, c, d)*t(aa, c, ii, l)*t(bb, d, jj, k),
v(k, l, d, c)*t(aa, d, ii, k)*t(bb, c, jj, l),
v(l, k, d, c)*t(aa, d, ii, l)*t(bb, c, jj, k),
]
for permut in exprs[1:]:
assert dums(exprs[0]) != dums(permut)
assert substitute_dummies(exprs[0]) == substitute_dummies(permut)
def test_dummy_order_well_defined():
aa, bb = symbols('a b', above_fermi=True)
k, l, m = symbols('k l m', below_fermi=True, cls=Dummy)
c, d = symbols('c d', above_fermi=True, cls=Dummy)
p, q = symbols('p q', cls=Dummy)
A = Function('A')
B = Function('B')
C = Function('C')
dums = _get_ordered_dummies
# We go through all key components in the order of increasing priority,
# and consider only fully orderable expressions. Non-orderable expressions
# are tested elsewhere.
# pos in first factor determines sort order
assert dums(A(k, l)*B(l, k)) == [k, l]
assert dums(A(l, k)*B(l, k)) == [l, k]
assert dums(A(k, l)*B(k, l)) == [k, l]
assert dums(A(l, k)*B(k, l)) == [l, k]
# factors involving the index
assert dums(A(k, l)*B(l, m)*C(k, m)) == [l, k, m]
assert dums(A(k, l)*B(l, m)*C(m, k)) == [l, k, m]
assert dums(A(l, k)*B(l, m)*C(k, m)) == [l, k, m]
assert dums(A(l, k)*B(l, m)*C(m, k)) == [l, k, m]
assert dums(A(k, l)*B(m, l)*C(k, m)) == [l, k, m]
assert dums(A(k, l)*B(m, l)*C(m, k)) == [l, k, m]
assert dums(A(l, k)*B(m, l)*C(k, m)) == [l, k, m]
assert dums(A(l, k)*B(m, l)*C(m, k)) == [l, k, m]
# same, but with factor order determined by non-dummies
assert dums(A(k, aa, l)*A(l, bb, m)*A(bb, k, m)) == [l, k, m]
assert dums(A(k, aa, l)*A(l, bb, m)*A(bb, m, k)) == [l, k, m]
assert dums(A(k, aa, l)*A(m, bb, l)*A(bb, k, m)) == [l, k, m]
assert dums(A(k, aa, l)*A(m, bb, l)*A(bb, m, k)) == [l, k, m]
assert dums(A(l, aa, k)*A(l, bb, m)*A(bb, k, m)) == [l, k, m]
assert dums(A(l, aa, k)*A(l, bb, m)*A(bb, m, k)) == [l, k, m]
assert dums(A(l, aa, k)*A(m, bb, l)*A(bb, k, m)) == [l, k, m]
assert dums(A(l, aa, k)*A(m, bb, l)*A(bb, m, k)) == [l, k, m]
# index range
assert dums(A(p, c, k)*B(p, c, k)) == [k, c, p]
assert dums(A(p, k, c)*B(p, c, k)) == [k, c, p]
assert dums(A(c, k, p)*B(p, c, k)) == [k, c, p]
assert dums(A(c, p, k)*B(p, c, k)) == [k, c, p]
assert dums(A(k, c, p)*B(p, c, k)) == [k, c, p]
assert dums(A(k, p, c)*B(p, c, k)) == [k, c, p]
assert dums(B(p, c, k)*A(p, c, k)) == [k, c, p]
assert dums(B(p, k, c)*A(p, c, k)) == [k, c, p]
assert dums(B(c, k, p)*A(p, c, k)) == [k, c, p]
assert dums(B(c, p, k)*A(p, c, k)) == [k, c, p]
assert dums(B(k, c, p)*A(p, c, k)) == [k, c, p]
assert dums(B(k, p, c)*A(p, c, k)) == [k, c, p]
def test_dummy_order_ambiguous():
aa, bb = symbols('a b', above_fermi=True)
i, j, k, l, m = symbols('i j k l m', below_fermi=True, cls=Dummy)
a, b, c, d, e = symbols('a b c d e', above_fermi=True, cls=Dummy)
p, q = symbols('p q', cls=Dummy)
p1, p2, p3, p4 = symbols('p1 p2 p3 p4', above_fermi=True, cls=Dummy)
p5, p6, p7, p8 = symbols('p5 p6 p7 p8', above_fermi=True, cls=Dummy)
h1, h2, h3, h4 = symbols('h1 h2 h3 h4', below_fermi=True, cls=Dummy)
h5, h6, h7, h8 = symbols('h5 h6 h7 h8', below_fermi=True, cls=Dummy)
A = Function('A')
B = Function('B')
from sympy.utilities.iterables import variations
# A*A*A*A*B -- ordering of p5 and p4 is used to figure out the rest
template = A(p1, p2)*A(p4, p1)*A(p2, p3)*A(p3, p5)*B(p5, p4)
permutator = variations([a, b, c, d, e], 5)
base = template.subs(zip([p1, p2, p3, p4, p5], next(permutator)))
for permut in permutator:
subslist = zip([p1, p2, p3, p4, p5], permut)
expr = template.subs(subslist)
assert substitute_dummies(expr) == substitute_dummies(base)
# A*A*A*A*A -- an arbitrary index is assigned and the rest are figured out
template = A(p1, p2)*A(p4, p1)*A(p2, p3)*A(p3, p5)*A(p5, p4)
permutator = variations([a, b, c, d, e], 5)
base = template.subs(zip([p1, p2, p3, p4, p5], next(permutator)))
for permut in permutator:
subslist = zip([p1, p2, p3, p4, p5], permut)
expr = template.subs(subslist)
assert substitute_dummies(expr) == substitute_dummies(base)
# A*A*A -- ordering of p5 and p4 is used to figure out the rest
template = A(p1, p2, p4, p1)*A(p2, p3, p3, p5)*A(p5, p4)
permutator = variations([a, b, c, d, e], 5)
base = template.subs(zip([p1, p2, p3, p4, p5], next(permutator)))
for permut in permutator:
subslist = zip([p1, p2, p3, p4, p5], permut)
expr = template.subs(subslist)
assert substitute_dummies(expr) == substitute_dummies(base)
def atv(*args):
return AntiSymmetricTensor('v', args[:2], args[2:] )
def att(*args):
if len(args) == 4:
return AntiSymmetricTensor('t', args[:2], args[2:] )
elif len(args) == 2:
return AntiSymmetricTensor('t', (args[0],), (args[1],))
def test_dummy_order_inner_outer_lines_VT1T1T1_AT():
ii = symbols('i', below_fermi=True)
aa = symbols('a', above_fermi=True)
k, l = symbols('k l', below_fermi=True, cls=Dummy)
c, d = symbols('c d', above_fermi=True, cls=Dummy)
# Coupled-Cluster T1 terms with V*T1*T1*T1
# t^{a}_{k} t^{c}_{i} t^{d}_{l} v^{lk}_{dc}
exprs = [
# permut v and t <=> swapping internal lines, equivalent
# irrespective of symmetries in v
atv(k, l, c, d)*att(c, ii)*att(d, l)*att(aa, k),
atv(l, k, c, d)*att(c, ii)*att(d, k)*att(aa, l),
atv(k, l, d, c)*att(d, ii)*att(c, l)*att(aa, k),
atv(l, k, d, c)*att(d, ii)*att(c, k)*att(aa, l),
]
for permut in exprs[1:]:
assert substitute_dummies(exprs[0]) == substitute_dummies(permut)
def test_dummy_order_inner_outer_lines_VT1T1T1T1_AT():
ii, jj = symbols('i j', below_fermi=True)
aa, bb = symbols('a b', above_fermi=True)
k, l = symbols('k l', below_fermi=True, cls=Dummy)
c, d = symbols('c d', above_fermi=True, cls=Dummy)
# Coupled-Cluster T2 terms with V*T1*T1*T1*T1
# non-equivalent substitutions (change of sign)
exprs = [
# permut t <=> swapping external lines
atv(k, l, c, d)*att(c, ii)*att(d, jj)*att(aa, k)*att(bb, l),
atv(k, l, c, d)*att(c, jj)*att(d, ii)*att(aa, k)*att(bb, l),
atv(k, l, c, d)*att(c, ii)*att(d, jj)*att(bb, k)*att(aa, l),
]
for permut in exprs[1:]:
assert substitute_dummies(exprs[0]) == -substitute_dummies(permut)
# equivalent substitutions
exprs = [
atv(k, l, c, d)*att(c, ii)*att(d, jj)*att(aa, k)*att(bb, l),
# permut t <=> swapping external lines
atv(k, l, c, d)*att(c, jj)*att(d, ii)*att(bb, k)*att(aa, l),
]
for permut in exprs[1:]:
assert substitute_dummies(exprs[0]) == substitute_dummies(permut)
def test_equivalent_internal_lines_VT1T1_AT():
i, j, k, l = symbols('i j k l', below_fermi=True, cls=Dummy)
a, b, c, d = symbols('a b c d', above_fermi=True, cls=Dummy)
exprs = [ # permute v. Different dummy order. Not equivalent.
atv(i, j, a, b)*att(a, i)*att(b, j),
atv(j, i, a, b)*att(a, i)*att(b, j),
atv(i, j, b, a)*att(a, i)*att(b, j),
]
for permut in exprs[1:]:
assert substitute_dummies(exprs[0]) != substitute_dummies(permut)
exprs = [ # permute v. Different dummy order. Equivalent
atv(i, j, a, b)*att(a, i)*att(b, j),
atv(j, i, b, a)*att(a, i)*att(b, j),
]
for permut in exprs[1:]:
assert substitute_dummies(exprs[0]) == substitute_dummies(permut)
exprs = [ # permute t. Same dummy order, not equivalent.
atv(i, j, a, b)*att(a, i)*att(b, j),
atv(i, j, a, b)*att(b, i)*att(a, j),
]
for permut in exprs[1:]:
assert substitute_dummies(exprs[0]) != substitute_dummies(permut)
exprs = [ # permute v and t. Different dummy order, equivalent
atv(i, j, a, b)*att(a, i)*att(b, j),
atv(j, i, a, b)*att(a, j)*att(b, i),
atv(i, j, b, a)*att(b, i)*att(a, j),
atv(j, i, b, a)*att(b, j)*att(a, i),
]
for permut in exprs[1:]:
assert substitute_dummies(exprs[0]) == substitute_dummies(permut)
def test_equivalent_internal_lines_VT2conjT2_AT():
# this diagram requires special handling in TCE
i, j, k, l, m, n = symbols('i j k l m n', below_fermi=True, cls=Dummy)
a, b, c, d, e, f = symbols('a b c d e f', above_fermi=True, cls=Dummy)
p1, p2, p3, p4 = symbols('p1 p2 p3 p4', above_fermi=True, cls=Dummy)
h1, h2, h3, h4 = symbols('h1 h2 h3 h4', below_fermi=True, cls=Dummy)
from sympy.utilities.iterables import variations
# atv(abcd)att(abij)att(ijcd)
template = atv(p1, p2, p3, p4)*att(p1, p2, i, j)*att(i, j, p3, p4)
permutator = variations([a, b, c, d], 4)
base = template.subs(zip([p1, p2, p3, p4], next(permutator)))
for permut in permutator:
subslist = zip([p1, p2, p3, p4], permut)
expr = template.subs(subslist)
assert substitute_dummies(expr) == substitute_dummies(base)
template = atv(p1, p2, p3, p4)*att(p1, p2, j, i)*att(j, i, p3, p4)
permutator = variations([a, b, c, d], 4)
base = template.subs(zip([p1, p2, p3, p4], next(permutator)))
for permut in permutator:
subslist = zip([p1, p2, p3, p4], permut)
expr = template.subs(subslist)
assert substitute_dummies(expr) == substitute_dummies(base)
# atv(abcd)att(abij)att(jicd)
template = atv(p1, p2, p3, p4)*att(p1, p2, i, j)*att(j, i, p3, p4)
permutator = variations([a, b, c, d], 4)
base = template.subs(zip([p1, p2, p3, p4], next(permutator)))
for permut in permutator:
subslist = zip([p1, p2, p3, p4], permut)
expr = template.subs(subslist)
assert substitute_dummies(expr) == substitute_dummies(base)
template = atv(p1, p2, p3, p4)*att(p1, p2, j, i)*att(i, j, p3, p4)
permutator = variations([a, b, c, d], 4)
base = template.subs(zip([p1, p2, p3, p4], next(permutator)))
for permut in permutator:
subslist = zip([p1, p2, p3, p4], permut)
expr = template.subs(subslist)
assert substitute_dummies(expr) == substitute_dummies(base)
def test_equivalent_internal_lines_VT2conjT2_ambiguous_order_AT():
# These diagrams invokes _determine_ambiguous() because the
# dummies can not be ordered unambiguously by the key alone
i, j, k, l, m, n = symbols('i j k l m n', below_fermi=True, cls=Dummy)
a, b, c, d, e, f = symbols('a b c d e f', above_fermi=True, cls=Dummy)
p1, p2, p3, p4 = symbols('p1 p2 p3 p4', above_fermi=True, cls=Dummy)
h1, h2, h3, h4 = symbols('h1 h2 h3 h4', below_fermi=True, cls=Dummy)
from sympy.utilities.iterables import variations
# atv(abcd)att(abij)att(cdij)
template = atv(p1, p2, p3, p4)*att(p1, p2, i, j)*att(p3, p4, i, j)
permutator = variations([a, b, c, d], 4)
base = template.subs(zip([p1, p2, p3, p4], next(permutator)))
for permut in permutator:
subslist = zip([p1, p2, p3, p4], permut)
expr = template.subs(subslist)
assert substitute_dummies(expr) == substitute_dummies(base)
template = atv(p1, p2, p3, p4)*att(p1, p2, j, i)*att(p3, p4, i, j)
permutator = variations([a, b, c, d], 4)
base = template.subs(zip([p1, p2, p3, p4], next(permutator)))
for permut in permutator:
subslist = zip([p1, p2, p3, p4], permut)
expr = template.subs(subslist)
assert substitute_dummies(expr) == substitute_dummies(base)
def test_equivalent_internal_lines_VT2_AT():
i, j, k, l = symbols('i j k l', below_fermi=True, cls=Dummy)
a, b, c, d = symbols('a b c d', above_fermi=True, cls=Dummy)
exprs = [
# permute v. Same dummy order, not equivalent.
atv(i, j, a, b)*att(a, b, i, j),
atv(j, i, a, b)*att(a, b, i, j),
atv(i, j, b, a)*att(a, b, i, j),
]
for permut in exprs[1:]:
assert substitute_dummies(exprs[0]) != substitute_dummies(permut)
exprs = [
# permute t.
atv(i, j, a, b)*att(a, b, i, j),
atv(i, j, a, b)*att(b, a, i, j),
atv(i, j, a, b)*att(a, b, j, i),
]
for permut in exprs[1:]:
assert substitute_dummies(exprs[0]) != substitute_dummies(permut)
exprs = [ # permute v and t. Relabelling of dummies should be equivalent.
atv(i, j, a, b)*att(a, b, i, j),
atv(j, i, a, b)*att(a, b, j, i),
atv(i, j, b, a)*att(b, a, i, j),
atv(j, i, b, a)*att(b, a, j, i),
]
for permut in exprs[1:]:
assert substitute_dummies(exprs[0]) == substitute_dummies(permut)
def test_internal_external_VT2T2_AT():
ii, jj = symbols('i j', below_fermi=True)
aa, bb = symbols('a b', above_fermi=True)
k, l = symbols('k l', below_fermi=True, cls=Dummy)
c, d = symbols('c d', above_fermi=True, cls=Dummy)
exprs = [
atv(k, l, c, d)*att(aa, c, ii, k)*att(bb, d, jj, l),
atv(l, k, c, d)*att(aa, c, ii, l)*att(bb, d, jj, k),
atv(k, l, d, c)*att(aa, d, ii, k)*att(bb, c, jj, l),
atv(l, k, d, c)*att(aa, d, ii, l)*att(bb, c, jj, k),
]
for permut in exprs[1:]:
assert substitute_dummies(exprs[0]) == substitute_dummies(permut)
exprs = [
atv(k, l, c, d)*att(aa, c, ii, k)*att(d, bb, jj, l),
atv(l, k, c, d)*att(aa, c, ii, l)*att(d, bb, jj, k),
atv(k, l, d, c)*att(aa, d, ii, k)*att(c, bb, jj, l),
atv(l, k, d, c)*att(aa, d, ii, l)*att(c, bb, jj, k),
]
for permut in exprs[1:]:
assert substitute_dummies(exprs[0]) == substitute_dummies(permut)
exprs = [
atv(k, l, c, d)*att(c, aa, ii, k)*att(bb, d, jj, l),
atv(l, k, c, d)*att(c, aa, ii, l)*att(bb, d, jj, k),
atv(k, l, d, c)*att(d, aa, ii, k)*att(bb, c, jj, l),
atv(l, k, d, c)*att(d, aa, ii, l)*att(bb, c, jj, k),
]
for permut in exprs[1:]:
assert substitute_dummies(exprs[0]) == substitute_dummies(permut)
def test_internal_external_pqrs_AT():
ii, jj = symbols('i j')
aa, bb = symbols('a b')
k, l = symbols('k l', cls=Dummy)
c, d = symbols('c d', cls=Dummy)
exprs = [
atv(k, l, c, d)*att(aa, c, ii, k)*att(bb, d, jj, l),
atv(l, k, c, d)*att(aa, c, ii, l)*att(bb, d, jj, k),
atv(k, l, d, c)*att(aa, d, ii, k)*att(bb, c, jj, l),
atv(l, k, d, c)*att(aa, d, ii, l)*att(bb, c, jj, k),
]
for permut in exprs[1:]:
assert substitute_dummies(exprs[0]) == substitute_dummies(permut)
def test_canonical_ordering_AntiSymmetricTensor():
v = symbols("v")
virtual_indices = ('c', 'd')
occupied_indices = ('k', 'l')
c, d = symbols(('c','d'), above_fermi=True,
cls=Dummy)
k, l = symbols(('k','l'), below_fermi=True,
cls=Dummy)
# formerly, the left gave either the left or the right
assert AntiSymmetricTensor(v, (k, l), (d, c)
) == -AntiSymmetricTensor(v, (l, k), (d, c))
|
45d98b2059ec87b88bc4b685ccef5565aca976957a561f1db1f2b8e19768826f | """
This module can be used to solve 2D beam bending problems with
singularity functions in mechanics.
"""
from __future__ import print_function, division
from sympy.core import S, Symbol, diff, symbols
from sympy.solvers import linsolve
from sympy.printing import sstr
from sympy.functions import SingularityFunction, Piecewise, factorial
from sympy.core import sympify
from sympy.integrals import integrate
from sympy.series import limit
from sympy.plotting import plot, PlotGrid
from sympy.geometry.entity import GeometryEntity
from sympy.external import import_module
from sympy import lambdify, Add
from sympy.core.compatibility import iterable
from sympy.utilities.decorator import doctest_depends_on
numpy = import_module('numpy', __import__kwargs={'fromlist':['arange']})
class Beam(object):
"""
A Beam is a structural element that is capable of withstanding load
primarily by resisting against bending. Beams are characterized by
their cross sectional profile(Second moment of area), their length
and their material.
.. note::
While solving a beam bending problem, a user should choose its
own sign convention and should stick to it. The results will
automatically follow the chosen sign convention.
Examples
========
There is a beam of length 4 meters. A constant distributed load of 6 N/m
is applied from half of the beam till the end. There are two simple supports
below the beam, one at the starting point and another at the ending point
of the beam. The deflection of the beam at the end is restricted.
Using the sign convention of downwards forces being positive.
>>> from sympy.physics.continuum_mechanics.beam import Beam
>>> from sympy import symbols, Piecewise
>>> E, I = symbols('E, I')
>>> R1, R2 = symbols('R1, R2')
>>> b = Beam(4, E, I)
>>> b.apply_load(R1, 0, -1)
>>> b.apply_load(6, 2, 0)
>>> b.apply_load(R2, 4, -1)
>>> b.bc_deflection = [(0, 0), (4, 0)]
>>> b.boundary_conditions
{'deflection': [(0, 0), (4, 0)], 'slope': []}
>>> b.load
R1*SingularityFunction(x, 0, -1) + R2*SingularityFunction(x, 4, -1) + 6*SingularityFunction(x, 2, 0)
>>> b.solve_for_reaction_loads(R1, R2)
>>> b.load
-3*SingularityFunction(x, 0, -1) + 6*SingularityFunction(x, 2, 0) - 9*SingularityFunction(x, 4, -1)
>>> b.shear_force()
-3*SingularityFunction(x, 0, 0) + 6*SingularityFunction(x, 2, 1) - 9*SingularityFunction(x, 4, 0)
>>> b.bending_moment()
-3*SingularityFunction(x, 0, 1) + 3*SingularityFunction(x, 2, 2) - 9*SingularityFunction(x, 4, 1)
>>> b.slope()
(-3*SingularityFunction(x, 0, 2)/2 + SingularityFunction(x, 2, 3) - 9*SingularityFunction(x, 4, 2)/2 + 7)/(E*I)
>>> b.deflection()
(7*x - SingularityFunction(x, 0, 3)/2 + SingularityFunction(x, 2, 4)/4 - 3*SingularityFunction(x, 4, 3)/2)/(E*I)
>>> b.deflection().rewrite(Piecewise)
(7*x - Piecewise((x**3, x > 0), (0, True))/2
- 3*Piecewise(((x - 4)**3, x - 4 > 0), (0, True))/2
+ Piecewise(((x - 2)**4, x - 2 > 0), (0, True))/4)/(E*I)
"""
def __init__(self, length, elastic_modulus, second_moment, variable=Symbol('x'), base_char='C'):
"""Initializes the class.
Parameters
==========
length : Sympifyable
A Symbol or value representing the Beam's length.
elastic_modulus : Sympifyable
A SymPy expression representing the Beam's Modulus of Elasticity.
It is a measure of the stiffness of the Beam material. It can
also be a continuous function of position along the beam.
second_moment : Sympifyable or Geometry object
Describes the cross-section of the beam via a SymPy expression
representing the Beam's second moment of area. It is a geometrical
property of an area which reflects how its points are distributed
with respect to its neutral axis. It can also be a continuous
function of position along the beam. Alternatively ``second_moment``
can be a shape object such as a ``Polygon`` from the geometry module
representing the shape of the cross-section of the beam. In such cases,
it is assumed that the x-axis of the shape object is aligned with the
bending axis of the beam. The second moment of area will be computed
from the shape object internally.
variable : Symbol, optional
A Symbol object that will be used as the variable along the beam
while representing the load, shear, moment, slope and deflection
curve. By default, it is set to ``Symbol('x')``.
base_char : String, optional
A String that will be used as base character to generate sequential
symbols for integration constants in cases where boundary conditions
are not sufficient to solve them.
"""
self.length = length
self.elastic_modulus = elastic_modulus
if isinstance(second_moment, GeometryEntity):
self.cross_section = second_moment
else:
self.cross_section = None
self.second_moment = second_moment
self.variable = variable
self._base_char = base_char
self._boundary_conditions = {'deflection': [], 'slope': []}
self._load = 0
self._applied_supports = []
self._support_as_loads = []
self._applied_loads = []
self._reaction_loads = {}
self._composite_type = None
self._hinge_position = None
def __str__(self):
shape_description = self._cross_section if self._cross_section else self._second_moment
str_sol = 'Beam({}, {}, {})'.format(sstr(self._length), sstr(self._elastic_modulus), sstr(shape_description))
return str_sol
@property
def reaction_loads(self):
""" Returns the reaction forces in a dictionary."""
return self._reaction_loads
@property
def length(self):
"""Length of the Beam."""
return self._length
@length.setter
def length(self, l):
self._length = sympify(l)
@property
def variable(self):
"""
A symbol that can be used as a variable along the length of the beam
while representing load distribution, shear force curve, bending
moment, slope curve and the deflection curve. By default, it is set
to ``Symbol('x')``, but this property is mutable.
Examples
========
>>> from sympy.physics.continuum_mechanics.beam import Beam
>>> from sympy import symbols
>>> E, I = symbols('E, I')
>>> x, y, z = symbols('x, y, z')
>>> b = Beam(4, E, I)
>>> b.variable
x
>>> b.variable = y
>>> b.variable
y
>>> b = Beam(4, E, I, z)
>>> b.variable
z
"""
return self._variable
@variable.setter
def variable(self, v):
if isinstance(v, Symbol):
self._variable = v
else:
raise TypeError("""The variable should be a Symbol object.""")
@property
def elastic_modulus(self):
"""Young's Modulus of the Beam. """
return self._elastic_modulus
@elastic_modulus.setter
def elastic_modulus(self, e):
self._elastic_modulus = sympify(e)
@property
def second_moment(self):
"""Second moment of area of the Beam. """
return self._second_moment
@second_moment.setter
def second_moment(self, i):
self._cross_section = None
if isinstance(i, GeometryEntity):
raise ValueError("To update cross-section geometry use `cross_section` attribute")
else:
self._second_moment = sympify(i)
@property
def cross_section(self):
"""Cross-section of the beam"""
return self._cross_section
@cross_section.setter
def cross_section(self, s):
if s:
self._second_moment = s.second_moment_of_area()[0]
self._cross_section = s
@property
def boundary_conditions(self):
"""
Returns a dictionary of boundary conditions applied on the beam.
The dictionary has three keywords namely moment, slope and deflection.
The value of each keyword is a list of tuple, where each tuple
contains location and value of a boundary condition in the format
(location, value).
Examples
========
There is a beam of length 4 meters. The bending moment at 0 should be 4
and at 4 it should be 0. The slope of the beam should be 1 at 0. The
deflection should be 2 at 0.
>>> from sympy.physics.continuum_mechanics.beam import Beam
>>> from sympy import symbols
>>> E, I = symbols('E, I')
>>> b = Beam(4, E, I)
>>> b.bc_deflection = [(0, 2)]
>>> b.bc_slope = [(0, 1)]
>>> b.boundary_conditions
{'deflection': [(0, 2)], 'slope': [(0, 1)]}
Here the deflection of the beam should be ``2`` at ``0``.
Similarly, the slope of the beam should be ``1`` at ``0``.
"""
return self._boundary_conditions
@property
def bc_slope(self):
return self._boundary_conditions['slope']
@bc_slope.setter
def bc_slope(self, s_bcs):
self._boundary_conditions['slope'] = s_bcs
@property
def bc_deflection(self):
return self._boundary_conditions['deflection']
@bc_deflection.setter
def bc_deflection(self, d_bcs):
self._boundary_conditions['deflection'] = d_bcs
def join(self, beam, via="fixed"):
"""
This method joins two beams to make a new composite beam system.
Passed Beam class instance is attached to the right end of calling
object. This method can be used to form beams having Discontinuous
values of Elastic modulus or Second moment.
Parameters
==========
beam : Beam class object
The Beam object which would be connected to the right of calling
object.
via : String
States the way two Beam object would get connected
- For axially fixed Beams, via="fixed"
- For Beams connected via hinge, via="hinge"
Examples
========
There is a cantilever beam of length 4 meters. For first 2 meters
its moment of inertia is `1.5*I` and `I` for the other end.
A pointload of magnitude 4 N is applied from the top at its free end.
>>> from sympy.physics.continuum_mechanics.beam import Beam
>>> from sympy import symbols
>>> E, I = symbols('E, I')
>>> R1, R2 = symbols('R1, R2')
>>> b1 = Beam(2, E, 1.5*I)
>>> b2 = Beam(2, E, I)
>>> b = b1.join(b2, "fixed")
>>> b.apply_load(20, 4, -1)
>>> b.apply_load(R1, 0, -1)
>>> b.apply_load(R2, 0, -2)
>>> b.bc_slope = [(0, 0)]
>>> b.bc_deflection = [(0, 0)]
>>> b.solve_for_reaction_loads(R1, R2)
>>> b.load
80*SingularityFunction(x, 0, -2) - 20*SingularityFunction(x, 0, -1) + 20*SingularityFunction(x, 4, -1)
>>> b.slope()
(((80*SingularityFunction(x, 0, 1) - 10*SingularityFunction(x, 0, 2) + 10*SingularityFunction(x, 4, 2))/I - 120/I)/E + 80.0/(E*I))*SingularityFunction(x, 2, 0)
+ 0.666666666666667*(80*SingularityFunction(x, 0, 1) - 10*SingularityFunction(x, 0, 2) + 10*SingularityFunction(x, 4, 2))*SingularityFunction(x, 0, 0)/(E*I)
- 0.666666666666667*(80*SingularityFunction(x, 0, 1) - 10*SingularityFunction(x, 0, 2) + 10*SingularityFunction(x, 4, 2))*SingularityFunction(x, 2, 0)/(E*I)
"""
x = self.variable
E = self.elastic_modulus
new_length = self.length + beam.length
if self.second_moment != beam.second_moment:
new_second_moment = Piecewise((self.second_moment, x<=self.length),
(beam.second_moment, x<=new_length))
else:
new_second_moment = self.second_moment
if via == "fixed":
new_beam = Beam(new_length, E, new_second_moment, x)
new_beam._composite_type = "fixed"
return new_beam
if via == "hinge":
new_beam = Beam(new_length, E, new_second_moment, x)
new_beam._composite_type = "hinge"
new_beam._hinge_position = self.length
return new_beam
def apply_support(self, loc, type="fixed"):
"""
This method applies support to a particular beam object.
Parameters
==========
loc : Sympifyable
Location of point at which support is applied.
type : String
Determines type of Beam support applied. To apply support structure
with
- zero degree of freedom, type = "fixed"
- one degree of freedom, type = "pin"
- two degrees of freedom, type = "roller"
Examples
========
There is a beam of length 30 meters. A moment of magnitude 120 Nm is
applied in the clockwise direction at the end of the beam. A pointload
of magnitude 8 N is applied from the top of the beam at the starting
point. There are two simple supports below the beam. One at the end
and another one at a distance of 10 meters from the start. The
deflection is restricted at both the supports.
Using the sign convention of upward forces and clockwise moment
being positive.
>>> from sympy.physics.continuum_mechanics.beam import Beam
>>> from sympy import symbols
>>> E, I = symbols('E, I')
>>> b = Beam(30, E, I)
>>> b.apply_support(10, 'roller')
>>> b.apply_support(30, 'roller')
>>> b.apply_load(-8, 0, -1)
>>> b.apply_load(120, 30, -2)
>>> R_10, R_30 = symbols('R_10, R_30')
>>> b.solve_for_reaction_loads(R_10, R_30)
>>> b.load
-8*SingularityFunction(x, 0, -1) + 6*SingularityFunction(x, 10, -1)
+ 120*SingularityFunction(x, 30, -2) + 2*SingularityFunction(x, 30, -1)
>>> b.slope()
(-4*SingularityFunction(x, 0, 2) + 3*SingularityFunction(x, 10, 2)
+ 120*SingularityFunction(x, 30, 1) + SingularityFunction(x, 30, 2) + 4000/3)/(E*I)
"""
loc = sympify(loc)
self._applied_supports.append((loc, type))
if type == "pin" or type == "roller":
reaction_load = Symbol('R_'+str(loc))
self.apply_load(reaction_load, loc, -1)
self.bc_deflection.append((loc, 0))
else:
reaction_load = Symbol('R_'+str(loc))
reaction_moment = Symbol('M_'+str(loc))
self.apply_load(reaction_load, loc, -1)
self.apply_load(reaction_moment, loc, -2)
self.bc_deflection.append((loc, 0))
self.bc_slope.append((loc, 0))
self._support_as_loads.append((reaction_moment, loc, -2, None))
self._support_as_loads.append((reaction_load, loc, -1, None))
def apply_load(self, value, start, order, end=None):
"""
This method adds up the loads given to a particular beam object.
Parameters
==========
value : Sympifyable
The magnitude of an applied load.
start : Sympifyable
The starting point of the applied load. For point moments and
point forces this is the location of application.
order : Integer
The order of the applied load.
- For moments, order = -2
- For point loads, order =-1
- For constant distributed load, order = 0
- For ramp loads, order = 1
- For parabolic ramp loads, order = 2
- ... so on.
end : Sympifyable, optional
An optional argument that can be used if the load has an end point
within the length of the beam.
Examples
========
There is a beam of length 4 meters. A moment of magnitude 3 Nm is
applied in the clockwise direction at the starting point of the beam.
A point load of magnitude 4 N is applied from the top of the beam at
2 meters from the starting point and a parabolic ramp load of magnitude
2 N/m is applied below the beam starting from 2 meters to 3 meters
away from the starting point of the beam.
>>> from sympy.physics.continuum_mechanics.beam import Beam
>>> from sympy import symbols
>>> E, I = symbols('E, I')
>>> b = Beam(4, E, I)
>>> b.apply_load(-3, 0, -2)
>>> b.apply_load(4, 2, -1)
>>> b.apply_load(-2, 2, 2, end=3)
>>> b.load
-3*SingularityFunction(x, 0, -2) + 4*SingularityFunction(x, 2, -1) - 2*SingularityFunction(x, 2, 2) + 2*SingularityFunction(x, 3, 0) + 4*SingularityFunction(x, 3, 1) + 2*SingularityFunction(x, 3, 2)
"""
x = self.variable
value = sympify(value)
start = sympify(start)
order = sympify(order)
self._applied_loads.append((value, start, order, end))
self._load += value*SingularityFunction(x, start, order)
if end:
if order.is_negative:
msg = ("If 'end' is provided the 'order' of the load cannot "
"be negative, i.e. 'end' is only valid for distributed "
"loads.")
raise ValueError(msg)
# NOTE : A Taylor series can be used to define the summation of
# singularity functions that subtract from the load past the end
# point such that it evaluates to zero past 'end'.
f = value * x**order
for i in range(0, order + 1):
self._load -= (f.diff(x, i).subs(x, end - start) *
SingularityFunction(x, end, i) / factorial(i))
def remove_load(self, value, start, order, end=None):
"""
This method removes a particular load present on the beam object.
Returns a ValueError if the load passed as an argument is not
present on the beam.
Parameters
==========
value : Sympifyable
The magnitude of an applied load.
start : Sympifyable
The starting point of the applied load. For point moments and
point forces this is the location of application.
order : Integer
The order of the applied load.
- For moments, order= -2
- For point loads, order=-1
- For constant distributed load, order=0
- For ramp loads, order=1
- For parabolic ramp loads, order=2
- ... so on.
end : Sympifyable, optional
An optional argument that can be used if the load has an end point
within the length of the beam.
Examples
========
There is a beam of length 4 meters. A moment of magnitude 3 Nm is
applied in the clockwise direction at the starting point of the beam.
A pointload of magnitude 4 N is applied from the top of the beam at
2 meters from the starting point and a parabolic ramp load of magnitude
2 N/m is applied below the beam starting from 2 meters to 3 meters
away from the starting point of the beam.
>>> from sympy.physics.continuum_mechanics.beam import Beam
>>> from sympy import symbols
>>> E, I = symbols('E, I')
>>> b = Beam(4, E, I)
>>> b.apply_load(-3, 0, -2)
>>> b.apply_load(4, 2, -1)
>>> b.apply_load(-2, 2, 2, end=3)
>>> b.load
-3*SingularityFunction(x, 0, -2) + 4*SingularityFunction(x, 2, -1) - 2*SingularityFunction(x, 2, 2) + 2*SingularityFunction(x, 3, 0) + 4*SingularityFunction(x, 3, 1) + 2*SingularityFunction(x, 3, 2)
>>> b.remove_load(-2, 2, 2, end = 3)
>>> b.load
-3*SingularityFunction(x, 0, -2) + 4*SingularityFunction(x, 2, -1)
"""
x = self.variable
value = sympify(value)
start = sympify(start)
order = sympify(order)
if (value, start, order, end) in self._applied_loads:
self._load -= value*SingularityFunction(x, start, order)
self._applied_loads.remove((value, start, order, end))
else:
msg = "No such load distribution exists on the beam object."
raise ValueError(msg)
if end:
# TODO : This is essentially duplicate code wrt to apply_load,
# would be better to move it to one location and both methods use
# it.
if order.is_negative:
msg = ("If 'end' is provided the 'order' of the load cannot "
"be negative, i.e. 'end' is only valid for distributed "
"loads.")
raise ValueError(msg)
# NOTE : A Taylor series can be used to define the summation of
# singularity functions that subtract from the load past the end
# point such that it evaluates to zero past 'end'.
f = value * x**order
for i in range(0, order + 1):
self._load += (f.diff(x, i).subs(x, end - start) *
SingularityFunction(x, end, i) / factorial(i))
@property
def load(self):
"""
Returns a Singularity Function expression which represents
the load distribution curve of the Beam object.
Examples
========
There is a beam of length 4 meters. A moment of magnitude 3 Nm is
applied in the clockwise direction at the starting point of the beam.
A point load of magnitude 4 N is applied from the top of the beam at
2 meters from the starting point and a parabolic ramp load of magnitude
2 N/m is applied below the beam starting from 3 meters away from the
starting point of the beam.
>>> from sympy.physics.continuum_mechanics.beam import Beam
>>> from sympy import symbols
>>> E, I = symbols('E, I')
>>> b = Beam(4, E, I)
>>> b.apply_load(-3, 0, -2)
>>> b.apply_load(4, 2, -1)
>>> b.apply_load(-2, 3, 2)
>>> b.load
-3*SingularityFunction(x, 0, -2) + 4*SingularityFunction(x, 2, -1) - 2*SingularityFunction(x, 3, 2)
"""
return self._load
@property
def applied_loads(self):
"""
Returns a list of all loads applied on the beam object.
Each load in the list is a tuple of form (value, start, order, end).
Examples
========
There is a beam of length 4 meters. A moment of magnitude 3 Nm is
applied in the clockwise direction at the starting point of the beam.
A pointload of magnitude 4 N is applied from the top of the beam at
2 meters from the starting point. Another pointload of magnitude 5 N
is applied at same position.
>>> from sympy.physics.continuum_mechanics.beam import Beam
>>> from sympy import symbols
>>> E, I = symbols('E, I')
>>> b = Beam(4, E, I)
>>> b.apply_load(-3, 0, -2)
>>> b.apply_load(4, 2, -1)
>>> b.apply_load(5, 2, -1)
>>> b.load
-3*SingularityFunction(x, 0, -2) + 9*SingularityFunction(x, 2, -1)
>>> b.applied_loads
[(-3, 0, -2, None), (4, 2, -1, None), (5, 2, -1, None)]
"""
return self._applied_loads
def _solve_hinge_beams(self, *reactions):
"""Method to find integration constants and reactional variables in a
composite beam connected via hinge.
This method resolves the composite Beam into its sub-beams and then
equations of shear force, bending moment, slope and deflection are
evaluated for both of them separately. These equations are then solved
for unknown reactions and integration constants using the boundary
conditions applied on the Beam. Equal deflection of both sub-beams
at the hinge joint gives us another equation to solve the system.
Examples
========
A combined beam, with constant fkexural rigidity E*I, is formed by joining
a Beam of length 2*l to the right of another Beam of length l. The whole beam
is fixed at both of its both end. A point load of magnitude P is also applied
from the top at a distance of 2*l from starting point.
>>> from sympy.physics.continuum_mechanics.beam import Beam
>>> from sympy import symbols
>>> E, I = symbols('E, I')
>>> l=symbols('l', positive=True)
>>> b1=Beam(l ,E,I)
>>> b2=Beam(2*l ,E,I)
>>> b=b1.join(b2,"hinge")
>>> M1, A1, M2, A2, P = symbols('M1 A1 M2 A2 P')
>>> b.apply_load(A1,0,-1)
>>> b.apply_load(M1,0,-2)
>>> b.apply_load(P,2*l,-1)
>>> b.apply_load(A2,3*l,-1)
>>> b.apply_load(M2,3*l,-2)
>>> b.bc_slope=[(0,0), (3*l, 0)]
>>> b.bc_deflection=[(0,0), (3*l, 0)]
>>> b.solve_for_reaction_loads(M1, A1, M2, A2)
>>> b.reaction_loads
{A1: -5*P/18, A2: -13*P/18, M1: 5*P*l/18, M2: -4*P*l/9}
>>> b.slope()
(5*P*l*SingularityFunction(x, 0, 1)/18 - 5*P*SingularityFunction(x, 0, 2)/36 + 5*P*SingularityFunction(x, l, 2)/36)*SingularityFunction(x, 0, 0)/(E*I)
- (5*P*l*SingularityFunction(x, 0, 1)/18 - 5*P*SingularityFunction(x, 0, 2)/36 + 5*P*SingularityFunction(x, l, 2)/36)*SingularityFunction(x, l, 0)/(E*I)
+ (P*l**2/18 - 4*P*l*SingularityFunction(-l + x, 2*l, 1)/9 - 5*P*SingularityFunction(-l + x, 0, 2)/36 + P*SingularityFunction(-l + x, l, 2)/2
- 13*P*SingularityFunction(-l + x, 2*l, 2)/36)*SingularityFunction(x, l, 0)/(E*I)
>>> b.deflection()
(5*P*l*SingularityFunction(x, 0, 2)/36 - 5*P*SingularityFunction(x, 0, 3)/108 + 5*P*SingularityFunction(x, l, 3)/108)*SingularityFunction(x, 0, 0)/(E*I)
- (5*P*l*SingularityFunction(x, 0, 2)/36 - 5*P*SingularityFunction(x, 0, 3)/108 + 5*P*SingularityFunction(x, l, 3)/108)*SingularityFunction(x, l, 0)/(E*I)
+ (5*P*l**3/54 + P*l**2*(-l + x)/18 - 2*P*l*SingularityFunction(-l + x, 2*l, 2)/9 - 5*P*SingularityFunction(-l + x, 0, 3)/108 + P*SingularityFunction(-l + x, l, 3)/6
- 13*P*SingularityFunction(-l + x, 2*l, 3)/108)*SingularityFunction(x, l, 0)/(E*I)
"""
x = self.variable
l = self._hinge_position
E = self._elastic_modulus
I = self._second_moment
if isinstance(I, Piecewise):
I1 = I.args[0][0]
I2 = I.args[1][0]
else:
I1 = I2 = I
load_1 = 0 # Load equation on first segment of composite beam
load_2 = 0 # Load equation on second segment of composite beam
# Distributing load on both segments
for load in self.applied_loads:
if load[1] < l:
load_1 += load[0]*SingularityFunction(x, load[1], load[2])
if load[2] == 0:
load_1 -= load[0]*SingularityFunction(x, load[3], load[2])
elif load[2] > 0:
load_1 -= load[0]*SingularityFunction(x, load[3], load[2]) + load[0]*SingularityFunction(x, load[3], 0)
elif load[1] == l:
load_1 += load[0]*SingularityFunction(x, load[1], load[2])
load_2 += load[0]*SingularityFunction(x, load[1] - l, load[2])
elif load[1] > l:
load_2 += load[0]*SingularityFunction(x, load[1] - l, load[2])
if load[2] == 0:
load_2 -= load[0]*SingularityFunction(x, load[3] - l, load[2])
elif load[2] > 0:
load_2 -= load[0]*SingularityFunction(x, load[3] - l, load[2]) + load[0]*SingularityFunction(x, load[3] - l, 0)
h = Symbol('h') # Force due to hinge
load_1 += h*SingularityFunction(x, l, -1)
load_2 -= h*SingularityFunction(x, 0, -1)
eq = []
shear_1 = integrate(load_1, x)
shear_curve_1 = limit(shear_1, x, l)
eq.append(shear_curve_1)
bending_1 = integrate(shear_1, x)
moment_curve_1 = limit(bending_1, x, l)
eq.append(moment_curve_1)
shear_2 = integrate(load_2, x)
shear_curve_2 = limit(shear_2, x, self.length - l)
eq.append(shear_curve_2)
bending_2 = integrate(shear_2, x)
moment_curve_2 = limit(bending_2, x, self.length - l)
eq.append(moment_curve_2)
C1 = Symbol('C1')
C2 = Symbol('C2')
C3 = Symbol('C3')
C4 = Symbol('C4')
slope_1 = S(1)/(E*I1)*(integrate(bending_1, x) + C1)
def_1 = S(1)/(E*I1)*(integrate((E*I)*slope_1, x) + C1*x + C2)
slope_2 = S(1)/(E*I2)*(integrate(integrate(integrate(load_2, x), x), x) + C3)
def_2 = S(1)/(E*I2)*(integrate((E*I)*slope_2, x) + C4)
for position, value in self.bc_slope:
if position<l:
eq.append(slope_1.subs(x, position) - value)
else:
eq.append(slope_2.subs(x, position - l) - value)
for position, value in self.bc_deflection:
if position<l:
eq.append(def_1.subs(x, position) - value)
else:
eq.append(def_2.subs(x, position - l) - value)
eq.append(def_1.subs(x, l) - def_2.subs(x, 0)) # Deflection of both the segments at hinge would be equal
constants = list(linsolve(eq, C1, C2, C3, C4, h, *reactions))
reaction_values = list(constants[0])[5:]
self._reaction_loads = dict(zip(reactions, reaction_values))
self._load = self._load.subs(self._reaction_loads)
# Substituting constants and reactional load and moments with their corresponding values
slope_1 = slope_1.subs({C1: constants[0][0], h:constants[0][4]}).subs(self._reaction_loads)
def_1 = def_1.subs({C1: constants[0][0], C2: constants[0][1], h:constants[0][4]}).subs(self._reaction_loads)
slope_2 = slope_2.subs({x: x-l, C3: constants[0][2], h:constants[0][4]}).subs(self._reaction_loads)
def_2 = def_2.subs({x: x-l,C3: constants[0][2], C4: constants[0][3], h:constants[0][4]}).subs(self._reaction_loads)
self._hinge_beam_slope = slope_1*SingularityFunction(x, 0, 0) - slope_1*SingularityFunction(x, l, 0) + slope_2*SingularityFunction(x, l, 0)
self._hinge_beam_deflection = def_1*SingularityFunction(x, 0, 0) - def_1*SingularityFunction(x, l, 0) + def_2*SingularityFunction(x, l, 0)
def solve_for_reaction_loads(self, *reactions):
"""
Solves for the reaction forces.
Examples
========
There is a beam of length 30 meters. A moment of magnitude 120 Nm is
applied in the clockwise direction at the end of the beam. A pointload
of magnitude 8 N is applied from the top of the beam at the starting
point. There are two simple supports below the beam. One at the end
and another one at a distance of 10 meters from the start. The
deflection is restricted at both the supports.
Using the sign convention of upward forces and clockwise moment
being positive.
>>> from sympy.physics.continuum_mechanics.beam import Beam
>>> from sympy import symbols, linsolve, limit
>>> E, I = symbols('E, I')
>>> R1, R2 = symbols('R1, R2')
>>> b = Beam(30, E, I)
>>> b.apply_load(-8, 0, -1)
>>> b.apply_load(R1, 10, -1) # Reaction force at x = 10
>>> b.apply_load(R2, 30, -1) # Reaction force at x = 30
>>> b.apply_load(120, 30, -2)
>>> b.bc_deflection = [(10, 0), (30, 0)]
>>> b.load
R1*SingularityFunction(x, 10, -1) + R2*SingularityFunction(x, 30, -1)
- 8*SingularityFunction(x, 0, -1) + 120*SingularityFunction(x, 30, -2)
>>> b.solve_for_reaction_loads(R1, R2)
>>> b.reaction_loads
{R1: 6, R2: 2}
>>> b.load
-8*SingularityFunction(x, 0, -1) + 6*SingularityFunction(x, 10, -1)
+ 120*SingularityFunction(x, 30, -2) + 2*SingularityFunction(x, 30, -1)
"""
if self._composite_type == "hinge":
return self._solve_hinge_beams(*reactions)
x = self.variable
l = self.length
C3 = Symbol('C3')
C4 = Symbol('C4')
shear_curve = limit(self.shear_force(), x, l)
moment_curve = limit(self.bending_moment(), x, l)
slope_eqs = []
deflection_eqs = []
slope_curve = integrate(self.bending_moment(), x) + C3
for position, value in self._boundary_conditions['slope']:
eqs = slope_curve.subs(x, position) - value
slope_eqs.append(eqs)
deflection_curve = integrate(slope_curve, x) + C4
for position, value in self._boundary_conditions['deflection']:
eqs = deflection_curve.subs(x, position) - value
deflection_eqs.append(eqs)
solution = list((linsolve([shear_curve, moment_curve] + slope_eqs
+ deflection_eqs, (C3, C4) + reactions).args)[0])
solution = solution[2:]
self._reaction_loads = dict(zip(reactions, solution))
self._load = self._load.subs(self._reaction_loads)
def shear_force(self):
"""
Returns a Singularity Function expression which represents
the shear force curve of the Beam object.
Examples
========
There is a beam of length 30 meters. A moment of magnitude 120 Nm is
applied in the clockwise direction at the end of the beam. A pointload
of magnitude 8 N is applied from the top of the beam at the starting
point. There are two simple supports below the beam. One at the end
and another one at a distance of 10 meters from the start. The
deflection is restricted at both the supports.
Using the sign convention of upward forces and clockwise moment
being positive.
>>> from sympy.physics.continuum_mechanics.beam import Beam
>>> from sympy import symbols
>>> E, I = symbols('E, I')
>>> R1, R2 = symbols('R1, R2')
>>> b = Beam(30, E, I)
>>> b.apply_load(-8, 0, -1)
>>> b.apply_load(R1, 10, -1)
>>> b.apply_load(R2, 30, -1)
>>> b.apply_load(120, 30, -2)
>>> b.bc_deflection = [(10, 0), (30, 0)]
>>> b.solve_for_reaction_loads(R1, R2)
>>> b.shear_force()
-8*SingularityFunction(x, 0, 0) + 6*SingularityFunction(x, 10, 0) + 120*SingularityFunction(x, 30, -1) + 2*SingularityFunction(x, 30, 0)
"""
x = self.variable
return integrate(self.load, x)
def max_shear_force(self):
"""Returns maximum Shear force and its coordinate
in the Beam object."""
from sympy import solve, Mul, Interval
shear_curve = self.shear_force()
x = self.variable
terms = shear_curve.args
singularity = [] # Points at which shear function changes
for term in terms:
if isinstance(term, Mul):
term = term.args[-1] # SingularityFunction in the term
singularity.append(term.args[1])
singularity.sort()
singularity = list(set(singularity))
intervals = [] # List of Intervals with discrete value of shear force
shear_values = [] # List of values of shear force in each interval
for i, s in enumerate(singularity):
if s == 0:
continue
try:
shear_slope = Piecewise((float("nan"), x<=singularity[i-1]),(self._load.rewrite(Piecewise), x<s), (float("nan"), True))
points = solve(shear_slope, x)
val = []
for point in points:
val.append(shear_curve.subs(x, point))
points.extend([singularity[i-1], s])
val.extend([limit(shear_curve, x, singularity[i-1], '+'), limit(shear_curve, x, s, '-')])
val = list(map(abs, val))
max_shear = max(val)
shear_values.append(max_shear)
intervals.append(points[val.index(max_shear)])
# If shear force in a particular Interval has zero or constant
# slope, then above block gives NotImplementedError as
# solve can't represent Interval solutions.
except NotImplementedError:
initial_shear = limit(shear_curve, x, singularity[i-1], '+')
final_shear = limit(shear_curve, x, s, '-')
# If shear_curve has a constant slope(it is a line).
if shear_curve.subs(x, (singularity[i-1] + s)/2) == (initial_shear + final_shear)/2 and initial_shear != final_shear:
shear_values.extend([initial_shear, final_shear])
intervals.extend([singularity[i-1], s])
else: # shear_curve has same value in whole Interval
shear_values.append(final_shear)
intervals.append(Interval(singularity[i-1], s))
shear_values = list(map(abs, shear_values))
maximum_shear = max(shear_values)
point = intervals[shear_values.index(maximum_shear)]
return (point, maximum_shear)
def bending_moment(self):
"""
Returns a Singularity Function expression which represents
the bending moment curve of the Beam object.
Examples
========
There is a beam of length 30 meters. A moment of magnitude 120 Nm is
applied in the clockwise direction at the end of the beam. A pointload
of magnitude 8 N is applied from the top of the beam at the starting
point. There are two simple supports below the beam. One at the end
and another one at a distance of 10 meters from the start. The
deflection is restricted at both the supports.
Using the sign convention of upward forces and clockwise moment
being positive.
>>> from sympy.physics.continuum_mechanics.beam import Beam
>>> from sympy import symbols
>>> E, I = symbols('E, I')
>>> R1, R2 = symbols('R1, R2')
>>> b = Beam(30, E, I)
>>> b.apply_load(-8, 0, -1)
>>> b.apply_load(R1, 10, -1)
>>> b.apply_load(R2, 30, -1)
>>> b.apply_load(120, 30, -2)
>>> b.bc_deflection = [(10, 0), (30, 0)]
>>> b.solve_for_reaction_loads(R1, R2)
>>> b.bending_moment()
-8*SingularityFunction(x, 0, 1) + 6*SingularityFunction(x, 10, 1) + 120*SingularityFunction(x, 30, 0) + 2*SingularityFunction(x, 30, 1)
"""
x = self.variable
return integrate(self.shear_force(), x)
def max_bmoment(self):
"""Returns maximum Shear force and its coordinate
in the Beam object."""
from sympy import solve, Mul, Interval
bending_curve = self.bending_moment()
x = self.variable
terms = bending_curve.args
singularity = [] # Points at which bending moment changes
for term in terms:
if isinstance(term, Mul):
term = term.args[-1] # SingularityFunction in the term
singularity.append(term.args[1])
singularity.sort()
singularity = list(set(singularity))
intervals = [] # List of Intervals with discrete value of bending moment
moment_values = [] # List of values of bending moment in each interval
for i, s in enumerate(singularity):
if s == 0:
continue
try:
moment_slope = Piecewise((float("nan"), x<=singularity[i-1]),(self.shear_force().rewrite(Piecewise), x<s), (float("nan"), True))
points = solve(moment_slope, x)
val = []
for point in points:
val.append(bending_curve.subs(x, point))
points.extend([singularity[i-1], s])
val.extend([limit(bending_curve, x, singularity[i-1], '+'), limit(bending_curve, x, s, '-')])
val = list(map(abs, val))
max_moment = max(val)
moment_values.append(max_moment)
intervals.append(points[val.index(max_moment)])
# If bending moment in a particular Interval has zero or constant
# slope, then above block gives NotImplementedError as solve
# can't represent Interval solutions.
except NotImplementedError:
initial_moment = limit(bending_curve, x, singularity[i-1], '+')
final_moment = limit(bending_curve, x, s, '-')
# If bending_curve has a constant slope(it is a line).
if bending_curve.subs(x, (singularity[i-1] + s)/2) == (initial_moment + final_moment)/2 and initial_moment != final_moment:
moment_values.extend([initial_moment, final_moment])
intervals.extend([singularity[i-1], s])
else: # bending_curve has same value in whole Interval
moment_values.append(final_moment)
intervals.append(Interval(singularity[i-1], s))
moment_values = list(map(abs, moment_values))
maximum_moment = max(moment_values)
point = intervals[moment_values.index(maximum_moment)]
return (point, maximum_moment)
def point_cflexure(self):
"""
Returns a Set of point(s) with zero bending moment and
where bending moment curve of the beam object changes
its sign from negative to positive or vice versa.
Examples
========
There is is 10 meter long overhanging beam. There are
two simple supports below the beam. One at the start
and another one at a distance of 6 meters from the start.
Point loads of magnitude 10KN and 20KN are applied at
2 meters and 4 meters from start respectively. A Uniformly
distribute load of magnitude of magnitude 3KN/m is also
applied on top starting from 6 meters away from starting
point till end.
Using the sign convention of upward forces and clockwise moment
being positive.
>>> from sympy.physics.continuum_mechanics.beam import Beam
>>> from sympy import symbols
>>> E, I = symbols('E, I')
>>> b = Beam(10, E, I)
>>> b.apply_load(-4, 0, -1)
>>> b.apply_load(-46, 6, -1)
>>> b.apply_load(10, 2, -1)
>>> b.apply_load(20, 4, -1)
>>> b.apply_load(3, 6, 0)
>>> b.point_cflexure()
[10/3]
"""
from sympy import solve, Piecewise
# To restrict the range within length of the Beam
moment_curve = Piecewise((float("nan"), self.variable<=0),
(self.bending_moment(), self.variable<self.length),
(float("nan"), True))
points = solve(moment_curve.rewrite(Piecewise), self.variable,
domain=S.Reals)
return points
def slope(self):
"""
Returns a Singularity Function expression which represents
the slope the elastic curve of the Beam object.
Examples
========
There is a beam of length 30 meters. A moment of magnitude 120 Nm is
applied in the clockwise direction at the end of the beam. A pointload
of magnitude 8 N is applied from the top of the beam at the starting
point. There are two simple supports below the beam. One at the end
and another one at a distance of 10 meters from the start. The
deflection is restricted at both the supports.
Using the sign convention of upward forces and clockwise moment
being positive.
>>> from sympy.physics.continuum_mechanics.beam import Beam
>>> from sympy import symbols
>>> E, I = symbols('E, I')
>>> R1, R2 = symbols('R1, R2')
>>> b = Beam(30, E, I)
>>> b.apply_load(-8, 0, -1)
>>> b.apply_load(R1, 10, -1)
>>> b.apply_load(R2, 30, -1)
>>> b.apply_load(120, 30, -2)
>>> b.bc_deflection = [(10, 0), (30, 0)]
>>> b.solve_for_reaction_loads(R1, R2)
>>> b.slope()
(-4*SingularityFunction(x, 0, 2) + 3*SingularityFunction(x, 10, 2)
+ 120*SingularityFunction(x, 30, 1) + SingularityFunction(x, 30, 2) + 4000/3)/(E*I)
"""
x = self.variable
E = self.elastic_modulus
I = self.second_moment
if self._composite_type == "hinge":
return self._hinge_beam_slope
if not self._boundary_conditions['slope']:
return diff(self.deflection(), x)
if isinstance(I, Piecewise) and self._composite_type == "fixed":
args = I.args
slope = 0
prev_slope = 0
prev_end = 0
for i in range(len(args)):
if i != 0:
prev_end = args[i-1][1].args[1]
slope_value = S(1)/E*integrate(self.bending_moment()/args[i][0], (x, prev_end, x))
if i != len(args) - 1:
slope += (prev_slope + slope_value)*SingularityFunction(x, prev_end, 0) - \
(prev_slope + slope_value)*SingularityFunction(x, args[i][1].args[1], 0)
else:
slope += (prev_slope + slope_value)*SingularityFunction(x, prev_end, 0)
prev_slope = slope_value.subs(x, args[i][1].args[1])
return slope
C3 = Symbol('C3')
slope_curve = integrate(S(1)/(E*I)*self.bending_moment(), x) + C3
bc_eqs = []
for position, value in self._boundary_conditions['slope']:
eqs = slope_curve.subs(x, position) - value
bc_eqs.append(eqs)
constants = list(linsolve(bc_eqs, C3))
slope_curve = slope_curve.subs({C3: constants[0][0]})
return slope_curve
def deflection(self):
"""
Returns a Singularity Function expression which represents
the elastic curve or deflection of the Beam object.
Examples
========
There is a beam of length 30 meters. A moment of magnitude 120 Nm is
applied in the clockwise direction at the end of the beam. A pointload
of magnitude 8 N is applied from the top of the beam at the starting
point. There are two simple supports below the beam. One at the end
and another one at a distance of 10 meters from the start. The
deflection is restricted at both the supports.
Using the sign convention of upward forces and clockwise moment
being positive.
>>> from sympy.physics.continuum_mechanics.beam import Beam
>>> from sympy import symbols
>>> E, I = symbols('E, I')
>>> R1, R2 = symbols('R1, R2')
>>> b = Beam(30, E, I)
>>> b.apply_load(-8, 0, -1)
>>> b.apply_load(R1, 10, -1)
>>> b.apply_load(R2, 30, -1)
>>> b.apply_load(120, 30, -2)
>>> b.bc_deflection = [(10, 0), (30, 0)]
>>> b.solve_for_reaction_loads(R1, R2)
>>> b.deflection()
(4000*x/3 - 4*SingularityFunction(x, 0, 3)/3 + SingularityFunction(x, 10, 3)
+ 60*SingularityFunction(x, 30, 2) + SingularityFunction(x, 30, 3)/3 - 12000)/(E*I)
"""
x = self.variable
E = self.elastic_modulus
I = self.second_moment
if self._composite_type == "hinge":
return self._hinge_beam_deflection
if not self._boundary_conditions['deflection'] and not self._boundary_conditions['slope']:
if isinstance(I, Piecewise) and self._composite_type == "fixed":
args = I.args
prev_slope = 0
prev_def = 0
prev_end = 0
deflection = 0
for i in range(len(args)):
if i != 0:
prev_end = args[i-1][1].args[1]
slope_value = S(1)/E*integrate(self.bending_moment()/args[i][0], (x, prev_end, x))
recent_segment_slope = prev_slope + slope_value
deflection_value = integrate(recent_segment_slope, (x, prev_end, x))
if i != len(args) - 1:
deflection += (prev_def + deflection_value)*SingularityFunction(x, prev_end, 0) \
- (prev_def + deflection_value)*SingularityFunction(x, args[i][1].args[1], 0)
else:
deflection += (prev_def + deflection_value)*SingularityFunction(x, prev_end, 0)
prev_slope = slope_value.subs(x, args[i][1].args[1])
prev_def = deflection_value.subs(x, args[i][1].args[1])
return deflection
base_char = self._base_char
constants = symbols(base_char + '3:5')
return S(1)/(E*I)*integrate(integrate(self.bending_moment(), x), x) + constants[0]*x + constants[1]
elif not self._boundary_conditions['deflection']:
base_char = self._base_char
constant = symbols(base_char + '4')
return integrate(self.slope(), x) + constant
elif not self._boundary_conditions['slope'] and self._boundary_conditions['deflection']:
if isinstance(I, Piecewise) and self._composite_type == "fixed":
args = I.args
prev_slope = 0
prev_def = 0
prev_end = 0
deflection = 0
for i in range(len(args)):
if i != 0:
prev_end = args[i-1][1].args[1]
slope_value = S(1)/E*integrate(self.bending_moment()/args[i][0], (x, prev_end, x))
recent_segment_slope = prev_slope + slope_value
deflection_value = integrate(recent_segment_slope, (x, prev_end, x))
if i != len(args) - 1:
deflection += (prev_def + deflection_value)*SingularityFunction(x, prev_end, 0) \
- (prev_def + deflection_value)*SingularityFunction(x, args[i][1].args[1], 0)
else:
deflection += (prev_def + deflection_value)*SingularityFunction(x, prev_end, 0)
prev_slope = slope_value.subs(x, args[i][1].args[1])
prev_def = deflection_value.subs(x, args[i][1].args[1])
return deflection
base_char = self._base_char
C3, C4 = symbols(base_char + '3:5') # Integration constants
slope_curve = integrate(self.bending_moment(), x) + C3
deflection_curve = integrate(slope_curve, x) + C4
bc_eqs = []
for position, value in self._boundary_conditions['deflection']:
eqs = deflection_curve.subs(x, position) - value
bc_eqs.append(eqs)
constants = list(linsolve(bc_eqs, (C3, C4)))
deflection_curve = deflection_curve.subs({C3: constants[0][0], C4: constants[0][1]})
return S(1)/(E*I)*deflection_curve
if isinstance(I, Piecewise) and self._composite_type == "fixed":
args = I.args
prev_slope = 0
prev_def = 0
prev_end = 0
deflection = 0
for i in range(len(args)):
if i != 0:
prev_end = args[i-1][1].args[1]
slope_value = S(1)/E*integrate(self.bending_moment()/args[i][0], (x, prev_end, x))
recent_segment_slope = prev_slope + slope_value
deflection_value = integrate(recent_segment_slope, (x, prev_end, x))
if i != len(args) - 1:
deflection += (prev_def + deflection_value)*SingularityFunction(x, prev_end, 0) \
- (prev_def + deflection_value)*SingularityFunction(x, args[i][1].args[1], 0)
else:
deflection += (prev_def + deflection_value)*SingularityFunction(x, prev_end, 0)
prev_slope = slope_value.subs(x, args[i][1].args[1])
prev_def = deflection_value.subs(x, args[i][1].args[1])
return deflection
C4 = Symbol('C4')
deflection_curve = integrate(self.slope(), x) + C4
bc_eqs = []
for position, value in self._boundary_conditions['deflection']:
eqs = deflection_curve.subs(x, position) - value
bc_eqs.append(eqs)
constants = list(linsolve(bc_eqs, C4))
deflection_curve = deflection_curve.subs({C4: constants[0][0]})
return deflection_curve
def max_deflection(self):
"""
Returns point of max deflection and its corresponding deflection value
in a Beam object.
"""
from sympy import solve, Piecewise
# To restrict the range within length of the Beam
slope_curve = Piecewise((float("nan"), self.variable<=0),
(self.slope(), self.variable<self.length),
(float("nan"), True))
points = solve(slope_curve.rewrite(Piecewise), self.variable,
domain=S.Reals)
deflection_curve = self.deflection()
deflections = [deflection_curve.subs(self.variable, x) for x in points]
deflections = list(map(abs, deflections))
if len(deflections) != 0:
max_def = max(deflections)
return (points[deflections.index(max_def)], max_def)
else:
return None
def plot_shear_force(self, subs=None):
"""
Returns a plot for Shear force present in the Beam object.
Parameters
==========
subs : dictionary
Python dictionary containing Symbols as key and their
corresponding values.
Examples
========
There is a beam of length 8 meters. A constant distributed load of 10 KN/m
is applied from half of the beam till the end. There are two simple supports
below the beam, one at the starting point and another at the ending point
of the beam. A pointload of magnitude 5 KN is also applied from top of the
beam, at a distance of 4 meters from the starting point.
Take E = 200 GPa and I = 400*(10**-6) meter**4.
Using the sign convention of downwards forces being positive.
.. plot::
:context: close-figs
:format: doctest
:include-source: True
>>> from sympy.physics.continuum_mechanics.beam import Beam
>>> from sympy import symbols
>>> R1, R2 = symbols('R1, R2')
>>> b = Beam(8, 200*(10**9), 400*(10**-6))
>>> b.apply_load(5000, 2, -1)
>>> b.apply_load(R1, 0, -1)
>>> b.apply_load(R2, 8, -1)
>>> b.apply_load(10000, 4, 0, end=8)
>>> b.bc_deflection = [(0, 0), (8, 0)]
>>> b.solve_for_reaction_loads(R1, R2)
>>> b.plot_shear_force()
Plot object containing:
[0]: cartesian line: -13750*SingularityFunction(x, 0, 0) + 5000*SingularityFunction(x, 2, 0)
+ 10000*SingularityFunction(x, 4, 1) - 31250*SingularityFunction(x, 8, 0)
- 10000*SingularityFunction(x, 8, 1) for x over (0.0, 8.0)
"""
shear_force = self.shear_force()
if subs is None:
subs = {}
for sym in shear_force.atoms(Symbol):
if sym == self.variable:
continue
if sym not in subs:
raise ValueError('Value of %s was not passed.' %sym)
if self.length in subs:
length = subs[self.length]
else:
length = self.length
return plot(shear_force.subs(subs), (self.variable, 0, length), title='Shear Force',
xlabel=r'$\mathrm{x}$', ylabel=r'$\mathrm{V}$', line_color='g')
def plot_bending_moment(self, subs=None):
"""
Returns a plot for Bending moment present in the Beam object.
Parameters
==========
subs : dictionary
Python dictionary containing Symbols as key and their
corresponding values.
Examples
========
There is a beam of length 8 meters. A constant distributed load of 10 KN/m
is applied from half of the beam till the end. There are two simple supports
below the beam, one at the starting point and another at the ending point
of the beam. A pointload of magnitude 5 KN is also applied from top of the
beam, at a distance of 4 meters from the starting point.
Take E = 200 GPa and I = 400*(10**-6) meter**4.
Using the sign convention of downwards forces being positive.
.. plot::
:context: close-figs
:format: doctest
:include-source: True
>>> from sympy.physics.continuum_mechanics.beam import Beam
>>> from sympy import symbols
>>> R1, R2 = symbols('R1, R2')
>>> b = Beam(8, 200*(10**9), 400*(10**-6))
>>> b.apply_load(5000, 2, -1)
>>> b.apply_load(R1, 0, -1)
>>> b.apply_load(R2, 8, -1)
>>> b.apply_load(10000, 4, 0, end=8)
>>> b.bc_deflection = [(0, 0), (8, 0)]
>>> b.solve_for_reaction_loads(R1, R2)
>>> b.plot_bending_moment()
Plot object containing:
[0]: cartesian line: -13750*SingularityFunction(x, 0, 1) + 5000*SingularityFunction(x, 2, 1)
+ 5000*SingularityFunction(x, 4, 2) - 31250*SingularityFunction(x, 8, 1)
- 5000*SingularityFunction(x, 8, 2) for x over (0.0, 8.0)
"""
bending_moment = self.bending_moment()
if subs is None:
subs = {}
for sym in bending_moment.atoms(Symbol):
if sym == self.variable:
continue
if sym not in subs:
raise ValueError('Value of %s was not passed.' %sym)
if self.length in subs:
length = subs[self.length]
else:
length = self.length
return plot(bending_moment.subs(subs), (self.variable, 0, length), title='Bending Moment',
xlabel=r'$\mathrm{x}$', ylabel=r'$\mathrm{M}$', line_color='b')
def plot_slope(self, subs=None):
"""
Returns a plot for slope of deflection curve of the Beam object.
Parameters
==========
subs : dictionary
Python dictionary containing Symbols as key and their
corresponding values.
Examples
========
There is a beam of length 8 meters. A constant distributed load of 10 KN/m
is applied from half of the beam till the end. There are two simple supports
below the beam, one at the starting point and another at the ending point
of the beam. A pointload of magnitude 5 KN is also applied from top of the
beam, at a distance of 4 meters from the starting point.
Take E = 200 GPa and I = 400*(10**-6) meter**4.
Using the sign convention of downwards forces being positive.
.. plot::
:context: close-figs
:format: doctest
:include-source: True
>>> from sympy.physics.continuum_mechanics.beam import Beam
>>> from sympy import symbols
>>> R1, R2 = symbols('R1, R2')
>>> b = Beam(8, 200*(10**9), 400*(10**-6))
>>> b.apply_load(5000, 2, -1)
>>> b.apply_load(R1, 0, -1)
>>> b.apply_load(R2, 8, -1)
>>> b.apply_load(10000, 4, 0, end=8)
>>> b.bc_deflection = [(0, 0), (8, 0)]
>>> b.solve_for_reaction_loads(R1, R2)
>>> b.plot_slope()
Plot object containing:
[0]: cartesian line: -8.59375e-5*SingularityFunction(x, 0, 2) + 3.125e-5*SingularityFunction(x, 2, 2)
+ 2.08333333333333e-5*SingularityFunction(x, 4, 3) - 0.0001953125*SingularityFunction(x, 8, 2)
- 2.08333333333333e-5*SingularityFunction(x, 8, 3) + 0.00138541666666667 for x over (0.0, 8.0)
"""
slope = self.slope()
if subs is None:
subs = {}
for sym in slope.atoms(Symbol):
if sym == self.variable:
continue
if sym not in subs:
raise ValueError('Value of %s was not passed.' %sym)
if self.length in subs:
length = subs[self.length]
else:
length = self.length
return plot(slope.subs(subs), (self.variable, 0, length), title='Slope',
xlabel=r'$\mathrm{x}$', ylabel=r'$\theta$', line_color='m')
def plot_deflection(self, subs=None):
"""
Returns a plot for deflection curve of the Beam object.
Parameters
==========
subs : dictionary
Python dictionary containing Symbols as key and their
corresponding values.
Examples
========
There is a beam of length 8 meters. A constant distributed load of 10 KN/m
is applied from half of the beam till the end. There are two simple supports
below the beam, one at the starting point and another at the ending point
of the beam. A pointload of magnitude 5 KN is also applied from top of the
beam, at a distance of 4 meters from the starting point.
Take E = 200 GPa and I = 400*(10**-6) meter**4.
Using the sign convention of downwards forces being positive.
.. plot::
:context: close-figs
:format: doctest
:include-source: True
>>> from sympy.physics.continuum_mechanics.beam import Beam
>>> from sympy import symbols
>>> R1, R2 = symbols('R1, R2')
>>> b = Beam(8, 200*(10**9), 400*(10**-6))
>>> b.apply_load(5000, 2, -1)
>>> b.apply_load(R1, 0, -1)
>>> b.apply_load(R2, 8, -1)
>>> b.apply_load(10000, 4, 0, end=8)
>>> b.bc_deflection = [(0, 0), (8, 0)]
>>> b.solve_for_reaction_loads(R1, R2)
>>> b.plot_deflection()
Plot object containing:
[0]: cartesian line: 0.00138541666666667*x - 2.86458333333333e-5*SingularityFunction(x, 0, 3)
+ 1.04166666666667e-5*SingularityFunction(x, 2, 3) + 5.20833333333333e-6*SingularityFunction(x, 4, 4)
- 6.51041666666667e-5*SingularityFunction(x, 8, 3) - 5.20833333333333e-6*SingularityFunction(x, 8, 4)
for x over (0.0, 8.0)
"""
deflection = self.deflection()
if subs is None:
subs = {}
for sym in deflection.atoms(Symbol):
if sym == self.variable:
continue
if sym not in subs:
raise ValueError('Value of %s was not passed.' %sym)
if self.length in subs:
length = subs[self.length]
else:
length = self.length
return plot(deflection.subs(subs), (self.variable, 0, length),
title='Deflection', xlabel=r'$\mathrm{x}$', ylabel=r'$\delta$',
line_color='r')
def plot_loading_results(self, subs=None):
"""
Returns a subplot of Shear Force, Bending Moment,
Slope and Deflection of the Beam object.
Parameters
==========
subs : dictionary
Python dictionary containing Symbols as key and their
corresponding values.
Examples
========
There is a beam of length 8 meters. A constant distributed load of 10 KN/m
is applied from half of the beam till the end. There are two simple supports
below the beam, one at the starting point and another at the ending point
of the beam. A pointload of magnitude 5 KN is also applied from top of the
beam, at a distance of 4 meters from the starting point.
Take E = 200 GPa and I = 400*(10**-6) meter**4.
Using the sign convention of downwards forces being positive.
.. plot::
:context: close-figs
:format: doctest
:include-source: True
>>> from sympy.physics.continuum_mechanics.beam import Beam
>>> from sympy import symbols
>>> from sympy.plotting import PlotGrid
>>> R1, R2 = symbols('R1, R2')
>>> b = Beam(8, 200*(10**9), 400*(10**-6))
>>> b.apply_load(5000, 2, -1)
>>> b.apply_load(R1, 0, -1)
>>> b.apply_load(R2, 8, -1)
>>> b.apply_load(10000, 4, 0, end=8)
>>> b.bc_deflection = [(0, 0), (8, 0)]
>>> b.solve_for_reaction_loads(R1, R2)
>>> axes = b.plot_loading_results()
"""
length = self.length
variable = self.variable
if subs is None:
subs = {}
for sym in self.deflection().atoms(Symbol):
if sym == self.variable:
continue
if sym not in subs:
raise ValueError('Value of %s was not passed.' %sym)
if self.length in subs:
length = subs[self.length]
else:
length = self.length
ax1 = plot(self.shear_force().subs(subs), (variable, 0, length),
title="Shear Force", xlabel=r'$\mathrm{x}$', ylabel=r'$\mathrm{V}$',
line_color='g', show=False)
ax2 = plot(self.bending_moment().subs(subs), (variable, 0, length),
title="Bending Moment", xlabel=r'$\mathrm{x}$', ylabel=r'$\mathrm{M}$',
line_color='b', show=False)
ax3 = plot(self.slope().subs(subs), (variable, 0, length),
title="Slope", xlabel=r'$\mathrm{x}$', ylabel=r'$\theta$',
line_color='m', show=False)
ax4 = plot(self.deflection().subs(subs), (variable, 0, length),
title="Deflection", xlabel=r'$\mathrm{x}$', ylabel=r'$\delta$',
line_color='r', show=False)
return PlotGrid(4, 1, ax1, ax2, ax3, ax4)
@doctest_depends_on(modules=('numpy',))
def draw(self, pictorial=True):
"""Returns a plot object representing the beam diagram of the beam.
Parameters
==========
pictorial: Boolean (default=True)
Setting ``pictorial=True`` would simply create a pictorial (scaled) view
of the beam diagram not with the exact dimensions.
Although setting ``pictorial=False`` would create a beam diagram with
the exact dimensions on the plot
Examples
========
.. plot::
:context: close-figs
:format: doctest
:include-source: True
>>> from sympy.physics.continuum_mechanics.beam import Beam
>>> from sympy import symbols
>>> R1, R2 = symbols('R1, R2')
>>> E, I = symbols('E, I')
>>> b = Beam(50, 20, 30)
>>> b.apply_load(10, 2, -1)
>>> b.apply_load(R1, 10, -1)
>>> b.apply_load(R2, 30, -1)
>>> b.apply_load(90, 5, 0, 23)
>>> b.apply_load(10, 30, 1, 50)
>>> b.apply_support(50, "pin")
>>> b.apply_support(0, "fixed")
>>> b.apply_support(20, "roller")
>>> b.draw()
Plot object containing:
[0]: cartesian line: 25*SingularityFunction(x, 5, 0)
- 25*SingularityFunction(x, 23, 0) + SingularityFunction(x, 30, 1)
- 20*SingularityFunction(x, 50, 0) - SingularityFunction(x, 50, 1)
+ 5 for x over (0.0, 50.0)
"""
if not numpy:
raise ImportError("To use this function numpy module is required")
x = self.variable
# checking whether length is an expression in terms of any Symbol.
from sympy import Expr
if isinstance(self.length, Expr):
l = list(self.length.atoms(Symbol))
# assigning every Symbol a default value of 10
l = {i:10 for i in l}
length = self.length.subs(l)
else:
l = {}
length = self.length
height = length/10
rectangles = []
rectangles.append({'xy':(0, 0), 'width':length, 'height': height, 'facecolor':"brown"})
annotations, markers, load_eq, fill = self._draw_load(pictorial, length, l)
support_markers, support_rectangles = self._draw_supports(length, l)
rectangles += support_rectangles
markers += support_markers
sing_plot = plot(height + load_eq, (x, 0, length),
xlim=(-height, length + height), ylim=(-length, 1.25*length), annotations=annotations,
markers=markers, rectangles=rectangles, fill=fill, axis=False, show=False)
return sing_plot
def _draw_load(self, pictorial, length, l):
loads = list(set(self.applied_loads) - set(self._support_as_loads))
height = length/10
x = self.variable
annotations = []
markers = []
load_args = []
scaled_load = 0
load_eq = 0
higher_order = False
fill = None
for load in loads:
# check if the position of load is in terms of the beam length.
if l:
pos = load[1].subs(l)
else:
pos = load[1]
# point loads
if load[2] == -1:
if isinstance(load[0], Symbol) or load[0].is_negative:
annotations.append({'s':'', 'xy':(pos, 0), 'xytext':(pos, height - 4*height), 'arrowprops':dict(width= 1.5, headlength=5, headwidth=5, facecolor='black')})
else:
annotations.append({'s':'', 'xy':(pos, height), 'xytext':(pos, height*4), 'arrowprops':dict(width= 1.5, headlength=4, headwidth=4, facecolor='black')})
# moment loads
elif load[2] == -2:
if load[0].is_negative:
markers.append({'args':[[pos], [height/2]], 'marker': r'$\circlearrowleft$', 'markersize':15})
else:
markers.append({'args':[[pos], [height/2]], 'marker': r'$\circlearrowright$', 'markersize':15})
# higher order loads
elif load[2] >= 0:
higher_order = True
# if pictorial is True we remake the load equation again with
# some constant magnitude values.
if pictorial:
value, start, order, end = load
value = 10**(1-order) if order > 0 else length/2
scaled_load += value*SingularityFunction(x, start, order)
if end:
f2 = 10**(1-order)*x**order if order > 0 else length/2*x**order
for i in range(0, order + 1):
scaled_load -= (f2.diff(x, i).subs(x, end - start)*
SingularityFunction(x, end, i) / factorial(i))
# `fill` will be assigned only when higher order loads are present
if higher_order:
if pictorial:
if isinstance(scaled_load, Add):
load_args = scaled_load.args
else:
# when the load equation consists of only a single term
load_args = (scaled_load,)
load_eq = [i.subs(l) for i in load_args]
else:
if isinstance(self.load, Add):
load_args = self.load.args
else:
load_args = (self.load,)
load_eq = [i.subs(l) for i in load_args if list(i.atoms(SingularityFunction))[0].args[2] >= 0]
load_eq = Add(*load_eq)
# filling higher order loads with colour
y = numpy.arange(0, float(length), 0.001)
expr = height + load_eq.rewrite(Piecewise)
y1 = lambdify(x, expr, 'numpy')
y2 = float(height)
fill = {'x': y, 'y1': y1(y), 'y2': y2, 'color':'darkkhaki'}
return annotations, markers, load_eq, fill
def _draw_supports(self, length, l):
height = float(length/10)
support_markers = []
support_rectangles = []
for support in self._applied_supports:
if l:
pos = support[0].subs(l)
else:
pos = support[0]
if support[1] == "pin":
support_markers.append({'args':[pos, [0]], 'marker':6, 'markersize':13, 'color':"black"})
elif support[1] == "roller":
support_markers.append({'args':[pos, [-height/2.5]], 'marker':'o', 'markersize':11, 'color':"black"})
elif support[1] == "fixed":
if pos == 0:
support_rectangles.append({'xy':(0, -3*height), 'width':-length/20, 'height':6*height + height, 'fill':False, 'hatch':'/////'})
else:
support_rectangles.append({'xy':(length, -3*height), 'width':length/20, 'height': 6*height + height, 'fill':False, 'hatch':'/////'})
return support_markers, support_rectangles
class Beam3D(Beam):
"""
This class handles loads applied in any direction of a 3D space along
with unequal values of Second moment along different axes.
.. note::
While solving a beam bending problem, a user should choose its
own sign convention and should stick to it. The results will
automatically follow the chosen sign convention.
This class assumes that any kind of distributed load/moment is
applied through out the span of a beam.
Examples
========
There is a beam of l meters long. A constant distributed load of magnitude q
is applied along y-axis from start till the end of beam. A constant distributed
moment of magnitude m is also applied along z-axis from start till the end of beam.
Beam is fixed at both of its end. So, deflection of the beam at the both ends
is restricted.
>>> from sympy.physics.continuum_mechanics.beam import Beam3D
>>> from sympy import symbols, simplify, collect
>>> l, E, G, I, A = symbols('l, E, G, I, A')
>>> b = Beam3D(l, E, G, I, A)
>>> x, q, m = symbols('x, q, m')
>>> b.apply_load(q, 0, 0, dir="y")
>>> b.apply_moment_load(m, 0, -1, dir="z")
>>> b.shear_force()
[0, -q*x, 0]
>>> b.bending_moment()
[0, 0, -m*x + q*x**2/2]
>>> b.bc_slope = [(0, [0, 0, 0]), (l, [0, 0, 0])]
>>> b.bc_deflection = [(0, [0, 0, 0]), (l, [0, 0, 0])]
>>> b.solve_slope_deflection()
>>> b.slope()
[0, 0, x*(l*(-l*q + 3*l*(A*G*l*(l*q - 2*m) + 12*E*I*q)/(2*(A*G*l**2 + 12*E*I)) + 3*m)/6
+ q*x**2/6 + x*(-l*(A*G*l*(l*q - 2*m) + 12*E*I*q)/(2*(A*G*l**2 + 12*E*I)) - m)/2)/(E*I)]
>>> dx, dy, dz = b.deflection()
>>> dy = collect(simplify(dy), x)
>>> dx == dz == 0
True
>>> dy == (x*(12*A*E*G*I*l**3*q - 24*A*E*G*I*l**2*m + 144*E**2*I**2*l*q +
... x**3*(A**2*G**2*l**2*q + 12*A*E*G*I*q) +
... x**2*(-2*A**2*G**2*l**3*q - 24*A*E*G*I*l*q - 48*A*E*G*I*m) +
... x*(A**2*G**2*l**4*q + 72*A*E*G*I*l*m - 144*E**2*I**2*q)
... )/(24*A*E*G*I*(A*G*l**2 + 12*E*I)))
True
References
==========
.. [1] http://homes.civil.aau.dk/jc/FemteSemester/Beams3D.pdf
"""
def __init__(self, length, elastic_modulus, shear_modulus , second_moment, area, variable=Symbol('x')):
"""Initializes the class.
Parameters
==========
length : Sympifyable
A Symbol or value representing the Beam's length.
elastic_modulus : Sympifyable
A SymPy expression representing the Beam's Modulus of Elasticity.
It is a measure of the stiffness of the Beam material.
shear_modulus : Sympifyable
A SymPy expression representing the Beam's Modulus of rigidity.
It is a measure of rigidity of the Beam material.
second_moment : Sympifyable or list
A list of two elements having SymPy expression representing the
Beam's Second moment of area. First value represent Second moment
across y-axis and second across z-axis.
Single SymPy expression can be passed if both values are same
area : Sympifyable
A SymPy expression representing the Beam's cross-sectional area
in a plane prependicular to length of the Beam.
variable : Symbol, optional
A Symbol object that will be used as the variable along the beam
while representing the load, shear, moment, slope and deflection
curve. By default, it is set to ``Symbol('x')``.
"""
super(Beam3D, self).__init__(length, elastic_modulus, second_moment, variable)
self.shear_modulus = shear_modulus
self.area = area
self._load_vector = [0, 0, 0]
self._moment_load_vector = [0, 0, 0]
self._load_Singularity = [0, 0, 0]
self._slope = [0, 0, 0]
self._deflection = [0, 0, 0]
@property
def shear_modulus(self):
"""Young's Modulus of the Beam. """
return self._shear_modulus
@shear_modulus.setter
def shear_modulus(self, e):
self._shear_modulus = sympify(e)
@property
def second_moment(self):
"""Second moment of area of the Beam. """
return self._second_moment
@second_moment.setter
def second_moment(self, i):
if isinstance(i, list):
i = [sympify(x) for x in i]
self._second_moment = i
else:
self._second_moment = sympify(i)
@property
def area(self):
"""Cross-sectional area of the Beam. """
return self._area
@area.setter
def area(self, a):
self._area = sympify(a)
@property
def load_vector(self):
"""
Returns a three element list representing the load vector.
"""
return self._load_vector
@property
def moment_load_vector(self):
"""
Returns a three element list representing moment loads on Beam.
"""
return self._moment_load_vector
@property
def boundary_conditions(self):
"""
Returns a dictionary of boundary conditions applied on the beam.
The dictionary has two keywords namely slope and deflection.
The value of each keyword is a list of tuple, where each tuple
contains location and value of a boundary condition in the format
(location, value). Further each value is a list corresponding to
slope or deflection(s) values along three axes at that location.
Examples
========
There is a beam of length 4 meters. The slope at 0 should be 4 along
the x-axis and 0 along others. At the other end of beam, deflection
along all the three axes should be zero.
>>> from sympy.physics.continuum_mechanics.beam import Beam3D
>>> from sympy import symbols
>>> l, E, G, I, A, x = symbols('l, E, G, I, A, x')
>>> b = Beam3D(30, E, G, I, A, x)
>>> b.bc_slope = [(0, (4, 0, 0))]
>>> b.bc_deflection = [(4, [0, 0, 0])]
>>> b.boundary_conditions
{'deflection': [(4, [0, 0, 0])], 'slope': [(0, (4, 0, 0))]}
Here the deflection of the beam should be ``0`` along all the three axes at ``4``.
Similarly, the slope of the beam should be ``4`` along x-axis and ``0``
along y and z axis at ``0``.
"""
return self._boundary_conditions
def polar_moment(self):
"""
Returns the polar moment of area of the beam
about the X axis with respect to the centroid.
Examples
========
>>> from sympy.physics.continuum_mechanics.beam import Beam3D
>>> from sympy import symbols
>>> l, E, G, I, A = symbols('l, E, G, I, A')
>>> b = Beam3D(l, E, G, I, A)
>>> b.polar_moment()
2*I
>>> I1 = [9, 15]
>>> b = Beam3D(l, E, G, I1, A)
>>> b.polar_moment()
24
"""
if not iterable(self.second_moment):
return 2*self.second_moment
return sum(self.second_moment)
def apply_load(self, value, start, order, dir="y"):
"""
This method adds up the force load to a particular beam object.
Parameters
==========
value : Sympifyable
The magnitude of an applied load.
dir : String
Axis along which load is applied.
order : Integer
The order of the applied load.
- For point loads, order=-1
- For constant distributed load, order=0
- For ramp loads, order=1
- For parabolic ramp loads, order=2
- ... so on.
"""
x = self.variable
value = sympify(value)
start = sympify(start)
order = sympify(order)
if dir == "x":
if not order == -1:
self._load_vector[0] += value
self._load_Singularity[0] += value*SingularityFunction(x, start, order)
elif dir == "y":
if not order == -1:
self._load_vector[1] += value
self._load_Singularity[1] += value*SingularityFunction(x, start, order)
else:
if not order == -1:
self._load_vector[2] += value
self._load_Singularity[2] += value*SingularityFunction(x, start, order)
def apply_moment_load(self, value, start, order, dir="y"):
"""
This method adds up the moment loads to a particular beam object.
Parameters
==========
value : Sympifyable
The magnitude of an applied moment.
dir : String
Axis along which moment is applied.
order : Integer
The order of the applied load.
- For point moments, order=-2
- For constant distributed moment, order=-1
- For ramp moments, order=0
- For parabolic ramp moments, order=1
- ... so on.
"""
x = self.variable
value = sympify(value)
start = sympify(start)
order = sympify(order)
if dir == "x":
if not order == -2:
self._moment_load_vector[0] += value
self._load_Singularity[0] += value*SingularityFunction(x, start, order)
elif dir == "y":
if not order == -2:
self._moment_load_vector[1] += value
self._load_Singularity[0] += value*SingularityFunction(x, start, order)
else:
if not order == -2:
self._moment_load_vector[2] += value
self._load_Singularity[0] += value*SingularityFunction(x, start, order)
def apply_support(self, loc, type="fixed"):
if type == "pin" or type == "roller":
reaction_load = Symbol('R_'+str(loc))
self._reaction_loads[reaction_load] = reaction_load
self.bc_deflection.append((loc, [0, 0, 0]))
else:
reaction_load = Symbol('R_'+str(loc))
reaction_moment = Symbol('M_'+str(loc))
self._reaction_loads[reaction_load] = [reaction_load, reaction_moment]
self.bc_deflection.append((loc, [0, 0, 0]))
self.bc_slope.append((loc, [0, 0, 0]))
def solve_for_reaction_loads(self, *reaction):
"""
Solves for the reaction forces.
Examples
========
There is a beam of length 30 meters. It it supported by rollers at
of its end. A constant distributed load of magnitude 8 N is applied
from start till its end along y-axis. Another linear load having
slope equal to 9 is applied along z-axis.
>>> from sympy.physics.continuum_mechanics.beam import Beam3D
>>> from sympy import symbols
>>> l, E, G, I, A, x = symbols('l, E, G, I, A, x')
>>> b = Beam3D(30, E, G, I, A, x)
>>> b.apply_load(8, start=0, order=0, dir="y")
>>> b.apply_load(9*x, start=0, order=0, dir="z")
>>> b.bc_deflection = [(0, [0, 0, 0]), (30, [0, 0, 0])]
>>> R1, R2, R3, R4 = symbols('R1, R2, R3, R4')
>>> b.apply_load(R1, start=0, order=-1, dir="y")
>>> b.apply_load(R2, start=30, order=-1, dir="y")
>>> b.apply_load(R3, start=0, order=-1, dir="z")
>>> b.apply_load(R4, start=30, order=-1, dir="z")
>>> b.solve_for_reaction_loads(R1, R2, R3, R4)
>>> b.reaction_loads
{R1: -120, R2: -120, R3: -1350, R4: -2700}
"""
x = self.variable
l = self.length
q = self._load_Singularity
shear_curves = [integrate(load, x) for load in q]
moment_curves = [integrate(shear, x) for shear in shear_curves]
for i in range(3):
react = [r for r in reaction if (shear_curves[i].has(r) or moment_curves[i].has(r))]
if len(react) == 0:
continue
shear_curve = limit(shear_curves[i], x, l)
moment_curve = limit(moment_curves[i], x, l)
sol = list((linsolve([shear_curve, moment_curve], react).args)[0])
sol_dict = dict(zip(react, sol))
reaction_loads = self._reaction_loads
# Check if any of the evaluated rection exists in another direction
# and if it exists then it should have same value.
for key in sol_dict:
if key in reaction_loads and sol_dict[key] != reaction_loads[key]:
raise ValueError("Ambiguous solution for %s in different directions." % key)
self._reaction_loads.update(sol_dict)
def shear_force(self):
"""
Returns a list of three expressions which represents the shear force
curve of the Beam object along all three axes.
"""
x = self.variable
q = self._load_vector
return [integrate(-q[0], x), integrate(-q[1], x), integrate(-q[2], x)]
def axial_force(self):
"""
Returns expression of Axial shear force present inside the Beam object.
"""
return self.shear_force()[0]
def bending_moment(self):
"""
Returns a list of three expressions which represents the bending moment
curve of the Beam object along all three axes.
"""
x = self.variable
m = self._moment_load_vector
shear = self.shear_force()
return [integrate(-m[0], x), integrate(-m[1] + shear[2], x),
integrate(-m[2] - shear[1], x) ]
def torsional_moment(self):
"""
Returns expression of Torsional moment present inside the Beam object.
"""
return self.bending_moment()[0]
def solve_slope_deflection(self):
from sympy import dsolve, Function, Derivative, Eq
x = self.variable
l = self.length
E = self.elastic_modulus
G = self.shear_modulus
I = self.second_moment
if isinstance(I, list):
I_y, I_z = I[0], I[1]
else:
I_y = I_z = I
A = self.area
load = self._load_vector
moment = self._moment_load_vector
defl = Function('defl')
theta = Function('theta')
# Finding deflection along x-axis(and corresponding slope value by differentiating it)
# Equation used: Derivative(E*A*Derivative(def_x(x), x), x) + load_x = 0
eq = Derivative(E*A*Derivative(defl(x), x), x) + load[0]
def_x = dsolve(Eq(eq, 0), defl(x)).args[1]
# Solving constants originated from dsolve
C1 = Symbol('C1')
C2 = Symbol('C2')
constants = list((linsolve([def_x.subs(x, 0), def_x.subs(x, l)], C1, C2).args)[0])
def_x = def_x.subs({C1:constants[0], C2:constants[1]})
slope_x = def_x.diff(x)
self._deflection[0] = def_x
self._slope[0] = slope_x
# Finding deflection along y-axis and slope across z-axis. System of equation involved:
# 1: Derivative(E*I_z*Derivative(theta_z(x), x), x) + G*A*(Derivative(defl_y(x), x) - theta_z(x)) + moment_z = 0
# 2: Derivative(G*A*(Derivative(defl_y(x), x) - theta_z(x)), x) + load_y = 0
C_i = Symbol('C_i')
# Substitute value of `G*A*(Derivative(defl_y(x), x) - theta_z(x))` from (2) in (1)
eq1 = Derivative(E*I_z*Derivative(theta(x), x), x) + (integrate(-load[1], x) + C_i) + moment[2]
slope_z = dsolve(Eq(eq1, 0)).args[1]
# Solve for constants originated from using dsolve on eq1
constants = list((linsolve([slope_z.subs(x, 0), slope_z.subs(x, l)], C1, C2).args)[0])
slope_z = slope_z.subs({C1:constants[0], C2:constants[1]})
# Put value of slope obtained back in (2) to solve for `C_i` and find deflection across y-axis
eq2 = G*A*(Derivative(defl(x), x)) + load[1]*x - C_i - G*A*slope_z
def_y = dsolve(Eq(eq2, 0), defl(x)).args[1]
# Solve for constants originated from using dsolve on eq2
constants = list((linsolve([def_y.subs(x, 0), def_y.subs(x, l)], C1, C_i).args)[0])
self._deflection[1] = def_y.subs({C1:constants[0], C_i:constants[1]})
self._slope[2] = slope_z.subs(C_i, constants[1])
# Finding deflection along z-axis and slope across y-axis. System of equation involved:
# 1: Derivative(E*I_y*Derivative(theta_y(x), x), x) - G*A*(Derivative(defl_z(x), x) + theta_y(x)) + moment_y = 0
# 2: Derivative(G*A*(Derivative(defl_z(x), x) + theta_y(x)), x) + load_z = 0
# Substitute value of `G*A*(Derivative(defl_y(x), x) + theta_z(x))` from (2) in (1)
eq1 = Derivative(E*I_y*Derivative(theta(x), x), x) + (integrate(load[2], x) - C_i) + moment[1]
slope_y = dsolve(Eq(eq1, 0)).args[1]
# Solve for constants originated from using dsolve on eq1
constants = list((linsolve([slope_y.subs(x, 0), slope_y.subs(x, l)], C1, C2).args)[0])
slope_y = slope_y.subs({C1:constants[0], C2:constants[1]})
# Put value of slope obtained back in (2) to solve for `C_i` and find deflection across z-axis
eq2 = G*A*(Derivative(defl(x), x)) + load[2]*x - C_i + G*A*slope_y
def_z = dsolve(Eq(eq2,0)).args[1]
# Solve for constants originated from using dsolve on eq2
constants = list((linsolve([def_z.subs(x, 0), def_z.subs(x, l)], C1, C_i).args)[0])
self._deflection[2] = def_z.subs({C1:constants[0], C_i:constants[1]})
self._slope[1] = slope_y.subs(C_i, constants[1])
def slope(self):
"""
Returns a three element list representing slope of deflection curve
along all the three axes.
"""
return self._slope
def deflection(self):
"""
Returns a three element list representing deflection curve along all
the three axes.
"""
return self._deflection
|
004deb7fcc00790b75c0d486b4f4f18c08d22b6263b86d1f005e5cec44bd2d6c | """
**Contains**
* refraction_angle
* fresnel_coefficients
* deviation
* brewster_angle
* critical_angle
* lens_makers_formula
* mirror_formula
* lens_formula
* hyperfocal_distance
* transverse_magnification
"""
from __future__ import division
__all__ = ['refraction_angle',
'deviation',
'fresnel_coefficients',
'brewster_angle',
'critical_angle',
'lens_makers_formula',
'mirror_formula',
'lens_formula',
'hyperfocal_distance',
'transverse_magnification'
]
from sympy import Symbol, sympify, sqrt, Matrix, acos, oo, Limit, atan2, asin,\
cos, sin, tan, I, cancel, pi, Float
from sympy.core.compatibility import is_sequence
from sympy.geometry.line import Ray3D, Point3D
from sympy.geometry.util import intersection
from sympy.geometry.plane import Plane
from .medium import Medium
def refractive_index_of_medium(medium):
"""
Helper function that returns refractive index, given a medium
"""
if isinstance(medium, Medium):
n = medium.refractive_index
else:
n = sympify(medium)
return n
def refraction_angle(incident, medium1, medium2, normal=None, plane=None):
"""
This function calculates transmitted vector after refraction at planar
surface. `medium1` and `medium2` can be `Medium` or any sympifiable object.
If `incident` is a number then treated as angle of incidence (in radians)
in which case refraction angle is returned.
If `incident` is an object of `Ray3D`, `normal` also has to be an instance
of `Ray3D` in order to get the output as a `Ray3D`. Please note that if
plane of separation is not provided and normal is an instance of `Ray3D`,
normal will be assumed to be intersecting incident ray at the plane of
separation. This will not be the case when `normal` is a `Matrix` or
any other sequence.
If `incident` is an instance of `Ray3D` and `plane` has not been provided
and `normal` is not `Ray3D`, output will be a `Matrix`.
Parameters
==========
incident : Matrix, Ray3D, sequence or a number
Incident vector or angle of incidence
medium1 : sympy.physics.optics.medium.Medium or sympifiable
Medium 1 or its refractive index
medium2 : sympy.physics.optics.medium.Medium or sympifiable
Medium 2 or its refractive index
normal : Matrix, Ray3D, or sequence
Normal vector
plane : Plane
Plane of separation of the two media.
Returns an angle of refraction or a refracted ray depending on inputs.
Examples
========
>>> from sympy.physics.optics import refraction_angle
>>> from sympy.geometry import Point3D, Ray3D, Plane
>>> from sympy.matrices import Matrix
>>> from sympy import symbols, pi
>>> n = Matrix([0, 0, 1])
>>> P = Plane(Point3D(0, 0, 0), normal_vector=[0, 0, 1])
>>> r1 = Ray3D(Point3D(-1, -1, 1), Point3D(0, 0, 0))
>>> refraction_angle(r1, 1, 1, n)
Matrix([
[ 1],
[ 1],
[-1]])
>>> refraction_angle(r1, 1, 1, plane=P)
Ray3D(Point3D(0, 0, 0), Point3D(1, 1, -1))
With different index of refraction of the two media
>>> n1, n2 = symbols('n1, n2')
>>> refraction_angle(r1, n1, n2, n)
Matrix([
[ n1/n2],
[ n1/n2],
[-sqrt(3)*sqrt(-2*n1**2/(3*n2**2) + 1)]])
>>> refraction_angle(r1, n1, n2, plane=P)
Ray3D(Point3D(0, 0, 0), Point3D(n1/n2, n1/n2, -sqrt(3)*sqrt(-2*n1**2/(3*n2**2) + 1)))
>>> round(refraction_angle(pi/6, 1.2, 1.5), 5)
0.41152
"""
n1 = refractive_index_of_medium(medium1)
n2 = refractive_index_of_medium(medium2)
# check if an incidence angle was supplied instead of a ray
try:
angle_of_incidence = float(incident)
except TypeError:
angle_of_incidence = None
try:
critical_angle_ = critical_angle(medium1, medium2)
except (ValueError, TypeError):
critical_angle_ = None
if angle_of_incidence is not None:
if normal is not None or plane is not None:
raise ValueError('Normal/plane not allowed if incident is an angle')
if not 0.0 <= angle_of_incidence < pi*0.5:
raise ValueError('Angle of incidence not in range [0:pi/2)')
if critical_angle_ and angle_of_incidence > critical_angle_:
raise ValueError('Ray undergoes total internal reflection')
return asin(n1*sin(angle_of_incidence)/n2)
if angle_of_incidence and not 0 <= angle_of_incidence < pi*0.5:
raise ValueError
# Treat the incident as ray below
# A flag to check whether to return Ray3D or not
return_ray = False
if plane is not None and normal is not None:
raise ValueError("Either plane or normal is acceptable.")
if not isinstance(incident, Matrix):
if is_sequence(incident):
_incident = Matrix(incident)
elif isinstance(incident, Ray3D):
_incident = Matrix(incident.direction_ratio)
else:
raise TypeError(
"incident should be a Matrix, Ray3D, or sequence")
else:
_incident = incident
# If plane is provided, get direction ratios of the normal
# to the plane from the plane else go with `normal` param.
if plane is not None:
if not isinstance(plane, Plane):
raise TypeError("plane should be an instance of geometry.plane.Plane")
# If we have the plane, we can get the intersection
# point of incident ray and the plane and thus return
# an instance of Ray3D.
if isinstance(incident, Ray3D):
return_ray = True
intersection_pt = plane.intersection(incident)[0]
_normal = Matrix(plane.normal_vector)
else:
if not isinstance(normal, Matrix):
if is_sequence(normal):
_normal = Matrix(normal)
elif isinstance(normal, Ray3D):
_normal = Matrix(normal.direction_ratio)
if isinstance(incident, Ray3D):
intersection_pt = intersection(incident, normal)
if len(intersection_pt) == 0:
raise ValueError(
"Normal isn't concurrent with the incident ray.")
else:
return_ray = True
intersection_pt = intersection_pt[0]
else:
raise TypeError(
"Normal should be a Matrix, Ray3D, or sequence")
else:
_normal = normal
eta = n1/n2 # Relative index of refraction
# Calculating magnitude of the vectors
mag_incident = sqrt(sum([i**2 for i in _incident]))
mag_normal = sqrt(sum([i**2 for i in _normal]))
# Converting vectors to unit vectors by dividing
# them with their magnitudes
_incident /= mag_incident
_normal /= mag_normal
c1 = -_incident.dot(_normal) # cos(angle_of_incidence)
cs2 = 1 - eta**2*(1 - c1**2) # cos(angle_of_refraction)**2
if cs2.is_negative: # This is the case of total internal reflection(TIR).
return 0
drs = eta*_incident + (eta*c1 - sqrt(cs2))*_normal
# Multiplying unit vector by its magnitude
drs = drs*mag_incident
if not return_ray:
return drs
else:
return Ray3D(intersection_pt, direction_ratio=drs)
def fresnel_coefficients(angle_of_incidence, medium1, medium2):
"""
This function uses Fresnel equations to calculate reflection and
transmission coefficients. Those are obtained for both polarisations
when the electric field vector is in the plane of incidence (labelled 'p')
and when the electric field vector is perpendicular to the plane of
incidence (labelled 's'). There are four real coefficients unless the
incident ray reflects in total internal in which case there are two complex
ones. Angle of incidence is the angle between the incident ray and the
surface normal. ``medium1`` and ``medium2`` can be ``Medium`` or any
sympifiable object.
Parameters
==========
angle_of_incidence : sympifiable
medium1 : Medium or sympifiable
Medium 1 or its refractive index
medium2 : Medium or sympifiable
Medium 2 or its refractive index
Returns a list with four real Fresnel coefficients:
[reflection p (TM), reflection s (TE),
transmission p (TM), transmission s (TE)]
If the ray is undergoes total internal reflection then returns a
list of two complex Fresnel coefficients:
[reflection p (TM), reflection s (TE)]
Examples
========
>>> from sympy.physics.optics import fresnel_coefficients
>>> fresnel_coefficients(0.3, 1, 2)
[0.317843553417859, -0.348645229818821,
0.658921776708929, 0.651354770181179]
>>> fresnel_coefficients(0.6, 2, 1)
[-0.235625382192159 - 0.971843958291041*I,
0.816477005968898 - 0.577377951366403*I]
References
==========
https://en.wikipedia.org/wiki/Fresnel_equations
"""
if not 0 <= 2*angle_of_incidence < pi:
raise ValueError('Angle of incidence not in range [0:pi/2)')
n1 = refractive_index_of_medium(medium1)
n2 = refractive_index_of_medium(medium2)
angle_of_refraction = asin(n1*sin(angle_of_incidence)/n2)
try:
angle_of_total_internal_reflection_onset = critical_angle(n1, n2)
except ValueError:
angle_of_total_internal_reflection_onset = None
if angle_of_total_internal_reflection_onset == None or\
angle_of_total_internal_reflection_onset > angle_of_incidence:
R_s = -sin(angle_of_incidence - angle_of_refraction)\
/sin(angle_of_incidence + angle_of_refraction)
R_p = tan(angle_of_incidence - angle_of_refraction)\
/tan(angle_of_incidence + angle_of_refraction)
T_s = 2*sin(angle_of_refraction)*cos(angle_of_incidence)\
/sin(angle_of_incidence + angle_of_refraction)
T_p = 2*sin(angle_of_refraction)*cos(angle_of_incidence)\
/(sin(angle_of_incidence + angle_of_refraction)\
*cos(angle_of_incidence - angle_of_refraction))
return [R_p, R_s, T_p, T_s]
else:
n = n2/n1
R_s = cancel((cos(angle_of_incidence)-\
I*sqrt(sin(angle_of_incidence)**2 - n**2))\
/(cos(angle_of_incidence)+\
I*sqrt(sin(angle_of_incidence)**2 - n**2)))
R_p = cancel((n**2*cos(angle_of_incidence)-\
I*sqrt(sin(angle_of_incidence)**2 - n**2))\
/(n**2*cos(angle_of_incidence)+\
I*sqrt(sin(angle_of_incidence)**2 - n**2)))
return [R_p, R_s]
def deviation(incident, medium1, medium2, normal=None, plane=None):
"""
This function calculates the angle of deviation of a ray
due to refraction at planar surface.
Parameters
==========
incident : Matrix, Ray3D, sequence or float
Incident vector or angle of incidence
medium1 : sympy.physics.optics.medium.Medium or sympifiable
Medium 1 or its refractive index
medium2 : sympy.physics.optics.medium.Medium or sympifiable
Medium 2 or its refractive index
normal : Matrix, Ray3D, or sequence
Normal vector
plane : Plane
Plane of separation of the two media.
Returns angular deviation between incident and refracted rays
Examples
========
>>> from sympy.physics.optics import deviation
>>> from sympy.geometry import Point3D, Ray3D, Plane
>>> from sympy.matrices import Matrix
>>> from sympy import symbols
>>> n1, n2 = symbols('n1, n2')
>>> n = Matrix([0, 0, 1])
>>> P = Plane(Point3D(0, 0, 0), normal_vector=[0, 0, 1])
>>> r1 = Ray3D(Point3D(-1, -1, 1), Point3D(0, 0, 0))
>>> deviation(r1, 1, 1, n)
0
>>> deviation(r1, n1, n2, plane=P)
-acos(-sqrt(-2*n1**2/(3*n2**2) + 1)) + acos(-sqrt(3)/3)
>>> round(deviation(0.1, 1.2, 1.5), 5)
-0.02005
"""
refracted = refraction_angle(incident,
medium1,
medium2,
normal=normal,
plane=plane)
try:
angle_of_incidence = Float(incident)
except TypeError:
angle_of_incidence = None
if angle_of_incidence is not None:
return float(refracted) - angle_of_incidence
if refracted != 0:
if isinstance(refracted, Ray3D):
refracted = Matrix(refracted.direction_ratio)
if not isinstance(incident, Matrix):
if is_sequence(incident):
_incident = Matrix(incident)
elif isinstance(incident, Ray3D):
_incident = Matrix(incident.direction_ratio)
else:
raise TypeError(
"incident should be a Matrix, Ray3D, or sequence")
else:
_incident = incident
if plane is None:
if not isinstance(normal, Matrix):
if is_sequence(normal):
_normal = Matrix(normal)
elif isinstance(normal, Ray3D):
_normal = Matrix(normal.direction_ratio)
else:
raise TypeError(
"normal should be a Matrix, Ray3D, or sequence")
else:
_normal = normal
else:
_normal = Matrix(plane.normal_vector)
mag_incident = sqrt(sum([i**2 for i in _incident]))
mag_normal = sqrt(sum([i**2 for i in _normal]))
mag_refracted = sqrt(sum([i**2 for i in refracted]))
_incident /= mag_incident
_normal /= mag_normal
refracted /= mag_refracted
i = acos(_incident.dot(_normal))
r = acos(refracted.dot(_normal))
return i - r
def brewster_angle(medium1, medium2):
"""
This function calculates the Brewster's angle of incidence to Medium 2 from
Medium 1 in radians.
Parameters
==========
medium 1 : Medium or sympifiable
Refractive index of Medium 1
medium 2 : Medium or sympifiable
Refractive index of Medium 1
Examples
========
>>> from sympy.physics.optics import brewster_angle
>>> brewster_angle(1, 1.33)
0.926093295503462
"""
n1 = refractive_index_of_medium(medium1)
n2 = refractive_index_of_medium(medium2)
return atan2(n2, n1)
def critical_angle(medium1, medium2):
"""
This function calculates the critical angle of incidence (marking the onset
of total internal) to Medium 2 from Medium 1 in radians.
Parameters
==========
medium 1 : Medium or sympifiable
Refractive index of Medium 1
medium 2 : Medium or sympifiable
Refractive index of Medium 1
Examples
========
>>> from sympy.physics.optics import critical_angle
>>> critical_angle(1.33, 1)
0.850908514477849
"""
n1 = refractive_index_of_medium(medium1)
n2 = refractive_index_of_medium(medium2)
if n2 > n1:
raise ValueError('Total internal reflection impossible for n1 < n2')
else:
return asin(n2/n1)
def lens_makers_formula(n_lens, n_surr, r1, r2):
"""
This function calculates focal length of a thin lens.
It follows cartesian sign convention.
Parameters
==========
n_lens : Medium or sympifiable
Index of refraction of lens.
n_surr : Medium or sympifiable
Index of reflection of surrounding.
r1 : sympifiable
Radius of curvature of first surface.
r2 : sympifiable
Radius of curvature of second surface.
Examples
========
>>> from sympy.physics.optics import lens_makers_formula
>>> lens_makers_formula(1.33, 1, 10, -10)
15.1515151515151
"""
if isinstance(n_lens, Medium):
n_lens = n_lens.refractive_index
else:
n_lens = sympify(n_lens)
if isinstance(n_surr, Medium):
n_surr = n_surr.refractive_index
else:
n_surr = sympify(n_surr)
r1 = sympify(r1)
r2 = sympify(r2)
return 1/((n_lens - n_surr)/n_surr*(1/r1 - 1/r2))
def mirror_formula(focal_length=None, u=None, v=None):
"""
This function provides one of the three parameters
when two of them are supplied.
This is valid only for paraxial rays.
Parameters
==========
focal_length : sympifiable
Focal length of the mirror.
u : sympifiable
Distance of object from the pole on
the principal axis.
v : sympifiable
Distance of the image from the pole
on the principal axis.
Examples
========
>>> from sympy.physics.optics import mirror_formula
>>> from sympy.abc import f, u, v
>>> mirror_formula(focal_length=f, u=u)
f*u/(-f + u)
>>> mirror_formula(focal_length=f, v=v)
f*v/(-f + v)
>>> mirror_formula(u=u, v=v)
u*v/(u + v)
"""
if focal_length and u and v:
raise ValueError("Please provide only two parameters")
focal_length = sympify(focal_length)
u = sympify(u)
v = sympify(v)
if u == oo:
_u = Symbol('u')
if v == oo:
_v = Symbol('v')
if focal_length == oo:
_f = Symbol('f')
if focal_length is None:
if u == oo and v == oo:
return Limit(Limit(_v*_u/(_v + _u), _u, oo), _v, oo).doit()
if u == oo:
return Limit(v*_u/(v + _u), _u, oo).doit()
if v == oo:
return Limit(_v*u/(_v + u), _v, oo).doit()
return v*u/(v + u)
if u is None:
if v == oo and focal_length == oo:
return Limit(Limit(_v*_f/(_v - _f), _v, oo), _f, oo).doit()
if v == oo:
return Limit(_v*focal_length/(_v - focal_length), _v, oo).doit()
if focal_length == oo:
return Limit(v*_f/(v - _f), _f, oo).doit()
return v*focal_length/(v - focal_length)
if v is None:
if u == oo and focal_length == oo:
return Limit(Limit(_u*_f/(_u - _f), _u, oo), _f, oo).doit()
if u == oo:
return Limit(_u*focal_length/(_u - focal_length), _u, oo).doit()
if focal_length == oo:
return Limit(u*_f/(u - _f), _f, oo).doit()
return u*focal_length/(u - focal_length)
def lens_formula(focal_length=None, u=None, v=None):
"""
This function provides one of the three parameters
when two of them are supplied.
This is valid only for paraxial rays.
Parameters
==========
focal_length : sympifiable
Focal length of the mirror.
u : sympifiable
Distance of object from the optical center on
the principal axis.
v : sympifiable
Distance of the image from the optical center
on the principal axis.
Examples
========
>>> from sympy.physics.optics import lens_formula
>>> from sympy.abc import f, u, v
>>> lens_formula(focal_length=f, u=u)
f*u/(f + u)
>>> lens_formula(focal_length=f, v=v)
f*v/(f - v)
>>> lens_formula(u=u, v=v)
u*v/(u - v)
"""
if focal_length and u and v:
raise ValueError("Please provide only two parameters")
focal_length = sympify(focal_length)
u = sympify(u)
v = sympify(v)
if u == oo:
_u = Symbol('u')
if v == oo:
_v = Symbol('v')
if focal_length == oo:
_f = Symbol('f')
if focal_length is None:
if u == oo and v == oo:
return Limit(Limit(_v*_u/(_u - _v), _u, oo), _v, oo).doit()
if u == oo:
return Limit(v*_u/(_u - v), _u, oo).doit()
if v == oo:
return Limit(_v*u/(u - _v), _v, oo).doit()
return v*u/(u - v)
if u is None:
if v == oo and focal_length == oo:
return Limit(Limit(_v*_f/(_f - _v), _v, oo), _f, oo).doit()
if v == oo:
return Limit(_v*focal_length/(focal_length - _v), _v, oo).doit()
if focal_length == oo:
return Limit(v*_f/(_f - v), _f, oo).doit()
return v*focal_length/(focal_length - v)
if v is None:
if u == oo and focal_length == oo:
return Limit(Limit(_u*_f/(_u + _f), _u, oo), _f, oo).doit()
if u == oo:
return Limit(_u*focal_length/(_u + focal_length), _u, oo).doit()
if focal_length == oo:
return Limit(u*_f/(u + _f), _f, oo).doit()
return u*focal_length/(u + focal_length)
def hyperfocal_distance(f, N, c):
"""
Parameters
==========
f: sympifiable
Focal length of a given lens
N: sympifiable
F-number of a given lens
c: sympifiable
Circle of Confusion (CoC) of a given image format
Example
=======
>>> from sympy.physics.optics import hyperfocal_distance
>>> from sympy.abc import f, N, c
>>> round(hyperfocal_distance(f = 0.5, N = 8, c = 0.0033), 2)
9.47
"""
f = sympify(f)
N = sympify(N)
c = sympify(c)
return (1/(N * c))*(f**2)
def transverse_magnification(si, so):
"""
Calculates the transverse magnification, which is the ratio of the
image size to the object size.
Parameters
==========
so: sympifiable
Lens-object distance
si: sympifiable
Lens-image distance
Example
=======
>>> from sympy.physics.optics import transverse_magnification
>>> transverse_magnification(30, 15)
-2
"""
si = sympify(si)
so = sympify(so)
return (-(si/so))
|
2bac52fc9c9368a1624aa0b672560725f5c78806c1910245075b2c0266724b6a | from sympy import symbols, S, log
from sympy.core.trace import Tr
from sympy.external import import_module
from sympy.physics.quantum.density import Density, entropy, fidelity
from sympy.physics.quantum.state import Ket, TimeDepKet
from sympy.physics.quantum.qubit import Qubit
from sympy.physics.quantum.represent import represent
from sympy.physics.quantum.dagger import Dagger
from sympy.physics.quantum.cartesian import XKet, PxKet, PxOp, XOp
from sympy.physics.quantum.spin import JzKet
from sympy.physics.quantum.operator import OuterProduct
from sympy.functions import sqrt
from sympy.utilities.pytest import raises, slow
from sympy.physics.quantum.matrixutils import scipy_sparse_matrix
from sympy.physics.quantum.tensorproduct import TensorProduct
def test_eval_args():
# check instance created
assert isinstance(Density([Ket(0), 0.5], [Ket(1), 0.5]), Density)
assert isinstance(Density([Qubit('00'), 1/sqrt(2)],
[Qubit('11'), 1/sqrt(2)]), Density)
#test if Qubit object type preserved
d = Density([Qubit('00'), 1/sqrt(2)], [Qubit('11'), 1/sqrt(2)])
for (state, prob) in d.args:
assert isinstance(state, Qubit)
# check for value error, when prob is not provided
raises(ValueError, lambda: Density([Ket(0)], [Ket(1)]))
def test_doit():
x, y = symbols('x y')
A, B, C, D, E, F = symbols('A B C D E F', commutative=False)
d = Density([XKet(), 0.5], [PxKet(), 0.5])
assert (0.5*(PxKet()*Dagger(PxKet())) +
0.5*(XKet()*Dagger(XKet()))) == d.doit()
# check for kets with expr in them
d_with_sym = Density([XKet(x*y), 0.5], [PxKet(x*y), 0.5])
assert (0.5*(PxKet(x*y)*Dagger(PxKet(x*y))) +
0.5*(XKet(x*y)*Dagger(XKet(x*y)))) == d_with_sym.doit()
d = Density([(A + B)*C, 1.0])
assert d.doit() == (1.0*A*C*Dagger(C)*Dagger(A) +
1.0*A*C*Dagger(C)*Dagger(B) +
1.0*B*C*Dagger(C)*Dagger(A) +
1.0*B*C*Dagger(C)*Dagger(B))
# With TensorProducts as args
# Density with simple tensor products as args
t = TensorProduct(A, B, C)
d = Density([t, 1.0])
assert d.doit() == \
1.0 * TensorProduct(A*Dagger(A), B*Dagger(B), C*Dagger(C))
# Density with multiple Tensorproducts as states
t2 = TensorProduct(A, B)
t3 = TensorProduct(C, D)
d = Density([t2, 0.5], [t3, 0.5])
assert d.doit() == (0.5 * TensorProduct(A*Dagger(A), B*Dagger(B)) +
0.5 * TensorProduct(C*Dagger(C), D*Dagger(D)))
#Density with mixed states
d = Density([t2 + t3, 1.0])
assert d.doit() == (1.0 * TensorProduct(A*Dagger(A), B*Dagger(B)) +
1.0 * TensorProduct(A*Dagger(C), B*Dagger(D)) +
1.0 * TensorProduct(C*Dagger(A), D*Dagger(B)) +
1.0 * TensorProduct(C*Dagger(C), D*Dagger(D)))
#Density operators with spin states
tp1 = TensorProduct(JzKet(1, 1), JzKet(1, -1))
d = Density([tp1, 1])
# full trace
t = Tr(d)
assert t.doit() == 1
#Partial trace on density operators with spin states
t = Tr(d, [0])
assert t.doit() == JzKet(1, -1) * Dagger(JzKet(1, -1))
t = Tr(d, [1])
assert t.doit() == JzKet(1, 1) * Dagger(JzKet(1, 1))
# with another spin state
tp2 = TensorProduct(JzKet(S(1)/2, S(1)/2), JzKet(S(1)/2, -S(1)/2))
d = Density([tp2, 1])
#full trace
t = Tr(d)
assert t.doit() == 1
#Partial trace on density operators with spin states
t = Tr(d, [0])
assert t.doit() == JzKet(S(1)/2, -S(1)/2) * Dagger(JzKet(S(1)/2, -S(1)/2))
t = Tr(d, [1])
assert t.doit() == JzKet(S(1)/2, S(1)/2) * Dagger(JzKet(S(1)/2, S(1)/2))
def test_apply_op():
d = Density([Ket(0), 0.5], [Ket(1), 0.5])
assert d.apply_op(XOp()) == Density([XOp()*Ket(0), 0.5],
[XOp()*Ket(1), 0.5])
def test_represent():
x, y = symbols('x y')
d = Density([XKet(), 0.5], [PxKet(), 0.5])
assert (represent(0.5*(PxKet()*Dagger(PxKet()))) +
represent(0.5*(XKet()*Dagger(XKet())))) == represent(d)
# check for kets with expr in them
d_with_sym = Density([XKet(x*y), 0.5], [PxKet(x*y), 0.5])
assert (represent(0.5*(PxKet(x*y)*Dagger(PxKet(x*y)))) +
represent(0.5*(XKet(x*y)*Dagger(XKet(x*y))))) == \
represent(d_with_sym)
# check when given explicit basis
assert (represent(0.5*(XKet()*Dagger(XKet())), basis=PxOp()) +
represent(0.5*(PxKet()*Dagger(PxKet())), basis=PxOp())) == \
represent(d, basis=PxOp())
def test_states():
d = Density([Ket(0), 0.5], [Ket(1), 0.5])
states = d.states()
assert states[0] == Ket(0) and states[1] == Ket(1)
def test_probs():
d = Density([Ket(0), .75], [Ket(1), 0.25])
probs = d.probs()
assert probs[0] == 0.75 and probs[1] == 0.25
#probs can be symbols
x, y = symbols('x y')
d = Density([Ket(0), x], [Ket(1), y])
probs = d.probs()
assert probs[0] == x and probs[1] == y
def test_get_state():
x, y = symbols('x y')
d = Density([Ket(0), x], [Ket(1), y])
states = (d.get_state(0), d.get_state(1))
assert states[0] == Ket(0) and states[1] == Ket(1)
def test_get_prob():
x, y = symbols('x y')
d = Density([Ket(0), x], [Ket(1), y])
probs = (d.get_prob(0), d.get_prob(1))
assert probs[0] == x and probs[1] == y
def test_entropy():
up = JzKet(S(1)/2, S(1)/2)
down = JzKet(S(1)/2, -S(1)/2)
d = Density((up, S(1)/2), (down, S(1)/2))
# test for density object
ent = entropy(d)
assert entropy(d) == log(2)/2
assert d.entropy() == log(2)/2
np = import_module('numpy', min_module_version='1.4.0')
if np:
#do this test only if 'numpy' is available on test machine
np_mat = represent(d, format='numpy')
ent = entropy(np_mat)
assert isinstance(np_mat, np.matrixlib.defmatrix.matrix)
assert ent.real == 0.69314718055994529
assert ent.imag == 0
scipy = import_module('scipy', __import__kwargs={'fromlist': ['sparse']})
if scipy and np:
#do this test only if numpy and scipy are available
mat = represent(d, format="scipy.sparse")
assert isinstance(mat, scipy_sparse_matrix)
assert ent.real == 0.69314718055994529
assert ent.imag == 0
def test_eval_trace():
up = JzKet(S(1)/2, S(1)/2)
down = JzKet(S(1)/2, -S(1)/2)
d = Density((up, 0.5), (down, 0.5))
t = Tr(d)
assert t.doit() == 1
#test dummy time dependent states
class TestTimeDepKet(TimeDepKet):
def _eval_trace(self, bra, **options):
return 1
x, t = symbols('x t')
k1 = TestTimeDepKet(0, 0.5)
k2 = TestTimeDepKet(0, 1)
d = Density([k1, 0.5], [k2, 0.5])
assert d.doit() == (0.5 * OuterProduct(k1, k1.dual) +
0.5 * OuterProduct(k2, k2.dual))
t = Tr(d)
assert t.doit() == 1
def test_fidelity():
#test with kets
up = JzKet(S(1)/2, S(1)/2)
down = JzKet(S(1)/2, -S(1)/2)
updown = (S(1)/sqrt(2))*up + (S(1)/sqrt(2))*down
#check with matrices
up_dm = represent(up * Dagger(up))
down_dm = represent(down * Dagger(down))
updown_dm = represent(updown * Dagger(updown))
assert abs(fidelity(up_dm, up_dm) - 1) < 1e-3
assert fidelity(up_dm, down_dm) < 1e-3
assert abs(fidelity(up_dm, updown_dm) - (S(1)/sqrt(2))) < 1e-3
assert abs(fidelity(updown_dm, down_dm) - (S(1)/sqrt(2))) < 1e-3
#check with density
up_dm = Density([up, 1.0])
down_dm = Density([down, 1.0])
updown_dm = Density([updown, 1.0])
assert abs(fidelity(up_dm, up_dm) - 1) < 1e-3
assert abs(fidelity(up_dm, down_dm)) < 1e-3
assert abs(fidelity(up_dm, updown_dm) - (S(1)/sqrt(2))) < 1e-3
assert abs(fidelity(updown_dm, down_dm) - (S(1)/sqrt(2))) < 1e-3
#check mixed states with density
updown2 = (sqrt(3)/2)*up + (S(1)/2)*down
d1 = Density([updown, 0.25], [updown2, 0.75])
d2 = Density([updown, 0.75], [updown2, 0.25])
assert abs(fidelity(d1, d2) - 0.991) < 1e-3
assert abs(fidelity(d2, d1) - fidelity(d1, d2)) < 1e-3
#using qubits/density(pure states)
state1 = Qubit('0')
state2 = Qubit('1')
state3 = (S(1)/sqrt(2))*state1 + (S(1)/sqrt(2))*state2
state4 = (sqrt(S(2)/3))*state1 + (S(1)/sqrt(3))*state2
state1_dm = Density([state1, 1])
state2_dm = Density([state2, 1])
state3_dm = Density([state3, 1])
assert fidelity(state1_dm, state1_dm) == 1
assert fidelity(state1_dm, state2_dm) == 0
assert abs(fidelity(state1_dm, state3_dm) - 1/sqrt(2)) < 1e-3
assert abs(fidelity(state3_dm, state2_dm) - 1/sqrt(2)) < 1e-3
#using qubits/density(mixed states)
d1 = Density([state3, 0.70], [state4, 0.30])
d2 = Density([state3, 0.20], [state4, 0.80])
assert abs(fidelity(d1, d1) - 1) < 1e-3
assert abs(fidelity(d1, d2) - 0.996) < 1e-3
assert abs(fidelity(d1, d2) - fidelity(d2, d1)) < 1e-3
#TODO: test for invalid arguments
# non-square matrix
mat1 = [[0, 0],
[0, 0],
[0, 0]]
mat2 = [[0, 0],
[0, 0]]
raises(ValueError, lambda: fidelity(mat1, mat2))
# unequal dimensions
mat1 = [[0, 0],
[0, 0]]
mat2 = [[0, 0, 0],
[0, 0, 0],
[0, 0, 0]]
raises(ValueError, lambda: fidelity(mat1, mat2))
# unsupported data-type
x, y = 1, 2 # random values that is not a matrix
raises(ValueError, lambda: fidelity(x, y))
|
39c71cf462897a2f90e1d63ab55e2b8d21d1d49660e6c998bf9f59b1f7a6ab4d | from sympy.physics.quantum.qasm import Qasm, prod, flip_index, trim,\
get_index, nonblank, fullsplit, fixcommand, stripquotes, read_qasm
from sympy.physics.quantum.gate import X, Z, H, S, T
from sympy.physics.quantum.gate import CNOT, SWAP, CPHASE, CGate, CGateS
from sympy.physics.quantum.circuitplot import Mz, CreateOneQubitGate, CreateCGate
def test_qasm_readqasm():
qasm_lines = """\
qubit q_0
qubit q_1
h q_0
cnot q_0,q_1
"""
q = read_qasm(qasm_lines)
assert q.get_circuit() == CNOT(1,0)*H(1)
def test_qasm_ex1():
q = Qasm('qubit q0', 'qubit q1', 'h q0', 'cnot q0,q1')
assert q.get_circuit() == CNOT(1,0)*H(1)
def test_qasm_ex1_methodcalls():
q = Qasm()
q.qubit('q_0')
q.qubit('q_1')
q.h('q_0')
q.cnot('q_0', 'q_1')
assert q.get_circuit() == CNOT(1,0)*H(1)
def test_qasm_swap():
q = Qasm('qubit q0', 'qubit q1', 'cnot q0,q1', 'cnot q1,q0', 'cnot q0,q1')
assert q.get_circuit() == CNOT(1,0)*CNOT(0,1)*CNOT(1,0)
def test_qasm_ex2():
q = Qasm('qubit q_0', 'qubit q_1', 'qubit q_2', 'h q_1',
'cnot q_1,q_2', 'cnot q_0,q_1', 'h q_0',
'measure q_1', 'measure q_0',
'c-x q_1,q_2', 'c-z q_0,q_2')
assert q.get_circuit() == CGate(2,Z(0))*CGate(1,X(0))*Mz(2)*Mz(1)*H(2)*CNOT(2,1)*CNOT(1,0)*H(1)
def test_qasm_1q():
for symbol, gate in [('x', X), ('z', Z), ('h', H), ('s', S), ('t', T), ('measure', Mz)]:
q = Qasm('qubit q_0', '%s q_0' % symbol)
assert q.get_circuit() == gate(0)
def test_qasm_2q():
for symbol, gate in [('cnot', CNOT), ('swap', SWAP), ('cphase', CPHASE)]:
q = Qasm('qubit q_0', 'qubit q_1', '%s q_0,q_1' % symbol)
assert q.get_circuit() == gate(1,0)
def test_qasm_3q():
q = Qasm('qubit q0', 'qubit q1', 'qubit q2', 'toffoli q2,q1,q0')
assert q.get_circuit() == CGateS((0,1),X(2))
def test_qasm_prod():
assert prod([1, 2, 3]) == 6
assert prod([H(0), X(1)])== H(0)*X(1)
def test_qasm_flip_index():
assert flip_index(0, 2) == 1
assert flip_index(1, 2) == 0
def test_qasm_trim():
assert trim('nothing happens here') == 'nothing happens here'
assert trim("Something #happens here") == "Something "
def test_qasm_get_index():
assert get_index('q0', ['q0', 'q1']) == 1
assert get_index('q1', ['q0', 'q1']) == 0
def test_qasm_nonblank():
assert list(nonblank('abcd')) == list('abcd')
assert list(nonblank('abc ')) == list('abc')
def test_qasm_fullsplit():
assert fullsplit('g q0,q1,q2, q3') == ('g', ['q0', 'q1', 'q2', 'q3'])
def test_qasm_fixcommand():
assert fixcommand('foo') == 'foo'
assert fixcommand('def') == 'qdef'
def test_qasm_stripquotes():
assert stripquotes("'S'") == 'S'
assert stripquotes('"S"') == 'S'
assert stripquotes('S') == 'S'
def test_qasm_qdef():
# weaker test condition (str) since we don't have access to the actual class
q = Qasm("def Q,0,Q",'qubit q0','Q q0')
assert str(q.get_circuit()) == 'Q(0)'
q = Qasm("def CQ,1,Q", 'qubit q0', 'qubit q1', 'CQ q0,q1')
assert str(q.get_circuit()) == 'C((1),Q(0))'
|
1c29c37a69c50f5af70c84f8a169f2a5cb192af175040f7afcc3181c4ed0ff1a | from sympy.core.backend import symbols
from sympy.physics.mechanics import dynamicsymbols
from sympy.physics.mechanics import ReferenceFrame, Point, Particle
from sympy.physics.mechanics import LagrangesMethod, Lagrangian
### This test asserts that a system with more than one external forces
### is acurately formed with Lagrange method (see issue #8626)
def test_lagrange_2forces():
### Equations for two damped springs in serie with two forces
### generalized coordinates
q1, q2 = dynamicsymbols('q1, q2')
### generalized speeds
q1d, q2d = dynamicsymbols('q1, q2', 1)
### Mass, spring strength, friction coefficient
m, k, nu = symbols('m, k, nu')
N = ReferenceFrame('N')
O = Point('O')
### Two points
P1 = O.locatenew('P1', q1 * N.x)
P1.set_vel(N, q1d * N.x)
P2 = O.locatenew('P1', q2 * N.x)
P2.set_vel(N, q2d * N.x)
pP1 = Particle('pP1', P1, m)
pP1.potential_energy = k * q1**2 / 2
pP2 = Particle('pP2', P2, m)
pP2.potential_energy = k * (q1 - q2)**2 / 2
#### Friction forces
forcelist = [(P1, - nu * q1d * N.x),
(P2, - nu * q2d * N.x)]
lag = Lagrangian(N, pP1, pP2)
l_method = LagrangesMethod(lag, (q1, q2), forcelist=forcelist, frame=N)
l_method.form_lagranges_equations()
eq1 = l_method.eom[0]
assert eq1.diff(q1d) == nu
eq2 = l_method.eom[1]
assert eq2.diff(q2d) == nu
|
e4bd23c13dafd9ce0c0ee0fafa4adcbaaf1d3acd86a85771cd891de2a22f3e08 | from sympy import (Abs, Add, Basic, Function, Number, Rational, S, Symbol,
diff, exp, integrate, log, sin, sqrt, symbols)
from sympy.physics.units import (amount_of_substance, convert_to, find_unit,
volume)
from sympy.physics.units.definitions import (amu, au, centimeter, coulomb,
day, energy, foot, grams, hour, inch, kg, km, m, meter, mile, millimeter,
minute, pressure, quart, s, second, speed_of_light, temperature, bit,
byte, kibibyte, mebibyte, gibibyte, tebibyte, pebibyte, exbibyte,
kilogram, gravitational_constant)
from sympy.physics.units.dimensions import Dimension, charge, length, time, dimsys_default
from sympy.physics.units.prefixes import PREFIXES, kilo
from sympy.physics.units.quantities import Quantity
from sympy.utilities.pytest import XFAIL, raises, warns_deprecated_sympy
k = PREFIXES["k"]
def test_str_repr():
assert str(kg) == "kilogram"
def test_eq():
# simple test
assert 10*m == 10*m
assert 10*m != 10*s
def test_convert_to():
q = Quantity("q1")
q.set_dimension(length)
q.set_scale_factor(S(5000))
assert q.convert_to(m) == 5000*m
assert speed_of_light.convert_to(m / s) == 299792458 * m / s
# TODO: eventually support this kind of conversion:
# assert (2*speed_of_light).convert_to(m / s) == 2 * 299792458 * m / s
assert day.convert_to(s) == 86400*s
# Wrong dimension to convert:
assert q.convert_to(s) == q
assert speed_of_light.convert_to(m) == speed_of_light
def test_Quantity_definition():
q = Quantity("s10", abbrev="sabbr")
q.set_dimension(time)
q.set_scale_factor(10)
u = Quantity("u", abbrev="dam")
u.set_dimension(length)
u.set_scale_factor(10)
km = Quantity("km")
km.set_dimension(length)
km.set_scale_factor(kilo)
v = Quantity("u")
v.set_dimension(length)
v.set_scale_factor(5*kilo)
assert q.scale_factor == 10
assert q.dimension == time
assert q.abbrev == Symbol("sabbr")
assert u.dimension == length
assert u.scale_factor == 10
assert u.abbrev == Symbol("dam")
assert km.scale_factor == 1000
assert km.func(*km.args) == km
assert km.func(*km.args).args == km.args
assert v.dimension == length
assert v.scale_factor == 5000
with warns_deprecated_sympy():
Quantity('invalid', 'dimension', 1)
with warns_deprecated_sympy():
Quantity('mismatch', dimension=length, scale_factor=kg)
def test_abbrev():
u = Quantity("u")
u.set_dimension(length)
u.set_scale_factor(S.One)
assert u.name == Symbol("u")
assert u.abbrev == Symbol("u")
u = Quantity("u", abbrev="om")
u.set_dimension(length)
u.set_scale_factor(S(2))
assert u.name == Symbol("u")
assert u.abbrev == Symbol("om")
assert u.scale_factor == 2
assert isinstance(u.scale_factor, Number)
u = Quantity("u", abbrev="ikm")
u.set_dimension(length)
u.set_scale_factor(3*kilo)
assert u.abbrev == Symbol("ikm")
assert u.scale_factor == 3000
def test_print():
u = Quantity("unitname", abbrev="dam")
assert repr(u) == "unitname"
assert str(u) == "unitname"
def test_Quantity_eq():
u = Quantity("u", abbrev="dam")
v = Quantity("v1")
assert u != v
v = Quantity("v2", abbrev="ds")
assert u != v
v = Quantity("v3", abbrev="dm")
assert u != v
def test_add_sub():
u = Quantity("u")
v = Quantity("v")
w = Quantity("w")
u.set_dimension(length)
v.set_dimension(length)
w.set_dimension(time)
u.set_scale_factor(S(10))
v.set_scale_factor(S(5))
w.set_scale_factor(S(2))
assert isinstance(u + v, Add)
assert (u + v.convert_to(u)) == (1 + S.Half)*u
# TODO: eventually add this:
# assert (u + v).convert_to(u) == (1 + S.Half)*u
assert isinstance(u - v, Add)
assert (u - v.convert_to(u)) == S.Half*u
# TODO: eventually add this:
# assert (u - v).convert_to(u) == S.Half*u
def test_quantity_abs():
v_w1 = Quantity('v_w1')
v_w2 = Quantity('v_w2')
v_w3 = Quantity('v_w3')
v_w1.set_dimension(length/time)
v_w2.set_dimension(length/time)
v_w3.set_dimension(length/time)
v_w1.set_scale_factor(meter/second)
v_w2.set_scale_factor(meter/second)
v_w3.set_scale_factor(meter/second)
expr = v_w3 - Abs(v_w1 - v_w2)
Dq = Dimension(Quantity.get_dimensional_expr(expr))
assert dimsys_default.get_dimensional_dependencies(Dq) == {
'length': 1,
'time': -1,
}
assert meter == sqrt(meter**2)
def test_check_unit_consistency():
u = Quantity("u")
v = Quantity("v")
w = Quantity("w")
u.set_dimension(length)
v.set_dimension(length)
w.set_dimension(time)
u.set_scale_factor(S(10))
v.set_scale_factor(S(5))
w.set_scale_factor(S(2))
def check_unit_consistency(expr):
Quantity._collect_factor_and_dimension(expr)
raises(ValueError, lambda: check_unit_consistency(u + w))
raises(ValueError, lambda: check_unit_consistency(u - w))
raises(ValueError, lambda: check_unit_consistency(u + 1))
raises(ValueError, lambda: check_unit_consistency(u - 1))
raises(ValueError, lambda: check_unit_consistency(1 - exp(u / w)))
def test_mul_div():
u = Quantity("u")
v = Quantity("v")
t = Quantity("t")
ut = Quantity("ut")
v2 = Quantity("v")
u.set_dimension(length)
v.set_dimension(length)
t.set_dimension(time)
ut.set_dimension(length*time)
v2.set_dimension(length/time)
u.set_scale_factor(S(10))
v.set_scale_factor(S(5))
t.set_scale_factor(S(2))
ut.set_scale_factor(S(20))
v2.set_scale_factor(S(5))
assert 1 / u == u**(-1)
assert u / 1 == u
v1 = u / t
v2 = v
# Pow only supports structural equality:
assert v1 != v2
assert v1 == v2.convert_to(v1)
# TODO: decide whether to allow such expression in the future
# (requires somehow manipulating the core).
# assert u / Quantity('l2', dimension=length, scale_factor=2) == 5
assert u * 1 == u
ut1 = u * t
ut2 = ut
# Mul only supports structural equality:
assert ut1 != ut2
assert ut1 == ut2.convert_to(ut1)
# Mul only supports structural equality:
lp1 = Quantity("lp1")
lp1.set_dimension(length**-1)
lp1.set_scale_factor(S(2))
assert u * lp1 != 20
assert u**0 == 1
assert u**1 == u
# TODO: Pow only support structural equality:
u2 = Quantity("u2")
u3 = Quantity("u3")
u2.set_dimension(length**2)
u3.set_dimension(length**-1)
u2.set_scale_factor(S(100))
u3.set_scale_factor(S(1)/10)
assert u ** 2 != u2
assert u ** -1 != u3
assert u ** 2 == u2.convert_to(u)
assert u ** -1 == u3.convert_to(u)
def test_units():
assert convert_to((5*m/s * day) / km, 1) == 432
assert convert_to(foot / meter, meter) == Rational(3048, 10000)
# amu is a pure mass so mass/mass gives a number, not an amount (mol)
# TODO: need better simplification routine:
assert str(convert_to(grams/amu, grams).n(2)) == '6.0e+23'
# Light from the sun needs about 8.3 minutes to reach earth
t = (1*au / speed_of_light) / minute
# TODO: need a better way to simplify expressions containing units:
t = convert_to(convert_to(t, meter / minute), meter)
assert t == S(49865956897)/5995849160
# TODO: fix this, it should give `m` without `Abs`
assert sqrt(m**2) == Abs(m)
assert (sqrt(m))**2 == m
t = Symbol('t')
assert integrate(t*m/s, (t, 1*s, 5*s)) == 12*m*s
assert (t * m/s).integrate((t, 1*s, 5*s)) == 12*m*s
def test_issue_quart():
assert convert_to(4 * quart / inch ** 3, meter) == 231
assert convert_to(4 * quart / inch ** 3, millimeter) == 231
def test_issue_5565():
assert (m < s).is_Relational
def test_find_unit():
assert find_unit('coulomb') == ['coulomb', 'coulombs', 'coulomb_constant']
assert find_unit(coulomb) == ['C', 'coulomb', 'coulombs', 'planck_charge', 'elementary_charge']
assert find_unit(charge) == ['C', 'coulomb', 'coulombs', 'planck_charge', 'elementary_charge']
assert find_unit(inch) == [
'm', 'au', 'cm', 'dm', 'ft', 'km', 'ly', 'mi', 'mm', 'nm', 'pm', 'um',
'yd', 'nmi', 'feet', 'foot', 'inch', 'mile', 'yard', 'meter', 'miles',
'yards', 'inches', 'meters', 'micron', 'microns', 'decimeter',
'kilometer', 'lightyear', 'nanometer', 'picometer', 'centimeter',
'decimeters', 'kilometers', 'lightyears', 'micrometer', 'millimeter',
'nanometers', 'picometers', 'centimeters', 'micrometers',
'millimeters', 'nautical_mile', 'planck_length', 'nautical_miles', 'astronomical_unit',
'astronomical_units']
assert find_unit(inch**-1) == ['D', 'dioptre', 'optical_power']
assert find_unit(length**-1) == ['D', 'dioptre', 'optical_power']
assert find_unit(inch ** 3) == [
'l', 'cl', 'dl', 'ml', 'liter', 'quart', 'liters', 'quarts',
'deciliter', 'centiliter', 'deciliters', 'milliliter',
'centiliters', 'milliliters', 'planck_volume']
assert find_unit('voltage') == ['V', 'v', 'volt', 'volts', 'planck_voltage']
def test_Quantity_derivative():
x = symbols("x")
assert diff(x*meter, x) == meter
assert diff(x**3*meter**2, x) == 3*x**2*meter**2
assert diff(meter, meter) == 1
assert diff(meter**2, meter) == 2*meter
def test_quantity_postprocessing():
q1 = Quantity('q1')
q2 = Quantity('q2')
q1.set_dimension(length*pressure**2*temperature/time)
q2.set_dimension(energy*pressure*temperature/(length**2*time))
assert q1 + q2
q = q1 + q2
Dq = Dimension(Quantity.get_dimensional_expr(q))
assert dimsys_default.get_dimensional_dependencies(Dq) == {
'length': -1,
'mass': 2,
'temperature': 1,
'time': -5,
}
def test_factor_and_dimension():
assert (3000, Dimension(1)) == Quantity._collect_factor_and_dimension(3000)
assert (1001, length) == Quantity._collect_factor_and_dimension(meter + km)
assert (2, length/time) == Quantity._collect_factor_and_dimension(
meter/second + 36*km/(10*hour))
x, y = symbols('x y')
assert (x + y/100, length) == Quantity._collect_factor_and_dimension(
x*m + y*centimeter)
cH = Quantity('cH')
cH.set_dimension(amount_of_substance/volume)
pH = -log(cH)
assert (1, volume/amount_of_substance) == Quantity._collect_factor_and_dimension(
exp(pH))
v_w1 = Quantity('v_w1')
v_w2 = Quantity('v_w2')
v_w1.set_dimension(length/time)
v_w2.set_dimension(length/time)
v_w1.set_scale_factor(S(3)/2*meter/second)
v_w2.set_scale_factor(2*meter/second)
expr = Abs(v_w1/2 - v_w2)
assert (S(5)/4, length/time) == \
Quantity._collect_factor_and_dimension(expr)
expr = S(5)/2*second/meter*v_w1 - 3000
assert (-(2996 + S(1)/4), Dimension(1)) == \
Quantity._collect_factor_and_dimension(expr)
expr = v_w1**(v_w2/v_w1)
assert ((S(3)/2)**(S(4)/3), (length/time)**(S(4)/3)) == \
Quantity._collect_factor_and_dimension(expr)
@XFAIL
def test_factor_and_dimension_with_Abs():
with warns_deprecated_sympy():
v_w1 = Quantity('v_w1', length/time, S(3)/2*meter/second)
v_w1.set_dimension(length/time)
v_w1.set_scale_factor(S(3)/2*meter/second)
expr = v_w1 - Abs(v_w1)
assert (0, length/time) == Quantity._collect_factor_and_dimension(expr)
def test_dimensional_expr_of_derivative():
l = Quantity('l')
t = Quantity('t')
t1 = Quantity('t1')
l.set_dimension(length)
t.set_dimension(time)
t1.set_dimension(time)
l.set_scale_factor(36*km)
t.set_scale_factor(hour)
t1.set_scale_factor(second)
x = Symbol('x')
y = Symbol('y')
f = Function('f')
dfdx = f(x, y).diff(x, y)
dl_dt = dfdx.subs({f(x, y): l, x: t, y: t1})
assert Quantity.get_dimensional_expr(dl_dt) ==\
Quantity.get_dimensional_expr(l / t / t1) ==\
Symbol("length")/Symbol("time")**2
assert Quantity._collect_factor_and_dimension(dl_dt) ==\
Quantity._collect_factor_and_dimension(l / t / t1) ==\
(10, length/time**2)
def test_get_dimensional_expr_with_function():
v_w1 = Quantity('v_w1')
v_w2 = Quantity('v_w2')
v_w1.set_dimension(length/time)
v_w2.set_dimension(length/time)
v_w1.set_scale_factor(meter/second)
v_w2.set_scale_factor(meter/second)
assert Quantity.get_dimensional_expr(sin(v_w1)) == \
sin(Quantity.get_dimensional_expr(v_w1))
assert Quantity.get_dimensional_expr(sin(v_w1/v_w2)) == 1
def test_binary_information():
assert convert_to(kibibyte, byte) == 1024*byte
assert convert_to(mebibyte, byte) == 1024**2*byte
assert convert_to(gibibyte, byte) == 1024**3*byte
assert convert_to(tebibyte, byte) == 1024**4*byte
assert convert_to(pebibyte, byte) == 1024**5*byte
assert convert_to(exbibyte, byte) == 1024**6*byte
assert kibibyte.convert_to(bit) == 8*1024*bit
assert byte.convert_to(bit) == 8*bit
a = 10*kibibyte*hour
assert convert_to(a, byte) == 10240*byte*hour
assert convert_to(a, minute) == 600*kibibyte*minute
assert convert_to(a, [byte, minute]) == 614400*byte*minute
def test_eval_subs():
energy, mass, force = symbols('energy mass force')
expr1 = energy/mass
units = {energy: kilogram*meter**2/second**2, mass: kilogram}
assert expr1.subs(units) == meter**2/second**2
expr2 = force/mass
units = {force:gravitational_constant*kilogram**2/meter**2, mass:kilogram}
assert expr2.subs(units) == gravitational_constant*kilogram/meter**2
def test_issue_14932():
assert (log(inch) - log(2)).simplify() == log(inch/2)
assert (log(inch) - log(foot)).simplify() == -log(12)
p = symbols('p', positive=True)
assert (log(inch) - log(p)).simplify() == log(inch/p)
def test_issue_14547():
# the root issue is that an argument with dimensions should
# not raise an error when the the `arg - 1` calculation is
# performed in the assumptions system
from sympy.physics.units import foot, inch
from sympy import Eq
assert log(foot).is_zero is None
assert log(foot).is_positive is None
assert log(foot).is_nonnegative is None
assert log(foot).is_negative is None
assert log(foot).is_algebraic is None
assert log(foot).is_rational is None
# doesn't raise error
assert Eq(log(foot), log(inch)) is not None # might be False or unevaluated
x = Symbol('x')
e = foot + x
assert e.is_Add and set(e.args) == {foot, x}
e = foot + 1
assert e.is_Add and set(e.args) == {foot, 1}
|
3e03d4a65281627c60c6801e91cfd9b793d62444faed2314b263aeb3d6249b05 | from sympy.utilities.pytest import warns_deprecated_sympy
from sympy import (Add, Mul, Pow, Tuple, pi, sin, sqrt, sstr, sympify,
symbols)
from sympy.physics.units import (
G, centimeter, coulomb, day, degree, gram, hbar, hour, inch, joule, kelvin,
kilogram, kilometer, length, meter, mile, minute, newton, planck,
planck_length, planck_mass, planck_temperature, planck_time, radians,
second, speed_of_light, steradian, time, km)
from sympy.physics.units.dimensions import dimsys_default
from sympy.physics.units.util import convert_to, dim_simplify, check_dimensions
from sympy.utilities.pytest import raises
def NS(e, n=15, **options):
return sstr(sympify(e).evalf(n, **options), full_prec=True)
L = length
T = time
def test_dim_simplify_add():
with warns_deprecated_sympy():
assert dim_simplify(Add(L, L)) == L
with warns_deprecated_sympy():
assert dim_simplify(L + L) == L
def test_dim_simplify_mul():
with warns_deprecated_sympy():
assert dim_simplify(Mul(L, T)) == L*T
with warns_deprecated_sympy():
assert dim_simplify(L*T) == L*T
def test_dim_simplify_pow():
with warns_deprecated_sympy():
assert dim_simplify(Pow(L, 2)) == L**2
with warns_deprecated_sympy():
assert dim_simplify(L**2) == L**2
def test_dim_simplify_rec():
with warns_deprecated_sympy():
assert dim_simplify(Mul(Add(L, L), T)) == L*T
with warns_deprecated_sympy():
assert dim_simplify((L + L) * T) == L*T
def test_dim_simplify_dimless():
# TODO: this should be somehow simplified on its own,
# without the need of calling `dim_simplify`:
with warns_deprecated_sympy():
assert dim_simplify(sin(L*L**-1)**2*L).get_dimensional_dependencies()\
== dimsys_default.get_dimensional_dependencies(L)
with warns_deprecated_sympy():
assert dim_simplify(sin(L * L**(-1))**2 * L).get_dimensional_dependencies()\
== dimsys_default.get_dimensional_dependencies(L)
def test_convert_to_quantities():
assert convert_to(3, meter) == 3
assert convert_to(mile, kilometer) == 25146*kilometer/15625
assert convert_to(meter/second, speed_of_light) == speed_of_light/299792458
assert convert_to(299792458*meter/second, speed_of_light) == speed_of_light
assert convert_to(2*299792458*meter/second, speed_of_light) == 2*speed_of_light
assert convert_to(speed_of_light, meter/second) == 299792458*meter/second
assert convert_to(2*speed_of_light, meter/second) == 599584916*meter/second
assert convert_to(day, second) == 86400*second
assert convert_to(2*hour, minute) == 120*minute
assert convert_to(mile, meter) == 201168*meter/125
assert convert_to(mile/hour, kilometer/hour) == 25146*kilometer/(15625*hour)
assert convert_to(3*newton, meter/second) == 3*newton
assert convert_to(3*newton, kilogram*meter/second**2) == 3*meter*kilogram/second**2
assert convert_to(kilometer + mile, meter) == 326168*meter/125
assert convert_to(2*kilometer + 3*mile, meter) == 853504*meter/125
assert convert_to(inch**2, meter**2) == 16129*meter**2/25000000
assert convert_to(3*inch**2, meter) == 48387*meter**2/25000000
assert convert_to(2*kilometer/hour + 3*mile/hour, meter/second) == 53344*meter/(28125*second)
assert convert_to(2*kilometer/hour + 3*mile/hour, centimeter/second) == 213376*centimeter/(1125*second)
assert convert_to(kilometer * (mile + kilometer), meter) == 2609344 * meter ** 2
assert convert_to(steradian, coulomb) == steradian
assert convert_to(radians, degree) == 180*degree/pi
assert convert_to(radians, [meter, degree]) == 180*degree/pi
assert convert_to(pi*radians, degree) == 180*degree
assert convert_to(pi, degree) == 180*degree
def test_convert_to_tuples_of_quantities():
assert convert_to(speed_of_light, [meter, second]) == 299792458 * meter / second
assert convert_to(speed_of_light, (meter, second)) == 299792458 * meter / second
assert convert_to(speed_of_light, Tuple(meter, second)) == 299792458 * meter / second
assert convert_to(joule, [meter, kilogram, second]) == kilogram*meter**2/second**2
assert convert_to(joule, [centimeter, gram, second]) == 10000000*centimeter**2*gram/second**2
assert convert_to(299792458*meter/second, [speed_of_light]) == speed_of_light
assert convert_to(speed_of_light / 2, [meter, second, kilogram]) == meter/second*299792458 / 2
# This doesn't make physically sense, but let's keep it as a conversion test:
assert convert_to(2 * speed_of_light, [meter, second, kilogram]) == 2 * 299792458 * meter / second
assert convert_to(G, [G, speed_of_light, planck]) == 1.0*G
assert NS(convert_to(meter, [G, speed_of_light, hbar]), n=7) == '6.187142e+34*gravitational_constant**0.5000000*hbar**0.5000000*speed_of_light**(-1.500000)'
assert NS(convert_to(planck_mass, kilogram), n=7) == '2.176434e-8*kilogram'
assert NS(convert_to(planck_length, meter), n=7) == '1.616255e-35*meter'
assert NS(convert_to(planck_time, second), n=6) == '5.39125e-44*second'
assert NS(convert_to(planck_temperature, kelvin), n=7) == '1.416784e+32*kelvin'
assert NS(convert_to(convert_to(meter, [G, speed_of_light, planck]), meter), n=10) == '1.000000000*meter'
def test_eval_simplify():
from sympy.physics.units import cm, mm, km, m, K, Quantity, kilo, foot
from sympy.simplify.simplify import simplify
from sympy.core.symbol import symbols
from sympy.utilities.pytest import raises
from sympy.core.function import Lambda
x, y = symbols('x y')
assert ((cm/mm).simplify()) == 10
assert ((km/m).simplify()) == 1000
assert ((km/cm).simplify()) == 100000
assert ((10*x*K*km**2/m/cm).simplify()) == 1000000000*x*kelvin
assert ((cm/km/m).simplify()) == 1/(10000000*centimeter)
assert (3*kilo*meter).simplify() == 3000*meter
assert (4*kilo*meter/(2*kilometer)).simplify() == 2
assert (4*kilometer**2/(kilo*meter)**2).simplify() == 4
def test_quantity_simplify():
from sympy.physics.units.util import quantity_simplify
from sympy.physics.units import kilo, foot
from sympy.core.symbol import symbols
x, y = symbols('x y')
assert quantity_simplify(x*(8*kilo*newton*meter + y)) == x*(8000*meter*newton + y)
assert quantity_simplify(foot*inch*(foot + inch)) == foot**2*(foot + foot/12)/12
assert quantity_simplify(foot*inch*(foot*foot + inch*(foot + inch))) == foot**2*(foot**2 + foot/12*(foot + foot/12))/12
assert quantity_simplify(2**(foot/inch*kilo/1000)*inch) == 4096*foot/12
assert quantity_simplify(foot**2*inch + inch**2*foot) == 13*foot**3/144
def test_check_dimensions():
x = symbols('x')
assert check_dimensions(inch + x) == inch + x
assert check_dimensions(length + x) == length + x
# after subs we get 2*length; check will clear the constant
assert check_dimensions((length + x).subs(x, length)) == length
raises(ValueError, lambda: check_dimensions(inch + 1))
raises(ValueError, lambda: check_dimensions(length + 1))
raises(ValueError, lambda: check_dimensions(length + time))
raises(ValueError, lambda: check_dimensions(meter + second))
raises(ValueError, lambda: check_dimensions(2 * meter + second))
raises(ValueError, lambda: check_dimensions(2 * meter + 3 * second))
raises(ValueError, lambda: check_dimensions(1 / second + 1 / meter))
raises(ValueError, lambda: check_dimensions(2 * meter*(mile + centimeter) + km))
|
69cd1d73e7f165910e1bfab493c64545355da518ce7348cfcf610084388c3b04 | from sympy import Matrix
from sympy.tensor.tensor import tensor_indices, TensorHead, tensor_heads, \
TensExpr, canon_bp
from sympy import eye
from sympy.physics.hep.gamma_matrices import GammaMatrix as G, LorentzIndex, \
kahane_simplify, gamma_trace, _simplify_single_line, simplify_gamma_expression
def _is_tensor_eq(arg1, arg2):
arg1 = canon_bp(arg1)
arg2 = canon_bp(arg2)
if isinstance(arg1, TensExpr):
return arg1.equals(arg2)
elif isinstance(arg2, TensExpr):
return arg2.equals(arg1)
return arg1 == arg2
def execute_gamma_simplify_tests_for_function(tfunc, D):
"""
Perform tests to check if sfunc is able to simplify gamma matrix expressions.
Parameters
==========
`sfunc` a function to simplify a `TIDS`, shall return the simplified `TIDS`.
`D` the number of dimension (in most cases `D=4`).
"""
mu, nu, rho, sigma = tensor_indices("mu, nu, rho, sigma", LorentzIndex)
a1, a2, a3, a4, a5, a6 = tensor_indices("a1:7", LorentzIndex)
mu11, mu12, mu21, mu31, mu32, mu41, mu51, mu52 = tensor_indices("mu11, mu12, mu21, mu31, mu32, mu41, mu51, mu52", LorentzIndex)
mu61, mu71, mu72 = tensor_indices("mu61, mu71, mu72", LorentzIndex)
m0, m1, m2, m3, m4, m5, m6 = tensor_indices("m0:7", LorentzIndex)
def g(xx, yy):
return (G(xx)*G(yy) + G(yy)*G(xx))/2
# Some examples taken from Kahane's paper, 4 dim only:
if D == 4:
t = (G(a1)*G(mu11)*G(a2)*G(mu21)*G(-a1)*G(mu31)*G(-a2))
assert _is_tensor_eq(tfunc(t), -4*G(mu11)*G(mu31)*G(mu21) - 4*G(mu31)*G(mu11)*G(mu21))
t = (G(a1)*G(mu11)*G(mu12)*\
G(a2)*G(mu21)*\
G(a3)*G(mu31)*G(mu32)*\
G(a4)*G(mu41)*\
G(-a2)*G(mu51)*G(mu52)*\
G(-a1)*G(mu61)*\
G(-a3)*G(mu71)*G(mu72)*\
G(-a4))
assert _is_tensor_eq(tfunc(t), \
16*G(mu31)*G(mu32)*G(mu72)*G(mu71)*G(mu11)*G(mu52)*G(mu51)*G(mu12)*G(mu61)*G(mu21)*G(mu41) + 16*G(mu31)*G(mu32)*G(mu72)*G(mu71)*G(mu12)*G(mu51)*G(mu52)*G(mu11)*G(mu61)*G(mu21)*G(mu41) + 16*G(mu71)*G(mu72)*G(mu32)*G(mu31)*G(mu11)*G(mu52)*G(mu51)*G(mu12)*G(mu61)*G(mu21)*G(mu41) + 16*G(mu71)*G(mu72)*G(mu32)*G(mu31)*G(mu12)*G(mu51)*G(mu52)*G(mu11)*G(mu61)*G(mu21)*G(mu41))
# Fully Lorentz-contracted expressions, these return scalars:
def add_delta(ne):
return ne * eye(4) # DiracSpinorIndex.delta(DiracSpinorIndex.auto_left, -DiracSpinorIndex.auto_right)
t = (G(mu)*G(-mu))
ts = add_delta(D)
assert _is_tensor_eq(tfunc(t), ts)
t = (G(mu)*G(nu)*G(-mu)*G(-nu))
ts = add_delta(2*D - D**2) # -8
assert _is_tensor_eq(tfunc(t), ts)
t = (G(mu)*G(nu)*G(-nu)*G(-mu))
ts = add_delta(D**2) # 16
assert _is_tensor_eq(tfunc(t), ts)
t = (G(mu)*G(nu)*G(-rho)*G(-nu)*G(-mu)*G(rho))
ts = add_delta(4*D - 4*D**2 + D**3) # 16
assert _is_tensor_eq(tfunc(t), ts)
t = (G(mu)*G(nu)*G(rho)*G(-rho)*G(-nu)*G(-mu))
ts = add_delta(D**3) # 64
assert _is_tensor_eq(tfunc(t), ts)
t = (G(a1)*G(a2)*G(a3)*G(a4)*G(-a3)*G(-a1)*G(-a2)*G(-a4))
ts = add_delta(-8*D + 16*D**2 - 8*D**3 + D**4) # -32
assert _is_tensor_eq(tfunc(t), ts)
t = (G(-mu)*G(-nu)*G(-rho)*G(-sigma)*G(nu)*G(mu)*G(sigma)*G(rho))
ts = add_delta(-16*D + 24*D**2 - 8*D**3 + D**4) # 64
assert _is_tensor_eq(tfunc(t), ts)
t = (G(-mu)*G(nu)*G(-rho)*G(sigma)*G(rho)*G(-nu)*G(mu)*G(-sigma))
ts = add_delta(8*D - 12*D**2 + 6*D**3 - D**4) # -32
assert _is_tensor_eq(tfunc(t), ts)
t = (G(a1)*G(a2)*G(a3)*G(a4)*G(a5)*G(-a3)*G(-a2)*G(-a1)*G(-a5)*G(-a4))
ts = add_delta(64*D - 112*D**2 + 60*D**3 - 12*D**4 + D**5) # 256
assert _is_tensor_eq(tfunc(t), ts)
t = (G(a1)*G(a2)*G(a3)*G(a4)*G(a5)*G(-a3)*G(-a1)*G(-a2)*G(-a4)*G(-a5))
ts = add_delta(64*D - 120*D**2 + 72*D**3 - 16*D**4 + D**5) # -128
assert _is_tensor_eq(tfunc(t), ts)
t = (G(a1)*G(a2)*G(a3)*G(a4)*G(a5)*G(a6)*G(-a3)*G(-a2)*G(-a1)*G(-a6)*G(-a5)*G(-a4))
ts = add_delta(416*D - 816*D**2 + 528*D**3 - 144*D**4 + 18*D**5 - D**6) # -128
assert _is_tensor_eq(tfunc(t), ts)
t = (G(a1)*G(a2)*G(a3)*G(a4)*G(a5)*G(a6)*G(-a2)*G(-a3)*G(-a1)*G(-a6)*G(-a4)*G(-a5))
ts = add_delta(416*D - 848*D**2 + 584*D**3 - 172*D**4 + 22*D**5 - D**6) # -128
assert _is_tensor_eq(tfunc(t), ts)
# Expressions with free indices:
t = (G(mu)*G(nu)*G(rho)*G(sigma)*G(-mu))
assert _is_tensor_eq(tfunc(t), (-2*G(sigma)*G(rho)*G(nu) + (4-D)*G(nu)*G(rho)*G(sigma)))
t = (G(mu)*G(nu)*G(-mu))
assert _is_tensor_eq(tfunc(t), (2-D)*G(nu))
t = (G(mu)*G(nu)*G(rho)*G(-mu))
assert _is_tensor_eq(tfunc(t), 2*G(nu)*G(rho) + 2*G(rho)*G(nu) - (4-D)*G(nu)*G(rho))
t = 2*G(m2)*G(m0)*G(m1)*G(-m0)*G(-m1)
st = tfunc(t)
assert _is_tensor_eq(st, (D*(-2*D + 4))*G(m2))
t = G(m2)*G(m0)*G(m1)*G(-m0)*G(-m2)
st = tfunc(t)
assert _is_tensor_eq(st, ((-D + 2)**2)*G(m1))
t = G(m0)*G(m1)*G(m2)*G(m3)*G(-m1)
st = tfunc(t)
assert _is_tensor_eq(st, (D - 4)*G(m0)*G(m2)*G(m3) + 4*G(m0)*g(m2, m3))
t = G(m0)*G(m1)*G(m2)*G(m3)*G(-m1)*G(-m0)
st = tfunc(t)
assert _is_tensor_eq(st, ((D - 4)**2)*G(m2)*G(m3) + (8*D - 16)*g(m2, m3))
t = G(m2)*G(m0)*G(m1)*G(-m2)*G(-m0)
st = tfunc(t)
assert _is_tensor_eq(st, ((-D + 2)*(D - 4) + 4)*G(m1))
t = G(m3)*G(m1)*G(m0)*G(m2)*G(-m3)*G(-m0)*G(-m2)
st = tfunc(t)
assert _is_tensor_eq(st, (-4*D + (-D + 2)**2*(D - 4) + 8)*G(m1))
t = 2*G(m0)*G(m1)*G(m2)*G(m3)*G(-m0)
st = tfunc(t)
assert _is_tensor_eq(st, ((-2*D + 8)*G(m1)*G(m2)*G(m3) - 4*G(m3)*G(m2)*G(m1)))
t = G(m5)*G(m0)*G(m1)*G(m4)*G(m2)*G(-m4)*G(m3)*G(-m0)
st = tfunc(t)
assert _is_tensor_eq(st, (((-D + 2)*(-D + 4))*G(m5)*G(m1)*G(m2)*G(m3) + (2*D - 4)*G(m5)*G(m3)*G(m2)*G(m1)))
t = -G(m0)*G(m1)*G(m2)*G(m3)*G(-m0)*G(m4)
st = tfunc(t)
assert _is_tensor_eq(st, ((D - 4)*G(m1)*G(m2)*G(m3)*G(m4) + 2*G(m3)*G(m2)*G(m1)*G(m4)))
t = G(-m5)*G(m0)*G(m1)*G(m2)*G(m3)*G(m4)*G(-m0)*G(m5)
st = tfunc(t)
result1 = ((-D + 4)**2 + 4)*G(m1)*G(m2)*G(m3)*G(m4) +\
(4*D - 16)*G(m3)*G(m2)*G(m1)*G(m4) + (4*D - 16)*G(m4)*G(m1)*G(m2)*G(m3)\
+ 4*G(m2)*G(m1)*G(m4)*G(m3) + 4*G(m3)*G(m4)*G(m1)*G(m2) +\
4*G(m4)*G(m3)*G(m2)*G(m1)
# Kahane's algorithm yields this result, which is equivalent to `result1`
# in four dimensions, but is not automatically recognized as equal:
result2 = 8*G(m1)*G(m2)*G(m3)*G(m4) + 8*G(m4)*G(m3)*G(m2)*G(m1)
if D == 4:
assert _is_tensor_eq(st, (result1)) or _is_tensor_eq(st, (result2))
else:
assert _is_tensor_eq(st, (result1))
# and a few very simple cases, with no contracted indices:
t = G(m0)
st = tfunc(t)
assert _is_tensor_eq(st, t)
t = -7*G(m0)
st = tfunc(t)
assert _is_tensor_eq(st, t)
t = 224*G(m0)*G(m1)*G(-m2)*G(m3)
st = tfunc(t)
assert _is_tensor_eq(st, t)
def test_kahane_algorithm():
# Wrap this function to convert to and from TIDS:
def tfunc(e):
return _simplify_single_line(e)
execute_gamma_simplify_tests_for_function(tfunc, D=4)
def test_kahane_simplify1():
i0,i1,i2,i3,i4,i5,i6,i7,i8,i9,i10,i11,i12,i13,i14,i15 = tensor_indices('i0:16', LorentzIndex)
mu, nu, rho, sigma = tensor_indices("mu, nu, rho, sigma", LorentzIndex)
D = 4
t = G(i0)*G(i1)
r = kahane_simplify(t)
assert r.equals(t)
t = G(i0)*G(i1)*G(-i0)
r = kahane_simplify(t)
assert r.equals(-2*G(i1))
t = G(i0)*G(i1)*G(-i0)
r = kahane_simplify(t)
assert r.equals(-2*G(i1))
t = G(i0)*G(i1)
r = kahane_simplify(t)
assert r.equals(t)
t = G(i0)*G(i1)
r = kahane_simplify(t)
assert r.equals(t)
t = G(i0)*G(-i0)
r = kahane_simplify(t)
assert r.equals(4*eye(4))
t = G(i0)*G(-i0)
r = kahane_simplify(t)
assert r.equals(4*eye(4))
t = G(i0)*G(-i0)
r = kahane_simplify(t)
assert r.equals(4*eye(4))
t = G(i0)*G(i1)*G(-i0)
r = kahane_simplify(t)
assert r.equals(-2*G(i1))
t = G(i0)*G(i1)*G(-i0)*G(-i1)
r = kahane_simplify(t)
assert r.equals((2*D - D**2)*eye(4))
t = G(i0)*G(i1)*G(-i0)*G(-i1)
r = kahane_simplify(t)
assert r.equals((2*D - D**2)*eye(4))
t = G(i0)*G(-i0)*G(i1)*G(-i1)
r = kahane_simplify(t)
assert r.equals(16*eye(4))
t = (G(mu)*G(nu)*G(-nu)*G(-mu))
r = kahane_simplify(t)
assert r.equals(D**2*eye(4))
t = (G(mu)*G(nu)*G(-nu)*G(-mu))
r = kahane_simplify(t)
assert r.equals(D**2*eye(4))
t = (G(mu)*G(nu)*G(-nu)*G(-mu))
r = kahane_simplify(t)
assert r.equals(D**2*eye(4))
t = (G(mu)*G(nu)*G(-rho)*G(-nu)*G(-mu)*G(rho))
r = kahane_simplify(t)
assert r.equals((4*D - 4*D**2 + D**3)*eye(4))
t = (G(-mu)*G(-nu)*G(-rho)*G(-sigma)*G(nu)*G(mu)*G(sigma)*G(rho))
r = kahane_simplify(t)
assert r.equals((-16*D + 24*D**2 - 8*D**3 + D**4)*eye(4))
t = (G(-mu)*G(nu)*G(-rho)*G(sigma)*G(rho)*G(-nu)*G(mu)*G(-sigma))
r = kahane_simplify(t)
assert r.equals((8*D - 12*D**2 + 6*D**3 - D**4)*eye(4))
# Expressions with free indices:
t = (G(mu)*G(nu)*G(rho)*G(sigma)*G(-mu))
r = kahane_simplify(t)
assert r.equals(-2*G(sigma)*G(rho)*G(nu))
t = (G(mu)*G(nu)*G(rho)*G(sigma)*G(-mu))
r = kahane_simplify(t)
assert r.equals(-2*G(sigma)*G(rho)*G(nu))
def test_gamma_matrix_class():
i, j, k = tensor_indices('i,j,k', LorentzIndex)
# define another type of TensorHead to see if exprs are correctly handled:
A = TensorHead('A', [LorentzIndex])
t = A(k)*G(i)*G(-i)
ts = simplify_gamma_expression(t)
assert _is_tensor_eq(ts, Matrix([
[4, 0, 0, 0],
[0, 4, 0, 0],
[0, 0, 4, 0],
[0, 0, 0, 4]])*A(k))
t = G(i)*A(k)*G(j)
ts = simplify_gamma_expression(t)
assert _is_tensor_eq(ts, A(k)*G(i)*G(j))
execute_gamma_simplify_tests_for_function(simplify_gamma_expression, D=4)
def test_gamma_matrix_trace():
g = LorentzIndex.metric
m0, m1, m2, m3, m4, m5, m6 = tensor_indices('m0:7', LorentzIndex)
n0, n1, n2, n3, n4, n5 = tensor_indices('n0:6', LorentzIndex)
# working in D=4 dimensions
D = 4
# traces of odd number of gamma matrices are zero:
t = G(m0)
t1 = gamma_trace(t)
assert t1.equals(0)
t = G(m0)*G(m1)*G(m2)
t1 = gamma_trace(t)
assert t1.equals(0)
t = G(m0)*G(m1)*G(-m0)
t1 = gamma_trace(t)
assert t1.equals(0)
t = G(m0)*G(m1)*G(m2)*G(m3)*G(m4)
t1 = gamma_trace(t)
assert t1.equals(0)
# traces without internal contractions:
t = G(m0)*G(m1)
t1 = gamma_trace(t)
assert _is_tensor_eq(t1, 4*g(m0, m1))
t = G(m0)*G(m1)*G(m2)*G(m3)
t1 = gamma_trace(t)
t2 = -4*g(m0, m2)*g(m1, m3) + 4*g(m0, m1)*g(m2, m3) + 4*g(m0, m3)*g(m1, m2)
st2 = str(t2)
assert _is_tensor_eq(t1, t2)
t = G(m0)*G(m1)*G(m2)*G(m3)*G(m4)*G(m5)
t1 = gamma_trace(t)
t2 = t1*g(-m0, -m5)
t2 = t2.contract_metric(g)
assert _is_tensor_eq(t2, D*gamma_trace(G(m1)*G(m2)*G(m3)*G(m4)))
# traces of expressions with internal contractions:
t = G(m0)*G(-m0)
t1 = gamma_trace(t)
assert t1.equals(4*D)
t = G(m0)*G(m1)*G(-m0)*G(-m1)
t1 = gamma_trace(t)
assert t1.equals(8*D - 4*D**2)
t = G(m0)*G(m1)*G(m2)*G(m3)*G(m4)*G(-m0)
t1 = gamma_trace(t)
t2 = (-4*D)*g(m1, m3)*g(m2, m4) + (4*D)*g(m1, m2)*g(m3, m4) + \
(4*D)*g(m1, m4)*g(m2, m3)
assert _is_tensor_eq(t1, t2)
t = G(-m5)*G(m0)*G(m1)*G(m2)*G(m3)*G(m4)*G(-m0)*G(m5)
t1 = gamma_trace(t)
t2 = (32*D + 4*(-D + 4)**2 - 64)*(g(m1, m2)*g(m3, m4) - \
g(m1, m3)*g(m2, m4) + g(m1, m4)*g(m2, m3))
assert _is_tensor_eq(t1, t2)
t = G(m0)*G(m1)*G(-m0)*G(m3)
t1 = gamma_trace(t)
assert t1.equals((-4*D + 8)*g(m1, m3))
# p, q = S1('p,q')
# ps = p(m0)*G(-m0)
# qs = q(m0)*G(-m0)
# t = ps*qs*ps*qs
# t1 = gamma_trace(t)
# assert t1 == 8*p(m0)*q(-m0)*p(m1)*q(-m1) - 4*p(m0)*p(-m0)*q(m1)*q(-m1)
t = G(m0)*G(m1)*G(m2)*G(m3)*G(m4)*G(m5)*G(-m0)*G(-m1)*G(-m2)*G(-m3)*G(-m4)*G(-m5)
t1 = gamma_trace(t)
assert t1.equals(-4*D**6 + 120*D**5 - 1040*D**4 + 3360*D**3 - 4480*D**2 + 2048*D)
t = G(m0)*G(m1)*G(n1)*G(m2)*G(n2)*G(m3)*G(m4)*G(-n2)*G(-n1)*G(-m0)*G(-m1)*G(-m2)*G(-m3)*G(-m4)
t1 = gamma_trace(t)
tresu = -7168*D + 16768*D**2 - 14400*D**3 + 5920*D**4 - 1232*D**5 + 120*D**6 - 4*D**7
assert t1.equals(tresu)
# checked with Mathematica
# In[1]:= <<Tracer.m
# In[2]:= Spur[l];
# In[3]:= GammaTrace[l, {m0},{m1},{n1},{m2},{n2},{m3},{m4},{n3},{n4},{m0},{m1},{m2},{m3},{m4}]
t = G(m0)*G(m1)*G(n1)*G(m2)*G(n2)*G(m3)*G(m4)*G(n3)*G(n4)*G(-m0)*G(-m1)*G(-m2)*G(-m3)*G(-m4)
t1 = gamma_trace(t)
# t1 = t1.expand_coeff()
c1 = -4*D**5 + 120*D**4 - 1200*D**3 + 5280*D**2 - 10560*D + 7808
c2 = -4*D**5 + 88*D**4 - 560*D**3 + 1440*D**2 - 1600*D + 640
assert _is_tensor_eq(t1, c1*g(n1, n4)*g(n2, n3) + c2*g(n1, n2)*g(n3, n4) + \
(-c1)*g(n1, n3)*g(n2, n4))
p, q = tensor_heads('p,q', [LorentzIndex])
ps = p(m0)*G(-m0)
qs = q(m0)*G(-m0)
p2 = p(m0)*p(-m0)
q2 = q(m0)*q(-m0)
pq = p(m0)*q(-m0)
t = ps*qs*ps*qs
r = gamma_trace(t)
assert _is_tensor_eq(r, 8*pq*pq - 4*p2*q2)
t = ps*qs*ps*qs*ps*qs
r = gamma_trace(t)
assert _is_tensor_eq(r, -12*p2*pq*q2 + 16*pq*pq*pq)
t = ps*qs*ps*qs*ps*qs*ps*qs
r = gamma_trace(t)
assert _is_tensor_eq(r, -32*pq*pq*p2*q2 + 32*pq*pq*pq*pq + 4*p2*p2*q2*q2)
t = 4*p(m1)*p(m0)*p(-m0)*q(-m1)*q(m2)*q(-m2)
assert _is_tensor_eq(gamma_trace(t), t)
t = ps*ps*ps*ps*ps*ps*ps*ps
r = gamma_trace(t)
assert r.equals(4*p2*p2*p2*p2)
|
6b99de1d5a70f6dcfa05bc3ef985e7deccfcaeeb5a650a305aeea0dea4e04aa9 | from __future__ import print_function, division
import functools, itertools
from sympy.core.sympify import sympify
from sympy.core.expr import Expr
from sympy.core import Basic
from sympy.core.compatibility import Iterable
from sympy.tensor.array import MutableDenseNDimArray, ImmutableDenseNDimArray
from sympy import Symbol
from sympy.core.sympify import sympify
from sympy.core.numbers import Integer
class ArrayComprehension(Basic):
"""
Generate a list comprehension
If there is a symbolic dimension, for example, say [i for i in range(1, N)] where
N is a Symbol, then the expression will not be expanded to an array. Otherwise,
calling the doit() function will launch the expansion.
Examples
========
>>> from sympy.tensor.array import ArrayComprehension
>>> from sympy import symbols
>>> i, j, k = symbols('i j k')
>>> a = ArrayComprehension(10*i + j, (i, 1, 4), (j, 1, 3))
>>> a
ArrayComprehension(10*i + j, (i, 1, 4), (j, 1, 3))
>>> a.doit()
[[11, 12, 13], [21, 22, 23], [31, 32, 33], [41, 42, 43]]
>>> b = ArrayComprehension(10*i + j, (i, 1, 4), (j, 1, k))
>>> b.doit()
ArrayComprehension(10*i + j, (i, 1, 4), (j, 1, k))
"""
def __new__(cls, function, *symbols, **assumptions):
if any(len(l) != 3 or None for l in symbols):
raise ValueError('ArrayComprehension requires values lower and upper bound'
' for the expression')
arglist = [sympify(function)]
arglist.extend(cls._check_limits_validity(function, symbols))
obj = Basic.__new__(cls, *arglist, **assumptions)
obj._limits = obj._args[1:]
obj._shape = cls._calculate_shape_from_limits(obj._limits)
obj._rank = len(obj._shape)
obj._loop_size = cls._calculate_loop_size(obj._shape)
return obj
@property
def function(self):
"""The function applied across limits
Examples
========
>>> from sympy.tensor.array import ArrayComprehension
>>> from sympy import symbols
>>> i, j = symbols('i j')
>>> a = ArrayComprehension(10*i + j, (i, 1, 4), (j, 1, 3))
>>> a.function
10*i + j
"""
return self._args[0]
@property
def limits(self):
"""
The list of limits that will be applied while expanding the array
Examples
========
>>> from sympy.tensor.array import ArrayComprehension
>>> from sympy import symbols
>>> i, j = symbols('i j')
>>> a = ArrayComprehension(10*i + j, (i, 1, 4), (j, 1, 3))
>>> a.limits
((i, 1, 4), (j, 1, 3))
"""
return self._limits
@property
def free_symbols(self):
"""
The set of the free_symbols in the array
Variables appeared in the bounds are supposed to be excluded
from the free symbol set.
Examples
========
>>> from sympy.tensor.array import ArrayComprehension
>>> from sympy import symbols
>>> i, j, k = symbols('i j k')
>>> a = ArrayComprehension(10*i + j, (i, 1, 4), (j, 1, 3))
>>> a.free_symbols
set()
>>> b = ArrayComprehension(10*i + j, (i, 1, 4), (j, 1, k+3))
>>> b.free_symbols
{k}
"""
expr_free_sym = self.function.free_symbols
for var, inf, sup in self._limits:
expr_free_sym.discard(var)
curr_free_syms = inf.free_symbols.union(sup.free_symbols)
expr_free_sym = expr_free_sym.union(curr_free_syms)
return expr_free_sym
@property
def variables(self):
"""The tuples of the variables in the limits
Examples
========
>>> from sympy.tensor.array import ArrayComprehension
>>> from sympy import symbols
>>> i, j, k = symbols('i j k')
>>> a = ArrayComprehension(10*i + j, (i, 1, 4), (j, 1, 3))
>>> a.variables
[i, j]
"""
return [l[0] for l in self._limits]
@property
def bound_symbols(self):
"""The list of dummy variables
Note
====
Note that all variables are dummy variables since a limit without
lower bound or upper bound is not accepted.
"""
return [l[0] for l in self._limits if len(l) != 1]
@property
def shape(self):
"""
The shape of the expanded array, which may have symbols
Note
====
Both the lower and the upper bounds are included while
calculating the shape.
Examples
========
>>> from sympy.tensor.array import ArrayComprehension
>>> from sympy import symbols
>>> i, j, k = symbols('i j k')
>>> a = ArrayComprehension(10*i + j, (i, 1, 4), (j, 1, 3))
>>> a.shape
(4, 3)
>>> b = ArrayComprehension(10*i + j, (i, 1, 4), (j, 1, k+3))
>>> b.shape
(4, k + 3)
"""
return self._shape
@property
def is_shape_numeric(self):
"""
Test if the array is shape-numeric which means there is no symbolic
dimension
Examples
========
>>> from sympy.tensor.array import ArrayComprehension
>>> from sympy import symbols
>>> i, j, k = symbols('i j k')
>>> a = ArrayComprehension(10*i + j, (i, 1, 4), (j, 1, 3))
>>> a.is_shape_numeric
True
>>> b = ArrayComprehension(10*i + j, (i, 1, 4), (j, 1, k+3))
>>> b.is_shape_numeric
False
"""
for _, inf, sup in self._limits:
if Basic(inf, sup).atoms(Symbol):
return False
return True
def rank(self):
"""The rank of the expanded array
Examples
========
>>> from sympy.tensor.array import ArrayComprehension
>>> from sympy import symbols
>>> i, j, k = symbols('i j k')
>>> a = ArrayComprehension(10*i + j, (i, 1, 4), (j, 1, 3))
>>> a.rank()
2
"""
return self._rank
def __len__(self):
"""
The length of the expanded array which means the number
of elements in the array.
Raises
======
ValueError : When the length of the array is symbolic
Examples
========
>>> from sympy.tensor.array import ArrayComprehension
>>> from sympy import symbols
>>> i, j = symbols('i j')
>>> a = ArrayComprehension(10*i + j, (i, 1, 4), (j, 1, 3))
>>> len(a)
12
"""
if self._loop_size.free_symbols:
raise ValueError('Symbolic length is not supported')
return self._loop_size
@classmethod
def _check_limits_validity(cls, function, limits):
limits = sympify(limits)
for var, inf, sup in limits:
if any((not isinstance(i, Expr)) or i.atoms(Symbol, Integer) != i.atoms()
for i in [inf, sup]):
raise TypeError('Bounds should be an Expression(combination of Integer and Symbol)')
if (inf > sup) == True:
raise ValueError('Lower bound should be inferior to upper bound')
if var in inf.free_symbols or var in sup.free_symbols:
raise ValueError('Variable should not be part of its bounds')
return limits
@classmethod
def _calculate_shape_from_limits(cls, limits):
return tuple([sup - inf + 1 for _, inf, sup in limits])
@classmethod
def _calculate_loop_size(cls, shape):
if not shape:
return 0
loop_size = 1
for l in shape:
loop_size = loop_size * l
return loop_size
def doit(self):
if not self.is_shape_numeric:
return self
return self._expand_array()
def _expand_array(self):
res = []
for values in itertools.product(*[range(inf, sup+1)
for var, inf, sup
in self._limits]):
res.append(self._get_element(values))
return ImmutableDenseNDimArray(res, self.shape)
def _get_element(self, values):
temp = self.function
for var, val in zip(self.variables, values):
temp = temp.subs(var, val)
return temp
def tolist(self):
"""Transform the expanded array to a list
Raises
======
ValueError : When there is a symbolic dimension
Examples
========
>>> from sympy.tensor.array import ArrayComprehension
>>> from sympy import symbols
>>> i, j = symbols('i j')
>>> a = ArrayComprehension(10*i + j, (i, 1, 4), (j, 1, 3))
>>> a.tolist()
[[11, 12, 13], [21, 22, 23], [31, 32, 33], [41, 42, 43]]
"""
if self.is_shape_numeric:
return self._expand_array().tolist()
raise ValueError("A symbolic array cannot be expanded to a list")
def tomatrix(self):
"""Transform the expanded array to a matrix
Raises
======
ValueError : When there is a symbolic dimension
ValueError : When the rank of the expanded array is not equal to 2
Examples
========
>>> from sympy.tensor.array import ArrayComprehension
>>> from sympy import symbols
>>> i, j = symbols('i j')
>>> a = ArrayComprehension(10*i + j, (i, 1, 4), (j, 1, 3))
>>> a.tomatrix()
Matrix([
[11, 12, 13],
[21, 22, 23],
[31, 32, 33],
[41, 42, 43]])
"""
from sympy.matrices import Matrix
if not self.is_shape_numeric:
raise ValueError("A symbolic array cannot be expanded to a matrix")
if self._rank != 2:
raise ValueError('Dimensions must be of size of 2')
return Matrix(self._expand_array().tomatrix())
def isLambda(v):
LAMBDA = lambda: 0
return isinstance(v, type(LAMBDA)) and v.__name__ == LAMBDA.__name__
class ArrayComprehensionMap(ArrayComprehension):
'''
A subclass of ArrayComprehension dedicated to map external function lambda.
Notes
=====
Only the lambda function is considered.
At most one argument in lambda function is accepted in order to avoid ambiguity
in value assignment.
Examples
========
>>> from sympy.tensor.array import ArrayComprehensionMap
>>> from sympy import symbols
>>> i, j, k = symbols('i j k')
>>> a = ArrayComprehensionMap(lambda: 1, (i, 1, 4))
>>> a.doit()
[1, 1, 1, 1]
>>> b = ArrayComprehensionMap(lambda a: a+1, (j, 1, 4))
>>> b.doit()
[2, 3, 4, 5]
'''
def __new__(cls, function, *symbols, **assumptions):
if any(len(l) != 3 or None for l in symbols):
raise ValueError('ArrayComprehension requires values lower and upper bound'
' for the expression')
if not isLambda(function):
raise ValueError('Data type not supported')
arglist = cls._check_limits_validity(function, symbols)
obj = Basic.__new__(cls, *arglist, **assumptions)
obj._limits = obj._args
obj._shape = cls._calculate_shape_from_limits(obj._limits)
obj._rank = len(obj._shape)
obj._loop_size = cls._calculate_loop_size(obj._shape)
obj._lambda = function
return obj
@property
def func(self):
class _(ArrayComprehensionMap):
def __new__(cls, *args, **kwargs):
return ArrayComprehensionMap(self._lambda, *args, **kwargs)
return _
def _get_element(self, values):
temp = self._lambda
if self._lambda.__code__.co_argcount == 0:
temp = temp()
elif self._lambda.__code__.co_argcount == 1:
temp = temp(functools.reduce(lambda a, b: a*b, values))
return temp
|
4a5350703b1d3c7473de1d49323b33f7d2825bc28be52b5f8ec59bdce5c9f126 | r"""
N-dim array module for SymPy.
Four classes are provided to handle N-dim arrays, given by the combinations
dense/sparse (i.e. whether to store all elements or only the non-zero ones in
memory) and mutable/immutable (immutable classes are SymPy objects, but cannot
change after they have been created).
Examples
========
The following examples show the usage of ``Array``. This is an abbreviation for
``ImmutableDenseNDimArray``, that is an immutable and dense N-dim array, the
other classes are analogous. For mutable classes it is also possible to change
element values after the object has been constructed.
Array construction can detect the shape of nested lists and tuples:
>>> from sympy import Array
>>> a1 = Array([[1, 2], [3, 4], [5, 6]])
>>> a1
[[1, 2], [3, 4], [5, 6]]
>>> a1.shape
(3, 2)
>>> a1.rank()
2
>>> from sympy.abc import x, y, z
>>> a2 = Array([[[x, y], [z, x*z]], [[1, x*y], [1/x, x/y]]])
>>> a2
[[[x, y], [z, x*z]], [[1, x*y], [1/x, x/y]]]
>>> a2.shape
(2, 2, 2)
>>> a2.rank()
3
Otherwise one could pass a 1-dim array followed by a shape tuple:
>>> m1 = Array(range(12), (3, 4))
>>> m1
[[0, 1, 2, 3], [4, 5, 6, 7], [8, 9, 10, 11]]
>>> m2 = Array(range(12), (3, 2, 2))
>>> m2
[[[0, 1], [2, 3]], [[4, 5], [6, 7]], [[8, 9], [10, 11]]]
>>> m2[1,1,1]
7
>>> m2.reshape(4, 3)
[[0, 1, 2], [3, 4, 5], [6, 7, 8], [9, 10, 11]]
Slice support:
>>> m2[:, 1, 1]
[3, 7, 11]
Elementwise derivative:
>>> from sympy.abc import x, y, z
>>> m3 = Array([x**3, x*y, z])
>>> m3.diff(x)
[3*x**2, y, 0]
>>> m3.diff(z)
[0, 0, 1]
Multiplication with other SymPy expressions is applied elementwisely:
>>> (1+x)*m3
[x**3*(x + 1), x*y*(x + 1), z*(x + 1)]
To apply a function to each element of the N-dim array, use ``applyfunc``:
>>> m3.applyfunc(lambda x: x/2)
[x**3/2, x*y/2, z/2]
N-dim arrays can be converted to nested lists by the ``tolist()`` method:
>>> m2.tolist()
[[[0, 1], [2, 3]], [[4, 5], [6, 7]], [[8, 9], [10, 11]]]
>>> isinstance(m2.tolist(), list)
True
If the rank is 2, it is possible to convert them to matrices with ``tomatrix()``:
>>> m1.tomatrix()
Matrix([
[0, 1, 2, 3],
[4, 5, 6, 7],
[8, 9, 10, 11]])
Products and contractions
-------------------------
Tensor product between arrays `A_{i_1,\ldots,i_n}` and `B_{j_1,\ldots,j_m}`
creates the combined array `P = A \otimes B` defined as
`P_{i_1,\ldots,i_n,j_1,\ldots,j_m} := A_{i_1,\ldots,i_n}\cdot B_{j_1,\ldots,j_m}.`
It is available through ``tensorproduct(...)``:
>>> from sympy import Array, tensorproduct
>>> from sympy.abc import x,y,z,t
>>> A = Array([x, y, z, t])
>>> B = Array([1, 2, 3, 4])
>>> tensorproduct(A, B)
[[x, 2*x, 3*x, 4*x], [y, 2*y, 3*y, 4*y], [z, 2*z, 3*z, 4*z], [t, 2*t, 3*t, 4*t]]
Tensor product between a rank-1 array and a matrix creates a rank-3 array:
>>> from sympy import eye
>>> p1 = tensorproduct(A, eye(4))
>>> p1
[[[x, 0, 0, 0], [0, x, 0, 0], [0, 0, x, 0], [0, 0, 0, x]], [[y, 0, 0, 0], [0, y, 0, 0], [0, 0, y, 0], [0, 0, 0, y]], [[z, 0, 0, 0], [0, z, 0, 0], [0, 0, z, 0], [0, 0, 0, z]], [[t, 0, 0, 0], [0, t, 0, 0], [0, 0, t, 0], [0, 0, 0, t]]]
Now, to get back `A_0 \otimes \mathbf{1}` one can access `p_{0,m,n}` by slicing:
>>> p1[0,:,:]
[[x, 0, 0, 0], [0, x, 0, 0], [0, 0, x, 0], [0, 0, 0, x]]
Tensor contraction sums over the specified axes, for example contracting
positions `a` and `b` means
`A_{i_1,\ldots,i_a,\ldots,i_b,\ldots,i_n} \implies \sum_k A_{i_1,\ldots,k,\ldots,k,\ldots,i_n}`
Remember that Python indexing is zero starting, to contract the a-th and b-th
axes it is therefore necessary to specify `a-1` and `b-1`
>>> from sympy import tensorcontraction
>>> C = Array([[x, y], [z, t]])
The matrix trace is equivalent to the contraction of a rank-2 array:
`A_{m,n} \implies \sum_k A_{k,k}`
>>> tensorcontraction(C, (0, 1))
t + x
Matrix product is equivalent to a tensor product of two rank-2 arrays, followed
by a contraction of the 2nd and 3rd axes (in Python indexing axes number 1, 2).
`A_{m,n}\cdot B_{i,j} \implies \sum_k A_{m, k}\cdot B_{k, j}`
>>> D = Array([[2, 1], [0, -1]])
>>> tensorcontraction(tensorproduct(C, D), (1, 2))
[[2*x, x - y], [2*z, -t + z]]
One may verify that the matrix product is equivalent:
>>> from sympy import Matrix
>>> Matrix([[x, y], [z, t]])*Matrix([[2, 1], [0, -1]])
Matrix([
[2*x, x - y],
[2*z, -t + z]])
or equivalently
>>> C.tomatrix()*D.tomatrix()
Matrix([
[2*x, x - y],
[2*z, -t + z]])
Derivatives by array
--------------------
The usual derivative operation may be extended to support derivation with
respect to arrays, provided that all elements in the that array are symbols or
expressions suitable for derivations.
The definition of a derivative by an array is as follows: given the array
`A_{i_1, \ldots, i_N}` and the array `X_{j_1, \ldots, j_M}`
the derivative of arrays will return a new array `B` defined by
`B_{j_1,\ldots,j_M,i_1,\ldots,i_N} := \frac{\partial A_{i_1,\ldots,i_N}}{\partial X_{j_1,\ldots,j_M}}`
The function ``derive_by_array`` performs such an operation:
>>> from sympy import derive_by_array
>>> from sympy.abc import x, y, z, t
>>> from sympy import sin, exp
With scalars, it behaves exactly as the ordinary derivative:
>>> derive_by_array(sin(x*y), x)
y*cos(x*y)
Scalar derived by an array basis:
>>> derive_by_array(sin(x*y), [x, y, z])
[y*cos(x*y), x*cos(x*y), 0]
Deriving array by an array basis: `B^{nm} := \frac{\partial A^m}{\partial x^n}`
>>> basis = [x, y, z]
>>> ax = derive_by_array([exp(x), sin(y*z), t], basis)
>>> ax
[[exp(x), 0, 0], [0, z*cos(y*z), 0], [0, y*cos(y*z), 0]]
Contraction of the resulting array: `\sum_m \frac{\partial A^m}{\partial x^m}`
>>> tensorcontraction(ax, (0, 1))
z*cos(y*z) + exp(x)
"""
from .dense_ndim_array import MutableDenseNDimArray, ImmutableDenseNDimArray, DenseNDimArray
from .sparse_ndim_array import MutableSparseNDimArray, ImmutableSparseNDimArray, SparseNDimArray
from .ndim_array import NDimArray
from .arrayop import tensorproduct, tensorcontraction, derive_by_array, permutedims
from .array_comprehension import ArrayComprehension, ArrayComprehensionMap
Array = ImmutableDenseNDimArray
|
3bf1f92100eadc97b679d868306b9be8ce72648e771339a67ce99362d1a065a0 | import itertools
from sympy import S, Tuple, diff, Basic
from sympy.core.compatibility import Iterable
from sympy.tensor.array import ImmutableDenseNDimArray
from sympy.tensor.array.ndim_array import NDimArray
from sympy.tensor.array.dense_ndim_array import DenseNDimArray
from sympy.tensor.array.sparse_ndim_array import SparseNDimArray
def _arrayfy(a):
from sympy.matrices import MatrixBase
if isinstance(a, NDimArray):
return a
if isinstance(a, (MatrixBase, list, tuple, Tuple)):
return ImmutableDenseNDimArray(a)
return a
def tensorproduct(*args):
"""
Tensor product among scalars or array-like objects.
Examples
========
>>> from sympy.tensor.array import tensorproduct, Array
>>> from sympy.abc import x, y, z, t
>>> A = Array([[1, 2], [3, 4]])
>>> B = Array([x, y])
>>> tensorproduct(A, B)
[[[x, y], [2*x, 2*y]], [[3*x, 3*y], [4*x, 4*y]]]
>>> tensorproduct(A, x)
[[x, 2*x], [3*x, 4*x]]
>>> tensorproduct(A, B, B)
[[[[x**2, x*y], [x*y, y**2]], [[2*x**2, 2*x*y], [2*x*y, 2*y**2]]], [[[3*x**2, 3*x*y], [3*x*y, 3*y**2]], [[4*x**2, 4*x*y], [4*x*y, 4*y**2]]]]
Applying this function on two matrices will result in a rank 4 array.
>>> from sympy import Matrix, eye
>>> m = Matrix([[x, y], [z, t]])
>>> p = tensorproduct(eye(3), m)
>>> p
[[[[x, y], [z, t]], [[0, 0], [0, 0]], [[0, 0], [0, 0]]], [[[0, 0], [0, 0]], [[x, y], [z, t]], [[0, 0], [0, 0]]], [[[0, 0], [0, 0]], [[0, 0], [0, 0]], [[x, y], [z, t]]]]
"""
from sympy.tensor.array import SparseNDimArray, ImmutableSparseNDimArray
if len(args) == 0:
return S.One
if len(args) == 1:
return _arrayfy(args[0])
if len(args) > 2:
return tensorproduct(tensorproduct(args[0], args[1]), *args[2:])
# length of args is 2:
a, b = map(_arrayfy, args)
if not isinstance(a, NDimArray) or not isinstance(b, NDimArray):
return a*b
if isinstance(a, SparseNDimArray) and isinstance(b, SparseNDimArray):
lp = len(b)
new_array = {k1*lp + k2: v1*v2 for k1, v1 in a._sparse_array.items() for k2, v2 in b._sparse_array.items()}
return ImmutableSparseNDimArray(new_array, a.shape + b.shape)
product_list = [i*j for i in Flatten(a) for j in Flatten(b)]
return ImmutableDenseNDimArray(product_list, a.shape + b.shape)
def tensorcontraction(array, *contraction_axes):
"""
Contraction of an array-like object on the specified axes.
Examples
========
>>> from sympy import Array, tensorcontraction
>>> from sympy import Matrix, eye
>>> tensorcontraction(eye(3), (0, 1))
3
>>> A = Array(range(18), (3, 2, 3))
>>> A
[[[0, 1, 2], [3, 4, 5]], [[6, 7, 8], [9, 10, 11]], [[12, 13, 14], [15, 16, 17]]]
>>> tensorcontraction(A, (0, 2))
[21, 30]
Matrix multiplication may be emulated with a proper combination of
``tensorcontraction`` and ``tensorproduct``
>>> from sympy import tensorproduct
>>> from sympy.abc import a,b,c,d,e,f,g,h
>>> m1 = Matrix([[a, b], [c, d]])
>>> m2 = Matrix([[e, f], [g, h]])
>>> p = tensorproduct(m1, m2)
>>> p
[[[[a*e, a*f], [a*g, a*h]], [[b*e, b*f], [b*g, b*h]]], [[[c*e, c*f], [c*g, c*h]], [[d*e, d*f], [d*g, d*h]]]]
>>> tensorcontraction(p, (1, 2))
[[a*e + b*g, a*f + b*h], [c*e + d*g, c*f + d*h]]
>>> m1*m2
Matrix([
[a*e + b*g, a*f + b*h],
[c*e + d*g, c*f + d*h]])
"""
array = _arrayfy(array)
# Verify contraction_axes:
taken_dims = set([])
for axes_group in contraction_axes:
if not isinstance(axes_group, Iterable):
raise ValueError("collections of contraction axes expected")
dim = array.shape[axes_group[0]]
for d in axes_group:
if d in taken_dims:
raise ValueError("dimension specified more than once")
if dim != array.shape[d]:
raise ValueError("cannot contract between axes of different dimension")
taken_dims.add(d)
rank = array.rank()
remaining_shape = [dim for i, dim in enumerate(array.shape) if i not in taken_dims]
cum_shape = [0]*rank
_cumul = 1
for i in range(rank):
cum_shape[rank - i - 1] = _cumul
_cumul *= int(array.shape[rank - i - 1])
# DEFINITION: by absolute position it is meant the position along the one
# dimensional array containing all the tensor components.
# Possible future work on this module: move computation of absolute
# positions to a class method.
# Determine absolute positions of the uncontracted indices:
remaining_indices = [[cum_shape[i]*j for j in range(array.shape[i])]
for i in range(rank) if i not in taken_dims]
# Determine absolute positions of the contracted indices:
summed_deltas = []
for axes_group in contraction_axes:
lidx = []
for js in range(array.shape[axes_group[0]]):
lidx.append(sum([cum_shape[ig] * js for ig in axes_group]))
summed_deltas.append(lidx)
# Compute the contracted array:
#
# 1. external for loops on all uncontracted indices.
# Uncontracted indices are determined by the combinatorial product of
# the absolute positions of the remaining indices.
# 2. internal loop on all contracted indices.
# It sum the values of the absolute contracted index and the absolute
# uncontracted index for the external loop.
contracted_array = []
for icontrib in itertools.product(*remaining_indices):
index_base_position = sum(icontrib)
isum = S.Zero
for sum_to_index in itertools.product(*summed_deltas):
idx = array._get_tuple_index(index_base_position + sum(sum_to_index))
isum += array[idx]
contracted_array.append(isum)
if len(remaining_indices) == 0:
assert len(contracted_array) == 1
return contracted_array[0]
return type(array)(contracted_array, remaining_shape)
def derive_by_array(expr, dx):
r"""
Derivative by arrays. Supports both arrays and scalars.
Given the array `A_{i_1, \ldots, i_N}` and the array `X_{j_1, \ldots, j_M}`
this function will return a new array `B` defined by
`B_{j_1,\ldots,j_M,i_1,\ldots,i_N} := \frac{\partial A_{i_1,\ldots,i_N}}{\partial X_{j_1,\ldots,j_M}}`
Examples
========
>>> from sympy import derive_by_array
>>> from sympy.abc import x, y, z, t
>>> from sympy import cos
>>> derive_by_array(cos(x*t), x)
-t*sin(t*x)
>>> derive_by_array(cos(x*t), [x, y, z, t])
[-t*sin(t*x), 0, 0, -x*sin(t*x)]
>>> derive_by_array([x, y**2*z], [[x, y], [z, t]])
[[[1, 0], [0, 2*y*z]], [[0, y**2], [0, 0]]]
"""
from sympy.matrices import MatrixBase
from sympy.tensor.array import SparseNDimArray
array_types = (Iterable, MatrixBase, NDimArray)
if isinstance(dx, array_types):
dx = ImmutableDenseNDimArray(dx)
for i in dx:
if not i._diff_wrt:
raise ValueError("cannot derive by this array")
if isinstance(expr, array_types):
if isinstance(expr, NDimArray):
expr = expr.as_immutable()
else:
expr = ImmutableDenseNDimArray(expr)
if isinstance(dx, array_types):
if isinstance(expr, SparseNDimArray):
lp = len(expr)
new_array = {k + i*lp: v
for i, x in enumerate(Flatten(dx))
for k, v in expr.diff(x)._sparse_array.items()}
else:
new_array = [[y.diff(x) for y in Flatten(expr)] for x in Flatten(dx)]
return type(expr)(new_array, dx.shape + expr.shape)
else:
return expr.diff(dx)
else:
if isinstance(dx, array_types):
return ImmutableDenseNDimArray([expr.diff(i) for i in Flatten(dx)], dx.shape)
else:
return diff(expr, dx)
def permutedims(expr, perm):
"""
Permutes the indices of an array.
Parameter specifies the permutation of the indices.
Examples
========
>>> from sympy.abc import x, y, z, t
>>> from sympy import sin
>>> from sympy import Array, permutedims
>>> a = Array([[x, y, z], [t, sin(x), 0]])
>>> a
[[x, y, z], [t, sin(x), 0]]
>>> permutedims(a, (1, 0))
[[x, t], [y, sin(x)], [z, 0]]
If the array is of second order, ``transpose`` can be used:
>>> from sympy import transpose
>>> transpose(a)
[[x, t], [y, sin(x)], [z, 0]]
Examples on higher dimensions:
>>> b = Array([[[1, 2], [3, 4]], [[5, 6], [7, 8]]])
>>> permutedims(b, (2, 1, 0))
[[[1, 5], [3, 7]], [[2, 6], [4, 8]]]
>>> permutedims(b, (1, 2, 0))
[[[1, 5], [2, 6]], [[3, 7], [4, 8]]]
``Permutation`` objects are also allowed:
>>> from sympy.combinatorics import Permutation
>>> permutedims(b, Permutation([1, 2, 0]))
[[[1, 5], [2, 6]], [[3, 7], [4, 8]]]
"""
from sympy.tensor.array import SparseNDimArray
if not isinstance(expr, NDimArray):
raise TypeError("expression has to be an N-dim array")
from sympy.combinatorics import Permutation
if not isinstance(perm, Permutation):
perm = Permutation(list(perm))
if perm.size != expr.rank():
raise ValueError("wrong permutation size")
# Get the inverse permutation:
iperm = ~perm
new_shape = perm(expr.shape)
if isinstance(expr, SparseNDimArray):
return type(expr)({tuple(perm(expr._get_tuple_index(k))): v
for k, v in expr._sparse_array.items()}, new_shape)
indices_span = perm([range(i) for i in expr.shape])
new_array = [None]*len(expr)
for i, idx in enumerate(itertools.product(*indices_span)):
t = iperm(idx)
new_array[i] = expr[t]
return type(expr)(new_array, new_shape)
class Flatten(Basic):
'''
Flatten an iterable object to a list in a lazy-evaluation way.
Notes
=====
This class is an iterator with which the memory cost can be economised.
Optimisation has been considered to ameliorate the performance for some
specific data types like DenseNDimArray and SparseNDimArray.
Examples
========
>>> from sympy.tensor.array.arrayop import Flatten
>>> from sympy.tensor.array import Array
>>> A = Array(range(6)).reshape(2, 3)
>>> Flatten(A)
Flatten([[0, 1, 2], [3, 4, 5]])
>>> [i for i in Flatten(A)]
[0, 1, 2, 3, 4, 5]
'''
def __init__(self, iterable):
from sympy.matrices.matrices import MatrixBase
from sympy.tensor.array import NDimArray
if not isinstance(iterable, (Iterable, MatrixBase)):
raise NotImplementedError("Data type not yet supported")
if isinstance(iterable, list):
iterable = NDimArray(iterable)
self._iter = iterable
self._idx = 0
def __iter__(self):
return self
def __next__(self):
from sympy.matrices.matrices import MatrixBase
if len(self._iter) > self._idx:
if isinstance(self._iter, DenseNDimArray):
result = self._iter._array[self._idx]
elif isinstance(self._iter, SparseNDimArray):
if self._idx in self._iter._sparse_array:
result = self._iter._sparse_array[self._idx]
else:
result = 0
elif isinstance(self._iter, MatrixBase):
result = self._iter[self._idx]
elif hasattr(self._iter, '__next__'):
result = next(self._iter)
else:
result = self._iter[self._idx]
else:
raise StopIteration
self._idx += 1
return result
def next(self):
return self.__next__()
|
b3ee405a29bee5835217bee2ab1e295c5174cef57ef7c244145fff9a3d60a704 | from __future__ import print_function, division
from sympy import S, Dict, Basic, Tuple
from sympy.core.sympify import _sympify
from sympy.tensor.array.mutable_ndim_array import MutableNDimArray
from sympy.tensor.array.ndim_array import NDimArray, ImmutableNDimArray
from sympy.core.numbers import Integer
from sympy.core.compatibility import SYMPY_INTS
import functools
class SparseNDimArray(NDimArray):
def __new__(self, *args, **kwargs):
return ImmutableSparseNDimArray(*args, **kwargs)
def __getitem__(self, index):
"""
Get an element from a sparse N-dim array.
Examples
========
>>> from sympy import MutableSparseNDimArray
>>> a = MutableSparseNDimArray(range(4), (2, 2))
>>> a
[[0, 1], [2, 3]]
>>> a[0, 0]
0
>>> a[1, 1]
3
>>> a[0]
[0, 1]
>>> a[1]
[2, 3]
Symbolic indexing:
>>> from sympy.abc import i, j
>>> a[i, j]
[[0, 1], [2, 3]][i, j]
Replace `i` and `j` to get element `(0, 0)`:
>>> a[i, j].subs({i: 0, j: 0})
0
"""
syindex = self._check_symbolic_index(index)
if syindex is not None:
return syindex
index = self._check_index_for_getitem(index)
# `index` is a tuple with one or more slices:
if isinstance(index, tuple) and any([isinstance(i, slice) for i in index]):
sl_factors, eindices = self._get_slice_data_for_array_access(index)
array = [self._sparse_array.get(self._parse_index(i), S.Zero) for i in eindices]
nshape = [len(el) for i, el in enumerate(sl_factors) if isinstance(index[i], slice)]
return type(self)(array, nshape)
else:
index = self._parse_index(index)
return self._sparse_array.get(index, S.Zero)
@classmethod
def zeros(cls, *shape):
"""
Return a sparse N-dim array of zeros.
"""
return cls({}, shape)
def tomatrix(self):
"""
Converts MutableDenseNDimArray to Matrix. Can convert only 2-dim array, else will raise error.
Examples
========
>>> from sympy import MutableSparseNDimArray
>>> a = MutableSparseNDimArray([1 for i in range(9)], (3, 3))
>>> b = a.tomatrix()
>>> b
Matrix([
[1, 1, 1],
[1, 1, 1],
[1, 1, 1]])
"""
from sympy.matrices import SparseMatrix
if self.rank() != 2:
raise ValueError('Dimensions must be of size of 2')
mat_sparse = {}
for key, value in self._sparse_array.items():
mat_sparse[self._get_tuple_index(key)] = value
return SparseMatrix(self.shape[0], self.shape[1], mat_sparse)
def reshape(self, *newshape):
new_total_size = functools.reduce(lambda x,y: x*y, newshape)
if new_total_size != self._loop_size:
raise ValueError("Invalid reshape parameters " + newshape)
return type(self)(self._sparse_array, newshape)
class ImmutableSparseNDimArray(SparseNDimArray, ImmutableNDimArray):
def __new__(cls, iterable=None, shape=None, **kwargs):
from sympy.utilities.iterables import flatten
shape, flat_list = cls._handle_ndarray_creation_inputs(iterable, shape, **kwargs)
shape = Tuple(*map(_sympify, shape))
cls._check_special_bounds(flat_list, shape)
loop_size = functools.reduce(lambda x,y: x*y, shape) if shape else len(flat_list)
# Sparse array:
if isinstance(flat_list, (dict, Dict)):
sparse_array = Dict(flat_list)
else:
sparse_array = {}
for i, el in enumerate(flatten(flat_list)):
if el != 0:
sparse_array[i] = _sympify(el)
sparse_array = Dict(sparse_array)
self = Basic.__new__(cls, sparse_array, shape, **kwargs)
self._shape = shape
self._rank = len(shape)
self._loop_size = loop_size
self._sparse_array = sparse_array
return self
def __setitem__(self, index, value):
raise TypeError("immutable N-dim array")
def as_mutable(self):
return MutableSparseNDimArray(self)
class MutableSparseNDimArray(MutableNDimArray, SparseNDimArray):
def __new__(cls, iterable=None, shape=None, **kwargs):
from sympy.utilities.iterables import flatten
shape, flat_list = cls._handle_ndarray_creation_inputs(iterable, shape, **kwargs)
self = object.__new__(cls)
self._shape = shape
self._rank = len(shape)
self._loop_size = functools.reduce(lambda x,y: x*y, shape) if shape else len(flat_list)
# Sparse array:
if isinstance(flat_list, (dict, Dict)):
self._sparse_array = dict(flat_list)
return self
self._sparse_array = {}
for i, el in enumerate(flatten(flat_list)):
if el != 0:
self._sparse_array[i] = _sympify(el)
return self
def __setitem__(self, index, value):
"""Allows to set items to MutableDenseNDimArray.
Examples
========
>>> from sympy import MutableSparseNDimArray
>>> a = MutableSparseNDimArray.zeros(2, 2)
>>> a[0, 0] = 1
>>> a[1, 1] = 1
>>> a
[[1, 0], [0, 1]]
"""
if isinstance(index, tuple) and any([isinstance(i, slice) for i in index]):
value, eindices, slice_offsets = self._get_slice_data_for_array_assignment(index, value)
for i in eindices:
other_i = [ind - j for ind, j in zip(i, slice_offsets) if j is not None]
other_value = value[other_i]
complete_index = self._parse_index(i)
if other_value != 0:
self._sparse_array[complete_index] = other_value
elif complete_index in self._sparse_array:
self._sparse_array.pop(complete_index)
else:
index = self._parse_index(index)
value = _sympify(value)
if value == 0 and index in self._sparse_array:
self._sparse_array.pop(index)
else:
self._sparse_array[index] = value
def as_immutable(self):
return ImmutableSparseNDimArray(self)
@property
def free_symbols(self):
return {i for j in self._sparse_array.values() for i in j.free_symbols}
|
a27fabb67087df4330dee2fb6d470ffc8b67178b3a2397e2ef133df2e11829a8 | from __future__ import print_function, division
from sympy import Basic
from sympy import S
from sympy.core.expr import Expr
from sympy.core.numbers import Integer
from sympy.core.sympify import sympify
from sympy.core.compatibility import SYMPY_INTS, Iterable
import itertools
class NDimArray(object):
"""
Examples
========
Create an N-dim array of zeros:
>>> from sympy import MutableDenseNDimArray
>>> a = MutableDenseNDimArray.zeros(2, 3, 4)
>>> a
[[[0, 0, 0, 0], [0, 0, 0, 0], [0, 0, 0, 0]], [[0, 0, 0, 0], [0, 0, 0, 0], [0, 0, 0, 0]]]
Create an N-dim array from a list;
>>> a = MutableDenseNDimArray([[2, 3], [4, 5]])
>>> a
[[2, 3], [4, 5]]
>>> b = MutableDenseNDimArray([[[1, 2], [3, 4], [5, 6]], [[7, 8], [9, 10], [11, 12]]])
>>> b
[[[1, 2], [3, 4], [5, 6]], [[7, 8], [9, 10], [11, 12]]]
Create an N-dim array from a flat list with dimension shape:
>>> a = MutableDenseNDimArray([1, 2, 3, 4, 5, 6], (2, 3))
>>> a
[[1, 2, 3], [4, 5, 6]]
Create an N-dim array from a matrix:
>>> from sympy import Matrix
>>> a = Matrix([[1,2],[3,4]])
>>> a
Matrix([
[1, 2],
[3, 4]])
>>> b = MutableDenseNDimArray(a)
>>> b
[[1, 2], [3, 4]]
Arithmetic operations on N-dim arrays
>>> a = MutableDenseNDimArray([1, 1, 1, 1], (2, 2))
>>> b = MutableDenseNDimArray([4, 4, 4, 4], (2, 2))
>>> c = a + b
>>> c
[[5, 5], [5, 5]]
>>> a - b
[[-3, -3], [-3, -3]]
"""
_diff_wrt = True
def __new__(cls, iterable, shape=None, **kwargs):
from sympy.tensor.array import ImmutableDenseNDimArray
return ImmutableDenseNDimArray(iterable, shape, **kwargs)
def _parse_index(self, index):
if isinstance(index, (SYMPY_INTS, Integer)):
raise ValueError("Only a tuple index is accepted")
if self._loop_size == 0:
raise ValueError("Index not valide with an empty array")
if len(index) != self._rank:
raise ValueError('Wrong number of array axes')
real_index = 0
# check if input index can exist in current indexing
for i in range(self._rank):
if index[i] >= self.shape[i]:
raise ValueError('Index ' + str(index) + ' out of border')
real_index = real_index*self.shape[i] + index[i]
return real_index
def _get_tuple_index(self, integer_index):
index = []
for i, sh in enumerate(reversed(self.shape)):
index.append(integer_index % sh)
integer_index //= sh
index.reverse()
return tuple(index)
def _check_symbolic_index(self, index):
# Check if any index is symbolic:
tuple_index = (index if isinstance(index, tuple) else (index,))
if any([(isinstance(i, Expr) and (not i.is_number)) for i in tuple_index]):
for i, nth_dim in zip(tuple_index, self.shape):
if ((i < 0) == True) or ((i >= nth_dim) == True):
raise ValueError("index out of range")
from sympy.tensor import Indexed
return Indexed(self, *tuple_index)
return None
def _setter_iterable_check(self, value):
from sympy.matrices.matrices import MatrixBase
if isinstance(value, (Iterable, MatrixBase, NDimArray)):
raise NotImplementedError
@classmethod
def _scan_iterable_shape(cls, iterable):
def f(pointer):
if not isinstance(pointer, Iterable):
return [pointer], ()
result = []
elems, shapes = zip(*[f(i) for i in pointer])
if len(set(shapes)) != 1:
raise ValueError("could not determine shape unambiguously")
for i in elems:
result.extend(i)
return result, (len(shapes),)+shapes[0]
return f(iterable)
@classmethod
def _handle_ndarray_creation_inputs(cls, iterable=None, shape=None, **kwargs):
from sympy.matrices.matrices import MatrixBase
from sympy.tensor.array import SparseNDimArray
from sympy import Dict, Tuple
if shape is None:
if iterable is None:
shape = ()
iterable = ()
# Construction of a sparse array from a sparse array
elif isinstance(iterable, SparseNDimArray):
return iterable._shape, iterable._sparse_array
# Construct N-dim array from an iterable (numpy arrays included):
elif isinstance(iterable, Iterable):
iterable, shape = cls._scan_iterable_shape(iterable)
# Construct N-dim array from a Matrix:
elif isinstance(iterable, MatrixBase):
shape = iterable.shape
# Construct N-dim array from another N-dim array:
elif isinstance(iterable, NDimArray):
shape = iterable.shape
else:
shape = ()
iterable = (iterable,)
if isinstance(iterable, (Dict, dict)) and shape is not None:
new_dict = iterable.copy()
for k, v in new_dict.items():
if isinstance(k, (tuple, Tuple)):
new_key = 0
for i, idx in enumerate(k):
new_key = new_key * shape[i] + idx
iterable[new_key] = iterable[k]
del iterable[k]
if isinstance(shape, (SYMPY_INTS, Integer)):
shape = (shape,)
if any([not isinstance(dim, (SYMPY_INTS, Integer)) for dim in shape]):
raise TypeError("Shape should contain integers only.")
return tuple(shape), iterable
def __len__(self):
"""Overload common function len(). Returns number of elements in array.
Examples
========
>>> from sympy import MutableDenseNDimArray
>>> a = MutableDenseNDimArray.zeros(3, 3)
>>> a
[[0, 0, 0], [0, 0, 0], [0, 0, 0]]
>>> len(a)
9
"""
return self._loop_size
@property
def shape(self):
"""
Returns array shape (dimension).
Examples
========
>>> from sympy import MutableDenseNDimArray
>>> a = MutableDenseNDimArray.zeros(3, 3)
>>> a.shape
(3, 3)
"""
return self._shape
def rank(self):
"""
Returns rank of array.
Examples
========
>>> from sympy import MutableDenseNDimArray
>>> a = MutableDenseNDimArray.zeros(3,4,5,6,3)
>>> a.rank()
5
"""
return self._rank
def diff(self, *args, **kwargs):
"""
Calculate the derivative of each element in the array.
Examples
========
>>> from sympy import ImmutableDenseNDimArray
>>> from sympy.abc import x, y
>>> M = ImmutableDenseNDimArray([[x, y], [1, x*y]])
>>> M.diff(x)
[[1, 0], [0, y]]
"""
from sympy import Derivative
kwargs.setdefault('evaluate', True)
return Derivative(self.as_immutable(), *args, **kwargs)
def _accept_eval_derivative(self, s):
return s._visit_eval_derivative_array(self)
def _visit_eval_derivative_scalar(self, base):
# Types are (base: scalar, self: array)
return self.applyfunc(lambda x: base.diff(x))
def _visit_eval_derivative_array(self, base):
# Types are (base: array/matrix, self: array)
from sympy import derive_by_array
return derive_by_array(base, self)
def _eval_derivative_n_times(self, s, n):
return Basic._eval_derivative_n_times(self, s, n)
def _eval_derivative(self, arg):
return self.applyfunc(lambda x: x.diff(arg))
def _eval_derivative_array(self, arg):
from sympy import derive_by_array
from sympy import Tuple
from sympy import SparseNDimArray
from sympy.matrices.common import MatrixCommon
if isinstance(arg, (Iterable, Tuple, MatrixCommon, NDimArray)):
return derive_by_array(self, arg)
else:
return self.applyfunc(lambda x: x.diff(arg))
def applyfunc(self, f):
"""Apply a function to each element of the N-dim array.
Examples
========
>>> from sympy import ImmutableDenseNDimArray
>>> m = ImmutableDenseNDimArray([i*2+j for i in range(2) for j in range(2)], (2, 2))
>>> m
[[0, 1], [2, 3]]
>>> m.applyfunc(lambda i: 2*i)
[[0, 2], [4, 6]]
"""
from sympy.tensor.array import SparseNDimArray
from sympy.tensor.array.arrayop import Flatten
if isinstance(self, SparseNDimArray) and f(S.Zero) == 0:
return type(self)({k: f(v) for k, v in self._sparse_array.items() if f(v) != 0}, self.shape)
return type(self)(map(f, Flatten(self)), self.shape)
def __str__(self):
"""Returns string, allows to use standard functions print() and str().
Examples
========
>>> from sympy import MutableDenseNDimArray
>>> a = MutableDenseNDimArray.zeros(2, 2)
>>> a
[[0, 0], [0, 0]]
"""
def f(sh, shape_left, i, j):
if len(shape_left) == 1:
return "["+", ".join([str(self[self._get_tuple_index(e)]) for e in range(i, j)])+"]"
sh //= shape_left[0]
return "[" + ", ".join([f(sh, shape_left[1:], i+e*sh, i+(e+1)*sh) for e in range(shape_left[0])]) + "]" # + "\n"*len(shape_left)
if self.rank() == 0:
return self[()].__str__()
return f(self._loop_size, self.shape, 0, self._loop_size)
def __repr__(self):
return self.__str__()
# We don't define _repr_png_ here because it would add a large amount of
# data to any notebook containing SymPy expressions, without adding
# anything useful to the notebook. It can still enabled manually, e.g.,
# for the qtconsole, with init_printing().
def _repr_latex_(self):
"""
IPython/Jupyter LaTeX printing
To change the behavior of this (e.g., pass in some settings to LaTeX),
use init_printing(). init_printing() will also enable LaTeX printing
for built in numeric types like ints and container types that contain
SymPy objects, like lists and dictionaries of expressions.
"""
from sympy.printing.latex import latex
s = latex(self, mode='plain')
return "$\\displaystyle %s$" % s
_repr_latex_orig = _repr_latex_
def tolist(self):
"""
Converting MutableDenseNDimArray to one-dim list
Examples
========
>>> from sympy import MutableDenseNDimArray
>>> a = MutableDenseNDimArray([1, 2, 3, 4], (2, 2))
>>> a
[[1, 2], [3, 4]]
>>> b = a.tolist()
>>> b
[[1, 2], [3, 4]]
"""
def f(sh, shape_left, i, j):
if len(shape_left) == 1:
return [self[self._get_tuple_index(e)] for e in range(i, j)]
result = []
sh //= shape_left[0]
for e in range(shape_left[0]):
result.append(f(sh, shape_left[1:], i+e*sh, i+(e+1)*sh))
return result
return f(self._loop_size, self.shape, 0, self._loop_size)
def __add__(self, other):
from sympy.tensor.array.arrayop import Flatten
if not isinstance(other, NDimArray):
raise TypeError(str(other))
if self.shape != other.shape:
raise ValueError("array shape mismatch")
result_list = [i+j for i,j in zip(Flatten(self), Flatten(other))]
return type(self)(result_list, self.shape)
def __sub__(self, other):
from sympy.tensor.array.arrayop import Flatten
if not isinstance(other, NDimArray):
raise TypeError(str(other))
if self.shape != other.shape:
raise ValueError("array shape mismatch")
result_list = [i-j for i,j in zip(Flatten(self), Flatten(other))]
return type(self)(result_list, self.shape)
def __mul__(self, other):
from sympy.matrices.matrices import MatrixBase
from sympy.tensor.array import SparseNDimArray
from sympy.tensor.array.arrayop import Flatten
if isinstance(other, (Iterable, NDimArray, MatrixBase)):
raise ValueError("scalar expected, use tensorproduct(...) for tensorial product")
other = sympify(other)
if isinstance(self, SparseNDimArray):
if(other == S.Zero):
return type(self)({}, self.shape)
return type(self)({k: other*v for (k, v) in self._sparse_array.items()}, self.shape)
result_list = [i*other for i in Flatten(self)]
return type(self)(result_list, self.shape)
def __rmul__(self, other):
from sympy.matrices.matrices import MatrixBase
from sympy.tensor.array import SparseNDimArray
from sympy.tensor.array.arrayop import Flatten
if isinstance(other, (Iterable, NDimArray, MatrixBase)):
raise ValueError("scalar expected, use tensorproduct(...) for tensorial product")
other = sympify(other)
if isinstance(self, SparseNDimArray):
if(other == S.Zero):
return type(self)({}, self.shape)
return type(self)({k: other*v for (k, v) in self._sparse_array.items()}, self.shape)
result_list = [other*i for i in Flatten(self)]
return type(self)(result_list, self.shape)
def __div__(self, other):
from sympy.matrices.matrices import MatrixBase
from sympy.tensor.array import SparseNDimArray
from sympy.tensor.array.arrayop import Flatten
if isinstance(other, (Iterable, NDimArray, MatrixBase)):
raise ValueError("scalar expected")
other = sympify(other)
if isinstance(self, SparseNDimArray) and other != S.Zero:
return type(self)({k: v/other for (k, v) in self._sparse_array.items()}, self.shape)
result_list = [i/other for i in Flatten(self)]
return type(self)(result_list, self.shape)
def __rdiv__(self, other):
raise NotImplementedError('unsupported operation on NDimArray')
def __neg__(self):
from sympy.tensor.array import SparseNDimArray
from sympy.tensor.array.arrayop import Flatten
if isinstance(self, SparseNDimArray):
return type(self)({k: -v for (k, v) in self._sparse_array.items()}, self.shape)
result_list = [-i for i in Flatten(self)]
return type(self)(result_list, self.shape)
def __iter__(self):
def iterator():
if self._shape:
for i in range(self._shape[0]):
yield self[i]
else:
yield self[()]
return iterator()
def __eq__(self, other):
"""
NDimArray instances can be compared to each other.
Instances equal if they have same shape and data.
Examples
========
>>> from sympy import MutableDenseNDimArray
>>> a = MutableDenseNDimArray.zeros(2, 3)
>>> b = MutableDenseNDimArray.zeros(2, 3)
>>> a == b
True
>>> c = a.reshape(3, 2)
>>> c == b
False
>>> a[0,0] = 1
>>> b[0,0] = 2
>>> a == b
False
"""
from sympy.tensor.array import SparseNDimArray
if not isinstance(other, NDimArray):
return False
if not self.shape == other.shape:
return False
if isinstance(self, SparseNDimArray) and isinstance(other, SparseNDimArray):
return dict(self._sparse_array) == dict(other._sparse_array)
return list(self) == list(other)
def __ne__(self, other):
return not self == other
__truediv__ = __div__
__rtruediv__ = __rdiv__
def _eval_transpose(self):
if self.rank() != 2:
raise ValueError("array rank not 2")
from .arrayop import permutedims
return permutedims(self, (1, 0))
def transpose(self):
return self._eval_transpose()
def _eval_conjugate(self):
from sympy.tensor.array.arrayop import Flatten
return self.func([i.conjugate() for i in Flatten(self)], self.shape)
def conjugate(self):
return self._eval_conjugate()
def _eval_adjoint(self):
return self.transpose().conjugate()
def adjoint(self):
return self._eval_adjoint()
def _slice_expand(self, s, dim):
if not isinstance(s, slice):
return (s,)
start, stop, step = s.indices(dim)
return [start + i*step for i in range((stop-start)//step)]
def _get_slice_data_for_array_access(self, index):
sl_factors = [self._slice_expand(i, dim) for (i, dim) in zip(index, self.shape)]
eindices = itertools.product(*sl_factors)
return sl_factors, eindices
def _get_slice_data_for_array_assignment(self, index, value):
if not isinstance(value, NDimArray):
value = type(self)(value)
sl_factors, eindices = self._get_slice_data_for_array_access(index)
slice_offsets = [min(i) if isinstance(i, list) else None for i in sl_factors]
# TODO: add checks for dimensions for `value`?
return value, eindices, slice_offsets
@classmethod
def _check_special_bounds(cls, flat_list, shape):
if shape == () and len(flat_list) != 1:
raise ValueError("arrays without shape need one scalar value")
if shape == (0,) and len(flat_list) > 0:
raise ValueError("if array shape is (0,) there cannot be elements")
def _check_index_for_getitem(self, index):
if isinstance(index, (SYMPY_INTS, Integer, slice)):
index = (index, )
if len(index) < self.rank():
index = tuple([i for i in index] + \
[slice(None) for i in range(len(index), self.rank())])
if len(index) > self.rank():
raise ValueError('Dimension of index greater than rank of array')
return index
class ImmutableNDimArray(NDimArray, Basic):
_op_priority = 11.0
def __hash__(self):
return Basic.__hash__(self)
def as_immutable(self):
return self
def as_mutable(self):
raise NotImplementedError("abstract method")
|
81a99c9134c77a8ec2a59684b3927538de91c9d6daa9adf1c464d09e23d38faa | from __future__ import print_function, division
import functools
from sympy import Basic, Tuple, S
from sympy.core.sympify import _sympify
from sympy.tensor.array.mutable_ndim_array import MutableNDimArray
from sympy.tensor.array.ndim_array import NDimArray, ImmutableNDimArray
from sympy.core.compatibility import SYMPY_INTS
from sympy.core.numbers import Integer
class DenseNDimArray(NDimArray):
def __new__(self, *args, **kwargs):
return ImmutableDenseNDimArray(*args, **kwargs)
def __getitem__(self, index):
"""
Allows to get items from N-dim array.
Examples
========
>>> from sympy import MutableDenseNDimArray
>>> a = MutableDenseNDimArray([0, 1, 2, 3], (2, 2))
>>> a
[[0, 1], [2, 3]]
>>> a[0, 0]
0
>>> a[1, 1]
3
>>> a[0]
[0, 1]
>>> a[1]
[2, 3]
Symbolic index:
>>> from sympy.abc import i, j
>>> a[i, j]
[[0, 1], [2, 3]][i, j]
Replace `i` and `j` to get element `(1, 1)`:
>>> a[i, j].subs({i: 1, j: 1})
3
"""
syindex = self._check_symbolic_index(index)
if syindex is not None:
return syindex
index = self._check_index_for_getitem(index)
if isinstance(index, tuple) and any([isinstance(i, slice) for i in index]):
sl_factors, eindices = self._get_slice_data_for_array_access(index)
array = [self._array[self._parse_index(i)] for i in eindices]
nshape = [len(el) for i, el in enumerate(sl_factors) if isinstance(index[i], slice)]
return type(self)(array, nshape)
else:
index = self._parse_index(index)
return self._array[index]
@classmethod
def zeros(cls, *shape):
list_length = functools.reduce(lambda x, y: x*y, shape, S.One)
return cls._new(([0]*list_length,), shape)
def tomatrix(self):
"""
Converts MutableDenseNDimArray to Matrix. Can convert only 2-dim array, else will raise error.
Examples
========
>>> from sympy import MutableDenseNDimArray
>>> a = MutableDenseNDimArray([1 for i in range(9)], (3, 3))
>>> b = a.tomatrix()
>>> b
Matrix([
[1, 1, 1],
[1, 1, 1],
[1, 1, 1]])
"""
from sympy.matrices import Matrix
if self.rank() != 2:
raise ValueError('Dimensions must be of size of 2')
return Matrix(self.shape[0], self.shape[1], self._array)
def reshape(self, *newshape):
"""
Returns MutableDenseNDimArray instance with new shape. Elements number
must be suitable to new shape. The only argument of method sets
new shape.
Examples
========
>>> from sympy import MutableDenseNDimArray
>>> a = MutableDenseNDimArray([1, 2, 3, 4, 5, 6], (2, 3))
>>> a.shape
(2, 3)
>>> a
[[1, 2, 3], [4, 5, 6]]
>>> b = a.reshape(3, 2)
>>> b.shape
(3, 2)
>>> b
[[1, 2], [3, 4], [5, 6]]
"""
new_total_size = functools.reduce(lambda x,y: x*y, newshape)
if new_total_size != self._loop_size:
raise ValueError("Invalid reshape parameters " + newshape)
# there is no `.func` as this class does not subtype `Basic`:
return type(self)(self._array, newshape)
class ImmutableDenseNDimArray(DenseNDimArray, ImmutableNDimArray):
"""
"""
def __new__(cls, iterable, shape=None, **kwargs):
return cls._new(iterable, shape, **kwargs)
@classmethod
def _new(cls, iterable, shape, **kwargs):
from sympy.utilities.iterables import flatten
shape, flat_list = cls._handle_ndarray_creation_inputs(iterable, shape, **kwargs)
shape = Tuple(*map(_sympify, shape))
cls._check_special_bounds(flat_list, shape)
flat_list = flatten(flat_list)
flat_list = Tuple(*flat_list)
self = Basic.__new__(cls, flat_list, shape, **kwargs)
self._shape = shape
self._array = list(flat_list)
self._rank = len(shape)
self._loop_size = functools.reduce(lambda x,y: x*y, shape, 1)
return self
def __setitem__(self, index, value):
raise TypeError('immutable N-dim array')
def as_mutable(self):
return MutableDenseNDimArray(self)
class MutableDenseNDimArray(DenseNDimArray, MutableNDimArray):
def __new__(cls, iterable=None, shape=None, **kwargs):
return cls._new(iterable, shape, **kwargs)
@classmethod
def _new(cls, iterable, shape, **kwargs):
from sympy.utilities.iterables import flatten
shape, flat_list = cls._handle_ndarray_creation_inputs(iterable, shape, **kwargs)
flat_list = flatten(flat_list)
self = object.__new__(cls)
self._shape = shape
self._array = list(flat_list)
self._rank = len(shape)
self._loop_size = functools.reduce(lambda x,y: x*y, shape) if shape else len(flat_list)
return self
def __setitem__(self, index, value):
"""Allows to set items to MutableDenseNDimArray.
Examples
========
>>> from sympy import MutableDenseNDimArray
>>> a = MutableDenseNDimArray.zeros(2, 2)
>>> a[0,0] = 1
>>> a[1,1] = 1
>>> a
[[1, 0], [0, 1]]
"""
if isinstance(index, tuple) and any([isinstance(i, slice) for i in index]):
value, eindices, slice_offsets = self._get_slice_data_for_array_assignment(index, value)
for i in eindices:
other_i = [ind - j for ind, j in zip(i, slice_offsets) if j is not None]
self._array[self._parse_index(i)] = value[other_i]
else:
index = self._parse_index(index)
self._setter_iterable_check(value)
value = _sympify(value)
self._array[index] = value
def as_immutable(self):
return ImmutableDenseNDimArray(self)
@property
def free_symbols(self):
return {i for j in self._array for i in j.free_symbols}
|
5a18f3eef058d81532cba0f0760e2ea85beee8484c55a1ac415dee11b6057093 | from sympy.tensor.toperators import PartialDerivative
from sympy.tensor.tensor import TensorIndexType, tensor_indices, TensorHead, \
tensor_heads
from sympy import symbols, diag
from sympy import Array
L = TensorIndexType("L")
i, j, k = tensor_indices("i j k", L)
i0 = tensor_indices("i0", L)
L_0 = tensor_indices("L_0", L)
A, B, C, D = tensor_heads("A B C D", [L])
H = TensorHead("H", [L, L])
def test_tensor_partial_deriv():
# Test flatten:
expr = PartialDerivative(PartialDerivative(A(i), A(j)), A(-i))
assert expr.expr == A(L_0)
assert expr.variables == (A(j), A(-L_0))
expr1 = PartialDerivative(A(i), A(j))
assert expr1.expr == A(i)
assert expr1.variables == (A(j),)
expr2 = A(i)*PartialDerivative(H(k, -i), A(j))
assert expr2.get_indices() == [L_0, k, -L_0, j]
expr3 = A(i)*PartialDerivative(B(k)*C(-i) + 3*H(k, -i), A(j))
assert expr3.get_indices() == [L_0, k, -L_0, j]
expr4 = (A(i) + B(i))*PartialDerivative(C(-j), D(j))
assert expr4.get_indices() == [i, -L_0, L_0]
expr5 = (A(i) + B(i))*PartialDerivative(C(-i), D(j))
assert expr5.get_indices() == [L_0, -L_0, j]
def test_replace_arrays_partial_derivative():
x, y, z, t = symbols("x y z t")
expr = PartialDerivative(A(i), A(j))
assert expr.replace_with_arrays({A(i): [x, y]}, [i, j]) == Array([[1, 0], [0, 1]])
expr = PartialDerivative(A(i), A(-i))
assert expr.replace_with_arrays({A(i): [x, y], L: diag(1, 1)}, []) == 2
assert expr.replace_with_arrays({A(i): [x, y], L: diag(1, -1)}, []) == 0
expr = PartialDerivative(A(-i), A(i))
assert expr.replace_with_arrays({A(i): [x, y], L: diag(1, 1)}, []) == 2
assert expr.replace_with_arrays({A(i): [x, y], L: diag(1, -1)}, []) == 0
|
d2051f3bce6d83d324be0ba34a48806fa7f28e0ccf904b72f3f72e54ca16e7fb | from functools import wraps
from sympy import Matrix, eye, Integer, expand, Indexed, Sum
from sympy.combinatorics import Permutation
from sympy.core import S, Rational, Symbol, Basic, Add
from sympy.core.containers import Tuple
from sympy.core.symbol import symbols
from sympy.functions.elementary.miscellaneous import sqrt
from sympy.printing.pretty.pretty import pretty
from sympy.tensor.array import Array
from sympy.tensor.tensor import TensorIndexType, tensor_indices, TensorSymmetry, \
get_symmetric_group_sgs, TensorIndex, tensor_mul, TensAdd, \
riemann_cyclic_replace, riemann_cyclic, TensMul, tensor_heads, \
TensorManager, TensExpr, TensorHead, canon_bp, \
tensorhead, tensorsymmetry, TensorType
from sympy.utilities.pytest import raises, XFAIL, warns_deprecated_sympy, ignore_warnings
from sympy.utilities.exceptions import SymPyDeprecationWarning
from sympy.core.compatibility import range
from sympy.matrices import diag
def filter_warnings_decorator(f):
@wraps(f)
def wrapper():
with ignore_warnings(SymPyDeprecationWarning):
f()
return wrapper
def _is_equal(arg1, arg2):
if isinstance(arg1, TensExpr):
return arg1.equals(arg2)
elif isinstance(arg2, TensExpr):
return arg2.equals(arg1)
return arg1 == arg2
#################### Tests from tensor_can.py #######################
def test_canonicalize_no_slot_sym():
# A_d0 * B^d0; T_c = A^d0*B_d0
Lorentz = TensorIndexType('Lorentz', dummy_fmt='L')
a, b, d0, d1 = tensor_indices('a,b,d0,d1', Lorentz)
A, B = tensor_heads('A,B', [Lorentz], TensorSymmetry.no_symmetry(1))
t = A(-d0)*B(d0)
tc = t.canon_bp()
assert str(tc) == 'A(L_0)*B(-L_0)'
# A^a * B^b; T_c = T
t = A(a)*B(b)
tc = t.canon_bp()
assert tc == t
# B^b * A^a
t1 = B(b)*A(a)
tc = t1.canon_bp()
assert str(tc) == 'A(a)*B(b)'
# A symmetric
# A^{b}_{d0}*A^{d0, a}; T_c = A^{a d0}*A{b}_{d0}
A = TensorHead('A', [Lorentz]*2, TensorSymmetry.fully_symmetric(2))
t = A(b, -d0)*A(d0, a)
tc = t.canon_bp()
assert str(tc) == 'A(a, L_0)*A(b, -L_0)'
# A^{d1}_{d0}*B^d0*C_d1
# T_c = A^{d0 d1}*B_d0*C_d1
B, C = tensor_heads('B,C', [Lorentz], TensorSymmetry.no_symmetry(1))
t = A(d1, -d0)*B(d0)*C(-d1)
tc = t.canon_bp()
assert str(tc) == 'A(L_0, L_1)*B(-L_0)*C(-L_1)'
# A without symmetry
# A^{d1}_{d0}*B^d0*C_d1 ord=[d0,-d0,d1,-d1]; g = [2,1,0,3,4,5]
# T_c = A^{d0 d1}*B_d1*C_d0; can = [0,2,3,1,4,5]
A = TensorHead('A', [Lorentz]*2, TensorSymmetry.no_symmetry(2))
t = A(d1, -d0)*B(d0)*C(-d1)
tc = t.canon_bp()
assert str(tc) == 'A(L_0, L_1)*B(-L_1)*C(-L_0)'
# A, B without symmetry
# A^{d1}_{d0}*B_{d1}^{d0}
# T_c = A^{d0 d1}*B_{d0 d1}
B = TensorHead('B', [Lorentz]*2, TensorSymmetry.no_symmetry(2))
t = A(d1, -d0)*B(-d1, d0)
tc = t.canon_bp()
assert str(tc) == 'A(L_0, L_1)*B(-L_0, -L_1)'
# A_{d0}^{d1}*B_{d1}^{d0}
# T_c = A^{d0 d1}*B_{d1 d0}
t = A(-d0, d1)*B(-d1, d0)
tc = t.canon_bp()
assert str(tc) == 'A(L_0, L_1)*B(-L_1, -L_0)'
# A, B, C without symmetry
# A^{d1 d0}*B_{a d0}*C_{d1 b}
# T_c=A^{d0 d1}*B_{a d1}*C_{d0 b}
C = TensorHead('C', [Lorentz]*2, TensorSymmetry.no_symmetry(2))
t = A(d1, d0)*B(-a, -d0)*C(-d1, -b)
tc = t.canon_bp()
assert str(tc) == 'A(L_0, L_1)*B(-a, -L_1)*C(-L_0, -b)'
# A symmetric, B and C without symmetry
# A^{d1 d0}*B_{a d0}*C_{d1 b}
# T_c = A^{d0 d1}*B_{a d0}*C_{d1 b}
A = TensorHead('A', [Lorentz]*2, TensorSymmetry.fully_symmetric(2))
t = A(d1, d0)*B(-a, -d0)*C(-d1, -b)
tc = t.canon_bp()
assert str(tc) == 'A(L_0, L_1)*B(-a, -L_0)*C(-L_1, -b)'
# A and C symmetric, B without symmetry
# A^{d1 d0}*B_{a d0}*C_{d1 b} ord=[a,b,d0,-d0,d1,-d1]
# T_c = A^{d0 d1}*B_{a d0}*C_{b d1}
C = TensorHead('C', [Lorentz]*2, TensorSymmetry.fully_symmetric(2))
t = A(d1, d0)*B(-a, -d0)*C(-d1, -b)
tc = t.canon_bp()
assert str(tc) == 'A(L_0, L_1)*B(-a, -L_0)*C(-b, -L_1)'
def test_canonicalize_no_dummies():
Lorentz = TensorIndexType('Lorentz', dummy_fmt='L')
a, b, c, d = tensor_indices('a, b, c, d', Lorentz)
# A commuting
# A^c A^b A^a
# T_c = A^a A^b A^c
A = TensorHead('A', [Lorentz], TensorSymmetry.no_symmetry(1))
t = A(c)*A(b)*A(a)
tc = t.canon_bp()
assert str(tc) == 'A(a)*A(b)*A(c)'
# A anticommuting
# A^c A^b A^a
# T_c = -A^a A^b A^c
A = TensorHead('A', [Lorentz], TensorSymmetry.no_symmetry(1), 1)
t = A(c)*A(b)*A(a)
tc = t.canon_bp()
assert str(tc) == '-A(a)*A(b)*A(c)'
# A commuting and symmetric
# A^{b,d}*A^{c,a}
# T_c = A^{a c}*A^{b d}
A = TensorHead('A', [Lorentz]*2, TensorSymmetry.fully_symmetric(2))
t = A(b, d)*A(c, a)
tc = t.canon_bp()
assert str(tc) == 'A(a, c)*A(b, d)'
# A anticommuting and symmetric
# A^{b,d}*A^{c,a}
# T_c = -A^{a c}*A^{b d}
A = TensorHead('A', [Lorentz]*2, TensorSymmetry.fully_symmetric(2), 1)
t = A(b, d)*A(c, a)
tc = t.canon_bp()
assert str(tc) == '-A(a, c)*A(b, d)'
# A^{c,a}*A^{b,d}
# T_c = A^{a c}*A^{b d}
t = A(c, a)*A(b, d)
tc = t.canon_bp()
assert str(tc) == 'A(a, c)*A(b, d)'
def test_tensorhead_construction_without_symmetry():
L = TensorIndexType('Lorentz')
A1 = TensorHead('A', [L, L])
A2 = TensorHead('A', [L, L], TensorSymmetry.no_symmetry(2))
assert A1 == A2
A3 = TensorHead('A', [L, L], TensorSymmetry.fully_symmetric(2)) # Symmetric
assert A1 != A3
def test_no_metric_symmetry():
# no metric symmetry; A no symmetry
# A^d1_d0 * A^d0_d1
# T_c = A^d0_d1 * A^d1_d0
Lorentz = TensorIndexType('Lorentz', metric=None, dummy_fmt='L')
d0, d1, d2, d3 = tensor_indices('d:4', Lorentz)
A = TensorHead('A', [Lorentz]*2, TensorSymmetry.no_symmetry(2))
t = A(d1, -d0)*A(d0, -d1)
tc = t.canon_bp()
assert str(tc) == 'A(L_0, -L_1)*A(L_1, -L_0)'
# A^d1_d2 * A^d0_d3 * A^d2_d1 * A^d3_d0
# T_c = A^d0_d1 * A^d1_d0 * A^d2_d3 * A^d3_d2
t = A(d1, -d2)*A(d0, -d3)*A(d2, -d1)*A(d3, -d0)
tc = t.canon_bp()
assert str(tc) == 'A(L_0, -L_1)*A(L_1, -L_0)*A(L_2, -L_3)*A(L_3, -L_2)'
# A^d0_d2 * A^d1_d3 * A^d3_d0 * A^d2_d1
# T_c = A^d0_d1 * A^d1_d2 * A^d2_d3 * A^d3_d0
t = A(d0, -d1)*A(d1, -d2)*A(d2, -d3)*A(d3, -d0)
tc = t.canon_bp()
assert str(tc) == 'A(L_0, -L_1)*A(L_1, -L_2)*A(L_2, -L_3)*A(L_3, -L_0)'
def test_canonicalize1():
Lorentz = TensorIndexType('Lorentz', dummy_fmt='L')
a, a0, a1, a2, a3, b, d0, d1, d2, d3 = \
tensor_indices('a,a0,a1,a2,a3,b,d0,d1,d2,d3', Lorentz)
# A_d0*A^d0; ord = [d0,-d0]
# T_c = A^d0*A_d0
A = TensorHead('A', [Lorentz], TensorSymmetry.no_symmetry(1))
t = A(-d0)*A(d0)
tc = t.canon_bp()
assert str(tc) == 'A(L_0)*A(-L_0)'
# A commuting
# A_d0*A_d1*A_d2*A^d2*A^d1*A^d0
# T_c = A^d0*A_d0*A^d1*A_d1*A^d2*A_d2
t = A(-d0)*A(-d1)*A(-d2)*A(d2)*A(d1)*A(d0)
tc = t.canon_bp()
assert str(tc) == 'A(L_0)*A(-L_0)*A(L_1)*A(-L_1)*A(L_2)*A(-L_2)'
# A anticommuting
# A_d0*A_d1*A_d2*A^d2*A^d1*A^d0
# T_c 0
A = TensorHead('A', [Lorentz], TensorSymmetry.no_symmetry(1), 1)
t = A(-d0)*A(-d1)*A(-d2)*A(d2)*A(d1)*A(d0)
tc = t.canon_bp()
assert tc == 0
# A commuting symmetric
# A^{d0 b}*A^a_d1*A^d1_d0
# T_c = A^{a d0}*A^{b d1}*A_{d0 d1}
A = TensorHead('A', [Lorentz]*2, TensorSymmetry.fully_symmetric(2))
t = A(d0, b)*A(a, -d1)*A(d1, -d0)
tc = t.canon_bp()
assert str(tc) == 'A(a, L_0)*A(b, L_1)*A(-L_0, -L_1)'
# A, B commuting symmetric
# A^{d0 b}*A^d1_d0*B^a_d1
# T_c = A^{b d0}*A_d0^d1*B^a_d1
B = TensorHead('B', [Lorentz]*2, TensorSymmetry.fully_symmetric(2))
t = A(d0, b)*A(d1, -d0)*B(a, -d1)
tc = t.canon_bp()
assert str(tc) == 'A(b, L_0)*A(-L_0, L_1)*B(a, -L_1)'
# A commuting symmetric
# A^{d1 d0 b}*A^{a}_{d1 d0}; ord=[a,b, d0,-d0,d1,-d1]
# T_c = A^{a d0 d1}*A^{b}_{d0 d1}
A = TensorHead('A', [Lorentz]*3, TensorSymmetry.fully_symmetric(3))
t = A(d1, d0, b)*A(a, -d1, -d0)
tc = t.canon_bp()
assert str(tc) == 'A(a, L_0, L_1)*A(b, -L_0, -L_1)'
# A^{d3 d0 d2}*A^a0_{d1 d2}*A^d1_d3^a1*A^{a2 a3}_d0
# T_c = A^{a0 d0 d1}*A^a1_d0^d2*A^{a2 a3 d3}*A_{d1 d2 d3}
t = A(d3, d0, d2)*A(a0, -d1, -d2)*A(d1, -d3, a1)*A(a2, a3, -d0)
tc = t.canon_bp()
assert str(tc) == 'A(a0, L_0, L_1)*A(a1, -L_0, L_2)*A(a2, a3, L_3)*A(-L_1, -L_2, -L_3)'
# A commuting symmetric, B antisymmetric
# A^{d0 d1 d2} * A_{d2 d3 d1} * B_d0^d3
# in this esxample and in the next three,
# renaming dummy indices and using symmetry of A,
# T = A^{d0 d1 d2} * A_{d0 d1 d3} * B_d2^d3
# can = 0
A = TensorHead('A', [Lorentz]*3, TensorSymmetry.fully_symmetric(3))
B = TensorHead('B', [Lorentz]*2, TensorSymmetry.fully_symmetric(-2))
t = A(d0, d1, d2)*A(-d2, -d3, -d1)*B(-d0, d3)
tc = t.canon_bp()
assert tc == 0
# A anticommuting symmetric, B antisymmetric
# A^{d0 d1 d2} * A_{d2 d3 d1} * B_d0^d3
# T_c = A^{d0 d1 d2} * A_{d0 d1}^d3 * B_{d2 d3}
A = TensorHead('A', [Lorentz]*3, TensorSymmetry.fully_symmetric(3), 1)
B = TensorHead('B', [Lorentz]*2, TensorSymmetry.fully_symmetric(-2))
t = A(d0, d1, d2)*A(-d2, -d3, -d1)*B(-d0, d3)
tc = t.canon_bp()
assert str(tc) == 'A(L_0, L_1, L_2)*A(-L_0, -L_1, L_3)*B(-L_2, -L_3)'
# A anticommuting symmetric, B antisymmetric commuting, antisymmetric metric
# A^{d0 d1 d2} * A_{d2 d3 d1} * B_d0^d3
# T_c = -A^{d0 d1 d2} * A_{d0 d1}^d3 * B_{d2 d3}
Spinor = TensorIndexType('Spinor', metric=1, dummy_fmt='S')
a, a0, a1, a2, a3, b, d0, d1, d2, d3 = \
tensor_indices('a,a0,a1,a2,a3,b,d0,d1,d2,d3', Spinor)
A = TensorHead('A', [Spinor]*3, TensorSymmetry.fully_symmetric(3), 1)
B = TensorHead('B', [Spinor]*2, TensorSymmetry.fully_symmetric(-2))
t = A(d0, d1, d2)*A(-d2, -d3, -d1)*B(-d0, d3)
tc = t.canon_bp()
assert str(tc) == '-A(S_0, S_1, S_2)*A(-S_0, -S_1, S_3)*B(-S_2, -S_3)'
# A anticommuting symmetric, B antisymmetric anticommuting,
# no metric symmetry
# A^{d0 d1 d2} * A_{d2 d3 d1} * B_d0^d3
# T_c = A^{d0 d1 d2} * A_{d0 d1 d3} * B_d2^d3
Mat = TensorIndexType('Mat', metric=None, dummy_fmt='M')
a, a0, a1, a2, a3, b, d0, d1, d2, d3 = \
tensor_indices('a,a0,a1,a2,a3,b,d0,d1,d2,d3', Mat)
A = TensorHead('A', [Mat]*3, TensorSymmetry.fully_symmetric(3), 1)
B = TensorHead('B', [Mat]*2, TensorSymmetry.fully_symmetric(-2))
t = A(d0, d1, d2)*A(-d2, -d3, -d1)*B(-d0, d3)
tc = t.canon_bp()
assert str(tc) == 'A(M_0, M_1, M_2)*A(-M_0, -M_1, -M_3)*B(-M_2, M_3)'
# Gamma anticommuting
# Gamma_{mu nu} * gamma^rho * Gamma^{nu mu alpha}
# T_c = -Gamma^{mu nu} * gamma^rho * Gamma_{alpha mu nu}
alpha, beta, gamma, mu, nu, rho = \
tensor_indices('alpha,beta,gamma,mu,nu,rho', Lorentz)
Gamma = TensorHead('Gamma', [Lorentz],
TensorSymmetry.fully_symmetric(1), 2)
Gamma2 = TensorHead('Gamma', [Lorentz]*2,
TensorSymmetry.fully_symmetric(-2), 2)
Gamma3 = TensorHead('Gamma', [Lorentz]*3,
TensorSymmetry.fully_symmetric(-3), 2)
t = Gamma2(-mu, -nu)*Gamma(rho)*Gamma3(nu, mu, alpha)
tc = t.canon_bp()
assert str(tc) == '-Gamma(L_0, L_1)*Gamma(rho)*Gamma(alpha, -L_0, -L_1)'
# Gamma_{mu nu} * Gamma^{gamma beta} * gamma_rho * Gamma^{nu mu alpha}
# T_c = Gamma^{mu nu} * Gamma^{beta gamma} * gamma_rho * Gamma^alpha_{mu nu}
t = Gamma2(mu, nu)*Gamma2(beta, gamma)*Gamma(-rho)*Gamma3(alpha, -mu, -nu)
tc = t.canon_bp()
assert str(tc) == 'Gamma(L_0, L_1)*Gamma(beta, gamma)*Gamma(-rho)*Gamma(alpha, -L_0, -L_1)'
# f^a_{b,c} antisymmetric in b,c; A_mu^a no symmetry
# f^c_{d a} * f_{c e b} * A_mu^d * A_nu^a * A^{nu e} * A^{mu b}
# g = [8,11,5, 9,13,7, 1,10, 3,4, 2,12, 0,6, 14,15]
# T_c = -f^{a b c} * f_a^{d e} * A^mu_b * A_{mu d} * A^nu_c * A_{nu e}
Flavor = TensorIndexType('Flavor', dummy_fmt='F')
a, b, c, d, e, ff = tensor_indices('a,b,c,d,e,f', Flavor)
mu, nu = tensor_indices('mu,nu', Lorentz)
f = TensorHead('f', [Flavor]*3, TensorSymmetry.direct_product(1, -2))
A = TensorHead('A', [Lorentz, Flavor], TensorSymmetry.no_symmetry(2))
t = f(c, -d, -a)*f(-c, -e, -b)*A(-mu, d)*A(-nu, a)*A(nu, e)*A(mu, b)
tc = t.canon_bp()
assert str(tc) == '-f(F_0, F_1, F_2)*f(-F_0, F_3, F_4)*A(L_0, -F_1)*A(-L_0, -F_3)*A(L_1, -F_2)*A(-L_1, -F_4)'
def test_bug_correction_tensor_indices():
# to make sure that tensor_indices does not return a list if creating
# only one index:
A = TensorIndexType("A")
i = tensor_indices('i', A)
assert not isinstance(i, (tuple, list))
assert isinstance(i, TensorIndex)
def test_riemann_invariants():
Lorentz = TensorIndexType('Lorentz', dummy_fmt='L')
d0, d1, d2, d3, d4, d5, d6, d7, d8, d9, d10, d11 = \
tensor_indices('d0:12', Lorentz)
# R^{d0 d1}_{d1 d0}; ord = [d0,-d0,d1,-d1]
# T_c = -R^{d0 d1}_{d0 d1}
R = TensorHead('R', [Lorentz]*4, TensorSymmetry.riemann())
t = R(d0, d1, -d1, -d0)
tc = t.canon_bp()
assert str(tc) == '-R(L_0, L_1, -L_0, -L_1)'
# R_d11^d1_d0^d5 * R^{d6 d4 d0}_d5 * R_{d7 d2 d8 d9} *
# R_{d10 d3 d6 d4} * R^{d2 d7 d11}_d1 * R^{d8 d9 d3 d10}
# can = [0,2,4,6, 1,3,8,10, 5,7,12,14, 9,11,16,18, 13,15,20,22,
# 17,19,21<F10,23, 24,25]
# T_c = R^{d0 d1 d2 d3} * R_{d0 d1}^{d4 d5} * R_{d2 d3}^{d6 d7} *
# R_{d4 d5}^{d8 d9} * R_{d6 d7}^{d10 d11} * R_{d8 d9 d10 d11}
t = R(-d11,d1,-d0,d5)*R(d6,d4,d0,-d5)*R(-d7,-d2,-d8,-d9)* \
R(-d10,-d3,-d6,-d4)*R(d2,d7,d11,-d1)*R(d8,d9,d3,d10)
tc = t.canon_bp()
assert str(tc) == 'R(L_0, L_1, L_2, L_3)*R(-L_0, -L_1, L_4, L_5)*R(-L_2, -L_3, L_6, L_7)*R(-L_4, -L_5, L_8, L_9)*R(-L_6, -L_7, L_10, L_11)*R(-L_8, -L_9, -L_10, -L_11)'
def test_riemann_products():
Lorentz = TensorIndexType('Lorentz', dummy_fmt='L')
d0, d1, d2, d3, d4, d5, d6 = tensor_indices('d0:7', Lorentz)
a0, a1, a2, a3, a4, a5 = tensor_indices('a0:6', Lorentz)
a, b = tensor_indices('a,b', Lorentz)
R = TensorHead('R', [Lorentz]*4, TensorSymmetry.riemann())
# R^{a b d0}_d0 = 0
t = R(a, b, d0, -d0)
tc = t.canon_bp()
assert tc == 0
# R^{d0 b a}_d0
# T_c = -R^{a d0 b}_d0
t = R(d0, b, a, -d0)
tc = t.canon_bp()
assert str(tc) == '-R(a, L_0, b, -L_0)'
# R^d1_d2^b_d0 * R^{d0 a}_d1^d2; ord=[a,b,d0,-d0,d1,-d1,d2,-d2]
# T_c = -R^{a d0 d1 d2}* R^b_{d0 d1 d2}
t = R(d1, -d2, b, -d0)*R(d0, a, -d1, d2)
tc = t.canon_bp()
assert str(tc) == '-R(a, L_0, L_1, L_2)*R(b, -L_0, -L_1, -L_2)'
# A symmetric commuting
# R^{d6 d5}_d2^d1 * R^{d4 d0 d2 d3} * A_{d6 d0} A_{d3 d1} * A_{d4 d5}
# g = [12,10,5,2, 8,0,4,6, 13,1, 7,3, 9,11,14,15]
# T_c = -R^{d0 d1 d2 d3} * R_d0^{d4 d5 d6} * A_{d1 d4}*A_{d2 d5}*A_{d3 d6}
V = TensorHead('V', [Lorentz]*2, TensorSymmetry.fully_symmetric(2))
t = R(d6, d5, -d2, d1)*R(d4, d0, d2, d3)*V(-d6, -d0)*V(-d3, -d1)*V(-d4, -d5)
tc = t.canon_bp()
assert str(tc) == '-R(L_0, L_1, L_2, L_3)*R(-L_0, L_4, L_5, L_6)*V(-L_1, -L_4)*V(-L_2, -L_5)*V(-L_3, -L_6)'
# R^{d2 a0 a2 d0} * R^d1_d2^{a1 a3} * R^{a4 a5}_{d0 d1}
# T_c = R^{a0 d0 a2 d1}*R^{a1 a3}_d0^d2*R^{a4 a5}_{d1 d2}
t = R(d2, a0, a2, d0)*R(d1, -d2, a1, a3)*R(a4, a5, -d0, -d1)
tc = t.canon_bp()
assert str(tc) == 'R(a0, L_0, a2, L_1)*R(a1, a3, -L_0, L_2)*R(a4, a5, -L_1, -L_2)'
######################################################################
def test_canonicalize2():
D = Symbol('D')
Eucl = TensorIndexType('Eucl', metric=0, dim=D, dummy_fmt='E')
i0,i1,i2,i3,i4,i5,i6,i7,i8,i9,i10,i11,i12,i13,i14 = \
tensor_indices('i0:15', Eucl)
A = TensorHead('A', [Eucl]*3, TensorSymmetry.fully_symmetric(-3))
# two examples from Cvitanovic, Group Theory page 59
# of identities for antisymmetric tensors of rank 3
# contracted according to the Kuratowski graph eq.(6.59)
t = A(i0,i1,i2)*A(-i1,i3,i4)*A(-i3,i7,i5)*A(-i2,-i5,i6)*A(-i4,-i6,i8)
t1 = t.canon_bp()
assert t1 == 0
# eq.(6.60)
#t = A(i0,i1,i2)*A(-i1,i3,i4)*A(-i2,i5,i6)*A(-i3,i7,i8)*A(-i6,-i7,i9)*
# A(-i8,i10,i13)*A(-i5,-i10,i11)*A(-i4,-i11,i12)*A(-i3,-i12,i14)
t = A(i0,i1,i2)*A(-i1,i3,i4)*A(-i2,i5,i6)*A(-i3,i7,i8)*A(-i6,-i7,i9)*\
A(-i8,i10,i13)*A(-i5,-i10,i11)*A(-i4,-i11,i12)*A(-i9,-i12,i14)
t1 = t.canon_bp()
assert t1 == 0
def test_canonicalize3():
D = Symbol('D')
Spinor = TensorIndexType('Spinor', dim=D, metric=True, dummy_fmt='S')
a0,a1,a2,a3,a4 = tensor_indices('a0:5', Spinor)
chi, psi = tensor_heads('chi,psi', [Spinor], TensorSymmetry.no_symmetry(1), 1)
t = chi(a1)*psi(a0)
t1 = t.canon_bp()
assert t1 == t
t = psi(a1)*chi(a0)
t1 = t.canon_bp()
assert t1 == -chi(a0)*psi(a1)
class Metric(Basic):
def __new__(cls, name, antisym, **kwargs):
obj = Basic.__new__(cls, name, antisym, **kwargs)
obj.name = name
obj.antisym = antisym
return obj
def test_TensorIndexType():
D = Symbol('D')
G = Metric('g', False)
Lorentz = TensorIndexType('Lorentz', metric=G, dim=D, dummy_fmt='L')
m0, m1, m2, m3, m4 = tensor_indices('m0:5', Lorentz)
sym2 = TensorSymmetry.fully_symmetric(2)
sym2n = TensorSymmetry(*get_symmetric_group_sgs(2))
assert sym2 == sym2n
g = Lorentz.metric
assert str(g) == 'g(Lorentz,Lorentz)'
assert Lorentz.eps_dim == Lorentz.dim
TSpace = TensorIndexType('TSpace')
i0, i1 = tensor_indices('i0 i1', TSpace)
g = TSpace.metric
A = TensorHead('A', [TSpace]*2, sym2)
assert str(A(i0,-i0).canon_bp()) == 'A(TSpace_0, -TSpace_0)'
def test_indices():
Lorentz = TensorIndexType('Lorentz', dummy_fmt='L')
a, b, c, d = tensor_indices('a,b,c,d', Lorentz)
assert a.tensor_index_type == Lorentz
assert a != -a
A, B = tensor_heads('A B', [Lorentz]*2, TensorSymmetry.fully_symmetric(2))
t = A(a,b)*B(-b,c)
indices = t.get_indices()
L_0 = TensorIndex('L_0', Lorentz)
assert indices == [a, L_0, -L_0, c]
raises(ValueError, lambda: tensor_indices(3, Lorentz))
raises(ValueError, lambda: A(a,b,c))
def test_TensorSymmetry():
assert TensorSymmetry.fully_symmetric(2) == \
TensorSymmetry(get_symmetric_group_sgs(2))
assert TensorSymmetry.fully_symmetric(-3) == \
TensorSymmetry(get_symmetric_group_sgs(3, True))
assert TensorSymmetry.direct_product(-4) == \
TensorSymmetry.fully_symmetric(-4)
assert TensorSymmetry.fully_symmetric(-1) == \
TensorSymmetry.fully_symmetric(1)
assert TensorSymmetry.direct_product(1, -1, 1) == \
TensorSymmetry.no_symmetry(3)
assert TensorSymmetry(get_symmetric_group_sgs(2)) == \
TensorSymmetry(*get_symmetric_group_sgs(2))
# TODO: add check for *get_symmetric_group_sgs(0)
sym = TensorSymmetry.fully_symmetric(-3)
assert sym.rank == 3
assert sym.base == Tuple(0, 1)
assert sym.generators == Tuple(Permutation(0, 1)(3, 4), Permutation(1, 2)(3, 4))
def test_TensExpr():
Lorentz = TensorIndexType('Lorentz', dummy_fmt='L')
a, b, c, d = tensor_indices('a,b,c,d', Lorentz)
g = Lorentz.metric
A, B = tensor_heads('A B', [Lorentz]*2, TensorSymmetry.fully_symmetric(2))
raises(ValueError, lambda: g(c, d)/g(a, b))
raises(ValueError, lambda: S.One/g(a, b))
raises(ValueError, lambda: (A(c, d) + g(c, d))/g(a, b))
raises(ValueError, lambda: S.One/(A(c, d) + g(c, d)))
raises(ValueError, lambda: A(a, b) + A(a, c))
A(a, b) + B(a, b) # assigned to t for below
#raises(NotImplementedError, lambda: TensExpr.__mul__(t, 'a'))
#raises(NotImplementedError, lambda: TensExpr.__add__(t, 'a'))
#raises(NotImplementedError, lambda: TensExpr.__radd__(t, 'a'))
#raises(NotImplementedError, lambda: TensExpr.__sub__(t, 'a'))
#raises(NotImplementedError, lambda: TensExpr.__rsub__(t, 'a'))
#raises(NotImplementedError, lambda: TensExpr.__div__(t, 'a'))
#raises(NotImplementedError, lambda: TensExpr.__rdiv__(t, 'a'))
with ignore_warnings(SymPyDeprecationWarning):
# DO NOT REMOVE THIS AFTER DEPRECATION REMOVED:
raises(ValueError, lambda: A(a, b)**2)
raises(NotImplementedError, lambda: 2**A(a, b))
raises(NotImplementedError, lambda: abs(A(a, b)))
def test_TensorHead():
# simple example of algebraic expression
Lorentz = TensorIndexType('Lorentz', dummy_fmt='L')
A = TensorHead('A', [Lorentz]*2)
assert A.name == 'A'
assert A.index_types == Tuple(Lorentz, Lorentz)
assert A.rank == 2
assert A.symmetry == TensorSymmetry.no_symmetry(2)
assert A.comm == 0
def test_add1():
assert TensAdd().args == ()
assert TensAdd().doit() == 0
# simple example of algebraic expression
Lorentz = TensorIndexType('Lorentz', dummy_fmt='L')
a,b,d0,d1,i,j,k = tensor_indices('a,b,d0,d1,i,j,k', Lorentz)
# A, B symmetric
A, B = tensor_heads('A,B', [Lorentz]*2, TensorSymmetry.fully_symmetric(2))
t1 = A(b, -d0)*B(d0, a)
assert TensAdd(t1).equals(t1)
t2a = B(d0, a) + A(d0, a)
t2 = A(b, -d0)*t2a
assert str(t2) == 'A(b, -L_0)*(A(L_0, a) + B(L_0, a))'
t2 = t2.expand()
assert str(t2) == 'A(b, -L_0)*A(L_0, a) + A(b, -L_0)*B(L_0, a)'
t2 = t2.canon_bp()
assert str(t2) == 'A(a, L_0)*A(b, -L_0) + A(b, L_0)*B(a, -L_0)'
t2b = t2 + t1
assert str(t2b) == 'A(a, L_0)*A(b, -L_0) + A(b, -L_0)*B(L_0, a) + A(b, L_0)*B(a, -L_0)'
t2b = t2b.canon_bp()
assert str(t2b) == '2*A(b, L_0)*B(a, -L_0) + A(a, L_0)*A(b, -L_0)'
p, q, r = tensor_heads('p,q,r', [Lorentz])
t = q(d0)*2
assert str(t) == '2*q(d0)'
t = 2*q(d0)
assert str(t) == '2*q(d0)'
t1 = p(d0) + 2*q(d0)
assert str(t1) == '2*q(d0) + p(d0)'
t2 = p(-d0) + 2*q(-d0)
assert str(t2) == '2*q(-d0) + p(-d0)'
t1 = p(d0)
t3 = t1*t2
assert str(t3) == 'p(L_0)*(2*q(-L_0) + p(-L_0))'
t3 = t3.expand()
assert str(t3) == '2*p(L_0)*q(-L_0) + p(L_0)*p(-L_0)'
t3 = t2*t1
t3 = t3.expand()
assert str(t3) == '2*q(-L_0)*p(L_0) + p(-L_0)*p(L_0)'
t3 = t3.canon_bp()
assert str(t3) == '2*p(L_0)*q(-L_0) + p(L_0)*p(-L_0)'
t1 = p(d0) + 2*q(d0)
t3 = t1*t2
t3 = t3.canon_bp()
assert str(t3) == '4*p(L_0)*q(-L_0) + 4*q(L_0)*q(-L_0) + p(L_0)*p(-L_0)'
t1 = p(d0) - 2*q(d0)
assert str(t1) == '-2*q(d0) + p(d0)'
t2 = p(-d0) + 2*q(-d0)
t3 = t1*t2
t3 = t3.canon_bp()
assert t3 == p(d0)*p(-d0) - 4*q(d0)*q(-d0)
t = p(i)*p(j)*(p(k) + q(k)) + p(i)*(p(j) + q(j))*(p(k) - 3*q(k))
t = t.canon_bp()
assert t == 2*p(i)*p(j)*p(k) - 2*p(i)*p(j)*q(k) + p(i)*p(k)*q(j) - 3*p(i)*q(j)*q(k)
t1 = (p(i) + q(i) + 2*r(i))*(p(j) - q(j))
t2 = (p(j) + q(j) + 2*r(j))*(p(i) - q(i))
t = t1 + t2
t = t.canon_bp()
assert t == 2*p(i)*p(j) + 2*p(i)*r(j) + 2*p(j)*r(i) - 2*q(i)*q(j) - 2*q(i)*r(j) - 2*q(j)*r(i)
t = p(i)*q(j)/2
assert 2*t == p(i)*q(j)
t = (p(i) + q(i))/2
assert 2*t == p(i) + q(i)
t = S.One - p(i)*p(-i)
t = t.canon_bp()
tz1 = t + p(-j)*p(j)
assert tz1 != 1
tz1 = tz1.canon_bp()
assert tz1.equals(1)
t = S.One + p(i)*p(-i)
assert (t - p(-j)*p(j)).canon_bp().equals(1)
t = A(a, b) + B(a, b)
assert t.rank == 2
t1 = t - A(a, b) - B(a, b)
assert t1 == 0
t = 1 - (A(a, -a) + B(a, -a))
t1 = 1 + (A(a, -a) + B(a, -a))
assert (t + t1).expand().equals(2)
t2 = 1 + A(a, -a)
assert t1 != t2
assert t2 != TensMul.from_data(0, [], [], [])
t = p(i) + q(i)
raises(ValueError, lambda: t(i, j))
def test_special_eq_ne():
# test special equality cases:
Lorentz = TensorIndexType('Lorentz', dummy_fmt='L')
a, b, d0, d1, i, j, k = tensor_indices('a,b,d0,d1,i,j,k', Lorentz)
# A, B symmetric
A, B = tensor_heads('A,B', [Lorentz]*2, TensorSymmetry.fully_symmetric(2))
p, q, r = tensor_heads('p,q,r', [Lorentz])
t = 0*A(a, b)
assert _is_equal(t, 0)
assert _is_equal(t, S.Zero)
assert p(i) != A(a, b)
assert A(a, -a) != A(a, b)
assert 0*(A(a, b) + B(a, b)) == 0
assert 0*(A(a, b) + B(a, b)) == S.Zero
assert 3*(A(a, b) - A(a, b)) == S.Zero
assert p(i) + q(i) != A(a, b)
assert p(i) + q(i) != A(a, b) + B(a, b)
assert p(i) - p(i) == 0
assert p(i) - p(i) == S.Zero
assert _is_equal(A(a, b), A(b, a))
def test_add2():
Lorentz = TensorIndexType('Lorentz', dummy_fmt='L')
m, n, p, q = tensor_indices('m,n,p,q', Lorentz)
R = TensorHead('R', [Lorentz]*4, TensorSymmetry.riemann())
A = TensorHead('A', [Lorentz]*3, TensorSymmetry.fully_symmetric(-3))
t1 = 2*R(m, n, p, q) - R(m, q, n, p) + R(m, p, n, q)
t2 = t1*A(-n, -p, -q)
t2 = t2.canon_bp()
assert t2 == 0
t1 = S(2)/3*R(m,n,p,q) - S(1)/3*R(m,q,n,p) + S(1)/3*R(m,p,n,q)
t2 = t1*A(-n, -p, -q)
t2 = t2.canon_bp()
assert t2 == 0
t = A(m, -m, n) + A(n, p, -p)
t = t.canon_bp()
assert t == 0
def test_add3():
Lorentz = TensorIndexType('Lorentz', dummy_fmt='L')
i0, i1 = tensor_indices('i0:2', Lorentz)
E, px, py, pz = symbols('E px py pz')
A = TensorHead('A', [Lorentz])
B = TensorHead('B', [Lorentz])
expr1 = A(i0)*A(-i0) - (E**2 - px**2 - py**2 - pz**2)
assert expr1.args == (px**2, py**2, pz**2, -E**2, A(i0)*A(-i0))
expr2 = E**2 - px**2 - py**2 - pz**2 - A(i0)*A(-i0)
assert expr2.args == (E**2, -px**2, -py**2, -pz**2, -A(i0)*A(-i0))
expr3 = A(i0)*A(-i0) - E**2 + px**2 + py**2 + pz**2
assert expr3.args == (px**2, py**2, pz**2, -E**2, A(i0)*A(-i0))
expr4 = B(i1)*B(-i1) + 2*E**2 - 2*px**2 - 2*py**2 - 2*pz**2 - A(i0)*A(-i0)
assert expr4.args == (-2*px**2, -2*py**2, -2*pz**2, 2*E**2, -A(i0)*A(-i0), B(i1)*B(-i1))
def test_mul():
from sympy.abc import x
Lorentz = TensorIndexType('Lorentz', dummy_fmt='L')
a, b, c, d = tensor_indices('a,b,c,d', Lorentz)
t = TensMul.from_data(S.One, [], [], [])
assert str(t) == '1'
A, B = tensor_heads('A B', [Lorentz]*2, TensorSymmetry.fully_symmetric(2))
t = (1 + x)*A(a, b)
assert str(t) == '(x + 1)*A(a, b)'
assert t.index_types == [Lorentz, Lorentz]
assert t.rank == 2
assert t.dum == []
assert t.coeff == 1 + x
assert sorted(t.free) == [(a, 0), (b, 1)]
assert t.components == [A]
ts = A(a, b)
assert str(ts) == 'A(a, b)'
assert ts.index_types == [Lorentz, Lorentz]
assert ts.rank == 2
assert ts.dum == []
assert ts.coeff == 1
assert sorted(ts.free) == [(a, 0), (b, 1)]
assert ts.components == [A]
t = A(-b, a)*B(-a, c)*A(-c, d)
t1 = tensor_mul(*t.split())
assert t == t(-b, d)
assert t == t1
assert tensor_mul(*[]) == TensMul.from_data(S.One, [], [], [])
t = TensMul.from_data(1, [], [], [])
C = TensorHead('C', [])
assert str(C()) == 'C'
assert str(t) == '1'
assert t == 1
raises(ValueError, lambda: A(a, b)*A(a, c))
t = A(a, b)*A(-a, c)
raises(ValueError, lambda: t(a, b, c))
def test_substitute_indices():
Lorentz = TensorIndexType('Lorentz', dummy_fmt='L')
i, j, k, l, m, n, p, q = tensor_indices('i,j,k,l,m,n,p,q', Lorentz)
A, B = tensor_heads('A,B', [Lorentz]*2, TensorSymmetry.fully_symmetric(2))
t = A(i, k)*B(-k, -j)
t1 = t.substitute_indices((i, j), (j, k))
t1a = A(j, l)*B(-l, -k)
assert t1 == t1a
p = TensorHead('p', [Lorentz])
t = p(i)
t1 = t.substitute_indices((j, k))
assert t1 == t
t1 = t.substitute_indices((i, j))
assert t1 == p(j)
t1 = t.substitute_indices((i, -j))
assert t1 == p(-j)
t1 = t.substitute_indices((-i, j))
assert t1 == p(-j)
t1 = t.substitute_indices((-i, -j))
assert t1 == p(j)
A_tmul = A(m, n)
A_c = A_tmul(m, -m)
assert _is_equal(A_c, A(n, -n))
ABm = A(i, j)*B(m, n)
ABc1 = ABm(i, j, -i, -j)
assert _is_equal(ABc1, A(i, -j)*B(-i, j))
ABc2 = ABm(i, -i, j, -j)
assert _is_equal(ABc2, A(m, -m)*B(-n, n))
asum = A(i, j) + B(i, j)
asc1 = asum(i, -i)
assert _is_equal(asc1, A(i, -i) + B(i, -i))
assert A(i, -i) == A(i, -i)()
assert canon_bp(A(i, -i) + B(-j, j) - (A(i, -i) + B(i, -i))()) == 0
assert _is_equal(A(i, j)*B(-j, k), (A(m, -j)*B(j, n))(i, k))
raises(ValueError, lambda: A(i, -i)(j, k))
def test_riemann_cyclic_replace():
Lorentz = TensorIndexType('Lorentz', dummy_fmt='L')
m0, m1, m2, m3 = tensor_indices('m:4', Lorentz)
R = TensorHead('R', [Lorentz]*4, TensorSymmetry.riemann())
t = R(m0, m2, m1, m3)
t1 = riemann_cyclic_replace(t)
t1a = -S.One/3*R(m0, m3, m2, m1) + S.One/3*R(m0, m1, m2, m3) + Rational(2, 3)*R(m0, m2, m1, m3)
assert t1 == t1a
def test_riemann_cyclic():
Lorentz = TensorIndexType('Lorentz', dummy_fmt='L')
i, j, k, l, m, n, p, q = tensor_indices('i,j,k,l,m,n,p,q', Lorentz)
R = TensorHead('R', [Lorentz]*4, TensorSymmetry.riemann())
t = R(i,j,k,l) + R(i,l,j,k) + R(i,k,l,j) - \
R(i,j,l,k) - R(i,l,k,j) - R(i,k,j,l)
t2 = t*R(-i,-j,-k,-l)
t3 = riemann_cyclic(t2)
assert t3 == 0
t = R(i,j,k,l)*(R(-i,-j,-k,-l) - 2*R(-i,-k,-j,-l))
t1 = riemann_cyclic(t)
assert t1 == 0
t = R(i,j,k,l)
t1 = riemann_cyclic(t)
assert t1 == -S(1)/3*R(i, l, j, k) + S(1)/3*R(i, k, j, l) + S(2)/3*R(i, j, k, l)
t = R(i,j,k,l)*R(-k,-l,m,n)*(R(-m,-n,-i,-j) + 2*R(-m,-j,-n,-i))
t1 = riemann_cyclic(t)
assert t1 == 0
@XFAIL
def test_div():
Lorentz = TensorIndexType('Lorentz', dummy_fmt='L')
m0, m1, m2, m3 = tensor_indices('m0:4', Lorentz)
R = TensorHead('R', [Lorentz]*4, TensorSymmetry.riemann())
t = R(m0,m1,-m1,m3)
t1 = t/S(4)
assert str(t1) == '(1/4)*R(m0, L_0, -L_0, m3)'
t = t.canon_bp()
assert not t1._is_canon_bp
t1 = t*4
assert t1._is_canon_bp
t1 = t1/4
assert t1._is_canon_bp
def test_contract_metric1():
D = Symbol('D')
Lorentz = TensorIndexType('Lorentz', dim=D, dummy_fmt='L')
a, b, c, d, e = tensor_indices('a,b,c,d,e', Lorentz)
g = Lorentz.metric
p = TensorHead('p', [Lorentz])
t = g(a, b)*p(-b)
t1 = t.contract_metric(g)
assert t1 == p(a)
A, B = tensor_heads('A,B', [Lorentz]*2, TensorSymmetry.fully_symmetric(2))
# case with g with all free indices
t1 = A(a,b)*B(-b,c)*g(d, e)
t2 = t1.contract_metric(g)
assert t1 == t2
# case of g(d, -d)
t1 = A(a,b)*B(-b,c)*g(-d, d)
t2 = t1.contract_metric(g)
assert t2 == D*A(a, d)*B(-d, c)
# g with one free index
t1 = A(a,b)*B(-b,-c)*g(c, d)
t2 = t1.contract_metric(g)
assert t2 == A(a, c)*B(-c, d)
# g with both indices contracted with another tensor
t1 = A(a,b)*B(-b,-c)*g(c, -a)
t2 = t1.contract_metric(g)
assert _is_equal(t2, A(a, b)*B(-b, -a))
t1 = A(a,b)*B(-b,-c)*g(c, d)*g(-a, -d)
t2 = t1.contract_metric(g)
assert _is_equal(t2, A(a,b)*B(-b,-a))
t1 = A(a,b)*g(-a,-b)
t2 = t1.contract_metric(g)
assert _is_equal(t2, A(a, -a))
assert not t2.free
Lorentz = TensorIndexType('Lorentz', dummy_fmt='L')
a, b = tensor_indices('a,b', Lorentz)
g = Lorentz.metric
raises(ValueError, lambda: g(a, -a).contract_metric(g)) # no dim
def test_contract_metric2():
D = Symbol('D')
Lorentz = TensorIndexType('Lorentz', dim=D, dummy_fmt='L')
a, b, c, d, e, L_0 = tensor_indices('a,b,c,d,e,L_0', Lorentz)
g = Lorentz.metric
p, q = tensor_heads('p,q', [Lorentz])
t1 = g(a,b)*p(c)*p(-c)
t2 = 3*g(-a,-b)*q(c)*q(-c)
t = t1*t2
t = t.contract_metric(g)
assert t == 3*D*p(a)*p(-a)*q(b)*q(-b)
t1 = g(a,b)*p(c)*p(-c)
t2 = 3*q(-a)*q(-b)
t = t1*t2
t = t.contract_metric(g)
t = t.canon_bp()
assert t == 3*p(a)*p(-a)*q(b)*q(-b)
t1 = 2*g(a,b)*p(c)*p(-c)
t2 = - 3*g(-a,-b)*q(c)*q(-c)
t = t1*t2
t = t.contract_metric(g)
t = 6*g(a,b)*g(-a,-b)*p(c)*p(-c)*q(d)*q(-d)
t = t.contract_metric(g)
t1 = 2*g(a,b)*p(c)*p(-c)
t2 = q(-a)*q(-b) + 3*g(-a,-b)*q(c)*q(-c)
t = t1*t2
t = t.contract_metric(g)
assert t == (2 + 6*D)*p(a)*p(-a)*q(b)*q(-b)
t1 = p(a)*p(b) + p(a)*q(b) + 2*g(a,b)*p(c)*p(-c)
t2 = q(-a)*q(-b) - g(-a,-b)*q(c)*q(-c)
t = t1*t2
t = t.contract_metric(g)
t1 = (1 - 2*D)*p(a)*p(-a)*q(b)*q(-b) + p(a)*q(-a)*p(b)*q(-b)
assert canon_bp(t - t1) == 0
t = g(a,b)*g(c,d)*g(-b,-c)
t1 = t.contract_metric(g)
assert t1 == g(a, d)
t1 = g(a,b)*g(c,d) + g(a,c)*g(b,d) + g(a,d)*g(b,c)
t2 = t1.substitute_indices((a,-a),(b,-b),(c,-c),(d,-d))
t = t1*t2
t = t.contract_metric(g)
assert t.equals(3*D**2 + 6*D)
t = 2*p(a)*g(b,-b)
t1 = t.contract_metric(g)
assert t1.equals(2*D*p(a))
t = 2*p(a)*g(b,-a)
t1 = t.contract_metric(g)
assert t1 == 2*p(b)
M = Symbol('M')
t = (p(a)*p(b) + g(a, b)*M**2)*g(-a, -b) - D*M**2
t1 = t.contract_metric(g)
assert t1 == p(a)*p(-a)
A = TensorHead('A', [Lorentz]*2, TensorSymmetry.fully_symmetric(2))
t = A(a, b)*p(L_0)*g(-a, -b)
t1 = t.contract_metric(g)
assert str(t1) == 'A(L_1, -L_1)*p(L_0)' or str(t1) == 'A(-L_1, L_1)*p(L_0)'
def test_metric_contract3():
D = Symbol('D')
Spinor = TensorIndexType('Spinor', dim=D, metric=True, dummy_fmt='S')
a0, a1, a2, a3, a4 = tensor_indices('a0:5', Spinor)
C = Spinor.metric
chi, psi = tensor_heads('chi,psi', [Spinor], TensorSymmetry.no_symmetry(1), 1)
B = TensorHead('B', [Spinor]*2, TensorSymmetry.no_symmetry(2))
t = C(a0,-a0)
t1 = t.contract_metric(C)
assert t1.equals(-D)
t = C(-a0,a0)
t1 = t.contract_metric(C)
assert t1.equals(D)
t = C(a0,a1)*C(-a0,-a1)
t1 = t.contract_metric(C)
assert t1.equals(D)
t = C(a1,a0)*C(-a0,-a1)
t1 = t.contract_metric(C)
assert t1.equals(-D)
t = C(-a0,a1)*C(a0,-a1)
t1 = t.contract_metric(C)
assert t1.equals(-D)
t = C(a1,-a0)*C(a0,-a1)
t1 = t.contract_metric(C)
assert t1.equals(D)
t = C(a0,a1)*B(-a1,-a0)
t1 = t.contract_metric(C)
t1 = t1.canon_bp()
assert _is_equal(t1, B(a0,-a0))
t = C(a1,a0)*B(-a1,-a0)
t1 = t.contract_metric(C)
assert _is_equal(t1, -B(a0,-a0))
t = C(a0,-a1)*B(a1,-a0)
t1 = t.contract_metric(C)
assert _is_equal(t1, -B(a0,-a0))
t = C(-a0,a1)*B(-a1,a0)
t1 = t.contract_metric(C)
assert _is_equal(t1, -B(a0,-a0))
t = C(-a0,-a1)*B(a1,a0)
t1 = t.contract_metric(C)
assert _is_equal(t1, B(a0,-a0))
t = C(-a1, a0)*B(a1,-a0)
t1 = t.contract_metric(C)
assert _is_equal(t1, B(a0,-a0))
t = C(a0,a1)*psi(-a1)
t1 = t.contract_metric(C)
assert _is_equal(t1, psi(a0))
t = C(a1,a0)*psi(-a1)
t1 = t.contract_metric(C)
assert _is_equal(t1, -psi(a0))
t = C(a0,a1)*chi(-a0)*psi(-a1)
t1 = t.contract_metric(C)
assert _is_equal(t1, -chi(a1)*psi(-a1))
t = C(a1,a0)*chi(-a0)*psi(-a1)
t1 = t.contract_metric(C)
assert _is_equal(t1, chi(a1)*psi(-a1))
t = C(-a1,a0)*chi(-a0)*psi(a1)
t1 = t.contract_metric(C)
assert _is_equal(t1, chi(-a1)*psi(a1))
t = C(a0,-a1)*chi(-a0)*psi(a1)
t1 = t.contract_metric(C)
assert _is_equal(t1, -chi(-a1)*psi(a1))
t = C(-a0,-a1)*chi(a0)*psi(a1)
t1 = t.contract_metric(C)
assert _is_equal(t1, chi(-a1)*psi(a1))
t = C(-a1,-a0)*chi(a0)*psi(a1)
t1 = t.contract_metric(C)
assert _is_equal(t1, -chi(-a1)*psi(a1))
t = C(-a1,-a0)*B(a0,a2)*psi(a1)
t1 = t.contract_metric(C)
assert _is_equal(t1, -B(-a1,a2)*psi(a1))
t = C(a1,a0)*B(-a2,-a0)*psi(-a1)
t1 = t.contract_metric(C)
assert _is_equal(t1, B(-a2,a1)*psi(-a1))
def test_epsilon():
Lorentz = TensorIndexType('Lorentz', dim=4, dummy_fmt='L')
a, b, c, d, e = tensor_indices('a,b,c,d,e', Lorentz)
epsilon = Lorentz.epsilon
p, q, r, s = tensor_heads('p,q,r,s', [Lorentz])
t = epsilon(b,a,c,d)
t1 = t.canon_bp()
assert t1 == -epsilon(a,b,c,d)
t = epsilon(c,b,d,a)
t1 = t.canon_bp()
assert t1 == epsilon(a,b,c,d)
t = epsilon(c,a,d,b)
t1 = t.canon_bp()
assert t1 == -epsilon(a,b,c,d)
t = epsilon(a,b,c,d)*p(-a)*q(-b)
t1 = t.canon_bp()
assert t1 == epsilon(c,d,a,b)*p(-a)*q(-b)
t = epsilon(c,b,d,a)*p(-a)*q(-b)
t1 = t.canon_bp()
assert t1 == epsilon(c,d,a,b)*p(-a)*q(-b)
t = epsilon(c,a,d,b)*p(-a)*q(-b)
t1 = t.canon_bp()
assert t1 == -epsilon(c,d,a,b)*p(-a)*q(-b)
t = epsilon(c,a,d,b)*p(-a)*p(-b)
t1 = t.canon_bp()
assert t1 == 0
t = epsilon(c,a,d,b)*p(-a)*q(-b) + epsilon(a,b,c,d)*p(-b)*q(-a)
t1 = t.canon_bp()
assert t1 == -2*epsilon(c,d,a,b)*p(-a)*q(-b)
# Test that epsilon can be create with a SymPy integer:
Lorentz = TensorIndexType('Lorentz', dim=Integer(4), dummy_fmt='L')
epsilon = Lorentz.epsilon
assert isinstance(epsilon, TensorHead)
def test_contract_delta1():
# see Group Theory by Cvitanovic page 9
n = Symbol('n')
Color = TensorIndexType('Color', metric=None, dim=n, dummy_fmt='C')
a, b, c, d, e, f = tensor_indices('a,b,c,d,e,f', Color)
delta = Color.delta
def idn(a, b, d, c):
assert a.is_up and d.is_up
assert not (b.is_up or c.is_up)
return delta(a,c)*delta(d,b)
def T(a, b, d, c):
assert a.is_up and d.is_up
assert not (b.is_up or c.is_up)
return delta(a,b)*delta(d,c)
def P1(a, b, c, d):
return idn(a,b,c,d) - 1/n*T(a,b,c,d)
def P2(a, b, c, d):
return 1/n*T(a,b,c,d)
t = P1(a, -b, e, -f)*P1(f, -e, d, -c)
t1 = t.contract_delta(delta)
assert canon_bp(t1 - P1(a, -b, d, -c)) == 0
t = P2(a, -b, e, -f)*P2(f, -e, d, -c)
t1 = t.contract_delta(delta)
assert t1 == P2(a, -b, d, -c)
t = P1(a, -b, e, -f)*P2(f, -e, d, -c)
t1 = t.contract_delta(delta)
assert t1 == 0
t = P1(a, -b, b, -a)
t1 = t.contract_delta(delta)
assert t1.equals(n**2 - 1)
def test_fun():
D = Symbol('D')
Lorentz = TensorIndexType('Lorentz', dim=D, dummy_fmt='L')
a, b, c, d, e = tensor_indices('a,b,c,d,e', Lorentz)
g = Lorentz.metric
p, q = tensor_heads('p q', [Lorentz])
t = q(c)*p(a)*q(b) + g(a,b)*g(c,d)*q(-d)
assert t(a,b,c) == t
assert canon_bp(t - t(b,a,c) - q(c)*p(a)*q(b) + q(c)*p(b)*q(a)) == 0
assert t(b,c,d) == q(d)*p(b)*q(c) + g(b,c)*g(d,e)*q(-e)
t1 = t.fun_eval((a,b),(b,a))
assert canon_bp(t1 - q(c)*p(b)*q(a) - g(a,b)*g(c,d)*q(-d)) == 0
# check that g_{a b; c} = 0
# example taken from L. Brewin
# "A brief introduction to Cadabra" arxiv:0903.2085
# dg_{a b c} = \partial_{a} g_{b c} is symmetric in b, c
dg = TensorHead('dg', [Lorentz]*3, TensorSymmetry.direct_product(1, 2))
# gamma^a_{b c} is the Christoffel symbol
gamma = S.Half*g(a,d)*(dg(-b,-d,-c) + dg(-c,-b,-d) - dg(-d,-b,-c))
# t = g_{a b; c}
t = dg(-c,-a,-b) - g(-a,-d)*gamma(d,-b,-c) - g(-b,-d)*gamma(d,-a,-c)
t = t.contract_metric(g)
assert t == 0
t = q(c)*p(a)*q(b)
assert t(b,c,d) == q(d)*p(b)*q(c)
def test_TensorManager():
Lorentz = TensorIndexType('Lorentz', dummy_fmt='L')
LorentzH = TensorIndexType('LorentzH', dummy_fmt='LH')
i, j = tensor_indices('i,j', Lorentz)
ih, jh = tensor_indices('ih,jh', LorentzH)
p, q = tensor_heads('p q', [Lorentz])
ph, qh = tensor_heads('ph qh', [LorentzH])
Gsymbol = Symbol('Gsymbol')
GHsymbol = Symbol('GHsymbol')
TensorManager.set_comm(Gsymbol, GHsymbol, 0)
G = TensorHead('G', [Lorentz], TensorSymmetry.no_symmetry(1), Gsymbol)
assert TensorManager._comm_i2symbol[G.comm] == Gsymbol
GH = TensorHead('GH', [LorentzH], TensorSymmetry.no_symmetry(1), GHsymbol)
ps = G(i)*p(-i)
psh = GH(ih)*ph(-ih)
t = ps + psh
t1 = t*t
assert canon_bp(t1 - ps*ps - 2*ps*psh - psh*psh) == 0
qs = G(i)*q(-i)
qsh = GH(ih)*qh(-ih)
assert _is_equal(ps*qsh, qsh*ps)
assert not _is_equal(ps*qs, qs*ps)
n = TensorManager.comm_symbols2i(Gsymbol)
assert TensorManager.comm_i2symbol(n) == Gsymbol
assert GHsymbol in TensorManager._comm_symbols2i
raises(ValueError, lambda: TensorManager.set_comm(GHsymbol, 1, 2))
TensorManager.set_comms((Gsymbol,GHsymbol,0),(Gsymbol,1,1))
assert TensorManager.get_comm(n, 1) == TensorManager.get_comm(1, n) == 1
TensorManager.clear()
assert TensorManager.comm == [{0:0, 1:0, 2:0}, {0:0, 1:1, 2:None}, {0:0, 1:None}]
assert GHsymbol not in TensorManager._comm_symbols2i
nh = TensorManager.comm_symbols2i(GHsymbol)
assert TensorManager.comm_i2symbol(nh) == GHsymbol
assert GHsymbol in TensorManager._comm_symbols2i
def test_hash():
D = Symbol('D')
Lorentz = TensorIndexType('Lorentz', dim=D, dummy_fmt='L')
a, b, c, d, e = tensor_indices('a,b,c,d,e', Lorentz)
g = Lorentz.metric
p, q = tensor_heads('p q', [Lorentz])
p_type = p.args[1]
t1 = p(a)*q(b)
t2 = p(a)*p(b)
assert hash(t1) != hash(t2)
t3 = p(a)*p(b) + g(a,b)
t4 = p(a)*p(b) - g(a,b)
assert hash(t3) != hash(t4)
assert a.func(*a.args) == a
assert Lorentz.func(*Lorentz.args) == Lorentz
assert g.func(*g.args) == g
assert p.func(*p.args) == p
assert p_type.func(*p_type.args) == p_type
assert p(a).func(*(p(a)).args) == p(a)
assert t1.func(*t1.args) == t1
assert t2.func(*t2.args) == t2
assert t3.func(*t3.args) == t3
assert t4.func(*t4.args) == t4
assert hash(a.func(*a.args)) == hash(a)
assert hash(Lorentz.func(*Lorentz.args)) == hash(Lorentz)
assert hash(g.func(*g.args)) == hash(g)
assert hash(p.func(*p.args)) == hash(p)
assert hash(p_type.func(*p_type.args)) == hash(p_type)
assert hash(p(a).func(*(p(a)).args)) == hash(p(a))
assert hash(t1.func(*t1.args)) == hash(t1)
assert hash(t2.func(*t2.args)) == hash(t2)
assert hash(t3.func(*t3.args)) == hash(t3)
assert hash(t4.func(*t4.args)) == hash(t4)
def check_all(obj):
return all([isinstance(_, Basic) for _ in obj.args])
assert check_all(a)
assert check_all(Lorentz)
assert check_all(g)
assert check_all(p)
assert check_all(p_type)
assert check_all(p(a))
assert check_all(t1)
assert check_all(t2)
assert check_all(t3)
assert check_all(t4)
tsymmetry = TensorSymmetry.direct_product(-2, 1, 3)
assert tsymmetry.func(*tsymmetry.args) == tsymmetry
assert hash(tsymmetry.func(*tsymmetry.args)) == hash(tsymmetry)
assert check_all(tsymmetry)
### TEST VALUED TENSORS ###
def _get_valued_base_test_variables():
minkowski = Matrix((
(1, 0, 0, 0),
(0, -1, 0, 0),
(0, 0, -1, 0),
(0, 0, 0, -1),
))
Lorentz = TensorIndexType('Lorentz', dim=4)
Lorentz.data = minkowski
i0, i1, i2, i3, i4 = tensor_indices('i0:5', Lorentz)
E, px, py, pz = symbols('E px py pz')
A = TensorHead('A', [Lorentz])
A.data = [E, px, py, pz]
B = TensorHead('B', [Lorentz], TensorSymmetry.no_symmetry(1), 'Gcomm')
B.data = range(4)
AB = TensorHead("AB", [Lorentz]*2)
AB.data = minkowski
ba_matrix = Matrix((
(1, 2, 3, 4),
(5, 6, 7, 8),
(9, 0, -1, -2),
(-3, -4, -5, -6),
))
BA = TensorHead("BA", [Lorentz]*2)
BA.data = ba_matrix
# Let's test the diagonal metric, with inverted Minkowski metric:
LorentzD = TensorIndexType('LorentzD')
LorentzD.data = [-1, 1, 1, 1]
mu0, mu1, mu2 = tensor_indices('mu0:3', LorentzD)
C = TensorHead('C', [LorentzD])
C.data = [E, px, py, pz]
### non-diagonal metric ###
ndm_matrix = (
(1, 1, 0,),
(1, 0, 1),
(0, 1, 0,),
)
ndm = TensorIndexType("ndm")
ndm.data = ndm_matrix
n0, n1, n2 = tensor_indices('n0:3', ndm)
NA = TensorHead('NA', [ndm])
NA.data = range(10, 13)
NB = TensorHead('NB', [ndm]*2)
NB.data = [[i+j for j in range(10, 13)] for i in range(10, 13)]
NC = TensorHead('NC', [ndm]*3)
NC.data = [[[i+j+k for k in range(4, 7)] for j in range(1, 4)] for i in range(2, 5)]
return (A, B, AB, BA, C, Lorentz, E, px, py, pz, LorentzD, mu0, mu1, mu2, ndm, n0, n1,
n2, NA, NB, NC, minkowski, ba_matrix, ndm_matrix, i0, i1, i2, i3, i4)
@filter_warnings_decorator
def test_valued_tensor_iter():
(A, B, AB, BA, C, Lorentz, E, px, py, pz, LorentzD, mu0, mu1, mu2, ndm, n0, n1,
n2, NA, NB, NC, minkowski, ba_matrix, ndm_matrix, i0, i1, i2, i3, i4) = _get_valued_base_test_variables()
list_BA = [Array([1, 2, 3, 4]), Array([5, 6, 7, 8]), Array([9, 0, -1, -2]), Array([-3, -4, -5, -6])]
# iteration on VTensorHead
assert list(A) == [E, px, py, pz]
assert list(ba_matrix) == [1, 2, 3, 4, 5, 6, 7, 8, 9, 0, -1, -2, -3, -4, -5, -6]
assert list(BA) == list_BA
# iteration on VTensMul
assert list(A(i1)) == [E, px, py, pz]
assert list(BA(i1, i2)) == list_BA
assert list(3 * BA(i1, i2)) == [3 * i for i in list_BA]
assert list(-5 * BA(i1, i2)) == [-5 * i for i in list_BA]
# iteration on VTensAdd
# A(i1) + A(i1)
assert list(A(i1) + A(i1)) == [2*E, 2*px, 2*py, 2*pz]
assert BA(i1, i2) - BA(i1, i2) == 0
assert list(BA(i1, i2) - 2 * BA(i1, i2)) == [-i for i in list_BA]
@filter_warnings_decorator
def test_valued_tensor_covariant_contravariant_elements():
(A, B, AB, BA, C, Lorentz, E, px, py, pz, LorentzD, mu0, mu1, mu2, ndm, n0, n1,
n2, NA, NB, NC, minkowski, ba_matrix, ndm_matrix, i0, i1, i2, i3, i4) = _get_valued_base_test_variables()
assert A(-i0)[0] == A(i0)[0]
assert A(-i0)[1] == -A(i0)[1]
assert AB(i0, i1)[1, 1] == -1
assert AB(i0, -i1)[1, 1] == 1
assert AB(-i0, -i1)[1, 1] == -1
assert AB(-i0, i1)[1, 1] == 1
@filter_warnings_decorator
def test_valued_tensor_get_matrix():
(A, B, AB, BA, C, Lorentz, E, px, py, pz, LorentzD, mu0, mu1, mu2, ndm, n0, n1,
n2, NA, NB, NC, minkowski, ba_matrix, ndm_matrix, i0, i1, i2, i3, i4) = _get_valued_base_test_variables()
matab = AB(i0, i1).get_matrix()
assert matab == Matrix([
[1, 0, 0, 0],
[0, -1, 0, 0],
[0, 0, -1, 0],
[0, 0, 0, -1],
])
# when alternating contravariant/covariant with [1, -1, -1, -1] metric
# it becomes the identity matrix:
assert AB(i0, -i1).get_matrix() == eye(4)
# covariant and contravariant forms:
assert A(i0).get_matrix() == Matrix([E, px, py, pz])
assert A(-i0).get_matrix() == Matrix([E, -px, -py, -pz])
@filter_warnings_decorator
def test_valued_tensor_contraction():
(A, B, AB, BA, C, Lorentz, E, px, py, pz, LorentzD, mu0, mu1, mu2, ndm, n0, n1,
n2, NA, NB, NC, minkowski, ba_matrix, ndm_matrix, i0, i1, i2, i3, i4) = _get_valued_base_test_variables()
assert (A(i0) * A(-i0)).data == E ** 2 - px ** 2 - py ** 2 - pz ** 2
assert (A(i0) * A(-i0)).data == A ** 2
assert (A(i0) * A(-i0)).data == A(i0) ** 2
assert (A(i0) * B(-i0)).data == -px - 2 * py - 3 * pz
for i in range(4):
for j in range(4):
assert (A(i0) * B(-i1))[i, j] == [E, px, py, pz][i] * [0, -1, -2, -3][j]
# test contraction on the alternative Minkowski metric: [-1, 1, 1, 1]
assert (C(mu0) * C(-mu0)).data == -E ** 2 + px ** 2 + py ** 2 + pz ** 2
contrexp = A(i0) * AB(i1, -i0)
assert A(i0).rank == 1
assert AB(i1, -i0).rank == 2
assert contrexp.rank == 1
for i in range(4):
assert contrexp[i] == [E, px, py, pz][i]
@filter_warnings_decorator
def test_valued_tensor_self_contraction():
(A, B, AB, BA, C, Lorentz, E, px, py, pz, LorentzD, mu0, mu1, mu2, ndm, n0, n1,
n2, NA, NB, NC, minkowski, ba_matrix, ndm_matrix, i0, i1, i2, i3, i4) = _get_valued_base_test_variables()
assert AB(i0, -i0).data == 4
assert BA(i0, -i0).data == 2
@filter_warnings_decorator
def test_valued_tensor_pow():
(A, B, AB, BA, C, Lorentz, E, px, py, pz, LorentzD, mu0, mu1, mu2, ndm, n0, n1,
n2, NA, NB, NC, minkowski, ba_matrix, ndm_matrix, i0, i1, i2, i3, i4) = _get_valued_base_test_variables()
assert C**2 == -E**2 + px**2 + py**2 + pz**2
assert C**1 == sqrt(-E**2 + px**2 + py**2 + pz**2)
assert C(mu0)**2 == C**2
assert C(mu0)**1 == C**1
@filter_warnings_decorator
def test_valued_tensor_expressions():
(A, B, AB, BA, C, Lorentz, E, px, py, pz, LorentzD, mu0, mu1, mu2, ndm, n0, n1,
n2, NA, NB, NC, minkowski, ba_matrix, ndm_matrix, i0, i1, i2, i3, i4) = _get_valued_base_test_variables()
x1, x2, x3 = symbols('x1:4')
# test coefficient in contraction:
rank2coeff = x1 * A(i3) * B(i2)
assert rank2coeff[1, 1] == x1 * px
assert rank2coeff[3, 3] == 3 * pz * x1
coeff_expr = ((x1 * A(i4)) * (B(-i4) / x2)).data
assert coeff_expr.expand() == -px*x1/x2 - 2*py*x1/x2 - 3*pz*x1/x2
add_expr = A(i0) + B(i0)
assert add_expr[0] == E
assert add_expr[1] == px + 1
assert add_expr[2] == py + 2
assert add_expr[3] == pz + 3
sub_expr = A(i0) - B(i0)
assert sub_expr[0] == E
assert sub_expr[1] == px - 1
assert sub_expr[2] == py - 2
assert sub_expr[3] == pz - 3
assert (add_expr * B(-i0)).data == -px - 2*py - 3*pz - 14
expr1 = x1*A(i0) + x2*B(i0)
expr2 = expr1 * B(i1) * (-4)
expr3 = expr2 + 3*x3*AB(i0, i1)
expr4 = expr3 / 2
assert expr4 * 2 == expr3
expr5 = (expr4 * BA(-i1, -i0))
assert expr5.data.expand() == 28*E*x1 + 12*px*x1 + 20*py*x1 + 28*pz*x1 + 136*x2 + 3*x3
@filter_warnings_decorator
def test_valued_tensor_add_scalar():
(A, B, AB, BA, C, Lorentz, E, px, py, pz, LorentzD, mu0, mu1, mu2, ndm, n0, n1,
n2, NA, NB, NC, minkowski, ba_matrix, ndm_matrix, i0, i1, i2, i3, i4) = _get_valued_base_test_variables()
# one scalar summand after the contracted tensor
expr1 = A(i0)*A(-i0) - (E**2 - px**2 - py**2 - pz**2)
assert expr1.data == 0
# multiple scalar summands in front of the contracted tensor
expr2 = E**2 - px**2 - py**2 - pz**2 - A(i0)*A(-i0)
assert expr2.data == 0
# multiple scalar summands after the contracted tensor
expr3 = A(i0)*A(-i0) - E**2 + px**2 + py**2 + pz**2
assert expr3.data == 0
# multiple scalar summands and multiple tensors
expr4 = C(mu0)*C(-mu0) + 2*E**2 - 2*px**2 - 2*py**2 - 2*pz**2 - A(i0)*A(-i0)
assert expr4.data == 0
@filter_warnings_decorator
def test_noncommuting_components():
(A, B, AB, BA, C, Lorentz, E, px, py, pz, LorentzD, mu0, mu1, mu2, ndm, n0, n1,
n2, NA, NB, NC, minkowski, ba_matrix, ndm_matrix, i0, i1, i2, i3, i4) = _get_valued_base_test_variables()
euclid = TensorIndexType('Euclidean')
euclid.data = [1, 1]
i1, i2, i3 = tensor_indices('i1:4', euclid)
a, b, c, d = symbols('a b c d', commutative=False)
V1 = TensorHead('V1', [euclid]*2)
V1.data = [[a, b], (c, d)]
V2 = TensorHead('V2', [euclid]*2)
V2.data = [[a, c], [b, d]]
vtp = V1(i1, i2) * V2(-i2, -i1)
assert vtp.data == a**2 + b**2 + c**2 + d**2
assert vtp.data != a**2 + 2*b*c + d**2
vtp2 = V1(i1, i2)*V1(-i2, -i1)
assert vtp2.data == a**2 + b*c + c*b + d**2
assert vtp2.data != a**2 + 2*b*c + d**2
Vc = (b * V1(i1, -i1)).data
assert Vc.expand() == b * a + b * d
@filter_warnings_decorator
def test_valued_non_diagonal_metric():
(A, B, AB, BA, C, Lorentz, E, px, py, pz, LorentzD, mu0, mu1, mu2, ndm, n0, n1,
n2, NA, NB, NC, minkowski, ba_matrix, ndm_matrix, i0, i1, i2, i3, i4) = _get_valued_base_test_variables()
mmatrix = Matrix(ndm_matrix)
assert (NA(n0)*NA(-n0)).data == (NA(n0).get_matrix().T * mmatrix * NA(n0).get_matrix())[0, 0]
@filter_warnings_decorator
def test_valued_assign_numpy_ndarray():
(A, B, AB, BA, C, Lorentz, E, px, py, pz, LorentzD, mu0, mu1, mu2, ndm, n0, n1,
n2, NA, NB, NC, minkowski, ba_matrix, ndm_matrix, i0, i1, i2, i3, i4) = _get_valued_base_test_variables()
# this is needed to make sure that a numpy.ndarray can be assigned to a
# tensor.
arr = [E+1, px-1, py, pz]
A.data = Array(arr)
for i in range(4):
assert A(i0).data[i] == arr[i]
qx, qy, qz = symbols('qx qy qz')
A(-i0).data = Array([E, qx, qy, qz])
for i in range(4):
assert A(i0).data[i] == [E, -qx, -qy, -qz][i]
assert A.data[i] == [E, -qx, -qy, -qz][i]
# test on multi-indexed tensors.
random_4x4_data = [[(i**3-3*i**2)%(j+7) for i in range(4)] for j in range(4)]
AB(-i0, -i1).data = random_4x4_data
for i in range(4):
for j in range(4):
assert AB(i0, i1).data[i, j] == random_4x4_data[i][j]*(-1 if i else 1)*(-1 if j else 1)
assert AB(-i0, i1).data[i, j] == random_4x4_data[i][j]*(-1 if j else 1)
assert AB(i0, -i1).data[i, j] == random_4x4_data[i][j]*(-1 if i else 1)
assert AB(-i0, -i1).data[i, j] == random_4x4_data[i][j]
AB(-i0, i1).data = random_4x4_data
for i in range(4):
for j in range(4):
assert AB(i0, i1).data[i, j] == random_4x4_data[i][j]*(-1 if i else 1)
assert AB(-i0, i1).data[i, j] == random_4x4_data[i][j]
assert AB(i0, -i1).data[i, j] == random_4x4_data[i][j]*(-1 if i else 1)*(-1 if j else 1)
assert AB(-i0, -i1).data[i, j] == random_4x4_data[i][j]*(-1 if j else 1)
@filter_warnings_decorator
def test_valued_metric_inverse():
(A, B, AB, BA, C, Lorentz, E, px, py, pz, LorentzD, mu0, mu1, mu2, ndm, n0, n1,
n2, NA, NB, NC, minkowski, ba_matrix, ndm_matrix, i0, i1, i2, i3, i4) = _get_valued_base_test_variables()
# let's assign some fancy matrix, just to verify it:
# (this has no physical sense, it's just testing sympy);
# it is symmetrical:
md = [[2, 2, 2, 1], [2, 3, 1, 0], [2, 1, 2, 3], [1, 0, 3, 2]]
Lorentz.data = md
m = Matrix(md)
metric = Lorentz.metric
minv = m.inv()
meye = eye(4)
# the Kronecker Delta:
KD = Lorentz.get_kronecker_delta()
for i in range(4):
for j in range(4):
assert metric(i0, i1).data[i, j] == m[i, j]
assert metric(-i0, -i1).data[i, j] == minv[i, j]
assert metric(i0, -i1).data[i, j] == meye[i, j]
assert metric(-i0, i1).data[i, j] == meye[i, j]
assert metric(i0, i1)[i, j] == m[i, j]
assert metric(-i0, -i1)[i, j] == minv[i, j]
assert metric(i0, -i1)[i, j] == meye[i, j]
assert metric(-i0, i1)[i, j] == meye[i, j]
assert KD(i0, -i1)[i, j] == meye[i, j]
@filter_warnings_decorator
def test_valued_canon_bp_swapaxes():
(A, B, AB, BA, C, Lorentz, E, px, py, pz, LorentzD, mu0, mu1, mu2, ndm, n0, n1,
n2, NA, NB, NC, minkowski, ba_matrix, ndm_matrix, i0, i1, i2, i3, i4) = _get_valued_base_test_variables()
e1 = A(i1)*A(i0)
e2 = e1.canon_bp()
assert e2 == A(i0)*A(i1)
for i in range(4):
for j in range(4):
assert e1[i, j] == e2[j, i]
o1 = B(i2)*A(i1)*B(i0)
o2 = o1.canon_bp()
for i in range(4):
for j in range(4):
for k in range(4):
assert o1[i, j, k] == o2[j, i, k]
@filter_warnings_decorator
def test_valued_components_with_wrong_symmetry():
IT = TensorIndexType('IT', dim=3)
i0, i1, i2, i3 = tensor_indices('i0:4', IT)
IT.data = [1, 1, 1]
A_nosym = TensorHead('A', [IT]*2)
A_sym = TensorHead('A', [IT]*2, TensorSymmetry.fully_symmetric(2))
A_antisym = TensorHead('A', [IT]*2, TensorSymmetry.fully_symmetric(-2))
mat_nosym = Matrix([[1,2,3],[4,5,6],[7,8,9]])
mat_sym = mat_nosym + mat_nosym.T
mat_antisym = mat_nosym - mat_nosym.T
A_nosym.data = mat_nosym
A_nosym.data = mat_sym
A_nosym.data = mat_antisym
def assign(A, dat):
A.data = dat
A_sym.data = mat_sym
raises(ValueError, lambda: assign(A_sym, mat_nosym))
raises(ValueError, lambda: assign(A_sym, mat_antisym))
A_antisym.data = mat_antisym
raises(ValueError, lambda: assign(A_antisym, mat_sym))
raises(ValueError, lambda: assign(A_antisym, mat_nosym))
A_sym.data = [[0, 0, 0], [0, 0, 0], [0, 0, 0]]
A_antisym.data = [[0, 0, 0], [0, 0, 0], [0, 0, 0]]
@filter_warnings_decorator
def test_issue_10972_TensMul_data():
Lorentz = TensorIndexType('Lorentz', metric=False, dummy_fmt='i', dim=2)
Lorentz.data = [-1, 1]
mu, nu, alpha, beta = tensor_indices('\\mu, \\nu, \\alpha, \\beta',
Lorentz)
u = TensorHead('u', [Lorentz])
u.data = [1, 0]
F = TensorHead('F', [Lorentz]*2, TensorSymmetry.fully_symmetric(-2))
F.data = [[0, 1],
[-1, 0]]
mul_1 = F(mu, alpha) * u(-alpha) * F(nu, beta) * u(-beta)
assert (mul_1.data == Array([[0, 0], [0, 1]]))
mul_2 = F(mu, alpha) * F(nu, beta) * u(-alpha) * u(-beta)
assert (mul_2.data == mul_1.data)
assert ((mul_1 + mul_1).data == 2 * mul_1.data)
@filter_warnings_decorator
def test_TensMul_data():
Lorentz = TensorIndexType('Lorentz', metric=False, dummy_fmt='L', dim=4)
Lorentz.data = [-1, 1, 1, 1]
mu, nu, alpha, beta = tensor_indices('\\mu, \\nu, \\alpha, \\beta',
Lorentz)
u = TensorHead('u', [Lorentz])
u.data = [1, 0, 0, 0]
F = TensorHead('F', [Lorentz]*2, TensorSymmetry.fully_symmetric(-2))
Ex, Ey, Ez, Bx, By, Bz = symbols('E_x E_y E_z B_x B_y B_z')
F.data = [
[0, Ex, Ey, Ez],
[-Ex, 0, Bz, -By],
[-Ey, -Bz, 0, Bx],
[-Ez, By, -Bx, 0]]
E = F(mu, nu) * u(-nu)
assert ((E(mu) * E(nu)).data ==
Array([[0, 0, 0, 0],
[0, Ex ** 2, Ex * Ey, Ex * Ez],
[0, Ex * Ey, Ey ** 2, Ey * Ez],
[0, Ex * Ez, Ey * Ez, Ez ** 2]])
)
assert ((E(mu) * E(nu)).canon_bp().data == (E(mu) * E(nu)).data)
assert ((F(mu, alpha) * F(beta, nu) * u(-alpha) * u(-beta)).data ==
- (E(mu) * E(nu)).data
)
assert ((F(alpha, mu) * F(beta, nu) * u(-alpha) * u(-beta)).data ==
(E(mu) * E(nu)).data
)
g = TensorHead('g', [Lorentz]*2, TensorSymmetry.fully_symmetric(2))
g.data = Lorentz.data
# tensor 'perp' is orthogonal to vector 'u'
perp = u(mu) * u(nu) + g(mu, nu)
mul_1 = u(-mu) * perp(mu, nu)
assert (mul_1.data == Array([0, 0, 0, 0]))
mul_2 = u(-mu) * perp(mu, alpha) * perp(nu, beta)
assert (mul_2.data == Array.zeros(4, 4, 4))
Fperp = perp(mu, alpha) * perp(nu, beta) * F(-alpha, -beta)
assert (Fperp.data[0, :] == Array([0, 0, 0, 0]))
assert (Fperp.data[:, 0] == Array([0, 0, 0, 0]))
mul_3 = u(-mu) * Fperp(mu, nu)
assert (mul_3.data == Array([0, 0, 0, 0]))
@filter_warnings_decorator
def test_issue_11020_TensAdd_data():
Lorentz = TensorIndexType('Lorentz', metric=False, dummy_fmt='i', dim=2)
Lorentz.data = [-1, 1]
a, b, c, d = tensor_indices('a, b, c, d', Lorentz)
i0, i1 = tensor_indices('i_0:2', Lorentz)
# metric tensor
g = TensorHead('g', [Lorentz]*2, TensorSymmetry.fully_symmetric(2))
g.data = Lorentz.data
u = TensorHead('u', [Lorentz])
u.data = [1, 0]
add_1 = g(b, c) * g(d, i0) * u(-i0) - g(b, c) * u(d)
assert (add_1.data == Array.zeros(2, 2, 2))
# Now let us replace index `d` with `a`:
add_2 = g(b, c) * g(a, i0) * u(-i0) - g(b, c) * u(a)
assert (add_2.data == Array.zeros(2, 2, 2))
# some more tests
# perp is tensor orthogonal to u^\mu
perp = u(a) * u(b) + g(a, b)
mul_1 = u(-a) * perp(a, b)
assert (mul_1.data == Array([0, 0]))
mul_2 = u(-c) * perp(c, a) * perp(d, b)
assert (mul_2.data == Array.zeros(2, 2, 2))
def test_index_iteration():
L = TensorIndexType("Lorentz", dummy_fmt="L")
i0, i1, i2, i3, i4 = tensor_indices('i0:5', L)
L0 = tensor_indices('L_0', L)
L1 = tensor_indices('L_1', L)
A = TensorHead("A", [L, L])
B = TensorHead("B", [L, L], TensorSymmetry.fully_symmetric(2))
e1 = A(i0,i2)
e2 = A(i0,-i0)
e3 = A(i0,i1)*B(i2,i3)
e4 = A(i0,i1)*B(i2,-i1)
e5 = A(i0,i1)*B(-i0,-i1)
e6 = e1 + e4
assert list(e1._iterate_free_indices) == [(i0, (1, 0)), (i2, (1, 1))]
assert list(e1._iterate_dummy_indices) == []
assert list(e1._iterate_indices) == [(i0, (1, 0)), (i2, (1, 1))]
assert list(e2._iterate_free_indices) == []
assert list(e2._iterate_dummy_indices) == [(L0, (1, 0)), (-L0, (1, 1))]
assert list(e2._iterate_indices) == [(L0, (1, 0)), (-L0, (1, 1))]
assert list(e3._iterate_free_indices) == [(i0, (0, 1, 0)), (i1, (0, 1, 1)), (i2, (1, 1, 0)), (i3, (1, 1, 1))]
assert list(e3._iterate_dummy_indices) == []
assert list(e3._iterate_indices) == [(i0, (0, 1, 0)), (i1, (0, 1, 1)), (i2, (1, 1, 0)), (i3, (1, 1, 1))]
assert list(e4._iterate_free_indices) == [(i0, (0, 1, 0)), (i2, (1, 1, 0))]
assert list(e4._iterate_dummy_indices) == [(L0, (0, 1, 1)), (-L0, (1, 1, 1))]
assert list(e4._iterate_indices) == [(i0, (0, 1, 0)), (L0, (0, 1, 1)), (i2, (1, 1, 0)), (-L0, (1, 1, 1))]
assert list(e5._iterate_free_indices) == []
assert list(e5._iterate_dummy_indices) == [(L0, (0, 1, 0)), (L1, (0, 1, 1)), (-L0, (1, 1, 0)), (-L1, (1, 1, 1))]
assert list(e5._iterate_indices) == [(L0, (0, 1, 0)), (L1, (0, 1, 1)), (-L0, (1, 1, 0)), (-L1, (1, 1, 1))]
assert list(e6._iterate_free_indices) == [(i0, (0, 1, 0)), (i2, (0, 1, 1)), (i0, (1, 0, 1, 0)), (i2, (1, 1, 1, 0))]
assert list(e6._iterate_dummy_indices) == [(L0, (1, 0, 1, 1)), (-L0, (1, 1, 1, 1))]
assert list(e6._iterate_indices) == [(i0, (0, 1, 0)), (i2, (0, 1, 1)), (i0, (1, 0, 1, 0)), (L0, (1, 0, 1, 1)), (i2, (1, 1, 1, 0)), (-L0, (1, 1, 1, 1))]
assert e1.get_indices() == [i0, i2]
assert e1.get_free_indices() == [i0, i2]
assert e2.get_indices() == [L0, -L0]
assert e2.get_free_indices() == []
assert e3.get_indices() == [i0, i1, i2, i3]
assert e3.get_free_indices() == [i0, i1, i2, i3]
assert e4.get_indices() == [i0, L0, i2, -L0]
assert e4.get_free_indices() == [i0, i2]
assert e5.get_indices() == [L0, L1, -L0, -L1]
assert e5.get_free_indices() == []
def test_tensor_expand():
L = TensorIndexType("L")
i, j, k = tensor_indices("i j k", L)
L_0 = TensorIndex("L_0", L)
A, B, C, D = tensor_heads("A B C D", [L])
assert isinstance(Add(A(i), B(i)), TensAdd)
assert isinstance(expand(A(i)+B(i)), TensAdd)
expr = A(i)*(A(-i)+B(-i))
assert expr.args == (A(L_0), A(-L_0) + B(-L_0))
assert expr != A(i)*A(-i) + A(i)*B(-i)
assert expr.expand() == A(i)*A(-i) + A(i)*B(-i)
assert str(expr) == "A(L_0)*(A(-L_0) + B(-L_0))"
expr = A(i)*A(j) + A(i)*B(j)
assert str(expr) == "A(i)*A(j) + A(i)*B(j)"
expr = A(-i)*(A(i)*A(j) + A(i)*B(j)*C(k)*C(-k))
assert expr != A(-i)*A(i)*A(j) + A(-i)*A(i)*B(j)*C(k)*C(-k)
assert expr.expand() == A(-i)*A(i)*A(j) + A(-i)*A(i)*B(j)*C(k)*C(-k)
assert str(expr) == "A(-L_0)*(A(L_0)*A(j) + A(L_0)*B(j)*C(L_1)*C(-L_1))"
assert str(expr.canon_bp()) == 'A(L_0)*A(-L_0)*B(j)*C(L_1)*C(-L_1) + A(j)*A(L_0)*A(-L_0)'
expr = A(-i)*(2*A(i)*A(j) + A(i)*B(j))
assert expr.expand() == 2*A(-i)*A(i)*A(j) + A(-i)*A(i)*B(j)
expr = 2*A(i)*A(-i)
assert expr.coeff == 2
expr = A(i)*(B(j)*C(k) + C(j)*(A(k) + D(k)))
assert str(expr) == "A(i)*(B(j)*C(k) + C(j)*(A(k) + D(k)))"
assert str(expr.expand()) == "A(i)*B(j)*C(k) + A(i)*C(j)*A(k) + A(i)*C(j)*D(k)"
assert isinstance(TensMul(3), TensMul)
tm = TensMul(3).doit()
assert tm == 3
assert isinstance(tm, Integer)
p1 = B(j)*B(-j) + B(j)*C(-j)
p2 = C(-i)*p1
p3 = A(i)*p2
assert p3.expand() == A(i)*C(-i)*B(j)*B(-j) + A(i)*C(-i)*B(j)*C(-j)
expr = A(i)*(B(-i) + C(-i)*(B(j)*B(-j) + B(j)*C(-j)))
assert expr.expand() == A(i)*B(-i) + A(i)*C(-i)*B(j)*B(-j) + A(i)*C(-i)*B(j)*C(-j)
expr = C(-i)*(B(j)*B(-j) + B(j)*C(-j))
assert expr.expand() == C(-i)*B(j)*B(-j) + C(-i)*B(j)*C(-j)
def test_tensor_alternative_construction():
L = TensorIndexType("L")
i0, i1, i2, i3 = tensor_indices('i0:4', L)
A = TensorHead("A", [L])
x, y = symbols("x y")
assert A(i0) == A(Symbol("i0"))
assert A(-i0) == A(-Symbol("i0"))
raises(TypeError, lambda: A(x+y))
raises(ValueError, lambda: A(2*x))
def test_tensor_replacement():
L = TensorIndexType("L")
L2 = TensorIndexType("L2", dim=2)
i, j, k, l = tensor_indices("i j k l", L)
A, B, C, D = tensor_heads("A B C D", [L])
H = TensorHead("H", [L, L])
K = TensorHead("K", [L]*4)
expr = H(i, j)
repl = {H(i,-j): [[1,2],[3,4]], L: diag(1, -1)}
assert expr._extract_data(repl) == ([i, j], Array([[1, -2], [3, -4]]))
assert expr.replace_with_arrays(repl) == Array([[1, -2], [3, -4]])
assert expr.replace_with_arrays(repl, [i, j]) == Array([[1, -2], [3, -4]])
assert expr.replace_with_arrays(repl, [i, -j]) == Array([[1, 2], [3, 4]])
assert expr.replace_with_arrays(repl, [-i, j]) == Array([[1, -2], [-3, 4]])
assert expr.replace_with_arrays(repl, [-i, -j]) == Array([[1, 2], [-3, -4]])
assert expr.replace_with_arrays(repl, [j, i]) == Array([[1, 3], [-2, -4]])
assert expr.replace_with_arrays(repl, [j, -i]) == Array([[1, -3], [-2, 4]])
assert expr.replace_with_arrays(repl, [-j, i]) == Array([[1, 3], [2, 4]])
assert expr.replace_with_arrays(repl, [-j, -i]) == Array([[1, -3], [2, -4]])
# Test stability of optional parameter 'indices'
assert expr.replace_with_arrays(repl) == Array([[1, -2], [3, -4]])
expr = H(i,j)
repl = {H(i,j): [[1,2],[3,4]], L: diag(1, -1)}
assert expr._extract_data(repl) == ([i, j], Array([[1, 2], [3, 4]]))
assert expr.replace_with_arrays(repl) == Array([[1, 2], [3, 4]])
assert expr.replace_with_arrays(repl, [i, j]) == Array([[1, 2], [3, 4]])
assert expr.replace_with_arrays(repl, [i, -j]) == Array([[1, -2], [3, -4]])
assert expr.replace_with_arrays(repl, [-i, j]) == Array([[1, 2], [-3, -4]])
assert expr.replace_with_arrays(repl, [-i, -j]) == Array([[1, -2], [-3, 4]])
assert expr.replace_with_arrays(repl, [j, i]) == Array([[1, 3], [2, 4]])
assert expr.replace_with_arrays(repl, [j, -i]) == Array([[1, -3], [2, -4]])
assert expr.replace_with_arrays(repl, [-j, i]) == Array([[1, 3], [-2, -4]])
assert expr.replace_with_arrays(repl, [-j, -i]) == Array([[1, -3], [-2, 4]])
# Not the same indices:
expr = H(i,k)
repl = {H(i,j): [[1,2],[3,4]], L: diag(1, -1)}
assert expr._extract_data(repl) == ([i, k], Array([[1, 2], [3, 4]]))
expr = A(i)*A(-i)
repl = {A(i): [1,2], L: diag(1, -1)}
assert expr._extract_data(repl) == ([], -3)
assert expr.replace_with_arrays(repl, []) == -3
expr = K(i, j, -j, k)*A(-i)*A(-k)
repl = {A(i): [1, 2], K(i,j,k,l): Array([1]*2**4).reshape(2,2,2,2), L: diag(1, -1)}
assert expr._extract_data(repl)
expr = H(j, k)
repl = {H(i,j): [[1,2],[3,4]], L: diag(1, -1)}
raises(ValueError, lambda: expr._extract_data(repl))
expr = A(i)
repl = {B(i): [1, 2]}
raises(ValueError, lambda: expr._extract_data(repl))
expr = A(i)
repl = {A(i): [[1, 2], [3, 4]]}
raises(ValueError, lambda: expr._extract_data(repl))
# TensAdd:
expr = A(k)*H(i, j) + B(k)*H(i, j)
repl = {A(k): [1], B(k): [1], H(i, j): [[1, 2],[3,4]], L:diag(1,1)}
assert expr._extract_data(repl) == ([k, i, j], Array([[[2, 4], [6, 8]]]))
assert expr.replace_with_arrays(repl, [k, i, j]) == Array([[[2, 4], [6, 8]]])
assert expr.replace_with_arrays(repl, [k, j, i]) == Array([[[2, 6], [4, 8]]])
expr = A(k)*A(-k) + 100
repl = {A(k): [2, 3], L: diag(1, 1)}
assert expr.replace_with_arrays(repl, []) == 113
## Symmetrization:
expr = H(i, j) + H(j, i)
repl = {H(i, j): [[1, 2], [3, 4]]}
assert expr._extract_data(repl) == ([i, j], Array([[2, 5], [5, 8]]))
assert expr.replace_with_arrays(repl, [i, j]) == Array([[2, 5], [5, 8]])
assert expr.replace_with_arrays(repl, [j, i]) == Array([[2, 5], [5, 8]])
## Anti-symmetrization:
expr = H(i, j) - H(j, i)
repl = {H(i, j): [[1, 2], [3, 4]]}
assert expr.replace_with_arrays(repl, [i, j]) == Array([[0, -1], [1, 0]])
assert expr.replace_with_arrays(repl, [j, i]) == Array([[0, 1], [-1, 0]])
# Tensors with contractions in replacements:
expr = K(i, j, k, -k)
repl = {K(i, j, k, -k): [[1, 2], [3, 4]]}
assert expr._extract_data(repl) == ([i, j], Array([[1, 2], [3, 4]]))
expr = H(i, -i)
repl = {H(i, -i): 42}
assert expr._extract_data(repl) == ([], 42)
# Replace with array, raise exception if indices are not compatible:
expr = A(i)*A(j)
repl = {A(i): [1, 2]}
raises(ValueError, lambda: expr.replace_with_arrays(repl, [j]))
# Raise exception if array dimension is not compatible:
expr = A(i)
repl = {A(i): [[1, 2]]}
raises(ValueError, lambda: expr.replace_with_arrays(repl, [i]))
# TensorIndexType with dimension, wrong dimension in replacement array:
u1, u2, u3 = tensor_indices("u1:4", L2)
U = TensorHead("U", [L2])
expr = U(u1)*U(-u2)
repl = {U(u1): [[1]]}
raises(ValueError, lambda: expr.replace_with_arrays(repl, [u1, -u2]))
def test_rewrite_tensor_to_Indexed():
L = TensorIndexType("L", dim=4)
A = TensorHead("A", [L]*4)
B = TensorHead("B", [L])
i0, i1, i2, i3 = symbols("i0:4")
L_0, L_1 = symbols("L_0:2")
a1 = A(i0, i1, i2, i3)
assert a1.rewrite(Indexed) == Indexed(Symbol("A"), i0, i1, i2, i3)
a2 = A(i0, -i0, i2, i3)
assert a2.rewrite(Indexed) == Sum(Indexed(Symbol("A"), L_0, L_0, i2, i3), (L_0, 0, 3))
a3 = a2 + A(i2, i3, i0, -i0)
assert a3.rewrite(Indexed) == \
Sum(Indexed(Symbol("A"), L_0, L_0, i2, i3), (L_0, 0, 3)) +\
Sum(Indexed(Symbol("A"), i2, i3, L_0, L_0), (L_0, 0, 3))
b1 = B(-i0)*a1
assert b1.rewrite(Indexed) == Sum(Indexed(Symbol("B"), L_0)*Indexed(Symbol("A"), L_0, i1, i2, i3), (L_0, 0, 3))
b2 = B(-i3)*a2
assert b2.rewrite(Indexed) == Sum(Indexed(Symbol("B"), L_1)*Indexed(Symbol("A"), L_0, L_0, i2, L_1), (L_0, 0, 3), (L_1, 0, 3))
def test_tensorsymmetry():
with warns_deprecated_sympy():
tensorsymmetry([1]*2)
def test_tensorhead():
with warns_deprecated_sympy():
tensorhead('A', [])
def test_TensorType():
with warns_deprecated_sympy():
sym2 = TensorSymmetry.fully_symmetric(2)
Lorentz = TensorIndexType('Lorentz')
S2 = TensorType([Lorentz]*2, sym2)
assert isinstance(S2, TensorType)
|
36d99b98fe32ecf72945bcd66abc2b5f210e2e1dd41787b8564697152cb61201 | from sympy.core import symbols, S, Pow, Function
from sympy.functions import exp
from sympy.utilities.pytest import raises
from sympy.tensor.indexed import Idx, IndexedBase
from sympy.tensor.index_methods import IndexConformanceException
from sympy import get_contraction_structure, get_indices
def test_trivial_indices():
x, y = symbols('x y')
assert get_indices(x) == (set([]), {})
assert get_indices(x*y) == (set([]), {})
assert get_indices(x + y) == (set([]), {})
assert get_indices(x**y) == (set([]), {})
def test_get_indices_Indexed():
x = IndexedBase('x')
i, j = Idx('i'), Idx('j')
assert get_indices(x[i, j]) == (set([i, j]), {})
assert get_indices(x[j, i]) == (set([j, i]), {})
def test_get_indices_Idx():
f = Function('f')
i, j = Idx('i'), Idx('j')
assert get_indices(f(i)*j) == (set([i, j]), {})
assert get_indices(f(j, i)) == (set([j, i]), {})
assert get_indices(f(i)*i) == (set(), {})
def test_get_indices_mul():
x = IndexedBase('x')
y = IndexedBase('y')
i, j = Idx('i'), Idx('j')
assert get_indices(x[j]*y[i]) == (set([i, j]), {})
assert get_indices(x[i]*y[j]) == (set([i, j]), {})
def test_get_indices_exceptions():
x = IndexedBase('x')
y = IndexedBase('y')
i, j = Idx('i'), Idx('j')
raises(IndexConformanceException, lambda: get_indices(x[i] + y[j]))
def test_scalar_broadcast():
x = IndexedBase('x')
y = IndexedBase('y')
i, j = Idx('i'), Idx('j')
assert get_indices(x[i] + y[i, i]) == (set([i]), {})
assert get_indices(x[i] + y[j, j]) == (set([i]), {})
def test_get_indices_add():
x = IndexedBase('x')
y = IndexedBase('y')
A = IndexedBase('A')
i, j, k = Idx('i'), Idx('j'), Idx('k')
assert get_indices(x[i] + 2*y[i]) == (set([i, ]), {})
assert get_indices(y[i] + 2*A[i, j]*x[j]) == (set([i, ]), {})
assert get_indices(y[i] + 2*(x[i] + A[i, j]*x[j])) == (set([i, ]), {})
assert get_indices(y[i] + x[i]*(A[j, j] + 1)) == (set([i, ]), {})
assert get_indices(
y[i] + x[i]*x[j]*(y[j] + A[j, k]*x[k])) == (set([i, ]), {})
def test_get_indices_Pow():
x = IndexedBase('x')
y = IndexedBase('y')
A = IndexedBase('A')
i, j, k = Idx('i'), Idx('j'), Idx('k')
assert get_indices(Pow(x[i], y[j])) == (set([i, j]), {})
assert get_indices(Pow(x[i, k], y[j, k])) == (set([i, j, k]), {})
assert get_indices(Pow(A[i, k], y[k] + A[k, j]*x[j])) == (set([i, k]), {})
assert get_indices(Pow(2, x[i])) == get_indices(exp(x[i]))
# test of a design decision, this may change:
assert get_indices(Pow(x[i], 2)) == (set([i, ]), {})
def test_get_contraction_structure_basic():
x = IndexedBase('x')
y = IndexedBase('y')
i, j = Idx('i'), Idx('j')
assert get_contraction_structure(x[i]*y[j]) == {None: set([x[i]*y[j]])}
assert get_contraction_structure(x[i] + y[j]) == {None: set([x[i], y[j]])}
assert get_contraction_structure(x[i]*y[i]) == {(i,): set([x[i]*y[i]])}
assert get_contraction_structure(
1 + x[i]*y[i]) == {None: set([S.One]), (i,): set([x[i]*y[i]])}
assert get_contraction_structure(x[i]**y[i]) == {None: set([x[i]**y[i]])}
def test_get_contraction_structure_complex():
x = IndexedBase('x')
y = IndexedBase('y')
A = IndexedBase('A')
i, j, k = Idx('i'), Idx('j'), Idx('k')
expr1 = y[i] + A[i, j]*x[j]
d1 = {None: set([y[i]]), (j,): set([A[i, j]*x[j]])}
assert get_contraction_structure(expr1) == d1
expr2 = expr1*A[k, i] + x[k]
d2 = {None: set([x[k]]), (i,): set([expr1*A[k, i]]), expr1*A[k, i]: [d1]}
assert get_contraction_structure(expr2) == d2
def test_contraction_structure_simple_Pow():
x = IndexedBase('x')
y = IndexedBase('y')
i, j, k = Idx('i'), Idx('j'), Idx('k')
ii_jj = x[i, i]**y[j, j]
assert get_contraction_structure(ii_jj) == {
None: set([ii_jj]),
ii_jj: [
{(i,): set([x[i, i]])},
{(j,): set([y[j, j]])}
]
}
ii_jk = x[i, i]**y[j, k]
assert get_contraction_structure(ii_jk) == {
None: set([x[i, i]**y[j, k]]),
x[i, i]**y[j, k]: [
{(i,): set([x[i, i]])}
]
}
def test_contraction_structure_Mul_and_Pow():
x = IndexedBase('x')
y = IndexedBase('y')
i, j, k = Idx('i'), Idx('j'), Idx('k')
i_ji = x[i]**(y[j]*x[i])
assert get_contraction_structure(i_ji) == {None: set([i_ji])}
ij_i = (x[i]*y[j])**(y[i])
assert get_contraction_structure(ij_i) == {None: set([ij_i])}
j_ij_i = x[j]*(x[i]*y[j])**(y[i])
assert get_contraction_structure(j_ij_i) == {(j,): set([j_ij_i])}
j_i_ji = x[j]*x[i]**(y[j]*x[i])
assert get_contraction_structure(j_i_ji) == {(j,): set([j_i_ji])}
ij_exp_kki = x[i]*y[j]*exp(y[i]*y[k, k])
result = get_contraction_structure(ij_exp_kki)
expected = {
(i,): set([ij_exp_kki]),
ij_exp_kki: [{
None: set([exp(y[i]*y[k, k])]),
exp(y[i]*y[k, k]): [{
None: set([y[i]*y[k, k]]),
y[i]*y[k, k]: [{(k,): set([y[k, k]])}]
}]}
]
}
assert result == expected
def test_contraction_structure_Add_in_Pow():
x = IndexedBase('x')
y = IndexedBase('y')
i, j, k = Idx('i'), Idx('j'), Idx('k')
s_ii_jj_s = (1 + x[i, i])**(1 + y[j, j])
expected = {
None: set([s_ii_jj_s]),
s_ii_jj_s: [
{None: set([S.One]), (i,): set([x[i, i]])},
{None: set([S.One]), (j,): set([y[j, j]])}
]
}
result = get_contraction_structure(s_ii_jj_s)
assert result == expected
s_ii_jk_s = (1 + x[i, i]) ** (1 + y[j, k])
expected_2 = {
None: set([(x[i, i] + 1)**(y[j, k] + 1)]),
s_ii_jk_s: [
{None: set([S.One]), (i,): set([x[i, i]])}
]
}
result_2 = get_contraction_structure(s_ii_jk_s)
assert result_2 == expected_2
def test_contraction_structure_Pow_in_Pow():
x = IndexedBase('x')
y = IndexedBase('y')
z = IndexedBase('z')
i, j, k = Idx('i'), Idx('j'), Idx('k')
ii_jj_kk = x[i, i]**y[j, j]**z[k, k]
expected = {
None: set([ii_jj_kk]),
ii_jj_kk: [
{(i,): set([x[i, i]])},
{
None: set([y[j, j]**z[k, k]]),
y[j, j]**z[k, k]: [
{(j,): set([y[j, j]])},
{(k,): set([z[k, k]])}
]
}
]
}
assert get_contraction_structure(ii_jj_kk) == expected
def test_ufunc_support():
f = Function('f')
g = Function('g')
x = IndexedBase('x')
y = IndexedBase('y')
i, j = Idx('i'), Idx('j')
a = symbols('a')
assert get_indices(f(x[i])) == (set([i]), {})
assert get_indices(f(x[i], y[j])) == (set([i, j]), {})
assert get_indices(f(y[i])*g(x[i])) == (set(), {})
assert get_indices(f(a, x[i])) == (set([i]), {})
assert get_indices(f(a, y[i], x[j])*g(x[i])) == (set([j]), {})
assert get_indices(g(f(x[i]))) == (set([i]), {})
assert get_contraction_structure(f(x[i])) == {None: set([f(x[i])])}
assert get_contraction_structure(
f(y[i])*g(x[i])) == {(i,): set([f(y[i])*g(x[i])])}
assert get_contraction_structure(
f(y[i])*g(f(x[i]))) == {(i,): set([f(y[i])*g(f(x[i]))])}
assert get_contraction_structure(
f(x[j], y[i])*g(x[i])) == {(i,): set([f(x[j], y[i])*g(x[i])])}
|
137e252e38a402bc9f086b49ee13f20a77af4eb9bb24f8ba4335b513bf593c10 | from sympy.tensor.tensor import (Tensor, TensorIndexType, TensorSymmetry,
tensor_indices, TensorHead, TensorElement)
from sympy.tensor import Array
from sympy import Symbol
def test_tensor_element():
L = TensorIndexType("L")
i, j, k, l, m, n = tensor_indices("i j k l m n", L)
A = TensorHead("A", [L, L], TensorSymmetry.no_symmetry(2))
a = A(i, j)
assert isinstance(TensorElement(a, {}), Tensor)
assert isinstance(TensorElement(a, {k: 1}), Tensor)
te1 = TensorElement(a, {Symbol("i"): 1})
assert te1.free == [(j, 0)]
assert te1.get_free_indices() == [j]
assert te1.dum == []
te2 = TensorElement(a, {i: 1})
assert te2.free == [(j, 0)]
assert te2.get_free_indices() == [j]
assert te2.dum == []
assert te1 == te2
array = Array([[1, 2], [3, 4]])
assert te1.replace_with_arrays({A(i, j): array}, [j]) == array[1, :]
|
305cd7a25be66d4fad3a8c01df0374c5422dd686999ac4f8cf8e82cc61b32438 | import random
from sympy.combinatorics import Permutation
from sympy.combinatorics.permutations import _af_invert
from sympy.utilities.pytest import raises
from sympy import symbols, sin, exp, log, cos, transpose, adjoint, conjugate, diff
from sympy.tensor.array import Array, ImmutableDenseNDimArray, ImmutableSparseNDimArray, MutableSparseNDimArray
from sympy.tensor.array.arrayop import tensorproduct, tensorcontraction, derive_by_array, permutedims, Flatten
# Test import although not used in file
from sympy.tensor.array import NDimArray
def test_tensorproduct():
x,y,z,t = symbols('x y z t')
from sympy.abc import a,b,c,d
assert tensorproduct() == 1
assert tensorproduct([x]) == Array([x])
assert tensorproduct([x], [y]) == Array([[x*y]])
assert tensorproduct([x], [y], [z]) == Array([[[x*y*z]]])
assert tensorproduct([x], [y], [z], [t]) == Array([[[[x*y*z*t]]]])
assert tensorproduct(x) == x
assert tensorproduct(x, y) == x*y
assert tensorproduct(x, y, z) == x*y*z
assert tensorproduct(x, y, z, t) == x*y*z*t
for ArrayType in [ImmutableDenseNDimArray, ImmutableSparseNDimArray]:
A = ArrayType([x, y])
B = ArrayType([1, 2, 3])
C = ArrayType([a, b, c, d])
assert tensorproduct(A, B, C) == ArrayType([[[a*x, b*x, c*x, d*x], [2*a*x, 2*b*x, 2*c*x, 2*d*x], [3*a*x, 3*b*x, 3*c*x, 3*d*x]],
[[a*y, b*y, c*y, d*y], [2*a*y, 2*b*y, 2*c*y, 2*d*y], [3*a*y, 3*b*y, 3*c*y, 3*d*y]]])
assert tensorproduct([x, y], [1, 2, 3]) == tensorproduct(A, B)
assert tensorproduct(A, 2) == ArrayType([2*x, 2*y])
assert tensorproduct(A, [2]) == ArrayType([[2*x], [2*y]])
assert tensorproduct([2], A) == ArrayType([[2*x, 2*y]])
assert tensorproduct(a, A) == ArrayType([a*x, a*y])
assert tensorproduct(a, A, B) == ArrayType([[a*x, 2*a*x, 3*a*x], [a*y, 2*a*y, 3*a*y]])
assert tensorproduct(A, B, a) == ArrayType([[a*x, 2*a*x, 3*a*x], [a*y, 2*a*y, 3*a*y]])
assert tensorproduct(B, a, A) == ArrayType([[a*x, a*y], [2*a*x, 2*a*y], [3*a*x, 3*a*y]])
# tests for large scale sparse array
for SparseArrayType in [ImmutableSparseNDimArray, MutableSparseNDimArray]:
a = SparseArrayType({1:2, 3:4},(1000, 2000))
b = SparseArrayType({1:2, 3:4},(1000, 2000))
assert tensorproduct(a, b) == ImmutableSparseNDimArray({2000001: 4, 2000003: 8, 6000001: 8, 6000003: 16}, (1000, 2000, 1000, 2000))
def test_tensorcontraction():
from sympy.abc import a,b,c,d,e,f,g,h,i,j,k,l,m,n,o,p,q,r,s,t,u,v,w,x
B = Array(range(18), (2, 3, 3))
assert tensorcontraction(B, (1, 2)) == Array([12, 39])
C1 = Array([a, b, c, d, e, f, g, h, i, j, k, l, m, n, o, p, q, r, s, t, u, v, w, x], (2, 3, 2, 2))
assert tensorcontraction(C1, (0, 2)) == Array([[a + o, b + p], [e + s, f + t], [i + w, j + x]])
assert tensorcontraction(C1, (0, 2, 3)) == Array([a + p, e + t, i + x])
assert tensorcontraction(C1, (2, 3)) == Array([[a + d, e + h, i + l], [m + p, q + t, u + x]])
def test_derivative_by_array():
from sympy.abc import i, j, t, x, y, z
bexpr = x*y**2*exp(z)*log(t)
sexpr = sin(bexpr)
cexpr = cos(bexpr)
a = Array([sexpr])
assert derive_by_array(sexpr, t) == x*y**2*exp(z)*cos(x*y**2*exp(z)*log(t))/t
assert derive_by_array(sexpr, [x, y, z]) == Array([bexpr/x*cexpr, 2*y*bexpr/y**2*cexpr, bexpr*cexpr])
assert derive_by_array(a, [x, y, z]) == Array([[bexpr/x*cexpr], [2*y*bexpr/y**2*cexpr], [bexpr*cexpr]])
assert derive_by_array(sexpr, [[x, y], [z, t]]) == Array([[bexpr/x*cexpr, 2*y*bexpr/y**2*cexpr], [bexpr*cexpr, bexpr/log(t)/t*cexpr]])
assert derive_by_array(a, [[x, y], [z, t]]) == Array([[[bexpr/x*cexpr], [2*y*bexpr/y**2*cexpr]], [[bexpr*cexpr], [bexpr/log(t)/t*cexpr]]])
assert derive_by_array([[x, y], [z, t]], [x, y]) == Array([[[1, 0], [0, 0]], [[0, 1], [0, 0]]])
assert derive_by_array([[x, y], [z, t]], [[x, y], [z, t]]) == Array([[[[1, 0], [0, 0]], [[0, 1], [0, 0]]],
[[[0, 0], [1, 0]], [[0, 0], [0, 1]]]])
assert diff(sexpr, t) == x*y**2*exp(z)*cos(x*y**2*exp(z)*log(t))/t
assert diff(sexpr, Array([x, y, z])) == Array([bexpr/x*cexpr, 2*y*bexpr/y**2*cexpr, bexpr*cexpr])
assert diff(a, Array([x, y, z])) == Array([[bexpr/x*cexpr], [2*y*bexpr/y**2*cexpr], [bexpr*cexpr]])
assert diff(sexpr, Array([[x, y], [z, t]])) == Array([[bexpr/x*cexpr, 2*y*bexpr/y**2*cexpr], [bexpr*cexpr, bexpr/log(t)/t*cexpr]])
assert diff(a, Array([[x, y], [z, t]])) == Array([[[bexpr/x*cexpr], [2*y*bexpr/y**2*cexpr]], [[bexpr*cexpr], [bexpr/log(t)/t*cexpr]]])
assert diff(Array([[x, y], [z, t]]), Array([x, y])) == Array([[[1, 0], [0, 0]], [[0, 1], [0, 0]]])
assert diff(Array([[x, y], [z, t]]), Array([[x, y], [z, t]])) == Array([[[[1, 0], [0, 0]], [[0, 1], [0, 0]]],
[[[0, 0], [1, 0]], [[0, 0], [0, 1]]]])
# test for large scale sparse array
for SparseArrayType in [ImmutableSparseNDimArray, MutableSparseNDimArray]:
b = MutableSparseNDimArray({0:i, 1:j}, (10000, 20000))
assert derive_by_array(b, i) == ImmutableSparseNDimArray({0: 1}, (10000, 20000))
assert derive_by_array(b, (i, j)) == ImmutableSparseNDimArray({0: 1, 200000001: 1}, (2, 10000, 20000))
def test_issue_emerged_while_discussing_10972():
ua = Array([-1,0])
Fa = Array([[0, 1], [-1, 0]])
po = tensorproduct(Fa, ua, Fa, ua)
assert tensorcontraction(po, (1, 2), (4, 5)) == Array([[0, 0], [0, 1]])
sa = symbols('a0:144')
po = Array(sa, [2, 2, 3, 3, 2, 2])
assert tensorcontraction(po, (0, 1), (2, 3), (4, 5)) == sa[0] + sa[108] + sa[111] + sa[124] + sa[127] + sa[140] + sa[143] + sa[16] + sa[19] + sa[3] + sa[32] + sa[35]
assert tensorcontraction(po, (0, 1, 4, 5), (2, 3)) == sa[0] + sa[111] + sa[127] + sa[143] + sa[16] + sa[32]
assert tensorcontraction(po, (0, 1), (4, 5)) == Array([[sa[0] + sa[108] + sa[111] + sa[3], sa[112] + sa[115] + sa[4] + sa[7],
sa[11] + sa[116] + sa[119] + sa[8]], [sa[12] + sa[120] + sa[123] + sa[15],
sa[124] + sa[127] + sa[16] + sa[19], sa[128] + sa[131] + sa[20] + sa[23]],
[sa[132] + sa[135] + sa[24] + sa[27], sa[136] + sa[139] + sa[28] + sa[31],
sa[140] + sa[143] + sa[32] + sa[35]]])
assert tensorcontraction(po, (0, 1), (2, 3)) == Array([[sa[0] + sa[108] + sa[124] + sa[140] + sa[16] + sa[32], sa[1] + sa[109] + sa[125] + sa[141] + sa[17] + sa[33]],
[sa[110] + sa[126] + sa[142] + sa[18] + sa[2] + sa[34], sa[111] + sa[127] + sa[143] + sa[19] + sa[3] + sa[35]]])
def test_array_permutedims():
sa = symbols('a0:144')
for ArrayType in [ImmutableDenseNDimArray, ImmutableSparseNDimArray]:
m1 = ArrayType(sa[:6], (2, 3))
assert permutedims(m1, (1, 0)) == transpose(m1)
assert m1.tomatrix().T == permutedims(m1, (1, 0)).tomatrix()
assert m1.tomatrix().T == transpose(m1).tomatrix()
assert m1.tomatrix().C == conjugate(m1).tomatrix()
assert m1.tomatrix().H == adjoint(m1).tomatrix()
assert m1.tomatrix().T == m1.transpose().tomatrix()
assert m1.tomatrix().C == m1.conjugate().tomatrix()
assert m1.tomatrix().H == m1.adjoint().tomatrix()
raises(ValueError, lambda: permutedims(m1, (0,)))
raises(ValueError, lambda: permutedims(m1, (0, 0)))
raises(ValueError, lambda: permutedims(m1, (1, 2, 0)))
# Some tests with random arrays:
dims = 6
shape = [random.randint(1,5) for i in range(dims)]
elems = [random.random() for i in range(tensorproduct(*shape))]
ra = ArrayType(elems, shape)
perm = list(range(dims))
# Randomize the permutation:
random.shuffle(perm)
# Test inverse permutation:
assert permutedims(permutedims(ra, perm), _af_invert(perm)) == ra
# Test that permuted shape corresponds to action by `Permutation`:
assert permutedims(ra, perm).shape == tuple(Permutation(perm)(shape))
z = ArrayType.zeros(4,5,6,7)
assert permutedims(z, (2, 3, 1, 0)).shape == (6, 7, 5, 4)
assert permutedims(z, [2, 3, 1, 0]).shape == (6, 7, 5, 4)
assert permutedims(z, Permutation([2, 3, 1, 0])).shape == (6, 7, 5, 4)
po = ArrayType(sa, [2, 2, 3, 3, 2, 2])
raises(ValueError, lambda: permutedims(po, (1, 1)))
raises(ValueError, lambda: po.transpose())
raises(ValueError, lambda: po.adjoint())
assert permutedims(po, reversed(range(po.rank()))) == ArrayType(
[[[[[[sa[0], sa[72]], [sa[36], sa[108]]], [[sa[12], sa[84]], [sa[48], sa[120]]], [[sa[24],
sa[96]], [sa[60], sa[132]]]],
[[[sa[4], sa[76]], [sa[40], sa[112]]], [[sa[16],
sa[88]], [sa[52], sa[124]]],
[[sa[28], sa[100]], [sa[64], sa[136]]]],
[[[sa[8],
sa[80]], [sa[44], sa[116]]], [[sa[20], sa[92]], [sa[56], sa[128]]], [[sa[32],
sa[104]], [sa[68], sa[140]]]]],
[[[[sa[2], sa[74]], [sa[38], sa[110]]], [[sa[14],
sa[86]], [sa[50], sa[122]]], [[sa[26], sa[98]], [sa[62], sa[134]]]],
[[[sa[6],
sa[78]], [sa[42], sa[114]]], [[sa[18], sa[90]], [sa[54], sa[126]]], [[sa[30],
sa[102]], [sa[66], sa[138]]]],
[[[sa[10], sa[82]], [sa[46], sa[118]]], [[sa[22],
sa[94]], [sa[58], sa[130]]],
[[sa[34], sa[106]], [sa[70], sa[142]]]]]],
[[[[[sa[1],
sa[73]], [sa[37], sa[109]]], [[sa[13], sa[85]], [sa[49], sa[121]]], [[sa[25],
sa[97]], [sa[61], sa[133]]]],
[[[sa[5], sa[77]], [sa[41], sa[113]]], [[sa[17],
sa[89]], [sa[53], sa[125]]],
[[sa[29], sa[101]], [sa[65], sa[137]]]],
[[[sa[9],
sa[81]], [sa[45], sa[117]]], [[sa[21], sa[93]], [sa[57], sa[129]]], [[sa[33],
sa[105]], [sa[69], sa[141]]]]],
[[[[sa[3], sa[75]], [sa[39], sa[111]]], [[sa[15],
sa[87]], [sa[51], sa[123]]], [[sa[27], sa[99]], [sa[63], sa[135]]]],
[[[sa[7],
sa[79]], [sa[43], sa[115]]], [[sa[19], sa[91]], [sa[55], sa[127]]], [[sa[31],
sa[103]], [sa[67], sa[139]]]],
[[[sa[11], sa[83]], [sa[47], sa[119]]], [[sa[23],
sa[95]], [sa[59], sa[131]]],
[[sa[35], sa[107]], [sa[71], sa[143]]]]]]])
assert permutedims(po, (1, 0, 2, 3, 4, 5)) == ArrayType(
[[[[[[sa[0], sa[1]], [sa[2], sa[3]]], [[sa[4], sa[5]], [sa[6], sa[7]]], [[sa[8], sa[9]], [sa[10],
sa[11]]]],
[[[sa[12], sa[13]], [sa[14], sa[15]]], [[sa[16], sa[17]], [sa[18],
sa[19]]], [[sa[20], sa[21]], [sa[22], sa[23]]]],
[[[sa[24], sa[25]], [sa[26],
sa[27]]], [[sa[28], sa[29]], [sa[30], sa[31]]], [[sa[32], sa[33]], [sa[34],
sa[35]]]]],
[[[[sa[72], sa[73]], [sa[74], sa[75]]], [[sa[76], sa[77]], [sa[78],
sa[79]]], [[sa[80], sa[81]], [sa[82], sa[83]]]],
[[[sa[84], sa[85]], [sa[86],
sa[87]]], [[sa[88], sa[89]], [sa[90], sa[91]]], [[sa[92], sa[93]], [sa[94],
sa[95]]]],
[[[sa[96], sa[97]], [sa[98], sa[99]]], [[sa[100], sa[101]], [sa[102],
sa[103]]],
[[sa[104], sa[105]], [sa[106], sa[107]]]]]], [[[[[sa[36], sa[37]], [sa[38],
sa[39]]],
[[sa[40], sa[41]], [sa[42], sa[43]]],
[[sa[44], sa[45]], [sa[46],
sa[47]]]],
[[[sa[48], sa[49]], [sa[50], sa[51]]],
[[sa[52], sa[53]], [sa[54],
sa[55]]],
[[sa[56], sa[57]], [sa[58], sa[59]]]],
[[[sa[60], sa[61]], [sa[62],
sa[63]]],
[[sa[64], sa[65]], [sa[66], sa[67]]],
[[sa[68], sa[69]], [sa[70],
sa[71]]]]], [
[[[sa[108], sa[109]], [sa[110], sa[111]]],
[[sa[112], sa[113]], [sa[114],
sa[115]]],
[[sa[116], sa[117]], [sa[118], sa[119]]]],
[[[sa[120], sa[121]], [sa[122],
sa[123]]],
[[sa[124], sa[125]], [sa[126], sa[127]]],
[[sa[128], sa[129]], [sa[130],
sa[131]]]],
[[[sa[132], sa[133]], [sa[134], sa[135]]],
[[sa[136], sa[137]], [sa[138],
sa[139]]],
[[sa[140], sa[141]], [sa[142], sa[143]]]]]]])
assert permutedims(po, (0, 2, 1, 4, 3, 5)) == ArrayType(
[[[[[[sa[0], sa[1]], [sa[4], sa[5]], [sa[8], sa[9]]], [[sa[2], sa[3]], [sa[6], sa[7]], [sa[10],
sa[11]]]],
[[[sa[36], sa[37]], [sa[40], sa[41]], [sa[44], sa[45]]], [[sa[38],
sa[39]], [sa[42], sa[43]], [sa[46], sa[47]]]]],
[[[[sa[12], sa[13]], [sa[16],
sa[17]], [sa[20], sa[21]]], [[sa[14], sa[15]], [sa[18], sa[19]], [sa[22],
sa[23]]]],
[[[sa[48], sa[49]], [sa[52], sa[53]], [sa[56], sa[57]]], [[sa[50],
sa[51]], [sa[54], sa[55]], [sa[58], sa[59]]]]],
[[[[sa[24], sa[25]], [sa[28],
sa[29]], [sa[32], sa[33]]], [[sa[26], sa[27]], [sa[30], sa[31]], [sa[34],
sa[35]]]],
[[[sa[60], sa[61]], [sa[64], sa[65]], [sa[68], sa[69]]], [[sa[62],
sa[63]], [sa[66], sa[67]], [sa[70], sa[71]]]]]],
[[[[[sa[72], sa[73]], [sa[76],
sa[77]], [sa[80], sa[81]]], [[sa[74], sa[75]], [sa[78], sa[79]], [sa[82],
sa[83]]]],
[[[sa[108], sa[109]], [sa[112], sa[113]], [sa[116], sa[117]]], [[sa[110],
sa[111]], [sa[114], sa[115]],
[sa[118], sa[119]]]]],
[[[[sa[84], sa[85]], [sa[88],
sa[89]], [sa[92], sa[93]]], [[sa[86], sa[87]], [sa[90], sa[91]], [sa[94],
sa[95]]]],
[[[sa[120], sa[121]], [sa[124], sa[125]], [sa[128], sa[129]]], [[sa[122],
sa[123]], [sa[126], sa[127]],
[sa[130], sa[131]]]]],
[[[[sa[96], sa[97]], [sa[100],
sa[101]], [sa[104], sa[105]]], [[sa[98], sa[99]], [sa[102], sa[103]], [sa[106],
sa[107]]]],
[[[sa[132], sa[133]], [sa[136], sa[137]], [sa[140], sa[141]]], [[sa[134],
sa[135]], [sa[138], sa[139]],
[sa[142], sa[143]]]]]]])
po2 = po.reshape(4, 9, 2, 2)
assert po2 == ArrayType([[[[sa[0], sa[1]], [sa[2], sa[3]]], [[sa[4], sa[5]], [sa[6], sa[7]]], [[sa[8], sa[9]], [sa[10], sa[11]]], [[sa[12], sa[13]], [sa[14], sa[15]]], [[sa[16], sa[17]], [sa[18], sa[19]]], [[sa[20], sa[21]], [sa[22], sa[23]]], [[sa[24], sa[25]], [sa[26], sa[27]]], [[sa[28], sa[29]], [sa[30], sa[31]]], [[sa[32], sa[33]], [sa[34], sa[35]]]], [[[sa[36], sa[37]], [sa[38], sa[39]]], [[sa[40], sa[41]], [sa[42], sa[43]]], [[sa[44], sa[45]], [sa[46], sa[47]]], [[sa[48], sa[49]], [sa[50], sa[51]]], [[sa[52], sa[53]], [sa[54], sa[55]]], [[sa[56], sa[57]], [sa[58], sa[59]]], [[sa[60], sa[61]], [sa[62], sa[63]]], [[sa[64], sa[65]], [sa[66], sa[67]]], [[sa[68], sa[69]], [sa[70], sa[71]]]], [[[sa[72], sa[73]], [sa[74], sa[75]]], [[sa[76], sa[77]], [sa[78], sa[79]]], [[sa[80], sa[81]], [sa[82], sa[83]]], [[sa[84], sa[85]], [sa[86], sa[87]]], [[sa[88], sa[89]], [sa[90], sa[91]]], [[sa[92], sa[93]], [sa[94], sa[95]]], [[sa[96], sa[97]], [sa[98], sa[99]]], [[sa[100], sa[101]], [sa[102], sa[103]]], [[sa[104], sa[105]], [sa[106], sa[107]]]], [[[sa[108], sa[109]], [sa[110], sa[111]]], [[sa[112], sa[113]], [sa[114], sa[115]]], [[sa[116], sa[117]], [sa[118], sa[119]]], [[sa[120], sa[121]], [sa[122], sa[123]]], [[sa[124], sa[125]], [sa[126], sa[127]]], [[sa[128], sa[129]], [sa[130], sa[131]]], [[sa[132], sa[133]], [sa[134], sa[135]]], [[sa[136], sa[137]], [sa[138], sa[139]]], [[sa[140], sa[141]], [sa[142], sa[143]]]]])
assert permutedims(po2, (3, 2, 0, 1)) == ArrayType([[[[sa[0], sa[4], sa[8], sa[12], sa[16], sa[20], sa[24], sa[28], sa[32]], [sa[36], sa[40], sa[44], sa[48], sa[52], sa[56], sa[60], sa[64], sa[68]], [sa[72], sa[76], sa[80], sa[84], sa[88], sa[92], sa[96], sa[100], sa[104]], [sa[108], sa[112], sa[116], sa[120], sa[124], sa[128], sa[132], sa[136], sa[140]]], [[sa[2], sa[6], sa[10], sa[14], sa[18], sa[22], sa[26], sa[30], sa[34]], [sa[38], sa[42], sa[46], sa[50], sa[54], sa[58], sa[62], sa[66], sa[70]], [sa[74], sa[78], sa[82], sa[86], sa[90], sa[94], sa[98], sa[102], sa[106]], [sa[110], sa[114], sa[118], sa[122], sa[126], sa[130], sa[134], sa[138], sa[142]]]], [[[sa[1], sa[5], sa[9], sa[13], sa[17], sa[21], sa[25], sa[29], sa[33]], [sa[37], sa[41], sa[45], sa[49], sa[53], sa[57], sa[61], sa[65], sa[69]], [sa[73], sa[77], sa[81], sa[85], sa[89], sa[93], sa[97], sa[101], sa[105]], [sa[109], sa[113], sa[117], sa[121], sa[125], sa[129], sa[133], sa[137], sa[141]]], [[sa[3], sa[7], sa[11], sa[15], sa[19], sa[23], sa[27], sa[31], sa[35]], [sa[39], sa[43], sa[47], sa[51], sa[55], sa[59], sa[63], sa[67], sa[71]], [sa[75], sa[79], sa[83], sa[87], sa[91], sa[95], sa[99], sa[103], sa[107]], [sa[111], sa[115], sa[119], sa[123], sa[127], sa[131], sa[135], sa[139], sa[143]]]]])
# test for large scale sparse array
for SparseArrayType in [ImmutableSparseNDimArray, MutableSparseNDimArray]:
A = SparseArrayType({1:1, 10000:2}, (10000, 20000, 10000))
assert permutedims(A, (0, 1, 2)) == A
assert permutedims(A, (1, 0, 2)) == SparseArrayType({1: 1, 100000000: 2}, (20000, 10000, 10000))
B = SparseArrayType({1:1, 20000:2}, (10000, 20000))
assert B.transpose() == SparseArrayType({10000: 1, 1: 2}, (20000, 10000))
def test_flatten():
from sympy import Matrix
for ArrayType in [ImmutableDenseNDimArray, ImmutableSparseNDimArray, Matrix]:
A = ArrayType(range(24)).reshape(4, 6)
assert [i for i in Flatten(A)] == [0, 1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, 15, 16, 17, 18, 19, 20, 21, 22, 23]
for i, v in enumerate(Flatten(A)):
i == v
|
d39f4eea1fa1272ef801166f2a90e6f7a522363660f729326973c19b203ea632 | from copy import copy
from sympy.tensor.array.dense_ndim_array import ImmutableDenseNDimArray
from sympy import Symbol, Rational, SparseMatrix, Dict, diff, symbols, Indexed, IndexedBase, S
from sympy.core.compatibility import long
from sympy.matrices import Matrix
from sympy.tensor.array.sparse_ndim_array import ImmutableSparseNDimArray
from sympy.utilities.pytest import raises
def test_ndim_array_initiation():
arr_with_no_elements = ImmutableDenseNDimArray([], shape=(0,))
assert len(arr_with_no_elements) == 0
assert arr_with_no_elements.rank() == 1
raises(ValueError, lambda: ImmutableDenseNDimArray([0], shape=(0,)))
raises(ValueError, lambda: ImmutableDenseNDimArray([1, 2, 3], shape=(0,)))
raises(ValueError, lambda: ImmutableDenseNDimArray([], shape=()))
raises(ValueError, lambda: ImmutableSparseNDimArray([0], shape=(0,)))
raises(ValueError, lambda: ImmutableSparseNDimArray([1, 2, 3], shape=(0,)))
raises(ValueError, lambda: ImmutableSparseNDimArray([], shape=()))
arr_with_one_element = ImmutableDenseNDimArray([23])
assert len(arr_with_one_element) == 1
assert arr_with_one_element[0] == 23
assert arr_with_one_element[:] == ImmutableDenseNDimArray([23])
assert arr_with_one_element.rank() == 1
arr_with_symbol_element = ImmutableDenseNDimArray([Symbol('x')])
assert len(arr_with_symbol_element) == 1
assert arr_with_symbol_element[0] == Symbol('x')
assert arr_with_symbol_element[:] == ImmutableDenseNDimArray([Symbol('x')])
assert arr_with_symbol_element.rank() == 1
number5 = 5
vector = ImmutableDenseNDimArray.zeros(number5)
assert len(vector) == number5
assert vector.shape == (number5,)
assert vector.rank() == 1
vector = ImmutableSparseNDimArray.zeros(number5)
assert len(vector) == number5
assert vector.shape == (number5,)
assert vector._sparse_array == Dict()
assert vector.rank() == 1
n_dim_array = ImmutableDenseNDimArray(range(3**4), (3, 3, 3, 3,))
assert len(n_dim_array) == 3 * 3 * 3 * 3
assert n_dim_array.shape == (3, 3, 3, 3)
assert n_dim_array.rank() == 4
array_shape = (3, 3, 3, 3)
sparse_array = ImmutableSparseNDimArray.zeros(*array_shape)
assert len(sparse_array._sparse_array) == 0
assert len(sparse_array) == 3 * 3 * 3 * 3
assert n_dim_array.shape == array_shape
assert n_dim_array.rank() == 4
one_dim_array = ImmutableDenseNDimArray([2, 3, 1])
assert len(one_dim_array) == 3
assert one_dim_array.shape == (3,)
assert one_dim_array.rank() == 1
assert one_dim_array.tolist() == [2, 3, 1]
shape = (3, 3)
array_with_many_args = ImmutableSparseNDimArray.zeros(*shape)
assert len(array_with_many_args) == 3 * 3
assert array_with_many_args.shape == shape
assert array_with_many_args[0, 0] == 0
assert array_with_many_args.rank() == 2
shape = (long(3), long(3))
array_with_long_shape = ImmutableSparseNDimArray.zeros(*shape)
assert len(array_with_long_shape) == 3 * 3
assert array_with_long_shape.shape == shape
assert array_with_long_shape[long(0), long(0)] == 0
assert array_with_long_shape.rank() == 2
vector_with_long_shape = ImmutableDenseNDimArray(range(5), long(5))
assert len(vector_with_long_shape) == 5
assert vector_with_long_shape.shape == (long(5),)
assert vector_with_long_shape.rank() == 1
raises(ValueError, lambda: vector_with_long_shape[long(5)])
from sympy.abc import x
for ArrayType in [ImmutableDenseNDimArray, ImmutableSparseNDimArray]:
rank_zero_array = ArrayType(x)
assert len(rank_zero_array) == 1
assert rank_zero_array.shape == ()
assert rank_zero_array.rank() == 0
assert rank_zero_array[()] == x
raises(ValueError, lambda: rank_zero_array[0])
def test_reshape():
array = ImmutableDenseNDimArray(range(50), 50)
assert array.shape == (50,)
assert array.rank() == 1
array = array.reshape(5, 5, 2)
assert array.shape == (5, 5, 2)
assert array.rank() == 3
assert len(array) == 50
def test_getitem():
for ArrayType in [ImmutableDenseNDimArray, ImmutableSparseNDimArray]:
array = ArrayType(range(24)).reshape(2, 3, 4)
assert array.tolist() == [[[0, 1, 2, 3], [4, 5, 6, 7], [8, 9, 10, 11]], [[12, 13, 14, 15], [16, 17, 18, 19], [20, 21, 22, 23]]]
assert array[0] == ArrayType([[0, 1, 2, 3], [4, 5, 6, 7], [8, 9, 10, 11]])
assert array[0, 0] == ArrayType([0, 1, 2, 3])
value = 0
for i in range(2):
for j in range(3):
for k in range(4):
assert array[i, j, k] == value
value += 1
raises(ValueError, lambda: array[3, 4, 5])
raises(ValueError, lambda: array[3, 4, 5, 6])
raises(ValueError, lambda: array[3, 4, 5, 3:4])
def test_iterator():
array = ImmutableDenseNDimArray(range(4), (2, 2))
array[0] == ImmutableDenseNDimArray([0, 1])
array[1] == ImmutableDenseNDimArray([2, 3])
array = array.reshape(4)
j = 0
for i in array:
assert i == j
j += 1
def test_sparse():
sparse_array = ImmutableSparseNDimArray([0, 0, 0, 1], (2, 2))
assert len(sparse_array) == 2 * 2
# dictionary where all data is, only non-zero entries are actually stored:
assert len(sparse_array._sparse_array) == 1
assert sparse_array.tolist() == [[0, 0], [0, 1]]
for i, j in zip(sparse_array, [[0, 0], [0, 1]]):
assert i == ImmutableSparseNDimArray(j)
def sparse_assignment():
sparse_array[0, 0] = 123
assert len(sparse_array._sparse_array) == 1
raises(TypeError, sparse_assignment)
assert len(sparse_array._sparse_array) == 1
assert sparse_array[0, 0] == 0
assert sparse_array/0 == ImmutableSparseNDimArray([[S.NaN, S.NaN], [S.NaN, S.ComplexInfinity]], (2, 2))
# test for large scale sparse array
# equality test
assert ImmutableSparseNDimArray.zeros(100000, 200000) == ImmutableSparseNDimArray.zeros(100000, 200000)
# __mul__ and __rmul__
a = ImmutableSparseNDimArray({200001: 1}, (100000, 200000))
assert a * 3 == ImmutableSparseNDimArray({200001: 3}, (100000, 200000))
assert 3 * a == ImmutableSparseNDimArray({200001: 3}, (100000, 200000))
assert a * 0 == ImmutableSparseNDimArray({}, (100000, 200000))
assert 0 * a == ImmutableSparseNDimArray({}, (100000, 200000))
# __div__
assert a/3 == ImmutableSparseNDimArray({200001: S.One/3}, (100000, 200000))
# __neg__
assert -a == ImmutableSparseNDimArray({200001: -1}, (100000, 200000))
def test_calculation():
a = ImmutableDenseNDimArray([1]*9, (3, 3))
b = ImmutableDenseNDimArray([9]*9, (3, 3))
c = a + b
for i in c:
assert i == ImmutableDenseNDimArray([10, 10, 10])
assert c == ImmutableDenseNDimArray([10]*9, (3, 3))
assert c == ImmutableSparseNDimArray([10]*9, (3, 3))
c = b - a
for i in c:
assert i == ImmutableDenseNDimArray([8, 8, 8])
assert c == ImmutableDenseNDimArray([8]*9, (3, 3))
assert c == ImmutableSparseNDimArray([8]*9, (3, 3))
def test_ndim_array_converting():
dense_array = ImmutableDenseNDimArray([1, 2, 3, 4], (2, 2))
alist = dense_array.tolist()
alist == [[1, 2], [3, 4]]
matrix = dense_array.tomatrix()
assert (isinstance(matrix, Matrix))
for i in range(len(dense_array)):
assert dense_array[dense_array._get_tuple_index(i)] == matrix[i]
assert matrix.shape == dense_array.shape
assert ImmutableDenseNDimArray(matrix) == dense_array
assert ImmutableDenseNDimArray(matrix.as_immutable()) == dense_array
assert ImmutableDenseNDimArray(matrix.as_mutable()) == dense_array
sparse_array = ImmutableSparseNDimArray([1, 2, 3, 4], (2, 2))
alist = sparse_array.tolist()
assert alist == [[1, 2], [3, 4]]
matrix = sparse_array.tomatrix()
assert(isinstance(matrix, SparseMatrix))
for i in range(len(sparse_array)):
assert sparse_array[sparse_array._get_tuple_index(i)] == matrix[i]
assert matrix.shape == sparse_array.shape
assert ImmutableSparseNDimArray(matrix) == sparse_array
assert ImmutableSparseNDimArray(matrix.as_immutable()) == sparse_array
assert ImmutableSparseNDimArray(matrix.as_mutable()) == sparse_array
def test_converting_functions():
arr_list = [1, 2, 3, 4]
arr_matrix = Matrix(((1, 2), (3, 4)))
# list
arr_ndim_array = ImmutableDenseNDimArray(arr_list, (2, 2))
assert (isinstance(arr_ndim_array, ImmutableDenseNDimArray))
assert arr_matrix.tolist() == arr_ndim_array.tolist()
# Matrix
arr_ndim_array = ImmutableDenseNDimArray(arr_matrix)
assert (isinstance(arr_ndim_array, ImmutableDenseNDimArray))
assert arr_matrix.tolist() == arr_ndim_array.tolist()
assert arr_matrix.shape == arr_ndim_array.shape
def test_equality():
first_list = [1, 2, 3, 4]
second_list = [1, 2, 3, 4]
third_list = [4, 3, 2, 1]
assert first_list == second_list
assert first_list != third_list
first_ndim_array = ImmutableDenseNDimArray(first_list, (2, 2))
second_ndim_array = ImmutableDenseNDimArray(second_list, (2, 2))
fourth_ndim_array = ImmutableDenseNDimArray(first_list, (2, 2))
assert first_ndim_array == second_ndim_array
def assignment_attempt(a):
a[0, 0] = 0
raises(TypeError, lambda: assignment_attempt(second_ndim_array))
assert first_ndim_array == second_ndim_array
assert first_ndim_array == fourth_ndim_array
def test_arithmetic():
a = ImmutableDenseNDimArray([3 for i in range(9)], (3, 3))
b = ImmutableDenseNDimArray([7 for i in range(9)], (3, 3))
c1 = a + b
c2 = b + a
assert c1 == c2
d1 = a - b
d2 = b - a
assert d1 == d2 * (-1)
e1 = a * 5
e2 = 5 * a
e3 = copy(a)
e3 *= 5
assert e1 == e2 == e3
f1 = a / 5
f2 = copy(a)
f2 /= 5
assert f1 == f2
assert f1[0, 0] == f1[0, 1] == f1[0, 2] == f1[1, 0] == f1[1, 1] == \
f1[1, 2] == f1[2, 0] == f1[2, 1] == f1[2, 2] == Rational(3, 5)
assert type(a) == type(b) == type(c1) == type(c2) == type(d1) == type(d2) \
== type(e1) == type(e2) == type(e3) == type(f1)
z0 = -a
assert z0 == ImmutableDenseNDimArray([-3 for i in range(9)], (3, 3))
def test_higher_dimenions():
m3 = ImmutableDenseNDimArray(range(10, 34), (2, 3, 4))
assert m3.tolist() == [[[10, 11, 12, 13],
[14, 15, 16, 17],
[18, 19, 20, 21]],
[[22, 23, 24, 25],
[26, 27, 28, 29],
[30, 31, 32, 33]]]
assert m3._get_tuple_index(0) == (0, 0, 0)
assert m3._get_tuple_index(1) == (0, 0, 1)
assert m3._get_tuple_index(4) == (0, 1, 0)
assert m3._get_tuple_index(12) == (1, 0, 0)
assert str(m3) == '[[[10, 11, 12, 13], [14, 15, 16, 17], [18, 19, 20, 21]], [[22, 23, 24, 25], [26, 27, 28, 29], [30, 31, 32, 33]]]'
m3_rebuilt = ImmutableDenseNDimArray([[[10, 11, 12, 13], [14, 15, 16, 17], [18, 19, 20, 21]], [[22, 23, 24, 25], [26, 27, 28, 29], [30, 31, 32, 33]]])
assert m3 == m3_rebuilt
m3_other = ImmutableDenseNDimArray([[[10, 11, 12, 13], [14, 15, 16, 17], [18, 19, 20, 21]], [[22, 23, 24, 25], [26, 27, 28, 29], [30, 31, 32, 33]]], (2, 3, 4))
assert m3 == m3_other
def test_rebuild_immutable_arrays():
sparr = ImmutableSparseNDimArray(range(10, 34), (2, 3, 4))
densarr = ImmutableDenseNDimArray(range(10, 34), (2, 3, 4))
assert sparr == sparr.func(*sparr.args)
assert densarr == densarr.func(*densarr.args)
def test_slices():
md = ImmutableDenseNDimArray(range(10, 34), (2, 3, 4))
assert md[:] == ImmutableDenseNDimArray(range(10, 34), (2, 3, 4))
assert md[:, :, 0].tomatrix() == Matrix([[10, 14, 18], [22, 26, 30]])
assert md[0, 1:2, :].tomatrix() == Matrix([[14, 15, 16, 17]])
assert md[0, 1:3, :].tomatrix() == Matrix([[14, 15, 16, 17], [18, 19, 20, 21]])
assert md[:, :, :] == md
sd = ImmutableSparseNDimArray(range(10, 34), (2, 3, 4))
assert sd == ImmutableSparseNDimArray(md)
assert sd[:] == ImmutableSparseNDimArray(range(10, 34), (2, 3, 4))
assert sd[:, :, 0].tomatrix() == Matrix([[10, 14, 18], [22, 26, 30]])
assert sd[0, 1:2, :].tomatrix() == Matrix([[14, 15, 16, 17]])
assert sd[0, 1:3, :].tomatrix() == Matrix([[14, 15, 16, 17], [18, 19, 20, 21]])
assert sd[:, :, :] == sd
def test_diff_and_applyfunc():
from sympy.abc import x, y, z
md = ImmutableDenseNDimArray([[x, y], [x*z, x*y*z]])
assert md.diff(x) == ImmutableDenseNDimArray([[1, 0], [z, y*z]])
assert diff(md, x) == ImmutableDenseNDimArray([[1, 0], [z, y*z]])
sd = ImmutableSparseNDimArray(md)
assert sd == ImmutableSparseNDimArray([x, y, x*z, x*y*z], (2, 2))
assert sd.diff(x) == ImmutableSparseNDimArray([[1, 0], [z, y*z]])
assert diff(sd, x) == ImmutableSparseNDimArray([[1, 0], [z, y*z]])
mdn = md.applyfunc(lambda x: x*3)
assert mdn == ImmutableDenseNDimArray([[3*x, 3*y], [3*x*z, 3*x*y*z]])
assert md != mdn
sdn = sd.applyfunc(lambda x: x/2)
assert sdn == ImmutableSparseNDimArray([[x/2, y/2], [x*z/2, x*y*z/2]])
assert sd != sdn
sdp = sd.applyfunc(lambda x: x+1)
assert sdp == ImmutableSparseNDimArray([[x + 1, y + 1], [x*z + 1, x*y*z + 1]])
assert sd != sdp
def test_op_priority():
from sympy.abc import x
md = ImmutableDenseNDimArray([1, 2, 3])
e1 = (1+x)*md
e2 = md*(1+x)
assert e1 == ImmutableDenseNDimArray([1+x, 2+2*x, 3+3*x])
assert e1 == e2
sd = ImmutableSparseNDimArray([1, 2, 3])
e3 = (1+x)*sd
e4 = sd*(1+x)
assert e3 == ImmutableDenseNDimArray([1+x, 2+2*x, 3+3*x])
assert e3 == e4
def test_symbolic_indexing():
x, y, z, w = symbols("x y z w")
M = ImmutableDenseNDimArray([[x, y], [z, w]])
i, j = symbols("i, j")
Mij = M[i, j]
assert isinstance(Mij, Indexed)
Ms = ImmutableSparseNDimArray([[2, 3*x], [4, 5]])
msij = Ms[i, j]
assert isinstance(msij, Indexed)
for oi, oj in [(0, 0), (0, 1), (1, 0), (1, 1)]:
assert Mij.subs({i: oi, j: oj}) == M[oi, oj]
assert msij.subs({i: oi, j: oj}) == Ms[oi, oj]
A = IndexedBase("A", (0, 2))
assert A[0, 0].subs(A, M) == x
assert A[i, j].subs(A, M) == M[i, j]
assert M[i, j].subs(M, A) == A[i, j]
assert isinstance(M[3 * i - 2, j], Indexed)
assert M[3 * i - 2, j].subs({i: 1, j: 0}) == M[1, 0]
assert isinstance(M[i, 0], Indexed)
assert M[i, 0].subs(i, 0) == M[0, 0]
assert M[0, i].subs(i, 1) == M[0, 1]
assert M[i, j].diff(x) == ImmutableDenseNDimArray([[1, 0], [0, 0]])[i, j]
assert Ms[i, j].diff(x) == ImmutableSparseNDimArray([[0, 3], [0, 0]])[i, j]
Mo = ImmutableDenseNDimArray([1, 2, 3])
assert Mo[i].subs(i, 1) == 2
Mos = ImmutableSparseNDimArray([1, 2, 3])
assert Mos[i].subs(i, 1) == 2
raises(ValueError, lambda: M[i, 2])
raises(ValueError, lambda: M[i, -1])
raises(ValueError, lambda: M[2, i])
raises(ValueError, lambda: M[-1, i])
raises(ValueError, lambda: Ms[i, 2])
raises(ValueError, lambda: Ms[i, -1])
raises(ValueError, lambda: Ms[2, i])
raises(ValueError, lambda: Ms[-1, i])
def test_issue_12665():
# Testing Python 3 hash of immutable arrays:
arr = ImmutableDenseNDimArray([1, 2, 3])
# This should NOT raise an exception:
hash(arr)
def test_zeros_without_shape():
arr = ImmutableDenseNDimArray.zeros()
assert arr == ImmutableDenseNDimArray(0)
|
8e8d3254d2b54e03a7bcc5db6de801308cd7d670b8f4fed51436eacf87c51ff5 | from copy import copy
from sympy.tensor.array.dense_ndim_array import MutableDenseNDimArray
from sympy import Symbol, Rational, SparseMatrix, diff, sympify, S
from sympy.core.compatibility import long
from sympy.matrices import Matrix
from sympy.tensor.array.sparse_ndim_array import MutableSparseNDimArray
from sympy.utilities.pytest import raises
def test_ndim_array_initiation():
arr_with_one_element = MutableDenseNDimArray([23])
assert len(arr_with_one_element) == 1
assert arr_with_one_element[0] == 23
assert arr_with_one_element.rank() == 1
raises(ValueError, lambda: arr_with_one_element[1])
arr_with_symbol_element = MutableDenseNDimArray([Symbol('x')])
assert len(arr_with_symbol_element) == 1
assert arr_with_symbol_element[0] == Symbol('x')
assert arr_with_symbol_element.rank() == 1
number5 = 5
vector = MutableDenseNDimArray.zeros(number5)
assert len(vector) == number5
assert vector.shape == (number5,)
assert vector.rank() == 1
raises(ValueError, lambda: arr_with_one_element[5])
vector = MutableSparseNDimArray.zeros(number5)
assert len(vector) == number5
assert vector.shape == (number5,)
assert vector._sparse_array == {}
assert vector.rank() == 1
n_dim_array = MutableDenseNDimArray(range(3**4), (3, 3, 3, 3,))
assert len(n_dim_array) == 3 * 3 * 3 * 3
assert n_dim_array.shape == (3, 3, 3, 3)
assert n_dim_array.rank() == 4
raises(ValueError, lambda: n_dim_array[0, 0, 0, 3])
raises(ValueError, lambda: n_dim_array[3, 0, 0, 0])
raises(ValueError, lambda: n_dim_array[3**4])
array_shape = (3, 3, 3, 3)
sparse_array = MutableSparseNDimArray.zeros(*array_shape)
assert len(sparse_array._sparse_array) == 0
assert len(sparse_array) == 3 * 3 * 3 * 3
assert n_dim_array.shape == array_shape
assert n_dim_array.rank() == 4
one_dim_array = MutableDenseNDimArray([2, 3, 1])
assert len(one_dim_array) == 3
assert one_dim_array.shape == (3,)
assert one_dim_array.rank() == 1
assert one_dim_array.tolist() == [2, 3, 1]
shape = (3, 3)
array_with_many_args = MutableSparseNDimArray.zeros(*shape)
assert len(array_with_many_args) == 3 * 3
assert array_with_many_args.shape == shape
assert array_with_many_args[0, 0] == 0
assert array_with_many_args.rank() == 2
shape = (long(3), long(3))
array_with_long_shape = MutableSparseNDimArray.zeros(*shape)
assert len(array_with_long_shape) == 3 * 3
assert array_with_long_shape.shape == shape
assert array_with_long_shape[long(0), long(0)] == 0
assert array_with_long_shape.rank() == 2
vector_with_long_shape = MutableDenseNDimArray(range(5), long(5))
assert len(vector_with_long_shape) == 5
assert vector_with_long_shape.shape == (long(5),)
assert vector_with_long_shape.rank() == 1
raises(ValueError, lambda: vector_with_long_shape[long(5)])
from sympy.abc import x
for ArrayType in [MutableDenseNDimArray, MutableSparseNDimArray]:
rank_zero_array = ArrayType(x)
assert len(rank_zero_array) == 1
assert rank_zero_array.shape == ()
assert rank_zero_array.rank() == 0
assert rank_zero_array[()] == x
raises(ValueError, lambda: rank_zero_array[0])
def test_sympify():
from sympy.abc import x, y, z, t
arr = MutableDenseNDimArray([[x, y], [1, z*t]])
arr_other = sympify(arr)
assert arr_other.shape == (2, 2)
assert arr_other == arr
def test_reshape():
array = MutableDenseNDimArray(range(50), 50)
assert array.shape == (50,)
assert array.rank() == 1
array = array.reshape(5, 5, 2)
assert array.shape == (5, 5, 2)
assert array.rank() == 3
assert len(array) == 50
def test_iterator():
array = MutableDenseNDimArray(range(4), (2, 2))
array[0] == MutableDenseNDimArray([0, 1])
array[1] == MutableDenseNDimArray([2, 3])
array = array.reshape(4)
j = 0
for i in array:
assert i == j
j += 1
def test_getitem():
for ArrayType in [MutableDenseNDimArray, MutableSparseNDimArray]:
array = ArrayType(range(24)).reshape(2, 3, 4)
assert array.tolist() == [[[0, 1, 2, 3], [4, 5, 6, 7], [8, 9, 10, 11]], [[12, 13, 14, 15], [16, 17, 18, 19], [20, 21, 22, 23]]]
assert array[0] == ArrayType([[0, 1, 2, 3], [4, 5, 6, 7], [8, 9, 10, 11]])
assert array[0, 0] == ArrayType([0, 1, 2, 3])
value = 0
for i in range(2):
for j in range(3):
for k in range(4):
assert array[i, j, k] == value
value += 1
raises(ValueError, lambda: array[3, 4, 5])
raises(ValueError, lambda: array[3, 4, 5, 6])
raises(ValueError, lambda: array[3, 4, 5, 3:4])
def test_sparse():
sparse_array = MutableSparseNDimArray([0, 0, 0, 1], (2, 2))
assert len(sparse_array) == 2 * 2
# dictionary where all data is, only non-zero entries are actually stored:
assert len(sparse_array._sparse_array) == 1
assert sparse_array.tolist() == [[0, 0], [0, 1]]
for i, j in zip(sparse_array, [[0, 0], [0, 1]]):
assert i == MutableSparseNDimArray(j)
sparse_array[0, 0] = 123
assert len(sparse_array._sparse_array) == 2
assert sparse_array[0, 0] == 123
assert sparse_array/0 == MutableSparseNDimArray([[S.ComplexInfinity, S.NaN], [S.NaN, S.ComplexInfinity]], (2, 2))
# when element in sparse array become zero it will disappear from
# dictionary
sparse_array[0, 0] = 0
assert len(sparse_array._sparse_array) == 1
sparse_array[1, 1] = 0
assert len(sparse_array._sparse_array) == 0
assert sparse_array[0, 0] == 0
# test for large scale sparse array
# equality test
a = MutableSparseNDimArray.zeros(100000, 200000)
b = MutableSparseNDimArray.zeros(100000, 200000)
assert a == b
a[1, 1] = 1
b[1, 1] = 2
assert a != b
# __mul__ and __rmul__
assert a * 3 == MutableSparseNDimArray({200001: 3}, (100000, 200000))
assert 3 * a == MutableSparseNDimArray({200001: 3}, (100000, 200000))
assert a * 0 == MutableSparseNDimArray({}, (100000, 200000))
assert 0 * a == MutableSparseNDimArray({}, (100000, 200000))
# __div__
assert a/3 == MutableSparseNDimArray({200001: S.One/3}, (100000, 200000))
# __neg__
assert -a == MutableSparseNDimArray({200001: -1}, (100000, 200000))
def test_calculation():
a = MutableDenseNDimArray([1]*9, (3, 3))
b = MutableDenseNDimArray([9]*9, (3, 3))
c = a + b
for i in c:
assert i == MutableDenseNDimArray([10, 10, 10])
assert c == MutableDenseNDimArray([10]*9, (3, 3))
assert c == MutableSparseNDimArray([10]*9, (3, 3))
c = b - a
for i in c:
assert i == MutableSparseNDimArray([8, 8, 8])
assert c == MutableDenseNDimArray([8]*9, (3, 3))
assert c == MutableSparseNDimArray([8]*9, (3, 3))
def test_ndim_array_converting():
dense_array = MutableDenseNDimArray([1, 2, 3, 4], (2, 2))
alist = dense_array.tolist()
alist == [[1, 2], [3, 4]]
matrix = dense_array.tomatrix()
assert (isinstance(matrix, Matrix))
for i in range(len(dense_array)):
assert dense_array[dense_array._get_tuple_index(i)] == matrix[i]
assert matrix.shape == dense_array.shape
assert MutableDenseNDimArray(matrix) == dense_array
assert MutableDenseNDimArray(matrix.as_immutable()) == dense_array
assert MutableDenseNDimArray(matrix.as_mutable()) == dense_array
sparse_array = MutableSparseNDimArray([1, 2, 3, 4], (2, 2))
alist = sparse_array.tolist()
assert alist == [[1, 2], [3, 4]]
matrix = sparse_array.tomatrix()
assert(isinstance(matrix, SparseMatrix))
for i in range(len(sparse_array)):
assert sparse_array[sparse_array._get_tuple_index(i)] == matrix[i]
assert matrix.shape == sparse_array.shape
assert MutableSparseNDimArray(matrix) == sparse_array
assert MutableSparseNDimArray(matrix.as_immutable()) == sparse_array
assert MutableSparseNDimArray(matrix.as_mutable()) == sparse_array
def test_converting_functions():
arr_list = [1, 2, 3, 4]
arr_matrix = Matrix(((1, 2), (3, 4)))
# list
arr_ndim_array = MutableDenseNDimArray(arr_list, (2, 2))
assert (isinstance(arr_ndim_array, MutableDenseNDimArray))
assert arr_matrix.tolist() == arr_ndim_array.tolist()
# Matrix
arr_ndim_array = MutableDenseNDimArray(arr_matrix)
assert (isinstance(arr_ndim_array, MutableDenseNDimArray))
assert arr_matrix.tolist() == arr_ndim_array.tolist()
assert arr_matrix.shape == arr_ndim_array.shape
def test_equality():
first_list = [1, 2, 3, 4]
second_list = [1, 2, 3, 4]
third_list = [4, 3, 2, 1]
assert first_list == second_list
assert first_list != third_list
first_ndim_array = MutableDenseNDimArray(first_list, (2, 2))
second_ndim_array = MutableDenseNDimArray(second_list, (2, 2))
third_ndim_array = MutableDenseNDimArray(third_list, (2, 2))
fourth_ndim_array = MutableDenseNDimArray(first_list, (2, 2))
assert first_ndim_array == second_ndim_array
second_ndim_array[0, 0] = 0
assert first_ndim_array != second_ndim_array
assert first_ndim_array != third_ndim_array
assert first_ndim_array == fourth_ndim_array
def test_arithmetic():
a = MutableDenseNDimArray([3 for i in range(9)], (3, 3))
b = MutableDenseNDimArray([7 for i in range(9)], (3, 3))
c1 = a + b
c2 = b + a
assert c1 == c2
d1 = a - b
d2 = b - a
assert d1 == d2 * (-1)
e1 = a * 5
e2 = 5 * a
e3 = copy(a)
e3 *= 5
assert e1 == e2 == e3
f1 = a / 5
f2 = copy(a)
f2 /= 5
assert f1 == f2
assert f1[0, 0] == f1[0, 1] == f1[0, 2] == f1[1, 0] == f1[1, 1] == \
f1[1, 2] == f1[2, 0] == f1[2, 1] == f1[2, 2] == Rational(3, 5)
assert type(a) == type(b) == type(c1) == type(c2) == type(d1) == type(d2) \
== type(e1) == type(e2) == type(e3) == type(f1)
z0 = -a
assert z0 == MutableDenseNDimArray([-3 for i in range(9)], (3, 3))
def test_higher_dimenions():
m3 = MutableDenseNDimArray(range(10, 34), (2, 3, 4))
assert m3.tolist() == [[[10, 11, 12, 13],
[14, 15, 16, 17],
[18, 19, 20, 21]],
[[22, 23, 24, 25],
[26, 27, 28, 29],
[30, 31, 32, 33]]]
assert m3._get_tuple_index(0) == (0, 0, 0)
assert m3._get_tuple_index(1) == (0, 0, 1)
assert m3._get_tuple_index(4) == (0, 1, 0)
assert m3._get_tuple_index(12) == (1, 0, 0)
assert str(m3) == '[[[10, 11, 12, 13], [14, 15, 16, 17], [18, 19, 20, 21]], [[22, 23, 24, 25], [26, 27, 28, 29], [30, 31, 32, 33]]]'
m3_rebuilt = MutableDenseNDimArray([[[10, 11, 12, 13], [14, 15, 16, 17], [18, 19, 20, 21]], [[22, 23, 24, 25], [26, 27, 28, 29], [30, 31, 32, 33]]])
assert m3 == m3_rebuilt
m3_other = MutableDenseNDimArray([[[10, 11, 12, 13], [14, 15, 16, 17], [18, 19, 20, 21]], [[22, 23, 24, 25], [26, 27, 28, 29], [30, 31, 32, 33]]], (2, 3, 4))
assert m3 == m3_other
def test_slices():
md = MutableDenseNDimArray(range(10, 34), (2, 3, 4))
assert md[:] == MutableDenseNDimArray(range(10, 34), (2, 3, 4))
assert md[:, :, 0].tomatrix() == Matrix([[10, 14, 18], [22, 26, 30]])
assert md[0, 1:2, :].tomatrix() == Matrix([[14, 15, 16, 17]])
assert md[0, 1:3, :].tomatrix() == Matrix([[14, 15, 16, 17], [18, 19, 20, 21]])
assert md[:, :, :] == md
sd = MutableSparseNDimArray(range(10, 34), (2, 3, 4))
assert sd == MutableSparseNDimArray(md)
assert sd[:] == MutableSparseNDimArray(range(10, 34), (2, 3, 4))
assert sd[:, :, 0].tomatrix() == Matrix([[10, 14, 18], [22, 26, 30]])
assert sd[0, 1:2, :].tomatrix() == Matrix([[14, 15, 16, 17]])
assert sd[0, 1:3, :].tomatrix() == Matrix([[14, 15, 16, 17], [18, 19, 20, 21]])
assert sd[:, :, :] == sd
def test_slices_assign():
a = MutableDenseNDimArray(range(12), shape=(4, 3))
b = MutableSparseNDimArray(range(12), shape=(4, 3))
for i in [a, b]:
assert i.tolist() == [[0, 1, 2], [3, 4, 5], [6, 7, 8], [9, 10, 11]]
i[0, :] = [2, 2, 2]
assert i.tolist() == [[2, 2, 2], [3, 4, 5], [6, 7, 8], [9, 10, 11]]
i[0, 1:] = [8, 8]
assert i.tolist() == [[2, 8, 8], [3, 4, 5], [6, 7, 8], [9, 10, 11]]
i[1:3, 1] = [20, 44]
assert i.tolist() == [[2, 8, 8], [3, 20, 5], [6, 44, 8], [9, 10, 11]]
def test_diff():
from sympy.abc import x, y, z
md = MutableDenseNDimArray([[x, y], [x*z, x*y*z]])
assert md.diff(x) == MutableDenseNDimArray([[1, 0], [z, y*z]])
assert diff(md, x) == MutableDenseNDimArray([[1, 0], [z, y*z]])
sd = MutableSparseNDimArray(md)
assert sd == MutableSparseNDimArray([x, y, x*z, x*y*z], (2, 2))
assert sd.diff(x) == MutableSparseNDimArray([[1, 0], [z, y*z]])
assert diff(sd, x) == MutableSparseNDimArray([[1, 0], [z, y*z]])
|
55bd17f1468b8b86352648801c4580394938a91006d0609da943de33159fa1b2 | from sympy.tensor.array.array_comprehension import ArrayComprehension, ArrayComprehensionMap
from sympy.tensor.array import ImmutableDenseNDimArray
from sympy.abc import i, j, k, l
from sympy.utilities.pytest import raises
from sympy.matrices import Matrix
def test_array_comprehension():
a = ArrayComprehension(i*j, (i, 1, 3), (j, 2, 4))
b = ArrayComprehension(i, (i, 1, j+1))
c = ArrayComprehension(i+j+k+l, (i, 1, 2), (j, 1, 3), (k, 1, 4), (l, 1, 5))
d = ArrayComprehension(k, (i, 1, 5))
e = ArrayComprehension(i, (j, k+1, k+5))
assert a.doit().tolist() == [[2, 3, 4], [4, 6, 8], [6, 9, 12]]
assert a.shape == (3, 3)
assert a.is_shape_numeric == True
assert a.tolist() == [[2, 3, 4], [4, 6, 8], [6, 9, 12]]
assert a.tomatrix() == Matrix([
[2, 3, 4],
[4, 6, 8],
[6, 9, 12]])
assert len(a) == 9
assert isinstance(b.doit(), ArrayComprehension)
assert isinstance(a.doit(), ImmutableDenseNDimArray)
assert b.subs(j, 3) == ArrayComprehension(i, (i, 1, 4))
assert b.free_symbols == {j}
assert b.shape == (j + 1,)
assert b.rank() == 1
assert b.is_shape_numeric == False
assert c.free_symbols == set()
assert c.function == i + j + k + l
assert c.limits == ((i, 1, 2), (j, 1, 3), (k, 1, 4), (l, 1, 5))
assert c.doit().tolist() == [[[[4, 5, 6, 7, 8], [5, 6, 7, 8, 9], [6, 7, 8, 9, 10], [7, 8, 9, 10, 11]],
[[5, 6, 7, 8, 9], [6, 7, 8, 9, 10], [7, 8, 9, 10, 11], [8, 9, 10, 11, 12]],
[[6, 7, 8, 9, 10], [7, 8, 9, 10, 11], [8, 9, 10, 11, 12], [9, 10, 11, 12, 13]]],
[[[5, 6, 7, 8, 9], [6, 7, 8, 9, 10], [7, 8, 9, 10, 11], [8, 9, 10, 11, 12]],
[[6, 7, 8, 9, 10], [7, 8, 9, 10, 11], [8, 9, 10, 11, 12], [9, 10, 11, 12, 13]],
[[7, 8, 9, 10, 11], [8, 9, 10, 11, 12], [9, 10, 11, 12, 13], [10, 11, 12, 13, 14]]]]
assert c.free_symbols == set()
assert c.variables == [i, j, k, l]
assert c.bound_symbols == [i, j, k, l]
assert d.doit().tolist() == [k, k, k, k, k]
assert len(e) == 5
raises(TypeError, lambda: ArrayComprehension(i*j, (i, 1, 3), (j, 2, [1, 3, 2])))
raises(ValueError, lambda: ArrayComprehension(i*j, (i, 1, 3), (j, 2, 1)))
raises(ValueError, lambda: ArrayComprehension(i*j, (i, 1, 3), (j, 2, j+1)))
raises(ValueError, lambda: len(ArrayComprehension(i*j, (i, 1, 3), (j, 2, j+4))))
raises(TypeError, lambda: ArrayComprehension(i*j, (i, 0, i + 1.5), (j, 0, 2)))
raises(ValueError, lambda: b.tolist())
raises(ValueError, lambda: b.tomatrix())
raises(ValueError, lambda: c.tomatrix())
def test_arraycomprehensionmap():
a = ArrayComprehensionMap(lambda i: i+1, (i, 1, 5))
assert a.doit().tolist() == [2, 3, 4, 5, 6]
assert a.shape == (5,)
assert a.is_shape_numeric
assert a.tolist() == [2, 3, 4, 5, 6]
assert len(a) == 5
assert isinstance(a.doit(), ImmutableDenseNDimArray)
expr = ArrayComprehensionMap(lambda i: i+1, (i, 1, k))
assert expr.doit() == expr
assert expr.subs(k, 4) == ArrayComprehensionMap(lambda i: i+1, (i, 1, 4))
assert expr.subs(k, 4).doit() == ImmutableDenseNDimArray([2, 3, 4, 5])
b = ArrayComprehensionMap(lambda i: i+1, (i, 1, 2), (i, 1, 3), (i, 1, 4), (i, 1, 5))
assert b.doit().tolist() == [[[[2, 3, 4, 5, 6], [3, 5, 7, 9, 11], [4, 7, 10, 13, 16], [5, 9, 13, 17, 21]],
[[3, 5, 7, 9, 11], [5, 9, 13, 17, 21], [7, 13, 19, 25, 31], [9, 17, 25, 33, 41]],
[[4, 7, 10, 13, 16], [7, 13, 19, 25, 31], [10, 19, 28, 37, 46], [13, 25, 37, 49, 61]]],
[[[3, 5, 7, 9, 11], [5, 9, 13, 17, 21], [7, 13, 19, 25, 31], [9, 17, 25, 33, 41]],
[[5, 9, 13, 17, 21], [9, 17, 25, 33, 41], [13, 25, 37, 49, 61], [17, 33, 49, 65, 81]],
[[7, 13, 19, 25, 31], [13, 25, 37, 49, 61], [19, 37, 55, 73, 91], [25, 49, 73, 97, 121]]]]
# tests about lambda expression
assert ArrayComprehensionMap(lambda: 3, (i, 1, 5)).doit().tolist() == [3, 3, 3, 3, 3]
assert ArrayComprehensionMap(lambda i: i+1, (i, 1, 5)).doit().tolist() == [2, 3, 4, 5, 6]
raises(ValueError, lambda: ArrayComprehensionMap(lambda i, j: i+j, (i, 1, 5)).doit())
raises(ValueError, lambda: ArrayComprehensionMap(i*j, (i, 1, 3), (j, 2, 4)))
|
34a37a74869b472c6ec507d46ee6b480c7b6e823aa7416970d2527e5984d49d2 | from __future__ import print_function, division
from sympy.assumptions.cnf import EncodedCNF
def pycosat_satisfiable(expr, all_models=False):
import pycosat
if not isinstance(expr, EncodedCNF):
exprs = EncodedCNF()
exprs.add_prop(expr)
expr = exprs
# Return UNSAT when False (encoded as 0) is present in the CNF
if {0} in expr.data:
if all_models:
return (f for f in [False])
return False
if not all_models:
r = pycosat.solve(expr.data)
result = (r != "UNSAT")
if not result:
return result
return dict((expr.symbols[abs(lit) - 1], lit > 0) for lit in r)
else:
r = pycosat.itersolve(expr.data)
result = (r != "UNSAT")
if not result:
return result
# Make solutions sympy compatible by creating a generator
def _gen(results):
satisfiable = False
try:
while True:
sol = next(results)
yield dict((expr.symbols[abs(lit) - 1], lit > 0) for lit in sol)
satisfiable = True
except StopIteration:
if not satisfiable:
yield False
return _gen(r)
|
d59bc2849638d53a40e9a278815a04611947743c40ceb5d166574cab743f2800 | """Implementation of DPLL algorithm
Features:
- Clause learning
- Watch literal scheme
- VSIDS heuristic
References:
- https://en.wikipedia.org/wiki/DPLL_algorithm
"""
from __future__ import print_function, division
from collections import defaultdict
from heapq import heappush, heappop
from sympy.core.compatibility import range
from sympy import ordered
from sympy.assumptions.cnf import EncodedCNF
def dpll_satisfiable(expr, all_models=False):
"""
Check satisfiability of a propositional sentence.
It returns a model rather than True when it succeeds.
Returns a generator of all models if all_models is True.
Examples
========
>>> from sympy.abc import A, B
>>> from sympy.logic.algorithms.dpll2 import dpll_satisfiable
>>> dpll_satisfiable(A & ~B)
{A: True, B: False}
>>> dpll_satisfiable(A & ~A)
False
"""
if not isinstance(expr, EncodedCNF):
exprs = EncodedCNF()
exprs.add_prop(expr)
expr = exprs
# Return UNSAT when False (encoded as 0) is present in the CNF
if {0} in expr.data:
if all_models:
return (f for f in [False])
return False
solver = SATSolver(expr.data, expr.variables, set(), expr.symbols)
models = solver._find_model()
if all_models:
return _all_models(models)
try:
return next(models)
except StopIteration:
return False
# Uncomment to confirm the solution is valid (hitting set for the clauses)
#else:
#for cls in clauses_int_repr:
#assert solver.var_settings.intersection(cls)
def _all_models(models):
satisfiable = False
try:
while True:
yield next(models)
satisfiable = True
except StopIteration:
if not satisfiable:
yield False
class SATSolver(object):
"""
Class for representing a SAT solver capable of
finding a model to a boolean theory in conjunctive
normal form.
"""
def __init__(self, clauses, variables, var_settings, symbols=None,
heuristic='vsids', clause_learning='none', INTERVAL=500):
self.var_settings = var_settings
self.heuristic = heuristic
self.is_unsatisfied = False
self._unit_prop_queue = []
self.update_functions = []
self.INTERVAL = INTERVAL
if symbols is None:
self.symbols = list(ordered(variables))
else:
self.symbols = symbols
self._initialize_variables(variables)
self._initialize_clauses(clauses)
if 'vsids' == heuristic:
self._vsids_init()
self.heur_calculate = self._vsids_calculate
self.heur_lit_assigned = self._vsids_lit_assigned
self.heur_lit_unset = self._vsids_lit_unset
self.heur_clause_added = self._vsids_clause_added
# Note: Uncomment this if/when clause learning is enabled
#self.update_functions.append(self._vsids_decay)
else:
raise NotImplementedError
if 'simple' == clause_learning:
self.add_learned_clause = self._simple_add_learned_clause
self.compute_conflict = self.simple_compute_conflict
self.update_functions.append(self.simple_clean_clauses)
elif 'none' == clause_learning:
self.add_learned_clause = lambda x: None
self.compute_conflict = lambda: None
else:
raise NotImplementedError
# Create the base level
self.levels = [Level(0)]
self._current_level.varsettings = var_settings
# Keep stats
self.num_decisions = 0
self.num_learned_clauses = 0
self.original_num_clauses = len(self.clauses)
def _initialize_variables(self, variables):
"""Set up the variable data structures needed."""
self.sentinels = defaultdict(set)
self.occurrence_count = defaultdict(int)
self.variable_set = [False] * (len(variables) + 1)
def _initialize_clauses(self, clauses):
"""Set up the clause data structures needed.
For each clause, the following changes are made:
- Unit clauses are queued for propagation right away.
- Non-unit clauses have their first and last literals set as sentinels.
- The number of clauses a literal appears in is computed.
"""
self.clauses = []
for cls in clauses:
self.clauses.append(list(cls))
for i in range(len(self.clauses)):
# Handle the unit clauses
if 1 == len(self.clauses[i]):
self._unit_prop_queue.append(self.clauses[i][0])
continue
self.sentinels[self.clauses[i][0]].add(i)
self.sentinels[self.clauses[i][-1]].add(i)
for lit in self.clauses[i]:
self.occurrence_count[lit] += 1
def _find_model(self):
"""
Main DPLL loop. Returns a generator of models.
Variables are chosen successively, and assigned to be either
True or False. If a solution is not found with this setting,
the opposite is chosen and the search continues. The solver
halts when every variable has a setting.
Examples
========
>>> from sympy.logic.algorithms.dpll2 import SATSolver
>>> l = SATSolver([{2, -3}, {1}, {3, -3}, {2, -2},
... {3, -2}], {1, 2, 3}, set())
>>> list(l._find_model())
[{1: True, 2: False, 3: False}, {1: True, 2: True, 3: True}]
>>> from sympy.abc import A, B, C
>>> l = SATSolver([{2, -3}, {1}, {3, -3}, {2, -2},
... {3, -2}], {1, 2, 3}, set(), [A, B, C])
>>> list(l._find_model())
[{A: True, B: False, C: False}, {A: True, B: True, C: True}]
"""
# We use this variable to keep track of if we should flip a
# variable setting in successive rounds
flip_var = False
# Check if unit prop says the theory is unsat right off the bat
self._simplify()
if self.is_unsatisfied:
return
# While the theory still has clauses remaining
while True:
# Perform cleanup / fixup at regular intervals
if self.num_decisions % self.INTERVAL == 0:
for func in self.update_functions:
func()
if flip_var:
# We have just backtracked and we are trying to opposite literal
flip_var = False
lit = self._current_level.decision
else:
# Pick a literal to set
lit = self.heur_calculate()
self.num_decisions += 1
# Stopping condition for a satisfying theory
if 0 == lit:
yield dict((self.symbols[abs(lit) - 1],
lit > 0) for lit in self.var_settings)
while self._current_level.flipped:
self._undo()
if len(self.levels) == 1:
return
flip_lit = -self._current_level.decision
self._undo()
self.levels.append(Level(flip_lit, flipped=True))
flip_var = True
continue
# Start the new decision level
self.levels.append(Level(lit))
# Assign the literal, updating the clauses it satisfies
self._assign_literal(lit)
# _simplify the theory
self._simplify()
# Check if we've made the theory unsat
if self.is_unsatisfied:
self.is_unsatisfied = False
# We unroll all of the decisions until we can flip a literal
while self._current_level.flipped:
self._undo()
# If we've unrolled all the way, the theory is unsat
if 1 == len(self.levels):
return
# Detect and add a learned clause
self.add_learned_clause(self.compute_conflict())
# Try the opposite setting of the most recent decision
flip_lit = -self._current_level.decision
self._undo()
self.levels.append(Level(flip_lit, flipped=True))
flip_var = True
########################
# Helper Methods #
########################
@property
def _current_level(self):
"""The current decision level data structure
Examples
========
>>> from sympy.logic.algorithms.dpll2 import SATSolver
>>> l = SATSolver([{1}, {2}], {1, 2}, set())
>>> next(l._find_model())
{1: True, 2: True}
>>> l._current_level.decision
0
>>> l._current_level.flipped
False
>>> l._current_level.var_settings
{1, 2}
"""
return self.levels[-1]
def _clause_sat(self, cls):
"""Check if a clause is satisfied by the current variable setting.
Examples
========
>>> from sympy.logic.algorithms.dpll2 import SATSolver
>>> l = SATSolver([{1}, {-1}], {1}, set())
>>> try:
... next(l._find_model())
... except StopIteration:
... pass
>>> l._clause_sat(0)
False
>>> l._clause_sat(1)
True
"""
for lit in self.clauses[cls]:
if lit in self.var_settings:
return True
return False
def _is_sentinel(self, lit, cls):
"""Check if a literal is a sentinel of a given clause.
Examples
========
>>> from sympy.logic.algorithms.dpll2 import SATSolver
>>> l = SATSolver([{2, -3}, {1}, {3, -3}, {2, -2},
... {3, -2}], {1, 2, 3}, set())
>>> next(l._find_model())
{1: True, 2: False, 3: False}
>>> l._is_sentinel(2, 3)
True
>>> l._is_sentinel(-3, 1)
False
"""
return cls in self.sentinels[lit]
def _assign_literal(self, lit):
"""Make a literal assignment.
The literal assignment must be recorded as part of the current
decision level. Additionally, if the literal is marked as a
sentinel of any clause, then a new sentinel must be chosen. If
this is not possible, then unit propagation is triggered and
another literal is added to the queue to be set in the future.
Examples
========
>>> from sympy.logic.algorithms.dpll2 import SATSolver
>>> l = SATSolver([{2, -3}, {1}, {3, -3}, {2, -2},
... {3, -2}], {1, 2, 3}, set())
>>> next(l._find_model())
{1: True, 2: False, 3: False}
>>> l.var_settings
{-3, -2, 1}
>>> l = SATSolver([{2, -3}, {1}, {3, -3}, {2, -2},
... {3, -2}], {1, 2, 3}, set())
>>> l._assign_literal(-1)
>>> try:
... next(l._find_model())
... except StopIteration:
... pass
>>> l.var_settings
{-1}
"""
self.var_settings.add(lit)
self._current_level.var_settings.add(lit)
self.variable_set[abs(lit)] = True
self.heur_lit_assigned(lit)
sentinel_list = list(self.sentinels[-lit])
for cls in sentinel_list:
if not self._clause_sat(cls):
other_sentinel = None
for newlit in self.clauses[cls]:
if newlit != -lit:
if self._is_sentinel(newlit, cls):
other_sentinel = newlit
elif not self.variable_set[abs(newlit)]:
self.sentinels[-lit].remove(cls)
self.sentinels[newlit].add(cls)
other_sentinel = None
break
# Check if no sentinel update exists
if other_sentinel:
self._unit_prop_queue.append(other_sentinel)
def _undo(self):
"""
_undo the changes of the most recent decision level.
Examples
========
>>> from sympy.logic.algorithms.dpll2 import SATSolver
>>> l = SATSolver([{2, -3}, {1}, {3, -3}, {2, -2},
... {3, -2}], {1, 2, 3}, set())
>>> next(l._find_model())
{1: True, 2: False, 3: False}
>>> level = l._current_level
>>> level.decision, level.var_settings, level.flipped
(-3, {-3, -2}, False)
>>> l._undo()
>>> level = l._current_level
>>> level.decision, level.var_settings, level.flipped
(0, {1}, False)
"""
# Undo the variable settings
for lit in self._current_level.var_settings:
self.var_settings.remove(lit)
self.heur_lit_unset(lit)
self.variable_set[abs(lit)] = False
# Pop the level off the stack
self.levels.pop()
#########################
# Propagation #
#########################
"""
Propagation methods should attempt to soundly simplify the boolean
theory, and return True if any simplification occurred and False
otherwise.
"""
def _simplify(self):
"""Iterate over the various forms of propagation to simplify the theory.
Examples
========
>>> from sympy.logic.algorithms.dpll2 import SATSolver
>>> l = SATSolver([{2, -3}, {1}, {3, -3}, {2, -2},
... {3, -2}], {1, 2, 3}, set())
>>> l.variable_set
[False, False, False, False]
>>> l.sentinels
{-3: {0, 2}, -2: {3, 4}, 2: {0, 3}, 3: {2, 4}}
>>> l._simplify()
>>> l.variable_set
[False, True, False, False]
>>> l.sentinels
{-3: {0, 2}, -2: {3, 4}, -1: set(), 2: {0, 3},
...3: {2, 4}}
"""
changed = True
while changed:
changed = False
changed |= self._unit_prop()
changed |= self._pure_literal()
def _unit_prop(self):
"""Perform unit propagation on the current theory."""
result = len(self._unit_prop_queue) > 0
while self._unit_prop_queue:
next_lit = self._unit_prop_queue.pop()
if -next_lit in self.var_settings:
self.is_unsatisfied = True
self._unit_prop_queue = []
return False
else:
self._assign_literal(next_lit)
return result
def _pure_literal(self):
"""Look for pure literals and assign them when found."""
return False
#########################
# Heuristics #
#########################
def _vsids_init(self):
"""Initialize the data structures needed for the VSIDS heuristic."""
self.lit_heap = []
self.lit_scores = {}
for var in range(1, len(self.variable_set)):
self.lit_scores[var] = float(-self.occurrence_count[var])
self.lit_scores[-var] = float(-self.occurrence_count[-var])
heappush(self.lit_heap, (self.lit_scores[var], var))
heappush(self.lit_heap, (self.lit_scores[-var], -var))
def _vsids_decay(self):
"""Decay the VSIDS scores for every literal.
Examples
========
>>> from sympy.logic.algorithms.dpll2 import SATSolver
>>> l = SATSolver([{2, -3}, {1}, {3, -3}, {2, -2},
... {3, -2}], {1, 2, 3}, set())
>>> l.lit_scores
{-3: -2.0, -2: -2.0, -1: 0.0, 1: 0.0, 2: -2.0, 3: -2.0}
>>> l._vsids_decay()
>>> l.lit_scores
{-3: -1.0, -2: -1.0, -1: 0.0, 1: 0.0, 2: -1.0, 3: -1.0}
"""
# We divide every literal score by 2 for a decay factor
# Note: This doesn't change the heap property
for lit in self.lit_scores.keys():
self.lit_scores[lit] /= 2.0
def _vsids_calculate(self):
"""
VSIDS Heuristic Calculation
Examples
========
>>> from sympy.logic.algorithms.dpll2 import SATSolver
>>> l = SATSolver([{2, -3}, {1}, {3, -3}, {2, -2},
... {3, -2}], {1, 2, 3}, set())
>>> l.lit_heap
[(-2.0, -3), (-2.0, 2), (-2.0, -2), (0.0, 1), (-2.0, 3), (0.0, -1)]
>>> l._vsids_calculate()
-3
>>> l.lit_heap
[(-2.0, -2), (-2.0, 2), (0.0, -1), (0.0, 1), (-2.0, 3)]
"""
if len(self.lit_heap) == 0:
return 0
# Clean out the front of the heap as long the variables are set
while self.variable_set[abs(self.lit_heap[0][1])]:
heappop(self.lit_heap)
if len(self.lit_heap) == 0:
return 0
return heappop(self.lit_heap)[1]
def _vsids_lit_assigned(self, lit):
"""Handle the assignment of a literal for the VSIDS heuristic."""
pass
def _vsids_lit_unset(self, lit):
"""Handle the unsetting of a literal for the VSIDS heuristic.
Examples
========
>>> from sympy.logic.algorithms.dpll2 import SATSolver
>>> l = SATSolver([{2, -3}, {1}, {3, -3}, {2, -2},
... {3, -2}], {1, 2, 3}, set())
>>> l.lit_heap
[(-2.0, -3), (-2.0, 2), (-2.0, -2), (0.0, 1), (-2.0, 3), (0.0, -1)]
>>> l._vsids_lit_unset(2)
>>> l.lit_heap
[(-2.0, -3), (-2.0, -2), (-2.0, -2), (-2.0, 2), (-2.0, 3), (0.0, -1),
...(-2.0, 2), (0.0, 1)]
"""
var = abs(lit)
heappush(self.lit_heap, (self.lit_scores[var], var))
heappush(self.lit_heap, (self.lit_scores[-var], -var))
def _vsids_clause_added(self, cls):
"""Handle the addition of a new clause for the VSIDS heuristic.
Examples
========
>>> from sympy.logic.algorithms.dpll2 import SATSolver
>>> l = SATSolver([{2, -3}, {1}, {3, -3}, {2, -2},
... {3, -2}], {1, 2, 3}, set())
>>> l.num_learned_clauses
0
>>> l.lit_scores
{-3: -2.0, -2: -2.0, -1: 0.0, 1: 0.0, 2: -2.0, 3: -2.0}
>>> l._vsids_clause_added({2, -3})
>>> l.num_learned_clauses
1
>>> l.lit_scores
{-3: -1.0, -2: -2.0, -1: 0.0, 1: 0.0, 2: -1.0, 3: -2.0}
"""
self.num_learned_clauses += 1
for lit in cls:
self.lit_scores[lit] += 1
########################
# Clause Learning #
########################
def _simple_add_learned_clause(self, cls):
"""Add a new clause to the theory.
Examples
========
>>> from sympy.logic.algorithms.dpll2 import SATSolver
>>> l = SATSolver([{2, -3}, {1}, {3, -3}, {2, -2},
... {3, -2}], {1, 2, 3}, set())
>>> l.num_learned_clauses
0
>>> l.clauses
[[2, -3], [1], [3, -3], [2, -2], [3, -2]]
>>> l.sentinels
{-3: {0, 2}, -2: {3, 4}, 2: {0, 3}, 3: {2, 4}}
>>> l._simple_add_learned_clause([3])
>>> l.clauses
[[2, -3], [1], [3, -3], [2, -2], [3, -2], [3]]
>>> l.sentinels
{-3: {0, 2}, -2: {3, 4}, 2: {0, 3}, 3: {2, 4, 5}}
"""
cls_num = len(self.clauses)
self.clauses.append(cls)
for lit in cls:
self.occurrence_count[lit] += 1
self.sentinels[cls[0]].add(cls_num)
self.sentinels[cls[-1]].add(cls_num)
self.heur_clause_added(cls)
def _simple_compute_conflict(self):
""" Build a clause representing the fact that at least one decision made
so far is wrong.
Examples
========
>>> from sympy.logic.algorithms.dpll2 import SATSolver
>>> l = SATSolver([{2, -3}, {1}, {3, -3}, {2, -2},
... {3, -2}], {1, 2, 3}, set())
>>> next(l._find_model())
{1: True, 2: False, 3: False}
>>> l._simple_compute_conflict()
[3]
"""
return [-(level.decision) for level in self.levels[1:]]
def _simple_clean_clauses(self):
"""Clean up learned clauses."""
pass
class Level(object):
"""
Represents a single level in the DPLL algorithm, and contains
enough information for a sound backtracking procedure.
"""
def __init__(self, decision, flipped=False):
self.decision = decision
self.var_settings = set()
self.flipped = flipped
|
89cc8f883ba35f4e9a0bae31c7ffb0b188aef440f10d65b6a7cc0b9a0db8752e | """Implementation of DPLL algorithm
Further improvements: eliminate calls to pl_true, implement branching rules,
efficient unit propagation.
References:
- https://en.wikipedia.org/wiki/DPLL_algorithm
- https://www.researchgate.net/publication/242384772_Implementations_of_the_DPLL_Algorithm
"""
from __future__ import print_function, division
from sympy.core.compatibility import range
from sympy import default_sort_key
from sympy.logic.boolalg import Or, Not, conjuncts, disjuncts, to_cnf, \
to_int_repr, _find_predicates
from sympy.assumptions.cnf import CNF
from sympy.logic.inference import pl_true, literal_symbol
def dpll_satisfiable(expr):
"""
Check satisfiability of a propositional sentence.
It returns a model rather than True when it succeeds
>>> from sympy.abc import A, B
>>> from sympy.logic.algorithms.dpll import dpll_satisfiable
>>> dpll_satisfiable(A & ~B)
{A: True, B: False}
>>> dpll_satisfiable(A & ~A)
False
"""
if not isinstance(expr, CNF):
clauses = conjuncts(to_cnf(expr))
else:
clauses = expr.clauses
if False in clauses:
return False
symbols = sorted(_find_predicates(expr), key=default_sort_key)
symbols_int_repr = set(range(1, len(symbols) + 1))
clauses_int_repr = to_int_repr(clauses, symbols)
result = dpll_int_repr(clauses_int_repr, symbols_int_repr, {})
if not result:
return result
output = {}
for key in result:
output.update({symbols[key - 1]: result[key]})
return output
def dpll(clauses, symbols, model):
"""
Compute satisfiability in a partial model.
Clauses is an array of conjuncts.
>>> from sympy.abc import A, B, D
>>> from sympy.logic.algorithms.dpll import dpll
>>> dpll([A, B, D], [A, B], {D: False})
False
"""
# compute DP kernel
P, value = find_unit_clause(clauses, model)
while P:
model.update({P: value})
symbols.remove(P)
if not value:
P = ~P
clauses = unit_propagate(clauses, P)
P, value = find_unit_clause(clauses, model)
P, value = find_pure_symbol(symbols, clauses)
while P:
model.update({P: value})
symbols.remove(P)
if not value:
P = ~P
clauses = unit_propagate(clauses, P)
P, value = find_pure_symbol(symbols, clauses)
# end DP kernel
unknown_clauses = []
for c in clauses:
val = pl_true(c, model)
if val is False:
return False
if val is not True:
unknown_clauses.append(c)
if not unknown_clauses:
return model
if not clauses:
return model
P = symbols.pop()
model_copy = model.copy()
model.update({P: True})
model_copy.update({P: False})
symbols_copy = symbols[:]
return (dpll(unit_propagate(unknown_clauses, P), symbols, model) or
dpll(unit_propagate(unknown_clauses, Not(P)), symbols_copy, model_copy))
def dpll_int_repr(clauses, symbols, model):
"""
Compute satisfiability in a partial model.
Arguments are expected to be in integer representation
>>> from sympy.logic.algorithms.dpll import dpll_int_repr
>>> dpll_int_repr([{1}, {2}, {3}], {1, 2}, {3: False})
False
"""
# compute DP kernel
P, value = find_unit_clause_int_repr(clauses, model)
while P:
model.update({P: value})
symbols.remove(P)
if not value:
P = -P
clauses = unit_propagate_int_repr(clauses, P)
P, value = find_unit_clause_int_repr(clauses, model)
P, value = find_pure_symbol_int_repr(symbols, clauses)
while P:
model.update({P: value})
symbols.remove(P)
if not value:
P = -P
clauses = unit_propagate_int_repr(clauses, P)
P, value = find_pure_symbol_int_repr(symbols, clauses)
# end DP kernel
unknown_clauses = []
for c in clauses:
val = pl_true_int_repr(c, model)
if val is False:
return False
if val is not True:
unknown_clauses.append(c)
if not unknown_clauses:
return model
P = symbols.pop()
model_copy = model.copy()
model.update({P: True})
model_copy.update({P: False})
symbols_copy = symbols.copy()
return (dpll_int_repr(unit_propagate_int_repr(unknown_clauses, P), symbols, model) or
dpll_int_repr(unit_propagate_int_repr(unknown_clauses, -P), symbols_copy, model_copy))
### helper methods for DPLL
def pl_true_int_repr(clause, model={}):
"""
Lightweight version of pl_true.
Argument clause represents the set of args of an Or clause. This is used
inside dpll_int_repr, it is not meant to be used directly.
>>> from sympy.logic.algorithms.dpll import pl_true_int_repr
>>> pl_true_int_repr({1, 2}, {1: False})
>>> pl_true_int_repr({1, 2}, {1: False, 2: False})
False
"""
result = False
for lit in clause:
if lit < 0:
p = model.get(-lit)
if p is not None:
p = not p
else:
p = model.get(lit)
if p is True:
return True
elif p is None:
result = None
return result
def unit_propagate(clauses, symbol):
"""
Returns an equivalent set of clauses
If a set of clauses contains the unit clause l, the other clauses are
simplified by the application of the two following rules:
1. every clause containing l is removed
2. in every clause that contains ~l this literal is deleted
Arguments are expected to be in CNF.
>>> from sympy import symbols
>>> from sympy.abc import A, B, D
>>> from sympy.logic.algorithms.dpll import unit_propagate
>>> unit_propagate([A | B, D | ~B, B], B)
[D, B]
"""
output = []
for c in clauses:
if c.func != Or:
output.append(c)
continue
for arg in c.args:
if arg == ~symbol:
output.append(Or(*[x for x in c.args if x != ~symbol]))
break
if arg == symbol:
break
else:
output.append(c)
return output
def unit_propagate_int_repr(clauses, s):
"""
Same as unit_propagate, but arguments are expected to be in integer
representation
>>> from sympy.logic.algorithms.dpll import unit_propagate_int_repr
>>> unit_propagate_int_repr([{1, 2}, {3, -2}, {2}], 2)
[{3}]
"""
negated = {-s}
return [clause - negated for clause in clauses if s not in clause]
def find_pure_symbol(symbols, unknown_clauses):
"""
Find a symbol and its value if it appears only as a positive literal
(or only as a negative) in clauses.
>>> from sympy import symbols
>>> from sympy.abc import A, B, D
>>> from sympy.logic.algorithms.dpll import find_pure_symbol
>>> find_pure_symbol([A, B, D], [A|~B,~B|~D,D|A])
(A, True)
"""
for sym in symbols:
found_pos, found_neg = False, False
for c in unknown_clauses:
if not found_pos and sym in disjuncts(c):
found_pos = True
if not found_neg and Not(sym) in disjuncts(c):
found_neg = True
if found_pos != found_neg:
return sym, found_pos
return None, None
def find_pure_symbol_int_repr(symbols, unknown_clauses):
"""
Same as find_pure_symbol, but arguments are expected
to be in integer representation
>>> from sympy.logic.algorithms.dpll import find_pure_symbol_int_repr
>>> find_pure_symbol_int_repr({1,2,3},
... [{1, -2}, {-2, -3}, {3, 1}])
(1, True)
"""
all_symbols = set().union(*unknown_clauses)
found_pos = all_symbols.intersection(symbols)
found_neg = all_symbols.intersection([-s for s in symbols])
for p in found_pos:
if -p not in found_neg:
return p, True
for p in found_neg:
if -p not in found_pos:
return -p, False
return None, None
def find_unit_clause(clauses, model):
"""
A unit clause has only 1 variable that is not bound in the model.
>>> from sympy import symbols
>>> from sympy.abc import A, B, D
>>> from sympy.logic.algorithms.dpll import find_unit_clause
>>> find_unit_clause([A | B | D, B | ~D, A | ~B], {A:True})
(B, False)
"""
for clause in clauses:
num_not_in_model = 0
for literal in disjuncts(clause):
sym = literal_symbol(literal)
if sym not in model:
num_not_in_model += 1
P, value = sym, not isinstance(literal, Not)
if num_not_in_model == 1:
return P, value
return None, None
def find_unit_clause_int_repr(clauses, model):
"""
Same as find_unit_clause, but arguments are expected to be in
integer representation.
>>> from sympy.logic.algorithms.dpll import find_unit_clause_int_repr
>>> find_unit_clause_int_repr([{1, 2, 3},
... {2, -3}, {1, -2}], {1: True})
(2, False)
"""
bound = set(model) | set(-sym for sym in model)
for clause in clauses:
unbound = clause - bound
if len(unbound) == 1:
p = unbound.pop()
if p < 0:
return -p, False
else:
return p, True
return None, None
|
fc10a0b4bd60933aaf888510815410ff7a3a942c2181dc80f461a70df8243bc2 | from sympy.assumptions.ask import Q
from sympy.core.numbers import oo
from sympy.core.relational import Equality, Eq, Ne
from sympy.core.singleton import S
from sympy.core.symbol import (Dummy, symbols)
from sympy.functions import Piecewise
from sympy.functions.elementary.miscellaneous import Max, Min
from sympy.functions.elementary.trigonometric import sin
from sympy.sets.sets import (EmptySet, Interval, Union)
from sympy.simplify.simplify import simplify
from sympy.logic.boolalg import (
And, Boolean, Equivalent, ITE, Implies, Nand, Nor, Not, Or,
POSform, SOPform, Xor, Xnor, conjuncts, disjuncts,
distribute_or_over_and, distribute_and_over_or,
eliminate_implications, is_nnf, is_cnf, is_dnf, simplify_logic,
to_nnf, to_cnf, to_dnf, to_int_repr, bool_map, true, false,
BooleanAtom, is_literal, term_to_integer, integer_to_term,
truth_table, as_Boolean)
from sympy.assumptions.cnf import CNF
from sympy.utilities.pytest import raises, XFAIL, slow
from sympy.utilities import cartes
from itertools import combinations
A, B, C, D = symbols('A:D')
a, b, c, d, e, w, x, y, z = symbols('a:e w:z')
def test_overloading():
"""Test that |, & are overloaded as expected"""
assert A & B == And(A, B)
assert A | B == Or(A, B)
assert (A & B) | C == Or(And(A, B), C)
assert A >> B == Implies(A, B)
assert A << B == Implies(B, A)
assert ~A == Not(A)
assert A ^ B == Xor(A, B)
def test_And():
assert And() is true
assert And(A) == A
assert And(True) is true
assert And(False) is false
assert And(True, True) is true
assert And(True, False) is false
assert And(False, False) is false
assert And(True, A) == A
assert And(False, A) is false
assert And(True, True, True) is true
assert And(True, True, A) == A
assert And(True, False, A) is false
assert And(1, A) == A
raises(TypeError, lambda: And(2, A))
raises(TypeError, lambda: And(A < 2, A))
assert And(A < 1, A >= 1) is false
e = A > 1
assert And(e, e.canonical) == e.canonical
g, l, ge, le = A > B, B < A, A >= B, B <= A
assert And(g, l, ge, le) == And(l, le)
def test_Or():
assert Or() is false
assert Or(A) == A
assert Or(True) is true
assert Or(False) is false
assert Or(True, True) is true
assert Or(True, False) is true
assert Or(False, False) is false
assert Or(True, A) is true
assert Or(False, A) == A
assert Or(True, False, False) is true
assert Or(True, False, A) is true
assert Or(False, False, A) == A
assert Or(1, A) is true
raises(TypeError, lambda: Or(2, A))
raises(TypeError, lambda: Or(A < 2, A))
assert Or(A < 1, A >= 1) is true
e = A > 1
assert Or(e, e.canonical) == e
g, l, ge, le = A > B, B < A, A >= B, B <= A
assert Or(g, l, ge, le) == Or(g, ge)
def test_Xor():
assert Xor() is false
assert Xor(A) == A
assert Xor(A, A) is false
assert Xor(True, A, A) is true
assert Xor(A, A, A, A, A) == A
assert Xor(True, False, False, A, B) == ~Xor(A, B)
assert Xor(True) is true
assert Xor(False) is false
assert Xor(True, True) is false
assert Xor(True, False) is true
assert Xor(False, False) is false
assert Xor(True, A) == ~A
assert Xor(False, A) == A
assert Xor(True, False, False) is true
assert Xor(True, False, A) == ~A
assert Xor(False, False, A) == A
assert isinstance(Xor(A, B), Xor)
assert Xor(A, B, Xor(C, D)) == Xor(A, B, C, D)
assert Xor(A, B, Xor(B, C)) == Xor(A, C)
assert Xor(A < 1, A >= 1, B) == Xor(0, 1, B) == Xor(1, 0, B)
e = A > 1
assert Xor(e, e.canonical) == Xor(0, 0) == Xor(1, 1)
def test_rewrite_as_And():
expr = x ^ y
assert expr.rewrite(And) == (x | y) & (~x | ~y)
def test_rewrite_as_Or():
expr = x ^ y
assert expr.rewrite(Or) == (x & ~y) | (y & ~x)
def test_rewrite_as_Nand():
expr = (y & z) | (z & ~w)
assert expr.rewrite(Nand) == ~(~(y & z) & ~(z & ~w))
def test_rewrite_as_Nor():
expr = z & (y | ~w)
assert expr.rewrite(Nor) == ~(~z | ~(y | ~w))
def test_Not():
raises(TypeError, lambda: Not(True, False))
assert Not(True) is false
assert Not(False) is true
assert Not(0) is true
assert Not(1) is false
assert Not(2) is false
def test_Nand():
assert Nand() is false
assert Nand(A) == ~A
assert Nand(True) is false
assert Nand(False) is true
assert Nand(True, True) is false
assert Nand(True, False) is true
assert Nand(False, False) is true
assert Nand(True, A) == ~A
assert Nand(False, A) is true
assert Nand(True, True, True) is false
assert Nand(True, True, A) == ~A
assert Nand(True, False, A) is true
def test_Nor():
assert Nor() is true
assert Nor(A) == ~A
assert Nor(True) is false
assert Nor(False) is true
assert Nor(True, True) is false
assert Nor(True, False) is false
assert Nor(False, False) is true
assert Nor(True, A) is false
assert Nor(False, A) == ~A
assert Nor(True, True, True) is false
assert Nor(True, True, A) is false
assert Nor(True, False, A) is false
def test_Xnor():
assert Xnor() is true
assert Xnor(A) == ~A
assert Xnor(A, A) is true
assert Xnor(True, A, A) is false
assert Xnor(A, A, A, A, A) == ~A
assert Xnor(True) is false
assert Xnor(False) is true
assert Xnor(True, True) is true
assert Xnor(True, False) is false
assert Xnor(False, False) is true
assert Xnor(True, A) == A
assert Xnor(False, A) == ~A
assert Xnor(True, False, False) is false
assert Xnor(True, False, A) == A
assert Xnor(False, False, A) == ~A
def test_Implies():
raises(ValueError, lambda: Implies(A, B, C))
assert Implies(True, True) is true
assert Implies(True, False) is false
assert Implies(False, True) is true
assert Implies(False, False) is true
assert Implies(0, A) is true
assert Implies(1, 1) is true
assert Implies(1, 0) is false
assert A >> B == B << A
assert (A < 1) >> (A >= 1) == (A >= 1)
assert (A < 1) >> (S(1) > A) is true
assert A >> A is true
def test_Equivalent():
assert Equivalent(A, B) == Equivalent(B, A) == Equivalent(A, B, A)
assert Equivalent() is true
assert Equivalent(A, A) == Equivalent(A) is true
assert Equivalent(True, True) == Equivalent(False, False) is true
assert Equivalent(True, False) == Equivalent(False, True) is false
assert Equivalent(A, True) == A
assert Equivalent(A, False) == Not(A)
assert Equivalent(A, B, True) == A & B
assert Equivalent(A, B, False) == ~A & ~B
assert Equivalent(1, A) == A
assert Equivalent(0, A) == Not(A)
assert Equivalent(A, Equivalent(B, C)) != Equivalent(Equivalent(A, B), C)
assert Equivalent(A < 1, A >= 1) is false
assert Equivalent(A < 1, A >= 1, 0) is false
assert Equivalent(A < 1, A >= 1, 1) is false
assert Equivalent(A < 1, S(1) > A) == Equivalent(1, 1) == Equivalent(0, 0)
assert Equivalent(Equality(A, B), Equality(B, A)) is true
def test_equals():
assert Not(Or(A, B)).equals(And(Not(A), Not(B))) is True
assert Equivalent(A, B).equals((A >> B) & (B >> A)) is True
assert ((A | ~B) & (~A | B)).equals((~A & ~B) | (A & B)) is True
assert (A >> B).equals(~A >> ~B) is False
assert (A >> (B >> A)).equals(A >> (C >> A)) is False
raises(NotImplementedError, lambda: (A & B).equals(A > B))
def test_simplification():
"""
Test working of simplification methods.
"""
set1 = [[0, 0, 1], [0, 1, 1], [1, 0, 0], [1, 1, 0]]
set2 = [[0, 0, 0], [0, 1, 0], [1, 0, 1], [1, 1, 1]]
assert SOPform([x, y, z], set1) == Or(And(Not(x), z), And(Not(z), x))
assert Not(SOPform([x, y, z], set2)) == \
Not(Or(And(Not(x), Not(z)), And(x, z)))
assert POSform([x, y, z], set1 + set2) is true
assert SOPform([x, y, z], set1 + set2) is true
assert SOPform([Dummy(), Dummy(), Dummy()], set1 + set2) is true
minterms = [[0, 0, 0, 1], [0, 0, 1, 1], [0, 1, 1, 1], [1, 0, 1, 1],
[1, 1, 1, 1]]
dontcares = [[0, 0, 0, 0], [0, 0, 1, 0], [0, 1, 0, 1]]
assert (
SOPform([w, x, y, z], minterms, dontcares) ==
Or(And(Not(w), z), And(y, z)))
assert POSform([w, x, y, z], minterms, dontcares) == And(Or(Not(w), y), z)
minterms = [1, 3, 7, 11, 15]
dontcares = [0, 2, 5]
assert (
SOPform([w, x, y, z], minterms, dontcares) ==
Or(And(Not(w), z), And(y, z)))
assert POSform([w, x, y, z], minterms, dontcares) == And(Or(Not(w), y), z)
minterms = [1, [0, 0, 1, 1], 7, [1, 0, 1, 1],
[1, 1, 1, 1]]
dontcares = [0, [0, 0, 1, 0], 5]
assert (
SOPform([w, x, y, z], minterms, dontcares) ==
Or(And(Not(w), z), And(y, z)))
assert POSform([w, x, y, z], minterms, dontcares) == And(Or(Not(w), y), z)
minterms = [1, {y: 1, z: 1}]
dontcares = [0, [0, 0, 1, 0], 5]
assert (
SOPform([w, x, y, z], minterms, dontcares) ==
Or(And(Not(w), z), And(y, z)))
assert POSform([w, x, y, z], minterms, dontcares) == And(Or(Not(w), y), z)
minterms = [{y: 1, z: 1}, 1]
dontcares = [[0, 0, 0, 0]]
minterms = [[0, 0, 0]]
raises(ValueError, lambda: SOPform([w, x, y, z], minterms))
raises(ValueError, lambda: POSform([w, x, y, z], minterms))
raises(TypeError, lambda: POSform([w, x, y, z], ["abcdefg"]))
# test simplification
ans = And(A, Or(B, C))
assert simplify_logic(A & (B | C)) == ans
assert simplify_logic((A & B) | (A & C)) == ans
assert simplify_logic(Implies(A, B)) == Or(Not(A), B)
assert simplify_logic(Equivalent(A, B)) == \
Or(And(A, B), And(Not(A), Not(B)))
assert simplify_logic(And(Equality(A, 2), C)) == And(Equality(A, 2), C)
assert simplify_logic(And(Equality(A, 2), A)) is S.false
assert simplify_logic(And(Equality(A, 2), A)) == And(Equality(A, 2), A)
assert simplify_logic(And(Equality(A, B), C)) == And(Equality(A, B), C)
assert simplify_logic(Or(And(Equality(A, 3), B), And(Equality(A, 3), C))) \
== And(Equality(A, 3), Or(B, C))
b = (~x & ~y & ~z) | (~x & ~y & z)
e = And(A, b)
assert simplify_logic(e) == A & ~x & ~y
raises(ValueError, lambda: simplify_logic(A & (B | C), form='blabla'))
# Check that expressions with nine variables or more are not simplified
# (without the force-flag)
a, b, c, d, e, f, g, h, j = symbols('a b c d e f g h j')
expr = a & b & c & d & e & f & g & h & j | \
a & b & c & d & e & f & g & h & ~j
# This expression can be simplified to get rid of the j variables
assert simplify_logic(expr) == expr
# check input
ans = SOPform([x, y], [[1, 0]])
assert SOPform([x, y], [[1, 0]]) == ans
assert POSform([x, y], [[1, 0]]) == ans
raises(ValueError, lambda: SOPform([x], [[1]], [[1]]))
assert SOPform([x], [[1]], [[0]]) is true
assert SOPform([x], [[0]], [[1]]) is true
assert SOPform([x], [], []) is false
raises(ValueError, lambda: POSform([x], [[1]], [[1]]))
assert POSform([x], [[1]], [[0]]) is true
assert POSform([x], [[0]], [[1]]) is true
assert POSform([x], [], []) is false
# check working of simplify
assert simplify((A & B) | (A & C)) == And(A, Or(B, C))
assert simplify(And(x, Not(x))) == False
assert simplify(Or(x, Not(x))) == True
assert simplify(And(Eq(x, 0), Eq(x, y))) == And(Eq(x, 0), Eq(y, 0))
assert And(Eq(x - 1, 0), Eq(x, y)).simplify() == And(Eq(x, 1), Eq(y, 1))
assert And(Ne(x - 1, 0), Ne(x, y)).simplify() == And(Ne(x, 1), Ne(x, y))
assert And(Eq(x - 1, 0), Ne(x, y)).simplify() == And(Eq(x, 1), Ne(y, 1))
assert And(Eq(x - 1, 0), Eq(x, z + y), Eq(y + x, 0)).simplify(
) == And(Eq(x, 1), Eq(y, -1), Eq(z, 2))
assert And(Eq(x - 1, 0), Eq(x + 2, 3)).simplify() == Eq(x, 1)
assert And(Ne(x - 1, 0), Ne(x + 2, 3)).simplify() == Ne(x, 1)
assert And(Eq(x - 1, 0), Eq(x + 2, 2)).simplify() == False
assert And(Ne(x - 1, 0), Ne(x + 2, 2)).simplify(
) == And(Ne(x, 1), Ne(x, 0))
def test_bool_map():
"""
Test working of bool_map function.
"""
minterms = [[0, 0, 0, 1], [0, 0, 1, 1], [0, 1, 1, 1], [1, 0, 1, 1],
[1, 1, 1, 1]]
assert bool_map(Not(Not(a)), a) == (a, {a: a})
assert bool_map(SOPform([w, x, y, z], minterms),
POSform([w, x, y, z], minterms)) == \
(And(Or(Not(w), y), Or(Not(x), y), z), {x: x, w: w, z: z, y: y})
assert bool_map(SOPform([x, z, y], [[1, 0, 1]]),
SOPform([a, b, c], [[1, 0, 1]])) != False
function1 = SOPform([x, z, y], [[1, 0, 1], [0, 0, 1]])
function2 = SOPform([a, b, c], [[1, 0, 1], [1, 0, 0]])
assert bool_map(function1, function2) == \
(function1, {y: a, z: b})
assert bool_map(Xor(x, y), ~Xor(x, y)) == False
assert bool_map(And(x, y), Or(x, y)) is None
assert bool_map(And(x, y), And(x, y, z)) is None
# issue 16179
assert bool_map(Xor(x, y, z), ~Xor(x, y, z)) == False
assert bool_map(Xor(a, x, y, z), ~Xor(a, x, y, z)) == False
def test_bool_symbol():
"""Test that mixing symbols with boolean values
works as expected"""
assert And(A, True) == A
assert And(A, True, True) == A
assert And(A, False) is false
assert And(A, True, False) is false
assert Or(A, True) is true
assert Or(A, False) == A
def test_is_boolean():
assert true.is_Boolean
assert (A & B).is_Boolean
assert (A | B).is_Boolean
assert (~A).is_Boolean
assert (A ^ B).is_Boolean
def test_subs():
assert (A & B).subs(A, True) == B
assert (A & B).subs(A, False) is false
assert (A & B).subs(B, True) == A
assert (A & B).subs(B, False) is false
assert (A & B).subs({A: True, B: True}) is true
assert (A | B).subs(A, True) is true
assert (A | B).subs(A, False) == B
assert (A | B).subs(B, True) is true
assert (A | B).subs(B, False) == A
assert (A | B).subs({A: True, B: True}) is true
"""
we test for axioms of boolean algebra
see https://en.wikipedia.org/wiki/Boolean_algebra_(structure)
"""
def test_commutative():
"""Test for commutativity of And and Or"""
A, B = map(Boolean, symbols('A,B'))
assert A & B == B & A
assert A | B == B | A
def test_and_associativity():
"""Test for associativity of And"""
assert (A & B) & C == A & (B & C)
def test_or_assicativity():
assert ((A | B) | C) == (A | (B | C))
def test_double_negation():
a = Boolean()
assert ~(~a) == a
# test methods
def test_eliminate_implications():
assert eliminate_implications(Implies(A, B, evaluate=False)) == (~A) | B
assert eliminate_implications(
A >> (C >> Not(B))) == Or(Or(Not(B), Not(C)), Not(A))
assert eliminate_implications(Equivalent(A, B, C, D)) == \
(~A | B) & (~B | C) & (~C | D) & (~D | A)
def test_conjuncts():
assert conjuncts(A & B & C) == {A, B, C}
assert conjuncts((A | B) & C) == {A | B, C}
assert conjuncts(A) == {A}
assert conjuncts(True) == {True}
assert conjuncts(False) == {False}
def test_disjuncts():
assert disjuncts(A | B | C) == {A, B, C}
assert disjuncts((A | B) & C) == {(A | B) & C}
assert disjuncts(A) == {A}
assert disjuncts(True) == {True}
assert disjuncts(False) == {False}
def test_distribute():
assert distribute_and_over_or(Or(And(A, B), C)) == And(Or(A, C), Or(B, C))
assert distribute_or_over_and(And(A, Or(B, C))) == Or(And(A, B), And(A, C))
def test_to_nnf():
assert to_nnf(true) is true
assert to_nnf(false) is false
assert to_nnf(A) == A
assert to_nnf(A | ~A | B) is true
assert to_nnf(A & ~A & B) is false
assert to_nnf(A >> B) == ~A | B
assert to_nnf(Equivalent(A, B, C)) == (~A | B) & (~B | C) & (~C | A)
assert to_nnf(A ^ B ^ C) == \
(A | B | C) & (~A | ~B | C) & (A | ~B | ~C) & (~A | B | ~C)
assert to_nnf(ITE(A, B, C)) == (~A | B) & (A | C)
assert to_nnf(Not(A | B | C)) == ~A & ~B & ~C
assert to_nnf(Not(A & B & C)) == ~A | ~B | ~C
assert to_nnf(Not(A >> B)) == A & ~B
assert to_nnf(Not(Equivalent(A, B, C))) == And(Or(A, B, C), Or(~A, ~B, ~C))
assert to_nnf(Not(A ^ B ^ C)) == \
(~A | B | C) & (A | ~B | C) & (A | B | ~C) & (~A | ~B | ~C)
assert to_nnf(Not(ITE(A, B, C))) == (~A | ~B) & (A | ~C)
assert to_nnf((A >> B) ^ (B >> A)) == (A & ~B) | (~A & B)
assert to_nnf((A >> B) ^ (B >> A), False) == \
(~A | ~B | A | B) & ((A & ~B) | (~A & B))
assert ITE(A, 1, 0).to_nnf() == A
assert ITE(A, 0, 1).to_nnf() == ~A
# although ITE can hold non-Boolean, it will complain if
# an attempt is made to convert the ITE to Boolean nnf
raises(TypeError, lambda: ITE(A < 1, [1], B).to_nnf())
def test_to_cnf():
assert to_cnf(~(B | C)) == And(Not(B), Not(C))
assert to_cnf((A & B) | C) == And(Or(A, C), Or(B, C))
assert to_cnf(A >> B) == (~A) | B
assert to_cnf(A >> (B & C)) == (~A | B) & (~A | C)
assert to_cnf(A & (B | C) | ~A & (B | C), True) == B | C
assert to_cnf(A & B) == And(A, B)
assert to_cnf(Equivalent(A, B)) == And(Or(A, Not(B)), Or(B, Not(A)))
assert to_cnf(Equivalent(A, B & C)) == \
(~A | B) & (~A | C) & (~B | ~C | A)
assert to_cnf(Equivalent(A, B | C), True) == \
And(Or(Not(B), A), Or(Not(C), A), Or(B, C, Not(A)))
assert to_cnf(A + 1) == A + 1
def test_to_CNF():
assert CNF.CNF_to_cnf(CNF.to_CNF(~(B | C))) == to_cnf(~(B | C))
assert CNF.CNF_to_cnf(CNF.to_CNF((A & B) | C)) == to_cnf((A & B) | C)
assert CNF.CNF_to_cnf(CNF.to_CNF(A >> B)) == to_cnf(A >> B)
assert CNF.CNF_to_cnf(CNF.to_CNF(A >> (B & C))) == to_cnf(A >> (B & C))
assert CNF.CNF_to_cnf(CNF.to_CNF(A & (B | C) | ~A & (B | C))) == to_cnf(A & (B | C) | ~A & (B | C))
assert CNF.CNF_to_cnf(CNF.to_CNF(A & B)) == to_cnf(A & B)
def test_to_dnf():
assert to_dnf(~(B | C)) == And(Not(B), Not(C))
assert to_dnf(A & (B | C)) == Or(And(A, B), And(A, C))
assert to_dnf(A >> B) == (~A) | B
assert to_dnf(A >> (B & C)) == (~A) | (B & C)
assert to_dnf(A | B) == A | B
assert to_dnf(Equivalent(A, B), True) == \
Or(And(A, B), And(Not(A), Not(B)))
assert to_dnf(Equivalent(A, B & C), True) == \
Or(And(A, B, C), And(Not(A), Not(B)), And(Not(A), Not(C)))
assert to_dnf(A + 1) == A + 1
def test_to_int_repr():
x, y, z = map(Boolean, symbols('x,y,z'))
def sorted_recursive(arg):
try:
return sorted(sorted_recursive(x) for x in arg)
except TypeError: # arg is not a sequence
return arg
assert sorted_recursive(to_int_repr([x | y, z | x], [x, y, z])) == \
sorted_recursive([[1, 2], [1, 3]])
assert sorted_recursive(to_int_repr([x | y, z | ~x], [x, y, z])) == \
sorted_recursive([[1, 2], [3, -1]])
def test_is_nnf():
assert is_nnf(true) is True
assert is_nnf(A) is True
assert is_nnf(~A) is True
assert is_nnf(A & B) is True
assert is_nnf((A & B) | (~A & A) | (~B & B) | (~A & ~B), False) is True
assert is_nnf((A | B) & (~A | ~B)) is True
assert is_nnf(Not(Or(A, B))) is False
assert is_nnf(A ^ B) is False
assert is_nnf((A & B) | (~A & A) | (~B & B) | (~A & ~B), True) is False
def test_is_cnf():
assert is_cnf(x) is True
assert is_cnf(x | y | z) is True
assert is_cnf(x & y & z) is True
assert is_cnf((x | y) & z) is True
assert is_cnf((x & y) | z) is False
assert is_cnf(~(x & y) | z) is False
def test_is_dnf():
assert is_dnf(x) is True
assert is_dnf(x | y | z) is True
assert is_dnf(x & y & z) is True
assert is_dnf((x & y) | z) is True
assert is_dnf((x | y) & z) is False
assert is_dnf(~(x | y) & z) is False
def test_ITE():
A, B, C = symbols('A:C')
assert ITE(True, False, True) is false
assert ITE(True, True, False) is true
assert ITE(False, True, False) is false
assert ITE(False, False, True) is true
assert isinstance(ITE(A, B, C), ITE)
A = True
assert ITE(A, B, C) == B
A = False
assert ITE(A, B, C) == C
B = True
assert ITE(And(A, B), B, C) == C
assert ITE(Or(A, False), And(B, True), False) is false
assert ITE(x, A, B) == Not(x)
assert ITE(x, B, A) == x
assert ITE(1, x, y) == x
assert ITE(0, x, y) == y
raises(TypeError, lambda: ITE(2, x, y))
raises(TypeError, lambda: ITE(1, [], y))
raises(TypeError, lambda: ITE(1, (), y))
raises(TypeError, lambda: ITE(1, y, []))
assert ITE(1, 1, 1) is S.true
assert isinstance(ITE(1, 1, 1, evaluate=False), ITE)
raises(TypeError, lambda: ITE(x > 1, y, x))
assert ITE(Eq(x, True), y, x) == ITE(x, y, x)
assert ITE(Eq(x, False), y, x) == ITE(~x, y, x)
assert ITE(Ne(x, True), y, x) == ITE(~x, y, x)
assert ITE(Ne(x, False), y, x) == ITE(x, y, x)
assert ITE(Eq(S. true, x), y, x) == ITE(x, y, x)
assert ITE(Eq(S.false, x), y, x) == ITE(~x, y, x)
assert ITE(Ne(S.true, x), y, x) == ITE(~x, y, x)
assert ITE(Ne(S.false, x), y, x) == ITE(x, y, x)
# 0 and 1 in the context are not treated as True/False
# so the equality must always be False since dissimilar
# objects cannot be equal
assert ITE(Eq(x, 0), y, x) == x
assert ITE(Eq(x, 1), y, x) == x
assert ITE(Ne(x, 0), y, x) == y
assert ITE(Ne(x, 1), y, x) == y
assert ITE(Eq(x, 0), y, z).subs(x, 0) == y
assert ITE(Eq(x, 0), y, z).subs(x, 1) == z
raises(ValueError, lambda: ITE(x > 1, y, x, z))
def test_is_literal():
assert is_literal(True) is True
assert is_literal(False) is True
assert is_literal(A) is True
assert is_literal(~A) is True
assert is_literal(Or(A, B)) is False
assert is_literal(Q.zero(A)) is True
assert is_literal(Not(Q.zero(A))) is True
assert is_literal(Or(A, B)) is False
assert is_literal(And(Q.zero(A), Q.zero(B))) is False
def test_operators():
# Mostly test __and__, __rand__, and so on
assert True & A == A & True == A
assert False & A == A & False == False
assert A & B == And(A, B)
assert True | A == A | True == True
assert False | A == A | False == A
assert A | B == Or(A, B)
assert ~A == Not(A)
assert True >> A == A << True == A
assert False >> A == A << False == True
assert A >> True == True << A == True
assert A >> False == False << A == ~A
assert A >> B == B << A == Implies(A, B)
assert True ^ A == A ^ True == ~A
assert False ^ A == A ^ False == A
assert A ^ B == Xor(A, B)
def test_true_false():
assert true is S.true
assert false is S.false
assert true is not True
assert false is not False
assert true
assert not false
assert true == True
assert false == False
assert not (true == False)
assert not (false == True)
assert not (true == false)
assert hash(true) == hash(True)
assert hash(false) == hash(False)
assert len({true, True}) == len({false, False}) == 1
assert isinstance(true, BooleanAtom)
assert isinstance(false, BooleanAtom)
# We don't want to subclass from bool, because bool subclasses from
# int. But operators like &, |, ^, <<, >>, and ~ act differently on 0 and
# 1 then we want them to on true and false. See the docstrings of the
# various And, Or, etc. functions for examples.
assert not isinstance(true, bool)
assert not isinstance(false, bool)
# Note: using 'is' comparison is important here. We want these to return
# true and false, not True and False
assert Not(true) is false
assert Not(True) is false
assert Not(false) is true
assert Not(False) is true
assert ~true is false
assert ~false is true
for T, F in cartes([True, true], [False, false]):
assert And(T, F) is false
assert And(F, T) is false
assert And(F, F) is false
assert And(T, T) is true
assert And(T, x) == x
assert And(F, x) is false
if not (T is True and F is False):
assert T & F is false
assert F & T is false
if F is not False:
assert F & F is false
if T is not True:
assert T & T is true
assert Or(T, F) is true
assert Or(F, T) is true
assert Or(F, F) is false
assert Or(T, T) is true
assert Or(T, x) is true
assert Or(F, x) == x
if not (T is True and F is False):
assert T | F is true
assert F | T is true
if F is not False:
assert F | F is false
if T is not True:
assert T | T is true
assert Xor(T, F) is true
assert Xor(F, T) is true
assert Xor(F, F) is false
assert Xor(T, T) is false
assert Xor(T, x) == ~x
assert Xor(F, x) == x
if not (T is True and F is False):
assert T ^ F is true
assert F ^ T is true
if F is not False:
assert F ^ F is false
if T is not True:
assert T ^ T is false
assert Nand(T, F) is true
assert Nand(F, T) is true
assert Nand(F, F) is true
assert Nand(T, T) is false
assert Nand(T, x) == ~x
assert Nand(F, x) is true
assert Nor(T, F) is false
assert Nor(F, T) is false
assert Nor(F, F) is true
assert Nor(T, T) is false
assert Nor(T, x) is false
assert Nor(F, x) == ~x
assert Implies(T, F) is false
assert Implies(F, T) is true
assert Implies(F, F) is true
assert Implies(T, T) is true
assert Implies(T, x) == x
assert Implies(F, x) is true
assert Implies(x, T) is true
assert Implies(x, F) == ~x
if not (T is True and F is False):
assert T >> F is false
assert F << T is false
assert F >> T is true
assert T << F is true
if F is not False:
assert F >> F is true
assert F << F is true
if T is not True:
assert T >> T is true
assert T << T is true
assert Equivalent(T, F) is false
assert Equivalent(F, T) is false
assert Equivalent(F, F) is true
assert Equivalent(T, T) is true
assert Equivalent(T, x) == x
assert Equivalent(F, x) == ~x
assert Equivalent(x, T) == x
assert Equivalent(x, F) == ~x
assert ITE(T, T, T) is true
assert ITE(T, T, F) is true
assert ITE(T, F, T) is false
assert ITE(T, F, F) is false
assert ITE(F, T, T) is true
assert ITE(F, T, F) is false
assert ITE(F, F, T) is true
assert ITE(F, F, F) is false
assert all(i.simplify(1, 2) is i for i in (S.true, S.false))
def test_bool_as_set():
assert ITE(y <= 0, False, y >= 1).as_set() == Interval(1, oo)
assert And(x <= 2, x >= -2).as_set() == Interval(-2, 2)
assert Or(x >= 2, x <= -2).as_set() == Interval(-oo, -2) + Interval(2, oo)
assert Not(x > 2).as_set() == Interval(-oo, 2)
# issue 10240
assert Not(And(x > 2, x < 3)).as_set() == \
Union(Interval(-oo, 2), Interval(3, oo))
assert true.as_set() == S.UniversalSet
assert false.as_set() == EmptySet()
assert x.as_set() == S.UniversalSet
assert And(Or(x < 1, x > 3), x < 2).as_set() == Interval.open(-oo, 1)
assert And(x < 1, sin(x) < 3).as_set() == (x < 1).as_set()
raises(NotImplementedError, lambda: (sin(x) < 1).as_set())
@XFAIL
def test_multivariate_bool_as_set():
x, y = symbols('x,y')
assert And(x >= 0, y >= 0).as_set() == Interval(0, oo)*Interval(0, oo)
assert Or(x >= 0, y >= 0).as_set() == S.Reals*S.Reals - \
Interval(-oo, 0, True, True)*Interval(-oo, 0, True, True)
def test_all_or_nothing():
x = symbols('x', extended_real=True)
args = x >= -oo, x <= oo
v = And(*args)
if v.func is And:
assert len(v.args) == len(args) - args.count(S.true)
else:
assert v == True
v = Or(*args)
if v.func is Or:
assert len(v.args) == 2
else:
assert v == True
def test_canonical_atoms():
assert true.canonical == true
assert false.canonical == false
def test_negated_atoms():
assert true.negated == false
assert false.negated == true
def test_issue_8777():
assert And(x > 2, x < oo).as_set() == Interval(2, oo, left_open=True)
assert And(x >= 1, x < oo).as_set() == Interval(1, oo)
assert (x < oo).as_set() == Interval(-oo, oo)
assert (x > -oo).as_set() == Interval(-oo, oo)
def test_issue_8975():
assert Or(And(-oo < x, x <= -2), And(2 <= x, x < oo)).as_set() == \
Interval(-oo, -2) + Interval(2, oo)
def test_term_to_integer():
assert term_to_integer([1, 0, 1, 0, 0, 1, 0]) == 82
assert term_to_integer('0010101000111001') == 10809
def test_integer_to_term():
assert integer_to_term(777) == [1, 1, 0, 0, 0, 0, 1, 0, 0, 1]
assert integer_to_term(123, 3) == [1, 1, 1, 1, 0, 1, 1]
assert integer_to_term(456, 16) == [0, 0, 0, 0, 0, 0, 0, 1,
1, 1, 0, 0, 1, 0, 0, 0]
def test_truth_table():
assert list(truth_table(And(x, y), [x, y], input=False)) == \
[False, False, False, True]
assert list(truth_table(x | y, [x, y], input=False)) == \
[False, True, True, True]
assert list(truth_table(x >> y, [x, y], input=False)) == \
[True, True, False, True]
assert list(truth_table(And(x, y), [x, y])) == \
[([0, 0], False), ([0, 1], False), ([1, 0], False), ([1, 1], True)]
def test_issue_8571():
for t in (S.true, S.false):
raises(TypeError, lambda: +t)
raises(TypeError, lambda: -t)
raises(TypeError, lambda: abs(t))
# use int(bool(t)) to get 0 or 1
raises(TypeError, lambda: int(t))
for o in [S.Zero, S.One, x]:
for _ in range(2):
raises(TypeError, lambda: o + t)
raises(TypeError, lambda: o - t)
raises(TypeError, lambda: o % t)
raises(TypeError, lambda: o*t)
raises(TypeError, lambda: o/t)
raises(TypeError, lambda: o**t)
o, t = t, o # do again in reversed order
def test_expand_relational():
n = symbols('n', negative=True)
p, q = symbols('p q', positive=True)
r = ((n + q*(-n/q + 1))/(q*(-n/q + 1)) < 0)
assert r is not S.false
assert r.expand() is S.false
assert (q > 0).expand() is S.true
def test_issue_12717():
assert S.true.is_Atom == True
assert S.false.is_Atom == True
def test_as_Boolean():
nz = symbols('nz', nonzero=True)
assert all(as_Boolean(i) is S.true for i in (True, S.true, 1, nz))
z = symbols('z', zero=True)
assert all(as_Boolean(i) is S.false for i in (False, S.false, 0, z))
assert all(as_Boolean(i) == i for i in (x, x < 0))
for i in (2, S(2), x + 1, []):
raises(TypeError, lambda: as_Boolean(i))
def test_binary_symbols():
assert ITE(x < 1, y, z).binary_symbols == set((y, z))
for f in (Eq, Ne):
assert f(x, 1).binary_symbols == set()
assert f(x, True).binary_symbols == set([x])
assert f(x, False).binary_symbols == set([x])
assert S.true.binary_symbols == set()
assert S.false.binary_symbols == set()
assert x.binary_symbols == set([x])
assert And(x, Eq(y, False), Eq(z, 1)).binary_symbols == set([x, y])
assert Q.prime(x).binary_symbols == set()
assert Q.is_true(x < 1).binary_symbols == set()
assert Q.is_true(x).binary_symbols == set([x])
assert Q.is_true(Eq(x, True)).binary_symbols == set([x])
assert Q.prime(x).binary_symbols == set()
def test_BooleanFunction_diff():
assert And(x, y).diff(x) == Piecewise((0, Eq(y, False)), (1, True))
def test_issue_14700():
A, B, C, D, E, F, G, H = symbols('A B C D E F G H')
q = ((B & D & H & ~F) | (B & H & ~C & ~D) | (B & H & ~C & ~F) |
(B & H & ~D & ~G) | (B & H & ~F & ~G) | (C & G & ~B & ~D) |
(C & G & ~D & ~H) | (C & G & ~F & ~H) | (D & F & H & ~B) |
(D & F & ~G & ~H) | (B & D & F & ~C & ~H) | (D & E & F & ~B & ~C) |
(D & F & ~A & ~B & ~C) | (D & F & ~A & ~C & ~H) |
(A & B & D & F & ~E & ~H))
soldnf = ((B & D & H & ~F) | (D & F & H & ~B) | (B & H & ~C & ~D) |
(B & H & ~D & ~G) | (C & G & ~B & ~D) | (C & G & ~D & ~H) |
(C & G & ~F & ~H) | (D & F & ~G & ~H) | (D & E & F & ~C & ~H) |
(D & F & ~A & ~C & ~H) | (A & B & D & F & ~E & ~H))
solcnf = ((B | C | D) & (B | D | G) & (C | D | H) & (C | F | H) &
(D | G | H) & (F | G | H) & (B | F | ~D | ~H) &
(~B | ~D | ~F | ~H) & (D | ~B | ~C | ~G | ~H) &
(A | H | ~C | ~D | ~F | ~G) & (H | ~C | ~D | ~E | ~F | ~G) &
(B | E | H | ~A | ~D | ~F | ~G))
assert simplify_logic(q, "dnf") == soldnf
assert simplify_logic(q, "cnf") == solcnf
minterms = [[0, 1, 0, 0], [0, 1, 0, 1], [0, 1, 1, 0], [0, 1, 1, 1],
[0, 0, 1, 1], [1, 0, 1, 1]]
dontcares = [[1, 0, 0, 0], [1, 0, 0, 1], [1, 1, 0, 0], [1, 1, 0, 1]]
assert SOPform([w, x, y, z], minterms) == (x & ~w) | (y & z & ~x)
# Should not be more complicated with don't cares
assert SOPform([w, x, y, z], minterms, dontcares) == \
(x & ~w) | (y & z & ~x)
def test_relational_simplification():
w, x, y, z = symbols('w x y z', real=True)
d, e = symbols('d e', real=False)
# Test all combinations or sign and order
assert Or(x >= y, x < y).simplify() == S.true
assert Or(x >= y, y > x).simplify() == S.true
assert Or(x >= y, -x > -y).simplify() == S.true
assert Or(x >= y, -y < -x).simplify() == S.true
assert Or(-x <= -y, x < y).simplify() == S.true
assert Or(-x <= -y, -x > -y).simplify() == S.true
assert Or(-x <= -y, y > x).simplify() == S.true
assert Or(-x <= -y, -y < -x).simplify() == S.true
assert Or(y <= x, x < y).simplify() == S.true
assert Or(y <= x, y > x).simplify() == S.true
assert Or(y <= x, -x > -y).simplify() == S.true
assert Or(y <= x, -y < -x).simplify() == S.true
assert Or(-y >= -x, x < y).simplify() == S.true
assert Or(-y >= -x, y > x).simplify() == S.true
assert Or(-y >= -x, -x > -y).simplify() == S.true
assert Or(-y >= -x, -y < -x).simplify() == S.true
assert Or(x < y, x >= y).simplify() == S.true
assert Or(y > x, x >= y).simplify() == S.true
assert Or(-x > -y, x >= y).simplify() == S.true
assert Or(-y < -x, x >= y).simplify() == S.true
assert Or(x < y, -x <= -y).simplify() == S.true
assert Or(-x > -y, -x <= -y).simplify() == S.true
assert Or(y > x, -x <= -y).simplify() == S.true
assert Or(-y < -x, -x <= -y).simplify() == S.true
assert Or(x < y, y <= x).simplify() == S.true
assert Or(y > x, y <= x).simplify() == S.true
assert Or(-x > -y, y <= x).simplify() == S.true
assert Or(-y < -x, y <= x).simplify() == S.true
assert Or(x < y, -y >= -x).simplify() == S.true
assert Or(y > x, -y >= -x).simplify() == S.true
assert Or(-x > -y, -y >= -x).simplify() == S.true
assert Or(-y < -x, -y >= -x).simplify() == S.true
# Some other tests
assert Or(x >= y, w < z, x <= y).simplify() == S.true
assert And(x >= y, x < y).simplify() == S.false
assert Or(x >= y, Eq(y, x)).simplify() == (x >= y)
assert And(x >= y, Eq(y, x)).simplify() == Eq(x, y)
assert Or(Eq(x, y), x >= y, w < y, z < y).simplify() == \
Or(x >= y, y > Min(w, z))
assert And(Eq(x, y), x >= y, w < y, y >= z, z < y).simplify() == \
And(Eq(x, y), y > Max(w, z))
assert Or(Eq(x, y), x >= 1, 2 < y, y >= 5, z < y).simplify() == \
(Eq(x, y) | (x >= 1) | (y > Min(2, z)))
assert And(Eq(x, y), x >= 1, 2 < y, y >= 5, z < y).simplify() == \
(Eq(x, y) & (x >= 1) & (y >= 5) & (y > z))
assert (Eq(x, y) & Eq(d, e) & (x >= y) & (d >= e)).simplify() == \
(Eq(x, y) & Eq(d, e) & (d >= e))
assert And(Eq(x, y), Eq(x, -y)).simplify() == And(Eq(x, 0), Eq(y, 0))
assert Xor(x >= y, x <= y).simplify() == Ne(x, y)
@slow
def test_relational_simplification_numerically():
def test_simplification_numerically_function(original, simplified):
symb = original.free_symbols
n = len(symb)
valuelist = list(set(list(combinations(list(range(-(n-1), n))*n, n))))
for values in valuelist:
sublist = dict(zip(symb, values))
originalvalue = original.subs(sublist)
simplifiedvalue = simplified.subs(sublist)
assert originalvalue == simplifiedvalue, "Original: {}\nand"\
" simplified: {}\ndo not evaluate to the same value for {}"\
"".format(original, simplified, sublist)
w, x, y, z = symbols('w x y z', real=True)
d, e = symbols('d e', real=False)
expressions = (And(Eq(x, y), x >= y, w < y, y >= z, z < y),
And(Eq(x, y), x >= 1, 2 < y, y >= 5, z < y),
Or(Eq(x, y), x >= 1, 2 < y, y >= 5, z < y),
And(x >= y, Eq(y, x)),
Or(And(Eq(x, y), x >= y, w < y, Or(y >= z, z < y)),
And(Eq(x, y), x >= 1, 2 < y, y >= -1, z < y)),
(Eq(x, y) & Eq(d, e) & (x >= y) & (d >= e)),
)
for expression in expressions:
test_simplification_numerically_function(expression,
expression.simplify())
def test_relational_simplification_patterns_numerically():
from sympy.core import Wild
from sympy.logic.boolalg import simplify_patterns_and, \
simplify_patterns_or, simplify_patterns_xor
a = Wild('a')
b = Wild('b')
c = Wild('c')
symb = [a, b, c]
patternlists = [simplify_patterns_and(), simplify_patterns_or(),
simplify_patterns_xor()]
for patternlist in patternlists:
for pattern in patternlist:
original = pattern[0]
simplified = pattern[1]
valuelist = list(set(list(combinations(list(range(-2, 2))*3, 3))))
for values in valuelist:
sublist = dict(zip(symb, values))
originalvalue = original.subs(sublist)
simplifiedvalue = simplified.subs(sublist)
assert originalvalue == simplifiedvalue, "Original: {}\nand"\
" simplified: {}\ndo not evaluate to the same value for"\
"{}".format(original, simplified, sublist)
def test_issue_16803():
n = symbols('n')
# No simplification done, but should not raise an exception
assert ((n > 3) | (n < 0) | ((n > 0) & (n < 3))).simplify() == \
((n > 3) | (n < 0) | ((n > 0) & (n < 3)))
def test_issue_17530():
r = {x: oo, y: oo}
assert Or(x + y > 0, x - y < 0).subs(r)
assert not And(x + y < 0, x - y < 0).subs(r)
raises(TypeError, lambda: Or(x + y < 0, x - y < 0).subs(r))
raises(TypeError, lambda: And(x + y > 0, x - y < 0).subs(r))
raises(TypeError, lambda: And(x + y > 0, x - y < 0).subs(r))
|
78ab1fa700515bd689c9772efa3bbc7016b0c001ea5e11a985affbf5d265bae3 | from sympy.assumptions import Q
from sympy.core.add import Add
from sympy.core.compatibility import range
from sympy.core.function import Function
from sympy.core.numbers import (Float, I, Integer, oo, pi)
from sympy.core.singleton import S
from sympy.core.symbol import (Symbol, symbols)
from sympy.functions.elementary.complexes import Abs
from sympy.functions.elementary.exponential import exp
from sympy.functions.elementary.miscellaneous import sqrt
from sympy.functions.elementary.trigonometric import cos, sin
from sympy.matrices.common import (ShapeError, MatrixError, NonSquareMatrixError,
_MinimalMatrix, MatrixShaping, MatrixProperties, MatrixOperations, MatrixArithmetic,
MatrixSpecial)
from sympy.matrices.matrices import (MatrixDeterminant,
MatrixReductions, MatrixSubspaces, MatrixEigen, MatrixCalculus)
from sympy.matrices import (Matrix, diag, eye,
matrix_multiply_elementwise, ones, zeros, SparseMatrix, banded)
from sympy.polys.polytools import Poly
from sympy.simplify.simplify import simplify
from sympy.utilities.iterables import flatten
from sympy.utilities.pytest import raises, XFAIL, warns_deprecated_sympy
from sympy.abc import x, y, z
# classes to test the basic matrix classes
class ShapingOnlyMatrix(_MinimalMatrix, MatrixShaping):
pass
def eye_Shaping(n):
return ShapingOnlyMatrix(n, n, lambda i, j: int(i == j))
def zeros_Shaping(n):
return ShapingOnlyMatrix(n, n, lambda i, j: 0)
class PropertiesOnlyMatrix(_MinimalMatrix, MatrixProperties):
pass
def eye_Properties(n):
return PropertiesOnlyMatrix(n, n, lambda i, j: int(i == j))
def zeros_Properties(n):
return PropertiesOnlyMatrix(n, n, lambda i, j: 0)
class OperationsOnlyMatrix(_MinimalMatrix, MatrixOperations):
pass
def eye_Operations(n):
return OperationsOnlyMatrix(n, n, lambda i, j: int(i == j))
def zeros_Operations(n):
return OperationsOnlyMatrix(n, n, lambda i, j: 0)
class ArithmeticOnlyMatrix(_MinimalMatrix, MatrixArithmetic):
pass
def eye_Arithmetic(n):
return ArithmeticOnlyMatrix(n, n, lambda i, j: int(i == j))
def zeros_Arithmetic(n):
return ArithmeticOnlyMatrix(n, n, lambda i, j: 0)
class DeterminantOnlyMatrix(_MinimalMatrix, MatrixDeterminant):
pass
def eye_Determinant(n):
return DeterminantOnlyMatrix(n, n, lambda i, j: int(i == j))
def zeros_Determinant(n):
return DeterminantOnlyMatrix(n, n, lambda i, j: 0)
class ReductionsOnlyMatrix(_MinimalMatrix, MatrixReductions):
pass
def eye_Reductions(n):
return ReductionsOnlyMatrix(n, n, lambda i, j: int(i == j))
def zeros_Reductions(n):
return ReductionsOnlyMatrix(n, n, lambda i, j: 0)
class SpecialOnlyMatrix(_MinimalMatrix, MatrixSpecial):
pass
class SubspaceOnlyMatrix(_MinimalMatrix, MatrixSubspaces):
pass
class EigenOnlyMatrix(_MinimalMatrix, MatrixEigen):
pass
class CalculusOnlyMatrix(_MinimalMatrix, MatrixCalculus):
pass
def test__MinimalMatrix():
x = _MinimalMatrix(2, 3, [1, 2, 3, 4, 5, 6])
assert x.rows == 2
assert x.cols == 3
assert x[2] == 3
assert x[1, 1] == 5
assert list(x) == [1, 2, 3, 4, 5, 6]
assert list(x[1, :]) == [4, 5, 6]
assert list(x[:, 1]) == [2, 5]
assert list(x[:, :]) == list(x)
assert x[:, :] == x
assert _MinimalMatrix(x) == x
assert _MinimalMatrix([[1, 2, 3], [4, 5, 6]]) == x
assert _MinimalMatrix(([1, 2, 3], [4, 5, 6])) == x
assert _MinimalMatrix([(1, 2, 3), (4, 5, 6)]) == x
assert _MinimalMatrix(((1, 2, 3), (4, 5, 6))) == x
assert not (_MinimalMatrix([[1, 2], [3, 4], [5, 6]]) == x)
# ShapingOnlyMatrix tests
def test_vec():
m = ShapingOnlyMatrix(2, 2, [1, 3, 2, 4])
m_vec = m.vec()
assert m_vec.cols == 1
for i in range(4):
assert m_vec[i] == i + 1
def test_tolist():
lst = [[S.One, S.Half, x*y, S.Zero], [x, y, z, x**2], [y, -S.One, z*x, 3]]
flat_lst = [S.One, S.Half, x*y, S.Zero, x, y, z, x**2, y, -S.One, z*x, 3]
m = ShapingOnlyMatrix(3, 4, flat_lst)
assert m.tolist() == lst
def test_row_col_del():
e = ShapingOnlyMatrix(3, 3, [1, 2, 3, 4, 5, 6, 7, 8, 9])
raises(ValueError, lambda: e.row_del(5))
raises(ValueError, lambda: e.row_del(-5))
raises(ValueError, lambda: e.col_del(5))
raises(ValueError, lambda: e.col_del(-5))
assert e.row_del(2) == e.row_del(-1) == Matrix([[1, 2, 3], [4, 5, 6]])
assert e.col_del(2) == e.col_del(-1) == Matrix([[1, 2], [4, 5], [7, 8]])
assert e.row_del(1) == e.row_del(-2) == Matrix([[1, 2, 3], [7, 8, 9]])
assert e.col_del(1) == e.col_del(-2) == Matrix([[1, 3], [4, 6], [7, 9]])
def test_get_diag_blocks1():
a = Matrix([[1, 2], [2, 3]])
b = Matrix([[3, x], [y, 3]])
c = Matrix([[3, x, 3], [y, 3, z], [x, y, z]])
assert a.get_diag_blocks() == [a]
assert b.get_diag_blocks() == [b]
assert c.get_diag_blocks() == [c]
def test_get_diag_blocks2():
a = Matrix([[1, 2], [2, 3]])
b = Matrix([[3, x], [y, 3]])
c = Matrix([[3, x, 3], [y, 3, z], [x, y, z]])
A, B, C, D = diag(a, b, b), diag(a, b, c), diag(a, c, b), diag(c, c, b)
A = ShapingOnlyMatrix(A.rows, A.cols, A)
B = ShapingOnlyMatrix(B.rows, B.cols, B)
C = ShapingOnlyMatrix(C.rows, C.cols, C)
D = ShapingOnlyMatrix(D.rows, D.cols, D)
assert A.get_diag_blocks() == [a, b, b]
assert B.get_diag_blocks() == [a, b, c]
assert C.get_diag_blocks() == [a, c, b]
assert D.get_diag_blocks() == [c, c, b]
def test_shape():
m = ShapingOnlyMatrix(1, 2, [0, 0])
m.shape == (1, 2)
def test_reshape():
m0 = eye_Shaping(3)
assert m0.reshape(1, 9) == Matrix(1, 9, (1, 0, 0, 0, 1, 0, 0, 0, 1))
m1 = ShapingOnlyMatrix(3, 4, lambda i, j: i + j)
assert m1.reshape(
4, 3) == Matrix(((0, 1, 2), (3, 1, 2), (3, 4, 2), (3, 4, 5)))
assert m1.reshape(2, 6) == Matrix(((0, 1, 2, 3, 1, 2), (3, 4, 2, 3, 4, 5)))
def test_row_col():
m = ShapingOnlyMatrix(3, 3, [1, 2, 3, 4, 5, 6, 7, 8, 9])
assert m.row(0) == Matrix(1, 3, [1, 2, 3])
assert m.col(0) == Matrix(3, 1, [1, 4, 7])
def test_row_join():
assert eye_Shaping(3).row_join(Matrix([7, 7, 7])) == \
Matrix([[1, 0, 0, 7],
[0, 1, 0, 7],
[0, 0, 1, 7]])
def test_col_join():
assert eye_Shaping(3).col_join(Matrix([[7, 7, 7]])) == \
Matrix([[1, 0, 0],
[0, 1, 0],
[0, 0, 1],
[7, 7, 7]])
def test_row_insert():
r4 = Matrix([[4, 4, 4]])
for i in range(-4, 5):
l = [1, 0, 0]
l.insert(i, 4)
assert flatten(eye_Shaping(3).row_insert(i, r4).col(0).tolist()) == l
def test_col_insert():
c4 = Matrix([4, 4, 4])
for i in range(-4, 5):
l = [0, 0, 0]
l.insert(i, 4)
assert flatten(zeros_Shaping(3).col_insert(i, c4).row(0).tolist()) == l
# issue 13643
assert eye_Shaping(6).col_insert(3, Matrix([[2, 2], [2, 2], [2, 2], [2, 2], [2, 2], [2, 2]])) == \
Matrix([[1, 0, 0, 2, 2, 0, 0, 0],
[0, 1, 0, 2, 2, 0, 0, 0],
[0, 0, 1, 2, 2, 0, 0, 0],
[0, 0, 0, 2, 2, 1, 0, 0],
[0, 0, 0, 2, 2, 0, 1, 0],
[0, 0, 0, 2, 2, 0, 0, 1]])
def test_extract():
m = ShapingOnlyMatrix(4, 3, lambda i, j: i*3 + j)
assert m.extract([0, 1, 3], [0, 1]) == Matrix(3, 2, [0, 1, 3, 4, 9, 10])
assert m.extract([0, 3], [0, 0, 2]) == Matrix(2, 3, [0, 0, 2, 9, 9, 11])
assert m.extract(range(4), range(3)) == m
raises(IndexError, lambda: m.extract([4], [0]))
raises(IndexError, lambda: m.extract([0], [3]))
def test_hstack():
m = ShapingOnlyMatrix(4, 3, lambda i, j: i*3 + j)
m2 = ShapingOnlyMatrix(3, 4, lambda i, j: i*3 + j)
assert m == m.hstack(m)
assert m.hstack(m, m, m) == ShapingOnlyMatrix.hstack(m, m, m) == Matrix([
[0, 1, 2, 0, 1, 2, 0, 1, 2],
[3, 4, 5, 3, 4, 5, 3, 4, 5],
[6, 7, 8, 6, 7, 8, 6, 7, 8],
[9, 10, 11, 9, 10, 11, 9, 10, 11]])
raises(ShapeError, lambda: m.hstack(m, m2))
assert Matrix.hstack() == Matrix()
# test regression #12938
M1 = Matrix.zeros(0, 0)
M2 = Matrix.zeros(0, 1)
M3 = Matrix.zeros(0, 2)
M4 = Matrix.zeros(0, 3)
m = ShapingOnlyMatrix.hstack(M1, M2, M3, M4)
assert m.rows == 0 and m.cols == 6
def test_vstack():
m = ShapingOnlyMatrix(4, 3, lambda i, j: i*3 + j)
m2 = ShapingOnlyMatrix(3, 4, lambda i, j: i*3 + j)
assert m == m.vstack(m)
assert m.vstack(m, m, m) == ShapingOnlyMatrix.vstack(m, m, m) == Matrix([
[0, 1, 2],
[3, 4, 5],
[6, 7, 8],
[9, 10, 11],
[0, 1, 2],
[3, 4, 5],
[6, 7, 8],
[9, 10, 11],
[0, 1, 2],
[3, 4, 5],
[6, 7, 8],
[9, 10, 11]])
raises(ShapeError, lambda: m.vstack(m, m2))
assert Matrix.vstack() == Matrix()
# PropertiesOnlyMatrix tests
def test_atoms():
m = PropertiesOnlyMatrix(2, 2, [1, 2, x, 1 - 1/x])
assert m.atoms() == {S(1), S(2), S(-1), x}
assert m.atoms(Symbol) == {x}
def test_free_symbols():
assert PropertiesOnlyMatrix([[x], [0]]).free_symbols == {x}
def test_has():
A = PropertiesOnlyMatrix(((x, y), (2, 3)))
assert A.has(x)
assert not A.has(z)
assert A.has(Symbol)
A = PropertiesOnlyMatrix(((2, y), (2, 3)))
assert not A.has(x)
def test_is_anti_symmetric():
x = symbols('x')
assert PropertiesOnlyMatrix(2, 1, [1, 2]).is_anti_symmetric() is False
m = PropertiesOnlyMatrix(3, 3, [0, x**2 + 2*x + 1, y, -(x + 1)**2, 0, x*y, -y, -x*y, 0])
assert m.is_anti_symmetric() is True
assert m.is_anti_symmetric(simplify=False) is False
assert m.is_anti_symmetric(simplify=lambda x: x) is False
m = PropertiesOnlyMatrix(3, 3, [x.expand() for x in m])
assert m.is_anti_symmetric(simplify=False) is True
m = PropertiesOnlyMatrix(3, 3, [x.expand() for x in [S.One] + list(m)[1:]])
assert m.is_anti_symmetric() is False
def test_diagonal_symmetrical():
m = PropertiesOnlyMatrix(2, 2, [0, 1, 1, 0])
assert not m.is_diagonal()
assert m.is_symmetric()
assert m.is_symmetric(simplify=False)
m = PropertiesOnlyMatrix(2, 2, [1, 0, 0, 1])
assert m.is_diagonal()
m = PropertiesOnlyMatrix(3, 3, diag(1, 2, 3))
assert m.is_diagonal()
assert m.is_symmetric()
m = PropertiesOnlyMatrix(3, 3, [1, 0, 0, 0, 2, 0, 0, 0, 3])
assert m == diag(1, 2, 3)
m = PropertiesOnlyMatrix(2, 3, zeros(2, 3))
assert not m.is_symmetric()
assert m.is_diagonal()
m = PropertiesOnlyMatrix(((5, 0), (0, 6), (0, 0)))
assert m.is_diagonal()
m = PropertiesOnlyMatrix(((5, 0, 0), (0, 6, 0)))
assert m.is_diagonal()
m = Matrix(3, 3, [1, x**2 + 2*x + 1, y, (x + 1)**2, 2, 0, y, 0, 3])
assert m.is_symmetric()
assert not m.is_symmetric(simplify=False)
assert m.expand().is_symmetric(simplify=False)
def test_is_hermitian():
a = PropertiesOnlyMatrix([[1, I], [-I, 1]])
assert a.is_hermitian
a = PropertiesOnlyMatrix([[2*I, I], [-I, 1]])
assert a.is_hermitian is False
a = PropertiesOnlyMatrix([[x, I], [-I, 1]])
assert a.is_hermitian is None
a = PropertiesOnlyMatrix([[x, 1], [-I, 1]])
assert a.is_hermitian is False
def test_is_Identity():
assert eye_Properties(3).is_Identity
assert not PropertiesOnlyMatrix(zeros(3)).is_Identity
assert not PropertiesOnlyMatrix(ones(3)).is_Identity
# issue 6242
assert not PropertiesOnlyMatrix([[1, 0, 0]]).is_Identity
def test_is_symbolic():
a = PropertiesOnlyMatrix([[x, x], [x, x]])
assert a.is_symbolic() is True
a = PropertiesOnlyMatrix([[1, 2, 3, 4], [5, 6, 7, 8]])
assert a.is_symbolic() is False
a = PropertiesOnlyMatrix([[1, 2, 3, 4], [5, 6, x, 8]])
assert a.is_symbolic() is True
a = PropertiesOnlyMatrix([[1, x, 3]])
assert a.is_symbolic() is True
a = PropertiesOnlyMatrix([[1, 2, 3]])
assert a.is_symbolic() is False
a = PropertiesOnlyMatrix([[1], [x], [3]])
assert a.is_symbolic() is True
a = PropertiesOnlyMatrix([[1], [2], [3]])
assert a.is_symbolic() is False
def test_is_upper():
a = PropertiesOnlyMatrix([[1, 2, 3]])
assert a.is_upper is True
a = PropertiesOnlyMatrix([[1], [2], [3]])
assert a.is_upper is False
def test_is_lower():
a = PropertiesOnlyMatrix([[1, 2, 3]])
assert a.is_lower is False
a = PropertiesOnlyMatrix([[1], [2], [3]])
assert a.is_lower is True
def test_is_square():
m = PropertiesOnlyMatrix([[1], [1]])
m2 = PropertiesOnlyMatrix([[2, 2], [2, 2]])
assert not m.is_square
assert m2.is_square
def test_is_symmetric():
m = PropertiesOnlyMatrix(2, 2, [0, 1, 1, 0])
assert m.is_symmetric()
m = PropertiesOnlyMatrix(2, 2, [0, 1, 0, 1])
assert not m.is_symmetric()
def test_is_hessenberg():
A = PropertiesOnlyMatrix([[3, 4, 1], [2, 4, 5], [0, 1, 2]])
assert A.is_upper_hessenberg
A = PropertiesOnlyMatrix(3, 3, [3, 2, 0, 4, 4, 1, 1, 5, 2])
assert A.is_lower_hessenberg
A = PropertiesOnlyMatrix(3, 3, [3, 2, -1, 4, 4, 1, 1, 5, 2])
assert A.is_lower_hessenberg is False
assert A.is_upper_hessenberg is False
A = PropertiesOnlyMatrix([[3, 4, 1], [2, 4, 5], [3, 1, 2]])
assert not A.is_upper_hessenberg
def test_is_zero():
assert PropertiesOnlyMatrix(0, 0, []).is_zero
assert PropertiesOnlyMatrix([[0, 0], [0, 0]]).is_zero
assert PropertiesOnlyMatrix(zeros(3, 4)).is_zero
assert not PropertiesOnlyMatrix(eye(3)).is_zero
assert PropertiesOnlyMatrix([[x, 0], [0, 0]]).is_zero == None
assert PropertiesOnlyMatrix([[x, 1], [0, 0]]).is_zero == False
a = Symbol('a', nonzero=True)
assert PropertiesOnlyMatrix([[a, 0], [0, 0]]).is_zero == False
def test_values():
assert set(PropertiesOnlyMatrix(2, 2, [0, 1, 2, 3]
).values()) == set([1, 2, 3])
x = Symbol('x', real=True)
assert set(PropertiesOnlyMatrix(2, 2, [x, 0, 0, 1]
).values()) == set([x, 1])
# OperationsOnlyMatrix tests
def test_applyfunc():
m0 = OperationsOnlyMatrix(eye(3))
assert m0.applyfunc(lambda x: 2*x) == eye(3)*2
assert m0.applyfunc(lambda x: 0) == zeros(3)
assert m0.applyfunc(lambda x: 1) == ones(3)
def test_adjoint():
dat = [[0, I], [1, 0]]
ans = OperationsOnlyMatrix([[0, 1], [-I, 0]])
assert ans.adjoint() == Matrix(dat)
def test_as_real_imag():
m1 = OperationsOnlyMatrix(2, 2, [1, 2, 3, 4])
m3 = OperationsOnlyMatrix(2, 2,
[1 + S.ImaginaryUnit, 2 + 2*S.ImaginaryUnit,
3 + 3*S.ImaginaryUnit, 4 + 4*S.ImaginaryUnit])
a, b = m3.as_real_imag()
assert a == m1
assert b == m1
def test_conjugate():
M = OperationsOnlyMatrix([[0, I, 5],
[1, 2, 0]])
assert M.T == Matrix([[0, 1],
[I, 2],
[5, 0]])
assert M.C == Matrix([[0, -I, 5],
[1, 2, 0]])
assert M.C == M.conjugate()
assert M.H == M.T.C
assert M.H == Matrix([[ 0, 1],
[-I, 2],
[ 5, 0]])
def test_doit():
a = OperationsOnlyMatrix([[Add(x, x, evaluate=False)]])
assert a[0] != 2*x
assert a.doit() == Matrix([[2*x]])
def test_evalf():
a = OperationsOnlyMatrix(2, 1, [sqrt(5), 6])
assert all(a.evalf()[i] == a[i].evalf() for i in range(2))
assert all(a.evalf(2)[i] == a[i].evalf(2) for i in range(2))
assert all(a.n(2)[i] == a[i].n(2) for i in range(2))
def test_expand():
m0 = OperationsOnlyMatrix([[x*(x + y), 2], [((x + y)*y)*x, x*(y + x*(x + y))]])
# Test if expand() returns a matrix
m1 = m0.expand()
assert m1 == Matrix(
[[x*y + x**2, 2], [x*y**2 + y*x**2, x*y + y*x**2 + x**3]])
a = Symbol('a', real=True)
assert OperationsOnlyMatrix(1, 1, [exp(I*a)]).expand(complex=True) == \
Matrix([cos(a) + I*sin(a)])
def test_refine():
m0 = OperationsOnlyMatrix([[Abs(x)**2, sqrt(x**2)],
[sqrt(x**2)*Abs(y)**2, sqrt(y**2)*Abs(x)**2]])
m1 = m0.refine(Q.real(x) & Q.real(y))
assert m1 == Matrix([[x**2, Abs(x)], [y**2*Abs(x), x**2*Abs(y)]])
m1 = m0.refine(Q.positive(x) & Q.positive(y))
assert m1 == Matrix([[x**2, x], [x*y**2, x**2*y]])
m1 = m0.refine(Q.negative(x) & Q.negative(y))
assert m1 == Matrix([[x**2, -x], [-x*y**2, -x**2*y]])
def test_replace():
F, G = symbols('F, G', cls=Function)
K = OperationsOnlyMatrix(2, 2, lambda i, j: G(i+j))
M = OperationsOnlyMatrix(2, 2, lambda i, j: F(i+j))
N = M.replace(F, G)
assert N == K
def test_replace_map():
F, G = symbols('F, G', cls=Function)
K = OperationsOnlyMatrix(2, 2, [(G(0), {F(0): G(0)}), (G(1), {F(1): G(1)}), (G(1), {F(1) \
: G(1)}), (G(2), {F(2): G(2)})])
M = OperationsOnlyMatrix(2, 2, lambda i, j: F(i+j))
N = M.replace(F, G, True)
assert N == K
def test_simplify():
n = Symbol('n')
f = Function('f')
M = OperationsOnlyMatrix([[ 1/x + 1/y, (x + x*y) / x ],
[ (f(x) + y*f(x))/f(x), 2 * (1/n - cos(n * pi)/n) / pi ]])
assert M.simplify() == Matrix([[ (x + y)/(x * y), 1 + y ],
[ 1 + y, 2*((1 - 1*cos(pi*n))/(pi*n)) ]])
eq = (1 + x)**2
M = OperationsOnlyMatrix([[eq]])
assert M.simplify() == Matrix([[eq]])
assert M.simplify(ratio=oo) == Matrix([[eq.simplify(ratio=oo)]])
def test_subs():
assert OperationsOnlyMatrix([[1, x], [x, 4]]).subs(x, 5) == Matrix([[1, 5], [5, 4]])
assert OperationsOnlyMatrix([[x, 2], [x + y, 4]]).subs([[x, -1], [y, -2]]) == \
Matrix([[-1, 2], [-3, 4]])
assert OperationsOnlyMatrix([[x, 2], [x + y, 4]]).subs([(x, -1), (y, -2)]) == \
Matrix([[-1, 2], [-3, 4]])
assert OperationsOnlyMatrix([[x, 2], [x + y, 4]]).subs({x: -1, y: -2}) == \
Matrix([[-1, 2], [-3, 4]])
assert OperationsOnlyMatrix([[x*y]]).subs({x: y - 1, y: x - 1}, simultaneous=True) == \
Matrix([[(x - 1)*(y - 1)]])
def test_trace():
M = OperationsOnlyMatrix([[1, 0, 0],
[0, 5, 0],
[0, 0, 8]])
assert M.trace() == 14
def test_xreplace():
assert OperationsOnlyMatrix([[1, x], [x, 4]]).xreplace({x: 5}) == \
Matrix([[1, 5], [5, 4]])
assert OperationsOnlyMatrix([[x, 2], [x + y, 4]]).xreplace({x: -1, y: -2}) == \
Matrix([[-1, 2], [-3, 4]])
def test_permute():
a = OperationsOnlyMatrix(3, 4, [1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12])
raises(IndexError, lambda: a.permute([[0, 5]]))
b = a.permute_rows([[0, 2], [0, 1]])
assert a.permute([[0, 2], [0, 1]]) == b == Matrix([
[5, 6, 7, 8],
[9, 10, 11, 12],
[1, 2, 3, 4]])
b = a.permute_cols([[0, 2], [0, 1]])
assert a.permute([[0, 2], [0, 1]], orientation='cols') == b ==\
Matrix([
[ 2, 3, 1, 4],
[ 6, 7, 5, 8],
[10, 11, 9, 12]])
b = a.permute_cols([[0, 2], [0, 1]], direction='backward')
assert a.permute([[0, 2], [0, 1]], orientation='cols', direction='backward') == b ==\
Matrix([
[ 3, 1, 2, 4],
[ 7, 5, 6, 8],
[11, 9, 10, 12]])
assert a.permute([1, 2, 0, 3]) == Matrix([
[5, 6, 7, 8],
[9, 10, 11, 12],
[1, 2, 3, 4]])
from sympy.combinatorics import Permutation
assert a.permute(Permutation([1, 2, 0, 3])) == Matrix([
[5, 6, 7, 8],
[9, 10, 11, 12],
[1, 2, 3, 4]])
# ArithmeticOnlyMatrix tests
def test_abs():
m = ArithmeticOnlyMatrix([[1, -2], [x, y]])
assert abs(m) == ArithmeticOnlyMatrix([[1, 2], [Abs(x), Abs(y)]])
def test_add():
m = ArithmeticOnlyMatrix([[1, 2, 3], [x, y, x], [2*y, -50, z*x]])
assert m + m == ArithmeticOnlyMatrix([[2, 4, 6], [2*x, 2*y, 2*x], [4*y, -100, 2*z*x]])
n = ArithmeticOnlyMatrix(1, 2, [1, 2])
raises(ShapeError, lambda: m + n)
def test_multiplication():
a = ArithmeticOnlyMatrix((
(1, 2),
(3, 1),
(0, 6),
))
b = ArithmeticOnlyMatrix((
(1, 2),
(3, 0),
))
raises(ShapeError, lambda: b*a)
raises(TypeError, lambda: a*{})
c = a*b
assert c[0, 0] == 7
assert c[0, 1] == 2
assert c[1, 0] == 6
assert c[1, 1] == 6
assert c[2, 0] == 18
assert c[2, 1] == 0
try:
eval('c = a @ b')
except SyntaxError:
pass
else:
assert c[0, 0] == 7
assert c[0, 1] == 2
assert c[1, 0] == 6
assert c[1, 1] == 6
assert c[2, 0] == 18
assert c[2, 1] == 0
h = a.multiply_elementwise(c)
assert h == matrix_multiply_elementwise(a, c)
assert h[0, 0] == 7
assert h[0, 1] == 4
assert h[1, 0] == 18
assert h[1, 1] == 6
assert h[2, 0] == 0
assert h[2, 1] == 0
raises(ShapeError, lambda: a.multiply_elementwise(b))
c = b * Symbol("x")
assert isinstance(c, ArithmeticOnlyMatrix)
assert c[0, 0] == x
assert c[0, 1] == 2*x
assert c[1, 0] == 3*x
assert c[1, 1] == 0
c2 = x * b
assert c == c2
c = 5 * b
assert isinstance(c, ArithmeticOnlyMatrix)
assert c[0, 0] == 5
assert c[0, 1] == 2*5
assert c[1, 0] == 3*5
assert c[1, 1] == 0
try:
eval('c = 5 @ b')
except SyntaxError:
pass
else:
assert isinstance(c, ArithmeticOnlyMatrix)
assert c[0, 0] == 5
assert c[0, 1] == 2*5
assert c[1, 0] == 3*5
assert c[1, 1] == 0
def test_matmul():
a = Matrix([[1, 2], [3, 4]])
assert a.__matmul__(2) == NotImplemented
assert a.__rmatmul__(2) == NotImplemented
#This is done this way because @ is only supported in Python 3.5+
#To check 2@a case
try:
eval('2 @ a')
except SyntaxError:
pass
except TypeError: #TypeError is raised in case of NotImplemented is returned
pass
#Check a@2 case
try:
eval('a @ 2')
except SyntaxError:
pass
except TypeError: #TypeError is raised in case of NotImplemented is returned
pass
def test_power():
raises(NonSquareMatrixError, lambda: Matrix((1, 2))**2)
A = ArithmeticOnlyMatrix([[2, 3], [4, 5]])
assert (A**5)[:] == (6140, 8097, 10796, 14237)
A = ArithmeticOnlyMatrix([[2, 1, 3], [4, 2, 4], [6, 12, 1]])
assert (A**3)[:] == (290, 262, 251, 448, 440, 368, 702, 954, 433)
assert A**0 == eye(3)
assert A**1 == A
assert (ArithmeticOnlyMatrix([[2]]) ** 100)[0, 0] == 2**100
assert ArithmeticOnlyMatrix([[1, 2], [3, 4]])**Integer(2) == ArithmeticOnlyMatrix([[7, 10], [15, 22]])
def test_neg():
n = ArithmeticOnlyMatrix(1, 2, [1, 2])
assert -n == ArithmeticOnlyMatrix(1, 2, [-1, -2])
def test_sub():
n = ArithmeticOnlyMatrix(1, 2, [1, 2])
assert n - n == ArithmeticOnlyMatrix(1, 2, [0, 0])
def test_div():
n = ArithmeticOnlyMatrix(1, 2, [1, 2])
assert n/2 == ArithmeticOnlyMatrix(1, 2, [S(1)/2, S(2)/2])
# DeterminantOnlyMatrix tests
def test_det():
a = DeterminantOnlyMatrix(2, 3, [1, 2, 3, 4, 5, 6])
raises(NonSquareMatrixError, lambda: a.det())
z = zeros_Determinant(2)
ey = eye_Determinant(2)
assert z.det() == 0
assert ey.det() == 1
x = Symbol('x')
a = DeterminantOnlyMatrix(0, 0, [])
b = DeterminantOnlyMatrix(1, 1, [5])
c = DeterminantOnlyMatrix(2, 2, [1, 2, 3, 4])
d = DeterminantOnlyMatrix(3, 3, [1, 2, 3, 4, 5, 6, 7, 8, 8])
e = DeterminantOnlyMatrix(4, 4,
[x, 1, 2, 3, 4, 5, 6, 7, 2, 9, 10, 11, 12, 13, 14, 14])
# the method keyword for `det` doesn't kick in until 4x4 matrices,
# so there is no need to test all methods on smaller ones
assert a.det() == 1
assert b.det() == 5
assert c.det() == -2
assert d.det() == 3
assert e.det() == 4*x - 24
assert e.det(method='bareiss') == 4*x - 24
assert e.det(method='berkowitz') == 4*x - 24
raises(ValueError, lambda: e.det(iszerofunc="test"))
def test_adjugate():
x = Symbol('x')
e = DeterminantOnlyMatrix(4, 4,
[x, 1, 2, 3, 4, 5, 6, 7, 2, 9, 10, 11, 12, 13, 14, 14])
adj = Matrix([
[ 4, -8, 4, 0],
[ 76, -14*x - 68, 14*x - 8, -4*x + 24],
[-122, 17*x + 142, -21*x + 4, 8*x - 48],
[ 48, -4*x - 72, 8*x, -4*x + 24]])
assert e.adjugate() == adj
assert e.adjugate(method='bareiss') == adj
assert e.adjugate(method='berkowitz') == adj
a = DeterminantOnlyMatrix(2, 3, [1, 2, 3, 4, 5, 6])
raises(NonSquareMatrixError, lambda: a.adjugate())
def test_cofactor_and_minors():
x = Symbol('x')
e = DeterminantOnlyMatrix(4, 4,
[x, 1, 2, 3, 4, 5, 6, 7, 2, 9, 10, 11, 12, 13, 14, 14])
m = Matrix([
[ x, 1, 3],
[ 2, 9, 11],
[12, 13, 14]])
cm = Matrix([
[ 4, 76, -122, 48],
[-8, -14*x - 68, 17*x + 142, -4*x - 72],
[ 4, 14*x - 8, -21*x + 4, 8*x],
[ 0, -4*x + 24, 8*x - 48, -4*x + 24]])
sub = Matrix([
[x, 1, 2],
[4, 5, 6],
[2, 9, 10]])
assert e.minor_submatrix(1, 2) == m
assert e.minor_submatrix(-1, -1) == sub
assert e.minor(1, 2) == -17*x - 142
assert e.cofactor(1, 2) == 17*x + 142
assert e.cofactor_matrix() == cm
assert e.cofactor_matrix(method="bareiss") == cm
assert e.cofactor_matrix(method="berkowitz") == cm
raises(ValueError, lambda: e.cofactor(4, 5))
raises(ValueError, lambda: e.minor(4, 5))
raises(ValueError, lambda: e.minor_submatrix(4, 5))
a = DeterminantOnlyMatrix(2, 3, [1, 2, 3, 4, 5, 6])
assert a.minor_submatrix(0, 0) == Matrix([[5, 6]])
raises(ValueError, lambda:
DeterminantOnlyMatrix(0, 0, []).minor_submatrix(0, 0))
raises(NonSquareMatrixError, lambda: a.cofactor(0, 0))
raises(NonSquareMatrixError, lambda: a.minor(0, 0))
raises(NonSquareMatrixError, lambda: a.cofactor_matrix())
def test_charpoly():
x, y = Symbol('x'), Symbol('y')
m = DeterminantOnlyMatrix(3, 3, [1, 2, 3, 4, 5, 6, 7, 8, 9])
assert eye_Determinant(3).charpoly(x) == Poly((x - 1)**3, x)
assert eye_Determinant(3).charpoly(y) == Poly((y - 1)**3, y)
assert m.charpoly() == Poly(x**3 - 15*x**2 - 18*x, x)
raises(NonSquareMatrixError, lambda: Matrix([[1], [2]]).charpoly())
# ReductionsOnlyMatrix tests
def test_row_op():
e = eye_Reductions(3)
raises(ValueError, lambda: e.elementary_row_op("abc"))
raises(ValueError, lambda: e.elementary_row_op())
raises(ValueError, lambda: e.elementary_row_op('n->kn', row=5, k=5))
raises(ValueError, lambda: e.elementary_row_op('n->kn', row=-5, k=5))
raises(ValueError, lambda: e.elementary_row_op('n<->m', row1=1, row2=5))
raises(ValueError, lambda: e.elementary_row_op('n<->m', row1=5, row2=1))
raises(ValueError, lambda: e.elementary_row_op('n<->m', row1=-5, row2=1))
raises(ValueError, lambda: e.elementary_row_op('n<->m', row1=1, row2=-5))
raises(ValueError, lambda: e.elementary_row_op('n->n+km', row1=1, row2=5, k=5))
raises(ValueError, lambda: e.elementary_row_op('n->n+km', row1=5, row2=1, k=5))
raises(ValueError, lambda: e.elementary_row_op('n->n+km', row1=-5, row2=1, k=5))
raises(ValueError, lambda: e.elementary_row_op('n->n+km', row1=1, row2=-5, k=5))
raises(ValueError, lambda: e.elementary_row_op('n->n+km', row1=1, row2=1, k=5))
# test various ways to set arguments
assert e.elementary_row_op("n->kn", 0, 5) == Matrix([[5, 0, 0], [0, 1, 0], [0, 0, 1]])
assert e.elementary_row_op("n->kn", 1, 5) == Matrix([[1, 0, 0], [0, 5, 0], [0, 0, 1]])
assert e.elementary_row_op("n->kn", row=1, k=5) == Matrix([[1, 0, 0], [0, 5, 0], [0, 0, 1]])
assert e.elementary_row_op("n->kn", row1=1, k=5) == Matrix([[1, 0, 0], [0, 5, 0], [0, 0, 1]])
assert e.elementary_row_op("n<->m", 0, 1) == Matrix([[0, 1, 0], [1, 0, 0], [0, 0, 1]])
assert e.elementary_row_op("n<->m", row1=0, row2=1) == Matrix([[0, 1, 0], [1, 0, 0], [0, 0, 1]])
assert e.elementary_row_op("n<->m", row=0, row2=1) == Matrix([[0, 1, 0], [1, 0, 0], [0, 0, 1]])
assert e.elementary_row_op("n->n+km", 0, 5, 1) == Matrix([[1, 5, 0], [0, 1, 0], [0, 0, 1]])
assert e.elementary_row_op("n->n+km", row=0, k=5, row2=1) == Matrix([[1, 5, 0], [0, 1, 0], [0, 0, 1]])
assert e.elementary_row_op("n->n+km", row1=0, k=5, row2=1) == Matrix([[1, 5, 0], [0, 1, 0], [0, 0, 1]])
# make sure the matrix doesn't change size
a = ReductionsOnlyMatrix(2, 3, [0]*6)
assert a.elementary_row_op("n->kn", 1, 5) == Matrix(2, 3, [0]*6)
assert a.elementary_row_op("n<->m", 0, 1) == Matrix(2, 3, [0]*6)
assert a.elementary_row_op("n->n+km", 0, 5, 1) == Matrix(2, 3, [0]*6)
def test_col_op():
e = eye_Reductions(3)
raises(ValueError, lambda: e.elementary_col_op("abc"))
raises(ValueError, lambda: e.elementary_col_op())
raises(ValueError, lambda: e.elementary_col_op('n->kn', col=5, k=5))
raises(ValueError, lambda: e.elementary_col_op('n->kn', col=-5, k=5))
raises(ValueError, lambda: e.elementary_col_op('n<->m', col1=1, col2=5))
raises(ValueError, lambda: e.elementary_col_op('n<->m', col1=5, col2=1))
raises(ValueError, lambda: e.elementary_col_op('n<->m', col1=-5, col2=1))
raises(ValueError, lambda: e.elementary_col_op('n<->m', col1=1, col2=-5))
raises(ValueError, lambda: e.elementary_col_op('n->n+km', col1=1, col2=5, k=5))
raises(ValueError, lambda: e.elementary_col_op('n->n+km', col1=5, col2=1, k=5))
raises(ValueError, lambda: e.elementary_col_op('n->n+km', col1=-5, col2=1, k=5))
raises(ValueError, lambda: e.elementary_col_op('n->n+km', col1=1, col2=-5, k=5))
raises(ValueError, lambda: e.elementary_col_op('n->n+km', col1=1, col2=1, k=5))
# test various ways to set arguments
assert e.elementary_col_op("n->kn", 0, 5) == Matrix([[5, 0, 0], [0, 1, 0], [0, 0, 1]])
assert e.elementary_col_op("n->kn", 1, 5) == Matrix([[1, 0, 0], [0, 5, 0], [0, 0, 1]])
assert e.elementary_col_op("n->kn", col=1, k=5) == Matrix([[1, 0, 0], [0, 5, 0], [0, 0, 1]])
assert e.elementary_col_op("n->kn", col1=1, k=5) == Matrix([[1, 0, 0], [0, 5, 0], [0, 0, 1]])
assert e.elementary_col_op("n<->m", 0, 1) == Matrix([[0, 1, 0], [1, 0, 0], [0, 0, 1]])
assert e.elementary_col_op("n<->m", col1=0, col2=1) == Matrix([[0, 1, 0], [1, 0, 0], [0, 0, 1]])
assert e.elementary_col_op("n<->m", col=0, col2=1) == Matrix([[0, 1, 0], [1, 0, 0], [0, 0, 1]])
assert e.elementary_col_op("n->n+km", 0, 5, 1) == Matrix([[1, 0, 0], [5, 1, 0], [0, 0, 1]])
assert e.elementary_col_op("n->n+km", col=0, k=5, col2=1) == Matrix([[1, 0, 0], [5, 1, 0], [0, 0, 1]])
assert e.elementary_col_op("n->n+km", col1=0, k=5, col2=1) == Matrix([[1, 0, 0], [5, 1, 0], [0, 0, 1]])
# make sure the matrix doesn't change size
a = ReductionsOnlyMatrix(2, 3, [0]*6)
assert a.elementary_col_op("n->kn", 1, 5) == Matrix(2, 3, [0]*6)
assert a.elementary_col_op("n<->m", 0, 1) == Matrix(2, 3, [0]*6)
assert a.elementary_col_op("n->n+km", 0, 5, 1) == Matrix(2, 3, [0]*6)
def test_is_echelon():
zro = zeros_Reductions(3)
ident = eye_Reductions(3)
assert zro.is_echelon
assert ident.is_echelon
a = ReductionsOnlyMatrix(0, 0, [])
assert a.is_echelon
a = ReductionsOnlyMatrix(2, 3, [3, 2, 1, 0, 0, 6])
assert a.is_echelon
a = ReductionsOnlyMatrix(2, 3, [0, 0, 6, 3, 2, 1])
assert not a.is_echelon
x = Symbol('x')
a = ReductionsOnlyMatrix(3, 1, [x, 0, 0])
assert a.is_echelon
a = ReductionsOnlyMatrix(3, 1, [x, x, 0])
assert not a.is_echelon
a = ReductionsOnlyMatrix(3, 3, [0, 0, 0, 1, 2, 3, 0, 0, 0])
assert not a.is_echelon
def test_echelon_form():
# echelon form is not unique, but the result
# must be row-equivalent to the original matrix
# and it must be in echelon form.
a = zeros_Reductions(3)
e = eye_Reductions(3)
# we can assume the zero matrix and the identity matrix shouldn't change
assert a.echelon_form() == a
assert e.echelon_form() == e
a = ReductionsOnlyMatrix(0, 0, [])
assert a.echelon_form() == a
a = ReductionsOnlyMatrix(1, 1, [5])
assert a.echelon_form() == a
# now we get to the real tests
def verify_row_null_space(mat, rows, nulls):
for v in nulls:
assert all(t.is_zero for t in a_echelon*v)
for v in rows:
if not all(t.is_zero for t in v):
assert not all(t.is_zero for t in a_echelon*v.transpose())
a = ReductionsOnlyMatrix(3, 3, [1, 2, 3, 4, 5, 6, 7, 8, 9])
nulls = [Matrix([
[ 1],
[-2],
[ 1]])]
rows = [a[i, :] for i in range(a.rows)]
a_echelon = a.echelon_form()
assert a_echelon.is_echelon
verify_row_null_space(a, rows, nulls)
a = ReductionsOnlyMatrix(3, 3, [1, 2, 3, 4, 5, 6, 7, 8, 8])
nulls = []
rows = [a[i, :] for i in range(a.rows)]
a_echelon = a.echelon_form()
assert a_echelon.is_echelon
verify_row_null_space(a, rows, nulls)
a = ReductionsOnlyMatrix(3, 3, [2, 1, 3, 0, 0, 0, 2, 1, 3])
nulls = [Matrix([
[-S(1)/2],
[ 1],
[ 0]]),
Matrix([
[-S(3)/2],
[ 0],
[ 1]])]
rows = [a[i, :] for i in range(a.rows)]
a_echelon = a.echelon_form()
assert a_echelon.is_echelon
verify_row_null_space(a, rows, nulls)
# this one requires a row swap
a = ReductionsOnlyMatrix(3, 3, [2, 1, 3, 0, 0, 0, 1, 1, 3])
nulls = [Matrix([
[ 0],
[ -3],
[ 1]])]
rows = [a[i, :] for i in range(a.rows)]
a_echelon = a.echelon_form()
assert a_echelon.is_echelon
verify_row_null_space(a, rows, nulls)
a = ReductionsOnlyMatrix(3, 3, [0, 3, 3, 0, 2, 2, 0, 1, 1])
nulls = [Matrix([
[1],
[0],
[0]]),
Matrix([
[ 0],
[-1],
[ 1]])]
rows = [a[i, :] for i in range(a.rows)]
a_echelon = a.echelon_form()
assert a_echelon.is_echelon
verify_row_null_space(a, rows, nulls)
a = ReductionsOnlyMatrix(2, 3, [2, 2, 3, 3, 3, 0])
nulls = [Matrix([
[-1],
[1],
[0]])]
rows = [a[i, :] for i in range(a.rows)]
a_echelon = a.echelon_form()
assert a_echelon.is_echelon
verify_row_null_space(a, rows, nulls)
def test_rref():
e = ReductionsOnlyMatrix(0, 0, [])
assert e.rref(pivots=False) == e
e = ReductionsOnlyMatrix(1, 1, [1])
a = ReductionsOnlyMatrix(1, 1, [5])
assert e.rref(pivots=False) == a.rref(pivots=False) == e
a = ReductionsOnlyMatrix(3, 1, [1, 2, 3])
assert a.rref(pivots=False) == Matrix([[1], [0], [0]])
a = ReductionsOnlyMatrix(1, 3, [1, 2, 3])
assert a.rref(pivots=False) == Matrix([[1, 2, 3]])
a = ReductionsOnlyMatrix(3, 3, [1, 2, 3, 4, 5, 6, 7, 8, 9])
assert a.rref(pivots=False) == Matrix([
[1, 0, -1],
[0, 1, 2],
[0, 0, 0]])
a = ReductionsOnlyMatrix(3, 3, [1, 2, 3, 1, 2, 3, 1, 2, 3])
b = ReductionsOnlyMatrix(3, 3, [1, 2, 3, 0, 0, 0, 0, 0, 0])
c = ReductionsOnlyMatrix(3, 3, [0, 0, 0, 1, 2, 3, 0, 0, 0])
d = ReductionsOnlyMatrix(3, 3, [0, 0, 0, 0, 0, 0, 1, 2, 3])
assert a.rref(pivots=False) == \
b.rref(pivots=False) == \
c.rref(pivots=False) == \
d.rref(pivots=False) == b
e = eye_Reductions(3)
z = zeros_Reductions(3)
assert e.rref(pivots=False) == e
assert z.rref(pivots=False) == z
a = ReductionsOnlyMatrix([
[ 0, 0, 1, 2, 2, -5, 3],
[-1, 5, 2, 2, 1, -7, 5],
[ 0, 0, -2, -3, -3, 8, -5],
[-1, 5, 0, -1, -2, 1, 0]])
mat, pivot_offsets = a.rref()
assert mat == Matrix([
[1, -5, 0, 0, 1, 1, -1],
[0, 0, 1, 0, 0, -1, 1],
[0, 0, 0, 1, 1, -2, 1],
[0, 0, 0, 0, 0, 0, 0]])
assert pivot_offsets == (0, 2, 3)
a = ReductionsOnlyMatrix([[S(1)/19, S(1)/5, 2, 3],
[ 4, 5, 6, 7],
[ 8, 9, 10, 11],
[ 12, 13, 14, 15]])
assert a.rref(pivots=False) == Matrix([
[1, 0, 0, -S(76)/157],
[0, 1, 0, -S(5)/157],
[0, 0, 1, S(238)/157],
[0, 0, 0, 0]])
x = Symbol('x')
a = ReductionsOnlyMatrix(2, 3, [x, 1, 1, sqrt(x), x, 1])
for i, j in zip(a.rref(pivots=False),
[1, 0, sqrt(x)*(-x + 1)/(-x**(S(5)/2) + x),
0, 1, 1/(sqrt(x) + x + 1)]):
assert simplify(i - j).is_zero
# SpecialOnlyMatrix tests
def test_eye():
assert list(SpecialOnlyMatrix.eye(2, 2)) == [1, 0, 0, 1]
assert list(SpecialOnlyMatrix.eye(2)) == [1, 0, 0, 1]
assert type(SpecialOnlyMatrix.eye(2)) == SpecialOnlyMatrix
assert type(SpecialOnlyMatrix.eye(2, cls=Matrix)) == Matrix
def test_ones():
assert list(SpecialOnlyMatrix.ones(2, 2)) == [1, 1, 1, 1]
assert list(SpecialOnlyMatrix.ones(2)) == [1, 1, 1, 1]
assert SpecialOnlyMatrix.ones(2, 3) == Matrix([[1, 1, 1], [1, 1, 1]])
assert type(SpecialOnlyMatrix.ones(2)) == SpecialOnlyMatrix
assert type(SpecialOnlyMatrix.ones(2, cls=Matrix)) == Matrix
def test_zeros():
assert list(SpecialOnlyMatrix.zeros(2, 2)) == [0, 0, 0, 0]
assert list(SpecialOnlyMatrix.zeros(2)) == [0, 0, 0, 0]
assert SpecialOnlyMatrix.zeros(2, 3) == Matrix([[0, 0, 0], [0, 0, 0]])
assert type(SpecialOnlyMatrix.zeros(2)) == SpecialOnlyMatrix
assert type(SpecialOnlyMatrix.zeros(2, cls=Matrix)) == Matrix
def test_diag_make():
diag = SpecialOnlyMatrix.diag
a = Matrix([[1, 2], [2, 3]])
b = Matrix([[3, x], [y, 3]])
c = Matrix([[3, x, 3], [y, 3, z], [x, y, z]])
assert diag(a, b, b) == Matrix([
[1, 2, 0, 0, 0, 0],
[2, 3, 0, 0, 0, 0],
[0, 0, 3, x, 0, 0],
[0, 0, y, 3, 0, 0],
[0, 0, 0, 0, 3, x],
[0, 0, 0, 0, y, 3],
])
assert diag(a, b, c) == Matrix([
[1, 2, 0, 0, 0, 0, 0],
[2, 3, 0, 0, 0, 0, 0],
[0, 0, 3, x, 0, 0, 0],
[0, 0, y, 3, 0, 0, 0],
[0, 0, 0, 0, 3, x, 3],
[0, 0, 0, 0, y, 3, z],
[0, 0, 0, 0, x, y, z],
])
assert diag(a, c, b) == Matrix([
[1, 2, 0, 0, 0, 0, 0],
[2, 3, 0, 0, 0, 0, 0],
[0, 0, 3, x, 3, 0, 0],
[0, 0, y, 3, z, 0, 0],
[0, 0, x, y, z, 0, 0],
[0, 0, 0, 0, 0, 3, x],
[0, 0, 0, 0, 0, y, 3],
])
a = Matrix([x, y, z])
b = Matrix([[1, 2], [3, 4]])
c = Matrix([[5, 6]])
# this "wandering diagonal" is what makes this
# a block diagonal where each block is independent
# of the others
assert diag(a, 7, b, c) == Matrix([
[x, 0, 0, 0, 0, 0],
[y, 0, 0, 0, 0, 0],
[z, 0, 0, 0, 0, 0],
[0, 7, 0, 0, 0, 0],
[0, 0, 1, 2, 0, 0],
[0, 0, 3, 4, 0, 0],
[0, 0, 0, 0, 5, 6]])
raises(ValueError, lambda: diag(a, 7, b, c, rows=5))
assert diag(1) == Matrix([[1]])
assert diag(1, rows=2) == Matrix([[1, 0], [0, 0]])
assert diag(1, cols=2) == Matrix([[1, 0], [0, 0]])
assert diag(1, rows=3, cols=2) == Matrix([[1, 0], [0, 0], [0, 0]])
assert diag(*[2, 3]) == Matrix([
[2, 0],
[0, 3]])
assert diag(Matrix([2, 3])) == Matrix([
[2],
[3]])
assert diag([1, [2, 3], 4], unpack=False) == \
diag([[1], [2, 3], [4]], unpack=False) == Matrix([
[1, 0],
[2, 3],
[4, 0]])
assert type(diag(1)) == SpecialOnlyMatrix
assert type(diag(1, cls=Matrix)) == Matrix
assert Matrix.diag([1, 2, 3]) == Matrix.diag(1, 2, 3)
assert Matrix.diag([1, 2, 3], unpack=False).shape == (3, 1)
assert Matrix.diag([[1, 2, 3]]).shape == (3, 1)
assert Matrix.diag([[1, 2, 3]], unpack=False).shape == (1, 3)
assert Matrix.diag([[[1, 2, 3]]]).shape == (1, 3)
# kerning can be used to move the starting point
assert Matrix.diag(ones(0, 2), 1, 2) == Matrix([
[0, 0, 1, 0],
[0, 0, 0, 2]])
assert Matrix.diag(ones(2, 0), 1, 2) == Matrix([
[0, 0],
[0, 0],
[1, 0],
[0, 2]])
def test_diagonal():
m = Matrix(3, 3, range(9))
d = m.diagonal()
assert d == m.diagonal(0)
assert tuple(d) == (0, 4, 8)
assert tuple(m.diagonal(1)) == (1, 5)
assert tuple(m.diagonal(-1)) == (3, 7)
assert tuple(m.diagonal(2)) == (2,)
assert type(m.diagonal()) == type(m)
s = SparseMatrix(3, 3, {(1, 1): 1})
assert type(s.diagonal()) == type(s)
assert type(m) != type(s)
raises(ValueError, lambda: m.diagonal(3))
raises(ValueError, lambda: m.diagonal(-3))
raises(ValueError, lambda: m.diagonal(pi))
M = ones(2, 3)
assert banded({i: list(M.diagonal(i))
for i in range(1-M.rows, M.cols)}) == M
def test_jordan_block():
assert SpecialOnlyMatrix.jordan_block(3, 2) == SpecialOnlyMatrix.jordan_block(3, eigenvalue=2) \
== SpecialOnlyMatrix.jordan_block(size=3, eigenvalue=2) \
== SpecialOnlyMatrix.jordan_block(3, 2, band='upper') \
== SpecialOnlyMatrix.jordan_block(
size=3, eigenval=2, eigenvalue=2) \
== Matrix([
[2, 1, 0],
[0, 2, 1],
[0, 0, 2]])
assert SpecialOnlyMatrix.jordan_block(3, 2, band='lower') == Matrix([
[2, 0, 0],
[1, 2, 0],
[0, 1, 2]])
# missing eigenvalue
raises(ValueError, lambda: SpecialOnlyMatrix.jordan_block(2))
# non-integral size
raises(ValueError, lambda: SpecialOnlyMatrix.jordan_block(3.5, 2))
# size not specified
raises(ValueError, lambda: SpecialOnlyMatrix.jordan_block(eigenvalue=2))
# inconsistent eigenvalue
raises(ValueError,
lambda: SpecialOnlyMatrix.jordan_block(
eigenvalue=2, eigenval=4))
# Deprecated feature
with warns_deprecated_sympy():
assert (SpecialOnlyMatrix.jordan_block(cols=3, eigenvalue=2) ==
SpecialOnlyMatrix(3, 3, (2, 1, 0, 0, 2, 1, 0, 0, 2)))
with warns_deprecated_sympy():
assert (SpecialOnlyMatrix.jordan_block(rows=3, eigenvalue=2) ==
SpecialOnlyMatrix(3, 3, (2, 1, 0, 0, 2, 1, 0, 0, 2)))
with warns_deprecated_sympy():
assert SpecialOnlyMatrix.jordan_block(3, 2) == \
SpecialOnlyMatrix.jordan_block(cols=3, eigenvalue=2) == \
SpecialOnlyMatrix.jordan_block(rows=3, eigenvalue=2)
with warns_deprecated_sympy():
assert SpecialOnlyMatrix.jordan_block(
rows=4, cols=3, eigenvalue=2) == \
Matrix([
[2, 1, 0],
[0, 2, 1],
[0, 0, 2],
[0, 0, 0]])
# Using alias keyword
assert SpecialOnlyMatrix.jordan_block(size=3, eigenvalue=2) == \
SpecialOnlyMatrix.jordan_block(size=3, eigenval=2)
# SubspaceOnlyMatrix tests
def test_columnspace():
m = SubspaceOnlyMatrix([[ 1, 2, 0, 2, 5],
[-2, -5, 1, -1, -8],
[ 0, -3, 3, 4, 1],
[ 3, 6, 0, -7, 2]])
basis = m.columnspace()
assert basis[0] == Matrix([1, -2, 0, 3])
assert basis[1] == Matrix([2, -5, -3, 6])
assert basis[2] == Matrix([2, -1, 4, -7])
assert len(basis) == 3
assert Matrix.hstack(m, *basis).columnspace() == basis
def test_rowspace():
m = SubspaceOnlyMatrix([[ 1, 2, 0, 2, 5],
[-2, -5, 1, -1, -8],
[ 0, -3, 3, 4, 1],
[ 3, 6, 0, -7, 2]])
basis = m.rowspace()
assert basis[0] == Matrix([[1, 2, 0, 2, 5]])
assert basis[1] == Matrix([[0, -1, 1, 3, 2]])
assert basis[2] == Matrix([[0, 0, 0, 5, 5]])
assert len(basis) == 3
def test_nullspace():
m = SubspaceOnlyMatrix([[ 1, 2, 0, 2, 5],
[-2, -5, 1, -1, -8],
[ 0, -3, 3, 4, 1],
[ 3, 6, 0, -7, 2]])
basis = m.nullspace()
assert basis[0] == Matrix([-2, 1, 1, 0, 0])
assert basis[1] == Matrix([-1, -1, 0, -1, 1])
# make sure the null space is really gets zeroed
assert all(e.is_zero for e in m*basis[0])
assert all(e.is_zero for e in m*basis[1])
def test_orthogonalize():
m = Matrix([[1, 2], [3, 4]])
assert m.orthogonalize(Matrix([[2], [1]])) == [Matrix([[2], [1]])]
assert m.orthogonalize(Matrix([[2], [1]]), normalize=True) == \
[Matrix([[2*sqrt(5)/5], [sqrt(5)/5]])]
assert m.orthogonalize(Matrix([[1], [2]]), Matrix([[-1], [4]])) == \
[Matrix([[1], [2]]), Matrix([[-S(12)/5], [S(6)/5]])]
assert m.orthogonalize(Matrix([[0], [0]]), Matrix([[-1], [4]])) == \
[Matrix([[-1], [4]])]
assert m.orthogonalize(Matrix([[0], [0]])) == []
n = Matrix([[9, 1, 9], [3, 6, 10], [8, 5, 2]])
vecs = [Matrix([[-5], [1]]), Matrix([[-5], [2]]), Matrix([[-5], [-2]])]
assert n.orthogonalize(*vecs) == \
[Matrix([[-5], [1]]), Matrix([[S(5)/26], [S(25)/26]])]
vecs = [Matrix([0, 0, 0]), Matrix([1, 2, 3]), Matrix([1, 4, 5])]
raises(ValueError, lambda: Matrix.orthogonalize(*vecs, rankcheck=True))
vecs = [Matrix([1, 2, 3]), Matrix([4, 5, 6]), Matrix([7, 8, 9])]
raises(ValueError, lambda: Matrix.orthogonalize(*vecs, rankcheck=True))
# EigenOnlyMatrix tests
def test_eigenvals():
M = EigenOnlyMatrix([[0, 1, 1],
[1, 0, 0],
[1, 1, 1]])
assert M.eigenvals() == {2*S.One: 1, -S.One: 1, S.Zero: 1}
# if we cannot factor the char poly, we raise an error
m = Matrix([
[3, 0, 0, 0, -3],
[0, -3, -3, 0, 3],
[0, 3, 0, 3, 0],
[0, 0, 3, 0, 3],
[3, 0, 0, 3, 0]])
raises(MatrixError, lambda: m.eigenvals())
def test_eigenvects():
M = EigenOnlyMatrix([[0, 1, 1],
[1, 0, 0],
[1, 1, 1]])
vecs = M.eigenvects()
for val, mult, vec_list in vecs:
assert len(vec_list) == 1
assert M*vec_list[0] == val*vec_list[0]
def test_left_eigenvects():
M = EigenOnlyMatrix([[0, 1, 1],
[1, 0, 0],
[1, 1, 1]])
vecs = M.left_eigenvects()
for val, mult, vec_list in vecs:
assert len(vec_list) == 1
assert vec_list[0]*M == val*vec_list[0]
def test_diagonalize():
m = EigenOnlyMatrix(2, 2, [0, -1, 1, 0])
raises(MatrixError, lambda: m.diagonalize(reals_only=True))
P, D = m.diagonalize()
assert D.is_diagonal()
assert D == Matrix([
[-I, 0],
[ 0, I]])
# make sure we use floats out if floats are passed in
m = EigenOnlyMatrix(2, 2, [0, .5, .5, 0])
P, D = m.diagonalize()
assert all(isinstance(e, Float) for e in D.values())
assert all(isinstance(e, Float) for e in P.values())
_, D2 = m.diagonalize(reals_only=True)
assert D == D2
def test_is_diagonalizable():
a, b, c = symbols('a b c')
m = EigenOnlyMatrix(2, 2, [a, c, c, b])
assert m.is_symmetric()
assert m.is_diagonalizable()
assert not EigenOnlyMatrix(2, 2, [1, 1, 0, 1]).is_diagonalizable()
m = EigenOnlyMatrix(2, 2, [0, -1, 1, 0])
assert m.is_diagonalizable()
assert not m.is_diagonalizable(reals_only=True)
def test_jordan_form():
m = Matrix(3, 2, [-3, 1, -3, 20, 3, 10])
raises(NonSquareMatrixError, lambda: m.jordan_form())
# the next two tests test the cases where the old
# algorithm failed due to the fact that the block structure can
# *NOT* be determined from algebraic and geometric multiplicity alone
# This can be seen most easily when one lets compute the J.c.f. of a matrix that
# is in J.c.f already.
m = EigenOnlyMatrix(4, 4, [2, 1, 0, 0,
0, 2, 1, 0,
0, 0, 2, 0,
0, 0, 0, 2
])
P, J = m.jordan_form()
assert m == J
m = EigenOnlyMatrix(4, 4, [2, 1, 0, 0,
0, 2, 0, 0,
0, 0, 2, 1,
0, 0, 0, 2
])
P, J = m.jordan_form()
assert m == J
A = Matrix([[ 2, 4, 1, 0],
[-4, 2, 0, 1],
[ 0, 0, 2, 4],
[ 0, 0, -4, 2]])
P, J = A.jordan_form()
assert simplify(P*J*P.inv()) == A
assert EigenOnlyMatrix(1, 1, [1]).jordan_form() == (
Matrix([1]), Matrix([1]))
assert EigenOnlyMatrix(1, 1, [1]).jordan_form(
calc_transform=False) == Matrix([1])
# make sure if we cannot factor the characteristic polynomial, we raise an error
m = Matrix([[3, 0, 0, 0, -3], [0, -3, -3, 0, 3], [0, 3, 0, 3, 0], [0, 0, 3, 0, 3], [3, 0, 0, 3, 0]])
raises(MatrixError, lambda: m.jordan_form())
# make sure that if the input has floats, the output does too
m = Matrix([
[ 0.6875, 0.125 + 0.1875*sqrt(3)],
[0.125 + 0.1875*sqrt(3), 0.3125]])
P, J = m.jordan_form()
assert all(isinstance(x, Float) or x == 0 for x in P)
assert all(isinstance(x, Float) or x == 0 for x in J)
def test_singular_values():
x = Symbol('x', real=True)
A = EigenOnlyMatrix([[0, 1*I], [2, 0]])
# if singular values can be sorted, they should be in decreasing order
assert A.singular_values() == [2, 1]
A = eye(3)
A[1, 1] = x
A[2, 2] = 5
vals = A.singular_values()
# since Abs(x) cannot be sorted, test set equality
assert set(vals) == set([5, 1, Abs(x)])
A = EigenOnlyMatrix([[sin(x), cos(x)], [-cos(x), sin(x)]])
vals = [sv.trigsimp() for sv in A.singular_values()]
assert vals == [S(1), S(1)]
A = EigenOnlyMatrix([
[2, 4],
[1, 3],
[0, 0],
[0, 0]
])
assert A.singular_values() == \
[sqrt(sqrt(221) + 15), sqrt(15 - sqrt(221))]
assert A.T.singular_values() == \
[sqrt(sqrt(221) + 15), sqrt(15 - sqrt(221)), 0, 0]
# CalculusOnlyMatrix tests
@XFAIL
def test_diff():
x, y = symbols('x y')
m = CalculusOnlyMatrix(2, 1, [x, y])
# TODO: currently not working as ``_MinimalMatrix`` cannot be sympified:
assert m.diff(x) == Matrix(2, 1, [1, 0])
def test_integrate():
x, y = symbols('x y')
m = CalculusOnlyMatrix(2, 1, [x, y])
assert m.integrate(x) == Matrix(2, 1, [x**2/2, y*x])
def test_jacobian2():
rho, phi = symbols("rho,phi")
X = CalculusOnlyMatrix(3, 1, [rho*cos(phi), rho*sin(phi), rho**2])
Y = CalculusOnlyMatrix(2, 1, [rho, phi])
J = Matrix([
[cos(phi), -rho*sin(phi)],
[sin(phi), rho*cos(phi)],
[ 2*rho, 0],
])
assert X.jacobian(Y) == J
m = CalculusOnlyMatrix(2, 2, [1, 2, 3, 4])
m2 = CalculusOnlyMatrix(4, 1, [1, 2, 3, 4])
raises(TypeError, lambda: m.jacobian(Matrix([1, 2])))
raises(TypeError, lambda: m2.jacobian(m))
def test_limit():
x, y = symbols('x y')
m = CalculusOnlyMatrix(2, 1, [1/x, y])
assert m.limit(x, 5) == Matrix(2, 1, [S(1)/5, y])
def test_issue_13774():
M = Matrix([[1, 2, 3], [4, 5, 6], [7, 8, 9]])
v = [1, 1, 1]
raises(TypeError, lambda: M*v)
raises(TypeError, lambda: v*M)
def test___eq__():
assert (EigenOnlyMatrix(
[[0, 1, 1],
[1, 0, 0],
[1, 1, 1]]) == {}) is False
|
5a5d95dccbe252f285854e08eb202ff0e3cae34c738be25367d969d196ceb22e | from sympy import Abs, S, Symbol, symbols, I, Rational, PurePoly, Float
from sympy.matrices import \
Matrix, MutableSparseMatrix, ImmutableSparseMatrix, SparseMatrix, eye, \
ones, zeros, ShapeError
from sympy.utilities.pytest import raises
def test_sparse_matrix():
def sparse_eye(n):
return SparseMatrix.eye(n)
def sparse_zeros(n):
return SparseMatrix.zeros(n)
# creation args
raises(TypeError, lambda: SparseMatrix(1, 2))
a = SparseMatrix((
(1, 0),
(0, 1)
))
assert SparseMatrix(a) == a
from sympy.matrices import MutableSparseMatrix, MutableDenseMatrix
a = MutableSparseMatrix([])
b = MutableDenseMatrix([1, 2])
assert a.row_join(b) == b
assert a.col_join(b) == b
assert type(a.row_join(b)) == type(a)
assert type(a.col_join(b)) == type(a)
# make sure 0 x n matrices get stacked correctly
sparse_matrices = [SparseMatrix.zeros(0, n) for n in range(4)]
assert SparseMatrix.hstack(*sparse_matrices) == Matrix(0, 6, [])
sparse_matrices = [SparseMatrix.zeros(n, 0) for n in range(4)]
assert SparseMatrix.vstack(*sparse_matrices) == Matrix(6, 0, [])
# test element assignment
a = SparseMatrix((
(1, 0),
(0, 1)
))
a[3] = 4
assert a[1, 1] == 4
a[3] = 1
a[0, 0] = 2
assert a == SparseMatrix((
(2, 0),
(0, 1)
))
a[1, 0] = 5
assert a == SparseMatrix((
(2, 0),
(5, 1)
))
a[1, 1] = 0
assert a == SparseMatrix((
(2, 0),
(5, 0)
))
assert a._smat == {(0, 0): 2, (1, 0): 5}
# test_multiplication
a = SparseMatrix((
(1, 2),
(3, 1),
(0, 6),
))
b = SparseMatrix((
(1, 2),
(3, 0),
))
c = a*b
assert c[0, 0] == 7
assert c[0, 1] == 2
assert c[1, 0] == 6
assert c[1, 1] == 6
assert c[2, 0] == 18
assert c[2, 1] == 0
try:
eval('c = a @ b')
except SyntaxError:
pass
else:
assert c[0, 0] == 7
assert c[0, 1] == 2
assert c[1, 0] == 6
assert c[1, 1] == 6
assert c[2, 0] == 18
assert c[2, 1] == 0
x = Symbol("x")
c = b * Symbol("x")
assert isinstance(c, SparseMatrix)
assert c[0, 0] == x
assert c[0, 1] == 2*x
assert c[1, 0] == 3*x
assert c[1, 1] == 0
c = 5 * b
assert isinstance(c, SparseMatrix)
assert c[0, 0] == 5
assert c[0, 1] == 2*5
assert c[1, 0] == 3*5
assert c[1, 1] == 0
#test_power
A = SparseMatrix([[2, 3], [4, 5]])
assert (A**5)[:] == [6140, 8097, 10796, 14237]
A = SparseMatrix([[2, 1, 3], [4, 2, 4], [6, 12, 1]])
assert (A**3)[:] == [290, 262, 251, 448, 440, 368, 702, 954, 433]
# test_creation
x = Symbol("x")
a = SparseMatrix([[x, 0], [0, 0]])
m = a
assert m.cols == m.rows
assert m.cols == 2
assert m[:] == [x, 0, 0, 0]
b = SparseMatrix(2, 2, [x, 0, 0, 0])
m = b
assert m.cols == m.rows
assert m.cols == 2
assert m[:] == [x, 0, 0, 0]
assert a == b
S = sparse_eye(3)
S.row_del(1)
assert S == SparseMatrix([
[1, 0, 0],
[0, 0, 1]])
S = sparse_eye(3)
S.col_del(1)
assert S == SparseMatrix([
[1, 0],
[0, 0],
[0, 1]])
S = SparseMatrix.eye(3)
S[2, 1] = 2
S.col_swap(1, 0)
assert S == SparseMatrix([
[0, 1, 0],
[1, 0, 0],
[2, 0, 1]])
a = SparseMatrix(1, 2, [1, 2])
b = a.copy()
c = a.copy()
assert a[0] == 1
a.row_del(0)
assert a == SparseMatrix(0, 2, [])
b.col_del(1)
assert b == SparseMatrix(1, 1, [1])
assert SparseMatrix([[1, 2, 3], [1, 2], [1]]) == Matrix([
[1, 2, 3],
[1, 2, 0],
[1, 0, 0]])
assert SparseMatrix(4, 4, {(1, 1): sparse_eye(2)}) == Matrix([
[0, 0, 0, 0],
[0, 1, 0, 0],
[0, 0, 1, 0],
[0, 0, 0, 0]])
raises(ValueError, lambda: SparseMatrix(1, 1, {(1, 1): 1}))
assert SparseMatrix(1, 2, [1, 2]).tolist() == [[1, 2]]
assert SparseMatrix(2, 2, [1, [2, 3]]).tolist() == [[1, 0], [2, 3]]
raises(ValueError, lambda: SparseMatrix(2, 2, [1]))
raises(ValueError, lambda: SparseMatrix(1, 1, [[1, 2]]))
assert SparseMatrix([.1]).has(Float)
# autosizing
assert SparseMatrix(None, {(0, 1): 0}).shape == (0, 0)
assert SparseMatrix(None, {(0, 1): 1}).shape == (1, 2)
assert SparseMatrix(None, None, {(0, 1): 1}).shape == (1, 2)
raises(ValueError, lambda: SparseMatrix(None, 1, [[1, 2]]))
raises(ValueError, lambda: SparseMatrix(1, None, [[1, 2]]))
raises(ValueError, lambda: SparseMatrix(3, 3, {(0, 0): ones(2), (1, 1): 2}))
# test_determinant
x, y = Symbol('x'), Symbol('y')
assert SparseMatrix(1, 1, [0]).det() == 0
assert SparseMatrix([[1]]).det() == 1
assert SparseMatrix(((-3, 2), (8, -5))).det() == -1
assert SparseMatrix(((x, 1), (y, 2*y))).det() == 2*x*y - y
assert SparseMatrix(( (1, 1, 1),
(1, 2, 3),
(1, 3, 6) )).det() == 1
assert SparseMatrix(( ( 3, -2, 0, 5),
(-2, 1, -2, 2),
( 0, -2, 5, 0),
( 5, 0, 3, 4) )).det() == -289
assert SparseMatrix(( ( 1, 2, 3, 4),
( 5, 6, 7, 8),
( 9, 10, 11, 12),
(13, 14, 15, 16) )).det() == 0
assert SparseMatrix(( (3, 2, 0, 0, 0),
(0, 3, 2, 0, 0),
(0, 0, 3, 2, 0),
(0, 0, 0, 3, 2),
(2, 0, 0, 0, 3) )).det() == 275
assert SparseMatrix(( (1, 0, 1, 2, 12),
(2, 0, 1, 1, 4),
(2, 1, 1, -1, 3),
(3, 2, -1, 1, 8),
(1, 1, 1, 0, 6) )).det() == -55
assert SparseMatrix(( (-5, 2, 3, 4, 5),
( 1, -4, 3, 4, 5),
( 1, 2, -3, 4, 5),
( 1, 2, 3, -2, 5),
( 1, 2, 3, 4, -1) )).det() == 11664
assert SparseMatrix(( ( 2, 7, -1, 3, 2),
( 0, 0, 1, 0, 1),
(-2, 0, 7, 0, 2),
(-3, -2, 4, 5, 3),
( 1, 0, 0, 0, 1) )).det() == 123
# test_slicing
m0 = sparse_eye(4)
assert m0[:3, :3] == sparse_eye(3)
assert m0[2:4, 0:2] == sparse_zeros(2)
m1 = SparseMatrix(3, 3, lambda i, j: i + j)
assert m1[0, :] == SparseMatrix(1, 3, (0, 1, 2))
assert m1[1:3, 1] == SparseMatrix(2, 1, (2, 3))
m2 = SparseMatrix(
[[0, 1, 2, 3], [4, 5, 6, 7], [8, 9, 10, 11], [12, 13, 14, 15]])
assert m2[:, -1] == SparseMatrix(4, 1, [3, 7, 11, 15])
assert m2[-2:, :] == SparseMatrix([[8, 9, 10, 11], [12, 13, 14, 15]])
assert SparseMatrix([[1, 2], [3, 4]])[[1], [1]] == Matrix([[4]])
# test_submatrix_assignment
m = sparse_zeros(4)
m[2:4, 2:4] = sparse_eye(2)
assert m == SparseMatrix([(0, 0, 0, 0),
(0, 0, 0, 0),
(0, 0, 1, 0),
(0, 0, 0, 1)])
assert len(m._smat) == 2
m[:2, :2] = sparse_eye(2)
assert m == sparse_eye(4)
m[:, 0] = SparseMatrix(4, 1, (1, 2, 3, 4))
assert m == SparseMatrix([(1, 0, 0, 0),
(2, 1, 0, 0),
(3, 0, 1, 0),
(4, 0, 0, 1)])
m[:, :] = sparse_zeros(4)
assert m == sparse_zeros(4)
m[:, :] = ((1, 2, 3, 4), (5, 6, 7, 8), (9, 10, 11, 12), (13, 14, 15, 16))
assert m == SparseMatrix((( 1, 2, 3, 4),
( 5, 6, 7, 8),
( 9, 10, 11, 12),
(13, 14, 15, 16)))
m[:2, 0] = [0, 0]
assert m == SparseMatrix((( 0, 2, 3, 4),
( 0, 6, 7, 8),
( 9, 10, 11, 12),
(13, 14, 15, 16)))
# test_reshape
m0 = sparse_eye(3)
assert m0.reshape(1, 9) == SparseMatrix(1, 9, (1, 0, 0, 0, 1, 0, 0, 0, 1))
m1 = SparseMatrix(3, 4, lambda i, j: i + j)
assert m1.reshape(4, 3) == \
SparseMatrix([(0, 1, 2), (3, 1, 2), (3, 4, 2), (3, 4, 5)])
assert m1.reshape(2, 6) == \
SparseMatrix([(0, 1, 2, 3, 1, 2), (3, 4, 2, 3, 4, 5)])
# test_applyfunc
m0 = sparse_eye(3)
assert m0.applyfunc(lambda x: 2*x) == sparse_eye(3)*2
assert m0.applyfunc(lambda x: 0 ) == sparse_zeros(3)
# test__eval_Abs
assert abs(SparseMatrix(((x, 1), (y, 2*y)))) == SparseMatrix(((Abs(x), 1), (Abs(y), 2*Abs(y))))
# test_LUdecomp
testmat = SparseMatrix([[ 0, 2, 5, 3],
[ 3, 3, 7, 4],
[ 8, 4, 0, 2],
[-2, 6, 3, 4]])
L, U, p = testmat.LUdecomposition()
assert L.is_lower
assert U.is_upper
assert (L*U).permute_rows(p, 'backward') - testmat == sparse_zeros(4)
testmat = SparseMatrix([[ 6, -2, 7, 4],
[ 0, 3, 6, 7],
[ 1, -2, 7, 4],
[-9, 2, 6, 3]])
L, U, p = testmat.LUdecomposition()
assert L.is_lower
assert U.is_upper
assert (L*U).permute_rows(p, 'backward') - testmat == sparse_zeros(4)
x, y, z = Symbol('x'), Symbol('y'), Symbol('z')
M = Matrix(((1, x, 1), (2, y, 0), (y, 0, z)))
L, U, p = M.LUdecomposition()
assert L.is_lower
assert U.is_upper
assert (L*U).permute_rows(p, 'backward') - M == sparse_zeros(3)
# test_LUsolve
A = SparseMatrix([[2, 3, 5],
[3, 6, 2],
[8, 3, 6]])
x = SparseMatrix(3, 1, [3, 7, 5])
b = A*x
soln = A.LUsolve(b)
assert soln == x
A = SparseMatrix([[0, -1, 2],
[5, 10, 7],
[8, 3, 4]])
x = SparseMatrix(3, 1, [-1, 2, 5])
b = A*x
soln = A.LUsolve(b)
assert soln == x
# test_inverse
A = sparse_eye(4)
assert A.inv() == sparse_eye(4)
assert A.inv(method="CH") == sparse_eye(4)
assert A.inv(method="LDL") == sparse_eye(4)
A = SparseMatrix([[2, 3, 5],
[3, 6, 2],
[7, 2, 6]])
Ainv = SparseMatrix(Matrix(A).inv())
assert A*Ainv == sparse_eye(3)
assert A.inv(method="CH") == Ainv
assert A.inv(method="LDL") == Ainv
A = SparseMatrix([[2, 3, 5],
[3, 6, 2],
[5, 2, 6]])
Ainv = SparseMatrix(Matrix(A).inv())
assert A*Ainv == sparse_eye(3)
assert A.inv(method="CH") == Ainv
assert A.inv(method="LDL") == Ainv
# test_cross
v1 = Matrix(1, 3, [1, 2, 3])
v2 = Matrix(1, 3, [3, 4, 5])
assert v1.cross(v2) == Matrix(1, 3, [-2, 4, -2])
assert v1.norm(2)**2 == 14
# conjugate
a = SparseMatrix(((1, 2 + I), (3, 4)))
assert a.C == SparseMatrix([
[1, 2 - I],
[3, 4]
])
# mul
assert a*Matrix(2, 2, [1, 0, 0, 1]) == a
assert a + Matrix(2, 2, [1, 1, 1, 1]) == SparseMatrix([
[2, 3 + I],
[4, 5]
])
# col join
assert a.col_join(sparse_eye(2)) == SparseMatrix([
[1, 2 + I],
[3, 4],
[1, 0],
[0, 1]
])
# symmetric
assert not a.is_symmetric(simplify=False)
# test_cofactor
assert sparse_eye(3) == sparse_eye(3).cofactor_matrix()
test = SparseMatrix([[1, 3, 2], [2, 6, 3], [2, 3, 6]])
assert test.cofactor_matrix() == \
SparseMatrix([[27, -6, -6], [-12, 2, 3], [-3, 1, 0]])
test = SparseMatrix([[1, 2, 3], [4, 5, 6], [7, 8, 9]])
assert test.cofactor_matrix() == \
SparseMatrix([[-3, 6, -3], [6, -12, 6], [-3, 6, -3]])
# test_jacobian
x = Symbol('x')
y = Symbol('y')
L = SparseMatrix(1, 2, [x**2*y, 2*y**2 + x*y])
syms = [x, y]
assert L.jacobian(syms) == Matrix([[2*x*y, x**2], [y, 4*y + x]])
L = SparseMatrix(1, 2, [x, x**2*y**3])
assert L.jacobian(syms) == SparseMatrix([[1, 0], [2*x*y**3, x**2*3*y**2]])
# test_QR
A = Matrix([[1, 2], [2, 3]])
Q, S = A.QRdecomposition()
R = Rational
assert Q == Matrix([
[ 5**R(-1, 2), (R(2)/5)*(R(1)/5)**R(-1, 2)],
[2*5**R(-1, 2), (-R(1)/5)*(R(1)/5)**R(-1, 2)]])
assert S == Matrix([
[5**R(1, 2), 8*5**R(-1, 2)],
[ 0, (R(1)/5)**R(1, 2)]])
assert Q*S == A
assert Q.T * Q == sparse_eye(2)
R = Rational
# test nullspace
# first test reduced row-ech form
M = SparseMatrix([[5, 7, 2, 1],
[1, 6, 2, -1]])
out, tmp = M.rref()
assert out == Matrix([[1, 0, -R(2)/23, R(13)/23],
[0, 1, R(8)/23, R(-6)/23]])
M = SparseMatrix([[ 1, 3, 0, 2, 6, 3, 1],
[-2, -6, 0, -2, -8, 3, 1],
[ 3, 9, 0, 0, 6, 6, 2],
[-1, -3, 0, 1, 0, 9, 3]])
out, tmp = M.rref()
assert out == Matrix([[1, 3, 0, 0, 2, 0, 0],
[0, 0, 0, 1, 2, 0, 0],
[0, 0, 0, 0, 0, 1, R(1)/3],
[0, 0, 0, 0, 0, 0, 0]])
# now check the vectors
basis = M.nullspace()
assert basis[0] == Matrix([-3, 1, 0, 0, 0, 0, 0])
assert basis[1] == Matrix([0, 0, 1, 0, 0, 0, 0])
assert basis[2] == Matrix([-2, 0, 0, -2, 1, 0, 0])
assert basis[3] == Matrix([0, 0, 0, 0, 0, R(-1)/3, 1])
# test eigen
x = Symbol('x')
y = Symbol('y')
sparse_eye3 = sparse_eye(3)
assert sparse_eye3.charpoly(x) == PurePoly(((x - 1)**3))
assert sparse_eye3.charpoly(y) == PurePoly(((y - 1)**3))
# test values
M = Matrix([( 0, 1, -1),
( 1, 1, 0),
(-1, 0, 1)])
vals = M.eigenvals()
assert sorted(vals.keys()) == [-1, 1, 2]
R = Rational
M = Matrix([[1, 0, 0],
[0, 1, 0],
[0, 0, 1]])
assert M.eigenvects() == [(1, 3, [
Matrix([1, 0, 0]),
Matrix([0, 1, 0]),
Matrix([0, 0, 1])])]
M = Matrix([[5, 0, 2],
[3, 2, 0],
[0, 0, 1]])
assert M.eigenvects() == [(1, 1, [Matrix([R(-1)/2, R(3)/2, 1])]),
(2, 1, [Matrix([0, 1, 0])]),
(5, 1, [Matrix([1, 1, 0])])]
assert M.zeros(3, 5) == SparseMatrix(3, 5, {})
A = SparseMatrix(10, 10, {(0, 0): 18, (0, 9): 12, (1, 4): 18, (2, 7): 16, (3, 9): 12, (4, 2): 19, (5, 7): 16, (6, 2): 12, (9, 7): 18})
assert A.row_list() == [(0, 0, 18), (0, 9, 12), (1, 4, 18), (2, 7, 16), (3, 9, 12), (4, 2, 19), (5, 7, 16), (6, 2, 12), (9, 7, 18)]
assert A.col_list() == [(0, 0, 18), (4, 2, 19), (6, 2, 12), (1, 4, 18), (2, 7, 16), (5, 7, 16), (9, 7, 18), (0, 9, 12), (3, 9, 12)]
assert SparseMatrix.eye(2).nnz() == 2
def test_transpose():
assert SparseMatrix(((1, 2), (3, 4))).transpose() == \
SparseMatrix(((1, 3), (2, 4)))
def test_trace():
assert SparseMatrix(((1, 2), (3, 4))).trace() == 5
assert SparseMatrix(((0, 0), (0, 4))).trace() == 4
def test_CL_RL():
assert SparseMatrix(((1, 2), (3, 4))).row_list() == \
[(0, 0, 1), (0, 1, 2), (1, 0, 3), (1, 1, 4)]
assert SparseMatrix(((1, 2), (3, 4))).col_list() == \
[(0, 0, 1), (1, 0, 3), (0, 1, 2), (1, 1, 4)]
def test_add():
assert SparseMatrix(((1, 0), (0, 1))) + SparseMatrix(((0, 1), (1, 0))) == \
SparseMatrix(((1, 1), (1, 1)))
a = SparseMatrix(100, 100, lambda i, j: int(j != 0 and i % j == 0))
b = SparseMatrix(100, 100, lambda i, j: int(i != 0 and j % i == 0))
assert (len(a._smat) + len(b._smat) - len((a + b)._smat) > 0)
def test_errors():
raises(ValueError, lambda: SparseMatrix(1.4, 2, lambda i, j: 0))
raises(TypeError, lambda: SparseMatrix([1, 2, 3], [1, 2]))
raises(ValueError, lambda: SparseMatrix([[1, 2], [3, 4]])[(1, 2, 3)])
raises(IndexError, lambda: SparseMatrix([[1, 2], [3, 4]])[5])
raises(ValueError, lambda: SparseMatrix([[1, 2], [3, 4]])[1, 2, 3])
raises(TypeError,
lambda: SparseMatrix([[1, 2], [3, 4]]).copyin_list([0, 1], set([])))
raises(
IndexError, lambda: SparseMatrix([[1, 2], [3, 4]])[1, 2])
raises(TypeError, lambda: SparseMatrix([1, 2, 3]).cross(1))
raises(IndexError, lambda: SparseMatrix(1, 2, [1, 2])[3])
raises(ShapeError,
lambda: SparseMatrix(1, 2, [1, 2]) + SparseMatrix(2, 1, [2, 1]))
def test_len():
assert not SparseMatrix()
assert SparseMatrix() == SparseMatrix([])
assert SparseMatrix() == SparseMatrix([[]])
def test_sparse_zeros_sparse_eye():
assert SparseMatrix.eye(3) == eye(3, cls=SparseMatrix)
assert len(SparseMatrix.eye(3)._smat) == 3
assert SparseMatrix.zeros(3) == zeros(3, cls=SparseMatrix)
assert len(SparseMatrix.zeros(3)._smat) == 0
def test_copyin():
s = SparseMatrix(3, 3, {})
s[1, 0] = 1
assert s[:, 0] == SparseMatrix(Matrix([0, 1, 0]))
assert s[3] == 1
assert s[3: 4] == [1]
s[1, 1] = 42
assert s[1, 1] == 42
assert s[1, 1:] == SparseMatrix([[42, 0]])
s[1, 1:] = Matrix([[5, 6]])
assert s[1, :] == SparseMatrix([[1, 5, 6]])
s[1, 1:] = [[42, 43]]
assert s[1, :] == SparseMatrix([[1, 42, 43]])
s[0, 0] = 17
assert s[:, :1] == SparseMatrix([17, 1, 0])
s[0, 0] = [1, 1, 1]
assert s[:, 0] == SparseMatrix([1, 1, 1])
s[0, 0] = Matrix([1, 1, 1])
assert s[:, 0] == SparseMatrix([1, 1, 1])
s[0, 0] = SparseMatrix([1, 1, 1])
assert s[:, 0] == SparseMatrix([1, 1, 1])
def test_sparse_solve():
from sympy.matrices import SparseMatrix
A = SparseMatrix(((25, 15, -5), (15, 18, 0), (-5, 0, 11)))
assert A.cholesky() == Matrix([
[ 5, 0, 0],
[ 3, 3, 0],
[-1, 1, 3]])
assert A.cholesky() * A.cholesky().T == Matrix([
[25, 15, -5],
[15, 18, 0],
[-5, 0, 11]])
A = SparseMatrix(((25, 15, -5), (15, 18, 0), (-5, 0, 11)))
L, D = A.LDLdecomposition()
assert 15*L == Matrix([
[15, 0, 0],
[ 9, 15, 0],
[-3, 5, 15]])
assert D == Matrix([
[25, 0, 0],
[ 0, 9, 0],
[ 0, 0, 9]])
assert L * D * L.T == A
A = SparseMatrix(((3, 0, 2), (0, 0, 1), (1, 2, 0)))
assert A.inv() * A == SparseMatrix(eye(3))
A = SparseMatrix([
[ 2, -1, 0],
[-1, 2, -1],
[ 0, 0, 2]])
ans = SparseMatrix([
[S(2)/3, S(1)/3, S(1)/6],
[S(1)/3, S(2)/3, S(1)/3],
[ 0, 0, S(1)/2]])
assert A.inv(method='CH') == ans
assert A.inv(method='LDL') == ans
assert A * ans == SparseMatrix(eye(3))
s = A.solve(A[:, 0], 'LDL')
assert A*s == A[:, 0]
s = A.solve(A[:, 0], 'CH')
assert A*s == A[:, 0]
A = A.col_join(A)
s = A.solve_least_squares(A[:, 0], 'CH')
assert A*s == A[:, 0]
s = A.solve_least_squares(A[:, 0], 'LDL')
assert A*s == A[:, 0]
def test_lower_triangular_solve():
a, b, c, d = symbols('a:d')
u, v, w, x = symbols('u:x')
A = SparseMatrix([[a, 0], [c, d]])
B = MutableSparseMatrix([[u, v], [w, x]])
C = ImmutableSparseMatrix([[u, v], [w, x]])
sol = Matrix([[u/a, v/a], [(w - c*u/a)/d, (x - c*v/a)/d]])
assert A.lower_triangular_solve(B) == sol
assert A.lower_triangular_solve(C) == sol
def test_upper_triangular_solve():
a, b, c, d = symbols('a:d')
u, v, w, x = symbols('u:x')
A = SparseMatrix([[a, b], [0, d]])
B = MutableSparseMatrix([[u, v], [w, x]])
C = ImmutableSparseMatrix([[u, v], [w, x]])
sol = Matrix([[(u - b*w/d)/a, (v - b*x/d)/a], [w/d, x/d]])
assert A.upper_triangular_solve(B) == sol
assert A.upper_triangular_solve(C) == sol
def test_diagonal_solve():
a, d = symbols('a d')
u, v, w, x = symbols('u:x')
A = SparseMatrix([[a, 0], [0, d]])
B = MutableSparseMatrix([[u, v], [w, x]])
C = ImmutableSparseMatrix([[u, v], [w, x]])
sol = Matrix([[u/a, v/a], [w/d, x/d]])
assert A.diagonal_solve(B) == sol
assert A.diagonal_solve(C) == sol
def test_hermitian():
x = Symbol('x')
a = SparseMatrix([[0, I], [-I, 0]])
assert a.is_hermitian
a = SparseMatrix([[1, I], [-I, 1]])
assert a.is_hermitian
a[0, 0] = 2*I
assert a.is_hermitian is False
a[0, 0] = x
assert a.is_hermitian is None
a[0, 1] = a[1, 0]*I
assert a.is_hermitian is False
|
d4e944bf4a6f0e3c6823e1acb0e6793d52175bc73466e98b8b622e6a49ef2ec0 | from sympy import Symbol, Poly
from sympy.polys.solvers import RawMatrix as Matrix
from sympy.matrices.normalforms import invariant_factors, smith_normal_form
from sympy.polys.domains import ZZ, QQ
def test_smith_normal():
m = Matrix([[12, 6, 4,8],[3,9,6,12],[2,16,14,28],[20,10,10,20]])
setattr(m, 'ring', ZZ)
smf = Matrix([[1, 0, 0, 0], [0, 10, 0, 0], [0, 0, -30, 0], [0, 0, 0, 0]])
assert smith_normal_form(m) == smf
x = Symbol('x')
m = Matrix([[Poly(x-1), Poly(1, x),Poly(-1,x)],
[0, Poly(x), Poly(-1,x)],
[Poly(0,x),Poly(-1,x),Poly(x)]])
setattr(m, 'ring', QQ[x])
invs = (Poly(1, x), Poly(x - 1), Poly(x**2 - 1))
assert invariant_factors(m) == invs
m = Matrix([[2, 4]])
setattr(m, 'ring', ZZ)
smf = Matrix([[2, 0]])
assert smith_normal_form(m) == smf
|
4d9a676298c2491e001a690abd70c45ea412c0e43e421510fb541498b91dcd11 | from sympy.utilities.pytest import ignore_warnings
from sympy.utilities.exceptions import SymPyDeprecationWarning
with ignore_warnings(SymPyDeprecationWarning):
from sympy.matrices.densetools import eye
from sympy.matrices.densearith import add, sub, mulmatmat, mulmatscaler
from sympy import ZZ
def test_add():
a = [[ZZ(3), ZZ(7), ZZ(4)], [ZZ(2), ZZ(4), ZZ(5)], [ZZ(6), ZZ(2), ZZ(3)]]
b = [[ZZ(5), ZZ(4), ZZ(9)], [ZZ(3), ZZ(7), ZZ(1)], [ZZ(12), ZZ(13), ZZ(14)]]
c = [[ZZ(12)], [ZZ(17)], [ZZ(21)]]
d = [[ZZ(3)], [ZZ(4)], [ZZ(5)]]
e = [[ZZ(12), ZZ(78)], [ZZ(56), ZZ(79)]]
f = [[ZZ.zero, ZZ.zero], [ZZ.zero, ZZ.zero]]
assert add(a, b, ZZ) == [[ZZ(8), ZZ(11), ZZ(13)], [ZZ(5), ZZ(11), ZZ(6)], [ZZ(18), ZZ(15), ZZ(17)]]
assert add(c, d, ZZ) == [[ZZ(15)], [ZZ(21)], [ZZ(26)]]
assert add(e, f, ZZ) == e
def test_sub():
a = [[ZZ(3), ZZ(7), ZZ(4)], [ZZ(2), ZZ(4), ZZ(5)], [ZZ(6), ZZ(2), ZZ(3)]]
b = [[ZZ(5), ZZ(4), ZZ(9)], [ZZ(3), ZZ(7), ZZ(1)], [ZZ(12), ZZ(13), ZZ(14)]]
c = [[ZZ(12)], [ZZ(17)], [ZZ(21)]]
d = [[ZZ(3)], [ZZ(4)], [ZZ(5)]]
e = [[ZZ(12), ZZ(78)], [ZZ(56), ZZ(79)]]
f = [[ZZ.zero, ZZ.zero], [ZZ.zero, ZZ.zero]]
assert sub(a, b, ZZ) == [[ZZ(-2), ZZ(3), ZZ(-5)], [ZZ(-1), ZZ(-3), ZZ(4)], [ZZ(-6), ZZ(-11), ZZ(-11)]]
assert sub(c, d, ZZ) == [[ZZ(9)], [ZZ(13)], [ZZ(16)]]
assert sub(e, f, ZZ) == e
def test_mulmatmat():
a = [[ZZ(3), ZZ(4)], [ZZ(5), ZZ(6)]]
b = [[ZZ(1), ZZ(2)], [ZZ(7), ZZ(8)]]
c = eye(2, ZZ)
d = [[ZZ(6)], [ZZ(7)]]
assert mulmatmat(a, b, ZZ) == [[ZZ(31), ZZ(38)], [ZZ(47), ZZ(58)]]
assert mulmatmat(a, c, ZZ) == [[ZZ(3), ZZ(4)], [ZZ(5), ZZ(6)]]
assert mulmatmat(b, d, ZZ) == [[ZZ(20)], [ZZ(98)]]
def test_mulmatscaler():
a = eye(3, ZZ)
b = [[ZZ(3), ZZ(7), ZZ(4)], [ZZ(2), ZZ(4), ZZ(5)], [ZZ(6), ZZ(2), ZZ(3)]]
assert mulmatscaler(a, ZZ(4), ZZ) == [[ZZ(4), ZZ(0), ZZ(0)], [ZZ(0), ZZ(4), ZZ(0)], [ZZ(0), ZZ(0), ZZ(4)]]
assert mulmatscaler(b, ZZ(1), ZZ) == [[ZZ(3), ZZ(7), ZZ(4)], [ZZ(2), ZZ(4), ZZ(5)], [ZZ(6), ZZ(2), ZZ(3)]]
|
223da0e15ca80b5debdce10a92dfa28885338d7be15f8f8b8e88e6b43911d09c | import random
from sympy import (
Abs, Add, E, Float, I, Integer, Max, Min, N, Poly, Pow, PurePoly, Rational,
S, Symbol, cos, exp, log, expand_mul, oo, pi, signsimp, simplify, sin,
sqrt, symbols, sympify, trigsimp, tan, sstr, diff, Function)
from sympy.matrices.matrices import (ShapeError, MatrixError,
NonSquareMatrixError, DeferredVector, _find_reasonable_pivot_naive,
_simplify)
from sympy.matrices import (
GramSchmidt, ImmutableMatrix, ImmutableSparseMatrix, Matrix,
SparseMatrix, casoratian, diag, eye, hessian,
matrix_multiply_elementwise, ones, randMatrix, rot_axis1, rot_axis2,
rot_axis3, wronskian, zeros, MutableDenseMatrix, ImmutableDenseMatrix, MatrixSymbol)
from sympy.core.compatibility import long, iterable, range, Hashable
from sympy.core import Tuple, Wild
from sympy.functions.special.tensor_functions import KroneckerDelta
from sympy.utilities.iterables import flatten, capture
from sympy.utilities.pytest import raises, XFAIL, skip, warns_deprecated_sympy
from sympy.solvers import solve
from sympy.assumptions import Q
from sympy.tensor.array import Array
from sympy.matrices.expressions import MatPow
from sympy.abc import a, b, c, d, x, y, z, t
# don't re-order this list
classes = (Matrix, SparseMatrix, ImmutableMatrix, ImmutableSparseMatrix)
def test_args():
for c, cls in enumerate(classes):
m = cls.zeros(3, 2)
# all should give back the same type of arguments, e.g. ints for shape
assert m.shape == (3, 2) and all(type(i) is int for i in m.shape)
assert m.rows == 3 and type(m.rows) is int
assert m.cols == 2 and type(m.cols) is int
if not c % 2:
assert type(m._mat) in (list, tuple, Tuple)
else:
assert type(m._smat) is dict
def test_division():
v = Matrix(1, 2, [x, y])
assert v.__div__(z) == Matrix(1, 2, [x/z, y/z])
assert v.__truediv__(z) == Matrix(1, 2, [x/z, y/z])
assert v/z == Matrix(1, 2, [x/z, y/z])
def test_sum():
m = Matrix([[1, 2, 3], [x, y, x], [2*y, -50, z*x]])
assert m + m == Matrix([[2, 4, 6], [2*x, 2*y, 2*x], [4*y, -100, 2*z*x]])
n = Matrix(1, 2, [1, 2])
raises(ShapeError, lambda: m + n)
def test_abs():
m = Matrix(1, 2, [-3, x])
n = Matrix(1, 2, [3, Abs(x)])
assert abs(m) == n
def test_addition():
a = Matrix((
(1, 2),
(3, 1),
))
b = Matrix((
(1, 2),
(3, 0),
))
assert a + b == a.add(b) == Matrix([[2, 4], [6, 1]])
def test_fancy_index_matrix():
for M in (Matrix, SparseMatrix):
a = M(3, 3, range(9))
assert a == a[:, :]
assert a[1, :] == Matrix(1, 3, [3, 4, 5])
assert a[:, 1] == Matrix([1, 4, 7])
assert a[[0, 1], :] == Matrix([[0, 1, 2], [3, 4, 5]])
assert a[[0, 1], 2] == a[[0, 1], [2]]
assert a[2, [0, 1]] == a[[2], [0, 1]]
assert a[:, [0, 1]] == Matrix([[0, 1], [3, 4], [6, 7]])
assert a[0, 0] == 0
assert a[0:2, :] == Matrix([[0, 1, 2], [3, 4, 5]])
assert a[:, 0:2] == Matrix([[0, 1], [3, 4], [6, 7]])
assert a[::2, 1] == a[[0, 2], 1]
assert a[1, ::2] == a[1, [0, 2]]
a = M(3, 3, range(9))
assert a[[0, 2, 1, 2, 1], :] == Matrix([
[0, 1, 2],
[6, 7, 8],
[3, 4, 5],
[6, 7, 8],
[3, 4, 5]])
assert a[:, [0,2,1,2,1]] == Matrix([
[0, 2, 1, 2, 1],
[3, 5, 4, 5, 4],
[6, 8, 7, 8, 7]])
a = SparseMatrix.zeros(3)
a[1, 2] = 2
a[0, 1] = 3
a[2, 0] = 4
assert a.extract([1, 1], [2]) == Matrix([
[2],
[2]])
assert a.extract([1, 0], [2, 2, 2]) == Matrix([
[2, 2, 2],
[0, 0, 0]])
assert a.extract([1, 0, 1, 2], [2, 0, 1, 0]) == Matrix([
[2, 0, 0, 0],
[0, 0, 3, 0],
[2, 0, 0, 0],
[0, 4, 0, 4]])
def test_multiplication():
a = Matrix((
(1, 2),
(3, 1),
(0, 6),
))
b = Matrix((
(1, 2),
(3, 0),
))
c = a*b
assert c[0, 0] == 7
assert c[0, 1] == 2
assert c[1, 0] == 6
assert c[1, 1] == 6
assert c[2, 0] == 18
assert c[2, 1] == 0
try:
eval('c = a @ b')
except SyntaxError:
pass
else:
assert c[0, 0] == 7
assert c[0, 1] == 2
assert c[1, 0] == 6
assert c[1, 1] == 6
assert c[2, 0] == 18
assert c[2, 1] == 0
h = matrix_multiply_elementwise(a, c)
assert h == a.multiply_elementwise(c)
assert h[0, 0] == 7
assert h[0, 1] == 4
assert h[1, 0] == 18
assert h[1, 1] == 6
assert h[2, 0] == 0
assert h[2, 1] == 0
raises(ShapeError, lambda: matrix_multiply_elementwise(a, b))
c = b * Symbol("x")
assert isinstance(c, Matrix)
assert c[0, 0] == x
assert c[0, 1] == 2*x
assert c[1, 0] == 3*x
assert c[1, 1] == 0
c2 = x * b
assert c == c2
c = 5 * b
assert isinstance(c, Matrix)
assert c[0, 0] == 5
assert c[0, 1] == 2*5
assert c[1, 0] == 3*5
assert c[1, 1] == 0
try:
eval('c = 5 @ b')
except SyntaxError:
pass
else:
assert isinstance(c, Matrix)
assert c[0, 0] == 5
assert c[0, 1] == 2*5
assert c[1, 0] == 3*5
assert c[1, 1] == 0
def test_power():
raises(NonSquareMatrixError, lambda: Matrix((1, 2))**2)
R = Rational
A = Matrix([[2, 3], [4, 5]])
assert (A**-3)[:] == [R(-269)/8, R(153)/8, R(51)/2, R(-29)/2]
assert (A**5)[:] == [6140, 8097, 10796, 14237]
A = Matrix([[2, 1, 3], [4, 2, 4], [6, 12, 1]])
assert (A**3)[:] == [290, 262, 251, 448, 440, 368, 702, 954, 433]
assert A**0 == eye(3)
assert A**1 == A
assert (Matrix([[2]]) ** 100)[0, 0] == 2**100
assert eye(2)**10000000 == eye(2)
assert Matrix([[1, 2], [3, 4]])**Integer(2) == Matrix([[7, 10], [15, 22]])
A = Matrix([[33, 24], [48, 57]])
assert (A**(S(1)/2))[:] == [5, 2, 4, 7]
A = Matrix([[0, 4], [-1, 5]])
assert (A**(S(1)/2))**2 == A
assert Matrix([[1, 0], [1, 1]])**(S(1)/2) == Matrix([[1, 0], [S.Half, 1]])
assert Matrix([[1, 0], [1, 1]])**0.5 == Matrix([[1.0, 0], [0.5, 1.0]])
from sympy.abc import a, b, n
assert Matrix([[1, a], [0, 1]])**n == Matrix([[1, a*n], [0, 1]])
assert Matrix([[b, a], [0, b]])**n == Matrix([[b**n, a*b**(n-1)*n], [0, b**n]])
assert Matrix([[a, 1, 0], [0, a, 1], [0, 0, a]])**n == Matrix([
[a**n, a**(n-1)*n, a**(n-2)*(n-1)*n/2],
[0, a**n, a**(n-1)*n],
[0, 0, a**n]])
assert Matrix([[a, 1, 0], [0, a, 0], [0, 0, b]])**n == Matrix([
[a**n, a**(n-1)*n, 0],
[0, a**n, 0],
[0, 0, b**n]])
A = Matrix([[1, 0], [1, 7]])
assert A._matrix_pow_by_jordan_blocks(S(3)) == A._eval_pow_by_recursion(3)
A = Matrix([[2]])
assert A**10 == Matrix([[2**10]]) == A._matrix_pow_by_jordan_blocks(S(10)) == \
A._eval_pow_by_recursion(10)
# testing a matrix that cannot be jordan blocked issue 11766
m = Matrix([[3, 0, 0, 0, -3], [0, -3, -3, 0, 3], [0, 3, 0, 3, 0], [0, 0, 3, 0, 3], [3, 0, 0, 3, 0]])
raises(MatrixError, lambda: m._matrix_pow_by_jordan_blocks(S(10)))
# test issue 11964
raises(MatrixError, lambda: Matrix([[1, 1], [3, 3]])._matrix_pow_by_jordan_blocks(S(-10)))
A = Matrix([[0, 1, 0], [0, 0, 1], [0, 0, 0]]) # Nilpotent jordan block size 3
assert A**10.0 == Matrix([[0, 0, 0], [0, 0, 0], [0, 0, 0]])
raises(ValueError, lambda: A**2.1)
raises(ValueError, lambda: A**(S(3)/2))
A = Matrix([[8, 1], [3, 2]])
assert A**10.0 == Matrix([[1760744107, 272388050], [817164150, 126415807]])
A = Matrix([[0, 0, 1], [0, 0, 1], [0, 0, 1]]) # Nilpotent jordan block size 1
assert A**10.0 == Matrix([[0, 0, 1], [0, 0, 1], [0, 0, 1]])
A = Matrix([[0, 1, 0], [0, 0, 1], [0, 0, 1]]) # Nilpotent jordan block size 2
assert A**10.0 == Matrix([[0, 0, 1], [0, 0, 1], [0, 0, 1]])
n = Symbol('n', integer=True)
assert isinstance(A**n, MatPow)
n = Symbol('n', integer=True, negative=True)
raises(ValueError, lambda: A**n)
n = Symbol('n', integer=True, nonnegative=True)
assert A**n == Matrix([
[KroneckerDelta(0, n), KroneckerDelta(1, n), -KroneckerDelta(0, n) - KroneckerDelta(1, n) + 1],
[ 0, KroneckerDelta(0, n), 1 - KroneckerDelta(0, n)],
[ 0, 0, 1]])
assert A**(n + 2) == Matrix([[0, 0, 1], [0, 0, 1], [0, 0, 1]])
raises(ValueError, lambda: A**(S(3)/2))
A = Matrix([[0, 0, 1], [3, 0, 1], [4, 3, 1]])
assert A**5.0 == Matrix([[168, 72, 89], [291, 144, 161], [572, 267, 329]])
assert A**5.0 == A**5
A = Matrix([[0, 1, 0],[-1, 0, 0],[0, 0, 0]])
n = Symbol("n")
An = A**n
assert An.subs(n, 2).doit() == A**2
raises(ValueError, lambda: An.subs(n, -2).doit())
assert An * An == A**(2*n)
# concretizing behavior for non-integer and complex powers
A = Matrix([[0,0,0],[0,0,0],[0,0,0]])
n = Symbol('n', integer=True, positive=True)
assert A**n == A
n = Symbol('n', integer=True, nonnegative=True)
assert A**n == diag(0**n, 0**n, 0**n)
assert (A**n).subs(n, 0) == eye(3)
assert (A**n).subs(n, 1) == zeros(3)
A = Matrix ([[2,0,0],[0,2,0],[0,0,2]])
assert A**2.1 == diag (2**2.1, 2**2.1, 2**2.1)
assert A**I == diag (2**I, 2**I, 2**I)
A = Matrix([[0, 1, 0], [0, 0, 1], [0, 0, 1]])
raises(ValueError, lambda: A**2.1)
raises(ValueError, lambda: A**I)
A = Matrix([[S.Half, S.Half], [S.Half, S.Half]])
assert A**S.Half == A
A = Matrix([[1, 1],[3, 3]])
assert A**S.Half == Matrix ([[S.Half, S.Half], [3*S.Half, 3*S.Half]])
@XFAIL
def test_issue_17247_expression_blowup_1():
M = Matrix([[1+x, 1-x], [1-x, 1+x]])
assert exp(M).expand() == Matrix([
[ (exp(2*x) + exp(2))/2, (-exp(2*x) + exp(2))/2],
[(-exp(2*x) + exp(2))/2, (exp(2*x) + exp(2))/2]])
@XFAIL
def test_issue_17247_expression_blowup_2():
M = Matrix([[1+x, 1-x], [1-x, 1+x]])
P, J = M.jordan_form ()
assert P*J*P.inv() == M
@XFAIL
def test_issue_17247_expression_blowup_3():
M = Matrix([[1+x, 1-x], [1-x, 1+x]])
assert M**100 == Matrix([
[633825300114114700748351602688*x**100 + 633825300114114700748351602688, 633825300114114700748351602688 - 633825300114114700748351602688*x**100],
[633825300114114700748351602688 - 633825300114114700748351602688*x**100, 633825300114114700748351602688*x**100 + 633825300114114700748351602688]])
# This test commented out because it takes extremely long on current master,
# it is here for testing when eventually matrix multiplication gets optimized.
# def test_issue_17247_expression_blowup_4():
# M = Matrix(S('''[
# [ -3/4, 45/32 - 37*I/16, 1/4 + I/2, -129/64 - 9*I/64, 1/4 - 5*I/16, 65/128 + 87*I/64, -9/32 - I/16, 183/256 - 97*I/128, 3/64 + 13*I/64, -23/32 - 59*I/256, 15/128 - 3*I/32, 19/256 + 551*I/1024],
# [-149/64 + 49*I/32, -177/128 - 1369*I/128, 125/64 + 87*I/64, -2063/256 + 541*I/128, 85/256 - 33*I/16, 805/128 + 2415*I/512, -219/128 + 115*I/256, 6301/4096 - 6609*I/1024, 119/128 + 143*I/128, -10879/2048 + 4343*I/4096, 129/256 - 549*I/512, 42533/16384 + 29103*I/8192],
# [ 1/2 - I, 9/4 + 55*I/16, -3/4, 45/32 - 37*I/16, 1/4 + I/2, -129/64 - 9*I/64, 1/4 - 5*I/16, 65/128 + 87*I/64, -9/32 - I/16, 183/256 - 97*I/128, 3/64 + 13*I/64, -23/32 - 59*I/256],
# [ -5/8 - 39*I/16, 2473/256 + 137*I/64, -149/64 + 49*I/32, -177/128 - 1369*I/128, 125/64 + 87*I/64, -2063/256 + 541*I/128, 85/256 - 33*I/16, 805/128 + 2415*I/512, -219/128 + 115*I/256, 6301/4096 - 6609*I/1024, 119/128 + 143*I/128, -10879/2048 + 4343*I/4096],
# [ 1 + I, -19/4 + 5*I/4, 1/2 - I, 9/4 + 55*I/16, -3/4, 45/32 - 37*I/16, 1/4 + I/2, -129/64 - 9*I/64, 1/4 - 5*I/16, 65/128 + 87*I/64, -9/32 - I/16, 183/256 - 97*I/128],
# [ 21/8 + I, -537/64 + 143*I/16, -5/8 - 39*I/16, 2473/256 + 137*I/64, -149/64 + 49*I/32, -177/128 - 1369*I/128, 125/64 + 87*I/64, -2063/256 + 541*I/128, 85/256 - 33*I/16, 805/128 + 2415*I/512, -219/128 + 115*I/256, 6301/4096 - 6609*I/1024],
# [ -2, 17/4 - 13*I/2, 1 + I, -19/4 + 5*I/4, 1/2 - I, 9/4 + 55*I/16, -3/4, 45/32 - 37*I/16, 1/4 + I/2, -129/64 - 9*I/64, 1/4 - 5*I/16, 65/128 + 87*I/64],
# [ 1/4 + 13*I/4, -825/64 - 147*I/32, 21/8 + I, -537/64 + 143*I/16, -5/8 - 39*I/16, 2473/256 + 137*I/64, -149/64 + 49*I/32, -177/128 - 1369*I/128, 125/64 + 87*I/64, -2063/256 + 541*I/128, 85/256 - 33*I/16, 805/128 + 2415*I/512],
# [ -4*I, 27/2 + 6*I, -2, 17/4 - 13*I/2, 1 + I, -19/4 + 5*I/4, 1/2 - I, 9/4 + 55*I/16, -3/4, 45/32 - 37*I/16, 1/4 + I/2, -129/64 - 9*I/64],
# [ 1/4 + 5*I/2, -23/8 - 57*I/16, 1/4 + 13*I/4, -825/64 - 147*I/32, 21/8 + I, -537/64 + 143*I/16, -5/8 - 39*I/16, 2473/256 + 137*I/64, -149/64 + 49*I/32, -177/128 - 1369*I/128, 125/64 + 87*I/64, -2063/256 + 541*I/128],
# [ -4, 9 - 5*I, -4*I, 27/2 + 6*I, -2, 17/4 - 13*I/2, 1 + I, -19/4 + 5*I/4, 1/2 - I, 9/4 + 55*I/16, -3/4, 45/32 - 37*I/16],
# [ -2*I, 119/8 + 29*I/4, 1/4 + 5*I/2, -23/8 - 57*I/16, 1/4 + 13*I/4, -825/64 - 147*I/32, 21/8 + I, -537/64 + 143*I/16, -5/8 - 39*I/16, 2473/256 + 137*I/64, -149/64 + 49*I/32, -177/128 - 1369*I/128]]'''))
# assert (M**10).expand() == Matrix([
# [ 7*(-221393644768594642173548179825793834595 - 1861633166167425978847110897013541127952*I)/9671406556917033397649408, 15*(31670992489131684885307005100073928751695 + 10329090958303458811115024718207404523808*I)/77371252455336267181195264, 7*(-3710978679372178839237291049477017392703 + 1377706064483132637295566581525806894169*I)/19342813113834066795298816, (9727707023582419994616144751727760051598 - 59261571067013123836477348473611225724433*I)/9671406556917033397649408, (31896723509506857062605551443641668183707 + 54643444538699269118869436271152084599580*I)/38685626227668133590597632, (-2024044860947539028275487595741003997397402 + 130959428791783397562960461903698670485863*I)/309485009821345068724781056, 3*(26190251453797590396533756519358368860907 - 27221191754180839338002754608545400941638*I)/77371252455336267181195264, (1154643595139959842768960128434994698330461 + 3385496216250226964322872072260446072295634*I)/618970019642690137449562112, 3*(-31849347263064464698310044805285774295286 - 11877437776464148281991240541742691164309*I)/77371252455336267181195264, (4661330392283532534549306589669150228040221 - 4171259766019818631067810706563064103956871*I)/1237940039285380274899124224, (9598353794289061833850770474812760144506 + 358027153990999990968244906482319780943983*I)/309485009821345068724781056, (-9755135335127734571547571921702373498554177 - 4837981372692695195747379349593041939686540*I)/2475880078570760549798248448],
# [(-379516731607474268954110071392894274962069 - 422272153179747548473724096872271700878296*I)/77371252455336267181195264, (41324748029613152354787280677832014263339501 - 12715121258662668420833935373453570749288074*I)/1237940039285380274899124224, (-339216903907423793947110742819264306542397 + 494174755147303922029979279454787373566517*I)/77371252455336267181195264, (-18121350839962855576667529908850640619878381 - 37413012454129786092962531597292531089199003*I)/1237940039285380274899124224, (2489661087330511608618880408199633556675926 + 1137821536550153872137379935240732287260863*I)/309485009821345068724781056, (-136644109701594123227587016790354220062972119 + 110130123468183660555391413889600443583585272*I)/4951760157141521099596496896, (1488043981274920070468141664150073426459593 - 9691968079933445130866371609614474474327650*I)/1237940039285380274899124224, 27*(4636797403026872518131756991410164760195942 + 3369103221138229204457272860484005850416533*I)/4951760157141521099596496896, (-8534279107365915284081669381642269800472363 + 2241118846262661434336333368511372725482742*I)/1237940039285380274899124224, (60923350128174260992536531692058086830950875 - 263673488093551053385865699805250505661590126*I)/9903520314283042199192993792, (18520943561240714459282253753348921824172569 + 24846649186468656345966986622110971925703604*I)/4951760157141521099596496896, (-232781130692604829085973604213529649638644431 + 35981505277760667933017117949103953338570617*I)/9903520314283042199192993792],
# [ (8742968295129404279528270438201520488950 + 3061473358639249112126847237482570858327*I)/4835703278458516698824704, (-245657313712011778432792959787098074935273 + 253113767861878869678042729088355086740856*I)/38685626227668133590597632, (1947031161734702327107371192008011621193 - 19462330079296259148177542369999791122762*I)/9671406556917033397649408, (552856485625209001527688949522750288619217 + 392928441196156725372494335248099016686580*I)/77371252455336267181195264, (-44542866621905323121630214897126343414629 + 3265340021421335059323962377647649632959*I)/19342813113834066795298816, (136272594005759723105646069956434264218730 - 330975364731707309489523680957584684763587*I)/38685626227668133590597632, (27392593965554149283318732469825168894401 + 75157071243800133880129376047131061115278*I)/38685626227668133590597632, 7*(-357821652913266734749960136017214096276154 - 45509144466378076475315751988405961498243*I)/309485009821345068724781056, (104485001373574280824835174390219397141149 - 99041000529599568255829489765415726168162*I)/77371252455336267181195264, (1198066993119982409323525798509037696321291 + 4249784165667887866939369628840569844519936*I)/618970019642690137449562112, (-114985392587849953209115599084503853611014 - 52510376847189529234864487459476242883449*I)/77371252455336267181195264, (6094620517051332877965959223269600650951573 - 4683469779240530439185019982269137976201163*I)/1237940039285380274899124224],
# [ (611292255597977285752123848828590587708323 - 216821743518546668382662964473055912169502*I)/77371252455336267181195264, (-1144023204575811464652692396337616594307487 + 12295317806312398617498029126807758490062855*I)/309485009821345068724781056, (-374093027769390002505693378578475235158281 - 573533923565898290299607461660384634333639*I)/77371252455336267181195264, (47405570632186659000138546955372796986832987 - 2837476058950808941605000274055970055096534*I)/1237940039285380274899124224, (-571573207393621076306216726219753090535121 + 533381457185823100878764749236639320783831*I)/77371252455336267181195264, (-7096548151856165056213543560958582513797519 - 24035731898756040059329175131592138642195366*I)/618970019642690137449562112, (2396762128833271142000266170154694033849225 + 1448501087375679588770230529017516492953051*I)/309485009821345068724781056, (-150609293845161968447166237242456473262037053 + 92581148080922977153207018003184520294188436*I)/4951760157141521099596496896, 5*(270278244730804315149356082977618054486347 - 1997830155222496880429743815321662710091562*I)/1237940039285380274899124224, (62978424789588828258068912690172109324360330 + 44803641177219298311493356929537007630129097*I)/2475880078570760549798248448, 19*(-451431106327656743945775812536216598712236 + 114924966793632084379437683991151177407937*I)/1237940039285380274899124224, (63417747628891221594106738815256002143915995 - 261508229397507037136324178612212080871150958*I)/9903520314283042199192993792],
# [ (-2144231934021288786200752920446633703357 + 2305614436009705803670842248131563850246*I)/1208925819614629174706176, (-90720949337459896266067589013987007078153 - 221951119475096403601562347412753844534569*I)/19342813113834066795298816, (11590973613116630788176337262688659880376 + 6514520676308992726483494976339330626159*I)/4835703278458516698824704, 3*(-131776217149000326618649542018343107657237 + 79095042939612668486212006406818285287004*I)/38685626227668133590597632, (10100577916793945997239221374025741184951 - 28631383488085522003281589065994018550748*I)/9671406556917033397649408, 67*(10090295594251078955008130473573667572549 + 10449901522697161049513326446427839676762*I)/77371252455336267181195264, (-54270981296988368730689531355811033930513 - 3413683117592637309471893510944045467443*I)/19342813113834066795298816, (440372322928679910536575560069973699181278 - 736603803202303189048085196176918214409081*I)/77371252455336267181195264, (33220374714789391132887731139763250155295 + 92055083048787219934030779066298919603554*I)/38685626227668133590597632, 5*(-594638554579967244348856981610805281527116 - 82309245323128933521987392165716076704057*I)/309485009821345068724781056, (128056368815300084550013708313312073721955 - 114619107488668120303579745393765245911404*I)/77371252455336267181195264, 21*(59839959255173222962789517794121843393573 + 241507883613676387255359616163487405826334*I)/618970019642690137449562112],
# [ (-13454485022325376674626653802541391955147 + 184471402121905621396582628515905949793486*I)/19342813113834066795298816, (-6158730123400322562149780662133074862437105 - 3416173052604643794120262081623703514107476*I)/154742504910672534362390528, (770558003844914708453618983120686116100419 - 127758381209767638635199674005029818518766*I)/77371252455336267181195264, (-4693005771813492267479835161596671660631703 + 12703585094750991389845384539501921531449948*I)/309485009821345068724781056, (-295028157441149027913545676461260860036601 - 841544569970643160358138082317324743450770*I)/77371252455336267181195264, (56716442796929448856312202561538574275502893 + 7216818824772560379753073185990186711454778*I)/1237940039285380274899124224, 15*(-87061038932753366532685677510172566368387 + 61306141156647596310941396434445461895538*I)/154742504910672534362390528, (-3455315109680781412178133042301025723909347 - 24969329563196972466388460746447646686670670*I)/618970019642690137449562112, (2453418854160886481106557323699250865361849 + 1497886802326243014471854112161398141242514*I)/309485009821345068724781056, (-151343224544252091980004429001205664193082173 + 90471883264187337053549090899816228846836628*I)/4951760157141521099596496896, (1652018205533026103358164026239417416432989 - 9959733619236515024261775397109724431400162*I)/1237940039285380274899124224, 3*(40676374242956907656984876692623172736522006 + 31023357083037817469535762230872667581366205*I)/4951760157141521099596496896],
# [ (-1226990509403328460274658603410696548387 - 4131739423109992672186585941938392788458*I)/1208925819614629174706176, (162392818524418973411975140074368079662703 + 23706194236915374831230612374344230400704*I)/9671406556917033397649408, (-3935678233089814180000602553655565621193 + 2283744757287145199688061892165659502483*I)/1208925819614629174706176, (-2400210250844254483454290806930306285131 - 315571356806370996069052930302295432758205*I)/19342813113834066795298816, (13365917938215281056563183751673390817910 + 15911483133819801118348625831132324863881*I)/4835703278458516698824704, 3*(-215950551370668982657516660700301003897855 + 51684341999223632631602864028309400489378*I)/38685626227668133590597632, (20886089946811765149439844691320027184765 - 30806277083146786592790625980769214361844*I)/9671406556917033397649408, (562180634592713285745940856221105667874855 + 1031543963988260765153550559766662245114916*I)/77371252455336267181195264, (-65820625814810177122941758625652476012867 - 12429918324787060890804395323920477537595*I)/19342813113834066795298816, (319147848192012911298771180196635859221089 - 402403304933906769233365689834404519960394*I)/38685626227668133590597632, (23035615120921026080284733394359587955057 + 115351677687031786114651452775242461310624*I)/38685626227668133590597632, (-3426830634881892756966440108592579264936130 - 1022954961164128745603407283836365128598559*I)/309485009821345068724781056],
# [ (-192574788060137531023716449082856117537757 - 69222967328876859586831013062387845780692*I)/19342813113834066795298816, (2736383768828013152914815341491629299773262 - 2773252698016291897599353862072533475408743*I)/77371252455336267181195264, (-23280005281223837717773057436155921656805 + 214784953368021840006305033048142888879224*I)/19342813113834066795298816, (-3035247484028969580570400133318947903462326 - 2195168903335435855621328554626336958674325*I)/77371252455336267181195264, (984552428291526892214541708637840971548653 - 64006622534521425620714598573494988589378*I)/77371252455336267181195264, (-3070650452470333005276715136041262898509903 + 7286424705750810474140953092161794621989080*I)/154742504910672534362390528, (-147848877109756404594659513386972921139270 - 416306113044186424749331418059456047650861*I)/38685626227668133590597632, (55272118474097814260289392337160619494260781 + 7494019668394781211907115583302403519488058*I)/1237940039285380274899124224, (-581537886583682322424771088996959213068864 + 542191617758465339135308203815256798407429*I)/77371252455336267181195264, (-6422548983676355789975736799494791970390991 - 23524183982209004826464749309156698827737702*I)/618970019642690137449562112, 7*(180747195387024536886923192475064903482083 + 84352527693562434817771649853047924991804*I)/154742504910672534362390528, (-135485179036717001055310712747643466592387031 + 102346575226653028836678855697782273460527608*I)/4951760157141521099596496896],
# [ (3384238362616083147067025892852431152105 + 156724444932584900214919898954874618256*I)/604462909807314587353088, (-59558300950677430189587207338385764871866 + 114427143574375271097298201388331237478857*I)/4835703278458516698824704, (-1356835789870635633517710130971800616227 - 7023484098542340388800213478357340875410*I)/1208925819614629174706176, (234884918567993750975181728413524549575881 + 79757294640629983786895695752733890213506*I)/9671406556917033397649408, (-7632732774935120473359202657160313866419 + 2905452608512927560554702228553291839465*I)/1208925819614629174706176, (52291747908702842344842889809762246649489 - 520996778817151392090736149644507525892649*I)/19342813113834066795298816, (17472406829219127839967951180375981717322 + 23464704213841582137898905375041819568669*I)/4835703278458516698824704, (-911026971811893092350229536132730760943307 + 150799318130900944080399439626714846752360*I)/38685626227668133590597632, (26234457233977042811089020440646443590687 - 45650293039576452023692126463683727692890*I)/9671406556917033397649408, 3*(288348388717468992528382586652654351121357 + 454526517721403048270274049572136109264668*I)/77371252455336267181195264, (-91583492367747094223295011999405657956347 - 12704691128268298435362255538069612411331*I)/19342813113834066795298816, (411208730251327843849027957710164064354221 - 569898526380691606955496789378230959965898*I)/38685626227668133590597632],
# [ (27127513117071487872628354831658811211795 - 37765296987901990355760582016892124833857*I)/4835703278458516698824704, (1741779916057680444272938534338833170625435 + 3083041729779495966997526404685535449810378*I)/77371252455336267181195264, 3*(-60642236251815783728374561836962709533401 - 24630301165439580049891518846174101510744*I)/19342813113834066795298816, 3*(445885207364591681637745678755008757483408 - 350948497734812895032502179455610024541643*I)/38685626227668133590597632, (-47373295621391195484367368282471381775684 + 219122969294089357477027867028071400054973*I)/19342813113834066795298816, (-2801565819673198722993348253876353741520438 - 2250142129822658548391697042460298703335701*I)/77371252455336267181195264, (801448252275607253266997552356128790317119 - 50890367688077858227059515894356594900558*I)/77371252455336267181195264, (-5082187758525931944557763799137987573501207 + 11610432359082071866576699236013484487676124*I)/309485009821345068724781056, (-328925127096560623794883760398247685166830 - 643447969697471610060622160899409680422019*I)/77371252455336267181195264, 15*(2954944669454003684028194956846659916299765 + 33434406416888505837444969347824812608566*I)/1237940039285380274899124224, (-415749104352001509942256567958449835766827 + 479330966144175743357171151440020955412219*I)/77371252455336267181195264, 3*(-4639987285852134369449873547637372282914255 - 11994411888966030153196659207284951579243273*I)/1237940039285380274899124224],
# [ (-478846096206269117345024348666145495601 + 1249092488629201351470551186322814883283*I)/302231454903657293676544, (-17749319421930878799354766626365926894989 - 18264580106418628161818752318217357231971*I)/1208925819614629174706176, (2801110795431528876849623279389579072819 + 363258850073786330770713557775566973248*I)/604462909807314587353088, (-59053496693129013745775512127095650616252 + 78143588734197260279248498898321500167517*I)/4835703278458516698824704, (-283186724922498212468162690097101115349 - 6443437753863179883794497936345437398276*I)/1208925819614629174706176, (188799118826748909206887165661384998787543 + 84274736720556630026311383931055307398820*I)/9671406556917033397649408, (-5482217151670072904078758141270295025989 + 1818284338672191024475557065444481298568*I)/1208925819614629174706176, (56564463395350195513805521309731217952281 - 360208541416798112109946262159695452898431*I)/19342813113834066795298816, 11*(1259539805728870739006416869463689438068 + 1409136581547898074455004171305324917387*I)/4835703278458516698824704, 5*(-123701190701414554945251071190688818343325 + 30997157322590424677294553832111902279712*I)/38685626227668133590597632, (16130917381301373033736295883982414239781 - 32752041297570919727145380131926943374516*I)/9671406556917033397649408, (650301385108223834347093740500375498354925 + 899526407681131828596801223402866051809258*I)/77371252455336267181195264],
# [ (9011388245256140876590294262420614839483 + 8167917972423946282513000869327525382672*I)/1208925819614629174706176, (-426393174084720190126376382194036323028924 + 180692224825757525982858693158209545430621*I)/9671406556917033397649408, (24588556702197802674765733448108154175535 - 45091766022876486566421953254051868331066*I)/4835703278458516698824704, (1872113939365285277373877183750416985089691 + 3030392393733212574744122057679633775773130*I)/77371252455336267181195264, (-222173405538046189185754954524429864167549 - 75193157893478637039381059488387511299116*I)/19342813113834066795298816, (2670821320766222522963689317316937579844558 - 2645837121493554383087981511645435472169191*I)/77371252455336267181195264, 5*(-2100110309556476773796963197283876204940 + 41957457246479840487980315496957337371937*I)/19342813113834066795298816, (-5733743755499084165382383818991531258980593 - 3328949988392698205198574824396695027195732*I)/154742504910672534362390528, (707827994365259025461378911159398206329247 - 265730616623227695108042528694302299777294*I)/77371252455336267181195264, (-1442501604682933002895864804409322823788319 + 11504137805563265043376405214378288793343879*I)/309485009821345068724781056, (-56130472299445561499538726459719629522285 - 61117552419727805035810982426639329818864*I)/9671406556917033397649408, (39053692321126079849054272431599539429908717 - 10209127700342570953247177602860848130710666*I)/1237940039285380274899124224]])
def test_creation():
raises(ValueError, lambda: Matrix(5, 5, range(20)))
raises(ValueError, lambda: Matrix(5, -1, []))
raises(IndexError, lambda: Matrix((1, 2))[2])
with raises(IndexError):
Matrix((1, 2))[1:2] = 5
with raises(IndexError):
Matrix((1, 2))[3] = 5
assert Matrix() == Matrix([]) == Matrix([[]]) == Matrix(0, 0, [])
# anything can go into a matrix (laplace_transform uses tuples)
assert Matrix([[[], ()]]).tolist() == [[[], ()]]
assert Matrix([[[], ()]]).T.tolist() == [[[]], [()]]
a = Matrix([[x, 0], [0, 0]])
m = a
assert m.cols == m.rows
assert m.cols == 2
assert m[:] == [x, 0, 0, 0]
b = Matrix(2, 2, [x, 0, 0, 0])
m = b
assert m.cols == m.rows
assert m.cols == 2
assert m[:] == [x, 0, 0, 0]
assert a == b
assert Matrix(b) == b
c23 = Matrix(2, 3, range(1, 7))
c13 = Matrix(1, 3, range(7, 10))
c = Matrix([c23, c13])
assert c.cols == 3
assert c.rows == 3
assert c[:] == [1, 2, 3, 4, 5, 6, 7, 8, 9]
assert Matrix(eye(2)) == eye(2)
assert ImmutableMatrix(ImmutableMatrix(eye(2))) == ImmutableMatrix(eye(2))
assert ImmutableMatrix(c) == c.as_immutable()
assert Matrix(ImmutableMatrix(c)) == ImmutableMatrix(c).as_mutable()
assert c is not Matrix(c)
dat = [[ones(3,2), ones(3,3)*2], [ones(2,3)*3, ones(2,2)*4]]
M = Matrix(dat)
assert M == Matrix([
[1, 1, 2, 2, 2],
[1, 1, 2, 2, 2],
[1, 1, 2, 2, 2],
[3, 3, 3, 4, 4],
[3, 3, 3, 4, 4]])
assert M.tolist() != dat
# keep block form if evaluate=False
assert Matrix(dat, evaluate=False).tolist() == dat
A = MatrixSymbol("A", 2, 2)
dat = [ones(2), A]
assert Matrix(dat) == Matrix([
[ 1, 1],
[ 1, 1],
[A[0, 0], A[0, 1]],
[A[1, 0], A[1, 1]]])
assert Matrix(dat, evaluate=False).tolist() == [[i] for i in dat]
# 0-dim tolerance
assert Matrix([ones(2), ones(0)]) == Matrix([ones(2)])
raises(ValueError, lambda: Matrix([ones(2), ones(0, 3)]))
raises(ValueError, lambda: Matrix([ones(2), ones(3, 0)]))
def test_irregular_block():
assert Matrix.irregular(3, ones(2,1), ones(3,3)*2, ones(2,2)*3,
ones(1,1)*4, ones(2,2)*5, ones(1,2)*6, ones(1,2)*7) == Matrix([
[1, 2, 2, 2, 3, 3],
[1, 2, 2, 2, 3, 3],
[4, 2, 2, 2, 5, 5],
[6, 6, 7, 7, 5, 5]])
def test_tolist():
lst = [[S.One, S.Half, x*y, S.Zero], [x, y, z, x**2], [y, -S.One, z*x, 3]]
m = Matrix(lst)
assert m.tolist() == lst
def test_as_mutable():
assert zeros(0, 3).as_mutable() == zeros(0, 3)
assert zeros(0, 3).as_immutable() == ImmutableMatrix(zeros(0, 3))
assert zeros(3, 0).as_immutable() == ImmutableMatrix(zeros(3, 0))
def test_determinant():
for M in [Matrix(), Matrix([[1]])]:
assert (
M.det() ==
M._eval_det_bareiss() ==
M._eval_det_berkowitz() ==
M._eval_det_lu() ==
1)
M = Matrix(( (-3, 2),
( 8, -5) ))
assert M.det(method="bareiss") == -1
assert M.det(method="berkowitz") == -1
assert M.det(method="lu") == -1
M = Matrix(( (x, 1),
(y, 2*y) ))
assert M.det(method="bareiss") == 2*x*y - y
assert M.det(method="berkowitz") == 2*x*y - y
assert M.det(method="lu") == 2*x*y - y
M = Matrix(( (1, 1, 1),
(1, 2, 3),
(1, 3, 6) ))
assert M.det(method="bareiss") == 1
assert M.det(method="berkowitz") == 1
assert M.det(method="lu") == 1
M = Matrix(( ( 3, -2, 0, 5),
(-2, 1, -2, 2),
( 0, -2, 5, 0),
( 5, 0, 3, 4) ))
assert M.det(method="bareiss") == -289
assert M.det(method="berkowitz") == -289
assert M.det(method="lu") == -289
M = Matrix(( ( 1, 2, 3, 4),
( 5, 6, 7, 8),
( 9, 10, 11, 12),
(13, 14, 15, 16) ))
assert M.det(method="bareiss") == 0
assert M.det(method="berkowitz") == 0
assert M.det(method="lu") == 0
M = Matrix(( (3, 2, 0, 0, 0),
(0, 3, 2, 0, 0),
(0, 0, 3, 2, 0),
(0, 0, 0, 3, 2),
(2, 0, 0, 0, 3) ))
assert M.det(method="bareiss") == 275
assert M.det(method="berkowitz") == 275
assert M.det(method="lu") == 275
M = Matrix(( (1, 0, 1, 2, 12),
(2, 0, 1, 1, 4),
(2, 1, 1, -1, 3),
(3, 2, -1, 1, 8),
(1, 1, 1, 0, 6) ))
assert M.det(method="bareiss") == -55
assert M.det(method="berkowitz") == -55
assert M.det(method="lu") == -55
M = Matrix(( (-5, 2, 3, 4, 5),
( 1, -4, 3, 4, 5),
( 1, 2, -3, 4, 5),
( 1, 2, 3, -2, 5),
( 1, 2, 3, 4, -1) ))
assert M.det(method="bareiss") == 11664
assert M.det(method="berkowitz") == 11664
assert M.det(method="lu") == 11664
M = Matrix(( ( 2, 7, -1, 3, 2),
( 0, 0, 1, 0, 1),
(-2, 0, 7, 0, 2),
(-3, -2, 4, 5, 3),
( 1, 0, 0, 0, 1) ))
assert M.det(method="bareiss") == 123
assert M.det(method="berkowitz") == 123
assert M.det(method="lu") == 123
M = Matrix(( (x, y, z),
(1, 0, 0),
(y, z, x) ))
assert M.det(method="bareiss") == z**2 - x*y
assert M.det(method="berkowitz") == z**2 - x*y
assert M.det(method="lu") == z**2 - x*y
# issue 13835
a = symbols('a')
M = lambda n: Matrix([[i + a*j for i in range(n)]
for j in range(n)])
assert M(5).det() == 0
assert M(6).det() == 0
assert M(7).det() == 0
def test_slicing():
m0 = eye(4)
assert m0[:3, :3] == eye(3)
assert m0[2:4, 0:2] == zeros(2)
m1 = Matrix(3, 3, lambda i, j: i + j)
assert m1[0, :] == Matrix(1, 3, (0, 1, 2))
assert m1[1:3, 1] == Matrix(2, 1, (2, 3))
m2 = Matrix([[0, 1, 2, 3], [4, 5, 6, 7], [8, 9, 10, 11], [12, 13, 14, 15]])
assert m2[:, -1] == Matrix(4, 1, [3, 7, 11, 15])
assert m2[-2:, :] == Matrix([[8, 9, 10, 11], [12, 13, 14, 15]])
def test_submatrix_assignment():
m = zeros(4)
m[2:4, 2:4] = eye(2)
assert m == Matrix(((0, 0, 0, 0),
(0, 0, 0, 0),
(0, 0, 1, 0),
(0, 0, 0, 1)))
m[:2, :2] = eye(2)
assert m == eye(4)
m[:, 0] = Matrix(4, 1, (1, 2, 3, 4))
assert m == Matrix(((1, 0, 0, 0),
(2, 1, 0, 0),
(3, 0, 1, 0),
(4, 0, 0, 1)))
m[:, :] = zeros(4)
assert m == zeros(4)
m[:, :] = [(1, 2, 3, 4), (5, 6, 7, 8), (9, 10, 11, 12), (13, 14, 15, 16)]
assert m == Matrix(((1, 2, 3, 4),
(5, 6, 7, 8),
(9, 10, 11, 12),
(13, 14, 15, 16)))
m[:2, 0] = [0, 0]
assert m == Matrix(((0, 2, 3, 4),
(0, 6, 7, 8),
(9, 10, 11, 12),
(13, 14, 15, 16)))
def test_extract():
m = Matrix(4, 3, lambda i, j: i*3 + j)
assert m.extract([0, 1, 3], [0, 1]) == Matrix(3, 2, [0, 1, 3, 4, 9, 10])
assert m.extract([0, 3], [0, 0, 2]) == Matrix(2, 3, [0, 0, 2, 9, 9, 11])
assert m.extract(range(4), range(3)) == m
raises(IndexError, lambda: m.extract([4], [0]))
raises(IndexError, lambda: m.extract([0], [3]))
def test_reshape():
m0 = eye(3)
assert m0.reshape(1, 9) == Matrix(1, 9, (1, 0, 0, 0, 1, 0, 0, 0, 1))
m1 = Matrix(3, 4, lambda i, j: i + j)
assert m1.reshape(
4, 3) == Matrix(((0, 1, 2), (3, 1, 2), (3, 4, 2), (3, 4, 5)))
assert m1.reshape(2, 6) == Matrix(((0, 1, 2, 3, 1, 2), (3, 4, 2, 3, 4, 5)))
def test_applyfunc():
m0 = eye(3)
assert m0.applyfunc(lambda x: 2*x) == eye(3)*2
assert m0.applyfunc(lambda x: 0) == zeros(3)
def test_expand():
m0 = Matrix([[x*(x + y), 2], [((x + y)*y)*x, x*(y + x*(x + y))]])
# Test if expand() returns a matrix
m1 = m0.expand()
assert m1 == Matrix(
[[x*y + x**2, 2], [x*y**2 + y*x**2, x*y + y*x**2 + x**3]])
a = Symbol('a', real=True)
assert Matrix([exp(I*a)]).expand(complex=True) == \
Matrix([cos(a) + I*sin(a)])
assert Matrix([[0, 1, 2], [0, 0, -1], [0, 0, 0]]).exp() == Matrix([
[1, 1, Rational(3, 2)],
[0, 1, -1],
[0, 0, 1]]
)
def test_refine():
m0 = Matrix([[Abs(x)**2, sqrt(x**2)],
[sqrt(x**2)*Abs(y)**2, sqrt(y**2)*Abs(x)**2]])
m1 = m0.refine(Q.real(x) & Q.real(y))
assert m1 == Matrix([[x**2, Abs(x)], [y**2*Abs(x), x**2*Abs(y)]])
m1 = m0.refine(Q.positive(x) & Q.positive(y))
assert m1 == Matrix([[x**2, x], [x*y**2, x**2*y]])
m1 = m0.refine(Q.negative(x) & Q.negative(y))
assert m1 == Matrix([[x**2, -x], [-x*y**2, -x**2*y]])
def test_random():
M = randMatrix(3, 3)
M = randMatrix(3, 3, seed=3)
assert M == randMatrix(3, 3, seed=3)
M = randMatrix(3, 4, 0, 150)
M = randMatrix(3, seed=4, symmetric=True)
assert M == randMatrix(3, seed=4, symmetric=True)
S = M.copy()
S.simplify()
assert S == M # doesn't fail when elements are Numbers, not int
rng = random.Random(4)
assert M == randMatrix(3, symmetric=True, prng=rng)
# Ensure symmetry
for size in (10, 11): # Test odd and even
for percent in (100, 70, 30):
M = randMatrix(size, symmetric=True, percent=percent, prng=rng)
assert M == M.T
M = randMatrix(10, min=1, percent=70)
zero_count = 0
for i in range(M.shape[0]):
for j in range(M.shape[1]):
if M[i, j] == 0:
zero_count += 1
assert zero_count == 30
def test_LUdecomp():
testmat = Matrix([[0, 2, 5, 3],
[3, 3, 7, 4],
[8, 4, 0, 2],
[-2, 6, 3, 4]])
L, U, p = testmat.LUdecomposition()
assert L.is_lower
assert U.is_upper
assert (L*U).permute_rows(p, 'backward') - testmat == zeros(4)
testmat = Matrix([[6, -2, 7, 4],
[0, 3, 6, 7],
[1, -2, 7, 4],
[-9, 2, 6, 3]])
L, U, p = testmat.LUdecomposition()
assert L.is_lower
assert U.is_upper
assert (L*U).permute_rows(p, 'backward') - testmat == zeros(4)
# non-square
testmat = Matrix([[1, 2, 3],
[4, 5, 6],
[7, 8, 9],
[10, 11, 12]])
L, U, p = testmat.LUdecomposition(rankcheck=False)
assert L.is_lower
assert U.is_upper
assert (L*U).permute_rows(p, 'backward') - testmat == zeros(4, 3)
# square and singular
testmat = Matrix([[1, 2, 3],
[2, 4, 6],
[4, 5, 6]])
L, U, p = testmat.LUdecomposition(rankcheck=False)
assert L.is_lower
assert U.is_upper
assert (L*U).permute_rows(p, 'backward') - testmat == zeros(3)
M = Matrix(((1, x, 1), (2, y, 0), (y, 0, z)))
L, U, p = M.LUdecomposition()
assert L.is_lower
assert U.is_upper
assert (L*U).permute_rows(p, 'backward') - M == zeros(3)
mL = Matrix((
(1, 0, 0),
(2, 3, 0),
))
assert mL.is_lower is True
assert mL.is_upper is False
mU = Matrix((
(1, 2, 3),
(0, 4, 5),
))
assert mU.is_lower is False
assert mU.is_upper is True
# test FF LUdecomp
M = Matrix([[1, 3, 3],
[3, 2, 6],
[3, 2, 2]])
P, L, Dee, U = M.LUdecompositionFF()
assert P*M == L*Dee.inv()*U
M = Matrix([[1, 2, 3, 4],
[3, -1, 2, 3],
[3, 1, 3, -2],
[6, -1, 0, 2]])
P, L, Dee, U = M.LUdecompositionFF()
assert P*M == L*Dee.inv()*U
M = Matrix([[0, 0, 1],
[2, 3, 0],
[3, 1, 4]])
P, L, Dee, U = M.LUdecompositionFF()
assert P*M == L*Dee.inv()*U
# issue 15794
M = Matrix(
[[1, 2, 3],
[4, 5, 6],
[7, 8, 9]]
)
raises(ValueError, lambda : M.LUdecomposition_Simple(rankcheck=True))
def test_LUsolve():
A = Matrix([[2, 3, 5],
[3, 6, 2],
[8, 3, 6]])
x = Matrix(3, 1, [3, 7, 5])
b = A*x
soln = A.LUsolve(b)
assert soln == x
A = Matrix([[0, -1, 2],
[5, 10, 7],
[8, 3, 4]])
x = Matrix(3, 1, [-1, 2, 5])
b = A*x
soln = A.LUsolve(b)
assert soln == x
A = Matrix([[2, 1], [1, 0], [1, 0]]) # issue 14548
b = Matrix([3, 1, 1])
assert A.LUsolve(b) == Matrix([1, 1])
b = Matrix([3, 1, 2]) # inconsistent
raises(ValueError, lambda: A.LUsolve(b))
A = Matrix([[0, -1, 2],
[5, 10, 7],
[8, 3, 4],
[2, 3, 5],
[3, 6, 2],
[8, 3, 6]])
x = Matrix([2, 1, -4])
b = A*x
soln = A.LUsolve(b)
assert soln == x
A = Matrix([[0, -1, 2], [5, 10, 7]]) # underdetermined
x = Matrix([-1, 2, 0])
b = A*x
raises(NotImplementedError, lambda: A.LUsolve(b))
A = Matrix(4, 4, lambda i, j: 1/(i+j+1) if i != 3 else 0)
b = Matrix.zeros(4, 1)
raises(NotImplementedError, lambda: A.LUsolve(b))
def test_QRsolve():
A = Matrix([[2, 3, 5],
[3, 6, 2],
[8, 3, 6]])
x = Matrix(3, 1, [3, 7, 5])
b = A*x
soln = A.QRsolve(b)
assert soln == x
x = Matrix([[1, 2], [3, 4], [5, 6]])
b = A*x
soln = A.QRsolve(b)
assert soln == x
A = Matrix([[0, -1, 2],
[5, 10, 7],
[8, 3, 4]])
x = Matrix(3, 1, [-1, 2, 5])
b = A*x
soln = A.QRsolve(b)
assert soln == x
x = Matrix([[7, 8], [9, 10], [11, 12]])
b = A*x
soln = A.QRsolve(b)
assert soln == x
def test_inverse():
A = eye(4)
assert A.inv() == eye(4)
assert A.inv(method="LU") == eye(4)
assert A.inv(method="ADJ") == eye(4)
A = Matrix([[2, 3, 5],
[3, 6, 2],
[8, 3, 6]])
Ainv = A.inv()
assert A*Ainv == eye(3)
assert A.inv(method="LU") == Ainv
assert A.inv(method="ADJ") == Ainv
# test that immutability is not a problem
cls = ImmutableMatrix
m = cls([[48, 49, 31],
[ 9, 71, 94],
[59, 28, 65]])
assert all(type(m.inv(s)) is cls for s in 'GE ADJ LU'.split())
cls = ImmutableSparseMatrix
m = cls([[48, 49, 31],
[ 9, 71, 94],
[59, 28, 65]])
assert all(type(m.inv(s)) is cls for s in 'CH LDL'.split())
def test_matrix_inverse_mod():
A = Matrix(2, 1, [1, 0])
raises(NonSquareMatrixError, lambda: A.inv_mod(2))
A = Matrix(2, 2, [1, 0, 0, 0])
raises(ValueError, lambda: A.inv_mod(2))
A = Matrix(2, 2, [1, 2, 3, 4])
Ai = Matrix(2, 2, [1, 1, 0, 1])
assert A.inv_mod(3) == Ai
A = Matrix(2, 2, [1, 0, 0, 1])
assert A.inv_mod(2) == A
A = Matrix(3, 3, [1, 2, 3, 4, 5, 6, 7, 8, 9])
raises(ValueError, lambda: A.inv_mod(5))
A = Matrix(3, 3, [5, 1, 3, 2, 6, 0, 2, 1, 1])
Ai = Matrix(3, 3, [6, 8, 0, 1, 5, 6, 5, 6, 4])
assert A.inv_mod(9) == Ai
A = Matrix(3, 3, [1, 6, -3, 4, 1, -5, 3, -5, 5])
Ai = Matrix(3, 3, [4, 3, 3, 1, 2, 5, 1, 5, 1])
assert A.inv_mod(6) == Ai
A = Matrix(3, 3, [1, 6, 1, 4, 1, 5, 3, 2, 5])
Ai = Matrix(3, 3, [6, 0, 3, 6, 6, 4, 1, 6, 1])
assert A.inv_mod(7) == Ai
def test_util():
R = Rational
v1 = Matrix(1, 3, [1, 2, 3])
v2 = Matrix(1, 3, [3, 4, 5])
assert v1.norm() == sqrt(14)
assert v1.project(v2) == Matrix(1, 3, [R(39)/25, R(52)/25, R(13)/5])
assert Matrix.zeros(1, 2) == Matrix(1, 2, [0, 0])
assert ones(1, 2) == Matrix(1, 2, [1, 1])
assert v1.copy() == v1
# cofactor
assert eye(3) == eye(3).cofactor_matrix()
test = Matrix([[1, 3, 2], [2, 6, 3], [2, 3, 6]])
assert test.cofactor_matrix() == \
Matrix([[27, -6, -6], [-12, 2, 3], [-3, 1, 0]])
test = Matrix([[1, 2, 3], [4, 5, 6], [7, 8, 9]])
assert test.cofactor_matrix() == \
Matrix([[-3, 6, -3], [6, -12, 6], [-3, 6, -3]])
def test_jacobian_hessian():
L = Matrix(1, 2, [x**2*y, 2*y**2 + x*y])
syms = [x, y]
assert L.jacobian(syms) == Matrix([[2*x*y, x**2], [y, 4*y + x]])
L = Matrix(1, 2, [x, x**2*y**3])
assert L.jacobian(syms) == Matrix([[1, 0], [2*x*y**3, x**2*3*y**2]])
f = x**2*y
syms = [x, y]
assert hessian(f, syms) == Matrix([[2*y, 2*x], [2*x, 0]])
f = x**2*y**3
assert hessian(f, syms) == \
Matrix([[2*y**3, 6*x*y**2], [6*x*y**2, 6*x**2*y]])
f = z + x*y**2
g = x**2 + 2*y**3
ans = Matrix([[0, 2*y],
[2*y, 2*x]])
assert ans == hessian(f, Matrix([x, y]))
assert ans == hessian(f, Matrix([x, y]).T)
assert hessian(f, (y, x), [g]) == Matrix([
[ 0, 6*y**2, 2*x],
[6*y**2, 2*x, 2*y],
[ 2*x, 2*y, 0]])
def test_QR():
A = Matrix([[1, 2], [2, 3]])
Q, S = A.QRdecomposition()
R = Rational
assert Q == Matrix([
[ 5**R(-1, 2), (R(2)/5)*(R(1)/5)**R(-1, 2)],
[2*5**R(-1, 2), (-R(1)/5)*(R(1)/5)**R(-1, 2)]])
assert S == Matrix([[5**R(1, 2), 8*5**R(-1, 2)], [0, (R(1)/5)**R(1, 2)]])
assert Q*S == A
assert Q.T * Q == eye(2)
A = Matrix([[1, 1, 1], [1, 1, 3], [2, 3, 4]])
Q, R = A.QRdecomposition()
assert Q.T * Q == eye(Q.cols)
assert R.is_upper
assert A == Q*R
def test_QR_non_square():
# Narrow (cols < rows) matrices
A = Matrix([[9, 0, 26], [12, 0, -7], [0, 4, 4], [0, -3, -3]])
Q, R = A.QRdecomposition()
assert Q.T * Q == eye(Q.cols)
assert R.is_upper
assert A == Q*R
A = Matrix([[1, -1, 4], [1, 4, -2], [1, 4, 2], [1, -1, 0]])
Q, R = A.QRdecomposition()
assert Q.T * Q == eye(Q.cols)
assert R.is_upper
assert A == Q*R
A = Matrix(2, 1, [1, 2])
Q, R = A.QRdecomposition()
assert Q.T * Q == eye(Q.cols)
assert R.is_upper
assert A == Q*R
# Wide (cols > rows) matrices
A = Matrix([[1, 2, 3], [4, 5, 6]])
Q, R = A.QRdecomposition()
assert Q.T * Q == eye(Q.cols)
assert R.is_upper
assert A == Q*R
A = Matrix([[1, 2, 3, 4], [1, 4, 9, 16], [1, 8, 27, 64]])
Q, R = A.QRdecomposition()
assert Q.T * Q == eye(Q.cols)
assert R.is_upper
assert A == Q*R
A = Matrix(1, 2, [1, 2])
Q, R = A.QRdecomposition()
assert Q.T * Q == eye(Q.cols)
assert R.is_upper
assert A == Q*R
def test_QR_trivial():
# Rank deficient matrices
A = Matrix([[1, 2, 3], [4, 5, 6], [7, 8, 9]])
Q, R = A.QRdecomposition()
assert Q.T * Q == eye(Q.cols)
assert R.is_upper
assert A == Q*R
A = Matrix([[1, 1, 1], [2, 2, 2], [3, 3, 3], [4, 4, 4]])
Q, R = A.QRdecomposition()
assert Q.T * Q == eye(Q.cols)
assert R.is_upper
assert A == Q*R
A = Matrix([[1, 1, 1], [2, 2, 2], [3, 3, 3], [4, 4, 4]]).T
Q, R = A.QRdecomposition()
assert Q.T * Q == eye(Q.cols)
assert R.is_upper
assert A == Q*R
# Zero rank matrices
A = Matrix([[0, 0, 0]])
Q, R = A.QRdecomposition()
assert Q.T * Q == eye(Q.cols)
assert R.is_upper
assert A == Q*R
A = Matrix([[0, 0, 0]]).T
Q, R = A.QRdecomposition()
assert Q.T * Q == eye(Q.cols)
assert R.is_upper
assert A == Q*R
A = Matrix([[0, 0, 0], [0, 0, 0]])
Q, R = A.QRdecomposition()
assert Q.T * Q == eye(Q.cols)
assert R.is_upper
assert A == Q*R
A = Matrix([[0, 0, 0], [0, 0, 0]]).T
Q, R = A.QRdecomposition()
assert Q.T * Q == eye(Q.cols)
assert R.is_upper
assert A == Q*R
# Rank deficient matrices with zero norm from beginning columns
A = Matrix([[0, 0, 0], [1, 2, 3]]).T
Q, R = A.QRdecomposition()
assert Q.T * Q == eye(Q.cols)
assert R.is_upper
assert A == Q*R
A = Matrix([[0, 0, 0, 0], [1, 2, 3, 4], [0, 0, 0, 0]]).T
Q, R = A.QRdecomposition()
assert Q.T * Q == eye(Q.cols)
assert R.is_upper
assert A == Q*R
A = Matrix([[0, 0, 0, 0], [1, 2, 3, 4], [0, 0, 0, 0], [2, 4, 6, 8]]).T
Q, R = A.QRdecomposition()
assert Q.T * Q == eye(Q.cols)
assert R.is_upper
assert A == Q*R
A = Matrix([[0, 0, 0], [0, 0, 0], [0, 0, 0], [1, 2, 3]]).T
Q, R = A.QRdecomposition()
assert Q.T * Q == eye(Q.cols)
assert R.is_upper
assert A == Q*R
def test_nullspace():
# first test reduced row-ech form
R = Rational
M = Matrix([[5, 7, 2, 1],
[1, 6, 2, -1]])
out, tmp = M.rref()
assert out == Matrix([[1, 0, -R(2)/23, R(13)/23],
[0, 1, R(8)/23, R(-6)/23]])
M = Matrix([[-5, -1, 4, -3, -1],
[ 1, -1, -1, 1, 0],
[-1, 0, 0, 0, 0],
[ 4, 1, -4, 3, 1],
[-2, 0, 2, -2, -1]])
assert M*M.nullspace()[0] == Matrix(5, 1, [0]*5)
M = Matrix([[ 1, 3, 0, 2, 6, 3, 1],
[-2, -6, 0, -2, -8, 3, 1],
[ 3, 9, 0, 0, 6, 6, 2],
[-1, -3, 0, 1, 0, 9, 3]])
out, tmp = M.rref()
assert out == Matrix([[1, 3, 0, 0, 2, 0, 0],
[0, 0, 0, 1, 2, 0, 0],
[0, 0, 0, 0, 0, 1, R(1)/3],
[0, 0, 0, 0, 0, 0, 0]])
# now check the vectors
basis = M.nullspace()
assert basis[0] == Matrix([-3, 1, 0, 0, 0, 0, 0])
assert basis[1] == Matrix([0, 0, 1, 0, 0, 0, 0])
assert basis[2] == Matrix([-2, 0, 0, -2, 1, 0, 0])
assert basis[3] == Matrix([0, 0, 0, 0, 0, R(-1)/3, 1])
# issue 4797; just see that we can do it when rows > cols
M = Matrix([[1, 2], [2, 4], [3, 6]])
assert M.nullspace()
def test_columnspace():
M = Matrix([[ 1, 2, 0, 2, 5],
[-2, -5, 1, -1, -8],
[ 0, -3, 3, 4, 1],
[ 3, 6, 0, -7, 2]])
# now check the vectors
basis = M.columnspace()
assert basis[0] == Matrix([1, -2, 0, 3])
assert basis[1] == Matrix([2, -5, -3, 6])
assert basis[2] == Matrix([2, -1, 4, -7])
#check by columnspace definition
a, b, c, d, e = symbols('a b c d e')
X = Matrix([a, b, c, d, e])
for i in range(len(basis)):
eq=M*X-basis[i]
assert len(solve(eq, X)) != 0
#check if rank-nullity theorem holds
assert M.rank() == len(basis)
assert len(M.nullspace()) + len(M.columnspace()) == M.cols
def test_wronskian():
assert wronskian([cos(x), sin(x)], x) == cos(x)**2 + sin(x)**2
assert wronskian([exp(x), exp(2*x)], x) == exp(3*x)
assert wronskian([exp(x), x], x) == exp(x) - x*exp(x)
assert wronskian([1, x, x**2], x) == 2
w1 = -6*exp(x)*sin(x)*x + 6*cos(x)*exp(x)*x**2 - 6*exp(x)*cos(x)*x - \
exp(x)*cos(x)*x**3 + exp(x)*sin(x)*x**3
assert wronskian([exp(x), cos(x), x**3], x).expand() == w1
assert wronskian([exp(x), cos(x), x**3], x, method='berkowitz').expand() \
== w1
w2 = -x**3*cos(x)**2 - x**3*sin(x)**2 - 6*x*cos(x)**2 - 6*x*sin(x)**2
assert wronskian([sin(x), cos(x), x**3], x).expand() == w2
assert wronskian([sin(x), cos(x), x**3], x, method='berkowitz').expand() \
== w2
assert wronskian([], x) == 1
def test_eigen():
R = Rational
assert eye(3).charpoly(x) == Poly((x - 1)**3, x)
assert eye(3).charpoly(y) == Poly((y - 1)**3, y)
M = Matrix([[1, 0, 0],
[0, 1, 0],
[0, 0, 1]])
assert M.eigenvals(multiple=False) == {S.One: 3}
assert M.eigenvals(multiple=True) == [1, 1, 1]
assert M.eigenvects() == (
[(1, 3, [Matrix([1, 0, 0]),
Matrix([0, 1, 0]),
Matrix([0, 0, 1])])])
assert M.left_eigenvects() == (
[(1, 3, [Matrix([[1, 0, 0]]),
Matrix([[0, 1, 0]]),
Matrix([[0, 0, 1]])])])
M = Matrix([[0, 1, 1],
[1, 0, 0],
[1, 1, 1]])
assert M.eigenvals() == {2*S.One: 1, -S.One: 1, S.Zero: 1}
assert M.eigenvects() == (
[
(-1, 1, [Matrix([-1, 1, 0])]),
( 0, 1, [Matrix([0, -1, 1])]),
( 2, 1, [Matrix([R(2, 3), R(1, 3), 1])])
])
assert M.left_eigenvects() == (
[
(-1, 1, [Matrix([[-2, 1, 1]])]),
(0, 1, [Matrix([[-1, -1, 1]])]),
(2, 1, [Matrix([[1, 1, 1]])])
])
a = Symbol('a')
M = Matrix([[a, 0],
[0, 1]])
assert M.eigenvals() == {a: 1, S.One: 1}
M = Matrix([[1, -1],
[1, 3]])
assert M.eigenvects() == ([(2, 2, [Matrix(2, 1, [-1, 1])])])
assert M.left_eigenvects() == ([(2, 2, [Matrix([[1, 1]])])])
M = Matrix([[1, 2, 3], [4, 5, 6], [7, 8, 9]])
a = R(15, 2)
b = 3*33**R(1, 2)
c = R(13, 2)
d = (R(33, 8) + 3*b/8)
e = (R(33, 8) - 3*b/8)
def NS(e, n):
return str(N(e, n))
r = [
(a - b/2, 1, [Matrix([(12 + 24/(c - b/2))/((c - b/2)*e) + 3/(c - b/2),
(6 + 12/(c - b/2))/e, 1])]),
( 0, 1, [Matrix([1, -2, 1])]),
(a + b/2, 1, [Matrix([(12 + 24/(c + b/2))/((c + b/2)*d) + 3/(c + b/2),
(6 + 12/(c + b/2))/d, 1])]),
]
r1 = [(NS(r[i][0], 2), NS(r[i][1], 2),
[NS(j, 2) for j in r[i][2][0]]) for i in range(len(r))]
r = M.eigenvects()
r2 = [(NS(r[i][0], 2), NS(r[i][1], 2),
[NS(j, 2) for j in r[i][2][0]]) for i in range(len(r))]
assert sorted(r1) == sorted(r2)
eps = Symbol('eps', real=True)
M = Matrix([[abs(eps), I*eps ],
[-I*eps, abs(eps) ]])
assert M.eigenvects() == (
[
( 0, 1, [Matrix([[-I*eps/abs(eps)], [1]])]),
( 2*abs(eps), 1, [ Matrix([[I*eps/abs(eps)], [1]]) ] ),
])
assert M.left_eigenvects() == (
[
(0, 1, [Matrix([[I*eps/Abs(eps), 1]])]),
(2*Abs(eps), 1, [Matrix([[-I*eps/Abs(eps), 1]])])
])
M = Matrix(3, 3, [1, 2, 0, 0, 3, 0, 2, -4, 2])
M._eigenvects = M.eigenvects(simplify=False)
assert max(i.q for i in M._eigenvects[0][2][0]) > 1
M._eigenvects = M.eigenvects(simplify=True)
assert max(i.q for i in M._eigenvects[0][2][0]) == 1
M = Matrix([[S(1)/4, 1], [1, 1]])
assert M.eigenvects(simplify=True) == [
(S(5)/8 - sqrt(73)/8, 1, [Matrix([[-sqrt(73)/8 - S(3)/8], [1]])]),
(S(5)/8 + sqrt(73)/8, 1, [Matrix([[-S(3)/8 + sqrt(73)/8], [1]])])]
assert M.eigenvects(simplify=False) ==[
(S(5)/8 - sqrt(73)/8, 1, [Matrix([[-1/(-S(3)/8 + sqrt(73)/8)],
[ 1]])]),
(S(5)/8 + sqrt(73)/8, 1, [Matrix([[-1/(-sqrt(73)/8 - S(3)/8)],
[ 1]])])]
m = Matrix([[1, .6, .6], [.6, .9, .9], [.9, .6, .6]])
evals = { S(5)/4 - sqrt(385)/20: 1, sqrt(385)/20 + S(5)/4: 1, S.Zero: 1}
assert m.eigenvals() == evals
nevals = list(sorted(m.eigenvals(rational=False).keys()))
sevals = list(sorted(evals.keys()))
assert all(abs(nevals[i] - sevals[i]) < 1e-9 for i in range(len(nevals)))
# issue 10719
assert Matrix([]).eigenvals() == {}
assert Matrix([]).eigenvects() == []
# issue 15119
raises(NonSquareMatrixError, lambda : Matrix([[1, 2], [0, 4], [0, 0]]).eigenvals())
raises(NonSquareMatrixError, lambda : Matrix([[1, 0], [3, 4], [5, 6]]).eigenvals())
raises(NonSquareMatrixError, lambda : Matrix([[1, 2, 3], [0, 5, 6]]).eigenvals())
raises(NonSquareMatrixError, lambda : Matrix([[1, 0, 0], [4, 5, 0]]).eigenvals())
raises(NonSquareMatrixError, lambda : Matrix([[1, 2, 3], [0, 5, 6]]).eigenvals(error_when_incomplete = False))
raises(NonSquareMatrixError, lambda : Matrix([[1, 0, 0], [4, 5, 0]]).eigenvals(error_when_incomplete = False))
# issue 15125
from sympy.core.function import count_ops
q = Symbol("q", positive = True)
m = Matrix([[-2, exp(-q), 1], [exp(q), -2, 1], [1, 1, -2]])
assert count_ops(m.eigenvals(simplify=False)) > count_ops(m.eigenvals(simplify=True))
assert count_ops(m.eigenvals(simplify=lambda x: x)) > count_ops(m.eigenvals(simplify=True))
assert isinstance(m.eigenvals(simplify=True, multiple=False), dict)
assert isinstance(m.eigenvals(simplify=True, multiple=True), list)
assert isinstance(m.eigenvals(simplify=lambda x: x, multiple=False), dict)
assert isinstance(m.eigenvals(simplify=lambda x: x, multiple=True), list)
def test_definite():
# Examples from Gilbert Strang, "Introduction to Linear Algebra"
# Positive definite matrices
m = Matrix([[2, -1, 0], [-1, 2, -1], [0, -1, 2]])
assert m.is_positive_definite == True
assert m.is_positive_semidefinite == True
assert m.is_negative_definite == False
assert m.is_negative_semidefinite == False
assert m.is_indefinite == False
m = Matrix([[5, 4], [4, 5]])
assert m.is_positive_definite == True
assert m.is_positive_semidefinite == True
assert m.is_negative_definite == False
assert m.is_negative_semidefinite == False
assert m.is_indefinite == False
# Positive semidefinite matrices
m = Matrix([[2, -1, -1], [-1, 2, -1], [-1, -1, 2]])
assert m.is_positive_definite == False
assert m.is_positive_semidefinite == True
assert m.is_negative_definite == False
assert m.is_negative_semidefinite == False
assert m.is_indefinite == False
m = Matrix([[1, 2], [2, 4]])
assert m.is_positive_definite == False
assert m.is_positive_semidefinite == True
assert m.is_negative_definite == False
assert m.is_negative_semidefinite == False
assert m.is_indefinite == False
# Examples from Mathematica documentation
# Non-hermitian positive definite matrices
m = Matrix([[2, 3], [4, 8]])
assert m.is_positive_definite == True
assert m.is_positive_semidefinite == True
assert m.is_negative_definite == False
assert m.is_negative_semidefinite == False
assert m.is_indefinite == False
m = Matrix([[1, 2*I], [-I, 4]])
assert m.is_positive_definite == True
assert m.is_positive_semidefinite == True
assert m.is_negative_definite == False
assert m.is_negative_semidefinite == False
assert m.is_indefinite == False
# Symbolic matrices examples
a = Symbol('a', positive=True)
b = Symbol('b', negative=True)
m = Matrix([[a, 0, 0], [0, a, 0], [0, 0, a]])
assert m.is_positive_definite == True
assert m.is_positive_semidefinite == True
assert m.is_negative_definite == False
assert m.is_negative_semidefinite == False
assert m.is_indefinite == False
m = Matrix([[b, 0, 0], [0, b, 0], [0, 0, b]])
assert m.is_positive_definite == False
assert m.is_positive_semidefinite == False
assert m.is_negative_definite == True
assert m.is_negative_semidefinite == True
assert m.is_indefinite == False
m = Matrix([[a, 0], [0, b]])
assert m.is_positive_definite == False
assert m.is_positive_semidefinite == False
assert m.is_negative_definite == False
assert m.is_negative_semidefinite == False
assert m.is_indefinite == True
def test_positive_definite():
# Test alternative algorithms for testing positive definitiveness.
m = Matrix([[2, -1, 0], [-1, 2, -1], [0, -1, 2]])
assert m._eval_is_positive_definite(method='eigen') == True
assert m._eval_is_positive_definite(method='LDL') == True
assert m._eval_is_positive_definite(method='CH') == True
m = Matrix([[5, 4], [4, 5]])
assert m._eval_is_positive_definite(method='eigen') == True
assert m._eval_is_positive_definite(method='LDL') == True
assert m._eval_is_positive_definite(method='CH') == True
m = Matrix([[2, -1, -1], [-1, 2, -1], [-1, -1, 2]])
assert m._eval_is_positive_definite(method='eigen') == False
assert m._eval_is_positive_definite(method='LDL') == False
assert m._eval_is_positive_definite(method='CH') == False
m = Matrix([[1, 2], [2, 4]])
assert m._eval_is_positive_definite(method='eigen') == False
assert m._eval_is_positive_definite(method='LDL') == False
assert m._eval_is_positive_definite(method='CH') == False
m = Matrix([[2, 3], [4, 8]])
assert m._eval_is_positive_definite(method='eigen') == True
assert m._eval_is_positive_definite(method='LDL') == True
assert m._eval_is_positive_definite(method='CH') == True
m = Matrix([[1, 2*I], [-I, 4]])
assert m._eval_is_positive_definite(method='eigen') == True
assert m._eval_is_positive_definite(method='LDL') == True
assert m._eval_is_positive_definite(method='CH') == True
a = Symbol('a', positive=True)
b = Symbol('b', negative=True)
m = Matrix([[a, 0, 0], [0, a, 0], [0, 0, a]])
assert m._eval_is_positive_definite(method='eigen') == True
assert m._eval_is_positive_definite(method='LDL') == True
assert m._eval_is_positive_definite(method='CH') == True
m = Matrix([[b, 0, 0], [0, b, 0], [0, 0, b]])
assert m._eval_is_positive_definite(method='eigen') == False
assert m._eval_is_positive_definite(method='LDL') == False
assert m._eval_is_positive_definite(method='CH') == False
m = Matrix([[a, 0], [0, b]])
assert m._eval_is_positive_definite(method='eigen') == False
assert m._eval_is_positive_definite(method='LDL') == False
assert m._eval_is_positive_definite(method='CH') == False
def test_subs():
assert Matrix([[1, x], [x, 4]]).subs(x, 5) == Matrix([[1, 5], [5, 4]])
assert Matrix([[x, 2], [x + y, 4]]).subs([[x, -1], [y, -2]]) == \
Matrix([[-1, 2], [-3, 4]])
assert Matrix([[x, 2], [x + y, 4]]).subs([(x, -1), (y, -2)]) == \
Matrix([[-1, 2], [-3, 4]])
assert Matrix([[x, 2], [x + y, 4]]).subs({x: -1, y: -2}) == \
Matrix([[-1, 2], [-3, 4]])
assert Matrix([x*y]).subs({x: y - 1, y: x - 1}, simultaneous=True) == \
Matrix([(x - 1)*(y - 1)])
for cls in classes:
assert Matrix([[2, 0], [0, 2]]) == cls.eye(2).subs(1, 2)
def test_xreplace():
assert Matrix([[1, x], [x, 4]]).xreplace({x: 5}) == \
Matrix([[1, 5], [5, 4]])
assert Matrix([[x, 2], [x + y, 4]]).xreplace({x: -1, y: -2}) == \
Matrix([[-1, 2], [-3, 4]])
for cls in classes:
assert Matrix([[2, 0], [0, 2]]) == cls.eye(2).xreplace({1: 2})
def test_simplify():
n = Symbol('n')
f = Function('f')
M = Matrix([[ 1/x + 1/y, (x + x*y) / x ],
[ (f(x) + y*f(x))/f(x), 2 * (1/n - cos(n * pi)/n) / pi ]])
M.simplify()
assert M == Matrix([[ (x + y)/(x * y), 1 + y ],
[ 1 + y, 2*((1 - 1*cos(pi*n))/(pi*n)) ]])
eq = (1 + x)**2
M = Matrix([[eq]])
M.simplify()
assert M == Matrix([[eq]])
M.simplify(ratio=oo) == M
assert M == Matrix([[eq.simplify(ratio=oo)]])
def test_transpose():
M = Matrix([[1, 2, 3, 4, 5, 6, 7, 8, 9, 0],
[1, 2, 3, 4, 5, 6, 7, 8, 9, 0]])
assert M.T == Matrix( [ [1, 1],
[2, 2],
[3, 3],
[4, 4],
[5, 5],
[6, 6],
[7, 7],
[8, 8],
[9, 9],
[0, 0] ])
assert M.T.T == M
assert M.T == M.transpose()
def test_conjugate():
M = Matrix([[0, I, 5],
[1, 2, 0]])
assert M.T == Matrix([[0, 1],
[I, 2],
[5, 0]])
assert M.C == Matrix([[0, -I, 5],
[1, 2, 0]])
assert M.C == M.conjugate()
assert M.H == M.T.C
assert M.H == Matrix([[ 0, 1],
[-I, 2],
[ 5, 0]])
def test_conj_dirac():
raises(AttributeError, lambda: eye(3).D)
M = Matrix([[1, I, I, I],
[0, 1, I, I],
[0, 0, 1, I],
[0, 0, 0, 1]])
assert M.D == Matrix([[ 1, 0, 0, 0],
[-I, 1, 0, 0],
[-I, -I, -1, 0],
[-I, -I, I, -1]])
def test_trace():
M = Matrix([[1, 0, 0],
[0, 5, 0],
[0, 0, 8]])
assert M.trace() == 14
def test_shape():
M = Matrix([[x, 0, 0],
[0, y, 0]])
assert M.shape == (2, 3)
def test_col_row_op():
M = Matrix([[x, 0, 0],
[0, y, 0]])
M.row_op(1, lambda r, j: r + j + 1)
assert M == Matrix([[x, 0, 0],
[1, y + 2, 3]])
M.col_op(0, lambda c, j: c + y**j)
assert M == Matrix([[x + 1, 0, 0],
[1 + y, y + 2, 3]])
# neither row nor slice give copies that allow the original matrix to
# be changed
assert M.row(0) == Matrix([[x + 1, 0, 0]])
r1 = M.row(0)
r1[0] = 42
assert M[0, 0] == x + 1
r1 = M[0, :-1] # also testing negative slice
r1[0] = 42
assert M[0, 0] == x + 1
c1 = M.col(0)
assert c1 == Matrix([x + 1, 1 + y])
c1[0] = 0
assert M[0, 0] == x + 1
c1 = M[:, 0]
c1[0] = 42
assert M[0, 0] == x + 1
def test_zip_row_op():
for cls in classes[:2]: # XXX: immutable matrices don't support row ops
M = cls.eye(3)
M.zip_row_op(1, 0, lambda v, u: v + 2*u)
assert M == cls([[1, 0, 0],
[2, 1, 0],
[0, 0, 1]])
M = cls.eye(3)*2
M[0, 1] = -1
M.zip_row_op(1, 0, lambda v, u: v + 2*u); M
assert M == cls([[2, -1, 0],
[4, 0, 0],
[0, 0, 2]])
def test_issue_3950():
m = Matrix([1, 2, 3])
a = Matrix([1, 2, 3])
b = Matrix([2, 2, 3])
assert not (m in [])
assert not (m in [1])
assert m != 1
assert m == a
assert m != b
def test_issue_3981():
class Index1(object):
def __index__(self):
return 1
class Index2(object):
def __index__(self):
return 2
index1 = Index1()
index2 = Index2()
m = Matrix([1, 2, 3])
assert m[index2] == 3
m[index2] = 5
assert m[2] == 5
m = Matrix([[1, 2, 3], [4, 5, 6]])
assert m[index1, index2] == 6
assert m[1, index2] == 6
assert m[index1, 2] == 6
m[index1, index2] = 4
assert m[1, 2] == 4
m[1, index2] = 6
assert m[1, 2] == 6
m[index1, 2] = 8
assert m[1, 2] == 8
def test_evalf():
a = Matrix([sqrt(5), 6])
assert all(a.evalf()[i] == a[i].evalf() for i in range(2))
assert all(a.evalf(2)[i] == a[i].evalf(2) for i in range(2))
assert all(a.n(2)[i] == a[i].n(2) for i in range(2))
def test_is_symbolic():
a = Matrix([[x, x], [x, x]])
assert a.is_symbolic() is True
a = Matrix([[1, 2, 3, 4], [5, 6, 7, 8]])
assert a.is_symbolic() is False
a = Matrix([[1, 2, 3, 4], [5, 6, x, 8]])
assert a.is_symbolic() is True
a = Matrix([[1, x, 3]])
assert a.is_symbolic() is True
a = Matrix([[1, 2, 3]])
assert a.is_symbolic() is False
a = Matrix([[1], [x], [3]])
assert a.is_symbolic() is True
a = Matrix([[1], [2], [3]])
assert a.is_symbolic() is False
def test_is_upper():
a = Matrix([[1, 2, 3]])
assert a.is_upper is True
a = Matrix([[1], [2], [3]])
assert a.is_upper is False
a = zeros(4, 2)
assert a.is_upper is True
def test_is_lower():
a = Matrix([[1, 2, 3]])
assert a.is_lower is False
a = Matrix([[1], [2], [3]])
assert a.is_lower is True
def test_is_nilpotent():
a = Matrix(4, 4, [0, 2, 1, 6, 0, 0, 1, 2, 0, 0, 0, 3, 0, 0, 0, 0])
assert a.is_nilpotent()
a = Matrix([[1, 0], [0, 1]])
assert not a.is_nilpotent()
a = Matrix([])
assert a.is_nilpotent()
def test_zeros_ones_fill():
n, m = 3, 5
a = zeros(n, m)
a.fill( 5 )
b = 5 * ones(n, m)
assert a == b
assert a.rows == b.rows == 3
assert a.cols == b.cols == 5
assert a.shape == b.shape == (3, 5)
assert zeros(2) == zeros(2, 2)
assert ones(2) == ones(2, 2)
assert zeros(2, 3) == Matrix(2, 3, [0]*6)
assert ones(2, 3) == Matrix(2, 3, [1]*6)
def test_empty_zeros():
a = zeros(0)
assert a == Matrix()
a = zeros(0, 2)
assert a.rows == 0
assert a.cols == 2
a = zeros(2, 0)
assert a.rows == 2
assert a.cols == 0
def test_issue_3749():
a = Matrix([[x**2, x*y], [x*sin(y), x*cos(y)]])
assert a.diff(x) == Matrix([[2*x, y], [sin(y), cos(y)]])
assert Matrix([
[x, -x, x**2],
[exp(x), 1/x - exp(-x), x + 1/x]]).limit(x, oo) == \
Matrix([[oo, -oo, oo], [oo, 0, oo]])
assert Matrix([
[(exp(x) - 1)/x, 2*x + y*x, x**x ],
[1/x, abs(x), abs(sin(x + 1))]]).limit(x, 0) == \
Matrix([[1, 0, 1], [oo, 0, sin(1)]])
assert a.integrate(x) == Matrix([
[Rational(1, 3)*x**3, y*x**2/2],
[x**2*sin(y)/2, x**2*cos(y)/2]])
def test_inv_iszerofunc():
A = eye(4)
A.col_swap(0, 1)
for method in "GE", "LU":
assert A.inv(method=method, iszerofunc=lambda x: x == 0) == \
A.inv(method="ADJ")
def test_jacobian_metrics():
rho, phi = symbols("rho,phi")
X = Matrix([rho*cos(phi), rho*sin(phi)])
Y = Matrix([rho, phi])
J = X.jacobian(Y)
assert J == X.jacobian(Y.T)
assert J == (X.T).jacobian(Y)
assert J == (X.T).jacobian(Y.T)
g = J.T*eye(J.shape[0])*J
g = g.applyfunc(trigsimp)
assert g == Matrix([[1, 0], [0, rho**2]])
def test_jacobian2():
rho, phi = symbols("rho,phi")
X = Matrix([rho*cos(phi), rho*sin(phi), rho**2])
Y = Matrix([rho, phi])
J = Matrix([
[cos(phi), -rho*sin(phi)],
[sin(phi), rho*cos(phi)],
[ 2*rho, 0],
])
assert X.jacobian(Y) == J
def test_issue_4564():
X = Matrix([exp(x + y + z), exp(x + y + z), exp(x + y + z)])
Y = Matrix([x, y, z])
for i in range(1, 3):
for j in range(1, 3):
X_slice = X[:i, :]
Y_slice = Y[:j, :]
J = X_slice.jacobian(Y_slice)
assert J.rows == i
assert J.cols == j
for k in range(j):
assert J[:, k] == X_slice
def test_nonvectorJacobian():
X = Matrix([[exp(x + y + z), exp(x + y + z)],
[exp(x + y + z), exp(x + y + z)]])
raises(TypeError, lambda: X.jacobian(Matrix([x, y, z])))
X = X[0, :]
Y = Matrix([[x, y], [x, z]])
raises(TypeError, lambda: X.jacobian(Y))
raises(TypeError, lambda: X.jacobian(Matrix([ [x, y], [x, z] ])))
def test_vec():
m = Matrix([[1, 3], [2, 4]])
m_vec = m.vec()
assert m_vec.cols == 1
for i in range(4):
assert m_vec[i] == i + 1
def test_vech():
m = Matrix([[1, 2], [2, 3]])
m_vech = m.vech()
assert m_vech.cols == 1
for i in range(3):
assert m_vech[i] == i + 1
m_vech = m.vech(diagonal=False)
assert m_vech[0] == 2
m = Matrix([[1, x*(x + y)], [y*x + x**2, 1]])
m_vech = m.vech(diagonal=False)
assert m_vech[0] == x*(x + y)
m = Matrix([[1, x*(x + y)], [y*x, 1]])
m_vech = m.vech(diagonal=False, check_symmetry=False)
assert m_vech[0] == y*x
def test_vech_errors():
m = Matrix([[1, 3]])
raises(ShapeError, lambda: m.vech())
m = Matrix([[1, 3], [2, 4]])
raises(ValueError, lambda: m.vech())
raises(ShapeError, lambda: Matrix([ [1, 3] ]).vech())
raises(ValueError, lambda: Matrix([ [1, 3], [2, 4] ]).vech())
def test_diag():
# mostly tested in testcommonmatrix.py
assert diag([1, 2, 3]) == Matrix([1, 2, 3])
m = [1, 2, [3]]
raises(ValueError, lambda: diag(m))
assert diag(m, strict=False) == Matrix([1, 2, 3])
def test_get_diag_blocks1():
a = Matrix([[1, 2], [2, 3]])
b = Matrix([[3, x], [y, 3]])
c = Matrix([[3, x, 3], [y, 3, z], [x, y, z]])
assert a.get_diag_blocks() == [a]
assert b.get_diag_blocks() == [b]
assert c.get_diag_blocks() == [c]
def test_get_diag_blocks2():
a = Matrix([[1, 2], [2, 3]])
b = Matrix([[3, x], [y, 3]])
c = Matrix([[3, x, 3], [y, 3, z], [x, y, z]])
assert diag(a, b, b).get_diag_blocks() == [a, b, b]
assert diag(a, b, c).get_diag_blocks() == [a, b, c]
assert diag(a, c, b).get_diag_blocks() == [a, c, b]
assert diag(c, c, b).get_diag_blocks() == [c, c, b]
def test_inv_block():
a = Matrix([[1, 2], [2, 3]])
b = Matrix([[3, x], [y, 3]])
c = Matrix([[3, x, 3], [y, 3, z], [x, y, z]])
A = diag(a, b, b)
assert A.inv(try_block_diag=True) == diag(a.inv(), b.inv(), b.inv())
A = diag(a, b, c)
assert A.inv(try_block_diag=True) == diag(a.inv(), b.inv(), c.inv())
A = diag(a, c, b)
assert A.inv(try_block_diag=True) == diag(a.inv(), c.inv(), b.inv())
A = diag(a, a, b, a, c, a)
assert A.inv(try_block_diag=True) == diag(
a.inv(), a.inv(), b.inv(), a.inv(), c.inv(), a.inv())
assert A.inv(try_block_diag=True, method="ADJ") == diag(
a.inv(method="ADJ"), a.inv(method="ADJ"), b.inv(method="ADJ"),
a.inv(method="ADJ"), c.inv(method="ADJ"), a.inv(method="ADJ"))
def test_creation_args():
"""
Check that matrix dimensions can be specified using any reasonable type
(see issue 4614).
"""
raises(ValueError, lambda: zeros(3, -1))
raises(TypeError, lambda: zeros(1, 2, 3, 4))
assert zeros(long(3)) == zeros(3)
assert zeros(Integer(3)) == zeros(3)
raises(ValueError, lambda: zeros(3.))
assert eye(long(3)) == eye(3)
assert eye(Integer(3)) == eye(3)
raises(ValueError, lambda: eye(3.))
assert ones(long(3), Integer(4)) == ones(3, 4)
raises(TypeError, lambda: Matrix(5))
raises(TypeError, lambda: Matrix(1, 2))
raises(ValueError, lambda: Matrix([1, [2]]))
def test_diagonal_symmetrical():
m = Matrix(2, 2, [0, 1, 1, 0])
assert not m.is_diagonal()
assert m.is_symmetric()
assert m.is_symmetric(simplify=False)
m = Matrix(2, 2, [1, 0, 0, 1])
assert m.is_diagonal()
m = diag(1, 2, 3)
assert m.is_diagonal()
assert m.is_symmetric()
m = Matrix(3, 3, [1, 0, 0, 0, 2, 0, 0, 0, 3])
assert m == diag(1, 2, 3)
m = Matrix(2, 3, zeros(2, 3))
assert not m.is_symmetric()
assert m.is_diagonal()
m = Matrix(((5, 0), (0, 6), (0, 0)))
assert m.is_diagonal()
m = Matrix(((5, 0, 0), (0, 6, 0)))
assert m.is_diagonal()
m = Matrix(3, 3, [1, x**2 + 2*x + 1, y, (x + 1)**2, 2, 0, y, 0, 3])
assert m.is_symmetric()
assert not m.is_symmetric(simplify=False)
assert m.expand().is_symmetric(simplify=False)
def test_diagonalization():
m = Matrix(3, 2, [-3, 1, -3, 20, 3, 10])
assert not m.is_diagonalizable()
assert not m.is_symmetric()
raises(NonSquareMatrixError, lambda: m.diagonalize())
# diagonalizable
m = diag(1, 2, 3)
(P, D) = m.diagonalize()
assert P == eye(3)
assert D == m
m = Matrix(2, 2, [0, 1, 1, 0])
assert m.is_symmetric()
assert m.is_diagonalizable()
(P, D) = m.diagonalize()
assert P.inv() * m * P == D
m = Matrix(2, 2, [1, 0, 0, 3])
assert m.is_symmetric()
assert m.is_diagonalizable()
(P, D) = m.diagonalize()
assert P.inv() * m * P == D
assert P == eye(2)
assert D == m
m = Matrix(2, 2, [1, 1, 0, 0])
assert m.is_diagonalizable()
(P, D) = m.diagonalize()
assert P.inv() * m * P == D
m = Matrix(3, 3, [1, 2, 0, 0, 3, 0, 2, -4, 2])
assert m.is_diagonalizable()
(P, D) = m.diagonalize()
assert P.inv() * m * P == D
for i in P:
assert i.as_numer_denom()[1] == 1
m = Matrix(2, 2, [1, 0, 0, 0])
assert m.is_diagonal()
assert m.is_diagonalizable()
(P, D) = m.diagonalize()
assert P.inv() * m * P == D
assert P == Matrix([[0, 1], [1, 0]])
# diagonalizable, complex only
m = Matrix(2, 2, [0, 1, -1, 0])
assert not m.is_diagonalizable(True)
raises(MatrixError, lambda: m.diagonalize(True))
assert m.is_diagonalizable()
(P, D) = m.diagonalize()
assert P.inv() * m * P == D
# not diagonalizable
m = Matrix(2, 2, [0, 1, 0, 0])
assert not m.is_diagonalizable()
raises(MatrixError, lambda: m.diagonalize())
m = Matrix(3, 3, [-3, 1, -3, 20, 3, 10, 2, -2, 4])
assert not m.is_diagonalizable()
raises(MatrixError, lambda: m.diagonalize())
# symbolic
a, b, c, d = symbols('a b c d')
m = Matrix(2, 2, [a, c, c, b])
assert m.is_symmetric()
assert m.is_diagonalizable()
def test_issue_15887():
# Mutable matrix should not use cache
a = MutableDenseMatrix([[0, 1], [1, 0]])
assert a.is_diagonalizable() is True
a[1, 0] = 0
assert a.is_diagonalizable() is False
a = MutableDenseMatrix([[0, 1], [1, 0]])
a.diagonalize()
a[1, 0] = 0
raises(MatrixError, lambda: a.diagonalize())
# Test deprecated cache and kwargs
with warns_deprecated_sympy():
a.is_diagonalizable(clear_cache=True)
with warns_deprecated_sympy():
a.is_diagonalizable(clear_subproducts=True)
@XFAIL
def test_eigen_vects():
m = Matrix(2, 2, [1, 0, 0, I])
raises(NotImplementedError, lambda: m.is_diagonalizable(True))
# !!! bug because of eigenvects() or roots(x**2 + (-1 - I)*x + I, x)
# see issue 5292
assert not m.is_diagonalizable(True)
raises(MatrixError, lambda: m.diagonalize(True))
(P, D) = m.diagonalize(True)
def test_jordan_form():
m = Matrix(3, 2, [-3, 1, -3, 20, 3, 10])
raises(NonSquareMatrixError, lambda: m.jordan_form())
# diagonalizable
m = Matrix(3, 3, [7, -12, 6, 10, -19, 10, 12, -24, 13])
Jmust = Matrix(3, 3, [-1, 0, 0, 0, 1, 0, 0, 0, 1])
P, J = m.jordan_form()
assert Jmust == J
assert Jmust == m.diagonalize()[1]
# m = Matrix(3, 3, [0, 6, 3, 1, 3, 1, -2, 2, 1])
# m.jordan_form() # very long
# m.jordan_form() #
# diagonalizable, complex only
# Jordan cells
# complexity: one of eigenvalues is zero
m = Matrix(3, 3, [0, 1, 0, -4, 4, 0, -2, 1, 2])
# The blocks are ordered according to the value of their eigenvalues,
# in order to make the matrix compatible with .diagonalize()
Jmust = Matrix(3, 3, [2, 1, 0, 0, 2, 0, 0, 0, 2])
P, J = m.jordan_form()
assert Jmust == J
# complexity: all of eigenvalues are equal
m = Matrix(3, 3, [2, 6, -15, 1, 1, -5, 1, 2, -6])
# Jmust = Matrix(3, 3, [-1, 0, 0, 0, -1, 1, 0, 0, -1])
# same here see 1456ff
Jmust = Matrix(3, 3, [-1, 1, 0, 0, -1, 0, 0, 0, -1])
P, J = m.jordan_form()
assert Jmust == J
# complexity: two of eigenvalues are zero
m = Matrix(3, 3, [4, -5, 2, 5, -7, 3, 6, -9, 4])
Jmust = Matrix(3, 3, [0, 1, 0, 0, 0, 0, 0, 0, 1])
P, J = m.jordan_form()
assert Jmust == J
m = Matrix(4, 4, [6, 5, -2, -3, -3, -1, 3, 3, 2, 1, -2, -3, -1, 1, 5, 5])
Jmust = Matrix(4, 4, [2, 1, 0, 0,
0, 2, 0, 0,
0, 0, 2, 1,
0, 0, 0, 2]
)
P, J = m.jordan_form()
assert Jmust == J
m = Matrix(4, 4, [6, 2, -8, -6, -3, 2, 9, 6, 2, -2, -8, -6, -1, 0, 3, 4])
# Jmust = Matrix(4, 4, [2, 0, 0, 0, 0, 2, 1, 0, 0, 0, 2, 0, 0, 0, 0, -2])
# same here see 1456ff
Jmust = Matrix(4, 4, [-2, 0, 0, 0,
0, 2, 1, 0,
0, 0, 2, 0,
0, 0, 0, 2])
P, J = m.jordan_form()
assert Jmust == J
m = Matrix(4, 4, [5, 4, 2, 1, 0, 1, -1, -1, -1, -1, 3, 0, 1, 1, -1, 2])
assert not m.is_diagonalizable()
Jmust = Matrix(4, 4, [1, 0, 0, 0, 0, 2, 0, 0, 0, 0, 4, 1, 0, 0, 0, 4])
P, J = m.jordan_form()
assert Jmust == J
# checking for maximum precision to remain unchanged
m = Matrix([[Float('1.0', precision=110), Float('2.0', precision=110)],
[Float('3.14159265358979323846264338327', precision=110), Float('4.0', precision=110)]])
P, J = m.jordan_form()
for term in J._mat:
if isinstance(term, Float):
assert term._prec == 110
def test_jordan_form_complex_issue_9274():
A = Matrix([[ 2, 4, 1, 0],
[-4, 2, 0, 1],
[ 0, 0, 2, 4],
[ 0, 0, -4, 2]])
p = 2 - 4*I;
q = 2 + 4*I;
Jmust1 = Matrix([[p, 1, 0, 0],
[0, p, 0, 0],
[0, 0, q, 1],
[0, 0, 0, q]])
Jmust2 = Matrix([[q, 1, 0, 0],
[0, q, 0, 0],
[0, 0, p, 1],
[0, 0, 0, p]])
P, J = A.jordan_form()
assert J == Jmust1 or J == Jmust2
assert simplify(P*J*P.inv()) == A
def test_issue_10220():
# two non-orthogonal Jordan blocks with eigenvalue 1
M = Matrix([[1, 0, 0, 1],
[0, 1, 1, 0],
[0, 0, 1, 1],
[0, 0, 0, 1]])
P, J = M.jordan_form()
assert P == Matrix([[0, 1, 0, 1],
[1, 0, 0, 0],
[0, 1, 0, 0],
[0, 0, 1, 0]])
assert J == Matrix([
[1, 1, 0, 0],
[0, 1, 1, 0],
[0, 0, 1, 0],
[0, 0, 0, 1]])
def test_jordan_form_issue_15858():
A = Matrix([
[1, 1, 1, 0],
[-2, -1, 0, -1],
[0, 0, -1, -1],
[0, 0, 2, 1]])
(P, J) = A.jordan_form()
assert simplify(P) == Matrix([
[-I, -I/2, I, I/2],
[-1 + I, 0, -1 - I, 0],
[0, I*(-1 + I)/2, 0, I*(1 + I)/2],
[0, 1, 0, 1]])
assert J == Matrix([
[-I, 1, 0, 0],
[0, -I, 0, 0],
[0, 0, I, 1],
[0, 0, 0, I]])
def test_Matrix_berkowitz_charpoly():
UA, K_i, K_w = symbols('UA K_i K_w')
A = Matrix([[-K_i - UA + K_i**2/(K_i + K_w), K_i*K_w/(K_i + K_w)],
[ K_i*K_w/(K_i + K_w), -K_w + K_w**2/(K_i + K_w)]])
charpoly = A.charpoly(x)
assert charpoly == \
Poly(x**2 + (K_i*UA + K_w*UA + 2*K_i*K_w)/(K_i + K_w)*x +
K_i*K_w*UA/(K_i + K_w), x, domain='ZZ(K_i,K_w,UA)')
assert type(charpoly) is PurePoly
A = Matrix([[1, 3], [2, 0]])
assert A.charpoly() == A.charpoly(x) == PurePoly(x**2 - x - 6)
A = Matrix([[1, 2], [x, 0]])
p = A.charpoly(x)
assert p.gen != x
assert p.as_expr().subs(p.gen, x) == x**2 - 3*x
def test_exp_jordan_block():
l = Symbol('lamda')
m = Matrix.jordan_block(1, l)
assert m._eval_matrix_exp_jblock() == Matrix([[exp(l)]])
m = Matrix.jordan_block(3, l)
assert m._eval_matrix_exp_jblock() == \
Matrix([
[exp(l), exp(l), exp(l)/2],
[0, exp(l), exp(l)],
[0, 0, exp(l)]])
def test_exp():
m = Matrix([[3, 4], [0, -2]])
m_exp = Matrix([[exp(3), -4*exp(-2)/5 + 4*exp(3)/5], [0, exp(-2)]])
assert m.exp() == m_exp
assert exp(m) == m_exp
m = Matrix([[1, 0], [0, 1]])
assert m.exp() == Matrix([[E, 0], [0, E]])
assert exp(m) == Matrix([[E, 0], [0, E]])
m = Matrix([[1, -1], [1, 1]])
assert m.exp() == Matrix([[E*cos(1), -E*sin(1)], [E*sin(1), E*cos(1)]])
def test_log():
l = Symbol('lamda')
m = Matrix.jordan_block(1, l)
assert m._eval_matrix_log_jblock() == Matrix([[log(l)]])
m = Matrix.jordan_block(4, l)
assert m._eval_matrix_log_jblock() == \
Matrix(
[
[log(l), 1/l, -1/(2*l**2), 1/(3*l**3)],
[0, log(l), 1/l, -1/(2*l**2)],
[0, 0, log(l), 1/l],
[0, 0, 0, log(l)]
]
)
m = Matrix(
[[0, 0, 1],
[0, 0, 0],
[-1, 0, 0]]
)
raises(MatrixError, lambda: m.log())
def test_has():
A = Matrix(((x, y), (2, 3)))
assert A.has(x)
assert not A.has(z)
assert A.has(Symbol)
A = A.subs(x, 2)
assert not A.has(x)
def test_LUdecomposition_Simple_iszerofunc():
# Test if callable passed to matrices.LUdecomposition_Simple() as iszerofunc keyword argument is used inside
# matrices.LUdecomposition_Simple()
magic_string = "I got passed in!"
def goofyiszero(value):
raise ValueError(magic_string)
try:
lu, p = Matrix([[1, 0], [0, 1]]).LUdecomposition_Simple(iszerofunc=goofyiszero)
except ValueError as err:
assert magic_string == err.args[0]
return
assert False
def test_LUdecomposition_iszerofunc():
# Test if callable passed to matrices.LUdecomposition() as iszerofunc keyword argument is used inside
# matrices.LUdecomposition_Simple()
magic_string = "I got passed in!"
def goofyiszero(value):
raise ValueError(magic_string)
try:
l, u, p = Matrix([[1, 0], [0, 1]]).LUdecomposition(iszerofunc=goofyiszero)
except ValueError as err:
assert magic_string == err.args[0]
return
assert False
def test_find_reasonable_pivot_naive_finds_guaranteed_nonzero1():
# Test if matrices._find_reasonable_pivot_naive()
# finds a guaranteed non-zero pivot when the
# some of the candidate pivots are symbolic expressions.
# Keyword argument: simpfunc=None indicates that no simplifications
# should be performed during the search.
x = Symbol('x')
column = Matrix(3, 1, [x, cos(x)**2 + sin(x)**2, Rational(1, 2)])
pivot_offset, pivot_val, pivot_assumed_nonzero, simplified =\
_find_reasonable_pivot_naive(column)
assert pivot_val == Rational(1, 2)
def test_find_reasonable_pivot_naive_finds_guaranteed_nonzero2():
# Test if matrices._find_reasonable_pivot_naive()
# finds a guaranteed non-zero pivot when the
# some of the candidate pivots are symbolic expressions.
# Keyword argument: simpfunc=_simplify indicates that the search
# should attempt to simplify candidate pivots.
x = Symbol('x')
column = Matrix(3, 1,
[x,
cos(x)**2+sin(x)**2+x**2,
cos(x)**2+sin(x)**2])
pivot_offset, pivot_val, pivot_assumed_nonzero, simplified =\
_find_reasonable_pivot_naive(column, simpfunc=_simplify)
assert pivot_val == 1
def test_find_reasonable_pivot_naive_simplifies():
# Test if matrices._find_reasonable_pivot_naive()
# simplifies candidate pivots, and reports
# their offsets correctly.
x = Symbol('x')
column = Matrix(3, 1,
[x,
cos(x)**2+sin(x)**2+x,
cos(x)**2+sin(x)**2])
pivot_offset, pivot_val, pivot_assumed_nonzero, simplified =\
_find_reasonable_pivot_naive(column, simpfunc=_simplify)
assert len(simplified) == 2
assert simplified[0][0] == 1
assert simplified[0][1] == 1+x
assert simplified[1][0] == 2
assert simplified[1][1] == 1
def test_errors():
raises(ValueError, lambda: Matrix([[1, 2], [1]]))
raises(IndexError, lambda: Matrix([[1, 2]])[1.2, 5])
raises(IndexError, lambda: Matrix([[1, 2]])[1, 5.2])
raises(ValueError, lambda: randMatrix(3, c=4, symmetric=True))
raises(ValueError, lambda: Matrix([1, 2]).reshape(4, 6))
raises(ShapeError,
lambda: Matrix([[1, 2], [3, 4]]).copyin_matrix([1, 0], Matrix([1, 2])))
raises(TypeError, lambda: Matrix([[1, 2], [3, 4]]).copyin_list([0,
1], set([])))
raises(NonSquareMatrixError, lambda: Matrix([[1, 2, 3], [2, 3, 0]]).inv())
raises(ShapeError,
lambda: Matrix(1, 2, [1, 2]).row_join(Matrix([[1, 2], [3, 4]])))
raises(
ShapeError, lambda: Matrix([1, 2]).col_join(Matrix([[1, 2], [3, 4]])))
raises(ShapeError, lambda: Matrix([1]).row_insert(1, Matrix([[1,
2], [3, 4]])))
raises(ShapeError, lambda: Matrix([1]).col_insert(1, Matrix([[1,
2], [3, 4]])))
raises(NonSquareMatrixError, lambda: Matrix([1, 2]).trace())
raises(TypeError, lambda: Matrix([1]).applyfunc(1))
raises(ShapeError, lambda: Matrix([1]).LUsolve(Matrix([[1, 2], [3, 4]])))
raises(ValueError, lambda: Matrix([[1, 2], [3, 4]]).minor(4, 5))
raises(ValueError, lambda: Matrix([[1, 2], [3, 4]]).minor_submatrix(4, 5))
raises(TypeError, lambda: Matrix([1, 2, 3]).cross(1))
raises(TypeError, lambda: Matrix([1, 2, 3]).dot(1))
raises(ShapeError, lambda: Matrix([1, 2, 3]).dot(Matrix([1, 2])))
raises(ShapeError, lambda: Matrix([1, 2]).dot([]))
raises(TypeError, lambda: Matrix([1, 2]).dot('a'))
with warns_deprecated_sympy():
Matrix([[1, 2], [3, 4]]).dot(Matrix([[4, 3], [1, 2]]))
raises(ShapeError, lambda: Matrix([1, 2]).dot([1, 2, 3]))
raises(NonSquareMatrixError, lambda: Matrix([1, 2, 3]).exp())
raises(ShapeError, lambda: Matrix([[1, 2], [3, 4]]).normalized())
raises(ValueError, lambda: Matrix([1, 2]).inv(method='not a method'))
raises(NonSquareMatrixError, lambda: Matrix([1, 2]).inverse_GE())
raises(ValueError, lambda: Matrix([[1, 2], [1, 2]]).inverse_GE())
raises(NonSquareMatrixError, lambda: Matrix([1, 2]).inverse_ADJ())
raises(ValueError, lambda: Matrix([[1, 2], [1, 2]]).inverse_ADJ())
raises(NonSquareMatrixError, lambda: Matrix([1, 2]).inverse_LU())
raises(NonSquareMatrixError, lambda: Matrix([1, 2]).is_nilpotent())
raises(NonSquareMatrixError, lambda: Matrix([1, 2]).det())
raises(ValueError,
lambda: Matrix([[1, 2], [3, 4]]).det(method='Not a real method'))
raises(ValueError,
lambda: Matrix([[1, 2, 3, 4], [5, 6, 7, 8],
[9, 10, 11, 12], [13, 14, 15, 16]]).det(iszerofunc="Not function"))
raises(ValueError,
lambda: Matrix([[1, 2, 3, 4], [5, 6, 7, 8],
[9, 10, 11, 12], [13, 14, 15, 16]]).det(iszerofunc=False))
raises(ValueError,
lambda: hessian(Matrix([[1, 2], [3, 4]]), Matrix([[1, 2], [2, 1]])))
raises(ValueError, lambda: hessian(Matrix([[1, 2], [3, 4]]), []))
raises(ValueError, lambda: hessian(Symbol('x')**2, 'a'))
raises(IndexError, lambda: eye(3)[5, 2])
raises(IndexError, lambda: eye(3)[2, 5])
M = Matrix(((1, 2, 3, 4), (5, 6, 7, 8), (9, 10, 11, 12), (13, 14, 15, 16)))
raises(ValueError, lambda: M.det('method=LU_decomposition()'))
V = Matrix([[10, 10, 10]])
M = Matrix([[1, 2, 3], [2, 3, 4], [3, 4, 5]])
raises(ValueError, lambda: M.row_insert(4.7, V))
M = Matrix([[1, 2, 3], [2, 3, 4], [3, 4, 5]])
raises(ValueError, lambda: M.col_insert(-4.2, V))
def test_len():
assert len(Matrix()) == 0
assert len(Matrix([[1, 2]])) == len(Matrix([[1], [2]])) == 2
assert len(Matrix(0, 2, lambda i, j: 0)) == \
len(Matrix(2, 0, lambda i, j: 0)) == 0
assert len(Matrix([[0, 1, 2], [3, 4, 5]])) == 6
assert Matrix([1]) == Matrix([[1]])
assert not Matrix()
assert Matrix() == Matrix([])
def test_integrate():
A = Matrix(((1, 4, x), (y, 2, 4), (10, 5, x**2)))
assert A.integrate(x) == \
Matrix(((x, 4*x, x**2/2), (x*y, 2*x, 4*x), (10*x, 5*x, x**3/3)))
assert A.integrate(y) == \
Matrix(((y, 4*y, x*y), (y**2/2, 2*y, 4*y), (10*y, 5*y, y*x**2)))
def test_limit():
A = Matrix(((1, 4, sin(x)/x), (y, 2, 4), (10, 5, x**2 + 1)))
assert A.limit(x, 0) == Matrix(((1, 4, 1), (y, 2, 4), (10, 5, 1)))
def test_diff():
A = MutableDenseMatrix(((1, 4, x), (y, 2, 4), (10, 5, x**2 + 1)))
assert isinstance(A.diff(x), type(A))
assert A.diff(x) == MutableDenseMatrix(((0, 0, 1), (0, 0, 0), (0, 0, 2*x)))
assert A.diff(y) == MutableDenseMatrix(((0, 0, 0), (1, 0, 0), (0, 0, 0)))
assert diff(A, x) == MutableDenseMatrix(((0, 0, 1), (0, 0, 0), (0, 0, 2*x)))
assert diff(A, y) == MutableDenseMatrix(((0, 0, 0), (1, 0, 0), (0, 0, 0)))
A_imm = A.as_immutable()
assert isinstance(A_imm.diff(x), type(A_imm))
assert A_imm.diff(x) == ImmutableDenseMatrix(((0, 0, 1), (0, 0, 0), (0, 0, 2*x)))
assert A_imm.diff(y) == ImmutableDenseMatrix(((0, 0, 0), (1, 0, 0), (0, 0, 0)))
assert diff(A_imm, x) == ImmutableDenseMatrix(((0, 0, 1), (0, 0, 0), (0, 0, 2*x)))
assert diff(A_imm, y) == ImmutableDenseMatrix(((0, 0, 0), (1, 0, 0), (0, 0, 0)))
def test_diff_by_matrix():
# Derive matrix by matrix:
A = MutableDenseMatrix([[x, y], [z, t]])
assert A.diff(A) == Array([[[[1, 0], [0, 0]], [[0, 1], [0, 0]]], [[[0, 0], [1, 0]], [[0, 0], [0, 1]]]])
assert diff(A, A) == Array([[[[1, 0], [0, 0]], [[0, 1], [0, 0]]], [[[0, 0], [1, 0]], [[0, 0], [0, 1]]]])
A_imm = A.as_immutable()
assert A_imm.diff(A_imm) == Array([[[[1, 0], [0, 0]], [[0, 1], [0, 0]]], [[[0, 0], [1, 0]], [[0, 0], [0, 1]]]])
assert diff(A_imm, A_imm) == Array([[[[1, 0], [0, 0]], [[0, 1], [0, 0]]], [[[0, 0], [1, 0]], [[0, 0], [0, 1]]]])
# Derive a constant matrix:
assert A.diff(a) == MutableDenseMatrix([[0, 0], [0, 0]])
B = ImmutableDenseMatrix([a, b])
assert A.diff(B) == Array.zeros(2, 1, 2, 2)
assert A.diff(A) == Array([[[[1, 0], [0, 0]], [[0, 1], [0, 0]]], [[[0, 0], [1, 0]], [[0, 0], [0, 1]]]])
# Test diff with tuples:
dB = B.diff([[a, b]])
assert dB.shape == (2, 2, 1)
assert dB == Array([[[1], [0]], [[0], [1]]])
f = Function("f")
fxyz = f(x, y, z)
assert fxyz.diff([[x, y, z]]) == Array([fxyz.diff(x), fxyz.diff(y), fxyz.diff(z)])
assert fxyz.diff(([x, y, z], 2)) == Array([
[fxyz.diff(x, 2), fxyz.diff(x, y), fxyz.diff(x, z)],
[fxyz.diff(x, y), fxyz.diff(y, 2), fxyz.diff(y, z)],
[fxyz.diff(x, z), fxyz.diff(z, y), fxyz.diff(z, 2)],
])
expr = sin(x)*exp(y)
assert expr.diff([[x, y]]) == Array([cos(x)*exp(y), sin(x)*exp(y)])
assert expr.diff(y, ((x, y),)) == Array([cos(x)*exp(y), sin(x)*exp(y)])
assert expr.diff(x, ((x, y),)) == Array([-sin(x)*exp(y), cos(x)*exp(y)])
assert expr.diff(((y, x),), [[x, y]]) == Array([[cos(x)*exp(y), -sin(x)*exp(y)], [sin(x)*exp(y), cos(x)*exp(y)]])
# Test different notations:
fxyz.diff(x).diff(y).diff(x) == fxyz.diff(((x, y, z),), 3)[0, 1, 0]
fxyz.diff(z).diff(y).diff(x) == fxyz.diff(((x, y, z),), 3)[2, 1, 0]
fxyz.diff([[x, y, z]], ((z, y, x),)) == Array([[fxyz.diff(i).diff(j) for i in (x, y, z)] for j in (z, y, x)])
# Test scalar derived by matrix remains matrix:
res = x.diff(Matrix([[x, y]]))
assert isinstance(res, ImmutableDenseMatrix)
assert res == Matrix([[1, 0]])
res = (x**3).diff(Matrix([[x, y]]))
assert isinstance(res, ImmutableDenseMatrix)
assert res == Matrix([[3*x**2, 0]])
def test_getattr():
A = Matrix(((1, 4, x), (y, 2, 4), (10, 5, x**2 + 1)))
raises(AttributeError, lambda: A.nonexistantattribute)
assert getattr(A, 'diff')(x) == Matrix(((0, 0, 1), (0, 0, 0), (0, 0, 2*x)))
def test_hessenberg():
A = Matrix([[3, 4, 1], [2, 4, 5], [0, 1, 2]])
assert A.is_upper_hessenberg
A = A.T
assert A.is_lower_hessenberg
A[0, -1] = 1
assert A.is_lower_hessenberg is False
A = Matrix([[3, 4, 1], [2, 4, 5], [3, 1, 2]])
assert not A.is_upper_hessenberg
A = zeros(5, 2)
assert A.is_upper_hessenberg
def test_cholesky():
raises(NonSquareMatrixError, lambda: Matrix((1, 2)).cholesky())
raises(ValueError, lambda: Matrix(((1, 2), (3, 4))).cholesky())
raises(ValueError, lambda: Matrix(((5 + I, 0), (0, 1))).cholesky())
raises(ValueError, lambda: Matrix(((1, 5), (5, 1))).cholesky())
raises(ValueError, lambda: Matrix(((1, 2), (3, 4))).cholesky(hermitian=False))
assert Matrix(((5 + I, 0), (0, 1))).cholesky(hermitian=False) == Matrix([
[sqrt(5 + I), 0], [0, 1]])
A = Matrix(((1, 5), (5, 1)))
L = A.cholesky(hermitian=False)
assert L == Matrix([[1, 0], [5, 2*sqrt(6)*I]])
assert L*L.T == A
A = Matrix(((25, 15, -5), (15, 18, 0), (-5, 0, 11)))
L = A.cholesky()
assert L * L.T == A
assert L.is_lower
assert L == Matrix([[5, 0, 0], [3, 3, 0], [-1, 1, 3]])
A = Matrix(((4, -2*I, 2 + 2*I), (2*I, 2, -1 + I), (2 - 2*I, -1 - I, 11)))
assert A.cholesky() == Matrix(((2, 0, 0), (I, 1, 0), (1 - I, 0, 3)))
def test_LDLdecomposition():
raises(NonSquareMatrixError, lambda: Matrix((1, 2)).LDLdecomposition())
raises(ValueError, lambda: Matrix(((1, 2), (3, 4))).LDLdecomposition())
raises(ValueError, lambda: Matrix(((5 + I, 0), (0, 1))).LDLdecomposition())
raises(ValueError, lambda: Matrix(((1, 5), (5, 1))).LDLdecomposition())
raises(ValueError, lambda: Matrix(((1, 2), (3, 4))).LDLdecomposition(hermitian=False))
A = Matrix(((1, 5), (5, 1)))
L, D = A.LDLdecomposition(hermitian=False)
assert L * D * L.T == A
A = Matrix(((25, 15, -5), (15, 18, 0), (-5, 0, 11)))
L, D = A.LDLdecomposition()
assert L * D * L.T == A
assert L.is_lower
assert L == Matrix([[1, 0, 0], [ S(3)/5, 1, 0], [S(-1)/5, S(1)/3, 1]])
assert D.is_diagonal()
assert D == Matrix([[25, 0, 0], [0, 9, 0], [0, 0, 9]])
A = Matrix(((4, -2*I, 2 + 2*I), (2*I, 2, -1 + I), (2 - 2*I, -1 - I, 11)))
L, D = A.LDLdecomposition()
assert expand_mul(L * D * L.H) == A
assert L == Matrix(((1, 0, 0), (I/2, 1, 0), (S(1)/2 - I/2, 0, 1)))
assert D == Matrix(((4, 0, 0), (0, 1, 0), (0, 0, 9)))
def test_cholesky_solve():
A = Matrix([[2, 3, 5],
[3, 6, 2],
[8, 3, 6]])
x = Matrix(3, 1, [3, 7, 5])
b = A*x
soln = A.cholesky_solve(b)
assert soln == x
A = Matrix([[0, -1, 2],
[5, 10, 7],
[8, 3, 4]])
x = Matrix(3, 1, [-1, 2, 5])
b = A*x
soln = A.cholesky_solve(b)
assert soln == x
A = Matrix(((1, 5), (5, 1)))
x = Matrix((4, -3))
b = A*x
soln = A.cholesky_solve(b)
assert soln == x
A = Matrix(((9, 3*I), (-3*I, 5)))
x = Matrix((-2, 1))
b = A*x
soln = A.cholesky_solve(b)
assert expand_mul(soln) == x
A = Matrix(((9*I, 3), (-3 + I, 5)))
x = Matrix((2 + 3*I, -1))
b = A*x
soln = A.cholesky_solve(b)
assert expand_mul(soln) == x
a00, a01, a11, b0, b1 = symbols('a00, a01, a11, b0, b1')
A = Matrix(((a00, a01), (a01, a11)))
b = Matrix((b0, b1))
x = A.cholesky_solve(b)
assert simplify(A*x) == b
def test_LDLsolve():
A = Matrix([[2, 3, 5],
[3, 6, 2],
[8, 3, 6]])
x = Matrix(3, 1, [3, 7, 5])
b = A*x
soln = A.LDLsolve(b)
assert soln == x
A = Matrix([[0, -1, 2],
[5, 10, 7],
[8, 3, 4]])
x = Matrix(3, 1, [-1, 2, 5])
b = A*x
soln = A.LDLsolve(b)
assert soln == x
A = Matrix(((9, 3*I), (-3*I, 5)))
x = Matrix((-2, 1))
b = A*x
soln = A.LDLsolve(b)
assert expand_mul(soln) == x
A = Matrix(((9*I, 3), (-3 + I, 5)))
x = Matrix((2 + 3*I, -1))
b = A*x
soln = A.LDLsolve(b)
assert expand_mul(soln) == x
A = Matrix(((9, 3), (3, 9)))
x = Matrix((1, 1))
b = A * x
soln = A.LDLsolve(b)
assert expand_mul(soln) == x
A = Matrix([[-5, -3, -4], [-3, -7, 7]])
x = Matrix([[8], [7], [-2]])
b = A * x
raises(NotImplementedError, lambda: A.LDLsolve(b))
def test_lower_triangular_solve():
raises(NonSquareMatrixError,
lambda: Matrix([1, 0]).lower_triangular_solve(Matrix([0, 1])))
raises(ShapeError,
lambda: Matrix([[1, 0], [0, 1]]).lower_triangular_solve(Matrix([1])))
raises(ValueError,
lambda: Matrix([[2, 1], [1, 2]]).lower_triangular_solve(
Matrix([[1, 0], [0, 1]])))
A = Matrix([[1, 0], [0, 1]])
B = Matrix([[x, y], [y, x]])
C = Matrix([[4, 8], [2, 9]])
assert A.lower_triangular_solve(B) == B
assert A.lower_triangular_solve(C) == C
def test_upper_triangular_solve():
raises(NonSquareMatrixError,
lambda: Matrix([1, 0]).upper_triangular_solve(Matrix([0, 1])))
raises(TypeError,
lambda: Matrix([[1, 0], [0, 1]]).upper_triangular_solve(Matrix([1])))
raises(TypeError,
lambda: Matrix([[2, 1], [1, 2]]).upper_triangular_solve(
Matrix([[1, 0], [0, 1]])))
A = Matrix([[1, 0], [0, 1]])
B = Matrix([[x, y], [y, x]])
C = Matrix([[2, 4], [3, 8]])
assert A.upper_triangular_solve(B) == B
assert A.upper_triangular_solve(C) == C
def test_diagonal_solve():
raises(TypeError, lambda: Matrix([1, 1]).diagonal_solve(Matrix([1])))
A = Matrix([[1, 0], [0, 1]])*2
B = Matrix([[x, y], [y, x]])
assert A.diagonal_solve(B) == B/2
A = Matrix([[1, 0], [1, 2]])
raises(TypeError, lambda: A.diagonal_solve(B))
def test_matrix_norm():
# Vector Tests
# Test columns and symbols
x = Symbol('x', real=True)
v = Matrix([cos(x), sin(x)])
assert trigsimp(v.norm(2)) == 1
assert v.norm(10) == Pow(cos(x)**10 + sin(x)**10, S(1)/10)
# Test Rows
A = Matrix([[5, Rational(3, 2)]])
assert A.norm() == Pow(25 + Rational(9, 4), S(1)/2)
assert A.norm(oo) == max(A._mat)
assert A.norm(-oo) == min(A._mat)
# Matrix Tests
# Intuitive test
A = Matrix([[1, 1], [1, 1]])
assert A.norm(2) == 2
assert A.norm(-2) == 0
assert A.norm('frobenius') == 2
assert eye(10).norm(2) == eye(10).norm(-2) == 1
assert A.norm(oo) == 2
# Test with Symbols and more complex entries
A = Matrix([[3, y, y], [x, S(1)/2, -pi]])
assert (A.norm('fro')
== sqrt(S(37)/4 + 2*abs(y)**2 + pi**2 + x**2))
# Check non-square
A = Matrix([[1, 2, -3], [4, 5, Rational(13, 2)]])
assert A.norm(2) == sqrt(S(389)/8 + sqrt(78665)/8)
assert A.norm(-2) == S(0)
assert A.norm('frobenius') == sqrt(389)/2
# Test properties of matrix norms
# https://en.wikipedia.org/wiki/Matrix_norm#Definition
# Two matrices
A = Matrix([[1, 2], [3, 4]])
B = Matrix([[5, 5], [-2, 2]])
C = Matrix([[0, -I], [I, 0]])
D = Matrix([[1, 0], [0, -1]])
L = [A, B, C, D]
alpha = Symbol('alpha', real=True)
for order in ['fro', 2, -2]:
# Zero Check
assert zeros(3).norm(order) == S(0)
# Check Triangle Inequality for all Pairs of Matrices
for X in L:
for Y in L:
dif = (X.norm(order) + Y.norm(order) -
(X + Y).norm(order))
assert (dif >= 0)
# Scalar multiplication linearity
for M in [A, B, C, D]:
dif = simplify((alpha*M).norm(order) -
abs(alpha) * M.norm(order))
assert dif == 0
# Test Properties of Vector Norms
# https://en.wikipedia.org/wiki/Vector_norm
# Two column vectors
a = Matrix([1, 1 - 1*I, -3])
b = Matrix([S(1)/2, 1*I, 1])
c = Matrix([-1, -1, -1])
d = Matrix([3, 2, I])
e = Matrix([Integer(1e2), Rational(1, 1e2), 1])
L = [a, b, c, d, e]
alpha = Symbol('alpha', real=True)
for order in [1, 2, -1, -2, S.Infinity, S.NegativeInfinity, pi]:
# Zero Check
if order > 0:
assert Matrix([0, 0, 0]).norm(order) == S(0)
# Triangle inequality on all pairs
if order >= 1: # Triangle InEq holds only for these norms
for X in L:
for Y in L:
dif = (X.norm(order) + Y.norm(order) -
(X + Y).norm(order))
assert simplify(dif >= 0) is S.true
# Linear to scalar multiplication
if order in [1, 2, -1, -2, S.Infinity, S.NegativeInfinity]:
for X in L:
dif = simplify((alpha*X).norm(order) -
(abs(alpha) * X.norm(order)))
assert dif == 0
# ord=1
M = Matrix(3, 3, [1, 3, 0, -2, -1, 0, 3, 9, 6])
assert M.norm(1) == 13
def test_condition_number():
x = Symbol('x', real=True)
A = eye(3)
A[0, 0] = 10
A[2, 2] = S(1)/10
assert A.condition_number() == 100
A[1, 1] = x
assert A.condition_number() == Max(10, Abs(x)) / Min(S(1)/10, Abs(x))
M = Matrix([[cos(x), sin(x)], [-sin(x), cos(x)]])
Mc = M.condition_number()
assert all(Float(1.).epsilon_eq(Mc.subs(x, val).evalf()) for val in
[Rational(1, 5), Rational(1, 2), Rational(1, 10), pi/2, pi, 7*pi/4 ])
#issue 10782
assert Matrix([]).condition_number() == 0
def test_equality():
A = Matrix(((1, 2, 3), (4, 5, 6), (7, 8, 9)))
B = Matrix(((9, 8, 7), (6, 5, 4), (3, 2, 1)))
assert A == A[:, :]
assert not A != A[:, :]
assert not A == B
assert A != B
assert A != 10
assert not A == 10
# A SparseMatrix can be equal to a Matrix
C = SparseMatrix(((1, 0, 0), (0, 1, 0), (0, 0, 1)))
D = Matrix(((1, 0, 0), (0, 1, 0), (0, 0, 1)))
assert C == D
assert not C != D
def test_col_join():
assert eye(3).col_join(Matrix([[7, 7, 7]])) == \
Matrix([[1, 0, 0],
[0, 1, 0],
[0, 0, 1],
[7, 7, 7]])
def test_row_insert():
r4 = Matrix([[4, 4, 4]])
for i in range(-4, 5):
l = [1, 0, 0]
l.insert(i, 4)
assert flatten(eye(3).row_insert(i, r4).col(0).tolist()) == l
def test_col_insert():
c4 = Matrix([4, 4, 4])
for i in range(-4, 5):
l = [0, 0, 0]
l.insert(i, 4)
assert flatten(zeros(3).col_insert(i, c4).row(0).tolist()) == l
def test_normalized():
assert Matrix([3, 4]).normalized() == \
Matrix([Rational(3, 5), Rational(4, 5)])
# Zero vector trivial cases
assert Matrix([0, 0, 0]).normalized() == Matrix([0, 0, 0])
# Machine precision error truncation trivial cases
m = Matrix([0,0,1.e-100])
assert m.normalized(
iszerofunc=lambda x: x.evalf(n=10, chop=True).is_zero
) == Matrix([0, 0, 0])
def test_print_nonzero():
assert capture(lambda: eye(3).print_nonzero()) == \
'[X ]\n[ X ]\n[ X]\n'
assert capture(lambda: eye(3).print_nonzero('.')) == \
'[. ]\n[ . ]\n[ .]\n'
def test_zeros_eye():
assert Matrix.eye(3) == eye(3)
assert Matrix.zeros(3) == zeros(3)
assert ones(3, 4) == Matrix(3, 4, [1]*12)
i = Matrix([[1, 0], [0, 1]])
z = Matrix([[0, 0], [0, 0]])
for cls in classes:
m = cls.eye(2)
assert i == m # but m == i will fail if m is immutable
assert i == eye(2, cls=cls)
assert type(m) == cls
m = cls.zeros(2)
assert z == m
assert z == zeros(2, cls=cls)
assert type(m) == cls
def test_is_zero():
assert Matrix().is_zero
assert Matrix([[0, 0], [0, 0]]).is_zero
assert zeros(3, 4).is_zero
assert not eye(3).is_zero
assert Matrix([[x, 0], [0, 0]]).is_zero == None
assert SparseMatrix([[x, 0], [0, 0]]).is_zero == None
assert ImmutableMatrix([[x, 0], [0, 0]]).is_zero == None
assert ImmutableSparseMatrix([[x, 0], [0, 0]]).is_zero == None
assert Matrix([[x, 1], [0, 0]]).is_zero == False
a = Symbol('a', nonzero=True)
assert Matrix([[a, 0], [0, 0]]).is_zero == False
def test_rotation_matrices():
# This tests the rotation matrices by rotating about an axis and back.
theta = pi/3
r3_plus = rot_axis3(theta)
r3_minus = rot_axis3(-theta)
r2_plus = rot_axis2(theta)
r2_minus = rot_axis2(-theta)
r1_plus = rot_axis1(theta)
r1_minus = rot_axis1(-theta)
assert r3_minus*r3_plus*eye(3) == eye(3)
assert r2_minus*r2_plus*eye(3) == eye(3)
assert r1_minus*r1_plus*eye(3) == eye(3)
# Check the correctness of the trace of the rotation matrix
assert r1_plus.trace() == 1 + 2*cos(theta)
assert r2_plus.trace() == 1 + 2*cos(theta)
assert r3_plus.trace() == 1 + 2*cos(theta)
# Check that a rotation with zero angle doesn't change anything.
assert rot_axis1(0) == eye(3)
assert rot_axis2(0) == eye(3)
assert rot_axis3(0) == eye(3)
def test_DeferredVector():
assert str(DeferredVector("vector")[4]) == "vector[4]"
assert sympify(DeferredVector("d")) == DeferredVector("d")
raises(IndexError, lambda: DeferredVector("d")[-1])
assert str(DeferredVector("d")) == "d"
assert repr(DeferredVector("test")) == "DeferredVector('test')"
def test_DeferredVector_not_iterable():
assert not iterable(DeferredVector('X'))
def test_DeferredVector_Matrix():
raises(TypeError, lambda: Matrix(DeferredVector("V")))
def test_GramSchmidt():
R = Rational
m1 = Matrix(1, 2, [1, 2])
m2 = Matrix(1, 2, [2, 3])
assert GramSchmidt([m1, m2]) == \
[Matrix(1, 2, [1, 2]), Matrix(1, 2, [R(2)/5, R(-1)/5])]
assert GramSchmidt([m1.T, m2.T]) == \
[Matrix(2, 1, [1, 2]), Matrix(2, 1, [R(2)/5, R(-1)/5])]
# from wikipedia
assert GramSchmidt([Matrix([3, 1]), Matrix([2, 2])], True) == [
Matrix([3*sqrt(10)/10, sqrt(10)/10]),
Matrix([-sqrt(10)/10, 3*sqrt(10)/10])]
def test_casoratian():
assert casoratian([1, 2, 3, 4], 1) == 0
assert casoratian([1, 2, 3, 4], 1, zero=False) == 0
def test_zero_dimension_multiply():
assert (Matrix()*zeros(0, 3)).shape == (0, 3)
assert zeros(3, 0)*zeros(0, 3) == zeros(3, 3)
assert zeros(0, 3)*zeros(3, 0) == Matrix()
def test_slice_issue_2884():
m = Matrix(2, 2, range(4))
assert m[1, :] == Matrix([[2, 3]])
assert m[-1, :] == Matrix([[2, 3]])
assert m[:, 1] == Matrix([[1, 3]]).T
assert m[:, -1] == Matrix([[1, 3]]).T
raises(IndexError, lambda: m[2, :])
raises(IndexError, lambda: m[2, 2])
def test_slice_issue_3401():
assert zeros(0, 3)[:, -1].shape == (0, 1)
assert zeros(3, 0)[0, :] == Matrix(1, 0, [])
def test_copyin():
s = zeros(3, 3)
s[3] = 1
assert s[:, 0] == Matrix([0, 1, 0])
assert s[3] == 1
assert s[3: 4] == [1]
s[1, 1] = 42
assert s[1, 1] == 42
assert s[1, 1:] == Matrix([[42, 0]])
s[1, 1:] = Matrix([[5, 6]])
assert s[1, :] == Matrix([[1, 5, 6]])
s[1, 1:] = [[42, 43]]
assert s[1, :] == Matrix([[1, 42, 43]])
s[0, 0] = 17
assert s[:, :1] == Matrix([17, 1, 0])
s[0, 0] = [1, 1, 1]
assert s[:, 0] == Matrix([1, 1, 1])
s[0, 0] = Matrix([1, 1, 1])
assert s[:, 0] == Matrix([1, 1, 1])
s[0, 0] = SparseMatrix([1, 1, 1])
assert s[:, 0] == Matrix([1, 1, 1])
def test_invertible_check():
# sometimes a singular matrix will have a pivot vector shorter than
# the number of rows in a matrix...
assert Matrix([[1, 2], [1, 2]]).rref() == (Matrix([[1, 2], [0, 0]]), (0,))
raises(ValueError, lambda: Matrix([[1, 2], [1, 2]]).inv())
m = Matrix([
[-1, -1, 0],
[ x, 1, 1],
[ 1, x, -1],
])
assert len(m.rref()[1]) != m.rows
# in addition, unless simplify=True in the call to rref, the identity
# matrix will be returned even though m is not invertible
assert m.rref()[0] != eye(3)
assert m.rref(simplify=signsimp)[0] != eye(3)
raises(ValueError, lambda: m.inv(method="ADJ"))
raises(ValueError, lambda: m.inv(method="GE"))
raises(ValueError, lambda: m.inv(method="LU"))
def test_issue_3959():
x, y = symbols('x, y')
e = x*y
assert e.subs(x, Matrix([3, 5, 3])) == Matrix([3, 5, 3])*y
def test_issue_5964():
assert str(Matrix([[1, 2], [3, 4]])) == 'Matrix([[1, 2], [3, 4]])'
def test_issue_7604():
x, y = symbols(u"x y")
assert sstr(Matrix([[x, 2*y], [y**2, x + 3]])) == \
'Matrix([\n[ x, 2*y],\n[y**2, x + 3]])'
def test_is_Identity():
assert eye(3).is_Identity
assert eye(3).as_immutable().is_Identity
assert not zeros(3).is_Identity
assert not ones(3).is_Identity
# issue 6242
assert not Matrix([[1, 0, 0]]).is_Identity
# issue 8854
assert SparseMatrix(3,3, {(0,0):1, (1,1):1, (2,2):1}).is_Identity
assert not SparseMatrix(2,3, range(6)).is_Identity
assert not SparseMatrix(3,3, {(0,0):1, (1,1):1}).is_Identity
assert not SparseMatrix(3,3, {(0,0):1, (1,1):1, (2,2):1, (0,1):2, (0,2):3}).is_Identity
def test_dot():
assert ones(1, 3).dot(ones(3, 1)) == 3
assert ones(1, 3).dot([1, 1, 1]) == 3
assert Matrix([1, 2, 3]).dot(Matrix([1, 2, 3])) == 14
assert Matrix([1, 2, 3*I]).dot(Matrix([I, 2, 3*I])) == -5 + I
assert Matrix([1, 2, 3*I]).dot(Matrix([I, 2, 3*I]), hermitian=False) == -5 + I
assert Matrix([1, 2, 3*I]).dot(Matrix([I, 2, 3*I]), hermitian=True) == 13 + I
assert Matrix([1, 2, 3*I]).dot(Matrix([I, 2, 3*I]), hermitian=True, conjugate_convention="physics") == 13 - I
assert Matrix([1, 2, 3*I]).dot(Matrix([4, 5*I, 6]), hermitian=True, conjugate_convention="right") == 4 + 8*I
assert Matrix([1, 2, 3*I]).dot(Matrix([4, 5*I, 6]), hermitian=True, conjugate_convention="left") == 4 - 8*I
assert Matrix([I, 2*I]).dot(Matrix([I, 2*I]), hermitian=False, conjugate_convention="left") == -5
assert Matrix([I, 2*I]).dot(Matrix([I, 2*I]), conjugate_convention="left") == 5
raises(ValueError, lambda: Matrix([1, 2]).dot(Matrix([3, 4]), hermitian=True, conjugate_convention="test"))
def test_dual():
B_x, B_y, B_z, E_x, E_y, E_z = symbols(
'B_x B_y B_z E_x E_y E_z', real=True)
F = Matrix((
( 0, E_x, E_y, E_z),
(-E_x, 0, B_z, -B_y),
(-E_y, -B_z, 0, B_x),
(-E_z, B_y, -B_x, 0)
))
Fd = Matrix((
( 0, -B_x, -B_y, -B_z),
(B_x, 0, E_z, -E_y),
(B_y, -E_z, 0, E_x),
(B_z, E_y, -E_x, 0)
))
assert F.dual().equals(Fd)
assert eye(3).dual().equals(zeros(3))
assert F.dual().dual().equals(-F)
def test_anti_symmetric():
assert Matrix([1, 2]).is_anti_symmetric() is False
m = Matrix(3, 3, [0, x**2 + 2*x + 1, y, -(x + 1)**2, 0, x*y, -y, -x*y, 0])
assert m.is_anti_symmetric() is True
assert m.is_anti_symmetric(simplify=False) is False
assert m.is_anti_symmetric(simplify=lambda x: x) is False
# tweak to fail
m[2, 1] = -m[2, 1]
assert m.is_anti_symmetric() is False
# untweak
m[2, 1] = -m[2, 1]
m = m.expand()
assert m.is_anti_symmetric(simplify=False) is True
m[0, 0] = 1
assert m.is_anti_symmetric() is False
def test_normalize_sort_diogonalization():
A = Matrix(((1, 2), (2, 1)))
P, Q = A.diagonalize(normalize=True)
assert P*P.T == P.T*P == eye(P.cols)
P, Q = A.diagonalize(normalize=True, sort=True)
assert P*P.T == P.T*P == eye(P.cols)
assert P*Q*P.inv() == A
def test_issue_5321():
raises(ValueError, lambda: Matrix([[1, 2, 3], Matrix(0, 1, [])]))
def test_issue_5320():
assert Matrix.hstack(eye(2), 2*eye(2)) == Matrix([
[1, 0, 2, 0],
[0, 1, 0, 2]
])
assert Matrix.vstack(eye(2), 2*eye(2)) == Matrix([
[1, 0],
[0, 1],
[2, 0],
[0, 2]
])
cls = SparseMatrix
assert cls.hstack(cls(eye(2)), cls(2*eye(2))) == Matrix([
[1, 0, 2, 0],
[0, 1, 0, 2]
])
def test_issue_11944():
A = Matrix([[1]])
AIm = sympify(A)
assert Matrix.hstack(AIm, A) == Matrix([[1, 1]])
assert Matrix.vstack(AIm, A) == Matrix([[1], [1]])
def test_cross():
a = [1, 2, 3]
b = [3, 4, 5]
col = Matrix([-2, 4, -2])
row = col.T
def test(M, ans):
assert ans == M
assert type(M) == cls
for cls in classes:
A = cls(a)
B = cls(b)
test(A.cross(B), col)
test(A.cross(B.T), col)
test(A.T.cross(B.T), row)
test(A.T.cross(B), row)
raises(ShapeError, lambda:
Matrix(1, 2, [1, 1]).cross(Matrix(1, 2, [1, 1])))
def test_hash():
for cls in classes[-2:]:
s = {cls.eye(1), cls.eye(1)}
assert len(s) == 1 and s.pop() == cls.eye(1)
# issue 3979
for cls in classes[:2]:
assert not isinstance(cls.eye(1), Hashable)
@XFAIL
def test_issue_3979():
# when this passes, delete this and change the [1:2]
# to [:2] in the test_hash above for issue 3979
cls = classes[0]
raises(AttributeError, lambda: hash(cls.eye(1)))
def test_adjoint():
dat = [[0, I], [1, 0]]
ans = Matrix([[0, 1], [-I, 0]])
for cls in classes:
assert ans == cls(dat).adjoint()
def test_simplify_immutable():
from sympy import simplify, sin, cos
assert simplify(ImmutableMatrix([[sin(x)**2 + cos(x)**2]])) == \
ImmutableMatrix([[1]])
def test_rank():
from sympy.abc import x
m = Matrix([[1, 2], [x, 1 - 1/x]])
assert m.rank() == 2
n = Matrix(3, 3, range(1, 10))
assert n.rank() == 2
p = zeros(3)
assert p.rank() == 0
def test_issue_11434():
ax, ay, bx, by, cx, cy, dx, dy, ex, ey, t0, t1 = \
symbols('a_x a_y b_x b_y c_x c_y d_x d_y e_x e_y t_0 t_1')
M = Matrix([[ax, ay, ax*t0, ay*t0, 0],
[bx, by, bx*t0, by*t0, 0],
[cx, cy, cx*t0, cy*t0, 1],
[dx, dy, dx*t0, dy*t0, 1],
[ex, ey, 2*ex*t1 - ex*t0, 2*ey*t1 - ey*t0, 0]])
assert M.rank() == 4
def test_rank_regression_from_so():
# see:
# https://stackoverflow.com/questions/19072700/why-does-sympy-give-me-the-wrong-answer-when-i-row-reduce-a-symbolic-matrix
nu, lamb = symbols('nu, lambda')
A = Matrix([[-3*nu, 1, 0, 0],
[ 3*nu, -2*nu - 1, 2, 0],
[ 0, 2*nu, (-1*nu) - lamb - 2, 3],
[ 0, 0, nu + lamb, -3]])
expected_reduced = Matrix([[1, 0, 0, 1/(nu**2*(-lamb - nu))],
[0, 1, 0, 3/(nu*(-lamb - nu))],
[0, 0, 1, 3/(-lamb - nu)],
[0, 0, 0, 0]])
expected_pivots = (0, 1, 2)
reduced, pivots = A.rref()
assert simplify(expected_reduced - reduced) == zeros(*A.shape)
assert pivots == expected_pivots
def test_replace():
from sympy import symbols, Function, Matrix
F, G = symbols('F, G', cls=Function)
K = Matrix(2, 2, lambda i, j: G(i+j))
M = Matrix(2, 2, lambda i, j: F(i+j))
N = M.replace(F, G)
assert N == K
def test_replace_map():
from sympy import symbols, Function, Matrix
F, G = symbols('F, G', cls=Function)
K = Matrix(2, 2, [(G(0), {F(0): G(0)}), (G(1), {F(1): G(1)}), (G(1), {F(1)\
: G(1)}), (G(2), {F(2): G(2)})])
M = Matrix(2, 2, lambda i, j: F(i+j))
N = M.replace(F, G, True)
assert N == K
def test_atoms():
m = Matrix([[1, 2], [x, 1 - 1/x]])
assert m.atoms() == {S(1),S(2),S(-1), x}
assert m.atoms(Symbol) == {x}
def test_pinv():
# Pseudoinverse of an invertible matrix is the inverse.
A1 = Matrix([[a, b], [c, d]])
assert simplify(A1.pinv(method="RD")) == simplify(A1.inv())
# Test the four properties of the pseudoinverse for various matrices.
As = [Matrix([[13, 104], [2212, 3], [-3, 5]]),
Matrix([[1, 7, 9], [11, 17, 19]]),
Matrix([a, b])]
for A in As:
A_pinv = A.pinv(method="RD")
AAp = A * A_pinv
ApA = A_pinv * A
assert simplify(AAp * A) == A
assert simplify(ApA * A_pinv) == A_pinv
assert AAp.H == AAp
assert ApA.H == ApA
# XXX Pinv with diagonalization makes expression too complicated.
for A in As:
A_pinv = simplify(A.pinv(method="ED"))
AAp = A * A_pinv
ApA = A_pinv * A
assert simplify(AAp * A) == A
assert simplify(ApA * A_pinv) == A_pinv
assert AAp.H == AAp
assert ApA.H == ApA
# XXX Computing pinv using diagonalization makes an expression that
# is too complicated to simplify.
# A1 = Matrix([[a, b], [c, d]])
# assert simplify(A1.pinv(method="ED")) == simplify(A1.inv())
# so this is tested numerically at a fixed random point
from sympy.core.numbers import comp
q = A1.pinv(method="ED")
w = A1.inv()
reps = {a: -73633, b: 11362, c: 55486, d: 62570}
assert all(
comp(i.n(), j.n())
for i, j in zip(q.subs(reps), w.subs(reps))
)
def test_pinv_solve():
# Fully determined system (unique result, identical to other solvers).
A = Matrix([[1, 5], [7, 9]])
B = Matrix([12, 13])
assert A.pinv_solve(B) == A.cholesky_solve(B)
assert A.pinv_solve(B) == A.LDLsolve(B)
assert A.pinv_solve(B) == Matrix([sympify('-43/26'), sympify('71/26')])
assert A * A.pinv() * B == B
# Fully determined, with two-dimensional B matrix.
B = Matrix([[12, 13, 14], [15, 16, 17]])
assert A.pinv_solve(B) == A.cholesky_solve(B)
assert A.pinv_solve(B) == A.LDLsolve(B)
assert A.pinv_solve(B) == Matrix([[-33, -37, -41], [69, 75, 81]]) / 26
assert A * A.pinv() * B == B
# Underdetermined system (infinite results).
A = Matrix([[1, 0, 1], [0, 1, 1]])
B = Matrix([5, 7])
solution = A.pinv_solve(B)
w = {}
for s in solution.atoms(Symbol):
# Extract dummy symbols used in the solution.
w[s.name] = s
assert solution == Matrix([[w['w0_0']/3 + w['w1_0']/3 - w['w2_0']/3 + 1],
[w['w0_0']/3 + w['w1_0']/3 - w['w2_0']/3 + 3],
[-w['w0_0']/3 - w['w1_0']/3 + w['w2_0']/3 + 4]])
assert A * A.pinv() * B == B
# Overdetermined system (least squares results).
A = Matrix([[1, 0], [0, 0], [0, 1]])
B = Matrix([3, 2, 1])
assert A.pinv_solve(B) == Matrix([3, 1])
# Proof the solution is not exact.
assert A * A.pinv() * B != B
def test_pinv_rank_deficient():
# Test the four properties of the pseudoinverse for various matrices.
As = [Matrix([[1, 1, 1], [2, 2, 2]]),
Matrix([[1, 0], [0, 0]]),
Matrix([[1, 2], [2, 4], [3, 6]])]
for A in As:
A_pinv = A.pinv(method="RD")
AAp = A * A_pinv
ApA = A_pinv * A
assert simplify(AAp * A) == A
assert simplify(ApA * A_pinv) == A_pinv
assert AAp.H == AAp
assert ApA.H == ApA
for A in As:
A_pinv = A.pinv(method="ED")
AAp = A * A_pinv
ApA = A_pinv * A
assert simplify(AAp * A) == A
assert simplify(ApA * A_pinv) == A_pinv
assert AAp.H == AAp
assert ApA.H == ApA
# Test solving with rank-deficient matrices.
A = Matrix([[1, 0], [0, 0]])
# Exact, non-unique solution.
B = Matrix([3, 0])
solution = A.pinv_solve(B)
w1 = solution.atoms(Symbol).pop()
assert w1.name == 'w1_0'
assert solution == Matrix([3, w1])
assert A * A.pinv() * B == B
# Least squares, non-unique solution.
B = Matrix([3, 1])
solution = A.pinv_solve(B)
w1 = solution.atoms(Symbol).pop()
assert w1.name == 'w1_0'
assert solution == Matrix([3, w1])
assert A * A.pinv() * B != B
@XFAIL
def test_pinv_rank_deficient_when_diagonalization_fails():
# Test the four properties of the pseudoinverse for matrices when
# diagonalization of A.H*A fails.
As = [Matrix([
[61, 89, 55, 20, 71, 0],
[62, 96, 85, 85, 16, 0],
[69, 56, 17, 4, 54, 0],
[10, 54, 91, 41, 71, 0],
[ 7, 30, 10, 48, 90, 0],
[0,0,0,0,0,0]])]
for A in As:
A_pinv = A.pinv(method="ED")
AAp = A * A_pinv
ApA = A_pinv * A
assert simplify(AAp * A) == A
assert simplify(ApA * A_pinv) == A_pinv
assert AAp.H == AAp
assert ApA.H == ApA
def test_pinv_succeeds_with_rank_decomposition_method():
# Test rank decomposition method of pseudoinverse succeeding
As = [Matrix([
[61, 89, 55, 20, 71, 0],
[62, 96, 85, 85, 16, 0],
[69, 56, 17, 4, 54, 0],
[10, 54, 91, 41, 71, 0],
[ 7, 30, 10, 48, 90, 0],
[0,0,0,0,0,0]])]
for A in As:
A_pinv = A.pinv(method="RD")
AAp = A * A_pinv
ApA = A_pinv * A
assert simplify(AAp * A) == A
assert simplify(ApA * A_pinv) == A_pinv
assert AAp.H == AAp
assert ApA.H == ApA
def test_gauss_jordan_solve():
# Square, full rank, unique solution
A = Matrix([[1, 2, 3], [4, 5, 6], [7, 8, 10]])
b = Matrix([3, 6, 9])
sol, params = A.gauss_jordan_solve(b)
assert sol == Matrix([[-1], [2], [0]])
assert params == Matrix(0, 1, [])
# Square, full rank, unique solution, B has more columns than rows
A = eye(3)
B = Matrix([[1, 2, 3, 4], [5, 6, 7, 8], [9, 10, 11, 12]])
sol, params = A.gauss_jordan_solve(B)
assert sol == B
assert params == Matrix(0, 4, [])
# Square, reduced rank, parametrized solution
A = Matrix([[1, 2, 3], [4, 5, 6], [7, 8, 9]])
b = Matrix([3, 6, 9])
sol, params, freevar = A.gauss_jordan_solve(b, freevar=True)
w = {}
for s in sol.atoms(Symbol):
# Extract dummy symbols used in the solution.
w[s.name] = s
assert sol == Matrix([[w['tau0'] - 1], [-2*w['tau0'] + 2], [w['tau0']]])
assert params == Matrix([[w['tau0']]])
assert freevar == [2]
# Square, reduced rank, parametrized solution, B has two columns
A = Matrix([[1, 2, 3], [4, 5, 6], [7, 8, 9]])
B = Matrix([[3, 4], [6, 8], [9, 12]])
sol, params, freevar = A.gauss_jordan_solve(B, freevar=True)
w = {}
for s in sol.atoms(Symbol):
# Extract dummy symbols used in the solution.
w[s.name] = s
assert sol == Matrix([[w['tau0'] - 1, w['tau1'] - S(4)/3],
[-2*w['tau0'] + 2, -2*w['tau1'] + S(8)/3],
[w['tau0'], w['tau1']],])
assert params == Matrix([[w['tau0'], w['tau1']]])
assert freevar == [2]
# Square, reduced rank, parametrized solution
A = Matrix([[1, 2, 3], [2, 4, 6], [3, 6, 9]])
b = Matrix([0, 0, 0])
sol, params = A.gauss_jordan_solve(b)
w = {}
for s in sol.atoms(Symbol):
w[s.name] = s
assert sol == Matrix([[-2*w['tau0'] - 3*w['tau1']],
[w['tau0']], [w['tau1']]])
assert params == Matrix([[w['tau0']], [w['tau1']]])
# Square, reduced rank, parametrized solution
A = Matrix([[0, 0, 0], [0, 0, 0], [0, 0, 0]])
b = Matrix([0, 0, 0])
sol, params = A.gauss_jordan_solve(b)
w = {}
for s in sol.atoms(Symbol):
w[s.name] = s
assert sol == Matrix([[w['tau0']], [w['tau1']], [w['tau2']]])
assert params == Matrix([[w['tau0']], [w['tau1']], [w['tau2']]])
# Square, reduced rank, no solution
A = Matrix([[1, 2, 3], [2, 4, 6], [3, 6, 9]])
b = Matrix([0, 0, 1])
raises(ValueError, lambda: A.gauss_jordan_solve(b))
# Rectangular, tall, full rank, unique solution
A = Matrix([[1, 5, 3], [2, 1, 6], [1, 7, 9], [1, 4, 3]])
b = Matrix([0, 0, 1, 0])
sol, params = A.gauss_jordan_solve(b)
assert sol == Matrix([[-S(1)/2], [0], [S(1)/6]])
assert params == Matrix(0, 1, [])
# Rectangular, tall, full rank, unique solution, B has less columns than rows
A = Matrix([[1, 5, 3], [2, 1, 6], [1, 7, 9], [1, 4, 3]])
B = Matrix([[0,0], [0, 0], [1, 2], [0, 0]])
sol, params = A.gauss_jordan_solve(B)
assert sol == Matrix([[-S(1)/2, -S(2)/2], [0, 0], [S(1)/6, S(2)/6]])
assert params == Matrix(0, 2, [])
# Rectangular, tall, full rank, no solution
A = Matrix([[1, 5, 3], [2, 1, 6], [1, 7, 9], [1, 4, 3]])
b = Matrix([0, 0, 0, 1])
raises(ValueError, lambda: A.gauss_jordan_solve(b))
# Rectangular, tall, full rank, no solution, B has two columns (2nd has no solution)
A = Matrix([[1, 5, 3], [2, 1, 6], [1, 7, 9], [1, 4, 3]])
B = Matrix([[0,0], [0, 0], [1, 0], [0, 1]])
raises(ValueError, lambda: A.gauss_jordan_solve(B))
# Rectangular, tall, full rank, no solution, B has two columns (1st has no solution)
A = Matrix([[1, 5, 3], [2, 1, 6], [1, 7, 9], [1, 4, 3]])
B = Matrix([[0,0], [0, 0], [0, 1], [1, 0]])
raises(ValueError, lambda: A.gauss_jordan_solve(B))
# Rectangular, tall, reduced rank, parametrized solution
A = Matrix([[1, 5, 3], [2, 10, 6], [3, 15, 9], [1, 4, 3]])
b = Matrix([0, 0, 0, 1])
sol, params = A.gauss_jordan_solve(b)
w = {}
for s in sol.atoms(Symbol):
w[s.name] = s
assert sol == Matrix([[-3*w['tau0'] + 5], [-1], [w['tau0']]])
assert params == Matrix([[w['tau0']]])
# Rectangular, tall, reduced rank, no solution
A = Matrix([[1, 5, 3], [2, 10, 6], [3, 15, 9], [1, 4, 3]])
b = Matrix([0, 0, 1, 1])
raises(ValueError, lambda: A.gauss_jordan_solve(b))
# Rectangular, wide, full rank, parametrized solution
A = Matrix([[1, 2, 3, 4], [5, 6, 7, 8], [9, 10, 1, 12]])
b = Matrix([1, 1, 1])
sol, params = A.gauss_jordan_solve(b)
w = {}
for s in sol.atoms(Symbol):
w[s.name] = s
assert sol == Matrix([[2*w['tau0'] - 1], [-3*w['tau0'] + 1], [0],
[w['tau0']]])
assert params == Matrix([[w['tau0']]])
# Rectangular, wide, reduced rank, parametrized solution
A = Matrix([[1, 2, 3, 4], [5, 6, 7, 8], [2, 4, 6, 8]])
b = Matrix([0, 1, 0])
sol, params = A.gauss_jordan_solve(b)
w = {}
for s in sol.atoms(Symbol):
w[s.name] = s
assert sol == Matrix([[w['tau0'] + 2*w['tau1'] + 1/S(2)],
[-2*w['tau0'] - 3*w['tau1'] - 1/S(4)],
[w['tau0']], [w['tau1']]])
assert params == Matrix([[w['tau0']], [w['tau1']]])
# watch out for clashing symbols
x0, x1, x2, _x0 = symbols('_tau0 _tau1 _tau2 tau1')
M = Matrix([[0, 1, 0, 0, 0, 0], [0, 0, 0, 1, 0, _x0]])
A = M[:, :-1]
b = M[:, -1:]
sol, params = A.gauss_jordan_solve(b)
assert params == Matrix(3, 1, [x0, x1, x2])
assert sol == Matrix(5, 1, [x1, 0, x0, _x0, x2])
# Rectangular, wide, reduced rank, no solution
A = Matrix([[1, 2, 3, 4], [5, 6, 7, 8], [2, 4, 6, 8]])
b = Matrix([1, 1, 1])
raises(ValueError, lambda: A.gauss_jordan_solve(b))
def test_solve():
A = Matrix([[1,2], [2,4]])
b = Matrix([[3], [4]])
raises(ValueError, lambda: A.solve(b)) #no solution
b = Matrix([[ 4], [8]])
raises(ValueError, lambda: A.solve(b)) #infinite solution
def test_issue_7201():
assert ones(0, 1) + ones(0, 1) == Matrix(0, 1, [])
assert ones(1, 0) + ones(1, 0) == Matrix(1, 0, [])
def test_free_symbols():
for M in ImmutableMatrix, ImmutableSparseMatrix, Matrix, SparseMatrix:
assert M([[x], [0]]).free_symbols == {x}
def test_from_ndarray():
"""See issue 7465."""
try:
from numpy import array
except ImportError:
skip('NumPy must be available to test creating matrices from ndarrays')
assert Matrix(array([1, 2, 3])) == Matrix([1, 2, 3])
assert Matrix(array([[1, 2, 3]])) == Matrix([[1, 2, 3]])
assert Matrix(array([[1, 2, 3], [4, 5, 6]])) == \
Matrix([[1, 2, 3], [4, 5, 6]])
assert Matrix(array([x, y, z])) == Matrix([x, y, z])
raises(NotImplementedError, lambda: Matrix(array([[
[1, 2], [3, 4]], [[5, 6], [7, 8]]])))
def test_hermitian():
a = Matrix([[1, I], [-I, 1]])
assert a.is_hermitian
a[0, 0] = 2*I
assert a.is_hermitian is False
a[0, 0] = x
assert a.is_hermitian is None
a[0, 1] = a[1, 0]*I
assert a.is_hermitian is False
def test_doit():
a = Matrix([[Add(x,x, evaluate=False)]])
assert a[0] != 2*x
assert a.doit() == Matrix([[2*x]])
def test_issue_9457_9467_9876():
# for row_del(index)
M = Matrix([[1, 2, 3], [2, 3, 4], [3, 4, 5]])
M.row_del(1)
assert M == Matrix([[1, 2, 3], [3, 4, 5]])
N = Matrix([[1, 2, 3], [2, 3, 4], [3, 4, 5]])
N.row_del(-2)
assert N == Matrix([[1, 2, 3], [3, 4, 5]])
O = Matrix([[1, 2, 3], [5, 6, 7], [9, 10, 11]])
O.row_del(-1)
assert O == Matrix([[1, 2, 3], [5, 6, 7]])
P = Matrix([[1, 2, 3], [2, 3, 4], [3, 4, 5]])
raises(IndexError, lambda: P.row_del(10))
Q = Matrix([[1, 2, 3], [2, 3, 4], [3, 4, 5]])
raises(IndexError, lambda: Q.row_del(-10))
# for col_del(index)
M = Matrix([[1, 2, 3], [2, 3, 4], [3, 4, 5]])
M.col_del(1)
assert M == Matrix([[1, 3], [2, 4], [3, 5]])
N = Matrix([[1, 2, 3], [2, 3, 4], [3, 4, 5]])
N.col_del(-2)
assert N == Matrix([[1, 3], [2, 4], [3, 5]])
P = Matrix([[1, 2, 3], [2, 3, 4], [3, 4, 5]])
raises(IndexError, lambda: P.col_del(10))
Q = Matrix([[1, 2, 3], [2, 3, 4], [3, 4, 5]])
raises(IndexError, lambda: Q.col_del(-10))
def test_issue_9422():
x, y = symbols('x y', commutative=False)
a, b = symbols('a b')
M = eye(2)
M1 = Matrix(2, 2, [x, y, y, z])
assert y*x*M != x*y*M
assert b*a*M == a*b*M
assert x*M1 != M1*x
assert a*M1 == M1*a
assert y*x*M == Matrix([[y*x, 0], [0, y*x]])
def test_issue_10770():
M = Matrix([])
a = ['col_insert', 'row_join'], Matrix([9, 6, 3])
b = ['row_insert', 'col_join'], a[1].T
c = ['row_insert', 'col_insert'], Matrix([[1, 2], [3, 4]])
for ops, m in (a, b, c):
for op in ops:
f = getattr(M, op)
new = f(m) if 'join' in op else f(42, m)
assert new == m and id(new) != id(m)
def test_issue_10658():
A = Matrix([[1, 2, 3], [4, 5, 6], [7, 8, 9]])
assert A.extract([0, 1, 2], [True, True, False]) == \
Matrix([[1, 2], [4, 5], [7, 8]])
assert A.extract([0, 1, 2], [True, False, False]) == Matrix([[1], [4], [7]])
assert A.extract([True, False, False], [0, 1, 2]) == Matrix([[1, 2, 3]])
assert A.extract([True, False, True], [0, 1, 2]) == \
Matrix([[1, 2, 3], [7, 8, 9]])
assert A.extract([0, 1, 2], [False, False, False]) == Matrix(3, 0, [])
assert A.extract([False, False, False], [0, 1, 2]) == Matrix(0, 3, [])
assert A.extract([True, False, True], [False, True, False]) == \
Matrix([[2], [8]])
def test_opportunistic_simplification():
# this test relates to issue #10718, #9480, #11434
# issue #9480
m = Matrix([[-5 + 5*sqrt(2), -5], [-5*sqrt(2)/2 + 5, -5*sqrt(2)/2]])
assert m.rank() == 1
# issue #10781
m = Matrix([[3+3*sqrt(3)*I, -9],[4,-3+3*sqrt(3)*I]])
assert simplify(m.rref()[0] - Matrix([[1, -9/(3 + 3*sqrt(3)*I)], [0, 0]])) == zeros(2, 2)
# issue #11434
ax,ay,bx,by,cx,cy,dx,dy,ex,ey,t0,t1 = symbols('a_x a_y b_x b_y c_x c_y d_x d_y e_x e_y t_0 t_1')
m = Matrix([[ax,ay,ax*t0,ay*t0,0],[bx,by,bx*t0,by*t0,0],[cx,cy,cx*t0,cy*t0,1],[dx,dy,dx*t0,dy*t0,1],[ex,ey,2*ex*t1-ex*t0,2*ey*t1-ey*t0,0]])
assert m.rank() == 4
def test_partial_pivoting():
# example from https://en.wikipedia.org/wiki/Pivot_element
# partial pivoting with back substitution gives a perfect result
# naive pivoting give an error ~1e-13, so anything better than
# 1e-15 is good
mm=Matrix([[0.003 ,59.14, 59.17],[ 5.291, -6.13,46.78]])
assert (mm.rref()[0] - Matrix([[1.0, 0, 10.0], [ 0, 1.0, 1.0]])).norm() < 1e-15
# issue #11549
m_mixed = Matrix([[6e-17, 1.0, 4],[ -1.0, 0, 8],[ 0, 0, 1]])
m_float = Matrix([[6e-17, 1.0, 4.],[ -1.0, 0., 8.],[ 0., 0., 1.]])
m_inv = Matrix([[ 0, -1.0, 8.0],[1.0, 6.0e-17, -4.0],[ 0, 0, 1]])
# this example is numerically unstable and involves a matrix with a norm >= 8,
# this comparing the difference of the results with 1e-15 is numerically sound.
assert (m_mixed.inv() - m_inv).norm() < 1e-15
assert (m_float.inv() - m_inv).norm() < 1e-15
def test_iszero_substitution():
""" When doing numerical computations, all elements that pass
the iszerofunc test should be set to numerically zero if they
aren't already. """
# Matrix from issue #9060
m = Matrix([[0.9, -0.1, -0.2, 0],[-0.8, 0.9, -0.4, 0],[-0.1, -0.8, 0.6, 0]])
m_rref = m.rref(iszerofunc=lambda x: abs(x)<6e-15)[0]
m_correct = Matrix([[1.0, 0, -0.301369863013699, 0],[ 0, 1.0, -0.712328767123288, 0],[ 0, 0, 0, 0]])
m_diff = m_rref - m_correct
assert m_diff.norm() < 1e-15
# if a zero-substitution wasn't made, this entry will be -1.11022302462516e-16
assert m_rref[2,2] == 0
def test_rank_decomposition():
a = Matrix(0, 0, [])
c, f = a.rank_decomposition()
assert f.is_echelon
assert c.cols == f.rows == a.rank()
assert c * f == a
a = Matrix(1, 1, [5])
c, f = a.rank_decomposition()
assert f.is_echelon
assert c.cols == f.rows == a.rank()
assert c * f == a
a = Matrix(3, 3, [1, 2, 3, 1, 2, 3, 1, 2, 3])
c, f = a.rank_decomposition()
assert f.is_echelon
assert c.cols == f.rows == a.rank()
assert c * f == a
a = Matrix([
[0, 0, 1, 2, 2, -5, 3],
[-1, 5, 2, 2, 1, -7, 5],
[0, 0, -2, -3, -3, 8, -5],
[-1, 5, 0, -1, -2, 1, 0]])
c, f = a.rank_decomposition()
assert f.is_echelon
assert c.cols == f.rows == a.rank()
assert c * f == a
def test_issue_11238():
from sympy import Point
xx = 8*tan(13*pi/45)/(tan(13*pi/45) + sqrt(3))
yy = (-8*sqrt(3)*tan(13*pi/45)**2 + 24*tan(13*pi/45))/(-3 + tan(13*pi/45)**2)
p1 = Point(0, 0)
p2 = Point(1, -sqrt(3))
p0 = Point(xx,yy)
m1 = Matrix([p1 - simplify(p0), p2 - simplify(p0)])
m2 = Matrix([p1 - p0, p2 - p0])
m3 = Matrix([simplify(p1 - p0), simplify(p2 - p0)])
# This system has expressions which are zero and
# cannot be easily proved to be such, so without
# numerical testing, these assertions will fail.
Z = lambda x: abs(x.n()) < 1e-20
assert m1.rank(simplify=True, iszerofunc=Z) == 1
assert m2.rank(simplify=True, iszerofunc=Z) == 1
assert m3.rank(simplify=True, iszerofunc=Z) == 1
def test_as_real_imag():
m1 = Matrix(2,2,[1,2,3,4])
m2 = m1*S.ImaginaryUnit
m3 = m1 + m2
for kls in classes:
a,b = kls(m3).as_real_imag()
assert list(a) == list(m1)
assert list(b) == list(m1)
def test_deprecated():
# Maintain tests for deprecated functions. We must capture
# the deprecation warnings. When the deprecated functionality is
# removed, the corresponding tests should be removed.
m = Matrix(3, 3, [0, 1, 0, -4, 4, 0, -2, 1, 2])
P, Jcells = m.jordan_cells()
assert Jcells[1] == Matrix(1, 1, [2])
assert Jcells[0] == Matrix(2, 2, [2, 1, 0, 2])
with warns_deprecated_sympy():
assert Matrix([[1,2],[3,4]]).dot(Matrix([[1,3],[4,5]])) == [10, 19, 14, 28]
def test_issue_14489():
from sympy import Mod
A = Matrix([-1, 1, 2])
B = Matrix([10, 20, -15])
assert Mod(A, 3) == Matrix([2, 1, 2])
assert Mod(B, 4) == Matrix([2, 0, 1])
def test_issue_14517():
M = Matrix([
[ 0, 10*I, 10*I, 0],
[10*I, 0, 0, 10*I],
[10*I, 0, 5 + 2*I, 10*I],
[ 0, 10*I, 10*I, 5 + 2*I]])
ev = M.eigenvals()
# test one random eigenvalue, the computation is a little slow
test_ev = random.choice(list(ev.keys()))
assert (M - test_ev*eye(4)).det() == 0
def test_issue_14943():
# Test that __array__ accepts the optional dtype argument
try:
from numpy import array
except ImportError:
skip('NumPy must be available to test creating matrices from ndarrays')
M = Matrix([[1,2], [3,4]])
assert array(M, dtype=float).dtype.name == 'float64'
def test_issue_8240():
# Eigenvalues of large triangular matrices
n = 200
diagonal_variables = [Symbol('x%s' % i) for i in range(n)]
M = [[0 for i in range(n)] for j in range(n)]
for i in range(n):
M[i][i] = diagonal_variables[i]
M = Matrix(M)
eigenvals = M.eigenvals()
assert len(eigenvals) == n
for i in range(n):
assert eigenvals[diagonal_variables[i]] == 1
eigenvals = M.eigenvals(multiple=True)
assert set(eigenvals) == set(diagonal_variables)
# with multiplicity
M = Matrix([[x, 0, 0], [1, y, 0], [2, 3, x]])
eigenvals = M.eigenvals()
assert eigenvals == {x: 2, y: 1}
eigenvals = M.eigenvals(multiple=True)
assert len(eigenvals) == 3
assert eigenvals.count(x) == 2
assert eigenvals.count(y) == 1
def test_legacy_det():
# Minimal support for legacy keys for 'method' in det()
# Partially copied from test_determinant()
M = Matrix(( ( 3, -2, 0, 5),
(-2, 1, -2, 2),
( 0, -2, 5, 0),
( 5, 0, 3, 4) ))
assert M.det(method="bareis") == -289
assert M.det(method="det_lu") == -289
assert M.det(method="det_LU") == -289
M = Matrix(( (3, 2, 0, 0, 0),
(0, 3, 2, 0, 0),
(0, 0, 3, 2, 0),
(0, 0, 0, 3, 2),
(2, 0, 0, 0, 3) ))
assert M.det(method="bareis") == 275
assert M.det(method="det_lu") == 275
assert M.det(method="Bareis") == 275
M = Matrix(( (1, 0, 1, 2, 12),
(2, 0, 1, 1, 4),
(2, 1, 1, -1, 3),
(3, 2, -1, 1, 8),
(1, 1, 1, 0, 6) ))
assert M.det(method="bareis") == -55
assert M.det(method="det_lu") == -55
assert M.det(method="BAREISS") == -55
M = Matrix(( (-5, 2, 3, 4, 5),
( 1, -4, 3, 4, 5),
( 1, 2, -3, 4, 5),
( 1, 2, 3, -2, 5),
( 1, 2, 3, 4, -1) ))
assert M.det(method="bareis") == 11664
assert M.det(method="det_lu") == 11664
assert M.det(method="BERKOWITZ") == 11664
M = Matrix(( ( 2, 7, -1, 3, 2),
( 0, 0, 1, 0, 1),
(-2, 0, 7, 0, 2),
(-3, -2, 4, 5, 3),
( 1, 0, 0, 0, 1) ))
assert M.det(method="bareis") == 123
assert M.det(method="det_lu") == 123
assert M.det(method="LU") == 123
def test_case_6913():
m = MatrixSymbol('m', 1, 1)
a = Symbol("a")
a = m[0, 0]>0
assert str(a) == 'm[0, 0] > 0'
def test_issue_15872():
A = Matrix([[1, 1, 1, 0], [-2, -1, 0, -1], [0, 0, -1, -1], [0, 0, 2, 1]])
B = A - Matrix.eye(4) * I
assert B.rank() == 3
assert (B**2).rank() == 2
assert (B**3).rank() == 2
def test_issue_11948():
A = MatrixSymbol('A', 3, 3)
a = Wild('a')
assert A.match(a) == {a: A}
def test_gramschmidt_conjugate_dot():
vecs = [Matrix([1, I]), Matrix([1, -I])]
assert Matrix.orthogonalize(*vecs) == \
[Matrix([[1], [I]]), Matrix([[1], [-I]])]
mat = Matrix([[1, I], [1, -I]])
Q, R = mat.QRdecomposition()
assert Q * Q.H == Matrix.eye(2)
|
6b279d487f00da935d6dd9f7f1fcdbff2a6bab13e0291b4f1d187c8fc87721ae | from sympy.matrices.expressions import MatrixExpr
from sympy import MatrixBase, Dummy, Lambda, Function, FunctionClass
class ElementwiseApplyFunction(MatrixExpr):
r"""
Apply function to a matrix elementwise without evaluating.
Examples
========
It can be created by calling ``.applyfunc(<function>)`` on a matrix
expression:
>>> from sympy.matrices.expressions import MatrixSymbol
>>> from sympy.matrices.expressions.applyfunc import ElementwiseApplyFunction
>>> from sympy import exp
>>> X = MatrixSymbol("X", 3, 3)
>>> X.applyfunc(exp)
exp(X...)
Otherwise using the class constructor:
>>> from sympy import eye
>>> expr = ElementwiseApplyFunction(exp, eye(3))
>>> expr
exp(Matrix([
[1, 0, 0],
[0, 1, 0],
[0, 0, 1]])...)
>>> expr.doit()
Matrix([
[E, 1, 1],
[1, E, 1],
[1, 1, E]])
Notice the difference with the real mathematical functions:
>>> exp(eye(3))
Matrix([
[E, 0, 0],
[0, E, 0],
[0, 0, E]])
"""
def __new__(cls, function, expr):
obj = MatrixExpr.__new__(cls, expr)
if not isinstance(function, FunctionClass):
d = Dummy("d")
function = Lambda(d, function(d))
obj._function = function
obj._expr = expr
return obj
def _hashable_content(self):
return (self.function, self.expr)
@property
def function(self):
return self._function
@property
def expr(self):
return self._expr
@property
def shape(self):
return self.expr.shape
@property
def func(self):
# This strange construction is required by the assumptions:
# (.func needs to be a class)
class _(ElementwiseApplyFunction):
def __new__(cls, expr):
return ElementwiseApplyFunction(self.function, expr)
return _
def doit(self, **kwargs):
deep = kwargs.get("deep", True)
expr = self.expr
if deep:
expr = expr.doit(**kwargs)
function = self.function
if isinstance(function, Lambda) and function.is_identity:
# This is a Lambda containing the identity function.
return expr
if isinstance(expr, MatrixBase):
return expr.applyfunc(self.function)
elif isinstance(expr, ElementwiseApplyFunction):
return ElementwiseApplyFunction(
lambda x: self.function(expr.function(x)),
expr.expr
).doit()
else:
return self
def _entry(self, i, j, **kwargs):
return self.function(self.expr._entry(i, j, **kwargs))
def _get_function_fdiff(self):
d = Dummy("d")
function = self.function(d)
fdiff = function.diff(d)
if isinstance(fdiff, Function):
fdiff = type(fdiff)
else:
fdiff = Lambda(d, fdiff)
return fdiff
def _eval_derivative(self, x):
from sympy import hadamard_product
dexpr = self.expr.diff(x)
fdiff = self._get_function_fdiff()
return hadamard_product(
dexpr,
ElementwiseApplyFunction(fdiff, self.expr)
)
def _eval_derivative_matrix_lines(self, x):
from sympy import Identity
from sympy.codegen.array_utils import CodegenArrayContraction, CodegenArrayTensorProduct, CodegenArrayDiagonal
from sympy.core.expr import ExprBuilder
fdiff = self._get_function_fdiff()
lr = self.expr._eval_derivative_matrix_lines(x)
ewdiff = ElementwiseApplyFunction(fdiff, self.expr)
if 1 in x.shape:
# Vector:
iscolumn = self.shape[1] == 1
for i in lr:
if iscolumn:
ptr1 = i.first_pointer
ptr2 = Identity(self.shape[1])
else:
ptr1 = Identity(self.shape[0])
ptr2 = i.second_pointer
subexpr = ExprBuilder(
CodegenArrayDiagonal,
[
ExprBuilder(
CodegenArrayTensorProduct,
[
ewdiff,
ptr1,
ptr2,
]
),
(0, 2) if iscolumn else (1, 4)
],
validator=CodegenArrayDiagonal._validate
)
i._lines = [subexpr]
i._first_pointer_parent = subexpr.args[0].args
i._first_pointer_index = 1
i._second_pointer_parent = subexpr.args[0].args
i._second_pointer_index = 2
else:
# Matrix case:
for i in lr:
ptr1 = i.first_pointer
ptr2 = i.second_pointer
newptr1 = Identity(ptr1.shape[1])
newptr2 = Identity(ptr2.shape[1])
subexpr = ExprBuilder(
CodegenArrayContraction,
[
ExprBuilder(
CodegenArrayTensorProduct,
[ptr1, newptr1, ewdiff, ptr2, newptr2]
),
(1, 2, 4),
(5, 7, 8),
],
validator=CodegenArrayContraction._validate
)
i._first_pointer_parent = subexpr.args[0].args
i._first_pointer_index = 1
i._second_pointer_parent = subexpr.args[0].args
i._second_pointer_index = 4
i._lines = [subexpr]
return lr
|
078e3f8e2820d0cfa2d54bcbc3f2696366fd2c608536f1bfb90ee433be64f179 | from __future__ import print_function, division
from sympy import Basic
from sympy.functions import adjoint, conjugate
from sympy.matrices.expressions.matexpr import MatrixExpr
class Transpose(MatrixExpr):
"""
The transpose of a matrix expression.
This is a symbolic object that simply stores its argument without
evaluating it. To actually compute the transpose, use the ``transpose()``
function, or the ``.T`` attribute of matrices.
Examples
========
>>> from sympy.matrices import MatrixSymbol, Transpose
>>> from sympy.functions import transpose
>>> A = MatrixSymbol('A', 3, 5)
>>> B = MatrixSymbol('B', 5, 3)
>>> Transpose(A)
A.T
>>> A.T == transpose(A) == Transpose(A)
True
>>> Transpose(A*B)
(A*B).T
>>> transpose(A*B)
B.T*A.T
"""
is_Transpose = True
def doit(self, **hints):
arg = self.arg
if hints.get('deep', True) and isinstance(arg, Basic):
arg = arg.doit(**hints)
_eval_transpose = getattr(arg, '_eval_transpose', None)
if _eval_transpose is not None:
result = _eval_transpose()
return result if result is not None else Transpose(arg)
else:
return Transpose(arg)
@property
def arg(self):
return self.args[0]
@property
def shape(self):
return self.arg.shape[::-1]
def _entry(self, i, j, expand=False, **kwargs):
return self.arg._entry(j, i, expand=expand, **kwargs)
def _eval_adjoint(self):
return conjugate(self.arg)
def _eval_conjugate(self):
return adjoint(self.arg)
def _eval_transpose(self):
return self.arg
def _eval_trace(self):
from .trace import Trace
return Trace(self.arg) # Trace(X.T) => Trace(X)
def _eval_determinant(self):
from sympy.matrices.expressions.determinant import det
return det(self.arg)
def _eval_derivative(self, x):
# x is a scalar:
return self.arg._eval_derivative(x)
def _eval_derivative_matrix_lines(self, x):
lines = self.args[0]._eval_derivative_matrix_lines(x)
return [i.transpose() for i in lines]
def transpose(expr):
"""Matrix transpose"""
return Transpose(expr).doit(deep=False)
from sympy.assumptions.ask import ask, Q
from sympy.assumptions.refine import handlers_dict
def refine_Transpose(expr, assumptions):
"""
>>> from sympy import MatrixSymbol, Q, assuming, refine
>>> X = MatrixSymbol('X', 2, 2)
>>> X.T
X.T
>>> with assuming(Q.symmetric(X)):
... print(refine(X.T))
X
"""
if ask(Q.symmetric(expr), assumptions):
return expr.arg
return expr
handlers_dict['Transpose'] = refine_Transpose
|
f0126c7b97aee9b004423237111d980827f6726480b0f98dd9262017fdf0565e | from __future__ import print_function, division
from .matexpr import MatrixExpr, ShapeError, Identity, ZeroMatrix
from sympy.core import S
from sympy.core.compatibility import range
from sympy.core.sympify import _sympify
from sympy.matrices import MatrixBase
class MatPow(MatrixExpr):
def __new__(cls, base, exp):
base = _sympify(base)
if not base.is_Matrix:
raise TypeError("Function parameter should be a matrix")
exp = _sympify(exp)
return super(MatPow, cls).__new__(cls, base, exp)
@property
def base(self):
return self.args[0]
@property
def exp(self):
return self.args[1]
@property
def shape(self):
return self.base.shape
def _entry(self, i, j, **kwargs):
from sympy.matrices.expressions import MatMul
A = self.doit()
if isinstance(A, MatPow):
# We still have a MatPow, make an explicit MatMul out of it.
if not A.base.is_square:
raise ShapeError("Power of non-square matrix %s" % A.base)
elif A.exp.is_Integer and A.exp.is_positive:
A = MatMul(*[A.base for k in range(A.exp)])
#elif A.exp.is_Integer and self.exp.is_negative:
# Note: possible future improvement: in principle we can take
# positive powers of the inverse, but carefully avoid recursion,
# perhaps by adding `_entry` to Inverse (as it is our subclass).
# T = A.base.as_explicit().inverse()
# A = MatMul(*[T for k in range(-A.exp)])
else:
# Leave the expression unevaluated:
from sympy.matrices.expressions.matexpr import MatrixElement
return MatrixElement(self, i, j)
return A._entry(i, j)
def doit(self, **kwargs):
from sympy.matrices.expressions import Inverse
deep = kwargs.get('deep', True)
if deep:
args = [arg.doit(**kwargs) for arg in self.args]
else:
args = self.args
base, exp = args
# combine all powers, e.g. (A**2)**3 = A**6
while isinstance(base, MatPow):
exp = exp*base.args[1]
base = base.args[0]
if exp.is_zero and base.is_square:
if isinstance(base, MatrixBase):
return base.func(Identity(base.shape[0]))
return Identity(base.shape[0])
elif isinstance(base, ZeroMatrix) and exp.is_negative:
raise ValueError("Matrix determinant is 0, not invertible.")
elif isinstance(base, (Identity, ZeroMatrix)):
return base
elif isinstance(base, MatrixBase):
if exp is S.One:
return base
return base**exp
# Note: just evaluate cases we know, return unevaluated on others.
# E.g., MatrixSymbol('x', n, m) to power 0 is not an error.
elif exp is S(-1) and base.is_square:
return Inverse(base).doit(**kwargs)
elif exp is S.One:
return base
return MatPow(base, exp)
def _eval_transpose(self):
base, exp = self.args
return MatPow(base.T, exp)
def _eval_derivative(self, x):
from sympy import Pow
return Pow._eval_derivative(self, x)
def _eval_derivative_matrix_lines(self, x):
from sympy.core.expr import ExprBuilder
from sympy.codegen.array_utils import CodegenArrayContraction, CodegenArrayTensorProduct
from .matmul import MatMul
from .inverse import Inverse
exp = self.exp
if self.base.shape == (1, 1) and not exp.has(x):
lr = self.base._eval_derivative_matrix_lines(x)
for i in lr:
subexpr = ExprBuilder(
CodegenArrayContraction,
[
ExprBuilder(
CodegenArrayTensorProduct,
[
Identity(1),
i._lines[0],
exp*self.base**(exp-1),
i._lines[1],
Identity(1),
]
),
(0, 3, 4), (5, 7, 8)
],
validator=CodegenArrayContraction._validate
)
i._first_pointer_parent = subexpr.args[0].args
i._first_pointer_index = 0
i._second_pointer_parent = subexpr.args[0].args
i._second_pointer_index = 4
i._lines = [subexpr]
return lr
if (exp > 0) == True:
newexpr = MatMul.fromiter([self.base for i in range(exp)])
elif (exp == -1) == True:
return Inverse(self.base)._eval_derivative_matrix_lines(x)
elif (exp < 0) == True:
newexpr = MatMul.fromiter([Inverse(self.base) for i in range(-exp)])
elif (exp == 0) == True:
return self.doit()._eval_derivative_matrix_lines(x)
else:
raise NotImplementedError("cannot evaluate %s derived by %s" % (self, x))
return newexpr._eval_derivative_matrix_lines(x)
|
287f03b2176200e89f539d6a7105e1f0171281592a32cf10314ab38aef7261f3 | from __future__ import print_function, division
from functools import wraps, reduce
import collections
from sympy.core import S, Symbol, Tuple, Integer, Basic, Expr, Eq, Mul, Add
from sympy.core.decorators import call_highest_priority
from sympy.core.compatibility import range, SYMPY_INTS, default_sort_key, string_types
from sympy.core.sympify import SympifyError, _sympify
from sympy.functions import conjugate, adjoint
from sympy.functions.special.tensor_functions import KroneckerDelta
from sympy.matrices import ShapeError
from sympy.simplify import simplify
from sympy.utilities.misc import filldedent
def _sympifyit(arg, retval=None):
# This version of _sympifyit sympifies MutableMatrix objects
def deco(func):
@wraps(func)
def __sympifyit_wrapper(a, b):
try:
b = _sympify(b)
return func(a, b)
except SympifyError:
return retval
return __sympifyit_wrapper
return deco
class MatrixExpr(Expr):
"""Superclass for Matrix Expressions
MatrixExprs represent abstract matrices, linear transformations represented
within a particular basis.
Examples
========
>>> from sympy import MatrixSymbol
>>> A = MatrixSymbol('A', 3, 3)
>>> y = MatrixSymbol('y', 3, 1)
>>> x = (A.T*A).I * A * y
See Also
========
MatrixSymbol, MatAdd, MatMul, Transpose, Inverse
"""
# Should not be considered iterable by the
# sympy.core.compatibility.iterable function. Subclass that actually are
# iterable (i.e., explicit matrices) should set this to True.
_iterable = False
_op_priority = 11.0
is_Matrix = True
is_MatrixExpr = True
is_Identity = None
is_Inverse = False
is_Transpose = False
is_ZeroMatrix = False
is_MatAdd = False
is_MatMul = False
is_commutative = False
is_number = False
is_symbol = False
is_scalar = False
def __new__(cls, *args, **kwargs):
args = map(_sympify, args)
return Basic.__new__(cls, *args, **kwargs)
# The following is adapted from the core Expr object
def __neg__(self):
return MatMul(S.NegativeOne, self).doit()
def __abs__(self):
raise NotImplementedError
@_sympifyit('other', NotImplemented)
@call_highest_priority('__radd__')
def __add__(self, other):
return MatAdd(self, other, check=True).doit()
@_sympifyit('other', NotImplemented)
@call_highest_priority('__add__')
def __radd__(self, other):
return MatAdd(other, self, check=True).doit()
@_sympifyit('other', NotImplemented)
@call_highest_priority('__rsub__')
def __sub__(self, other):
return MatAdd(self, -other, check=True).doit()
@_sympifyit('other', NotImplemented)
@call_highest_priority('__sub__')
def __rsub__(self, other):
return MatAdd(other, -self, check=True).doit()
@_sympifyit('other', NotImplemented)
@call_highest_priority('__rmul__')
def __mul__(self, other):
return MatMul(self, other).doit()
@_sympifyit('other', NotImplemented)
@call_highest_priority('__rmul__')
def __matmul__(self, other):
return MatMul(self, other).doit()
@_sympifyit('other', NotImplemented)
@call_highest_priority('__mul__')
def __rmul__(self, other):
return MatMul(other, self).doit()
@_sympifyit('other', NotImplemented)
@call_highest_priority('__mul__')
def __rmatmul__(self, other):
return MatMul(other, self).doit()
@_sympifyit('other', NotImplemented)
@call_highest_priority('__rpow__')
def __pow__(self, other):
if not self.is_square:
raise ShapeError("Power of non-square matrix %s" % self)
elif self.is_Identity:
return self
elif other is S.Zero:
return Identity(self.rows)
elif other is S.One:
return self
return MatPow(self, other).doit(deep=False)
@_sympifyit('other', NotImplemented)
@call_highest_priority('__pow__')
def __rpow__(self, other):
raise NotImplementedError("Matrix Power not defined")
@_sympifyit('other', NotImplemented)
@call_highest_priority('__rdiv__')
def __div__(self, other):
return self * other**S.NegativeOne
@_sympifyit('other', NotImplemented)
@call_highest_priority('__div__')
def __rdiv__(self, other):
raise NotImplementedError()
#return MatMul(other, Pow(self, S.NegativeOne))
__truediv__ = __div__
__rtruediv__ = __rdiv__
@property
def rows(self):
return self.shape[0]
@property
def cols(self):
return self.shape[1]
@property
def is_square(self):
return self.rows == self.cols
def _eval_conjugate(self):
from sympy.matrices.expressions.adjoint import Adjoint
from sympy.matrices.expressions.transpose import Transpose
return Adjoint(Transpose(self))
def as_real_imag(self):
from sympy import I
real = (S(1)/2) * (self + self._eval_conjugate())
im = (self - self._eval_conjugate())/(2*I)
return (real, im)
def _eval_inverse(self):
from sympy.matrices.expressions.inverse import Inverse
return Inverse(self)
def _eval_transpose(self):
return Transpose(self)
def _eval_power(self, exp):
return MatPow(self, exp)
def _eval_simplify(self, **kwargs):
if self.is_Atom:
return self
else:
return self.func(*[simplify(x, **kwargs) for x in self.args])
def _eval_adjoint(self):
from sympy.matrices.expressions.adjoint import Adjoint
return Adjoint(self)
def _eval_derivative_array(self, x):
if isinstance(x, MatrixExpr):
return _matrix_derivative(self, x)
else:
return self._eval_derivative(x)
def _eval_derivative_n_times(self, x, n):
return Basic._eval_derivative_n_times(self, x, n)
def _visit_eval_derivative_scalar(self, x):
# `x` is a scalar:
if x.has(self):
return _matrix_derivative(x, self)
else:
return ZeroMatrix(*self.shape)
def _visit_eval_derivative_array(self, x):
if x.has(self):
return _matrix_derivative(x, self)
else:
from sympy import Derivative
return Derivative(x, self)
def _accept_eval_derivative(self, s):
from sympy import MatrixBase, NDimArray
if isinstance(s, (MatrixBase, NDimArray, MatrixExpr)):
return s._visit_eval_derivative_array(self)
else:
return s._visit_eval_derivative_scalar(self)
@classmethod
def _check_dim(cls, dim):
"""Helper function to check invalid matrix dimensions"""
from sympy.solvers.solvers import check_assumptions
ok = check_assumptions(dim, integer=True, nonnegative=True)
if ok is False:
raise ValueError(
"The dimension specification {} should be "
"a nonnegative integer.".format(dim))
def _entry(self, i, j, **kwargs):
raise NotImplementedError(
"Indexing not implemented for %s" % self.__class__.__name__)
def adjoint(self):
return adjoint(self)
def as_coeff_Mul(self, rational=False):
"""Efficiently extract the coefficient of a product. """
return S.One, self
def conjugate(self):
return conjugate(self)
def transpose(self):
from sympy.matrices.expressions.transpose import transpose
return transpose(self)
T = property(transpose, None, None, 'Matrix transposition.')
def inverse(self):
return self._eval_inverse()
inv = inverse
@property
def I(self):
return self.inverse()
def valid_index(self, i, j):
def is_valid(idx):
return isinstance(idx, (int, Integer, Symbol, Expr))
return (is_valid(i) and is_valid(j) and
(self.rows is None or
(0 <= i) != False and (i < self.rows) != False) and
(0 <= j) != False and (j < self.cols) != False)
def __getitem__(self, key):
if not isinstance(key, tuple) and isinstance(key, slice):
from sympy.matrices.expressions.slice import MatrixSlice
return MatrixSlice(self, key, (0, None, 1))
if isinstance(key, tuple) and len(key) == 2:
i, j = key
if isinstance(i, slice) or isinstance(j, slice):
from sympy.matrices.expressions.slice import MatrixSlice
return MatrixSlice(self, i, j)
i, j = _sympify(i), _sympify(j)
if self.valid_index(i, j) != False:
return self._entry(i, j)
else:
raise IndexError("Invalid indices (%s, %s)" % (i, j))
elif isinstance(key, (SYMPY_INTS, Integer)):
# row-wise decomposition of matrix
rows, cols = self.shape
# allow single indexing if number of columns is known
if not isinstance(cols, Integer):
raise IndexError(filldedent('''
Single indexing is only supported when the number
of columns is known.'''))
key = _sympify(key)
i = key // cols
j = key % cols
if self.valid_index(i, j) != False:
return self._entry(i, j)
else:
raise IndexError("Invalid index %s" % key)
elif isinstance(key, (Symbol, Expr)):
raise IndexError(filldedent('''
Only integers may be used when addressing the matrix
with a single index.'''))
raise IndexError("Invalid index, wanted %s[i,j]" % self)
def as_explicit(self):
"""
Returns a dense Matrix with elements represented explicitly
Returns an object of type ImmutableDenseMatrix.
Examples
========
>>> from sympy import Identity
>>> I = Identity(3)
>>> I
I
>>> I.as_explicit()
Matrix([
[1, 0, 0],
[0, 1, 0],
[0, 0, 1]])
See Also
========
as_mutable: returns mutable Matrix type
"""
from sympy.matrices.immutable import ImmutableDenseMatrix
return ImmutableDenseMatrix([[ self[i, j]
for j in range(self.cols)]
for i in range(self.rows)])
def as_mutable(self):
"""
Returns a dense, mutable matrix with elements represented explicitly
Examples
========
>>> from sympy import Identity
>>> I = Identity(3)
>>> I
I
>>> I.shape
(3, 3)
>>> I.as_mutable()
Matrix([
[1, 0, 0],
[0, 1, 0],
[0, 0, 1]])
See Also
========
as_explicit: returns ImmutableDenseMatrix
"""
return self.as_explicit().as_mutable()
def __array__(self):
from numpy import empty
a = empty(self.shape, dtype=object)
for i in range(self.rows):
for j in range(self.cols):
a[i, j] = self[i, j]
return a
def equals(self, other):
"""
Test elementwise equality between matrices, potentially of different
types
>>> from sympy import Identity, eye
>>> Identity(3).equals(eye(3))
True
"""
return self.as_explicit().equals(other)
def canonicalize(self):
return self
def as_coeff_mmul(self):
return 1, MatMul(self)
@staticmethod
def from_index_summation(expr, first_index=None, last_index=None, dimensions=None):
r"""
Parse expression of matrices with explicitly summed indices into a
matrix expression without indices, if possible.
This transformation expressed in mathematical notation:
`\sum_{j=0}^{N-1} A_{i,j} B_{j,k} \Longrightarrow \mathbf{A}\cdot \mathbf{B}`
Optional parameter ``first_index``: specify which free index to use as
the index starting the expression.
Examples
========
>>> from sympy import MatrixSymbol, MatrixExpr, Sum, Symbol
>>> from sympy.abc import i, j, k, l, N
>>> A = MatrixSymbol("A", N, N)
>>> B = MatrixSymbol("B", N, N)
>>> expr = Sum(A[i, j]*B[j, k], (j, 0, N-1))
>>> MatrixExpr.from_index_summation(expr)
A*B
Transposition is detected:
>>> expr = Sum(A[j, i]*B[j, k], (j, 0, N-1))
>>> MatrixExpr.from_index_summation(expr)
A.T*B
Detect the trace:
>>> expr = Sum(A[i, i], (i, 0, N-1))
>>> MatrixExpr.from_index_summation(expr)
Trace(A)
More complicated expressions:
>>> expr = Sum(A[i, j]*B[k, j]*A[l, k], (j, 0, N-1), (k, 0, N-1))
>>> MatrixExpr.from_index_summation(expr)
A*B.T*A.T
"""
from sympy import Sum, Mul, Add, MatMul, transpose, trace
from sympy.strategies.traverse import bottom_up
def remove_matelement(expr, i1, i2):
def repl_match(pos):
def func(x):
if not isinstance(x, MatrixElement):
return False
if x.args[pos] != i1:
return False
if x.args[3-pos] == 0:
if x.args[0].shape[2-pos] == 1:
return True
else:
return False
return True
return func
expr = expr.replace(repl_match(1),
lambda x: x.args[0])
expr = expr.replace(repl_match(2),
lambda x: transpose(x.args[0]))
# Make sure that all Mul are transformed to MatMul and that they
# are flattened:
rule = bottom_up(lambda x: reduce(lambda a, b: a*b, x.args) if isinstance(x, (Mul, MatMul)) else x)
return rule(expr)
def recurse_expr(expr, index_ranges={}):
if expr.is_Mul:
nonmatargs = []
pos_arg = []
pos_ind = []
dlinks = {}
link_ind = []
counter = 0
args_ind = []
for arg in expr.args:
retvals = recurse_expr(arg, index_ranges)
assert isinstance(retvals, list)
if isinstance(retvals, list):
for i in retvals:
args_ind.append(i)
else:
args_ind.append(retvals)
for arg_symbol, arg_indices in args_ind:
if arg_indices is None:
nonmatargs.append(arg_symbol)
continue
if isinstance(arg_symbol, MatrixElement):
arg_symbol = arg_symbol.args[0]
pos_arg.append(arg_symbol)
pos_ind.append(arg_indices)
link_ind.append([None]*len(arg_indices))
for i, ind in enumerate(arg_indices):
if ind in dlinks:
other_i = dlinks[ind]
link_ind[counter][i] = other_i
link_ind[other_i[0]][other_i[1]] = (counter, i)
dlinks[ind] = (counter, i)
counter += 1
counter2 = 0
lines = {}
while counter2 < len(link_ind):
for i, e in enumerate(link_ind):
if None in e:
line_start_index = (i, e.index(None))
break
cur_ind_pos = line_start_index
cur_line = []
index1 = pos_ind[cur_ind_pos[0]][cur_ind_pos[1]]
while True:
d, r = cur_ind_pos
if pos_arg[d] != 1:
if r % 2 == 1:
cur_line.append(transpose(pos_arg[d]))
else:
cur_line.append(pos_arg[d])
next_ind_pos = link_ind[d][1-r]
counter2 += 1
# Mark as visited, there will be no `None` anymore:
link_ind[d] = (-1, -1)
if next_ind_pos is None:
index2 = pos_ind[d][1-r]
lines[(index1, index2)] = cur_line
break
cur_ind_pos = next_ind_pos
lines = {k: MatMul.fromiter(v) if len(v) != 1 else v[0] for k, v in lines.items()}
return [(Mul.fromiter(nonmatargs), None)] + [
(MatrixElement(a, i, j), (i, j)) for (i, j), a in lines.items()
]
elif expr.is_Add:
res = [recurse_expr(i) for i in expr.args]
d = collections.defaultdict(list)
for res_addend in res:
scalar = 1
for elem, indices in res_addend:
if indices is None:
scalar = elem
continue
indices = tuple(sorted(indices, key=default_sort_key))
d[indices].append(scalar*remove_matelement(elem, *indices))
scalar = 1
return [(MatrixElement(Add.fromiter(v), *k), k) for k, v in d.items()]
elif isinstance(expr, KroneckerDelta):
i1, i2 = expr.args
if dimensions is not None:
identity = Identity(dimensions[0])
else:
identity = S.One
return [(MatrixElement(identity, i1, i2), (i1, i2))]
elif isinstance(expr, MatrixElement):
matrix_symbol, i1, i2 = expr.args
if i1 in index_ranges:
r1, r2 = index_ranges[i1]
if r1 != 0 or matrix_symbol.shape[0] != r2+1:
raise ValueError("index range mismatch: {0} vs. (0, {1})".format(
(r1, r2), matrix_symbol.shape[0]))
if i2 in index_ranges:
r1, r2 = index_ranges[i2]
if r1 != 0 or matrix_symbol.shape[1] != r2+1:
raise ValueError("index range mismatch: {0} vs. (0, {1})".format(
(r1, r2), matrix_symbol.shape[1]))
if (i1 == i2) and (i1 in index_ranges):
return [(trace(matrix_symbol), None)]
return [(MatrixElement(matrix_symbol, i1, i2), (i1, i2))]
elif isinstance(expr, Sum):
return recurse_expr(
expr.args[0],
index_ranges={i[0]: i[1:] for i in expr.args[1:]}
)
else:
return [(expr, None)]
retvals = recurse_expr(expr)
factors, indices = zip(*retvals)
retexpr = Mul.fromiter(factors)
if len(indices) == 0 or list(set(indices)) == [None]:
return retexpr
if first_index is None:
for i in indices:
if i is not None:
ind0 = i
break
return remove_matelement(retexpr, *ind0)
else:
return remove_matelement(retexpr, first_index, last_index)
def applyfunc(self, func):
from .applyfunc import ElementwiseApplyFunction
return ElementwiseApplyFunction(func, self)
def _eval_Eq(self, other):
if not isinstance(other, MatrixExpr):
return False
if self.shape != other.shape:
return False
if (self - other).is_ZeroMatrix:
return True
return Eq(self, other, evaluate=False)
def get_postprocessor(cls):
def _postprocessor(expr):
# To avoid circular imports, we can't have MatMul/MatAdd on the top level
mat_class = {Mul: MatMul, Add: MatAdd}[cls]
nonmatrices = []
matrices = []
for term in expr.args:
if isinstance(term, MatrixExpr):
matrices.append(term)
else:
nonmatrices.append(term)
if not matrices:
return cls._from_args(nonmatrices)
if nonmatrices:
if cls == Mul:
for i in range(len(matrices)):
if not matrices[i].is_MatrixExpr:
# If one of the matrices explicit, absorb the scalar into it
# (doit will combine all explicit matrices into one, so it
# doesn't matter which)
matrices[i] = matrices[i].__mul__(cls._from_args(nonmatrices))
nonmatrices = []
break
else:
# Maintain the ability to create Add(scalar, matrix) without
# raising an exception. That way different algorithms can
# replace matrix expressions with non-commutative symbols to
# manipulate them like non-commutative scalars.
return cls._from_args(nonmatrices + [mat_class(*matrices).doit(deep=False)])
return mat_class(cls._from_args(nonmatrices), *matrices).doit(deep=False)
return _postprocessor
Basic._constructor_postprocessor_mapping[MatrixExpr] = {
"Mul": [get_postprocessor(Mul)],
"Add": [get_postprocessor(Add)],
}
def _matrix_derivative(expr, x):
from sympy import Derivative
lines = expr._eval_derivative_matrix_lines(x)
parts = [i.build() for i in lines]
from sympy.codegen.array_utils import recognize_matrix_expression
parts = [[recognize_matrix_expression(j).doit() for j in i] for i in parts]
def _get_shape(elem):
if isinstance(elem, MatrixExpr):
return elem.shape
return (1, 1)
def get_rank(parts):
return sum([j not in (1, None) for i in parts for j in _get_shape(i)])
ranks = [get_rank(i) for i in parts]
rank = ranks[0]
def contract_one_dims(parts):
if len(parts) == 1:
return parts[0]
else:
p1, p2 = parts[:2]
if p2.is_Matrix:
p2 = p2.T
if p1 == Identity(1):
pbase = p2
elif p2 == Identity(1):
pbase = p1
else:
pbase = p1*p2
if len(parts) == 2:
return pbase
else: # len(parts) > 2
if pbase.is_Matrix:
raise ValueError("")
return pbase*Mul.fromiter(parts[2:])
if rank <= 2:
return Add.fromiter([contract_one_dims(i) for i in parts])
return Derivative(expr, x)
class MatrixElement(Expr):
parent = property(lambda self: self.args[0])
i = property(lambda self: self.args[1])
j = property(lambda self: self.args[2])
_diff_wrt = True
is_symbol = True
is_commutative = True
def __new__(cls, name, n, m):
n, m = map(_sympify, (n, m))
from sympy import MatrixBase
if isinstance(name, (MatrixBase,)):
if n.is_Integer and m.is_Integer:
return name[n, m]
if isinstance(name, string_types):
name = Symbol(name)
name = _sympify(name)
obj = Expr.__new__(cls, name, n, m)
return obj
def doit(self, **kwargs):
deep = kwargs.get('deep', True)
if deep:
args = [arg.doit(**kwargs) for arg in self.args]
else:
args = self.args
return args[0][args[1], args[2]]
@property
def indices(self):
return self.args[1:]
def _eval_derivative(self, v):
from sympy import Sum, symbols, Dummy
if not isinstance(v, MatrixElement):
from sympy import MatrixBase
if isinstance(self.parent, MatrixBase):
return self.parent.diff(v)[self.i, self.j]
return S.Zero
M = self.args[0]
m, n = self.parent.shape
if M == v.args[0]:
return KroneckerDelta(self.args[1], v.args[1], (0, m-1)) * \
KroneckerDelta(self.args[2], v.args[2], (0, n-1))
if isinstance(M, Inverse):
i, j = self.args[1:]
i1, i2 = symbols("z1, z2", cls=Dummy)
Y = M.args[0]
r1, r2 = Y.shape
return -Sum(M[i, i1]*Y[i1, i2].diff(v)*M[i2, j], (i1, 0, r1-1), (i2, 0, r2-1))
if self.has(v.args[0]):
return None
return S.Zero
class MatrixSymbol(MatrixExpr):
"""Symbolic representation of a Matrix object
Creates a SymPy Symbol to represent a Matrix. This matrix has a shape and
can be included in Matrix Expressions
Examples
========
>>> from sympy import MatrixSymbol, Identity
>>> A = MatrixSymbol('A', 3, 4) # A 3 by 4 Matrix
>>> B = MatrixSymbol('B', 4, 3) # A 4 by 3 Matrix
>>> A.shape
(3, 4)
>>> 2*A*B + Identity(3)
I + 2*A*B
"""
is_commutative = False
is_symbol = True
_diff_wrt = True
def __new__(cls, name, n, m):
n, m = _sympify(n), _sympify(m)
cls._check_dim(m)
cls._check_dim(n)
if isinstance(name, string_types):
name = Symbol(name)
obj = Basic.__new__(cls, name, n, m)
return obj
def _hashable_content(self):
return (self.name, self.shape)
@property
def shape(self):
return self.args[1:3]
@property
def name(self):
return self.args[0].name
def _eval_subs(self, old, new):
# only do substitutions in shape
shape = Tuple(*self.shape)._subs(old, new)
return MatrixSymbol(self.args[0], *shape)
def __call__(self, *args):
raise TypeError("%s object is not callable" % self.__class__)
def _entry(self, i, j, **kwargs):
return MatrixElement(self, i, j)
@property
def free_symbols(self):
return set((self,))
def doit(self, **hints):
if hints.get('deep', True):
return type(self)(self.args[0], self.args[1].doit(**hints),
self.args[2].doit(**hints))
else:
return self
def _eval_simplify(self, **kwargs):
return self
def _eval_derivative(self, x):
# x is a scalar:
return ZeroMatrix(self.shape[0], self.shape[1])
def _eval_derivative_matrix_lines(self, x):
if self != x:
first = ZeroMatrix(x.shape[0], self.shape[0]) if self.shape[0] != 1 else S.Zero
second = ZeroMatrix(x.shape[1], self.shape[1]) if self.shape[1] != 1 else S.Zero
return [_LeftRightArgs(
[first, second],
)]
else:
first = Identity(self.shape[0]) if self.shape[0] != 1 else S.One
second = Identity(self.shape[1]) if self.shape[1] != 1 else S.One
return [_LeftRightArgs(
[first, second],
)]
class Identity(MatrixExpr):
"""The Matrix Identity I - multiplicative identity
Examples
========
>>> from sympy.matrices import Identity, MatrixSymbol
>>> A = MatrixSymbol('A', 3, 5)
>>> I = Identity(3)
>>> I*A
A
"""
is_Identity = True
def __new__(cls, n):
n = _sympify(n)
cls._check_dim(n)
return super(Identity, cls).__new__(cls, n)
@property
def rows(self):
return self.args[0]
@property
def cols(self):
return self.args[0]
@property
def shape(self):
return (self.args[0], self.args[0])
@property
def is_square(self):
return True
def _eval_transpose(self):
return self
def _eval_trace(self):
return self.rows
def _eval_inverse(self):
return self
def conjugate(self):
return self
def _entry(self, i, j, **kwargs):
eq = Eq(i, j)
if eq is S.true:
return S.One
elif eq is S.false:
return S.Zero
return KroneckerDelta(i, j, (0, self.cols-1))
def _eval_determinant(self):
return S.One
class GenericIdentity(Identity):
"""
An identity matrix without a specified shape
This exists primarily so MatMul() with no arguments can return something
meaningful.
"""
def __new__(cls):
# super(Identity, cls) instead of super(GenericIdentity, cls) because
# Identity.__new__ doesn't have the same signature
return super(Identity, cls).__new__(cls)
@property
def rows(self):
raise TypeError("GenericIdentity does not have a specified shape")
@property
def cols(self):
raise TypeError("GenericIdentity does not have a specified shape")
@property
def shape(self):
raise TypeError("GenericIdentity does not have a specified shape")
# Avoid Matrix.__eq__ which might call .shape
def __eq__(self, other):
return isinstance(other, GenericIdentity)
def __ne__(self, other):
return not (self == other)
def __hash__(self):
return super(GenericIdentity, self).__hash__()
class ZeroMatrix(MatrixExpr):
"""The Matrix Zero 0 - additive identity
Examples
========
>>> from sympy import MatrixSymbol, ZeroMatrix
>>> A = MatrixSymbol('A', 3, 5)
>>> Z = ZeroMatrix(3, 5)
>>> A + Z
A
>>> Z*A.T
0
"""
is_ZeroMatrix = True
def __new__(cls, m, n):
m, n = _sympify(m), _sympify(n)
cls._check_dim(m)
cls._check_dim(n)
return super(ZeroMatrix, cls).__new__(cls, m, n)
@property
def shape(self):
return (self.args[0], self.args[1])
@_sympifyit('other', NotImplemented)
@call_highest_priority('__rpow__')
def __pow__(self, other):
if other != 1 and not self.is_square:
raise ShapeError("Power of non-square matrix %s" % self)
if other == 0:
return Identity(self.rows)
if other < 1:
raise ValueError("Matrix det == 0; not invertible.")
return self
def _eval_transpose(self):
return ZeroMatrix(self.cols, self.rows)
def _eval_trace(self):
return S.Zero
def _eval_determinant(self):
return S.Zero
def conjugate(self):
return self
def _entry(self, i, j, **kwargs):
return S.Zero
def __nonzero__(self):
return False
__bool__ = __nonzero__
class GenericZeroMatrix(ZeroMatrix):
"""
A zero matrix without a specified shape
This exists primarily so MatAdd() with no arguments can return something
meaningful.
"""
def __new__(cls):
# super(ZeroMatrix, cls) instead of super(GenericZeroMatrix, cls)
# because ZeroMatrix.__new__ doesn't have the same signature
return super(ZeroMatrix, cls).__new__(cls)
@property
def rows(self):
raise TypeError("GenericZeroMatrix does not have a specified shape")
@property
def cols(self):
raise TypeError("GenericZeroMatrix does not have a specified shape")
@property
def shape(self):
raise TypeError("GenericZeroMatrix does not have a specified shape")
# Avoid Matrix.__eq__ which might call .shape
def __eq__(self, other):
return isinstance(other, GenericZeroMatrix)
def __ne__(self, other):
return not (self == other)
def __hash__(self):
return super(GenericZeroMatrix, self).__hash__()
class OneMatrix(MatrixExpr):
"""
Matrix whose all entries are ones.
"""
def __new__(cls, m, n):
m, n = _sympify(m), _sympify(n)
cls._check_dim(m)
cls._check_dim(n)
obj = super(OneMatrix, cls).__new__(cls, m, n)
return obj
@property
def shape(self):
return self._args
def as_explicit(self):
from sympy import ImmutableDenseMatrix
return ImmutableDenseMatrix.ones(*self.shape)
def _eval_transpose(self):
return OneMatrix(self.cols, self.rows)
def _eval_trace(self):
return S.One*self.rows
def _eval_determinant(self):
condition = Eq(self.shape[0], 1) & Eq(self.shape[1], 1)
if condition == True:
return S.One
elif condition == False:
return S.Zero
else:
from sympy import Determinant
return Determinant(self)
def conjugate(self):
return self
def _entry(self, i, j, **kwargs):
return S.One
def matrix_symbols(expr):
return [sym for sym in expr.free_symbols if sym.is_Matrix]
class _LeftRightArgs(object):
r"""
Helper class to compute matrix derivatives.
The logic: when an expression is derived by a matrix `X_{mn}`, two lines of
matrix multiplications are created: the one contracted to `m` (first line),
and the one contracted to `n` (second line).
Transposition flips the side by which new matrices are connected to the
lines.
The trace connects the end of the two lines.
"""
def __init__(self, lines, higher=S.One):
self._lines = [i for i in lines]
self._first_pointer_parent = self._lines
self._first_pointer_index = 0
self._first_line_index = 0
self._second_pointer_parent = self._lines
self._second_pointer_index = 1
self._second_line_index = 1
self.higher = higher
@property
def first_pointer(self):
return self._first_pointer_parent[self._first_pointer_index]
@first_pointer.setter
def first_pointer(self, value):
self._first_pointer_parent[self._first_pointer_index] = value
@property
def second_pointer(self):
return self._second_pointer_parent[self._second_pointer_index]
@second_pointer.setter
def second_pointer(self, value):
self._second_pointer_parent[self._second_pointer_index] = value
def __repr__(self):
try:
built = [self._build(i) for i in self._lines]
except Exception:
built = self._lines
return "_LeftRightArgs(lines=%s, higher=%s)" % (
built,
self.higher,
)
def transpose(self):
self._first_pointer_parent, self._second_pointer_parent = self._second_pointer_parent, self._first_pointer_parent
self._first_pointer_index, self._second_pointer_index = self._second_pointer_index, self._first_pointer_index
self._first_line_index, self._second_line_index = self._second_line_index, self._first_line_index
return self
@staticmethod
def _build(expr):
from sympy.core.expr import ExprBuilder
if isinstance(expr, ExprBuilder):
return expr.build()
if isinstance(expr, list):
if len(expr) == 1:
return expr[0]
else:
return expr[0](*[_LeftRightArgs._build(i) for i in expr[1]])
else:
return expr
def build(self):
data = [self._build(i) for i in self._lines]
if self.higher != 1:
data += [self._build(self.higher)]
data = [i.doit() for i in data]
return data
def matrix_form(self):
if self.first != 1 and self.higher != 1:
raise ValueError("higher dimensional array cannot be represented")
def _get_shape(elem):
if isinstance(elem, MatrixExpr):
return elem.shape
return (None, None)
if _get_shape(self.first)[1] != _get_shape(self.second)[1]:
# Remove one-dimensional identity matrices:
# (this is needed by `a.diff(a)` where `a` is a vector)
if _get_shape(self.second) == (1, 1):
return self.first*self.second[0, 0]
if _get_shape(self.first) == (1, 1):
return self.first[1, 1]*self.second.T
raise ValueError("incompatible shapes")
if self.first != 1:
return self.first*self.second.T
else:
return self.higher
def rank(self):
"""
Number of dimensions different from trivial (warning: not related to
matrix rank).
"""
rank = 0
if self.first != 1:
rank += sum([i != 1 for i in self.first.shape])
if self.second != 1:
rank += sum([i != 1 for i in self.second.shape])
if self.higher != 1:
rank += 2
return rank
def _multiply_pointer(self, pointer, other):
from sympy.core.expr import ExprBuilder
from sympy.codegen.array_utils import CodegenArrayContraction, CodegenArrayTensorProduct
subexpr = ExprBuilder(
CodegenArrayContraction,
[
ExprBuilder(
CodegenArrayTensorProduct,
[
pointer,
other
]
),
(1, 2)
],
validator=CodegenArrayContraction._validate
)
return subexpr
def append_first(self, other):
self.first_pointer *= other
def append_second(self, other):
self.second_pointer *= other
def __hash__(self):
return hash((self.first, self.second))
def __eq__(self, other):
if not isinstance(other, _LeftRightArgs):
return False
return (self.first == other.first) and (self.second == other.second)
def _make_matrix(x):
from sympy import ImmutableDenseMatrix
if isinstance(x, MatrixExpr):
return x
return ImmutableDenseMatrix([[x]])
from .matmul import MatMul
from .matadd import MatAdd
from .matpow import MatPow
from .transpose import Transpose
from .inverse import Inverse
|
8ee52e411ac92ec92781986722f8b954078794ae46065cb89825dc145990b8bb | from __future__ import print_function, division
from sympy.core.sympify import _sympify
from sympy.matrices.expressions import MatrixExpr
from sympy import S, I, sqrt, exp
class DFT(MatrixExpr):
""" Discrete Fourier Transform """
def __new__(cls, n):
n = _sympify(n)
cls._check_dim(n)
obj = super(DFT, cls).__new__(cls, n)
return obj
n = property(lambda self: self.args[0])
shape = property(lambda self: (self.n, self.n))
def _entry(self, i, j, **kwargs):
w = exp(-2*S.Pi*I/self.n)
return w**(i*j) / sqrt(self.n)
def _eval_inverse(self):
return IDFT(self.n)
class IDFT(DFT):
""" Inverse Discrete Fourier Transform """
def _entry(self, i, j, **kwargs):
w = exp(-2*S.Pi*I/self.n)
return w**(-i*j) / sqrt(self.n)
def _eval_inverse(self):
return DFT(self.n)
|
fd2cabdba9c2b3c529a5edf567085a37ea6a98fdf8ff1c296e095f584ca367e5 | """Implementation of the Kronecker product"""
from __future__ import division, print_function
from sympy.core import Mul, prod, sympify
from sympy.core.compatibility import range
from sympy.functions import adjoint
from sympy.matrices.expressions.matexpr import MatrixExpr, ShapeError, Identity
from sympy.matrices.expressions.transpose import transpose
from sympy.matrices.matrices import MatrixBase
from sympy.strategies import (
canon, condition, distribute, do_one, exhaust, flatten, typed, unpack)
from sympy.strategies.traverse import bottom_up
from sympy.utilities import sift
from .matadd import MatAdd
from .matmul import MatMul
from .matpow import MatPow
def kronecker_product(*matrices):
"""
The Kronecker product of two or more arguments.
This computes the explicit Kronecker product for subclasses of
``MatrixBase`` i.e. explicit matrices. Otherwise, a symbolic
``KroneckerProduct`` object is returned.
Examples
========
For ``MatrixSymbol`` arguments a ``KroneckerProduct`` object is returned.
Elements of this matrix can be obtained by indexing, or for MatrixSymbols
with known dimension the explicit matrix can be obtained with
``.as_explicit()``
>>> from sympy.matrices import kronecker_product, MatrixSymbol
>>> A = MatrixSymbol('A', 2, 2)
>>> B = MatrixSymbol('B', 2, 2)
>>> kronecker_product(A)
A
>>> kronecker_product(A, B)
KroneckerProduct(A, B)
>>> kronecker_product(A, B)[0, 1]
A[0, 0]*B[0, 1]
>>> kronecker_product(A, B).as_explicit()
Matrix([
[A[0, 0]*B[0, 0], A[0, 0]*B[0, 1], A[0, 1]*B[0, 0], A[0, 1]*B[0, 1]],
[A[0, 0]*B[1, 0], A[0, 0]*B[1, 1], A[0, 1]*B[1, 0], A[0, 1]*B[1, 1]],
[A[1, 0]*B[0, 0], A[1, 0]*B[0, 1], A[1, 1]*B[0, 0], A[1, 1]*B[0, 1]],
[A[1, 0]*B[1, 0], A[1, 0]*B[1, 1], A[1, 1]*B[1, 0], A[1, 1]*B[1, 1]]])
For explicit matrices the Kronecker product is returned as a Matrix
>>> from sympy.matrices import Matrix, kronecker_product
>>> sigma_x = Matrix([
... [0, 1],
... [1, 0]])
...
>>> Isigma_y = Matrix([
... [0, 1],
... [-1, 0]])
...
>>> kronecker_product(sigma_x, Isigma_y)
Matrix([
[ 0, 0, 0, 1],
[ 0, 0, -1, 0],
[ 0, 1, 0, 0],
[-1, 0, 0, 0]])
See Also
========
KroneckerProduct
"""
if not matrices:
raise TypeError("Empty Kronecker product is undefined")
validate(*matrices)
if len(matrices) == 1:
return matrices[0]
else:
return KroneckerProduct(*matrices).doit()
class KroneckerProduct(MatrixExpr):
"""
The Kronecker product of two or more arguments.
The Kronecker product is a non-commutative product of matrices.
Given two matrices of dimension (m, n) and (s, t) it produces a matrix
of dimension (m s, n t).
This is a symbolic object that simply stores its argument without
evaluating it. To actually compute the product, use the function
``kronecker_product()`` or call the the ``.doit()`` or ``.as_explicit()``
methods.
>>> from sympy.matrices import KroneckerProduct, MatrixSymbol
>>> A = MatrixSymbol('A', 5, 5)
>>> B = MatrixSymbol('B', 5, 5)
>>> isinstance(KroneckerProduct(A, B), KroneckerProduct)
True
"""
is_KroneckerProduct = True
def __new__(cls, *args, **kwargs):
args = list(map(sympify, args))
if all(a.is_Identity for a in args):
ret = Identity(prod(a.rows for a in args))
if all(isinstance(a, MatrixBase) for a in args):
return ret.as_explicit()
else:
return ret
check = kwargs.get('check', True)
if check:
validate(*args)
return super(KroneckerProduct, cls).__new__(cls, *args)
@property
def shape(self):
rows, cols = self.args[0].shape
for mat in self.args[1:]:
rows *= mat.rows
cols *= mat.cols
return (rows, cols)
def _entry(self, i, j, **kwargs):
result = 1
for mat in reversed(self.args):
i, m = divmod(i, mat.rows)
j, n = divmod(j, mat.cols)
result *= mat[m, n]
return result
def _eval_adjoint(self):
return KroneckerProduct(*list(map(adjoint, self.args))).doit()
def _eval_conjugate(self):
return KroneckerProduct(*[a.conjugate() for a in self.args]).doit()
def _eval_transpose(self):
return KroneckerProduct(*list(map(transpose, self.args))).doit()
def _eval_trace(self):
from .trace import trace
return prod(trace(a) for a in self.args)
def _eval_determinant(self):
from .determinant import det, Determinant
if not all(a.is_square for a in self.args):
return Determinant(self)
m = self.rows
return prod(det(a)**(m/a.rows) for a in self.args)
def _eval_inverse(self):
try:
return KroneckerProduct(*[a.inverse() for a in self.args])
except ShapeError:
from sympy.matrices.expressions.inverse import Inverse
return Inverse(self)
def structurally_equal(self, other):
'''Determine whether two matrices have the same Kronecker product structure
Examples
========
>>> from sympy import KroneckerProduct, MatrixSymbol, symbols
>>> m, n = symbols(r'm, n', integer=True)
>>> A = MatrixSymbol('A', m, m)
>>> B = MatrixSymbol('B', n, n)
>>> C = MatrixSymbol('C', m, m)
>>> D = MatrixSymbol('D', n, n)
>>> KroneckerProduct(A, B).structurally_equal(KroneckerProduct(C, D))
True
>>> KroneckerProduct(A, B).structurally_equal(KroneckerProduct(D, C))
False
>>> KroneckerProduct(A, B).structurally_equal(C)
False
'''
# Inspired by BlockMatrix
return (isinstance(other, KroneckerProduct)
and self.shape == other.shape
and len(self.args) == len(other.args)
and all(a.shape == b.shape for (a, b) in zip(self.args, other.args)))
def has_matching_shape(self, other):
'''Determine whether two matrices have the appropriate structure to bring matrix
multiplication inside the KroneckerProdut
Examples
========
>>> from sympy import KroneckerProduct, MatrixSymbol, symbols
>>> m, n = symbols(r'm, n', integer=True)
>>> A = MatrixSymbol('A', m, n)
>>> B = MatrixSymbol('B', n, m)
>>> KroneckerProduct(A, B).has_matching_shape(KroneckerProduct(B, A))
True
>>> KroneckerProduct(A, B).has_matching_shape(KroneckerProduct(A, B))
False
>>> KroneckerProduct(A, B).has_matching_shape(A)
False
'''
return (isinstance(other, KroneckerProduct)
and self.cols == other.rows
and len(self.args) == len(other.args)
and all(a.cols == b.rows for (a, b) in zip(self.args, other.args)))
def _eval_expand_kroneckerproduct(self, **hints):
return flatten(canon(typed({KroneckerProduct: distribute(KroneckerProduct, MatAdd)}))(self))
def _kronecker_add(self, other):
if self.structurally_equal(other):
return self.__class__(*[a + b for (a, b) in zip(self.args, other.args)])
else:
return self + other
def _kronecker_mul(self, other):
if self.has_matching_shape(other):
return self.__class__(*[a*b for (a, b) in zip(self.args, other.args)])
else:
return self * other
def doit(self, **kwargs):
deep = kwargs.get('deep', True)
if deep:
args = [arg.doit(**kwargs) for arg in self.args]
else:
args = self.args
return canonicalize(KroneckerProduct(*args))
def validate(*args):
if not all(arg.is_Matrix for arg in args):
raise TypeError("Mix of Matrix and Scalar symbols")
# rules
def extract_commutative(kron):
c_part = []
nc_part = []
for arg in kron.args:
c, nc = arg.args_cnc()
c_part.extend(c)
nc_part.append(Mul._from_args(nc))
c_part = Mul(*c_part)
if c_part != 1:
return c_part*KroneckerProduct(*nc_part)
return kron
def matrix_kronecker_product(*matrices):
"""Compute the Kronecker product of a sequence of SymPy Matrices.
This is the standard Kronecker product of matrices [1].
Parameters
==========
matrices : tuple of MatrixBase instances
The matrices to take the Kronecker product of.
Returns
=======
matrix : MatrixBase
The Kronecker product matrix.
Examples
========
>>> from sympy import Matrix
>>> from sympy.matrices.expressions.kronecker import (
... matrix_kronecker_product)
>>> m1 = Matrix([[1,2],[3,4]])
>>> m2 = Matrix([[1,0],[0,1]])
>>> matrix_kronecker_product(m1, m2)
Matrix([
[1, 0, 2, 0],
[0, 1, 0, 2],
[3, 0, 4, 0],
[0, 3, 0, 4]])
>>> matrix_kronecker_product(m2, m1)
Matrix([
[1, 2, 0, 0],
[3, 4, 0, 0],
[0, 0, 1, 2],
[0, 0, 3, 4]])
References
==========
[1] https://en.wikipedia.org/wiki/Kronecker_product
"""
# Make sure we have a sequence of Matrices
if not all(isinstance(m, MatrixBase) for m in matrices):
raise TypeError(
'Sequence of Matrices expected, got: %s' % repr(matrices)
)
# Pull out the first element in the product.
matrix_expansion = matrices[-1]
# Do the kronecker product working from right to left.
for mat in reversed(matrices[:-1]):
rows = mat.rows
cols = mat.cols
# Go through each row appending kronecker product to.
# running matrix_expansion.
for i in range(rows):
start = matrix_expansion*mat[i*cols]
# Go through each column joining each item
for j in range(cols - 1):
start = start.row_join(
matrix_expansion*mat[i*cols + j + 1]
)
# If this is the first element, make it the start of the
# new row.
if i == 0:
next = start
else:
next = next.col_join(start)
matrix_expansion = next
MatrixClass = max(matrices, key=lambda M: M._class_priority).__class__
if isinstance(matrix_expansion, MatrixClass):
return matrix_expansion
else:
return MatrixClass(matrix_expansion)
def explicit_kronecker_product(kron):
# Make sure we have a sequence of Matrices
if not all(isinstance(m, MatrixBase) for m in kron.args):
return kron
return matrix_kronecker_product(*kron.args)
rules = (unpack,
explicit_kronecker_product,
flatten,
extract_commutative)
canonicalize = exhaust(condition(lambda x: isinstance(x, KroneckerProduct),
do_one(*rules)))
def _kronecker_dims_key(expr):
if isinstance(expr, KroneckerProduct):
return tuple(a.shape for a in expr.args)
else:
return (0,)
def kronecker_mat_add(expr):
from functools import reduce
args = sift(expr.args, _kronecker_dims_key)
nonkrons = args.pop((0,), None)
if not args:
return expr
krons = [reduce(lambda x, y: x._kronecker_add(y), group)
for group in args.values()]
if not nonkrons:
return MatAdd(*krons)
else:
return MatAdd(*krons) + nonkrons
def kronecker_mat_mul(expr):
# modified from block matrix code
factor, matrices = expr.as_coeff_matrices()
i = 0
while i < len(matrices) - 1:
A, B = matrices[i:i+2]
if isinstance(A, KroneckerProduct) and isinstance(B, KroneckerProduct):
matrices[i] = A._kronecker_mul(B)
matrices.pop(i+1)
else:
i += 1
return factor*MatMul(*matrices)
def kronecker_mat_pow(expr):
if isinstance(expr.base, KroneckerProduct):
return KroneckerProduct(*[MatPow(a, expr.exp) for a in expr.base.args])
else:
return expr
def combine_kronecker(expr):
"""Combine KronekeckerProduct with expression.
If possible write operations on KroneckerProducts of compatible shapes
as a single KroneckerProduct.
Examples
========
>>> from sympy.matrices.expressions import MatrixSymbol, KroneckerProduct, combine_kronecker
>>> from sympy import symbols
>>> m, n = symbols(r'm, n', integer=True)
>>> A = MatrixSymbol('A', m, n)
>>> B = MatrixSymbol('B', n, m)
>>> combine_kronecker(KroneckerProduct(A, B)*KroneckerProduct(B, A))
KroneckerProduct(A*B, B*A)
>>> combine_kronecker(KroneckerProduct(A, B)+KroneckerProduct(B.T, A.T))
KroneckerProduct(A + B.T, B + A.T)
>>> combine_kronecker(KroneckerProduct(A, B)**m)
KroneckerProduct(A**m, B**m)
"""
def haskron(expr):
return isinstance(expr, MatrixExpr) and expr.has(KroneckerProduct)
rule = exhaust(
bottom_up(exhaust(condition(haskron, typed(
{MatAdd: kronecker_mat_add,
MatMul: kronecker_mat_mul,
MatPow: kronecker_mat_pow})))))
result = rule(expr)
doit = getattr(result, 'doit', None)
if doit is not None:
return doit()
else:
return result
|
e57a6ffd2bc34fd06a20ab3716972b8df3f6777da5214d4cbb22c0762ad89655 | from __future__ import print_function, division
from sympy.core.sympify import _sympify
from sympy.matrices.expressions import MatrixExpr
from sympy.core import S, Eq, Ge
from sympy.functions.special.tensor_functions import KroneckerDelta
class DiagonalMatrix(MatrixExpr):
"""DiagonalMatrix(M) will create a matrix expression that
behaves as though all off-diagonal elements,
`M[i, j]` where `i != j`, are zero.
Examples
========
>>> from sympy import MatrixSymbol, DiagonalMatrix, Symbol
>>> n = Symbol('n', integer=True)
>>> m = Symbol('m', integer=True)
>>> D = DiagonalMatrix(MatrixSymbol('x', 2, 3))
>>> D[1, 2]
0
>>> D[1, 1]
x[1, 1]
The length of the diagonal -- the lesser of the two dimensions of `M` --
is accessed through the `diagonal_length` property:
>>> D.diagonal_length
2
>>> DiagonalMatrix(MatrixSymbol('x', n + 1, n)).diagonal_length
n
When one of the dimensions is symbolic the other will be treated as
though it is smaller:
>>> tall = DiagonalMatrix(MatrixSymbol('x', n, 3))
>>> tall.diagonal_length
3
>>> tall[10, 1]
0
When the size of the diagonal is not known, a value of None will
be returned:
>>> DiagonalMatrix(MatrixSymbol('x', n, m)).diagonal_length is None
True
"""
arg = property(lambda self: self.args[0])
shape = property(lambda self: self.arg.shape)
@property
def diagonal_length(self):
r, c = self.shape
if r.is_Integer and c.is_Integer:
m = min(r, c)
elif r.is_Integer and not c.is_Integer:
m = r
elif c.is_Integer and not r.is_Integer:
m = c
elif r == c:
m = r
else:
try:
m = min(r, c)
except TypeError:
m = None
return m
def _entry(self, i, j, **kwargs):
if self.diagonal_length is not None:
if Ge(i, self.diagonal_length) is S.true:
return S.Zero
elif Ge(j, self.diagonal_length) is S.true:
return S.Zero
eq = Eq(i, j)
if eq is S.true:
return self.arg[i, i]
elif eq is S.false:
return S.Zero
return self.arg[i, j]*KroneckerDelta(i, j)
class DiagonalOf(MatrixExpr):
"""DiagonalOf(M) will create a matrix expression that
is equivalent to the diagonal of `M`, represented as
a single column matrix.
Examples
========
>>> from sympy import MatrixSymbol, DiagonalOf, Symbol
>>> n = Symbol('n', integer=True)
>>> m = Symbol('m', integer=True)
>>> x = MatrixSymbol('x', 2, 3)
>>> diag = DiagonalOf(x)
>>> diag.shape
(2, 1)
The diagonal can be addressed like a matrix or vector and will
return the corresponding element of the original matrix:
>>> diag[1, 0] == diag[1] == x[1, 1]
True
The length of the diagonal -- the lesser of the two dimensions of `M` --
is accessed through the `diagonal_length` property:
>>> diag.diagonal_length
2
>>> DiagonalOf(MatrixSymbol('x', n + 1, n)).diagonal_length
n
When only one of the dimensions is symbolic the other will be
treated as though it is smaller:
>>> dtall = DiagonalOf(MatrixSymbol('x', n, 3))
>>> dtall.diagonal_length
3
When the size of the diagonal is not known, a value of None will
be returned:
>>> DiagonalOf(MatrixSymbol('x', n, m)).diagonal_length is None
True
"""
arg = property(lambda self: self.args[0])
@property
def shape(self):
r, c = self.arg.shape
if r.is_Integer and c.is_Integer:
m = min(r, c)
elif r.is_Integer and not c.is_Integer:
m = r
elif c.is_Integer and not r.is_Integer:
m = c
elif r == c:
m = r
else:
try:
m = min(r, c)
except TypeError:
m = None
return m, S.One
@property
def diagonal_length(self):
return self.shape[0]
def _entry(self, i, j, **kwargs):
return self.arg._entry(i, i, **kwargs)
class DiagonalizeVector(MatrixExpr):
"""
Turn a vector into a diagonal matrix.
"""
def __new__(cls, vector):
vector = _sympify(vector)
obj = MatrixExpr.__new__(cls, vector)
shape = vector.shape
dim = shape[1] if shape[0] == 1 else shape[0]
if vector.shape[0] != 1:
obj._iscolumn = True
else:
obj._iscolumn = False
obj._shape = (dim, dim)
obj._vector = vector
return obj
@property
def shape(self):
return self._shape
def _entry(self, i, j, **kwargs):
if self._iscolumn:
result = self._vector._entry(i, 0, **kwargs)
else:
result = self._vector._entry(0, j, **kwargs)
if i != j:
result *= KroneckerDelta(i, j)
return result
def _eval_transpose(self):
return self
def as_explicit(self):
from sympy import diag
return diag(*list(self._vector.as_explicit()))
def doit(self, **hints):
from sympy.assumptions import ask, Q
from sympy import Transpose, Mul, MatMul
from sympy import MatrixBase, eye
vector = self._vector
# This accounts for shape (1, 1) and identity matrices, among others:
if ask(Q.diagonal(vector)):
return vector
if isinstance(vector, MatrixBase):
ret = eye(max(vector.shape))
for i in range(ret.shape[0]):
ret[i, i] = vector[i]
return type(vector)(ret)
if vector.is_MatMul:
matrices = [arg for arg in vector.args if arg.is_Matrix]
scalars = [arg for arg in vector.args if arg not in matrices]
if scalars:
return Mul.fromiter(scalars)*DiagonalizeVector(MatMul.fromiter(matrices).doit()).doit()
if isinstance(vector, Transpose):
vector = vector.arg
return DiagonalizeVector(vector)
def diagonalize_vector(vector):
return DiagonalizeVector(vector).doit()
|
cb1aceeb68233a85d0d23669a82f6c08809ef4d7fc9cc110d257ee9331c0bdf8 | from __future__ import print_function, division
from sympy import Basic, Expr, sympify, S
from sympy.matrices.matrices import MatrixBase
from .matexpr import ShapeError
class Trace(Expr):
"""Matrix Trace
Represents the trace of a matrix expression.
Examples
========
>>> from sympy import MatrixSymbol, Trace, eye
>>> A = MatrixSymbol('A', 3, 3)
>>> Trace(A)
Trace(A)
"""
is_Trace = True
is_commutative = True
def __new__(cls, mat):
mat = sympify(mat)
if not mat.is_Matrix:
raise TypeError("input to Trace, %s, is not a matrix" % str(mat))
if not mat.is_square:
raise ShapeError("Trace of a non-square matrix")
return Basic.__new__(cls, mat)
def _eval_transpose(self):
return self
def _eval_derivative(self, v):
from sympy import Sum
from .matexpr import MatrixElement
if isinstance(v, MatrixElement):
return self.rewrite(Sum).diff(v)
expr = self.doit()
if isinstance(expr, Trace):
# Avoid looping infinitely:
raise NotImplementedError
return expr._eval_derivative(v)
def _eval_derivative_matrix_lines(self, x):
from sympy.codegen.array_utils import CodegenArrayContraction, CodegenArrayTensorProduct
from sympy.core.expr import ExprBuilder
r = self.args[0]._eval_derivative_matrix_lines(x)
for lr in r:
if lr.higher == 1:
lr.higher = ExprBuilder(
CodegenArrayContraction,
[
ExprBuilder(
CodegenArrayTensorProduct,
[
lr._lines[0],
lr._lines[1],
]
),
(1, 3),
],
validator=CodegenArrayContraction._validate
)
else:
# This is not a matrix line:
lr.higher = ExprBuilder(
CodegenArrayContraction,
[
ExprBuilder(
CodegenArrayTensorProduct,
[
lr._lines[0],
lr._lines[1],
lr.higher,
]
),
(1, 3), (0, 2)
]
)
lr._lines = [S.One, S.One]
lr._first_pointer_parent = lr._lines
lr._second_pointer_parent = lr._lines
lr._first_pointer_index = 0
lr._second_pointer_index = 1
return r
@property
def arg(self):
return self.args[0]
def doit(self, **kwargs):
if kwargs.get('deep', True):
arg = self.arg.doit(**kwargs)
try:
return arg._eval_trace()
except (AttributeError, NotImplementedError):
return Trace(arg)
else:
# _eval_trace would go too deep here
if isinstance(self.arg, MatrixBase):
return trace(self.arg)
else:
return Trace(self.arg)
def _eval_rewrite_as_Sum(self, expr, **kwargs):
from sympy import Sum, Dummy
i = Dummy('i')
return Sum(self.arg[i, i], (i, 0, self.arg.rows-1)).doit()
def trace(expr):
"""Trace of a Matrix. Sum of the diagonal elements.
Examples
========
>>> from sympy import trace, Symbol, MatrixSymbol, pprint, eye
>>> n = Symbol('n')
>>> X = MatrixSymbol('X', n, n) # A square matrix
>>> trace(2*X)
2*Trace(X)
>>> trace(eye(3))
3
"""
return Trace(expr).doit()
|
b2d57b303262523b3b8cae3b85379b7c891dc0a566a8ef60db2d8752f8a63a52 | from __future__ import print_function, division
from sympy.core import Mul, sympify
from sympy.matrices.expressions.matexpr import (
MatrixExpr, ShapeError, OneMatrix, ZeroMatrix
)
from sympy.strategies import (
unpack, flatten, condition, exhaust, rm_id, sort
)
def hadamard_product(*matrices):
"""
Return the elementwise (aka Hadamard) product of matrices.
Examples
========
>>> from sympy.matrices import hadamard_product, MatrixSymbol
>>> A = MatrixSymbol('A', 2, 3)
>>> B = MatrixSymbol('B', 2, 3)
>>> hadamard_product(A)
A
>>> hadamard_product(A, B)
HadamardProduct(A, B)
>>> hadamard_product(A, B)[0, 1]
A[0, 1]*B[0, 1]
"""
if not matrices:
raise TypeError("Empty Hadamard product is undefined")
validate(*matrices)
if len(matrices) == 1:
return matrices[0]
else:
matrices = [i for i in matrices if not i.is_Identity]
return HadamardProduct(*matrices).doit()
class HadamardProduct(MatrixExpr):
"""
Elementwise product of matrix expressions
Examples
========
Hadamard product for matrix symbols:
>>> from sympy.matrices import hadamard_product, HadamardProduct, MatrixSymbol
>>> A = MatrixSymbol('A', 5, 5)
>>> B = MatrixSymbol('B', 5, 5)
>>> isinstance(hadamard_product(A, B), HadamardProduct)
True
Notes
=====
This is a symbolic object that simply stores its argument without
evaluating it. To actually compute the product, use the function
``hadamard_product()`` or ``HadamardProduct.doit``
"""
is_HadamardProduct = True
def __new__(cls, *args, **kwargs):
args = list(map(sympify, args))
check = kwargs.get('check', True)
if check:
validate(*args)
return super(HadamardProduct, cls).__new__(cls, *args)
@property
def shape(self):
return self.args[0].shape
def _entry(self, i, j, **kwargs):
return Mul(*[arg._entry(i, j, **kwargs) for arg in self.args])
def _eval_transpose(self):
from sympy.matrices.expressions.transpose import transpose
return HadamardProduct(*list(map(transpose, self.args)))
def doit(self, **ignored):
expr = self.func(*[i.doit(**ignored) for i in self.args])
# Check for explicit matrices:
from sympy import MatrixBase
from sympy.matrices.immutable import ImmutableMatrix
explicit = [i for i in expr.args if isinstance(i, MatrixBase)]
if explicit:
remainder = [i for i in expr.args if i not in explicit]
expl_mat = ImmutableMatrix([
Mul.fromiter(i) for i in zip(*explicit)
]).reshape(*self.shape)
expr = HadamardProduct(*([expl_mat] + remainder))
return canonicalize(expr)
def _eval_derivative(self, x):
from sympy import Add
terms = []
args = list(self.args)
for i in range(len(args)):
factors = args[:i] + [args[i].diff(x)] + args[i+1:]
terms.append(hadamard_product(*factors))
return Add.fromiter(terms)
def _eval_derivative_matrix_lines(self, x):
from sympy.core.expr import ExprBuilder
from sympy.codegen.array_utils import CodegenArrayDiagonal, CodegenArrayTensorProduct
from sympy.matrices.expressions.matexpr import _make_matrix
with_x_ind = [i for i, arg in enumerate(self.args) if arg.has(x)]
lines = []
for ind in with_x_ind:
left_args = self.args[:ind]
right_args = self.args[ind+1:]
d = self.args[ind]._eval_derivative_matrix_lines(x)
hadam = hadamard_product(*(right_args + left_args))
diagonal = [(0, 2), (3, 4)]
diagonal = [e for j, e in enumerate(diagonal) if self.shape[j] != 1]
for i in d:
l1 = i._lines[i._first_line_index]
l2 = i._lines[i._second_line_index]
subexpr = ExprBuilder(
CodegenArrayDiagonal,
[
ExprBuilder(
CodegenArrayTensorProduct,
[
ExprBuilder(_make_matrix, [l1]),
hadam,
ExprBuilder(_make_matrix, [l2]),
]
),
] + diagonal, # turn into *diagonal after dropping Python 2.7
)
i._first_pointer_parent = subexpr.args[0].args[0].args
i._first_pointer_index = 0
i._second_pointer_parent = subexpr.args[0].args[2].args
i._second_pointer_index = 0
i._lines = [subexpr]
lines.append(i)
return lines
def validate(*args):
if not all(arg.is_Matrix for arg in args):
raise TypeError("Mix of Matrix and Scalar symbols")
A = args[0]
for B in args[1:]:
if A.shape != B.shape:
raise ShapeError("Matrices %s and %s are not aligned" % (A, B))
# TODO Implement algorithm for rewriting Hadamard product as diagonal matrix
# if matmul identy matrix is multiplied.
def canonicalize(x):
"""Canonicalize the Hadamard product ``x`` with mathematical properties.
Examples
========
>>> from sympy.matrices.expressions import MatrixSymbol, HadamardProduct
>>> from sympy.matrices.expressions import OneMatrix, ZeroMatrix
>>> from sympy.matrices.expressions.hadamard import canonicalize
>>> from sympy import init_printing
>>> init_printing(use_unicode=False)
>>> A = MatrixSymbol('A', 2, 2)
>>> B = MatrixSymbol('B', 2, 2)
>>> C = MatrixSymbol('C', 2, 2)
Hadamard product associativity:
>>> X = HadamardProduct(A, HadamardProduct(B, C))
>>> X
A.*(B.*C)
>>> canonicalize(X)
A.*B.*C
Hadamard product commutativity:
>>> X = HadamardProduct(A, B)
>>> Y = HadamardProduct(B, A)
>>> X
A.*B
>>> Y
B.*A
>>> canonicalize(X)
A.*B
>>> canonicalize(Y)
A.*B
Hadamard product identity:
>>> X = HadamardProduct(A, OneMatrix(2, 2))
>>> X
A.*1
>>> canonicalize(X)
A
Absorbing element of Hadamard product:
>>> X = HadamardProduct(A, ZeroMatrix(2, 2))
>>> X
A.*0
>>> canonicalize(X)
0
Rewriting to Hadamard Power
>>> X = HadamardProduct(A, A, A)
>>> X
A.*A.*A
>>> canonicalize(X)
.3
A
Notes
=====
As the Hadamard product is associative, nested products can be flattened.
The Hadamard product is commutative so that factors can be sorted for
canonical form.
A matrix of only ones is an identity for Hadamard product,
so every matrices of only ones can be removed.
Any zero matrix will make the whole product a zero matrix.
Duplicate elements can be collected and rewritten as HadamardPower
References
==========
.. [1] https://en.wikipedia.org/wiki/Hadamard_product_(matrices)
"""
from sympy.core.compatibility import default_sort_key
# Associativity
rule = condition(
lambda x: isinstance(x, HadamardProduct),
flatten
)
fun = exhaust(rule)
x = fun(x)
# Identity
fun = condition(
lambda x: isinstance(x, HadamardProduct),
rm_id(lambda x: isinstance(x, OneMatrix))
)
x = fun(x)
# Absorbing by Zero Matrix
def absorb(x):
if any(isinstance(c, ZeroMatrix) for c in x.args):
return ZeroMatrix(*x.shape)
else:
return x
fun = condition(
lambda x: isinstance(x, HadamardProduct),
absorb
)
x = fun(x)
# Rewriting with HadamardPower
if isinstance(x, HadamardProduct):
from collections import Counter
tally = Counter(x.args)
new_arg = []
for base, exp in tally.items():
if exp == 1:
new_arg.append(base)
else:
new_arg.append(HadamardPower(base, exp))
x = HadamardProduct(*new_arg)
# Commutativity
fun = condition(
lambda x: isinstance(x, HadamardProduct),
sort(default_sort_key)
)
x = fun(x)
# Unpacking
x = unpack(x)
return x
def hadamard_power(base, exp):
base = sympify(base)
exp = sympify(exp)
if exp == 1:
return base
if not base.is_Matrix:
return base**exp
if exp.is_Matrix:
raise ValueError("cannot raise expression to a matrix")
return HadamardPower(base, exp)
class HadamardPower(MatrixExpr):
r"""
Elementwise power of matrix expressions
Parameters
==========
base : scalar or matrix
exp : scalar or matrix
Notes
=====
There are four definitions for the hadamard power which can be used.
Let's consider `A, B` as `(m, n)` matrices, and `a, b` as scalars.
Matrix raised to a scalar exponent:
.. math::
A^{\circ b} = \begin{bmatrix}
A_{0, 0}^b & A_{0, 1}^b & \cdots & A_{0, n-1}^b \\
A_{1, 0}^b & A_{1, 1}^b & \cdots & A_{1, n-1}^b \\
\vdots & \vdots & \ddots & \vdots \\
A_{m-1, 0}^b & A_{m-1, 1}^b & \cdots & A_{m-1, n-1}^b
\end{bmatrix}
Scalar raised to a matrix exponent:
.. math::
a^{\circ B} = \begin{bmatrix}
a^{B_{0, 0}} & a^{B_{0, 1}} & \cdots & a^{B_{0, n-1}} \\
a^{B_{1, 0}} & a^{B_{1, 1}} & \cdots & a^{B_{1, n-1}} \\
\vdots & \vdots & \ddots & \vdots \\
a^{B_{m-1, 0}} & a^{B_{m-1, 1}} & \cdots & a^{B_{m-1, n-1}}
\end{bmatrix}
Matrix raised to a matrix exponent:
.. math::
A^{\circ B} = \begin{bmatrix}
A_{0, 0}^{B_{0, 0}} & A_{0, 1}^{B_{0, 1}} &
\cdots & A_{0, n-1}^{B_{0, n-1}} \\
A_{1, 0}^{B_{1, 0}} & A_{1, 1}^{B_{1, 1}} &
\cdots & A_{1, n-1}^{B_{1, n-1}} \\
\vdots & \vdots &
\ddots & \vdots \\
A_{m-1, 0}^{B_{m-1, 0}} & A_{m-1, 1}^{B_{m-1, 1}} &
\cdots & A_{m-1, n-1}^{B_{m-1, n-1}}
\end{bmatrix}
Scalar raised to a scalar exponent:
.. math::
a^{\circ b} = a^b
"""
def __new__(cls, base, exp):
base = sympify(base)
exp = sympify(exp)
if base.is_scalar and exp.is_scalar:
return base ** exp
if base.is_Matrix and exp.is_Matrix and base.shape != exp.shape:
raise ValueError(
'The shape of the base {} and '
'the shape of the exponent {} do not match.'
.format(base.shape, exp.shape)
)
obj = super(HadamardPower, cls).__new__(cls, base, exp)
return obj
@property
def base(self):
return self._args[0]
@property
def exp(self):
return self._args[1]
@property
def shape(self):
if self.base.is_Matrix:
return self.base.shape
return self.exp.shape
def _entry(self, i, j, **kwargs):
base = self.base
exp = self.exp
if base.is_Matrix:
a = base._entry(i, j, **kwargs)
elif base.is_scalar:
a = base
else:
raise ValueError(
'The base {} must be a scalar or a matrix.'.format(base))
if exp.is_Matrix:
b = exp._entry(i, j, **kwargs)
elif exp.is_scalar:
b = exp
else:
raise ValueError(
'The exponent {} must be a scalar or a matrix.'.format(exp))
return a ** b
def _eval_transpose(self):
from sympy.matrices.expressions.transpose import transpose
return HadamardPower(transpose(self.base), self.exp)
def _eval_derivative(self, x):
from sympy import log
dexp = self.exp.diff(x)
logbase = self.base.applyfunc(log)
dlbase = logbase.diff(x)
return hadamard_product(
dexp*logbase + self.exp*dlbase,
self
)
def _eval_derivative_matrix_lines(self, x):
from sympy.codegen.array_utils import CodegenArrayTensorProduct
from sympy.codegen.array_utils import CodegenArrayDiagonal
from sympy.core.expr import ExprBuilder
from sympy.matrices.expressions.matexpr import _make_matrix
lr = self.base._eval_derivative_matrix_lines(x)
for i in lr:
diagonal = [(1, 2), (3, 4)]
diagonal = [e for j, e in enumerate(diagonal) if self.base.shape[j] != 1]
l1 = i._lines[i._first_line_index]
l2 = i._lines[i._second_line_index]
subexpr = ExprBuilder(
CodegenArrayDiagonal,
[
ExprBuilder(
CodegenArrayTensorProduct,
[
ExprBuilder(_make_matrix, [l1]),
self.exp*hadamard_power(self.base, self.exp-1),
ExprBuilder(_make_matrix, [l2]),
]
),
] + diagonal, # turn into *diagonal after dropping Python 2.7
validator=CodegenArrayDiagonal._validate
)
i._first_pointer_parent = subexpr.args[0].args[0].args
i._first_pointer_index = 0
i._first_line_index = 0
i._second_pointer_parent = subexpr.args[0].args[2].args
i._second_pointer_index = 0
i._second_line_index = 0
i._lines = [subexpr]
return lr
|
3836415a9edc1eadf8675c5f92d6b26ea34812f3d39884ab187a6fb8dbc132c9 | from __future__ import print_function, division
from sympy import ask, Q
from sympy.core import Basic, Add
from sympy.core.compatibility import range
from sympy.strategies import typed, exhaust, condition, do_one, unpack
from sympy.strategies.traverse import bottom_up
from sympy.utilities import sift
from sympy.utilities.misc import filldedent
from sympy.matrices.expressions.matexpr import MatrixExpr, ZeroMatrix, Identity
from sympy.matrices.expressions.matmul import MatMul
from sympy.matrices.expressions.matadd import MatAdd
from sympy.matrices.expressions.matpow import MatPow
from sympy.matrices.expressions.transpose import Transpose, transpose
from sympy.matrices.expressions.trace import Trace
from sympy.matrices.expressions.determinant import det, Determinant
from sympy.matrices.expressions.slice import MatrixSlice
from sympy.matrices.expressions.inverse import Inverse
from sympy.matrices import Matrix, ShapeError
from sympy.functions.elementary.complexes import re, im
class BlockMatrix(MatrixExpr):
"""A BlockMatrix is a Matrix comprised of other matrices.
The submatrices are stored in a SymPy Matrix object but accessed as part of
a Matrix Expression
>>> from sympy import (MatrixSymbol, BlockMatrix, symbols,
... Identity, ZeroMatrix, block_collapse)
>>> n,m,l = symbols('n m l')
>>> X = MatrixSymbol('X', n, n)
>>> Y = MatrixSymbol('Y', m ,m)
>>> Z = MatrixSymbol('Z', n, m)
>>> B = BlockMatrix([[X, Z], [ZeroMatrix(m,n), Y]])
>>> print(B)
Matrix([
[X, Z],
[0, Y]])
>>> C = BlockMatrix([[Identity(n), Z]])
>>> print(C)
Matrix([[I, Z]])
>>> print(block_collapse(C*B))
Matrix([[X, Z + Z*Y]])
Some matrices might be comprised of rows of blocks with
the matrices in each row having the same height and the
rows all having the same total number of columns but
not having the same number of columns for each matrix
in each row. In this case, the matrix is not a block
matrix and should be instantiated by Matrix.
>>> from sympy import ones, Matrix
>>> dat = [
... [ones(3,2), ones(3,3)*2],
... [ones(2,3)*3, ones(2,2)*4]]
...
>>> BlockMatrix(dat)
Traceback (most recent call last):
...
ValueError:
Although this matrix is comprised of blocks, the blocks do not fill
the matrix in a size-symmetric fashion. To create a full matrix from
these arguments, pass them directly to Matrix.
>>> Matrix(dat)
Matrix([
[1, 1, 2, 2, 2],
[1, 1, 2, 2, 2],
[1, 1, 2, 2, 2],
[3, 3, 3, 4, 4],
[3, 3, 3, 4, 4]])
See Also
========
sympy.matrices.matrices.MatrixBase.irregular
"""
def __new__(cls, *args, **kwargs):
from sympy.matrices.immutable import ImmutableDenseMatrix
from sympy.utilities.iterables import is_sequence
isMat = lambda i: getattr(i, 'is_Matrix', False)
if len(args) != 1 or \
not is_sequence(args[0]) or \
len(set([isMat(r) for r in args[0]])) != 1:
raise ValueError(filldedent('''
expecting a sequence of 1 or more rows
containing Matrices.'''))
rows = args[0] if args else []
if not isMat(rows):
if rows and isMat(rows[0]):
rows = [rows] # rows is not list of lists or []
# regularity check
# same number of matrices in each row
blocky = ok = len(set([len(r) for r in rows])) == 1
if ok:
# same number of rows for each matrix in a row
for r in rows:
ok = len(set([i.rows for i in r])) == 1
if not ok:
break
blocky = ok
# same number of cols for each matrix in each col
for c in range(len(rows[0])):
ok = len(set([rows[i][c].cols
for i in range(len(rows))])) == 1
if not ok:
break
if not ok:
# same total cols in each row
ok = len(set([
sum([i.cols for i in r]) for r in rows])) == 1
if blocky and ok:
raise ValueError(filldedent('''
Although this matrix is comprised of blocks,
the blocks do not fill the matrix in a
size-symmetric fashion. To create a full matrix
from these arguments, pass them directly to
Matrix.'''))
raise ValueError(filldedent('''
When there are not the same number of rows in each
row's matrices or there are not the same number of
total columns in each row, the matrix is not a
block matrix. If this matrix is known to consist of
blocks fully filling a 2-D space then see
Matrix.irregular.'''))
mat = ImmutableDenseMatrix(rows, evaluate=False)
obj = Basic.__new__(cls, mat)
return obj
@property
def shape(self):
numrows = numcols = 0
M = self.blocks
for i in range(M.shape[0]):
numrows += M[i, 0].shape[0]
for i in range(M.shape[1]):
numcols += M[0, i].shape[1]
return (numrows, numcols)
@property
def blockshape(self):
return self.blocks.shape
@property
def blocks(self):
return self.args[0]
@property
def rowblocksizes(self):
return [self.blocks[i, 0].rows for i in range(self.blockshape[0])]
@property
def colblocksizes(self):
return [self.blocks[0, i].cols for i in range(self.blockshape[1])]
def structurally_equal(self, other):
return (isinstance(other, BlockMatrix)
and self.shape == other.shape
and self.blockshape == other.blockshape
and self.rowblocksizes == other.rowblocksizes
and self.colblocksizes == other.colblocksizes)
def _blockmul(self, other):
if (isinstance(other, BlockMatrix) and
self.colblocksizes == other.rowblocksizes):
return BlockMatrix(self.blocks*other.blocks)
return self * other
def _blockadd(self, other):
if (isinstance(other, BlockMatrix)
and self.structurally_equal(other)):
return BlockMatrix(self.blocks + other.blocks)
return self + other
def _eval_transpose(self):
# Flip all the individual matrices
matrices = [transpose(matrix) for matrix in self.blocks]
# Make a copy
M = Matrix(self.blockshape[0], self.blockshape[1], matrices)
# Transpose the block structure
M = M.transpose()
return BlockMatrix(M)
def _eval_trace(self):
if self.rowblocksizes == self.colblocksizes:
return Add(*[Trace(self.blocks[i, i])
for i in range(self.blockshape[0])])
raise NotImplementedError(
"Can't perform trace of irregular blockshape")
def _eval_determinant(self):
if self.blockshape == (2, 2):
[[A, B],
[C, D]] = self.blocks.tolist()
if ask(Q.invertible(A)):
return det(A)*det(D - C*A.I*B)
elif ask(Q.invertible(D)):
return det(D)*det(A - B*D.I*C)
return Determinant(self)
def as_real_imag(self):
real_matrices = [re(matrix) for matrix in self.blocks]
real_matrices = Matrix(self.blockshape[0], self.blockshape[1], real_matrices)
im_matrices = [im(matrix) for matrix in self.blocks]
im_matrices = Matrix(self.blockshape[0], self.blockshape[1], im_matrices)
return (real_matrices, im_matrices)
def transpose(self):
"""Return transpose of matrix.
Examples
========
>>> from sympy import MatrixSymbol, BlockMatrix, ZeroMatrix
>>> from sympy.abc import l, m, n
>>> X = MatrixSymbol('X', n, n)
>>> Y = MatrixSymbol('Y', m ,m)
>>> Z = MatrixSymbol('Z', n, m)
>>> B = BlockMatrix([[X, Z], [ZeroMatrix(m,n), Y]])
>>> B.transpose()
Matrix([
[X.T, 0],
[Z.T, Y.T]])
>>> _.transpose()
Matrix([
[X, Z],
[0, Y]])
"""
return self._eval_transpose()
def _entry(self, i, j, **kwargs):
# Find row entry
for row_block, numrows in enumerate(self.rowblocksizes):
if (i < numrows) != False:
break
else:
i -= numrows
for col_block, numcols in enumerate(self.colblocksizes):
if (j < numcols) != False:
break
else:
j -= numcols
return self.blocks[row_block, col_block][i, j]
@property
def is_Identity(self):
if self.blockshape[0] != self.blockshape[1]:
return False
for i in range(self.blockshape[0]):
for j in range(self.blockshape[1]):
if i==j and not self.blocks[i, j].is_Identity:
return False
if i!=j and not self.blocks[i, j].is_ZeroMatrix:
return False
return True
@property
def is_structurally_symmetric(self):
return self.rowblocksizes == self.colblocksizes
def equals(self, other):
if self == other:
return True
if (isinstance(other, BlockMatrix) and self.blocks == other.blocks):
return True
return super(BlockMatrix, self).equals(other)
class BlockDiagMatrix(BlockMatrix):
"""
A BlockDiagMatrix is a BlockMatrix with matrices only along the diagonal
>>> from sympy import MatrixSymbol, BlockDiagMatrix, symbols, Identity
>>> n, m, l = symbols('n m l')
>>> X = MatrixSymbol('X', n, n)
>>> Y = MatrixSymbol('Y', m ,m)
>>> BlockDiagMatrix(X, Y)
Matrix([
[X, 0],
[0, Y]])
See Also
========
sympy.matrices.common.diag
"""
def __new__(cls, *mats):
return Basic.__new__(BlockDiagMatrix, *mats)
@property
def diag(self):
return self.args
@property
def blocks(self):
from sympy.matrices.immutable import ImmutableDenseMatrix
mats = self.args
data = [[mats[i] if i == j else ZeroMatrix(mats[i].rows, mats[j].cols)
for j in range(len(mats))]
for i in range(len(mats))]
return ImmutableDenseMatrix(data)
@property
def shape(self):
return (sum(block.rows for block in self.args),
sum(block.cols for block in self.args))
@property
def blockshape(self):
n = len(self.args)
return (n, n)
@property
def rowblocksizes(self):
return [block.rows for block in self.args]
@property
def colblocksizes(self):
return [block.cols for block in self.args]
def _eval_inverse(self, expand='ignored'):
return BlockDiagMatrix(*[mat.inverse() for mat in self.args])
def _eval_transpose(self):
return BlockDiagMatrix(*[mat.transpose() for mat in self.args])
def _blockmul(self, other):
if (isinstance(other, BlockDiagMatrix) and
self.colblocksizes == other.rowblocksizes):
return BlockDiagMatrix(*[a*b for a, b in zip(self.args, other.args)])
else:
return BlockMatrix._blockmul(self, other)
def _blockadd(self, other):
if (isinstance(other, BlockDiagMatrix) and
self.blockshape == other.blockshape and
self.rowblocksizes == other.rowblocksizes and
self.colblocksizes == other.colblocksizes):
return BlockDiagMatrix(*[a + b for a, b in zip(self.args, other.args)])
else:
return BlockMatrix._blockadd(self, other)
def block_collapse(expr):
"""Evaluates a block matrix expression
>>> from sympy import MatrixSymbol, BlockMatrix, symbols, \
Identity, Matrix, ZeroMatrix, block_collapse
>>> n,m,l = symbols('n m l')
>>> X = MatrixSymbol('X', n, n)
>>> Y = MatrixSymbol('Y', m ,m)
>>> Z = MatrixSymbol('Z', n, m)
>>> B = BlockMatrix([[X, Z], [ZeroMatrix(m, n), Y]])
>>> print(B)
Matrix([
[X, Z],
[0, Y]])
>>> C = BlockMatrix([[Identity(n), Z]])
>>> print(C)
Matrix([[I, Z]])
>>> print(block_collapse(C*B))
Matrix([[X, Z + Z*Y]])
"""
from sympy.strategies.util import expr_fns
hasbm = lambda expr: isinstance(expr, MatrixExpr) and expr.has(BlockMatrix)
conditioned_rl = condition(
hasbm,
typed(
{MatAdd: do_one(bc_matadd, bc_block_plus_ident),
MatMul: do_one(bc_matmul, bc_dist),
MatPow: bc_matmul,
Transpose: bc_transpose,
Inverse: bc_inverse,
BlockMatrix: do_one(bc_unpack, deblock)}
)
)
rule = exhaust(
bottom_up(
exhaust(conditioned_rl),
fns=expr_fns
)
)
result = rule(expr)
doit = getattr(result, 'doit', None)
if doit is not None:
return doit()
else:
return result
def bc_unpack(expr):
if expr.blockshape == (1, 1):
return expr.blocks[0, 0]
return expr
def bc_matadd(expr):
args = sift(expr.args, lambda M: isinstance(M, BlockMatrix))
blocks = args[True]
if not blocks:
return expr
nonblocks = args[False]
block = blocks[0]
for b in blocks[1:]:
block = block._blockadd(b)
if nonblocks:
return MatAdd(*nonblocks) + block
else:
return block
def bc_block_plus_ident(expr):
idents = [arg for arg in expr.args if arg.is_Identity]
if not idents:
return expr
blocks = [arg for arg in expr.args if isinstance(arg, BlockMatrix)]
if (blocks and all(b.structurally_equal(blocks[0]) for b in blocks)
and blocks[0].is_structurally_symmetric):
block_id = BlockDiagMatrix(*[Identity(k)
for k in blocks[0].rowblocksizes])
return MatAdd(block_id * len(idents), *blocks).doit()
return expr
def bc_dist(expr):
""" Turn a*[X, Y] into [a*X, a*Y] """
factor, mat = expr.as_coeff_mmul()
if factor == 1:
return expr
unpacked = unpack(mat)
if isinstance(unpacked, BlockDiagMatrix):
B = unpacked.diag
new_B = [factor * mat for mat in B]
return BlockDiagMatrix(*new_B)
elif isinstance(unpacked, BlockMatrix):
B = unpacked.blocks
new_B = [
[factor * B[i, j] for j in range(B.cols)] for i in range(B.rows)]
return BlockMatrix(new_B)
return unpacked
def bc_matmul(expr):
if isinstance(expr, MatPow):
if expr.args[1].is_Integer:
factor, matrices = (1, [expr.args[0]]*expr.args[1])
else:
return expr
else:
factor, matrices = expr.as_coeff_matrices()
i = 0
while (i+1 < len(matrices)):
A, B = matrices[i:i+2]
if isinstance(A, BlockMatrix) and isinstance(B, BlockMatrix):
matrices[i] = A._blockmul(B)
matrices.pop(i+1)
elif isinstance(A, BlockMatrix):
matrices[i] = A._blockmul(BlockMatrix([[B]]))
matrices.pop(i+1)
elif isinstance(B, BlockMatrix):
matrices[i] = BlockMatrix([[A]])._blockmul(B)
matrices.pop(i+1)
else:
i+=1
return MatMul(factor, *matrices).doit()
def bc_transpose(expr):
collapse = block_collapse(expr.arg)
return collapse._eval_transpose()
def bc_inverse(expr):
if isinstance(expr.arg, BlockDiagMatrix):
return expr._eval_inverse()
expr2 = blockinverse_1x1(expr)
if expr != expr2:
return expr2
return blockinverse_2x2(Inverse(reblock_2x2(expr.arg)))
def blockinverse_1x1(expr):
if isinstance(expr.arg, BlockMatrix) and expr.arg.blockshape == (1, 1):
mat = Matrix([[expr.arg.blocks[0].inverse()]])
return BlockMatrix(mat)
return expr
def blockinverse_2x2(expr):
if isinstance(expr.arg, BlockMatrix) and expr.arg.blockshape == (2, 2):
# Cite: The Matrix Cookbook Section 9.1.3
[[A, B],
[C, D]] = expr.arg.blocks.tolist()
return BlockMatrix([[ (A - B*D.I*C).I, (-A).I*B*(D - C*A.I*B).I],
[-(D - C*A.I*B).I*C*A.I, (D - C*A.I*B).I]])
else:
return expr
def deblock(B):
""" Flatten a BlockMatrix of BlockMatrices """
if not isinstance(B, BlockMatrix) or not B.blocks.has(BlockMatrix):
return B
wrap = lambda x: x if isinstance(x, BlockMatrix) else BlockMatrix([[x]])
bb = B.blocks.applyfunc(wrap) # everything is a block
from sympy import Matrix
try:
MM = Matrix(0, sum(bb[0, i].blocks.shape[1] for i in range(bb.shape[1])), [])
for row in range(0, bb.shape[0]):
M = Matrix(bb[row, 0].blocks)
for col in range(1, bb.shape[1]):
M = M.row_join(bb[row, col].blocks)
MM = MM.col_join(M)
return BlockMatrix(MM)
except ShapeError:
return B
def reblock_2x2(B):
""" Reblock a BlockMatrix so that it has 2x2 blocks of block matrices """
if not isinstance(B, BlockMatrix) or not all(d > 2 for d in B.blocks.shape):
return B
BM = BlockMatrix # for brevity's sake
return BM([[ B.blocks[0, 0], BM(B.blocks[0, 1:])],
[BM(B.blocks[1:, 0]), BM(B.blocks[1:, 1:])]])
def bounds(sizes):
""" Convert sequence of numbers into pairs of low-high pairs
>>> from sympy.matrices.expressions.blockmatrix import bounds
>>> bounds((1, 10, 50))
[(0, 1), (1, 11), (11, 61)]
"""
low = 0
rv = []
for size in sizes:
rv.append((low, low + size))
low += size
return rv
def blockcut(expr, rowsizes, colsizes):
""" Cut a matrix expression into Blocks
>>> from sympy import ImmutableMatrix, blockcut
>>> M = ImmutableMatrix(4, 4, range(16))
>>> B = blockcut(M, (1, 3), (1, 3))
>>> type(B).__name__
'BlockMatrix'
>>> ImmutableMatrix(B.blocks[0, 1])
Matrix([[1, 2, 3]])
"""
rowbounds = bounds(rowsizes)
colbounds = bounds(colsizes)
return BlockMatrix([[MatrixSlice(expr, rowbound, colbound)
for colbound in colbounds]
for rowbound in rowbounds])
|
71a0b5696cbc3c3e69c5c104d2a887bc670bb1fbddcf26e0415a0a830d9be0b3 | from __future__ import print_function, division
from .matexpr import MatrixExpr
from sympy.core.function import FunctionClass, Lambda
from sympy.core.sympify import _sympify, sympify
from sympy.matrices import Matrix
from sympy.functions.elementary.complexes import re, im
class FunctionMatrix(MatrixExpr):
"""Represents a matrix using a function (``Lambda``) which gives
outputs according to the coordinates of each matrix entries.
Parameters
==========
rows : nonnegative integer. Can be symbolic.
cols : nonnegative integer. Can be symbolic.
lamda : Function, Lambda or str
If it is a SymPy ``Function`` or ``Lambda`` instance,
it should be able to accept two arguments which represents the
matrix coordinates.
If it is a pure string containing python ``lambda`` semantics,
it is interpreted by the SymPy parser and casted into a SymPy
``Lambda`` instance.
Examples
========
Creating a ``FunctionMatrix`` from ``Lambda``:
>>> from sympy import FunctionMatrix, symbols, Lambda, MatPow, Matrix
>>> i, j, n, m = symbols('i,j,n,m')
>>> FunctionMatrix(n, m, Lambda((i, j), i + j))
FunctionMatrix(n, m, Lambda((i, j), i + j))
Creating a ``FunctionMatrix`` from a sympy function:
>>> from sympy.functions import KroneckerDelta
>>> X = FunctionMatrix(3, 3, KroneckerDelta)
>>> X.as_explicit()
Matrix([
[1, 0, 0],
[0, 1, 0],
[0, 0, 1]])
Creating a ``FunctionMatrix`` from a sympy undefined function:
>>> from sympy.core.function import Function
>>> f = Function('f')
>>> X = FunctionMatrix(3, 3, f)
>>> X.as_explicit()
Matrix([
[f(0, 0), f(0, 1), f(0, 2)],
[f(1, 0), f(1, 1), f(1, 2)],
[f(2, 0), f(2, 1), f(2, 2)]])
Creating a ``FunctionMatrix`` from python ``lambda``:
>>> FunctionMatrix(n, m, 'lambda i, j: i + j')
FunctionMatrix(n, m, Lambda((i, j), i + j))
Example of lazy evaluation of matrix product:
>>> Y = FunctionMatrix(1000, 1000, Lambda((i, j), i + j))
>>> isinstance(Y*Y, MatPow) # this is an expression object
True
>>> (Y**2)[10,10] # So this is evaluated lazily
342923500
Notes
=====
This class provides an alternative way to represent an extremely
dense matrix with entries in some form of a sequence, in a most
sparse way.
"""
def __new__(cls, rows, cols, lamda):
rows, cols = _sympify(rows), _sympify(cols)
cls._check_dim(rows)
cls._check_dim(cols)
lamda = sympify(lamda)
if not isinstance(lamda, (FunctionClass, Lambda)):
raise ValueError(
"{} should be compatible with SymPy function classes."
.format(lamda))
if 2 not in lamda.nargs:
raise ValueError(
'{} should be able to accept 2 arguments.'.format(lamda))
return super(FunctionMatrix, cls).__new__(cls, rows, cols, lamda)
@property
def shape(self):
return self.args[0:2]
@property
def lamda(self):
return self.args[2]
def _entry(self, i, j, **kwargs):
return self.lamda(i, j)
def _eval_trace(self):
from sympy.matrices.expressions.trace import Trace
from sympy import Sum
return Trace(self).rewrite(Sum).doit()
def as_real_imag(self):
return (re(Matrix(self)), im(Matrix(self)))
|
2d777da1d35e96dba72465fd6272667c45a08c0bd5424bcd394bb4bca56db43b | from sympy.matrices.expressions.blockmatrix import (
block_collapse, bc_matmul, bc_block_plus_ident, BlockDiagMatrix,
BlockMatrix, bc_dist, bc_matadd, bc_transpose, bc_inverse,
blockcut, reblock_2x2, deblock)
from sympy.matrices.expressions import (MatrixSymbol, Identity,
Inverse, trace, Transpose, det)
from sympy.matrices import (
Matrix, ImmutableMatrix, ImmutableSparseMatrix)
from sympy.core import Tuple, symbols, Expr
from sympy.core.compatibility import range
from sympy.functions import transpose
i, j, k, l, m, n, p = symbols('i:n, p', integer=True)
A = MatrixSymbol('A', n, n)
B = MatrixSymbol('B', n, n)
C = MatrixSymbol('C', n, n)
D = MatrixSymbol('D', n, n)
G = MatrixSymbol('G', n, n)
H = MatrixSymbol('H', n, n)
b1 = BlockMatrix([[G, H]])
b2 = BlockMatrix([[G], [H]])
def test_bc_matmul():
assert bc_matmul(H*b1*b2*G) == BlockMatrix([[(H*G*G + H*H*H)*G]])
def test_bc_matadd():
assert bc_matadd(BlockMatrix([[G, H]]) + BlockMatrix([[H, H]])) == \
BlockMatrix([[G+H, H+H]])
def test_bc_transpose():
assert bc_transpose(Transpose(BlockMatrix([[A, B], [C, D]]))) == \
BlockMatrix([[A.T, C.T], [B.T, D.T]])
def test_bc_dist_diag():
A = MatrixSymbol('A', n, n)
B = MatrixSymbol('B', m, m)
C = MatrixSymbol('C', l, l)
X = BlockDiagMatrix(A, B, C)
assert bc_dist(X+X).equals(BlockDiagMatrix(2*A, 2*B, 2*C))
def test_block_plus_ident():
A = MatrixSymbol('A', n, n)
B = MatrixSymbol('B', n, m)
C = MatrixSymbol('C', m, n)
D = MatrixSymbol('D', m, m)
X = BlockMatrix([[A, B], [C, D]])
assert bc_block_plus_ident(X+Identity(m+n)) == \
BlockDiagMatrix(Identity(n), Identity(m)) + X
def test_BlockMatrix():
A = MatrixSymbol('A', n, m)
B = MatrixSymbol('B', n, k)
C = MatrixSymbol('C', l, m)
D = MatrixSymbol('D', l, k)
M = MatrixSymbol('M', m + k, p)
N = MatrixSymbol('N', l + n, k + m)
X = BlockMatrix(Matrix([[A, B], [C, D]]))
assert X.__class__(*X.args) == X
# block_collapse does nothing on normal inputs
E = MatrixSymbol('E', n, m)
assert block_collapse(A + 2*E) == A + 2*E
F = MatrixSymbol('F', m, m)
assert block_collapse(E.T*A*F) == E.T*A*F
assert X.shape == (l + n, k + m)
assert X.blockshape == (2, 2)
assert transpose(X) == BlockMatrix(Matrix([[A.T, C.T], [B.T, D.T]]))
assert transpose(X).shape == X.shape[::-1]
# Test that BlockMatrices and MatrixSymbols can still mix
assert (X*M).is_MatMul
assert X._blockmul(M).is_MatMul
assert (X*M).shape == (n + l, p)
assert (X + N).is_MatAdd
assert X._blockadd(N).is_MatAdd
assert (X + N).shape == X.shape
E = MatrixSymbol('E', m, 1)
F = MatrixSymbol('F', k, 1)
Y = BlockMatrix(Matrix([[E], [F]]))
assert (X*Y).shape == (l + n, 1)
assert block_collapse(X*Y).blocks[0, 0] == A*E + B*F
assert block_collapse(X*Y).blocks[1, 0] == C*E + D*F
# block_collapse passes down into container objects, transposes, and inverse
assert block_collapse(transpose(X*Y)) == transpose(block_collapse(X*Y))
assert block_collapse(Tuple(X*Y, 2*X)) == (
block_collapse(X*Y), block_collapse(2*X))
# Make sure that MatrixSymbols will enter 1x1 BlockMatrix if it simplifies
Ab = BlockMatrix([[A]])
Z = MatrixSymbol('Z', *A.shape)
assert block_collapse(Ab + Z) == A + Z
def test_block_collapse_explicit_matrices():
A = Matrix([[1, 2], [3, 4]])
assert block_collapse(BlockMatrix([[A]])) == A
A = ImmutableSparseMatrix([[1, 2], [3, 4]])
assert block_collapse(BlockMatrix([[A]])) == A
def test_BlockMatrix_trace():
A, B, C, D = [MatrixSymbol(s, 3, 3) for s in 'ABCD']
X = BlockMatrix([[A, B], [C, D]])
assert trace(X) == trace(A) + trace(D)
def test_BlockMatrix_Determinant():
A, B, C, D = [MatrixSymbol(s, 3, 3) for s in 'ABCD']
X = BlockMatrix([[A, B], [C, D]])
from sympy import assuming, Q
with assuming(Q.invertible(A)):
assert det(X) == det(A) * det(D - C*A.I*B)
assert isinstance(det(X), Expr)
def test_squareBlockMatrix():
A = MatrixSymbol('A', n, n)
B = MatrixSymbol('B', n, m)
C = MatrixSymbol('C', m, n)
D = MatrixSymbol('D', m, m)
X = BlockMatrix([[A, B], [C, D]])
Y = BlockMatrix([[A]])
assert X.is_square
Q = X + Identity(m + n)
assert (block_collapse(Q) ==
BlockMatrix([[A + Identity(n), B], [C, D + Identity(m)]]))
assert (X + MatrixSymbol('Q', n + m, n + m)).is_MatAdd
assert (X * MatrixSymbol('Q', n + m, n + m)).is_MatMul
assert block_collapse(Y.I) == A.I
assert block_collapse(X.inverse()) == BlockMatrix([
[(-B*D.I*C + A).I, -A.I*B*(D + -C*A.I*B).I],
[-(D - C*A.I*B).I*C*A.I, (D - C*A.I*B).I]])
assert isinstance(X.inverse(), Inverse)
assert not X.is_Identity
Z = BlockMatrix([[Identity(n), B], [C, D]])
assert not Z.is_Identity
def test_BlockDiagMatrix():
A = MatrixSymbol('A', n, n)
B = MatrixSymbol('B', m, m)
C = MatrixSymbol('C', l, l)
M = MatrixSymbol('M', n + m + l, n + m + l)
X = BlockDiagMatrix(A, B, C)
Y = BlockDiagMatrix(A, 2*B, 3*C)
assert X.blocks[1, 1] == B
assert X.shape == (n + m + l, n + m + l)
assert all(X.blocks[i, j].is_ZeroMatrix if i != j else X.blocks[i, j] in [A, B, C]
for i in range(3) for j in range(3))
assert X.__class__(*X.args) == X
assert isinstance(block_collapse(X.I * X), Identity)
assert bc_matmul(X*X) == BlockDiagMatrix(A*A, B*B, C*C)
assert block_collapse(X*X) == BlockDiagMatrix(A*A, B*B, C*C)
#XXX: should be == ??
assert block_collapse(X + X).equals(BlockDiagMatrix(2*A, 2*B, 2*C))
assert block_collapse(X*Y) == BlockDiagMatrix(A*A, 2*B*B, 3*C*C)
assert block_collapse(X + Y) == BlockDiagMatrix(2*A, 3*B, 4*C)
# Ensure that BlockDiagMatrices can still interact with normal MatrixExprs
assert (X*(2*M)).is_MatMul
assert (X + (2*M)).is_MatAdd
assert (X._blockmul(M)).is_MatMul
assert (X._blockadd(M)).is_MatAdd
def test_blockcut():
A = MatrixSymbol('A', n, m)
B = blockcut(A, (n/2, n/2), (m/2, m/2))
assert A[i, j] == B[i, j]
assert B == BlockMatrix([[A[:n/2, :m/2], A[:n/2, m/2:]],
[A[n/2:, :m/2], A[n/2:, m/2:]]])
M = ImmutableMatrix(4, 4, range(16))
B = blockcut(M, (2, 2), (2, 2))
assert M == ImmutableMatrix(B)
B = blockcut(M, (1, 3), (2, 2))
assert ImmutableMatrix(B.blocks[0, 1]) == ImmutableMatrix([[2, 3]])
def test_reblock_2x2():
B = BlockMatrix([[MatrixSymbol('A_%d%d'%(i,j), 2, 2)
for j in range(3)]
for i in range(3)])
assert B.blocks.shape == (3, 3)
BB = reblock_2x2(B)
assert BB.blocks.shape == (2, 2)
assert B.shape == BB.shape
assert B.as_explicit() == BB.as_explicit()
def test_deblock():
B = BlockMatrix([[MatrixSymbol('A_%d%d'%(i,j), n, n)
for j in range(4)]
for i in range(4)])
assert deblock(reblock_2x2(B)) == B
def test_block_collapse_type():
bm1 = BlockDiagMatrix(ImmutableMatrix([1]), ImmutableMatrix([2]))
bm2 = BlockDiagMatrix(ImmutableMatrix([3]), ImmutableMatrix([4]))
assert bm1.T.__class__ == BlockDiagMatrix
assert block_collapse(bm1 - bm2).__class__ == BlockDiagMatrix
assert block_collapse(Inverse(bm1)).__class__ == BlockDiagMatrix
assert block_collapse(Transpose(bm1)).__class__ == BlockDiagMatrix
assert bc_transpose(Transpose(bm1)).__class__ == BlockDiagMatrix
assert bc_inverse(Inverse(bm1)).__class__ == BlockDiagMatrix
|
94546f9a275c031ca4829d576dd05965bcc80b785236d431689e08272c90aee6 | from sympy.core import symbols, Lambda
from sympy.functions import KroneckerDelta
from sympy.matrices import Matrix
from sympy.matrices.expressions import FunctionMatrix, MatrixExpr, Identity
from sympy.utilities.pytest import raises
def test_funcmatrix_creation():
i, j, k = symbols('i j k')
assert FunctionMatrix(2, 2, Lambda((i, j), 0))
assert FunctionMatrix(0, 0, Lambda((i, j), 0))
raises(ValueError, lambda: FunctionMatrix(-1, 0, Lambda((i, j), 0)))
raises(ValueError, lambda: FunctionMatrix(2.0, 0, Lambda((i, j), 0)))
raises(ValueError, lambda: FunctionMatrix(2j, 0, Lambda((i, j), 0)))
raises(ValueError, lambda: FunctionMatrix(0, -1, Lambda((i, j), 0)))
raises(ValueError, lambda: FunctionMatrix(0, 2.0, Lambda((i, j), 0)))
raises(ValueError, lambda: FunctionMatrix(0, 2j, Lambda((i, j), 0)))
raises(ValueError, lambda: FunctionMatrix(2, 2, Lambda(i, 0)))
raises(ValueError, lambda: FunctionMatrix(2, 2, lambda i, j: 0))
raises(ValueError, lambda: FunctionMatrix(2, 2, Lambda((i,), 0)))
raises(ValueError, lambda: FunctionMatrix(2, 2, Lambda((i, j, k), 0)))
raises(ValueError, lambda: FunctionMatrix(2, 2, i+j))
assert FunctionMatrix(2, 2, "lambda i, j: 0") == \
FunctionMatrix(2, 2, Lambda((i, j), 0))
assert FunctionMatrix(2, 2, KroneckerDelta).as_explicit() == \
Identity(2).as_explicit()
n = symbols('n')
assert FunctionMatrix(n, n, Lambda((i, j), 0))
n = symbols('n', integer=False)
raises(ValueError, lambda: FunctionMatrix(n, n, Lambda((i, j), 0)))
n = symbols('n', negative=True)
raises(ValueError, lambda: FunctionMatrix(n, n, Lambda((i, j), 0)))
def test_funcmatrix():
i, j = symbols('i,j')
X = FunctionMatrix(3, 3, Lambda((i, j), i - j))
assert X[1, 1] == 0
assert X[1, 2] == -1
assert X.shape == (3, 3)
assert X.rows == X.cols == 3
assert Matrix(X) == Matrix(3, 3, lambda i, j: i - j)
assert isinstance(X*X + X, MatrixExpr)
|
a33ca6323b9cb74eda172a6523cb37efd0161f2c43fbb9ef590cdd782f6c6c85 | """
Some examples have been taken from:
http://www.math.uwaterloo.ca/~hwolkowi//matrixcookbook.pdf
"""
from sympy import (MatrixSymbol, Inverse, symbols, Determinant, Trace,
Derivative, sin, exp, cos, tan, log, S, sqrt,
hadamard_product, DiagonalizeVector, OneMatrix, HadamardProduct, HadamardPower, KroneckerDelta, Sum)
from sympy import MatAdd, Identity, MatMul, ZeroMatrix
from sympy.matrices.expressions import hadamard_power
k = symbols("k")
i, j = symbols("i j")
m, n = symbols("m n")
X = MatrixSymbol("X", k, k)
x = MatrixSymbol("x", k, 1)
y = MatrixSymbol("y", k, 1)
A = MatrixSymbol("A", k, k)
B = MatrixSymbol("B", k, k)
C = MatrixSymbol("C", k, k)
D = MatrixSymbol("D", k, k)
a = MatrixSymbol("a", k, 1)
b = MatrixSymbol("b", k, 1)
c = MatrixSymbol("c", k, 1)
d = MatrixSymbol("d", k, 1)
KDelta = lambda i, j: KroneckerDelta(i, j, (0, k-1))
def _check_derivative_with_explicit_matrix(expr, x, diffexpr, dim=2):
# TODO: this is commented because it slows down the tests.
return
expr = expr.xreplace({k: dim})
x = x.xreplace({k: dim})
diffexpr = diffexpr.xreplace({k: dim})
expr = expr.as_explicit()
x = x.as_explicit()
diffexpr = diffexpr.as_explicit()
assert expr.diff(x).reshape(*diffexpr.shape).tomatrix() == diffexpr
def test_matrix_derivative_by_scalar():
assert A.diff(i) == ZeroMatrix(k, k)
assert (A*(X + B)*c).diff(i) == ZeroMatrix(k, 1)
assert x.diff(i) == ZeroMatrix(k, 1)
assert (x.T*y).diff(i) == ZeroMatrix(1, 1)
assert (x*x.T).diff(i) == ZeroMatrix(k, k)
assert (x + y).diff(i) == ZeroMatrix(k, 1)
assert hadamard_power(x, 2).diff(i) == ZeroMatrix(k, 1)
assert hadamard_power(x, i).diff(i) == HadamardProduct(x.applyfunc(log), HadamardPower(x, i))
assert hadamard_product(x, y).diff(i) == ZeroMatrix(k, 1)
assert hadamard_product(i*OneMatrix(k, 1), x, y).diff(i) == hadamard_product(x, y)
assert (i*x).diff(i) == x
assert (sin(i)*A*B*x).diff(i) == cos(i)*A*B*x
assert x.applyfunc(sin).diff(i) == ZeroMatrix(k, 1)
assert Trace(i**2*X).diff(i) == 2*i*Trace(X)
mu = symbols("mu")
expr = (2*mu*x)
assert expr.diff(x) == 2*mu*Identity(k)
def test_matrix_derivative_non_matrix_result():
# This is a 4-dimensional array:
assert A.diff(A) == Derivative(A, A)
assert A.T.diff(A) == Derivative(A.T, A)
assert (2*A).diff(A) == Derivative(2*A, A)
assert MatAdd(A, A).diff(A) == Derivative(MatAdd(A, A), A)
assert (A + B).diff(A) == Derivative(A + B, A) # TODO: `B` can be removed.
def test_matrix_derivative_trivial_cases():
# Cookbook example 33:
# TODO: find a way to represent a four-dimensional zero-array:
assert X.diff(A) == Derivative(X, A)
def test_matrix_derivative_with_inverse():
# Cookbook example 61:
expr = a.T*Inverse(X)*b
assert expr.diff(X) == -Inverse(X).T*a*b.T*Inverse(X).T
# Cookbook example 62:
expr = Determinant(Inverse(X))
# Not implemented yet:
# assert expr.diff(X) == -Determinant(X.inv())*(X.inv()).T
# Cookbook example 63:
expr = Trace(A*Inverse(X)*B)
assert expr.diff(X) == -(X**(-1)*B*A*X**(-1)).T
# Cookbook example 64:
expr = Trace(Inverse(X + A))
assert expr.diff(X) == -(Inverse(X + A)).T**2
def test_matrix_derivative_vectors_and_scalars():
assert x.diff(x) == Identity(k)
assert x[i, 0].diff(x[m, 0]).doit() == KDelta(m, i)
assert x.T.diff(x) == Identity(k)
# Cookbook example 69:
expr = x.T*a
assert expr.diff(x) == a
assert expr[0, 0].diff(x[m, 0]).doit() == a[m, 0]
expr = a.T*x
assert expr.diff(x) == a
# Cookbook example 70:
expr = a.T*X*b
assert expr.diff(X) == a*b.T
# Cookbook example 71:
expr = a.T*X.T*b
assert expr.diff(X) == b*a.T
# Cookbook example 72:
expr = a.T*X*a
assert expr.diff(X) == a*a.T
expr = a.T*X.T*a
assert expr.diff(X) == a*a.T
# Cookbook example 77:
expr = b.T*X.T*X*c
assert expr.diff(X) == X*b*c.T + X*c*b.T
# Cookbook example 78:
expr = (B*x + b).T*C*(D*x + d)
assert expr.diff(x) == B.T*C*(D*x + d) + D.T*C.T*(B*x + b)
# Cookbook example 81:
expr = x.T*B*x
assert expr.diff(x) == B*x + B.T*x
# Cookbook example 82:
expr = b.T*X.T*D*X*c
assert expr.diff(X) == D.T*X*b*c.T + D*X*c*b.T
# Cookbook example 83:
expr = (X*b + c).T*D*(X*b + c)
assert expr.diff(X) == D*(X*b + c)*b.T + D.T*(X*b + c)*b.T
assert str(expr[0, 0].diff(X[m, n]).doit()) == \
'b[n, 0]*Sum((c[_i_1, 0] + Sum(X[_i_1, _i_3]*b[_i_3, 0], (_i_3, 0, k - 1)))*D[_i_1, m], (_i_1, 0, k - 1)) + Sum((c[_i_2, 0] + Sum(X[_i_2, _i_4]*b[_i_4, 0], (_i_4, 0, k - 1)))*D[m, _i_2]*b[n, 0], (_i_2, 0, k - 1))'
def test_matrix_derivatives_of_traces():
expr = Trace(A)*A
assert expr.diff(A) == Derivative(Trace(A)*A, A)
assert expr[i, j].diff(A[m, n]).doit() == (
KDelta(i, m)*KDelta(j, n)*Trace(A) +
KDelta(m, n)*A[i, j]
)
## First order:
# Cookbook example 99:
expr = Trace(X)
assert expr.diff(X) == Identity(k)
assert expr.rewrite(Sum).diff(X[m, n]).doit() == KDelta(m, n)
# Cookbook example 100:
expr = Trace(X*A)
assert expr.diff(X) == A.T
assert expr.rewrite(Sum).diff(X[m, n]).doit() == A[n, m]
# Cookbook example 101:
expr = Trace(A*X*B)
assert expr.diff(X) == A.T*B.T
assert expr.rewrite(Sum).diff(X[m, n]).doit().dummy_eq((A.T*B.T)[m, n])
# Cookbook example 102:
expr = Trace(A*X.T*B)
assert expr.diff(X) == B*A
# Cookbook example 103:
expr = Trace(X.T*A)
assert expr.diff(X) == A
# Cookbook example 104:
expr = Trace(A*X.T)
assert expr.diff(X) == A
# Cookbook example 105:
# TODO: TensorProduct is not supported
#expr = Trace(TensorProduct(A, X))
#assert expr.diff(X) == Trace(A)*Identity(k)
## Second order:
# Cookbook example 106:
expr = Trace(X**2)
assert expr.diff(X) == 2*X.T
# Cookbook example 107:
expr = Trace(X**2*B)
assert expr.diff(X) == (X*B + B*X).T
expr = Trace(MatMul(X, X, B))
assert expr.diff(X) == (X*B + B*X).T
# Cookbook example 108:
expr = Trace(X.T*B*X)
assert expr.diff(X) == B*X + B.T*X
# Cookbook example 109:
expr = Trace(B*X*X.T)
assert expr.diff(X) == B*X + B.T*X
# Cookbook example 110:
expr = Trace(X*X.T*B)
assert expr.diff(X) == B*X + B.T*X
# Cookbook example 111:
expr = Trace(X*B*X.T)
assert expr.diff(X) == X*B.T + X*B
# Cookbook example 112:
expr = Trace(B*X.T*X)
assert expr.diff(X) == X*B.T + X*B
# Cookbook example 113:
expr = Trace(X.T*X*B)
assert expr.diff(X) == X*B.T + X*B
# Cookbook example 114:
expr = Trace(A*X*B*X)
assert expr.diff(X) == A.T*X.T*B.T + B.T*X.T*A.T
# Cookbook example 115:
expr = Trace(X.T*X)
assert expr.diff(X) == 2*X
expr = Trace(X*X.T)
assert expr.diff(X) == 2*X
# Cookbook example 116:
expr = Trace(B.T*X.T*C*X*B)
assert expr.diff(X) == C.T*X*B*B.T + C*X*B*B.T
# Cookbook example 117:
expr = Trace(X.T*B*X*C)
assert expr.diff(X) == B*X*C + B.T*X*C.T
# Cookbook example 118:
expr = Trace(A*X*B*X.T*C)
assert expr.diff(X) == A.T*C.T*X*B.T + C*A*X*B
# Cookbook example 119:
expr = Trace((A*X*B + C)*(A*X*B + C).T)
assert expr.diff(X) == 2*A.T*(A*X*B + C)*B.T
# Cookbook example 120:
# TODO: no support for TensorProduct.
# expr = Trace(TensorProduct(X, X))
# expr = Trace(X)*Trace(X)
# expr.diff(X) == 2*Trace(X)*Identity(k)
# Higher Order
# Cookbook example 121:
expr = Trace(X**k)
#assert expr.diff(X) == k*(X**(k-1)).T
# Cookbook example 122:
expr = Trace(A*X**k)
#assert expr.diff(X) == # Needs indices
# Cookbook example 123:
expr = Trace(B.T*X.T*C*X*X.T*C*X*B)
assert expr.diff(X) == C*X*X.T*C*X*B*B.T + C.T*X*B*B.T*X.T*C.T*X + C*X*B*B.T*X.T*C*X + C.T*X*X.T*C.T*X*B*B.T
# Other
# Cookbook example 124:
expr = Trace(A*X**(-1)*B)
assert expr.diff(X) == -Inverse(X).T*A.T*B.T*Inverse(X).T
# Cookbook example 125:
expr = Trace(Inverse(X.T*C*X)*A)
# Warning: result in the cookbook is equivalent if B and C are symmetric:
assert expr.diff(X) == - X.inv().T*A.T*X.inv()*C.inv().T*X.inv().T - X.inv().T*A*X.inv()*C.inv()*X.inv().T
# Cookbook example 126:
expr = Trace((X.T*C*X).inv()*(X.T*B*X))
assert expr.diff(X) == -2*C*X*(X.T*C*X).inv()*X.T*B*X*(X.T*C*X).inv() + 2*B*X*(X.T*C*X).inv()
# Cookbook example 127:
expr = Trace((A + X.T*C*X).inv()*(X.T*B*X))
# Warning: result in the cookbook is equivalent if B and C are symmetric:
assert expr.diff(X) == B*X*Inverse(A + X.T*C*X) - C*X*Inverse(A + X.T*C*X)*X.T*B*X*Inverse(A + X.T*C*X) - C.T*X*Inverse(A.T + (C*X).T*X)*X.T*B.T*X*Inverse(A.T + (C*X).T*X) + B.T*X*Inverse(A.T + (C*X).T*X)
def test_derivatives_of_complicated_matrix_expr():
expr = a.T*(A*X*(X.T*B + X*A) + B.T*X.T*(a*b.T*(X*D*X.T + X*(X.T*B + A*X)*D*B - X.T*C.T*A)*B + B*(X*D.T + B*A*X*A.T - 3*X*D))*B + 42*X*B*X.T*A.T*(X + X.T))*b
result = (B*(B*A*X*A.T - 3*X*D + X*D.T) + a*b.T*(X*(A*X + X.T*B)*D*B + X*D*X.T - X.T*C.T*A)*B)*B*b*a.T*B.T + B**2*b*a.T*B.T*X.T*a*b.T*X*D + 42*A*X*B.T*X.T*a*b.T + B*D*B**3*b*a.T*B.T*X.T*a*b.T*X + B*b*a.T*A*X + 42*a*b.T*(X + X.T)*A*X*B.T + b*a.T*X*B*a*b.T*B.T**2*X*D.T + b*a.T*X*B*a*b.T*B.T**3*D.T*(B.T*X + X.T*A.T) + 42*b*a.T*X*B*X.T*A.T + 42*A.T*(X + X.T)*b*a.T*X*B + A.T*B.T**2*X*B*a*b.T*B.T*A + A.T*a*b.T*(A.T*X.T + B.T*X) + A.T*X.T*b*a.T*X*B*a*b.T*B.T**3*D.T + B.T*X*B*a*b.T*B.T*D - 3*B.T*X*B*a*b.T*B.T*D.T - C.T*A*B**2*b*a.T*B.T*X.T*a*b.T + X.T*A.T*a*b.T*A.T
assert expr.diff(X) == result
def test_mixed_deriv_mixed_expressions():
expr = 3*Trace(A)
assert expr.diff(A) == 3*Identity(k)
expr = k
deriv = expr.diff(A)
assert isinstance(deriv, ZeroMatrix)
assert deriv == ZeroMatrix(k, k)
expr = Trace(A)**2
assert expr.diff(A) == (2*Trace(A))*Identity(k)
expr = Trace(A)*A
# TODO: this is not yet supported:
assert expr.diff(A) == Derivative(expr, A)
expr = Trace(Trace(A)*A)
assert expr.diff(A) == (2*Trace(A))*Identity(k)
expr = Trace(Trace(Trace(A)*A)*A)
assert expr.diff(A) == (3*Trace(A)**2)*Identity(k)
def test_derivatives_matrix_norms():
expr = x.T*y
assert expr.diff(x) == y
assert expr[0, 0].diff(x[m, 0]).doit() == y[m, 0]
expr = (x.T*y)**S.Half
assert expr.diff(x) == y/(2*sqrt(x.T*y))
expr = (x.T*x)**S.Half
assert expr.diff(x) == x*(x.T*x)**(-S.Half)
expr = (c.T*a*x.T*b)**S.Half
assert expr.diff(x) == b/(2*sqrt(c.T*a*x.T*b))*c.T*a
expr = (c.T*a*x.T*b)**(S.One/3)
assert expr.diff(x) == b*(c.T*a*x.T*b)**(-2*S.One/3)*c.T*a/3
expr = (a.T*X*b)**S.Half
assert expr.diff(X) == a/(2*sqrt(a.T*X*b))*b.T
expr = d.T*x*(a.T*X*b)**S.Half*y.T*c
assert expr.diff(X) == a*x.T*d/(2*sqrt(a.T*X*b))*y.T*c*b.T
def test_derivatives_elementwise_applyfunc():
from sympy.matrices.expressions.diagonal import DiagonalizeVector
expr = x.applyfunc(tan)
assert expr.diff(x) == DiagonalizeVector(x.applyfunc(lambda x: tan(x)**2 + 1))
assert expr[i, 0].diff(x[m, 0]).doit() == (tan(x[i, 0])**2 + 1)*KDelta(i, m)
_check_derivative_with_explicit_matrix(expr, x, expr.diff(x))
expr = (i**2*x).applyfunc(sin)
assert expr.diff(i) == HadamardProduct((2*i)*x, (i**2*x).applyfunc(cos))
assert expr[i, 0].diff(i).doit() == 2*i*x[i, 0]*cos(i**2*x[i, 0])
_check_derivative_with_explicit_matrix(expr, i, expr.diff(i))
expr = (log(i)*A*B).applyfunc(sin)
assert expr.diff(i) == HadamardProduct(A*B/i, (log(i)*A*B).applyfunc(cos))
_check_derivative_with_explicit_matrix(expr, i, expr.diff(i))
expr = A*x.applyfunc(exp)
assert expr.diff(x) == DiagonalizeVector(x.applyfunc(exp))*A.T
_check_derivative_with_explicit_matrix(expr, x, expr.diff(x))
expr = x.T*A*x + k*y.applyfunc(sin).T*x
assert expr.diff(x) == A.T*x + A*x + k*y.applyfunc(sin)
_check_derivative_with_explicit_matrix(expr, x, expr.diff(x))
expr = x.applyfunc(sin).T*y
assert expr.diff(x) == DiagonalizeVector(x.applyfunc(cos))*y
_check_derivative_with_explicit_matrix(expr, x, expr.diff(x))
expr = (a.T * X * b).applyfunc(sin)
assert expr.diff(X) == a*(a.T*X*b).applyfunc(cos)*b.T
_check_derivative_with_explicit_matrix(expr, X, expr.diff(X))
expr = a.T * X.applyfunc(sin) * b
assert expr.diff(X) == DiagonalizeVector(a)*X.applyfunc(cos)*DiagonalizeVector(b)
_check_derivative_with_explicit_matrix(expr, X, expr.diff(X))
expr = a.T * (A*X*B).applyfunc(sin) * b
assert expr.diff(X) == A.T*DiagonalizeVector(a)*(A*X*B).applyfunc(cos)*DiagonalizeVector(b)*B.T
_check_derivative_with_explicit_matrix(expr, X, expr.diff(X))
expr = a.T * (A*X*b).applyfunc(sin) * b.T
# TODO: not implemented
#assert expr.diff(X) == ...
#_check_derivative_with_explicit_matrix(expr, X, expr.diff(X))
expr = a.T*A*X.applyfunc(sin)*B*b
assert expr.diff(X) == DiagonalizeVector(A.T*a)*X.applyfunc(cos)*DiagonalizeVector(B*b)
expr = a.T * (A*X.applyfunc(sin)*B).applyfunc(log) * b
# TODO: wrong
# assert expr.diff(X) == A.T*DiagonalizeVector(a)*(A*X.applyfunc(sin)*B).applyfunc(Lambda(k, 1/k))*DiagonalizeVector(b)*B.T
expr = a.T * (X.applyfunc(sin)).applyfunc(log) * b
# TODO: wrong
# assert expr.diff(X) == DiagonalizeVector(a)*X.applyfunc(sin).applyfunc(Lambda(k, 1/k))*DiagonalizeVector(b)
def test_derivatives_of_hadamard_expressions():
# Hadamard Product
expr = hadamard_product(a, x, b)
assert expr.diff(x) == DiagonalizeVector(hadamard_product(b, a))
expr = a.T*hadamard_product(A, X, B)*b
assert expr.diff(X) == DiagonalizeVector(a)*hadamard_product(B, A)*DiagonalizeVector(b)
# Hadamard Power
expr = hadamard_power(x, 2)
assert expr.diff(x).doit() == 2*DiagonalizeVector(x)
expr = hadamard_power(x.T, 2)
assert expr.diff(x).doit() == 2*DiagonalizeVector(x)
expr = hadamard_power(x, S.Half)
assert expr.diff(x) == S.Half*DiagonalizeVector(hadamard_power(x, -S.Half))
expr = hadamard_power(a.T*X*b, 2)
assert expr.diff(X) == 2*a*a.T*X*b*b.T
expr = hadamard_power(a.T*X*b, S.Half)
assert expr.diff(X) == a/2*hadamard_power(a.T*X*b, -S.Half)*b.T
|
64d4bd5fdf6d60791ba5da0a42903991d7f20d16f193249f7e8965d72d7feb8f | from sympy import (KroneckerDelta, diff, Piecewise, Sum, Dummy, factor,
expand, zeros, gcd_terms, Eq, Symbol)
from sympy.core import S, symbols, Add, Mul, SympifyError
from sympy.core.expr import unchanged
from sympy.core.compatibility import long
from sympy.functions import transpose, sin, cos, sqrt, cbrt, exp
from sympy.simplify import simplify
from sympy.matrices import (Identity, ImmutableMatrix, Inverse, MatAdd, MatMul,
MatPow, Matrix, MatrixExpr, MatrixSymbol, ShapeError, ZeroMatrix,
SparseMatrix, Transpose, Adjoint)
from sympy.matrices.expressions.matexpr import (MatrixElement,
GenericZeroMatrix, GenericIdentity, OneMatrix)
from sympy.utilities.pytest import raises, XFAIL
n, m, l, k, p = symbols('n m l k p', integer=True)
x = symbols('x')
A = MatrixSymbol('A', n, m)
B = MatrixSymbol('B', m, l)
C = MatrixSymbol('C', n, n)
D = MatrixSymbol('D', n, n)
E = MatrixSymbol('E', m, n)
w = MatrixSymbol('w', n, 1)
def test_matrix_symbol_creation():
assert MatrixSymbol('A', 2, 2)
assert MatrixSymbol('A', 0, 0)
raises(ValueError, lambda: MatrixSymbol('A', -1, 2))
raises(ValueError, lambda: MatrixSymbol('A', 2.0, 2))
raises(ValueError, lambda: MatrixSymbol('A', 2j, 2))
raises(ValueError, lambda: MatrixSymbol('A', 2, -1))
raises(ValueError, lambda: MatrixSymbol('A', 2, 2.0))
raises(ValueError, lambda: MatrixSymbol('A', 2, 2j))
n = symbols('n')
assert MatrixSymbol('A', n, n)
n = symbols('n', integer=False)
raises(ValueError, lambda: MatrixSymbol('A', n, n))
n = symbols('n', negative=True)
raises(ValueError, lambda: MatrixSymbol('A', n, n))
def test_zero_matrix_creation():
assert unchanged(ZeroMatrix, 2, 2)
assert unchanged(ZeroMatrix, 0, 0)
raises(ValueError, lambda: ZeroMatrix(-1, 2))
raises(ValueError, lambda: ZeroMatrix(2.0, 2))
raises(ValueError, lambda: ZeroMatrix(2j, 2))
raises(ValueError, lambda: ZeroMatrix(2, -1))
raises(ValueError, lambda: ZeroMatrix(2, 2.0))
raises(ValueError, lambda: ZeroMatrix(2, 2j))
n = symbols('n')
assert unchanged(ZeroMatrix, n, n)
n = symbols('n', integer=False)
raises(ValueError, lambda: ZeroMatrix(n, n))
n = symbols('n', negative=True)
raises(ValueError, lambda: ZeroMatrix(n, n))
def test_one_matrix_creation():
assert OneMatrix(2, 2)
assert OneMatrix(0, 0)
raises(ValueError, lambda: OneMatrix(-1, 2))
raises(ValueError, lambda: OneMatrix(2.0, 2))
raises(ValueError, lambda: OneMatrix(2j, 2))
raises(ValueError, lambda: OneMatrix(2, -1))
raises(ValueError, lambda: OneMatrix(2, 2.0))
raises(ValueError, lambda: OneMatrix(2, 2j))
n = symbols('n')
assert OneMatrix(n, n)
n = symbols('n', integer=False)
raises(ValueError, lambda: OneMatrix(n, n))
n = symbols('n', negative=True)
raises(ValueError, lambda: OneMatrix(n, n))
def test_identity_matrix_creation():
assert Identity(2)
assert Identity(0)
raises(ValueError, lambda: Identity(-1))
raises(ValueError, lambda: Identity(2.0))
raises(ValueError, lambda: Identity(2j))
n = symbols('n')
assert Identity(n)
n = symbols('n', integer=False)
raises(ValueError, lambda: Identity(n))
n = symbols('n', negative=True)
raises(ValueError, lambda: Identity(n))
def test_shape():
assert A.shape == (n, m)
assert (A*B).shape == (n, l)
raises(ShapeError, lambda: B*A)
def test_matexpr():
assert (x*A).shape == A.shape
assert (x*A).__class__ == MatMul
assert 2*A - A - A == ZeroMatrix(*A.shape)
assert (A*B).shape == (n, l)
def test_subs():
A = MatrixSymbol('A', n, m)
B = MatrixSymbol('B', m, l)
C = MatrixSymbol('C', m, l)
assert A.subs(n, m).shape == (m, m)
assert (A*B).subs(B, C) == A*C
assert (A*B).subs(l, n).is_square
def test_ZeroMatrix():
A = MatrixSymbol('A', n, m)
Z = ZeroMatrix(n, m)
assert A + Z == A
assert A*Z.T == ZeroMatrix(n, n)
assert Z*A.T == ZeroMatrix(n, n)
assert A - A == ZeroMatrix(*A.shape)
assert not Z
assert transpose(Z) == ZeroMatrix(m, n)
assert Z.conjugate() == Z
assert ZeroMatrix(n, n)**0 == Identity(n)
with raises(ShapeError):
Z**0
with raises(ShapeError):
Z**2
def test_ZeroMatrix_doit():
Znn = ZeroMatrix(Add(n, n, evaluate=False), n)
assert isinstance(Znn.rows, Add)
assert Znn.doit() == ZeroMatrix(2*n, n)
assert isinstance(Znn.doit().rows, Mul)
def test_OneMatrix():
A = MatrixSymbol('A', n, m)
a = MatrixSymbol('a', n, 1)
U = OneMatrix(n, m)
assert U.shape == (n, m)
assert isinstance(A + U, Add)
assert transpose(U) == OneMatrix(m, n)
assert U.conjugate() == U
assert OneMatrix(n, n) ** 0 == Identity(n)
with raises(ShapeError):
U ** 0
with raises(ShapeError):
U ** 2
with raises(ShapeError):
a + U
U = OneMatrix(n, n)
assert U[1, 2] == 1
U = OneMatrix(2, 3)
assert U.as_explicit() == ImmutableMatrix.ones(2, 3)
def test_OneMatrix_doit():
Unn = OneMatrix(Add(n, n, evaluate=False), n)
assert isinstance(Unn.rows, Add)
assert Unn.doit() == OneMatrix(2 * n, n)
assert isinstance(Unn.doit().rows, Mul)
def test_Identity():
A = MatrixSymbol('A', n, m)
i, j = symbols('i j')
In = Identity(n)
Im = Identity(m)
assert A*Im == A
assert In*A == A
assert transpose(In) == In
assert In.inverse() == In
assert In.conjugate() == In
assert In[i, j] != 0
assert Sum(In[i, j], (i, 0, n-1), (j, 0, n-1)).subs(n,3).doit() == 3
assert Sum(Sum(In[i, j], (i, 0, n-1)), (j, 0, n-1)).subs(n,3).doit() == 3
# If range exceeds the limit `(0, n-1)`, do not remove `Piecewise`:
expr = Sum(In[i, j], (i, 0, n-1))
assert expr.doit() == 1
expr = Sum(In[i, j], (i, 0, n-2))
assert expr.doit().dummy_eq(
Piecewise(
(1, (j >= 0) & (j <= n-2)),
(0, True)
)
)
expr = Sum(In[i, j], (i, 1, n-1))
assert expr.doit().dummy_eq(
Piecewise(
(1, (j >= 1) & (j <= n-1)),
(0, True)
)
)
def test_Identity_doit():
Inn = Identity(Add(n, n, evaluate=False))
assert isinstance(Inn.rows, Add)
assert Inn.doit() == Identity(2*n)
assert isinstance(Inn.doit().rows, Mul)
def test_addition():
A = MatrixSymbol('A', n, m)
B = MatrixSymbol('B', n, m)
assert isinstance(A + B, MatAdd)
assert (A + B).shape == A.shape
assert isinstance(A - A + 2*B, MatMul)
raises(ShapeError, lambda: A + B.T)
raises(TypeError, lambda: A + 1)
raises(TypeError, lambda: 5 + A)
raises(TypeError, lambda: 5 - A)
assert A + ZeroMatrix(n, m) - A == ZeroMatrix(n, m)
with raises(TypeError):
ZeroMatrix(n,m) + S(0)
def test_multiplication():
A = MatrixSymbol('A', n, m)
B = MatrixSymbol('B', m, l)
C = MatrixSymbol('C', n, n)
assert (2*A*B).shape == (n, l)
assert (A*0*B) == ZeroMatrix(n, l)
raises(ShapeError, lambda: B*A)
assert (2*A).shape == A.shape
assert A * ZeroMatrix(m, m) * B == ZeroMatrix(n, l)
assert C * Identity(n) * C.I == Identity(n)
assert B/2 == S.Half*B
raises(NotImplementedError, lambda: 2/B)
A = MatrixSymbol('A', n, n)
B = MatrixSymbol('B', n, n)
assert Identity(n) * (A + B) == A + B
assert A**2*A == A**3
assert A**2*(A.I)**3 == A.I
assert A**3*(A.I)**2 == A
def test_MatPow():
A = MatrixSymbol('A', n, n)
AA = MatPow(A, 2)
assert AA.exp == 2
assert AA.base == A
assert (A**n).exp == n
assert A**0 == Identity(n)
assert A**1 == A
assert A**2 == AA
assert A**-1 == Inverse(A)
assert (A**-1)**-1 == A
assert (A**2)**3 == A**6
assert A**S.Half == sqrt(A)
assert A**(S(1)/3) == cbrt(A)
raises(ShapeError, lambda: MatrixSymbol('B', 3, 2)**2)
def test_MatrixSymbol():
n, m, t = symbols('n,m,t')
X = MatrixSymbol('X', n, m)
assert X.shape == (n, m)
raises(TypeError, lambda: MatrixSymbol('X', n, m)(t)) # issue 5855
assert X.doit() == X
def test_dense_conversion():
X = MatrixSymbol('X', 2, 2)
assert ImmutableMatrix(X) == ImmutableMatrix(2, 2, lambda i, j: X[i, j])
assert Matrix(X) == Matrix(2, 2, lambda i, j: X[i, j])
def test_free_symbols():
assert (C*D).free_symbols == set((C, D))
def test_zero_matmul():
assert isinstance(S.Zero * MatrixSymbol('X', 2, 2), MatrixExpr)
def test_matadd_simplify():
A = MatrixSymbol('A', 1, 1)
assert simplify(MatAdd(A, ImmutableMatrix([[sin(x)**2 + cos(x)**2]]))) == \
MatAdd(A, Matrix([[1]]))
def test_matmul_simplify():
A = MatrixSymbol('A', 1, 1)
assert simplify(MatMul(A, ImmutableMatrix([[sin(x)**2 + cos(x)**2]]))) == \
MatMul(A, Matrix([[1]]))
def test_invariants():
A = MatrixSymbol('A', n, m)
B = MatrixSymbol('B', m, l)
X = MatrixSymbol('X', n, n)
objs = [Identity(n), ZeroMatrix(m, n), A, MatMul(A, B), MatAdd(A, A),
Transpose(A), Adjoint(A), Inverse(X), MatPow(X, 2), MatPow(X, -1),
MatPow(X, 0)]
for obj in objs:
assert obj == obj.__class__(*obj.args)
def test_indexing():
A = MatrixSymbol('A', n, m)
A[1, 2]
A[l, k]
A[l+1, k+1]
def test_single_indexing():
A = MatrixSymbol('A', 2, 3)
assert A[1] == A[0, 1]
assert A[long(1)] == A[0, 1]
assert A[3] == A[1, 0]
assert list(A[:2, :2]) == [A[0, 0], A[0, 1], A[1, 0], A[1, 1]]
raises(IndexError, lambda: A[6])
raises(IndexError, lambda: A[n])
B = MatrixSymbol('B', n, m)
raises(IndexError, lambda: B[1])
B = MatrixSymbol('B', n, 3)
assert B[3] == B[1, 0]
def test_MatrixElement_commutative():
assert A[0, 1]*A[1, 0] == A[1, 0]*A[0, 1]
def test_MatrixSymbol_determinant():
A = MatrixSymbol('A', 4, 4)
assert A.as_explicit().det() == A[0, 0]*A[1, 1]*A[2, 2]*A[3, 3] - \
A[0, 0]*A[1, 1]*A[2, 3]*A[3, 2] - A[0, 0]*A[1, 2]*A[2, 1]*A[3, 3] + \
A[0, 0]*A[1, 2]*A[2, 3]*A[3, 1] + A[0, 0]*A[1, 3]*A[2, 1]*A[3, 2] - \
A[0, 0]*A[1, 3]*A[2, 2]*A[3, 1] - A[0, 1]*A[1, 0]*A[2, 2]*A[3, 3] + \
A[0, 1]*A[1, 0]*A[2, 3]*A[3, 2] + A[0, 1]*A[1, 2]*A[2, 0]*A[3, 3] - \
A[0, 1]*A[1, 2]*A[2, 3]*A[3, 0] - A[0, 1]*A[1, 3]*A[2, 0]*A[3, 2] + \
A[0, 1]*A[1, 3]*A[2, 2]*A[3, 0] + A[0, 2]*A[1, 0]*A[2, 1]*A[3, 3] - \
A[0, 2]*A[1, 0]*A[2, 3]*A[3, 1] - A[0, 2]*A[1, 1]*A[2, 0]*A[3, 3] + \
A[0, 2]*A[1, 1]*A[2, 3]*A[3, 0] + A[0, 2]*A[1, 3]*A[2, 0]*A[3, 1] - \
A[0, 2]*A[1, 3]*A[2, 1]*A[3, 0] - A[0, 3]*A[1, 0]*A[2, 1]*A[3, 2] + \
A[0, 3]*A[1, 0]*A[2, 2]*A[3, 1] + A[0, 3]*A[1, 1]*A[2, 0]*A[3, 2] - \
A[0, 3]*A[1, 1]*A[2, 2]*A[3, 0] - A[0, 3]*A[1, 2]*A[2, 0]*A[3, 1] + \
A[0, 3]*A[1, 2]*A[2, 1]*A[3, 0]
def test_MatrixElement_diff():
assert (A[3, 0]*A[0, 0]).diff(A[0, 0]) == A[3, 0]
def test_MatrixElement_doit():
u = MatrixSymbol('u', 2, 1)
v = ImmutableMatrix([3, 5])
assert u[0, 0].subs(u, v).doit() == v[0, 0]
def test_identity_powers():
M = Identity(n)
assert MatPow(M, 3).doit() == M**3
assert M**n == M
assert MatPow(M, 0).doit() == M**2
assert M**-2 == M
assert MatPow(M, -2).doit() == M**0
N = Identity(3)
assert MatPow(N, 2).doit() == N**n
assert MatPow(N, 3).doit() == N
assert MatPow(N, -2).doit() == N**4
assert MatPow(N, 2).doit() == N**0
def test_Zero_power():
z1 = ZeroMatrix(n, n)
assert z1**4 == z1
raises(ValueError, lambda:z1**-2)
assert z1**0 == Identity(n)
assert MatPow(z1, 2).doit() == z1**2
raises(ValueError, lambda:MatPow(z1, -2).doit())
z2 = ZeroMatrix(3, 3)
assert MatPow(z2, 4).doit() == z2**4
raises(ValueError, lambda:z2**-3)
assert z2**3 == MatPow(z2, 3).doit()
assert z2**0 == Identity(3)
raises(ValueError, lambda:MatPow(z2, -1).doit())
def test_matrixelement_diff():
dexpr = diff((D*w)[k,0], w[p,0])
assert w[k, p].diff(w[k, p]) == 1
assert w[k, p].diff(w[0, 0]) == KroneckerDelta(0, k, (0, n-1))*KroneckerDelta(0, p, (0, 0))
_i_1 = Dummy("_i_1")
assert dexpr.dummy_eq(Sum(KroneckerDelta(_i_1, p, (0, n-1))*D[k, _i_1], (_i_1, 0, n - 1)))
assert dexpr.doit() == D[k, p]
def test_MatrixElement_with_values():
x, y, z, w = symbols("x y z w")
M = Matrix([[x, y], [z, w]])
i, j = symbols("i, j")
Mij = M[i, j]
assert isinstance(Mij, MatrixElement)
Ms = SparseMatrix([[2, 3], [4, 5]])
msij = Ms[i, j]
assert isinstance(msij, MatrixElement)
for oi, oj in [(0, 0), (0, 1), (1, 0), (1, 1)]:
assert Mij.subs({i: oi, j: oj}) == M[oi, oj]
assert msij.subs({i: oi, j: oj}) == Ms[oi, oj]
A = MatrixSymbol("A", 2, 2)
assert A[0, 0].subs(A, M) == x
assert A[i, j].subs(A, M) == M[i, j]
assert M[i, j].subs(M, A) == A[i, j]
assert isinstance(M[3*i - 2, j], MatrixElement)
assert M[3*i - 2, j].subs({i: 1, j: 0}) == M[1, 0]
assert isinstance(M[i, 0], MatrixElement)
assert M[i, 0].subs(i, 0) == M[0, 0]
assert M[0, i].subs(i, 1) == M[0, 1]
assert M[i, j].diff(x) == Matrix([[1, 0], [0, 0]])[i, j]
raises(ValueError, lambda: M[i, 2])
raises(ValueError, lambda: M[i, -1])
raises(ValueError, lambda: M[2, i])
raises(ValueError, lambda: M[-1, i])
def test_inv():
B = MatrixSymbol('B', 3, 3)
assert B.inv() == B**-1
@XFAIL
def test_factor_expand():
A = MatrixSymbol("A", n, n)
B = MatrixSymbol("B", n, n)
expr1 = (A + B)*(C + D)
expr2 = A*C + B*C + A*D + B*D
assert expr1 != expr2
assert expand(expr1) == expr2
assert factor(expr2) == expr1
expr = B**(-1)*(A**(-1)*B**(-1) - A**(-1)*C*B**(-1))**(-1)*A**(-1)
I = Identity(n)
# Ideally we get the first, but we at least don't want a wrong answer
assert factor(expr) in [I - C, B**-1*(A**-1*(I - C)*B**-1)**-1*A**-1]
def test_issue_2749():
A = MatrixSymbol("A", 5, 2)
assert (A.T * A).I.as_explicit() == Matrix([[(A.T * A).I[0, 0], (A.T * A).I[0, 1]], \
[(A.T * A).I[1, 0], (A.T * A).I[1, 1]]])
def test_issue_2750():
x = MatrixSymbol('x', 1, 1)
assert (x.T*x).as_explicit()**-1 == Matrix([[x[0, 0]**(-2)]])
def test_issue_7842():
A = MatrixSymbol('A', 3, 1)
B = MatrixSymbol('B', 2, 1)
assert Eq(A, B) == False
assert Eq(A[1,0], B[1, 0]).func is Eq
A = ZeroMatrix(2, 3)
B = ZeroMatrix(2, 3)
assert Eq(A, B) == True
def test_generic_zero_matrix():
z = GenericZeroMatrix()
A = MatrixSymbol("A", n, n)
assert z == z
assert z != A
assert A != z
assert z.is_ZeroMatrix
raises(TypeError, lambda: z.shape)
raises(TypeError, lambda: z.rows)
raises(TypeError, lambda: z.cols)
assert MatAdd() == z
assert MatAdd(z, A) == MatAdd(A)
# Make sure it is hashable
hash(z)
def test_generic_identity():
I = GenericIdentity()
A = MatrixSymbol("A", n, n)
assert I == I
assert I != A
assert A != I
assert I.is_Identity
assert I**-1 == I
raises(TypeError, lambda: I.shape)
raises(TypeError, lambda: I.rows)
raises(TypeError, lambda: I.cols)
assert MatMul() == I
assert MatMul(I, A) == MatMul(A)
# Make sure it is hashable
hash(I)
def test_MatMul_postprocessor():
z = zeros(2)
z1 = ZeroMatrix(2, 2)
assert Mul(0, z) == Mul(z, 0) in [z, z1]
M = Matrix([[1, 2], [3, 4]])
Mx = Matrix([[x, 2*x], [3*x, 4*x]])
assert Mul(x, M) == Mul(M, x) == Mx
A = MatrixSymbol("A", 2, 2)
assert Mul(A, M) == MatMul(A, M)
assert Mul(M, A) == MatMul(M, A)
# Scalars should be absorbed into constant matrices
a = Mul(x, M, A)
b = Mul(M, x, A)
c = Mul(M, A, x)
assert a == b == c == MatMul(Mx, A)
a = Mul(x, A, M)
b = Mul(A, x, M)
c = Mul(A, M, x)
assert a == b == c == MatMul(A, Mx)
assert Mul(M, M) == M**2
assert Mul(A, M, M) == MatMul(A, M**2)
assert Mul(M, M, A) == MatMul(M**2, A)
assert Mul(M, A, M) == MatMul(M, A, M)
assert Mul(A, x, M, M, x) == MatMul(A, Mx**2)
@XFAIL
def test_MatAdd_postprocessor_xfail():
# This is difficult to get working because of the way that Add processes
# its args.
z = zeros(2)
assert Add(z, S.NaN) == Add(S.NaN, z)
def test_MatAdd_postprocessor():
# Some of these are nonsensical, but we do not raise errors for Add
# because that breaks algorithms that want to replace matrices with dummy
# symbols.
z = zeros(2)
assert Add(0, z) == Add(z, 0) == z
a = Add(S.Infinity, z)
assert a == Add(z, S.Infinity)
assert isinstance(a, Add)
assert a.args == (S.Infinity, z)
a = Add(S.ComplexInfinity, z)
assert a == Add(z, S.ComplexInfinity)
assert isinstance(a, Add)
assert a.args == (S.ComplexInfinity, z)
a = Add(z, S.NaN)
# assert a == Add(S.NaN, z) # See the XFAIL above
assert isinstance(a, Add)
assert a.args == (S.NaN, z)
M = Matrix([[1, 2], [3, 4]])
a = Add(x, M)
assert a == Add(M, x)
assert isinstance(a, Add)
assert a.args == (x, M)
A = MatrixSymbol("A", 2, 2)
assert Add(A, M) == Add(M, A) == A + M
# Scalars should be absorbed into constant matrices (producing an error)
a = Add(x, M, A)
assert a == Add(M, x, A) == Add(M, A, x) == Add(x, A, M) == Add(A, x, M) == Add(A, M, x)
assert isinstance(a, Add)
assert a.args == (x, A + M)
assert Add(M, M) == 2*M
assert Add(M, A, M) == Add(M, M, A) == Add(A, M, M) == A + 2*M
a = Add(A, x, M, M, x)
assert isinstance(a, Add)
assert a.args == (2*x, A + 2*M)
def test_simplify_matrix_expressions():
# Various simplification functions
assert type(gcd_terms(C*D + D*C)) == MatAdd
a = gcd_terms(2*C*D + 4*D*C)
assert type(a) == MatMul
assert a.args == (2, (C*D + 2*D*C))
def test_exp():
A = MatrixSymbol('A', 2, 2)
B = MatrixSymbol('B', 2, 2)
expr1 = exp(A)*exp(B)
expr2 = exp(B)*exp(A)
assert expr1 != expr2
assert expr1 - expr2 != 0
assert not isinstance(expr1, exp)
assert not isinstance(expr2, exp)
def test_invalid_args():
raises(SympifyError, lambda: MatrixSymbol(1, 2, 'A'))
def test_matrixsymbol_from_symbol():
# The label should be preserved during doit and subs
A_label = Symbol('A', complex=True)
A = MatrixSymbol(A_label, 2, 2)
A_1 = A.doit()
A_2 = A.subs(2, 3)
assert A_1.args == A.args
assert A_2.args[0] == A.args[0]
|
1c93622788443c0bf180cf52120fbee1fe888bd99c2a4ee06c9a1a85302475fc | from sympy.matrices.expressions.factorizations import lu, LofCholesky, qr, svd
from sympy import Symbol, MatrixSymbol, ask, Q
n = Symbol('n')
X = MatrixSymbol('X', n, n)
def test_LU():
L, U = lu(X)
assert L.shape == U.shape == X.shape
assert ask(Q.lower_triangular(L))
assert ask(Q.upper_triangular(U))
def test_Cholesky():
LofCholesky(X)
def test_QR():
Q_, R = qr(X)
assert Q_.shape == R.shape == X.shape
assert ask(Q.orthogonal(Q_))
assert ask(Q.upper_triangular(R))
def test_svd():
U, S, V = svd(X)
assert U.shape == S.shape == V.shape == X.shape
assert ask(Q.orthogonal(U))
assert ask(Q.orthogonal(V))
assert ask(Q.diagonal(S))
|
53d7f52f126a8445c087cc97cd93794ca691c0a47d9ad47bf9323563aff05101 | from sympy import (symbols, MatrixSymbol, MatPow, BlockMatrix, KroneckerDelta,
Identity, ZeroMatrix, ImmutableMatrix, eye, Sum, Dummy, trace,
Symbol)
from sympy.utilities.pytest import raises
from sympy.matrices.expressions.matexpr import MatrixElement, MatrixExpr
k, l, m, n = symbols('k l m n', integer=True)
i, j = symbols('i j', integer=True)
W = MatrixSymbol('W', k, l)
X = MatrixSymbol('X', l, m)
Y = MatrixSymbol('Y', l, m)
Z = MatrixSymbol('Z', m, n)
X1 = MatrixSymbol('X1', m, m)
X2 = MatrixSymbol('X2', m, m)
X3 = MatrixSymbol('X3', m, m)
X4 = MatrixSymbol('X4', m, m)
A = MatrixSymbol('A', 2, 2)
B = MatrixSymbol('B', 2, 2)
x = MatrixSymbol('x', 1, 2)
y = MatrixSymbol('x', 2, 1)
def test_symbolic_indexing():
x12 = X[1, 2]
assert all(s in str(x12) for s in ['1', '2', X.name])
# We don't care about the exact form of this. We do want to make sure
# that all of these features are present
def test_add_index():
assert (X + Y)[i, j] == X[i, j] + Y[i, j]
def test_mul_index():
assert (A*y)[0, 0] == A[0, 0]*y[0, 0] + A[0, 1]*y[1, 0]
assert (A*B).as_mutable() == (A.as_mutable() * B.as_mutable())
X = MatrixSymbol('X', n, m)
Y = MatrixSymbol('Y', m, k)
result = (X*Y)[4,2]
expected = Sum(X[4, i]*Y[i, 2], (i, 0, m - 1))
assert result.args[0].dummy_eq(expected.args[0], i)
assert result.args[1][1:] == expected.args[1][1:]
def test_pow_index():
Q = MatPow(A, 2)
assert Q[0, 0] == A[0, 0]**2 + A[0, 1]*A[1, 0]
n = symbols("n")
Q2 = A**n
assert Q2[0, 0] == MatrixElement(Q2, 0, 0)
def test_transpose_index():
assert X.T[i, j] == X[j, i]
def test_Identity_index():
I = Identity(3)
assert I[0, 0] == I[1, 1] == I[2, 2] == 1
assert I[1, 0] == I[0, 1] == I[2, 1] == 0
assert I[i, 0].delta_range == (0, 2)
raises(IndexError, lambda: I[3, 3])
def test_block_index():
I = Identity(3)
Z = ZeroMatrix(3, 3)
B = BlockMatrix([[I, I], [I, I]])
e3 = ImmutableMatrix(eye(3))
BB = BlockMatrix([[e3, e3], [e3, e3]])
assert B[0, 0] == B[3, 0] == B[0, 3] == B[3, 3] == 1
assert B[4, 3] == B[5, 1] == 0
BB = BlockMatrix([[e3, e3], [e3, e3]])
assert B.as_explicit() == BB.as_explicit()
BI = BlockMatrix([[I, Z], [Z, I]])
assert BI.as_explicit().equals(eye(6))
def test_slicing():
A.as_explicit()[0, :] # does not raise an error
def test_errors():
raises(IndexError, lambda: Identity(2)[1, 2, 3, 4, 5])
raises(IndexError, lambda: Identity(2)[[1, 2, 3, 4, 5]])
def test_matrix_expression_to_indices():
i, j = symbols("i, j")
i1, i2, i3 = symbols("i_1:4")
def replace_dummies(expr):
repl = {i: Symbol(i.name) for i in expr.atoms(Dummy)}
return expr.xreplace(repl)
expr = W*X*Z
assert replace_dummies(expr._entry(i, j)) == \
Sum(W[i, i1]*X[i1, i2]*Z[i2, j], (i1, 0, l-1), (i2, 0, m-1))
assert MatrixExpr.from_index_summation(expr._entry(i, j)) == expr
expr = Z.T*X.T*W.T
assert replace_dummies(expr._entry(i, j)) == \
Sum(W[j, i2]*X[i2, i1]*Z[i1, i], (i1, 0, m-1), (i2, 0, l-1))
assert MatrixExpr.from_index_summation(expr._entry(i, j), i) == expr
expr = W*X*Z + W*Y*Z
assert replace_dummies(expr._entry(i, j)) == \
Sum(W[i, i1]*X[i1, i2]*Z[i2, j], (i1, 0, l-1), (i2, 0, m-1)) +\
Sum(W[i, i1]*Y[i1, i2]*Z[i2, j], (i1, 0, l-1), (i2, 0, m-1))
assert MatrixExpr.from_index_summation(expr._entry(i, j)) == expr
expr = 2*W*X*Z + 3*W*Y*Z
assert replace_dummies(expr._entry(i, j)) == \
2*Sum(W[i, i1]*X[i1, i2]*Z[i2, j], (i1, 0, l-1), (i2, 0, m-1)) +\
3*Sum(W[i, i1]*Y[i1, i2]*Z[i2, j], (i1, 0, l-1), (i2, 0, m-1))
assert MatrixExpr.from_index_summation(expr._entry(i, j)) == expr
expr = W*(X + Y)*Z
assert replace_dummies(expr._entry(i, j)) == \
Sum(W[i, i1]*(X[i1, i2] + Y[i1, i2])*Z[i2, j], (i1, 0, l-1), (i2, 0, m-1))
assert MatrixExpr.from_index_summation(expr._entry(i, j)) == expr
expr = A*B**2*A
#assert replace_dummies(expr._entry(i, j)) == \
# Sum(A[i, i1]*B[i1, i2]*B[i2, i3]*A[i3, j], (i1, 0, 1), (i2, 0, 1), (i3, 0, 1))
# Check that different dummies are used in sub-multiplications:
expr = (X1*X2 + X2*X1)*X3
assert replace_dummies(expr._entry(i, j)) == \
Sum((Sum(X1[i, i2] * X2[i2, i1], (i2, 0, m - 1)) + Sum(X1[i3, i1] * X2[i, i3], (i3, 0, m - 1))) * X3[
i1, j], (i1, 0, m - 1))
def test_matrix_expression_from_index_summation():
from sympy.abc import a,b,c,d
A = MatrixSymbol("A", k, k)
B = MatrixSymbol("B", k, k)
C = MatrixSymbol("C", k, k)
w1 = MatrixSymbol("w1", k, 1)
i0, i1, i2, i3, i4 = symbols("i0:5", cls=Dummy)
expr = Sum(W[a,b]*X[b,c]*Z[c,d], (b, 0, l-1), (c, 0, m-1))
assert MatrixExpr.from_index_summation(expr, a) == W*X*Z
expr = Sum(W.T[b,a]*X[b,c]*Z[c,d], (b, 0, l-1), (c, 0, m-1))
assert MatrixExpr.from_index_summation(expr, a) == W*X*Z
expr = Sum(A[b, a]*B[b, c]*C[c, d], (b, 0, k-1), (c, 0, k-1))
assert MatrixSymbol.from_index_summation(expr, a) == A.T*B*C
expr = Sum(A[b, a]*B[c, b]*C[c, d], (b, 0, k-1), (c, 0, k-1))
assert MatrixSymbol.from_index_summation(expr, a) == A.T*B.T*C
expr = Sum(C[c, d]*A[b, a]*B[c, b], (b, 0, k-1), (c, 0, k-1))
assert MatrixSymbol.from_index_summation(expr, a) == A.T*B.T*C
expr = Sum(A[a, b] + B[a, b], (a, 0, k-1), (b, 0, k-1))
assert MatrixExpr.from_index_summation(expr, a) == A + B
expr = Sum((A[a, b] + B[a, b])*C[b, c], (b, 0, k-1))
assert MatrixExpr.from_index_summation(expr, a) == (A+B)*C
expr = Sum((A[a, b] + B[b, a])*C[b, c], (b, 0, k-1))
assert MatrixExpr.from_index_summation(expr, a) == (A+B.T)*C
expr = Sum(A[a, b]*A[b, c]*A[c, d], (b, 0, k-1), (c, 0, k-1))
assert MatrixExpr.from_index_summation(expr, a) == A**3
expr = Sum(A[a, b]*A[b, c]*B[c, d], (b, 0, k-1), (c, 0, k-1))
assert MatrixExpr.from_index_summation(expr, a) == A**2*B
# Parse the trace of a matrix:
expr = Sum(A[a, a], (a, 0, k-1))
assert MatrixExpr.from_index_summation(expr, None) == trace(A)
expr = Sum(A[a, a]*B[b, c]*C[c, d], (a, 0, k-1), (c, 0, k-1))
assert MatrixExpr.from_index_summation(expr, b) == trace(A)*B*C
# Check wrong sum ranges (should raise an exception):
## Case 1: 0 to m instead of 0 to m-1
expr = Sum(W[a,b]*X[b,c]*Z[c,d], (b, 0, l-1), (c, 0, m))
raises(ValueError, lambda: MatrixExpr.from_index_summation(expr, a))
## Case 2: 1 to m-1 instead of 0 to m-1
expr = Sum(W[a,b]*X[b,c]*Z[c,d], (b, 0, l-1), (c, 1, m-1))
raises(ValueError, lambda: MatrixExpr.from_index_summation(expr, a))
# Parse nested sums:
expr = Sum(A[a, b]*Sum(B[b, c]*C[c, d], (c, 0, k-1)), (b, 0, k-1))
assert MatrixExpr.from_index_summation(expr, a) == A*B*C
# Test Kronecker delta:
expr = Sum(A[a, b]*KroneckerDelta(b, c)*B[c, d], (b, 0, k-1), (c, 0, k-1))
assert MatrixExpr.from_index_summation(expr, a) == A*B
expr = Sum(KroneckerDelta(i1, m)*KroneckerDelta(i2, n)*A[i, i1]*A[j, i2], (i1, 0, k-1), (i2, 0, k-1))
assert MatrixExpr.from_index_summation(expr, m) == A.T*A[j, n]
# Test numbered indices:
expr = Sum(A[i1, i2]*w1[i2, 0], (i2, 0, k-1))
assert MatrixExpr.from_index_summation(expr, i1) == A*w1
expr = Sum(A[i1, i2]*B[i2, 0], (i2, 0, k-1))
assert MatrixExpr.from_index_summation(expr, i1) == MatrixElement(A*B, i1, 0)
|
b18a3f4496feda493d624b093e6b9a4a3757402cf1018832e50e17870c3cd915 | from sympy import S, I, ask, Q, Abs, simplify, exp, sqrt
from sympy.core.symbol import symbols
from sympy.matrices.expressions.fourier import DFT, IDFT
from sympy.matrices import det, Matrix, Identity
from sympy.utilities.pytest import raises
def test_dft_creation():
assert DFT(2)
assert DFT(0)
raises(ValueError, lambda: DFT(-1))
raises(ValueError, lambda: DFT(2.0))
raises(ValueError, lambda: DFT(2 + 1j))
n = symbols('n')
assert DFT(n)
n = symbols('n', integer=False)
raises(ValueError, lambda: DFT(n))
n = symbols('n', negative=True)
raises(ValueError, lambda: DFT(n))
def test_dft():
n, i, j = symbols('n i j')
assert DFT(4).shape == (4, 4)
assert ask(Q.unitary(DFT(4)))
assert Abs(simplify(det(Matrix(DFT(4))))) == 1
assert DFT(n)*IDFT(n) == Identity(n)
assert DFT(n)[i, j] == exp(-2*S.Pi*I/n)**(i*j) / sqrt(n)
|
88357ccf4675565f64b5a151b52af6745440411f97da2a49c8c08ecff470da85 | from sympy.matrices.expressions import MatrixSymbol
from sympy.matrices.expressions.diagonal import DiagonalMatrix, DiagonalOf, DiagonalizeVector, diagonalize_vector
from sympy import Symbol, ask, Q, KroneckerDelta, Identity, Matrix, MatMul
from sympy.utilities.pytest import raises
n = Symbol('n')
m = Symbol('m')
def test_DiagonalMatrix():
x = MatrixSymbol('x', n, m)
D = DiagonalMatrix(x)
assert D.diagonal_length is None
assert D.shape == (n, m)
x = MatrixSymbol('x', n, n)
D = DiagonalMatrix(x)
assert D.diagonal_length == n
assert D.shape == (n, n)
assert D[1, 2] == 0
assert D[1, 1] == x[1, 1]
i = Symbol('i')
j = Symbol('j')
x = MatrixSymbol('x', 3, 3)
ij = DiagonalMatrix(x)[i, j]
assert ij != 0
assert ij.subs({i:0, j:0}) == x[0, 0]
assert ij.subs({i:0, j:1}) == 0
assert ij.subs({i:1, j:1}) == x[1, 1]
assert ask(Q.diagonal(D)) # affirm that D is diagonal
x = MatrixSymbol('x', n, 3)
D = DiagonalMatrix(x)
assert D.diagonal_length == 3
assert D.shape == (n, 3)
assert D[2, m] == KroneckerDelta(2, m)*x[2, m]
assert D[3, m] == 0
raises(IndexError, lambda: D[m, 3])
x = MatrixSymbol('x', 3, n)
D = DiagonalMatrix(x)
assert D.diagonal_length == 3
assert D.shape == (3, n)
assert D[m, 2] == KroneckerDelta(m, 2)*x[m, 2]
assert D[m, 3] == 0
raises(IndexError, lambda: D[3, m])
x = MatrixSymbol('x', n, m)
D = DiagonalMatrix(x)
assert D.diagonal_length is None
assert D.shape == (n, m)
assert D[m, 4] != 0
x = MatrixSymbol('x', 3, 4)
assert [DiagonalMatrix(x)[i] for i in range(12)] == [
x[0, 0], 0, 0, 0, 0, x[1, 1], 0, 0, 0, 0, x[2, 2], 0]
# shape is retained, issue 12427
assert (
DiagonalMatrix(MatrixSymbol('x', 3, 4))*
DiagonalMatrix(MatrixSymbol('x', 4, 2))).shape == (3, 2)
def test_DiagonalOf():
x = MatrixSymbol('x', n, n)
d = DiagonalOf(x)
assert d.shape == (n, 1)
assert d.diagonal_length == n
assert d[2, 0] == d[2] == x[2, 2]
x = MatrixSymbol('x', n, m)
d = DiagonalOf(x)
assert d.shape == (None, 1)
assert d.diagonal_length is None
assert d[2, 0] == d[2] == x[2, 2]
d = DiagonalOf(MatrixSymbol('x', 4, 3))
assert d.shape == (3, 1)
d = DiagonalOf(MatrixSymbol('x', n, 3))
assert d.shape == (3, 1)
d = DiagonalOf(MatrixSymbol('x', 3, n))
assert d.shape == (3, 1)
x = MatrixSymbol('x', n, m)
assert [DiagonalOf(x)[i] for i in range(4)] ==[
x[0, 0], x[1, 1], x[2, 2], x[3, 3]]
def test_DiagonalizeVector():
x = MatrixSymbol('x', n, 1)
d = DiagonalizeVector(x)
assert d.shape == (n, n)
assert d[0, 1] == 0
assert d[0, 0] == x[0, 0]
a = MatrixSymbol('a', 1, 1)
d = diagonalize_vector(a)
assert isinstance(d, MatrixSymbol)
assert a == d
assert diagonalize_vector(Identity(3)) == Identity(3)
assert DiagonalizeVector(Identity(3)).doit() == Identity(3)
assert isinstance(DiagonalizeVector(Identity(3)), DiagonalizeVector)
# A diagonal matrix is equal to its transpose:
assert DiagonalizeVector(x).T == DiagonalizeVector(x)
assert diagonalize_vector(x.T) == DiagonalizeVector(x)
dx = DiagonalizeVector(x)
assert dx[0, 0] == x[0, 0]
assert dx[1, 1] == x[1, 0]
assert dx[0, 1] == 0
assert dx[0, m] == x[0, 0]*KroneckerDelta(0, m)
z = MatrixSymbol('z', 1, n)
dz = DiagonalizeVector(z)
assert dz[0, 0] == z[0, 0]
assert dz[1, 1] == z[0, 1]
assert dz[0, 1] == 0
assert dz[0, m] == z[0, m]*KroneckerDelta(0, m)
v = MatrixSymbol('v', 3, 1)
dv = DiagonalizeVector(v)
assert dv.as_explicit() == Matrix([
[v[0, 0], 0, 0],
[0, v[1, 0], 0],
[0, 0, v[2, 0]],
])
v = MatrixSymbol('v', 1, 3)
dv = DiagonalizeVector(v)
assert dv.as_explicit() == Matrix([
[v[0, 0], 0, 0],
[0, v[0, 1], 0],
[0, 0, v[0, 2]],
])
dv = DiagonalizeVector(3*v)
assert dv.args == (3*v,)
assert dv.doit() == 3*DiagonalizeVector(v)
assert isinstance(dv.doit(), MatMul)
a = MatrixSymbol("a", 3, 1).as_explicit()
expr = DiagonalizeVector(a)
result = Matrix([
[a[0, 0], 0, 0],
[0, a[1, 0], 0],
[0, 0, a[2, 0]],
])
assert expr.doit() == result
expr = DiagonalizeVector(a.T)
assert expr.doit() == result
|
658c7571c5431d0af54a4c615bbd2338d0db3fb3de9a6670c7e80666252b6536 | from sympy.matrices.expressions.applyfunc import ElementwiseApplyFunction
from sympy import (Matrix, Lambda, MatrixSymbol, exp, symbols, MatMul, sin, simplify)
from sympy.utilities.pytest import raises
from sympy.matrices.common import ShapeError
X = MatrixSymbol("X", 3, 3)
Y = MatrixSymbol("Y", 3, 3)
k = symbols("k")
Xk = MatrixSymbol("X", k, k)
Xd = X.as_explicit()
x, y, z, t = symbols("x y z t")
def test_applyfunc_matrix():
double = Lambda(x, x**2)
expr = ElementwiseApplyFunction(double, Xd)
assert isinstance(expr, ElementwiseApplyFunction)
assert expr.doit() == Xd.applyfunc(lambda x: x**2)
assert expr.shape == (3, 3)
assert expr.func(*expr.args) == expr
assert simplify(expr) == expr
assert expr[0, 0] == double(Xd[0, 0])
expr = ElementwiseApplyFunction(double, X)
assert isinstance(expr, ElementwiseApplyFunction)
assert isinstance(expr.doit(), ElementwiseApplyFunction)
assert expr == X.applyfunc(double)
assert expr.func(*expr.args) == expr
expr = ElementwiseApplyFunction(exp, X*Y)
assert expr.expr == X*Y
assert expr.function == exp
assert expr == (X*Y).applyfunc(exp)
assert expr.func(*expr.args) == expr
assert isinstance(X*expr, MatMul)
assert (X*expr).shape == (3, 3)
Z = MatrixSymbol("Z", 2, 3)
assert (Z*expr).shape == (2, 3)
expr = ElementwiseApplyFunction(exp, Z.T)*ElementwiseApplyFunction(exp, Z)
assert expr.shape == (3, 3)
expr = ElementwiseApplyFunction(exp, Z)*ElementwiseApplyFunction(exp, Z.T)
assert expr.shape == (2, 2)
raises(ShapeError, lambda: ElementwiseApplyFunction(exp, Z)*ElementwiseApplyFunction(exp, Z))
M = Matrix([[x, y], [z, t]])
expr = ElementwiseApplyFunction(sin, M)
assert isinstance(expr, ElementwiseApplyFunction)
assert expr.function == sin
assert expr.expr == M
assert expr.doit() == M.applyfunc(sin)
assert expr.doit() == Matrix([[sin(x), sin(y)], [sin(z), sin(t)]])
assert expr.func(*expr.args) == expr
expr = ElementwiseApplyFunction(double, Xk)
assert expr.doit() == expr
assert expr.subs(k, 2).shape == (2, 2)
assert (expr*expr).shape == (k, k)
M = MatrixSymbol("M", k, t)
expr2 = M.T*expr*M
assert isinstance(expr2, MatMul)
assert expr2.args[1] == expr
assert expr2.shape == (t, t)
expr3 = expr*M
assert expr3.shape == (k, t)
raises(ShapeError, lambda: M*expr)
expr1 = ElementwiseApplyFunction(lambda x: x+1, Xk)
expr2 = ElementwiseApplyFunction(lambda x: x, Xk)
assert expr1 != expr2
def test_applyfunc_entry():
af = X.applyfunc(sin)
assert af[0, 0] == sin(X[0, 0])
af = Xd.applyfunc(sin)
assert af[0, 0] == sin(X[0, 0])
def test_applyfunc_as_explicit():
af = X.applyfunc(sin)
assert af.as_explicit() == Matrix([
[sin(X[0, 0]), sin(X[0, 1]), sin(X[0, 2])],
[sin(X[1, 0]), sin(X[1, 1]), sin(X[1, 2])],
[sin(X[2, 0]), sin(X[2, 1]), sin(X[2, 2])],
])
|
b7c1da4b015d54d6427b483aac71bb177bca32b72fcbd0a2e2171d6e20ebee4a | from sympy import I, symbols, Matrix, eye, Mod, floor
from sympy.matrices import MatrixSymbol, Identity
from sympy.matrices.expressions import det, trace
from sympy.matrices.expressions.kronecker import (KroneckerProduct,
kronecker_product,
combine_kronecker)
mat1 = Matrix([[1, 2 * I], [1 + I, 3]])
mat2 = Matrix([[2 * I, 3], [4 * I, 2]])
i, j, k, n, m, o, p, x = symbols('i,j,k,n,m,o,p,x')
Z = MatrixSymbol('Z', n, n)
W = MatrixSymbol('W', m, m)
A = MatrixSymbol('A', n, m)
B = MatrixSymbol('B', n, m)
C = MatrixSymbol('C', m, k)
def test_KroneckerProduct():
assert isinstance(KroneckerProduct(A, B), KroneckerProduct)
assert KroneckerProduct(A, B).subs(A, C) == KroneckerProduct(C, B)
assert KroneckerProduct(A, C).shape == (n*m, m*k)
assert (KroneckerProduct(A, C) + KroneckerProduct(-A, C)).is_ZeroMatrix
assert (KroneckerProduct(W, Z) * KroneckerProduct(W.I, Z.I)).is_Identity
def test_KroneckerProduct_identity():
assert KroneckerProduct(Identity(m), Identity(n)) == Identity(m*n)
assert KroneckerProduct(eye(2), eye(3)) == eye(6)
def test_KroneckerProduct_explicit():
X = MatrixSymbol('X', 2, 2)
Y = MatrixSymbol('Y', 2, 2)
kp = KroneckerProduct(X, Y)
assert kp.shape == (4, 4)
assert kp.as_explicit() == Matrix(
[
[X[0, 0]*Y[0, 0], X[0, 0]*Y[0, 1], X[0, 1]*Y[0, 0], X[0, 1]*Y[0, 1]],
[X[0, 0]*Y[1, 0], X[0, 0]*Y[1, 1], X[0, 1]*Y[1, 0], X[0, 1]*Y[1, 1]],
[X[1, 0]*Y[0, 0], X[1, 0]*Y[0, 1], X[1, 1]*Y[0, 0], X[1, 1]*Y[0, 1]],
[X[1, 0]*Y[1, 0], X[1, 0]*Y[1, 1], X[1, 1]*Y[1, 0], X[1, 1]*Y[1, 1]]
]
)
def test_tensor_product_adjoint():
assert KroneckerProduct(I*A, B).adjoint() == \
-I*KroneckerProduct(A.adjoint(), B.adjoint())
assert KroneckerProduct(mat1, mat2).adjoint() == \
kronecker_product(mat1.adjoint(), mat2.adjoint())
def test_tensor_product_conjugate():
assert KroneckerProduct(I*A, B).conjugate() == \
-I*KroneckerProduct(A.conjugate(), B.conjugate())
assert KroneckerProduct(mat1, mat2).conjugate() == \
kronecker_product(mat1.conjugate(), mat2.conjugate())
def test_tensor_product_transpose():
assert KroneckerProduct(I*A, B).transpose() == \
I*KroneckerProduct(A.transpose(), B.transpose())
assert KroneckerProduct(mat1, mat2).transpose() == \
kronecker_product(mat1.transpose(), mat2.transpose())
def test_KroneckerProduct_is_associative():
assert kronecker_product(A, kronecker_product(
B, C)) == kronecker_product(kronecker_product(A, B), C)
assert kronecker_product(A, kronecker_product(
B, C)) == KroneckerProduct(A, B, C)
def test_KroneckerProduct_is_bilinear():
assert kronecker_product(x*A, B) == x*kronecker_product(A, B)
assert kronecker_product(A, x*B) == x*kronecker_product(A, B)
def test_KroneckerProduct_determinant():
kp = kronecker_product(W, Z)
assert det(kp) == det(W)**n * det(Z)**m
def test_KroneckerProduct_trace():
kp = kronecker_product(W, Z)
assert trace(kp) == trace(W)*trace(Z)
def test_KroneckerProduct_isnt_commutative():
assert KroneckerProduct(A, B) != KroneckerProduct(B, A)
assert KroneckerProduct(A, B).is_commutative is False
def test_KroneckerProduct_extracts_commutative_part():
assert kronecker_product(x * A, 2 * B) == x * \
2 * KroneckerProduct(A, B)
def test_KroneckerProduct_inverse():
kp = kronecker_product(W, Z)
assert kp.inverse() == kronecker_product(W.inverse(), Z.inverse())
def test_KroneckerProduct_combine_add():
kp1 = kronecker_product(A, B)
kp2 = kronecker_product(C, W)
assert combine_kronecker(kp1*kp2) == kronecker_product(A*C, B*W)
def test_KroneckerProduct_combine_mul():
X = MatrixSymbol('X', m, n)
Y = MatrixSymbol('Y', m, n)
kp1 = kronecker_product(A, X)
kp2 = kronecker_product(B, Y)
assert combine_kronecker(kp1+kp2) == kronecker_product(A+B, X+Y)
def test_KroneckerProduct_combine_pow():
X = MatrixSymbol('X', n, n)
Y = MatrixSymbol('Y', n, n)
assert combine_kronecker(KroneckerProduct(
X, Y)**x) == KroneckerProduct(X**x, Y**x)
assert combine_kronecker(x * KroneckerProduct(X, Y)
** 2) == x * KroneckerProduct(X**2, Y**2)
assert combine_kronecker(
x * (KroneckerProduct(X, Y)**2) * KroneckerProduct(A, B)) == x * KroneckerProduct(X**2 * A, Y**2 * B)
def test_KroneckerProduct_expand():
X = MatrixSymbol('X', n, n)
Y = MatrixSymbol('Y', n, n)
assert KroneckerProduct(X + Y, Y + Z).expand(kroneckerproduct=True) == \
KroneckerProduct(X, Y) + KroneckerProduct(X, Z) + \
KroneckerProduct(Y, Y) + KroneckerProduct(Y, Z)
def test_KroneckerProduct_entry():
A = MatrixSymbol('A', n, m)
B = MatrixSymbol('B', o, p)
assert KroneckerProduct(A, B)._entry(i, j) == A[Mod(floor(i/o), n), Mod(floor(j/p), m)]*B[Mod(i, o), Mod(j, p)]
|
b698d654ba30a3cae4661a434b1fed804533b93a78064a144a4690665bb9db12 | from sympy.core import Lambda, S, symbols
from sympy.concrete import Sum
from sympy.functions import adjoint, conjugate, transpose
from sympy.matrices import eye, Matrix, ShapeError, ImmutableMatrix
from sympy.matrices.expressions import (
Adjoint, Identity, FunctionMatrix, MatrixExpr, MatrixSymbol, Trace,
ZeroMatrix, trace, MatPow, MatAdd, MatMul
)
from sympy.matrices.expressions.matexpr import OneMatrix
from sympy.utilities.pytest import raises
n = symbols('n', integer=True)
A = MatrixSymbol('A', n, n)
B = MatrixSymbol('B', n, n)
C = MatrixSymbol('C', 3, 4)
def test_Trace():
assert isinstance(Trace(A), Trace)
assert not isinstance(Trace(A), MatrixExpr)
raises(ShapeError, lambda: Trace(C))
assert trace(eye(3)) == 3
assert trace(Matrix(3, 3, [1, 2, 3, 4, 5, 6, 7, 8, 9])) == 15
assert adjoint(Trace(A)) == trace(Adjoint(A))
assert conjugate(Trace(A)) == trace(Adjoint(A))
assert transpose(Trace(A)) == Trace(A)
A / Trace(A) # Make sure this is possible
# Some easy simplifications
assert trace(Identity(5)) == 5
assert trace(ZeroMatrix(5, 5)) == 0
assert trace(OneMatrix(1, 1)) == 1
assert trace(OneMatrix(2, 2)) == 2
assert trace(OneMatrix(n, n)) == n
assert trace(2*A*B) == 2*Trace(A*B)
assert trace(A.T) == trace(A)
i, j = symbols('i j')
F = FunctionMatrix(3, 3, Lambda((i, j), i + j))
assert trace(F) == (0 + 0) + (1 + 1) + (2 + 2)
raises(TypeError, lambda: Trace(S.One))
assert Trace(A).arg is A
assert str(trace(A)) == str(Trace(A).doit())
assert Trace(A).is_commutative is True
def test_Trace_A_plus_B():
assert trace(A + B) == Trace(A) + Trace(B)
assert Trace(A + B).arg == MatAdd(A, B)
assert Trace(A + B).doit() == Trace(A) + Trace(B)
def test_Trace_MatAdd_doit():
# See issue #9028
X = ImmutableMatrix([[1, 2, 3]]*3)
Y = MatrixSymbol('Y', 3, 3)
q = MatAdd(X, 2*X, Y, -3*Y)
assert Trace(q).arg == q
assert Trace(q).doit() == 18 - 2*Trace(Y)
def test_Trace_MatPow_doit():
X = Matrix([[1, 2], [3, 4]])
assert Trace(X).doit() == 5
q = MatPow(X, 2)
assert Trace(q).arg == q
assert Trace(q).doit() == 29
def test_Trace_MutableMatrix_plus():
# See issue #9043
X = Matrix([[1, 2], [3, 4]])
assert Trace(X) + Trace(X) == 2*Trace(X)
def test_Trace_doit_deep_False():
X = Matrix([[1, 2], [3, 4]])
q = MatPow(X, 2)
assert Trace(q).doit(deep=False).arg == q
q = MatAdd(X, 2*X)
assert Trace(q).doit(deep=False).arg == q
q = MatMul(X, 2*X)
assert Trace(q).doit(deep=False).arg == q
def test_trace_constant_factor():
# Issue 9052: gave 2*Trace(MatMul(A)) instead of 2*Trace(A)
assert trace(2*A) == 2*Trace(A)
X = ImmutableMatrix([[1, 2], [3, 4]])
assert trace(MatMul(2, X)) == 10
def test_rewrite():
assert isinstance(trace(A).rewrite(Sum), Sum)
|
f1c65524f779f8449e3958b8918b1b1df5c16bf8bb3f5662a28086be6d09497b | from sympy import Identity, OneMatrix, ZeroMatrix, Matrix, MatAdd
from sympy.core import symbols
from sympy.utilities.pytest import raises
from sympy.matrices import ShapeError, MatrixSymbol
from sympy.matrices.expressions import (HadamardProduct, hadamard_product, HadamardPower, hadamard_power)
n, m, k = symbols('n,m,k')
Z = MatrixSymbol('Z', n, n)
A = MatrixSymbol('A', n, m)
B = MatrixSymbol('B', n, m)
C = MatrixSymbol('C', m, k)
def test_HadamardProduct():
assert HadamardProduct(A, B, A).shape == A.shape
raises(ShapeError, lambda: HadamardProduct(A, B.T))
raises(TypeError, lambda: HadamardProduct(A, n))
raises(TypeError, lambda: HadamardProduct(A, 1))
assert HadamardProduct(A, 2*B, -A)[1, 1] == \
-2 * A[1, 1] * B[1, 1] * A[1, 1]
mix = HadamardProduct(Z*A, B)*C
assert mix.shape == (n, k)
assert set(HadamardProduct(A, B, A).T.args) == set((A.T, A.T, B.T))
def test_HadamardProduct_isnt_commutative():
assert HadamardProduct(A, B) != HadamardProduct(B, A)
def test_mixed_indexing():
X = MatrixSymbol('X', 2, 2)
Y = MatrixSymbol('Y', 2, 2)
Z = MatrixSymbol('Z', 2, 2)
assert (X*HadamardProduct(Y, Z))[0, 0] == \
X[0, 0]*Y[0, 0]*Z[0, 0] + X[0, 1]*Y[1, 0]*Z[1, 0]
def test_canonicalize():
X = MatrixSymbol('X', 2, 2)
Y = MatrixSymbol('Y', 2, 2)
expr = HadamardProduct(X, check=False)
assert isinstance(expr, HadamardProduct)
expr2 = expr.doit() # unpack is called
assert isinstance(expr2, MatrixSymbol)
Z = ZeroMatrix(2, 2)
U = OneMatrix(2, 2)
assert HadamardProduct(Z, X).doit() == Z
assert HadamardProduct(U, X, X, U).doit() == HadamardPower(X, 2)
assert HadamardProduct(X, U, Y).doit() == HadamardProduct(X, Y)
assert HadamardProduct(X, Z, U, Y).doit() == Z
def test_hadamard():
m, n, p = symbols('m, n, p', integer=True)
A = MatrixSymbol('A', m, n)
B = MatrixSymbol('B', m, n)
C = MatrixSymbol('C', m, p)
X = MatrixSymbol('X', m, m)
I = Identity(m)
with raises(TypeError):
hadamard_product()
assert hadamard_product(A) == A
assert isinstance(hadamard_product(A, B), HadamardProduct)
assert hadamard_product(A, B).doit() == hadamard_product(A, B)
with raises(ShapeError):
hadamard_product(A, C)
hadamard_product(A, I)
assert hadamard_product(X, I) == X
assert isinstance(hadamard_product(X, I), MatrixSymbol)
a = MatrixSymbol("a", k, 1)
expr = MatAdd(ZeroMatrix(k, 1), OneMatrix(k, 1))
expr = HadamardProduct(expr, a)
assert expr.doit() == a
def test_hadamard_product_with_explicit_mat():
A = MatrixSymbol("A", 3, 3).as_explicit()
B = MatrixSymbol("B", 3, 3).as_explicit()
X = MatrixSymbol("X", 3, 3)
expr = hadamard_product(A, B)
ret = Matrix([i*j for i, j in zip(A, B)]).reshape(3, 3)
assert expr == ret
expr = hadamard_product(A, X, B)
assert expr == HadamardProduct(ret, X)
def test_hadamard_power():
m, n, p = symbols('m, n, p', integer=True)
A = MatrixSymbol('A', m, n)
assert hadamard_power(A, 1) == A
assert isinstance(hadamard_power(A, 2), HadamardPower)
assert hadamard_power(A, n).T == hadamard_power(A.T, n)
assert hadamard_power(A, n)[0, 0] == A[0, 0]**n
assert hadamard_power(m, n) == m**n
raises(ValueError, lambda: hadamard_power(A, A))
def test_hadamard_power_explicit():
from sympy.matrices import Matrix
A = MatrixSymbol('A', 2, 2)
B = MatrixSymbol('B', 2, 2)
a, b = symbols('a b')
assert HadamardPower(a, b) == a**b
assert HadamardPower(a, B).as_explicit() == \
Matrix([
[a**B[0, 0], a**B[0, 1]],
[a**B[1, 0], a**B[1, 1]]])
assert HadamardPower(A, b).as_explicit() == \
Matrix([
[A[0, 0]**b, A[0, 1]**b],
[A[1, 0]**b, A[1, 1]**b]])
assert HadamardPower(A, B).as_explicit() == \
Matrix([
[A[0, 0]**B[0, 0], A[0, 1]**B[0, 1]],
[A[1, 0]**B[1, 0], A[1, 1]**B[1, 1]]])
|
a29ecffd12807700a6fb75895ef947888d97ded2bbe2aaf04d8b08ea768fc49c | from sympy import (S, Dummy, Lambda, symbols, Interval, Intersection, Set,
EmptySet, FiniteSet, Union, ComplexRegion, ProductSet)
from sympy.multipledispatch import dispatch
from sympy.sets.conditionset import ConditionSet
from sympy.sets.fancysets import (Integers, Naturals, Reals, Range,
ImageSet, Rationals)
from sympy.sets.sets import UniversalSet, imageset, ProductSet
@dispatch(ConditionSet, ConditionSet)
def intersection_sets(a, b):
return None
@dispatch(ConditionSet, Set)
def intersection_sets(a, b):
return ConditionSet(a.sym, a.condition, Intersection(a.base_set, b))
@dispatch(Naturals, Integers)
def intersection_sets(a, b):
return a
@dispatch(Naturals, Naturals)
def intersection_sets(a, b):
return a if a is S.Naturals else b
@dispatch(Interval, Naturals)
def intersection_sets(a, b):
return intersection_sets(b, a)
@dispatch(ComplexRegion, Set)
def intersection_sets(self, other):
if other.is_ComplexRegion:
# self in rectangular form
if (not self.polar) and (not other.polar):
return ComplexRegion(Intersection(self.sets, other.sets))
# self in polar form
elif self.polar and other.polar:
r1, theta1 = self.a_interval, self.b_interval
r2, theta2 = other.a_interval, other.b_interval
new_r_interval = Intersection(r1, r2)
new_theta_interval = Intersection(theta1, theta2)
# 0 and 2*Pi means the same
if ((2*S.Pi in theta1 and S.Zero in theta2) or
(2*S.Pi in theta2 and S.Zero in theta1)):
new_theta_interval = Union(new_theta_interval,
FiniteSet(0))
return ComplexRegion(new_r_interval*new_theta_interval,
polar=True)
if other.is_subset(S.Reals):
new_interval = []
x = symbols("x", cls=Dummy, real=True)
# self in rectangular form
if not self.polar:
for element in self.psets:
if S.Zero in element.args[1]:
new_interval.append(element.args[0])
new_interval = Union(*new_interval)
return Intersection(new_interval, other)
# self in polar form
elif self.polar:
for element in self.psets:
if S.Zero in element.args[1]:
new_interval.append(element.args[0])
if S.Pi in element.args[1]:
new_interval.append(ImageSet(Lambda(x, -x), element.args[0]))
if S.Zero in element.args[0]:
new_interval.append(FiniteSet(0))
new_interval = Union(*new_interval)
return Intersection(new_interval, other)
@dispatch(Integers, Reals)
def intersection_sets(a, b):
return a
@dispatch(Range, Interval)
def intersection_sets(a, b):
from sympy.functions.elementary.integers import floor, ceiling
if not all(i.is_number for i in b.args[:2]):
return
# In case of null Range, return an EmptySet.
if a.size == 0:
return S.EmptySet
# trim down to self's size, and represent
# as a Range with step 1.
start = ceiling(max(b.inf, a.inf))
if start not in b:
start += 1
end = floor(min(b.sup, a.sup))
if end not in b:
end -= 1
return intersection_sets(a, Range(start, end + 1))
@dispatch(Range, Naturals)
def intersection_sets(a, b):
return intersection_sets(a, Interval(b.inf, S.Infinity))
@dispatch(Range, Range)
def intersection_sets(a, b):
from sympy.solvers.diophantine import diop_linear
from sympy.core.numbers import ilcm
from sympy import sign
# non-overlap quick exits
if not b:
return S.EmptySet
if not a:
return S.EmptySet
if b.sup < a.inf:
return S.EmptySet
if b.inf > a.sup:
return S.EmptySet
# work with finite end at the start
r1 = a
if r1.start.is_infinite:
r1 = r1.reversed
r2 = b
if r2.start.is_infinite:
r2 = r2.reversed
# this equation represents the values of the Range;
# it's a linear equation
eq = lambda r, i: r.start + i*r.step
# we want to know when the two equations might
# have integer solutions so we use the diophantine
# solver
va, vb = diop_linear(eq(r1, Dummy('a')) - eq(r2, Dummy('b')))
# check for no solution
no_solution = va is None and vb is None
if no_solution:
return S.EmptySet
# there is a solution
# -------------------
# find the coincident point, c
a0 = va.as_coeff_Add()[0]
c = eq(r1, a0)
# find the first point, if possible, in each range
# since c may not be that point
def _first_finite_point(r1, c):
if c == r1.start:
return c
# st is the signed step we need to take to
# get from c to r1.start
st = sign(r1.start - c)*step
# use Range to calculate the first point:
# we want to get as close as possible to
# r1.start; the Range will not be null since
# it will at least contain c
s1 = Range(c, r1.start + st, st)[-1]
if s1 == r1.start:
pass
else:
# if we didn't hit r1.start then, if the
# sign of st didn't match the sign of r1.step
# we are off by one and s1 is not in r1
if sign(r1.step) != sign(st):
s1 -= st
if s1 not in r1:
return
return s1
# calculate the step size of the new Range
step = abs(ilcm(r1.step, r2.step))
s1 = _first_finite_point(r1, c)
if s1 is None:
return S.EmptySet
s2 = _first_finite_point(r2, c)
if s2 is None:
return S.EmptySet
# replace the corresponding start or stop in
# the original Ranges with these points; the
# result must have at least one point since
# we know that s1 and s2 are in the Ranges
def _updated_range(r, first):
st = sign(r.step)*step
if r.start.is_finite:
rv = Range(first, r.stop, st)
else:
rv = Range(r.start, first + st, st)
return rv
r1 = _updated_range(a, s1)
r2 = _updated_range(b, s2)
# work with them both in the increasing direction
if sign(r1.step) < 0:
r1 = r1.reversed
if sign(r2.step) < 0:
r2 = r2.reversed
# return clipped Range with positive step; it
# can't be empty at this point
start = max(r1.start, r2.start)
stop = min(r1.stop, r2.stop)
return Range(start, stop, step)
@dispatch(Range, Integers)
def intersection_sets(a, b):
return a
@dispatch(ImageSet, Set)
def intersection_sets(self, other):
from sympy.solvers.diophantine import diophantine
if self.base_set is S.Integers:
g = None
if isinstance(other, ImageSet) and other.base_set is S.Integers:
g = other.lamda.expr
m = other.lamda.variables[0]
elif other is S.Integers:
m = g = Dummy('x')
if g is not None:
f = self.lamda.expr
n = self.lamda.variables[0]
# Diophantine sorts the solutions according to the alphabetic
# order of the variable names, since the result should not depend
# on the variable name, they are replaced by the dummy variables
# below
a, b = Dummy('a'), Dummy('b')
fa, ga = f.subs(n, a), g.subs(m, b)
solns = list(diophantine(fa - ga))
if not solns:
return EmptySet()
if len(solns) != 1:
return
nsol = solns[0][0] # since 'a' < 'b', nsol is first
t = nsol.free_symbols.pop() # diophantine supplied symbol
nsol = nsol.subs(t, n)
if nsol != n:
# if nsol == n and we know were are working with
# a base_set of Integers then this was an unevaluated
# ImageSet representation of Integers, otherwise
# it is a new ImageSet intersection with a subset
# of integers
nsol = f.subs(n, nsol)
return imageset(Lambda(n, nsol), S.Integers)
if other == S.Reals:
from sympy.solvers.solveset import solveset_real
from sympy.core.function import expand_complex
if len(self.lamda.variables) > 1:
return None
f = self.lamda.expr
n = self.lamda.variables[0]
n_ = Dummy(n.name, real=True)
f_ = f.subs(n, n_)
re, im = f_.as_real_imag()
im = expand_complex(im)
re = re.subs(n_, n)
im = im.subs(n_, n)
ifree = im.free_symbols
lam = Lambda(n, re)
base = self.base_set
if not im:
# allow re-evaluation
# of self in this case to make
# the result canonical
pass
elif im.is_zero is False:
return S.EmptySet
elif ifree != {n}:
return None
else:
# univarite imaginary part in same variable
base = base.intersect(solveset_real(im, n))
return imageset(lam, base)
elif isinstance(other, Interval):
from sympy.solvers.solveset import (invert_real, invert_complex,
solveset)
f = self.lamda.expr
n = self.lamda.variables[0]
base_set = self.base_set
new_inf, new_sup = None, None
new_lopen, new_ropen = other.left_open, other.right_open
if f.is_real:
inverter = invert_real
else:
inverter = invert_complex
g1, h1 = inverter(f, other.inf, n)
g2, h2 = inverter(f, other.sup, n)
if all(isinstance(i, FiniteSet) for i in (h1, h2)):
if g1 == n:
if len(h1) == 1:
new_inf = h1.args[0]
if g2 == n:
if len(h2) == 1:
new_sup = h2.args[0]
# TODO: Design a technique to handle multiple-inverse
# functions
# Any of the new boundary values cannot be determined
if any(i is None for i in (new_sup, new_inf)):
return
range_set = S.EmptySet
if all(i.is_real for i in (new_sup, new_inf)):
# this assumes continuity of underlying function
# however fixes the case when it is decreasing
if new_inf > new_sup:
new_inf, new_sup = new_sup, new_inf
new_interval = Interval(new_inf, new_sup, new_lopen, new_ropen)
range_set = base_set.intersect(new_interval)
else:
if other.is_subset(S.Reals):
solutions = solveset(f, n, S.Reals)
if not isinstance(range_set, (ImageSet, ConditionSet)):
range_set = solutions.intersect(other)
else:
return
if range_set is S.EmptySet:
return S.EmptySet
elif isinstance(range_set, Range) and range_set.size is not S.Infinity:
range_set = FiniteSet(*list(range_set))
if range_set is not None:
return imageset(Lambda(n, f), range_set)
return
else:
return
@dispatch(ProductSet, ProductSet)
def intersection_sets(a, b):
if len(b.args) != len(a.args):
return S.EmptySet
return ProductSet(*(i.intersect(j) for i, j in zip(a.sets, b.sets)))
@dispatch(Interval, Interval)
def intersection_sets(a, b):
# handle (-oo, oo)
infty = S.NegativeInfinity, S.Infinity
if a == Interval(*infty):
l, r = a.left, a.right
if l.is_real or l in infty or r.is_real or r in infty:
return b
# We can't intersect [0,3] with [x,6] -- we don't know if x>0 or x<0
if not a._is_comparable(b):
return None
empty = False
if a.start <= b.end and b.start <= a.end:
# Get topology right.
if a.start < b.start:
start = b.start
left_open = b.left_open
elif a.start > b.start:
start = a.start
left_open = a.left_open
else:
start = a.start
left_open = a.left_open or b.left_open
if a.end < b.end:
end = a.end
right_open = a.right_open
elif a.end > b.end:
end = b.end
right_open = b.right_open
else:
end = a.end
right_open = a.right_open or b.right_open
if end - start == 0 and (left_open or right_open):
empty = True
else:
empty = True
if empty:
return S.EmptySet
return Interval(start, end, left_open, right_open)
@dispatch(EmptySet, Set)
def intersection_sets(a, b):
return S.EmptySet
@dispatch(UniversalSet, Set)
def intersection_sets(a, b):
return b
@dispatch(FiniteSet, FiniteSet)
def intersection_sets(a, b):
return FiniteSet(*(a._elements & b._elements))
@dispatch(FiniteSet, Set)
def intersection_sets(a, b):
try:
return FiniteSet(*[el for el in a if el in b])
except TypeError:
return None # could not evaluate `el in b` due to symbolic ranges.
@dispatch(Set, Set)
def intersection_sets(a, b):
return None
@dispatch(Integers, Rationals)
def intersection_sets(a, b):
return a
@dispatch(Naturals, Rationals)
def intersection_sets(a, b):
return a
@dispatch(Rationals, Reals)
def intersection_sets(a, b):
return a
def _intlike_interval(a, b):
try:
from sympy.functions.elementary.integers import floor, ceiling
if b._inf is S.NegativeInfinity and b._sup is S.Infinity:
return a
s = Range(max(a.inf, ceiling(b.left)), floor(b.right) + 1)
return intersection_sets(s, b) # take out endpoints if open interval
except ValueError:
return None
@dispatch(Integers, Interval)
def intersection_sets(a, b):
return _intlike_interval(a, b)
@dispatch(Naturals, Interval)
def intersection_sets(a, b):
return _intlike_interval(a, b)
|
a528cdef7764bfb6cd4bc887783ba38be83d4eeeea09002abcc7bbd302e1c692 | from sympy import (Interval, Intersection, Set, EmptySet, S, sympify,
FiniteSet, Union, ComplexRegion, ProductSet)
from sympy.multipledispatch import dispatch
from sympy.sets.fancysets import Integers
from sympy.sets.sets import UniversalSet
@dispatch(Integers, Set)
def union_sets(a, b):
intersect = Intersection(a, b)
if intersect == a:
return b
elif intersect == b:
return a
@dispatch(ComplexRegion, Set)
def union_sets(a, b):
if b.is_subset(S.Reals):
# treat a subset of reals as a complex region
b = ComplexRegion.from_real(b)
if b.is_ComplexRegion:
# a in rectangular form
if (not a.polar) and (not b.polar):
return ComplexRegion(Union(a.sets, b.sets))
# a in polar form
elif a.polar and b.polar:
return ComplexRegion(Union(a.sets, b.sets), polar=True)
return None
@dispatch(EmptySet, Set)
def union_sets(a, b):
return b
@dispatch(UniversalSet, Set)
def union_sets(a, b):
return a
@dispatch(ProductSet, ProductSet)
def union_sets(a, b):
if b.is_subset(a):
return a
if len(b.sets) != len(a.sets):
return None
if len(a.sets) == 2:
a1, a2 = a.sets
b1, b2 = b.sets
if a1 == b1:
return a1 * Union(a2, b2)
if a2 == b2:
return Union(a1, b1) * a2
return None
@dispatch(ProductSet, Set)
def union_sets(a, b):
if b.is_subset(a):
return a
return None
@dispatch(Interval, Interval)
def union_sets(a, b):
if a._is_comparable(b):
from sympy.functions.elementary.miscellaneous import Min, Max
# Non-overlapping intervals
end = Min(a.end, b.end)
start = Max(a.start, b.start)
if (end < start or
(end == start and (end not in a and end not in b))):
return None
else:
start = Min(a.start, b.start)
end = Max(a.end, b.end)
left_open = ((a.start != start or a.left_open) and
(b.start != start or b.left_open))
right_open = ((a.end != end or a.right_open) and
(b.end != end or b.right_open))
return Interval(start, end, left_open, right_open)
@dispatch(Interval, UniversalSet)
def union_sets(a, b):
return S.UniversalSet
@dispatch(Interval, Set)
def union_sets(a, b):
# If I have open end points and these endpoints are contained in b
# But only in case, when endpoints are finite. Because
# interval does not contain oo or -oo.
open_left_in_b_and_finite = (a.left_open and
sympify(b.contains(a.start)) is S.true and
a.start.is_finite)
open_right_in_b_and_finite = (a.right_open and
sympify(b.contains(a.end)) is S.true and
a.end.is_finite)
if open_left_in_b_and_finite or open_right_in_b_and_finite:
# Fill in my end points and return
open_left = a.left_open and a.start not in b
open_right = a.right_open and a.end not in b
new_a = Interval(a.start, a.end, open_left, open_right)
return set((new_a, b))
return None
@dispatch(FiniteSet, FiniteSet)
def union_sets(a, b):
return FiniteSet(*(a._elements | b._elements))
@dispatch(FiniteSet, Set)
def union_sets(a, b):
# If `b` set contains one of my elements, remove it from `a`
if any(b.contains(x) == True for x in a):
return set((
FiniteSet(*[x for x in a if not b.contains(x)]), b))
return None
@dispatch(Set, Set)
def union_sets(a, b):
return None
|
c1508a6197ca2519d2c27867111e98de689290fd61e90ba4801810629993b48c | from sympy.core.compatibility import range, PY3
from sympy.core.expr import unchanged
from sympy.sets.fancysets import (ImageSet, Range, normalize_theta_set,
ComplexRegion)
from sympy.sets.sets import (FiniteSet, Interval, imageset, Union,
Intersection, ProductSet, Contains)
from sympy.simplify.simplify import simplify
from sympy import (S, Symbol, Lambda, symbols, cos, sin, pi, oo, Basic,
Rational, sqrt, tan, log, exp, Abs, I, Tuple, eye,
Dummy, floor, And, Eq)
from sympy.utilities.iterables import cartes
from sympy.utilities.pytest import XFAIL, raises
from sympy.abc import x, y, t
import itertools
def test_naturals():
N = S.Naturals
assert 5 in N
assert -5 not in N
assert 5.5 not in N
ni = iter(N)
a, b, c, d = next(ni), next(ni), next(ni), next(ni)
assert (a, b, c, d) == (1, 2, 3, 4)
assert isinstance(a, Basic)
assert N.intersect(Interval(-5, 5)) == Range(1, 6)
assert N.intersect(Interval(-5, 5, True, True)) == Range(1, 5)
assert N.boundary == N
assert N.inf == 1
assert N.sup == oo
assert not N.contains(oo)
for s in (S.Naturals0, S.Naturals):
assert s.intersection(S.Reals) is s
assert s.is_subset(S.Reals)
assert N.as_relational(x) == And(Eq(floor(x), x), x >= S.One, x < oo)
def test_naturals0():
N = S.Naturals0
assert 0 in N
assert -1 not in N
assert next(iter(N)) == 0
assert not N.contains(oo)
assert N.contains(sin(x)) == Contains(sin(x), N)
def test_integers():
Z = S.Integers
assert 5 in Z
assert -5 in Z
assert 5.5 not in Z
assert not Z.contains(oo)
assert not Z.contains(-oo)
zi = iter(Z)
a, b, c, d = next(zi), next(zi), next(zi), next(zi)
assert (a, b, c, d) == (0, 1, -1, 2)
assert isinstance(a, Basic)
assert Z.intersect(Interval(-5, 5)) == Range(-5, 6)
assert Z.intersect(Interval(-5, 5, True, True)) == Range(-4, 5)
assert Z.intersect(Interval(5, S.Infinity)) == Range(5, S.Infinity)
assert Z.intersect(Interval.Lopen(5, S.Infinity)) == Range(6, S.Infinity)
assert Z.inf == -oo
assert Z.sup == oo
assert Z.boundary == Z
assert Z.as_relational(x) == And(Eq(floor(x), x), -oo < x, x < oo)
def test_ImageSet():
raises(ValueError, lambda: ImageSet(x, S.Integers))
assert ImageSet(Lambda(x, 1), S.Integers) == FiniteSet(1)
assert ImageSet(Lambda(x, y), S.Integers) == {y}
assert ImageSet(Lambda(x, 1), S.EmptySet) == S.EmptySet
empty = Intersection(FiniteSet(log(2)/pi), S.Integers)
assert unchanged(ImageSet, Lambda(x, 1), empty) # issue #17471
squares = ImageSet(Lambda(x, x**2), S.Naturals)
assert 4 in squares
assert 5 not in squares
assert FiniteSet(*range(10)).intersect(squares) == FiniteSet(1, 4, 9)
assert 16 not in squares.intersect(Interval(0, 10))
si = iter(squares)
a, b, c, d = next(si), next(si), next(si), next(si)
assert (a, b, c, d) == (1, 4, 9, 16)
harmonics = ImageSet(Lambda(x, 1/x), S.Naturals)
assert Rational(1, 5) in harmonics
assert Rational(.25) in harmonics
assert 0.25 not in harmonics
assert Rational(.3) not in harmonics
assert (1, 2) not in harmonics
assert harmonics.is_iterable
assert imageset(x, -x, Interval(0, 1)) == Interval(-1, 0)
assert ImageSet(Lambda(x, x**2), Interval(0, 2)).doit() == Interval(0, 4)
c = ComplexRegion(Interval(1, 3)*Interval(1, 3))
assert Tuple(2, 6) in ImageSet(Lambda((x, y), (x, 2*y)), c)
assert Tuple(2, S.Half) in ImageSet(Lambda((x, y), (x, 1/y)), c)
assert Tuple(2, -2) not in ImageSet(Lambda((x, y), (x, y**2)), c)
assert Tuple(2, -2) in ImageSet(Lambda((x, y), (x, -2)), c)
c3 = Interval(3, 7)*Interval(8, 11)*Interval(5, 9)
assert Tuple(8, 3, 9) in ImageSet(Lambda((t, y, x), (y, t, x)), c3)
assert Tuple(S(1)/8, 3, 9) in ImageSet(Lambda((t, y, x), (1/y, t, x)), c3)
assert 2/pi not in ImageSet(Lambda((x, y), 2/x), c)
assert 2/S(100) not in ImageSet(Lambda((x, y), 2/x), c)
assert 2/S(3) in ImageSet(Lambda((x, y), 2/x), c)
assert imageset(lambda x, y: x + y, S.Integers, S.Naturals
).base_set == ProductSet(S.Integers, S.Naturals)
# Passing a set instead of a FiniteSet shouldn't raise
assert unchanged(ImageSet, Lambda(x, x**2), {1, 2, 3})
raises(TypeError, lambda: ImageSet(Lambda(x, x**2), 1))
def test_image_is_ImageSet():
assert isinstance(imageset(x, sqrt(sin(x)), Range(5)), ImageSet)
def test_halfcircle():
# This test sometimes works and sometimes doesn't.
# It may be an issue with solve? Maybe with using Lambdas/dummys?
# I believe the code within fancysets is correct
r, th = symbols('r, theta', real=True)
L = Lambda((r, th), (r*cos(th), r*sin(th)))
halfcircle = ImageSet(L, Interval(0, 1)*Interval(0, pi))
assert (r, 0) in halfcircle
assert (1, 0) in halfcircle
assert (0, -1) not in halfcircle
assert (r, 2*pi) not in halfcircle
assert (0, 0) in halfcircle
assert not halfcircle.is_iterable
def test_ImageSet_iterator_not_injective():
L = Lambda(x, x - x % 2) # produces 0, 2, 2, 4, 4, 6, 6, ...
evens = ImageSet(L, S.Naturals)
i = iter(evens)
# No repeats here
assert (next(i), next(i), next(i), next(i)) == (0, 2, 4, 6)
def test_inf_Range_len():
raises(ValueError, lambda: len(Range(0, oo, 2)))
assert Range(0, oo, 2).size is S.Infinity
assert Range(0, -oo, -2).size is S.Infinity
assert Range(oo, 0, -2).size is S.Infinity
assert Range(-oo, 0, 2).size is S.Infinity
def test_Range_set():
empty = Range(0)
assert Range(5) == Range(0, 5) == Range(0, 5, 1)
r = Range(10, 20, 2)
assert 12 in r
assert 8 not in r
assert 11 not in r
assert 30 not in r
assert list(Range(0, 5)) == list(range(5))
assert list(Range(5, 0, -1)) == list(range(5, 0, -1))
assert Range(5, 15).sup == 14
assert Range(5, 15).inf == 5
assert Range(15, 5, -1).sup == 15
assert Range(15, 5, -1).inf == 6
assert Range(10, 67, 10).sup == 60
assert Range(60, 7, -10).inf == 10
assert len(Range(10, 38, 10)) == 3
assert Range(0, 0, 5) == empty
assert Range(oo, oo, 1) == empty
assert Range(oo, 1, 1) == empty
assert Range(-oo, 1, -1) == empty
assert Range(1, oo, -1) == empty
assert Range(1, -oo, 1) == empty
assert Range(1, -4, oo) == empty
assert Range(1, -4, -oo) == Range(1, 2)
assert Range(1, 4, oo) == Range(1, 2)
assert Range(-oo, oo).size == oo
assert Range(oo, -oo, -1).size == oo
raises(ValueError, lambda: Range(-oo, oo, 2))
raises(ValueError, lambda: Range(x, pi, y))
raises(ValueError, lambda: Range(x, y, 0))
assert 5 in Range(0, oo, 5)
assert -5 in Range(-oo, 0, 5)
assert oo not in Range(0, oo)
ni = symbols('ni', integer=False)
assert ni not in Range(oo)
u = symbols('u', integer=None)
assert Range(oo).contains(u) is not False
inf = symbols('inf', infinite=True)
assert inf not in Range(-oo, oo)
raises(ValueError, lambda: Range(0, oo, 2)[-1])
raises(ValueError, lambda: Range(0, -oo, -2)[-1])
assert Range(-oo, 1, 1)[-1] is S.Zero
assert Range(oo, 1, -1)[-1] == 2
assert Range(1, 10, 1)[-1] == 9
assert all(i.is_Integer for i in Range(0, -1, 1))
it = iter(Range(-oo, 0, 2))
raises(ValueError, lambda: next(it))
assert empty.intersect(S.Integers) == empty
assert Range(-1, 10, 1).intersect(S.Integers) == Range(-1, 10, 1)
assert Range(-1, 10, 1).intersect(S.Naturals) == Range(1, 10, 1)
assert Range(-1, 10, 1).intersect(S.Naturals0) == Range(0, 10, 1)
# test slicing
assert Range(1, 10, 1)[5] == 6
assert Range(1, 12, 2)[5] == 11
assert Range(1, 10, 1)[-1] == 9
assert Range(1, 10, 3)[-1] == 7
raises(ValueError, lambda: Range(oo,0,-1)[1:3:0])
raises(ValueError, lambda: Range(oo,0,-1)[:1])
raises(ValueError, lambda: Range(1, oo)[-2])
raises(ValueError, lambda: Range(-oo, 1)[2])
raises(IndexError, lambda: Range(10)[-20])
raises(IndexError, lambda: Range(10)[20])
raises(ValueError, lambda: Range(2, -oo, -2)[2:2:0])
assert Range(2, -oo, -2)[2:2:2] == empty
assert Range(2, -oo, -2)[:2:2] == Range(2, -2, -4)
raises(ValueError, lambda: Range(-oo, 4, 2)[:2:2])
assert Range(-oo, 4, 2)[::-2] == Range(2, -oo, -4)
raises(ValueError, lambda: Range(-oo, 4, 2)[::2])
assert Range(oo, 2, -2)[::] == Range(oo, 2, -2)
assert Range(-oo, 4, 2)[:-2:-2] == Range(2, 0, -4)
assert Range(-oo, 4, 2)[:-2:2] == Range(-oo, 0, 4)
raises(ValueError, lambda: Range(-oo, 4, 2)[:0:-2])
raises(ValueError, lambda: Range(-oo, 4, 2)[:2:-2])
assert Range(-oo, 4, 2)[-2::-2] == Range(0, -oo, -4)
raises(ValueError, lambda: Range(-oo, 4, 2)[-2:0:-2])
raises(ValueError, lambda: Range(-oo, 4, 2)[0::2])
assert Range(oo, 2, -2)[0::] == Range(oo, 2, -2)
raises(ValueError, lambda: Range(-oo, 4, 2)[0:-2:2])
assert Range(oo, 2, -2)[0:-2:] == Range(oo, 6, -2)
raises(ValueError, lambda: Range(oo, 2, -2)[0:2:])
raises(ValueError, lambda: Range(-oo, 4, 2)[2::-1])
assert Range(-oo, 4, 2)[-2::2] == Range(0, 4, 4)
assert Range(oo, 0, -2)[-10:0:2] == empty
raises(ValueError, lambda: Range(oo, 0, -2)[-10:10:2])
raises(ValueError, lambda: Range(oo, 0, -2)[0::-2])
assert Range(oo, 0, -2)[0:-4:-2] == empty
assert Range(oo, 0, -2)[:0:2] == empty
raises(ValueError, lambda: Range(oo, 0, -2)[:1:-1])
# test empty Range
assert Range(x, x, y) == empty
assert empty.reversed == empty
assert 0 not in empty
assert list(empty) == []
assert len(empty) == 0
assert empty.size is S.Zero
assert empty.intersect(FiniteSet(0)) is S.EmptySet
assert bool(empty) is False
raises(IndexError, lambda: empty[0])
assert empty[:0] == empty
raises(NotImplementedError, lambda: empty.inf)
raises(NotImplementedError, lambda: empty.sup)
AB = [None] + list(range(12))
for R in [
Range(1, 10),
Range(1, 10, 2),
]:
r = list(R)
for a, b, c in cartes(AB, AB, [-3, -1, None, 1, 3]):
for reverse in range(2):
r = list(reversed(r))
R = R.reversed
result = list(R[a:b:c])
ans = r[a:b:c]
txt = ('\n%s[%s:%s:%s] = %s -> %s' % (
R, a, b, c, result, ans))
check = ans == result
assert check, txt
assert Range(1, 10, 1).boundary == Range(1, 10, 1)
for r in (Range(1, 10, 2), Range(1, oo, 2)):
rev = r.reversed
assert r.inf == rev.inf and r.sup == rev.sup
assert r.step == -rev.step
# Make sure to use range in Python 3 and xrange in Python 2 (regardless of
# compatibility imports above)
if PY3:
builtin_range = range
else:
builtin_range = xrange
raises(TypeError, lambda: Range(builtin_range(1)))
assert S(builtin_range(10)) == Range(10)
if PY3:
assert S(builtin_range(1000000000000)) == \
Range(1000000000000)
# test Range.as_relational
assert Range(1, 4).as_relational(x) == (x >= 1) & (x <= 3) & Eq(x, floor(x))
assert Range(oo, 1, -2).as_relational(x) == (x >= 3) & (x < oo) & Eq(x, floor(x))
# symbolic Range
sr = Range(x, y, t)
i = Symbol('i', integer=True)
ip = Symbol('i', integer=True, positive=True)
ir = Range(i, i + 20, 2)
# args
assert sr.args == (x, y, t)
assert ir.args == (i, i + 20, 2)
# reversed
raises(ValueError, lambda: sr.reversed)
assert ir.reversed == Range(i + 18, i - 2, -2)
# contains
assert inf not in sr
assert inf not in ir
assert .1 not in sr
assert .1 not in ir
assert i + 1 not in ir
assert i + 2 in ir
raises(TypeError, lambda: 1 in sr) # XXX is this what contains is supposed to do?
# iter
raises(ValueError, lambda: next(iter(sr)))
assert next(iter(ir)) == i
assert sr.intersect(S.Integers) == sr
assert sr.intersect(FiniteSet(x)) == Intersection({x}, sr)
raises(ValueError, lambda: sr[:2])
raises(ValueError, lambda: sr[0])
raises(ValueError, lambda: sr.as_relational(x))
# len
assert len(ir) == ir.size == 10
raises(ValueError, lambda: len(sr))
raises(ValueError, lambda: sr.size)
# bool
assert bool(ir) == bool(sr) == True
# getitem
raises(ValueError, lambda: sr[0])
raises(ValueError, lambda: sr[-1])
raises(ValueError, lambda: sr[:2])
assert ir[:2] == Range(i, i + 4, 2)
assert ir[0] == i
assert ir[-2] == i + 16
assert ir[-1] == i + 18
raises(ValueError, lambda: Range(i)[-1])
assert Range(ip)[-1] == ip - 1
assert ir.inf == i
assert ir.sup == i + 18
assert Range(ip).inf == 0
assert Range(ip).sup == ip - 1
raises(ValueError, lambda: Range(i).inf)
raises(ValueError, lambda: sr.as_relational(x))
assert ir.as_relational(x) == (
x >= i) & Eq(x, floor(x)) & (x <= i + 18)
def test_range_range_intersection():
for a, b, r in [
(Range(0), Range(1), S.EmptySet),
(Range(3), Range(4, oo), S.EmptySet),
(Range(3), Range(-3, -1), S.EmptySet),
(Range(1, 3), Range(0, 3), Range(1, 3)),
(Range(1, 3), Range(1, 4), Range(1, 3)),
(Range(1, oo, 2), Range(2, oo, 2), S.EmptySet),
(Range(0, oo, 2), Range(oo), Range(0, oo, 2)),
(Range(0, oo, 2), Range(100), Range(0, 100, 2)),
(Range(2, oo, 2), Range(oo), Range(2, oo, 2)),
(Range(0, oo, 2), Range(5, 6), S.EmptySet),
(Range(2, 80, 1), Range(55, 71, 4), Range(55, 71, 4)),
(Range(0, 6, 3), Range(-oo, 5, 3), S.EmptySet),
(Range(0, oo, 2), Range(5, oo, 3), Range(8, oo, 6)),
(Range(4, 6, 2), Range(2, 16, 7), S.EmptySet),]:
assert a.intersect(b) == r
assert a.intersect(b.reversed) == r
assert a.reversed.intersect(b) == r
assert a.reversed.intersect(b.reversed) == r
a, b = b, a
assert a.intersect(b) == r
assert a.intersect(b.reversed) == r
assert a.reversed.intersect(b) == r
assert a.reversed.intersect(b.reversed) == r
def test_range_interval_intersection():
p = symbols('p', positive=True)
assert isinstance(Range(3).intersect(Interval(p, p + 2)), Intersection)
assert Range(4).intersect(Interval(0, 3)) == Range(4)
assert Range(4).intersect(Interval(-oo, oo)) == Range(4)
assert Range(4).intersect(Interval(1, oo)) == Range(1, 4)
assert Range(4).intersect(Interval(1.1, oo)) == Range(2, 4)
assert Range(4).intersect(Interval(0.1, 3)) == Range(1, 4)
assert Range(4).intersect(Interval(0.1, 3.1)) == Range(1, 4)
assert Range(4).intersect(Interval.open(0, 3)) == Range(1, 3)
assert Range(4).intersect(Interval.open(0.1, 0.5)) is S.EmptySet
# Null Range intersections
assert Range(0).intersect(Interval(0.2, 0.8)) is S.EmptySet
assert Range(0).intersect(Interval(-oo, oo)) is S.EmptySet
def test_Integers_eval_imageset():
ans = ImageSet(Lambda(x, 2*x + S(3)/7), S.Integers)
im = imageset(Lambda(x, -2*x + S(3)/7), S.Integers)
assert im == ans
im = imageset(Lambda(x, -2*x - S(11)/7), S.Integers)
assert im == ans
y = Symbol('y')
L = imageset(x, 2*x + y, S.Integers)
assert y + 4 in L
_x = symbols('x', negative=True)
eq = _x**2 - _x + 1
assert imageset(_x, eq, S.Integers).lamda.expr == _x**2 + _x + 1
eq = 3*_x - 1
assert imageset(_x, eq, S.Integers).lamda.expr == 3*_x + 2
assert imageset(x, (x, 1/x), S.Integers) == \
ImageSet(Lambda(x, (x, 1/x)), S.Integers)
def test_Range_eval_imageset():
a, b, c = symbols('a b c')
assert imageset(x, a*(x + b) + c, Range(3)) == \
imageset(x, a*x + a*b + c, Range(3))
eq = (x + 1)**2
assert imageset(x, eq, Range(3)).lamda.expr == eq
eq = a*(x + b) + c
r = Range(3, -3, -2)
imset = imageset(x, eq, r)
assert imset.lamda.expr != eq
assert list(imset) == [eq.subs(x, i).expand() for i in list(r)]
def test_fun():
assert (FiniteSet(*ImageSet(Lambda(x, sin(pi*x/4)),
Range(-10, 11))) == FiniteSet(-1, -sqrt(2)/2, 0, sqrt(2)/2, 1))
def test_Reals():
assert 5 in S.Reals
assert S.Pi in S.Reals
assert -sqrt(2) in S.Reals
assert (2, 5) not in S.Reals
assert sqrt(-1) not in S.Reals
assert S.Reals == Interval(-oo, oo)
assert S.Reals != Interval(0, oo)
assert S.Reals.is_subset(Interval(-oo, oo))
def test_Complex():
assert 5 in S.Complexes
assert 5 + 4*I in S.Complexes
assert S.Pi in S.Complexes
assert -sqrt(2) in S.Complexes
assert -I in S.Complexes
assert sqrt(-1) in S.Complexes
assert S.Complexes.intersect(S.Reals) == S.Reals
assert S.Complexes.union(S.Reals) == S.Complexes
assert S.Complexes == ComplexRegion(S.Reals*S.Reals)
assert (S.Complexes == ComplexRegion(Interval(1, 2)*Interval(3, 4))) == False
assert str(S.Complexes) == "S.Complexes"
assert repr(S.Complexes) == "S.Complexes"
def take(n, iterable):
"Return first n items of the iterable as a list"
return list(itertools.islice(iterable, n))
def test_intersections():
assert S.Integers.intersect(S.Reals) == S.Integers
assert 5 in S.Integers.intersect(S.Reals)
assert 5 in S.Integers.intersect(S.Reals)
assert -5 not in S.Naturals.intersect(S.Reals)
assert 5.5 not in S.Integers.intersect(S.Reals)
assert 5 in S.Integers.intersect(Interval(3, oo))
assert -5 in S.Integers.intersect(Interval(-oo, 3))
assert all(x.is_Integer
for x in take(10, S.Integers.intersect(Interval(3, oo)) ))
def test_infinitely_indexed_set_1():
from sympy.abc import n, m, t
assert imageset(Lambda(n, n), S.Integers) == imageset(Lambda(m, m), S.Integers)
assert imageset(Lambda(n, 2*n), S.Integers).intersect(
imageset(Lambda(m, 2*m + 1), S.Integers)) is S.EmptySet
assert imageset(Lambda(n, 2*n), S.Integers).intersect(
imageset(Lambda(n, 2*n + 1), S.Integers)) is S.EmptySet
assert imageset(Lambda(m, 2*m), S.Integers).intersect(
imageset(Lambda(n, 3*n), S.Integers)) == \
ImageSet(Lambda(t, 6*t), S.Integers)
assert imageset(x, x/2 + S(1)/3, S.Integers).intersect(S.Integers) is S.EmptySet
assert imageset(x, x/2 + S.Half, S.Integers).intersect(S.Integers) is S.Integers
def test_infinitely_indexed_set_2():
from sympy.abc import n
a = Symbol('a', integer=True)
assert imageset(Lambda(n, n), S.Integers) == \
imageset(Lambda(n, n + a), S.Integers)
assert imageset(Lambda(n, n + pi), S.Integers) == \
imageset(Lambda(n, n + a + pi), S.Integers)
assert imageset(Lambda(n, n), S.Integers) == \
imageset(Lambda(n, -n + a), S.Integers)
assert imageset(Lambda(n, -6*n), S.Integers) == \
ImageSet(Lambda(n, 6*n), S.Integers)
assert imageset(Lambda(n, 2*n + pi), S.Integers) == \
ImageSet(Lambda(n, 2*n + pi - 2), S.Integers)
def test_imageset_intersect_real():
from sympy import I
from sympy.abc import n
assert imageset(Lambda(n, n + (n - 1)*(n + 1)*I), S.Integers).intersect(S.Reals) == \
FiniteSet(-1, 1)
s = ImageSet(
Lambda(n, -I*(I*(2*pi*n - pi/4) + log(Abs(sqrt(-I))))),
S.Integers)
# s is unevaluated, but after intersection the result
# should be canonical
assert s.intersect(S.Reals) == imageset(
Lambda(n, 2*n*pi - pi/4), S.Integers) == ImageSet(
Lambda(n, 2*pi*n + 7*pi/4), S.Integers)
def test_imageset_intersect_interval():
from sympy.abc import n
f1 = ImageSet(Lambda(n, n*pi), S.Integers)
f2 = ImageSet(Lambda(n, 2*n), Interval(0, pi))
f3 = ImageSet(Lambda(n, 2*n*pi + pi/2), S.Integers)
# complex expressions
f4 = ImageSet(Lambda(n, n*I*pi), S.Integers)
f5 = ImageSet(Lambda(n, 2*I*n*pi + pi/2), S.Integers)
# non-linear expressions
f6 = ImageSet(Lambda(n, log(n)), S.Integers)
f7 = ImageSet(Lambda(n, n**2), S.Integers)
f8 = ImageSet(Lambda(n, Abs(n)), S.Integers)
f9 = ImageSet(Lambda(n, exp(n)), S.Naturals0)
assert f1.intersect(Interval(-1, 1)) == FiniteSet(0)
assert f1.intersect(Interval(0, 2*pi, False, True)) == FiniteSet(0, pi)
assert f2.intersect(Interval(1, 2)) == Interval(1, 2)
assert f3.intersect(Interval(-1, 1)) == S.EmptySet
assert f3.intersect(Interval(-5, 5)) == FiniteSet(-3*pi/2, pi/2)
assert f4.intersect(Interval(-1, 1)) == FiniteSet(0)
assert f4.intersect(Interval(1, 2)) == S.EmptySet
assert f5.intersect(Interval(0, 1)) == S.EmptySet
assert f6.intersect(Interval(0, 1)) == FiniteSet(S.Zero, log(2))
assert f7.intersect(Interval(0, 10)) == Intersection(f7, Interval(0, 10))
assert f8.intersect(Interval(0, 2)) == Intersection(f8, Interval(0, 2))
assert f9.intersect(Interval(1, 2)) == Intersection(f9, Interval(1, 2))
def test_infinitely_indexed_set_3():
from sympy.abc import n, m, t
assert imageset(Lambda(m, 2*pi*m), S.Integers).intersect(
imageset(Lambda(n, 3*pi*n), S.Integers)) == \
ImageSet(Lambda(t, 6*pi*t), S.Integers)
assert imageset(Lambda(n, 2*n + 1), S.Integers) == \
imageset(Lambda(n, 2*n - 1), S.Integers)
assert imageset(Lambda(n, 3*n + 2), S.Integers) == \
imageset(Lambda(n, 3*n - 1), S.Integers)
def test_ImageSet_simplification():
from sympy.abc import n, m
assert imageset(Lambda(n, n), S.Integers) == S.Integers
assert imageset(Lambda(n, sin(n)),
imageset(Lambda(m, tan(m)), S.Integers)) == \
imageset(Lambda(m, sin(tan(m))), S.Integers)
assert imageset(n, 1 + 2*n, S.Naturals) == Range(3, oo, 2)
assert imageset(n, 1 + 2*n, S.Naturals0) == Range(1, oo, 2)
assert imageset(n, 1 - 2*n, S.Naturals) == Range(-1, -oo, -2)
def test_ImageSet_contains():
from sympy.abc import x
assert (2, S.Half) in imageset(x, (x, 1/x), S.Integers)
assert imageset(x, x + I*3, S.Integers).intersection(S.Reals) is S.EmptySet
i = Dummy(integer=True)
q = imageset(x, x + I*y, S.Integers).intersection(S.Reals)
assert q.subs(y, I*i).intersection(S.Integers) is S.Integers
q = imageset(x, x + I*y/x, S.Integers).intersection(S.Reals)
assert q.subs(y, 0) is S.Integers
assert q.subs(y, I*i*x).intersection(S.Integers) is S.Integers
z = cos(1)**2 + sin(1)**2 - 1
q = imageset(x, x + I*z, S.Integers).intersection(S.Reals)
assert q is not S.EmptySet
def test_ComplexRegion_contains():
# contains in ComplexRegion
a = Interval(2, 3)
b = Interval(4, 6)
c = Interval(7, 9)
c1 = ComplexRegion(a*b)
c2 = ComplexRegion(Union(a*b, c*a))
assert 2.5 + 4.5*I in c1
assert 2 + 4*I in c1
assert 3 + 4*I in c1
assert 8 + 2.5*I in c2
assert 2.5 + 6.1*I not in c1
assert 4.5 + 3.2*I not in c1
r1 = Interval(0, 1)
theta1 = Interval(0, 2*S.Pi)
c3 = ComplexRegion(r1*theta1, polar=True)
assert (0.5 + 6*I/10) in c3
assert (S.Half + 6*I/10) in c3
assert (S.Half + .6*I) in c3
assert (0.5 + .6*I) in c3
assert I in c3
assert 1 in c3
assert 0 in c3
assert 1 + I not in c3
assert 1 - I not in c3
raises(ValueError, lambda: ComplexRegion(r1*theta1, polar=2))
def test_ComplexRegion_intersect():
# Polar form
X_axis = ComplexRegion(Interval(0, oo)*FiniteSet(0, S.Pi), polar=True)
unit_disk = ComplexRegion(Interval(0, 1)*Interval(0, 2*S.Pi), polar=True)
upper_half_unit_disk = ComplexRegion(Interval(0, 1)*Interval(0, S.Pi), polar=True)
upper_half_disk = ComplexRegion(Interval(0, oo)*Interval(0, S.Pi), polar=True)
lower_half_disk = ComplexRegion(Interval(0, oo)*Interval(S.Pi, 2*S.Pi), polar=True)
right_half_disk = ComplexRegion(Interval(0, oo)*Interval(-S.Pi/2, S.Pi/2), polar=True)
first_quad_disk = ComplexRegion(Interval(0, oo)*Interval(0, S.Pi/2), polar=True)
assert upper_half_disk.intersect(unit_disk) == upper_half_unit_disk
assert right_half_disk.intersect(first_quad_disk) == first_quad_disk
assert upper_half_disk.intersect(right_half_disk) == first_quad_disk
assert upper_half_disk.intersect(lower_half_disk) == X_axis
c1 = ComplexRegion(Interval(0, 4)*Interval(0, 2*S.Pi), polar=True)
assert c1.intersect(Interval(1, 5)) == Interval(1, 4)
assert c1.intersect(Interval(4, 9)) == FiniteSet(4)
assert c1.intersect(Interval(5, 12)) is S.EmptySet
# Rectangular form
X_axis = ComplexRegion(Interval(-oo, oo)*FiniteSet(0))
unit_square = ComplexRegion(Interval(-1, 1)*Interval(-1, 1))
upper_half_unit_square = ComplexRegion(Interval(-1, 1)*Interval(0, 1))
upper_half_plane = ComplexRegion(Interval(-oo, oo)*Interval(0, oo))
lower_half_plane = ComplexRegion(Interval(-oo, oo)*Interval(-oo, 0))
right_half_plane = ComplexRegion(Interval(0, oo)*Interval(-oo, oo))
first_quad_plane = ComplexRegion(Interval(0, oo)*Interval(0, oo))
assert upper_half_plane.intersect(unit_square) == upper_half_unit_square
assert right_half_plane.intersect(first_quad_plane) == first_quad_plane
assert upper_half_plane.intersect(right_half_plane) == first_quad_plane
assert upper_half_plane.intersect(lower_half_plane) == X_axis
c1 = ComplexRegion(Interval(-5, 5)*Interval(-10, 10))
assert c1.intersect(Interval(2, 7)) == Interval(2, 5)
assert c1.intersect(Interval(5, 7)) == FiniteSet(5)
assert c1.intersect(Interval(6, 9)) is S.EmptySet
# unevaluated object
C1 = ComplexRegion(Interval(0, 1)*Interval(0, 2*S.Pi), polar=True)
C2 = ComplexRegion(Interval(-1, 1)*Interval(-1, 1))
assert C1.intersect(C2) == Intersection(C1, C2, evaluate=False)
def test_ComplexRegion_union():
# Polar form
c1 = ComplexRegion(Interval(0, 1)*Interval(0, 2*S.Pi), polar=True)
c2 = ComplexRegion(Interval(0, 1)*Interval(0, S.Pi), polar=True)
c3 = ComplexRegion(Interval(0, oo)*Interval(0, S.Pi), polar=True)
c4 = ComplexRegion(Interval(0, oo)*Interval(S.Pi, 2*S.Pi), polar=True)
p1 = Union(Interval(0, 1)*Interval(0, 2*S.Pi), Interval(0, 1)*Interval(0, S.Pi))
p2 = Union(Interval(0, oo)*Interval(0, S.Pi), Interval(0, oo)*Interval(S.Pi, 2*S.Pi))
assert c1.union(c2) == ComplexRegion(p1, polar=True)
assert c3.union(c4) == ComplexRegion(p2, polar=True)
# Rectangular form
c5 = ComplexRegion(Interval(2, 5)*Interval(6, 9))
c6 = ComplexRegion(Interval(4, 6)*Interval(10, 12))
c7 = ComplexRegion(Interval(0, 10)*Interval(-10, 0))
c8 = ComplexRegion(Interval(12, 16)*Interval(14, 20))
p3 = Union(Interval(2, 5)*Interval(6, 9), Interval(4, 6)*Interval(10, 12))
p4 = Union(Interval(0, 10)*Interval(-10, 0), Interval(12, 16)*Interval(14, 20))
assert c5.union(c6) == ComplexRegion(p3)
assert c7.union(c8) == ComplexRegion(p4)
assert c1.union(Interval(2, 4)) == Union(c1, Interval(2, 4), evaluate=False)
assert c5.union(Interval(2, 4)) == Union(c5, ComplexRegion.from_real(Interval(2, 4)))
def test_ComplexRegion_from_real():
c1 = ComplexRegion(Interval(0, 1) * Interval(0, 2 * S.Pi), polar=True)
raises(ValueError, lambda: c1.from_real(c1))
assert c1.from_real(Interval(-1, 1)) == ComplexRegion(Interval(-1, 1) * FiniteSet(0), False)
def test_ComplexRegion_measure():
a, b = Interval(2, 5), Interval(4, 8)
theta1, theta2 = Interval(0, 2*S.Pi), Interval(0, S.Pi)
c1 = ComplexRegion(a*b)
c2 = ComplexRegion(Union(a*theta1, b*theta2), polar=True)
assert c1.measure == 12
assert c2.measure == 9*pi
def test_normalize_theta_set():
# Interval
assert normalize_theta_set(Interval(pi, 2*pi)) == \
Union(FiniteSet(0), Interval.Ropen(pi, 2*pi))
assert normalize_theta_set(Interval(9*pi/2, 5*pi)) == Interval(pi/2, pi)
assert normalize_theta_set(Interval(-3*pi/2, pi/2)) == Interval.Ropen(0, 2*pi)
assert normalize_theta_set(Interval.open(-3*pi/2, pi/2)) == \
Union(Interval.Ropen(0, pi/2), Interval.open(pi/2, 2*pi))
assert normalize_theta_set(Interval.open(-7*pi/2, -3*pi/2)) == \
Union(Interval.Ropen(0, pi/2), Interval.open(pi/2, 2*pi))
assert normalize_theta_set(Interval(-pi/2, pi/2)) == \
Union(Interval(0, pi/2), Interval.Ropen(3*pi/2, 2*pi))
assert normalize_theta_set(Interval.open(-pi/2, pi/2)) == \
Union(Interval.Ropen(0, pi/2), Interval.open(3*pi/2, 2*pi))
assert normalize_theta_set(Interval(-4*pi, 3*pi)) == Interval.Ropen(0, 2*pi)
assert normalize_theta_set(Interval(-3*pi/2, -pi/2)) == Interval(pi/2, 3*pi/2)
assert normalize_theta_set(Interval.open(0, 2*pi)) == Interval.open(0, 2*pi)
assert normalize_theta_set(Interval.Ropen(-pi/2, pi/2)) == \
Union(Interval.Ropen(0, pi/2), Interval.Ropen(3*pi/2, 2*pi))
assert normalize_theta_set(Interval.Lopen(-pi/2, pi/2)) == \
Union(Interval(0, pi/2), Interval.open(3*pi/2, 2*pi))
assert normalize_theta_set(Interval(-pi/2, pi/2)) == \
Union(Interval(0, pi/2), Interval.Ropen(3*pi/2, 2*pi))
assert normalize_theta_set(Interval.open(4*pi, 9*pi/2)) == Interval.open(0, pi/2)
assert normalize_theta_set(Interval.Lopen(4*pi, 9*pi/2)) == Interval.Lopen(0, pi/2)
assert normalize_theta_set(Interval.Ropen(4*pi, 9*pi/2)) == Interval.Ropen(0, pi/2)
assert normalize_theta_set(Interval.open(3*pi, 5*pi)) == \
Union(Interval.Ropen(0, pi), Interval.open(pi, 2*pi))
# FiniteSet
assert normalize_theta_set(FiniteSet(0, pi, 3*pi)) == FiniteSet(0, pi)
assert normalize_theta_set(FiniteSet(0, pi/2, pi, 2*pi)) == FiniteSet(0, pi/2, pi)
assert normalize_theta_set(FiniteSet(0, -pi/2, -pi, -2*pi)) == FiniteSet(0, pi, 3*pi/2)
assert normalize_theta_set(FiniteSet(-3*pi/2, pi/2)) == \
FiniteSet(pi/2)
assert normalize_theta_set(FiniteSet(2*pi)) == FiniteSet(0)
# Unions
assert normalize_theta_set(Union(Interval(0, pi/3), Interval(pi/2, pi))) == \
Union(Interval(0, pi/3), Interval(pi/2, pi))
assert normalize_theta_set(Union(Interval(0, pi), Interval(2*pi, 7*pi/3))) == \
Interval(0, pi)
# ValueError for non-real sets
raises(ValueError, lambda: normalize_theta_set(S.Complexes))
# NotImplementedError for subset of reals
raises(NotImplementedError, lambda: normalize_theta_set(Interval(0, 1)))
# NotImplementedError without pi as coefficient
raises(NotImplementedError, lambda: normalize_theta_set(Interval(1, 2*pi)))
raises(NotImplementedError, lambda: normalize_theta_set(Interval(2*pi, 10)))
raises(NotImplementedError, lambda: normalize_theta_set(FiniteSet(0, 3, 3*pi)))
def test_ComplexRegion_FiniteSet():
x, y, z, a, b, c = symbols('x y z a b c')
# Issue #9669
assert ComplexRegion(FiniteSet(a, b, c)*FiniteSet(x, y, z)) == \
FiniteSet(a + I*x, a + I*y, a + I*z, b + I*x, b + I*y,
b + I*z, c + I*x, c + I*y, c + I*z)
assert ComplexRegion(FiniteSet(2)*FiniteSet(3)) == FiniteSet(2 + 3*I)
def test_union_RealSubSet():
assert (S.Complexes).union(Interval(1, 2)) == S.Complexes
assert (S.Complexes).union(S.Integers) == S.Complexes
def test_issue_9980():
c1 = ComplexRegion(Interval(1, 2)*Interval(2, 3))
c2 = ComplexRegion(Interval(1, 5)*Interval(1, 3))
R = Union(c1, c2)
assert simplify(R) == ComplexRegion(Union(Interval(1, 2)*Interval(2, 3), \
Interval(1, 5)*Interval(1, 3)), False)
assert c1.func(*c1.args) == c1
assert R.func(*R.args) == R
def test_issue_11732():
interval12 = Interval(1, 2)
finiteset1234 = FiniteSet(1, 2, 3, 4)
pointComplex = Tuple(1, 5)
assert (interval12 in S.Naturals) == False
assert (interval12 in S.Naturals0) == False
assert (interval12 in S.Integers) == False
assert (interval12 in S.Complexes) == False
assert (finiteset1234 in S.Naturals) == False
assert (finiteset1234 in S.Naturals0) == False
assert (finiteset1234 in S.Integers) == False
assert (finiteset1234 in S.Complexes) == False
assert (pointComplex in S.Naturals) == False
assert (pointComplex in S.Naturals0) == False
assert (pointComplex in S.Integers) == False
assert (pointComplex in S.Complexes) == True
def test_issue_11730():
unit = Interval(0, 1)
square = ComplexRegion(unit ** 2)
assert Union(S.Complexes, FiniteSet(oo)) != S.Complexes
assert Union(S.Complexes, FiniteSet(eye(4))) != S.Complexes
assert Union(unit, square) == square
assert Intersection(S.Reals, square) == unit
def test_issue_11938():
unit = Interval(0, 1)
ival = Interval(1, 2)
cr1 = ComplexRegion(ival * unit)
assert Intersection(cr1, S.Reals) == ival
assert Intersection(cr1, unit) == FiniteSet(1)
arg1 = Interval(0, S.Pi)
arg2 = FiniteSet(S.Pi)
arg3 = Interval(S.Pi / 4, 3 * S.Pi / 4)
cp1 = ComplexRegion(unit * arg1, polar=True)
cp2 = ComplexRegion(unit * arg2, polar=True)
cp3 = ComplexRegion(unit * arg3, polar=True)
assert Intersection(cp1, S.Reals) == Interval(-1, 1)
assert Intersection(cp2, S.Reals) == Interval(-1, 0)
assert Intersection(cp3, S.Reals) == FiniteSet(0)
def test_issue_11914():
a, b = Interval(0, 1), Interval(0, pi)
c, d = Interval(2, 3), Interval(pi, 3 * pi / 2)
cp1 = ComplexRegion(a * b, polar=True)
cp2 = ComplexRegion(c * d, polar=True)
assert -3 in cp1.union(cp2)
assert -3 in cp2.union(cp1)
assert -5 not in cp1.union(cp2)
def test_issue_9543():
assert ImageSet(Lambda(x, x**2), S.Naturals).is_subset(S.Reals)
def test_issue_16871():
assert ImageSet(Lambda(x, x), FiniteSet(1)) == {1}
assert ImageSet(Lambda(x, x - 3), S.Integers
).intersection(S.Integers) is S.Integers
@XFAIL
def test_issue_16871b():
assert ImageSet(Lambda(x, x - 3), S.Integers).is_subset(S.Integers)
def test_no_mod_on_imaginary():
assert imageset(Lambda(x, 2*x + 3*I), S.Integers
) == ImageSet(Lambda(x, 2*x + I), S.Integers)
def test_Rationals():
assert S.Integers.is_subset(S.Rationals)
assert S.Naturals.is_subset(S.Rationals)
assert S.Naturals0.is_subset(S.Rationals)
assert S.Rationals.is_subset(S.Reals)
assert S.Rationals.inf == -oo
assert S.Rationals.sup == oo
it = iter(S.Rationals)
assert [next(it) for i in range(12)] == [
0, 1, -1, S(1)/2, 2, -S(1)/2, -2,
S(1)/3, 3, -S(1)/3, -3, S(2)/3]
assert Basic() not in S.Rationals
assert S.Half in S.Rationals
assert 1.0 not in S.Rationals
assert 2 in S.Rationals
r = symbols('r', rational=True)
assert r in S.Rationals
raises(TypeError, lambda: x in S.Rationals)
assert S.Rationals.boundary == S.Rationals
def test_imageset_intersection():
n = Dummy()
s = ImageSet(Lambda(n, -I*(I*(2*pi*n - pi/4) +
log(Abs(sqrt(-I))))), S.Integers)
assert s.intersect(S.Reals) == ImageSet(
Lambda(n, 2*pi*n + 7*pi/4), S.Integers)
|
e1ffa9f9c3bddd607de3e64b227f37ed5bea4731c7e32421e3bb53cb6301ab85 | from sympy import (Symbol, Set, Union, Interval, oo, S, sympify, nan,
Max, Min, Float,
FiniteSet, Intersection, imageset, I, true, false, ProductSet,
sqrt, Complement, EmptySet, sin, cos, Lambda, ImageSet, pi,
Pow, Contains, Sum, rootof, SymmetricDifference, Piecewise,
Matrix, Range, Add, symbols, zoo)
from mpmath import mpi
from sympy.core.compatibility import range
from sympy.core.expr import unchanged
from sympy.core.relational import \
Eq, Ne, Le, Lt, LessThan
from sympy.logic import And, Or, Xor
from sympy.utilities.pytest import raises, XFAIL, warns_deprecated_sympy
from sympy.abc import x, y, z, m, n
def test_imageset():
ints = S.Integers
assert imageset(x, x - 1, S.Naturals) is S.Naturals0
assert imageset(x, x + 1, S.Naturals0) is S.Naturals
assert imageset(x, abs(x), S.Naturals0) is S.Naturals0
assert imageset(x, abs(x), S.Naturals) is S.Naturals
assert imageset(x, abs(x), S.Integers) is S.Naturals0
# issue 16878a
r = symbols('r', real=True)
assert imageset(x, (x, x), S.Reals)._contains((1, r)) == None
assert imageset(x, (x, x), S.Reals)._contains((1, 2)) == False
assert (r, r) in imageset(x, (x, x), S.Reals)
assert 1 + I in imageset(x, x + I, S.Reals)
assert {1} not in imageset(x, (x,), S.Reals)
assert (1, 1) not in imageset(x, (x,) , S.Reals)
raises(TypeError, lambda: imageset(x, ints))
raises(ValueError, lambda: imageset(x, y, z, ints))
raises(ValueError, lambda: imageset(Lambda(x, cos(x)), y))
raises(ValueError, lambda: imageset(Lambda(x, x), ints, ints))
assert imageset(cos, ints) == ImageSet(Lambda(x, cos(x)), ints)
def f(x):
return cos(x)
assert imageset(f, ints) == imageset(x, cos(x), ints)
f = lambda x: cos(x)
assert imageset(f, ints) == ImageSet(Lambda(x, cos(x)), ints)
assert imageset(x, 1, ints) == FiniteSet(1)
assert imageset(x, y, ints) == {y}
assert imageset((x, y), (1, z), ints*S.Reals) == {(1, z)}
clash = Symbol('x', integer=true)
assert (str(imageset(lambda x: x + clash, Interval(-2, 1)).lamda.expr)
in ('_x + x', 'x + _x'))
x1, x2 = symbols("x1, x2")
assert imageset(lambda x,y: Add(x,y), Interval(1,2), Interval(2, 3)) == \
ImageSet(Lambda((x1, x2), x1+x2), Interval(1,2), Interval(2,3))
def test_is_empty():
for s in [S.Naturals, S.Naturals0, S.Integers, S.Rationals, S.Reals,
S.UniversalSet]:
assert s.is_empty == False
def test_deprecated_is_EmptySet():
with warns_deprecated_sympy():
S.EmptySet.is_EmptySet
def test_interval_arguments():
assert Interval(0, oo) == Interval(0, oo, False, True)
assert Interval(0, oo).right_open is true
assert Interval(-oo, 0) == Interval(-oo, 0, True, False)
assert Interval(-oo, 0).left_open is true
assert Interval(oo, -oo) == S.EmptySet
assert Interval(oo, oo) == S.EmptySet
assert Interval(-oo, -oo) == S.EmptySet
assert Interval(oo, x) == S.EmptySet
assert Interval(oo, oo) == S.EmptySet
assert Interval(x, -oo) == S.EmptySet
assert Interval(x, x) == {x}
assert isinstance(Interval(1, 1), FiniteSet)
e = Sum(x, (x, 1, 3))
assert isinstance(Interval(e, e), FiniteSet)
assert Interval(1, 0) == S.EmptySet
assert Interval(1, 1).measure == 0
assert Interval(1, 1, False, True) == S.EmptySet
assert Interval(1, 1, True, False) == S.EmptySet
assert Interval(1, 1, True, True) == S.EmptySet
assert isinstance(Interval(0, Symbol('a')), Interval)
assert Interval(Symbol('a', real=True, positive=True), 0) == S.EmptySet
raises(ValueError, lambda: Interval(0, S.ImaginaryUnit))
raises(ValueError, lambda: Interval(0, Symbol('z', extended_real=False)))
raises(NotImplementedError, lambda: Interval(0, 1, And(x, y)))
raises(NotImplementedError, lambda: Interval(0, 1, False, And(x, y)))
raises(NotImplementedError, lambda: Interval(0, 1, z, And(x, y)))
def test_interval_symbolic_end_points():
a = Symbol('a', real=True)
assert Union(Interval(0, a), Interval(0, 3)).sup == Max(a, 3)
assert Union(Interval(a, 0), Interval(-3, 0)).inf == Min(-3, a)
assert Interval(0, a).contains(1) == LessThan(1, a)
def test_interval_is_empty():
x, y = symbols('x, y')
r = Symbol('r', real=True)
p = Symbol('p', positive=True)
n = Symbol('n', negative=True)
nn = Symbol('nn', nonnegative=True)
assert Interval(1, 2).is_empty == False
assert Interval(3, 3).is_empty == False # FiniteSet
assert Interval(r, r).is_empty == False # FiniteSet
assert Interval(r, r + nn).is_empty == False
assert Interval(x, x).is_empty == False
assert Interval(1, oo).is_empty == False
assert Interval(-oo, oo).is_empty == False
assert Interval(-oo, 1).is_empty == False
assert Interval(x, y).is_empty == None
assert Interval(r, oo).is_empty == False # real implies finite
assert Interval(n, 0).is_empty == False
assert Interval(n, 0, left_open=True).is_empty == False
assert Interval(p, 0).is_empty == True # EmptySet
assert Interval(nn, 0).is_empty == None
assert Interval(n, p).is_empty == False
assert Interval(0, p, left_open=True).is_empty == False
assert Interval(0, p, right_open=True).is_empty == False
assert Interval(0, nn, left_open=True).is_empty == None
assert Interval(0, nn, right_open=True).is_empty == None
def test_union():
assert Union(Interval(1, 2), Interval(2, 3)) == Interval(1, 3)
assert Union(Interval(1, 2), Interval(2, 3, True)) == Interval(1, 3)
assert Union(Interval(1, 3), Interval(2, 4)) == Interval(1, 4)
assert Union(Interval(1, 2), Interval(1, 3)) == Interval(1, 3)
assert Union(Interval(1, 3), Interval(1, 2)) == Interval(1, 3)
assert Union(Interval(1, 3, False, True), Interval(1, 2)) == \
Interval(1, 3, False, True)
assert Union(Interval(1, 3), Interval(1, 2, False, True)) == Interval(1, 3)
assert Union(Interval(1, 2, True), Interval(1, 3)) == Interval(1, 3)
assert Union(Interval(1, 2, True), Interval(1, 3, True)) == \
Interval(1, 3, True)
assert Union(Interval(1, 2, True), Interval(1, 3, True, True)) == \
Interval(1, 3, True, True)
assert Union(Interval(1, 2, True, True), Interval(1, 3, True)) == \
Interval(1, 3, True)
assert Union(Interval(1, 3), Interval(2, 3)) == Interval(1, 3)
assert Union(Interval(1, 3, False, True), Interval(2, 3)) == \
Interval(1, 3)
assert Union(Interval(1, 2, False, True), Interval(2, 3, True)) != \
Interval(1, 3)
assert Union(Interval(1, 2), S.EmptySet) == Interval(1, 2)
assert Union(S.EmptySet) == S.EmptySet
assert Union(Interval(0, 1), *[FiniteSet(1.0/n) for n in range(1, 10)]) == \
Interval(0, 1)
assert Interval(1, 2).union(Interval(2, 3)) == \
Interval(1, 2) + Interval(2, 3)
assert Interval(1, 2).union(Interval(2, 3)) == Interval(1, 3)
assert Union(Set()) == Set()
assert FiniteSet(1) + FiniteSet(2) + FiniteSet(3) == FiniteSet(1, 2, 3)
assert FiniteSet('ham') + FiniteSet('eggs') == FiniteSet('ham', 'eggs')
assert FiniteSet(1, 2, 3) + S.EmptySet == FiniteSet(1, 2, 3)
assert FiniteSet(1, 2, 3) & FiniteSet(2, 3, 4) == FiniteSet(2, 3)
assert FiniteSet(1, 2, 3) | FiniteSet(2, 3, 4) == FiniteSet(1, 2, 3, 4)
x = Symbol("x")
y = Symbol("y")
z = Symbol("z")
assert S.EmptySet | FiniteSet(x, FiniteSet(y, z)) == \
FiniteSet(x, FiniteSet(y, z))
# Test that Intervals and FiniteSets play nicely
assert Interval(1, 3) + FiniteSet(2) == Interval(1, 3)
assert Interval(1, 3, True, True) + FiniteSet(3) == \
Interval(1, 3, True, False)
X = Interval(1, 3) + FiniteSet(5)
Y = Interval(1, 2) + FiniteSet(3)
XandY = X.intersect(Y)
assert 2 in X and 3 in X and 3 in XandY
assert XandY.is_subset(X) and XandY.is_subset(Y)
raises(TypeError, lambda: Union(1, 2, 3))
assert X.is_iterable is False
# issue 7843
assert Union(S.EmptySet, FiniteSet(-sqrt(-I), sqrt(-I))) == \
FiniteSet(-sqrt(-I), sqrt(-I))
assert Union(S.Reals, S.Integers) == S.Reals
def test_union_iter():
# Use Range because it is ordered
u = Union(Range(3), Range(5), Range(4), evaluate=False)
# Round robin
assert list(u) == [0, 0, 0, 1, 1, 1, 2, 2, 2, 3, 3, 4]
def test_union_is_empty():
assert (Interval(x, y) + FiniteSet(1)).is_empty == False
assert (Interval(x, y) + Interval(-x, y)).is_empty == None
def test_difference():
assert Interval(1, 3) - Interval(1, 2) == Interval(2, 3, True)
assert Interval(1, 3) - Interval(2, 3) == Interval(1, 2, False, True)
assert Interval(1, 3, True) - Interval(2, 3) == Interval(1, 2, True, True)
assert Interval(1, 3, True) - Interval(2, 3, True) == \
Interval(1, 2, True, False)
assert Interval(0, 2) - FiniteSet(1) == \
Union(Interval(0, 1, False, True), Interval(1, 2, True, False))
assert FiniteSet(1, 2, 3) - FiniteSet(2) == FiniteSet(1, 3)
assert FiniteSet('ham', 'eggs') - FiniteSet('eggs') == FiniteSet('ham')
assert FiniteSet(1, 2, 3, 4) - Interval(2, 10, True, False) == \
FiniteSet(1, 2)
assert FiniteSet(1, 2, 3, 4) - S.EmptySet == FiniteSet(1, 2, 3, 4)
assert Union(Interval(0, 2), FiniteSet(2, 3, 4)) - Interval(1, 3) == \
Union(Interval(0, 1, False, True), FiniteSet(4))
assert -1 in S.Reals - S.Naturals
def test_Complement():
assert Complement(Interval(1, 3), Interval(1, 2)) == Interval(2, 3, True)
assert Complement(FiniteSet(1, 3, 4), FiniteSet(3, 4)) == FiniteSet(1)
assert Complement(Union(Interval(0, 2), FiniteSet(2, 3, 4)),
Interval(1, 3)) == \
Union(Interval(0, 1, False, True), FiniteSet(4))
assert not 3 in Complement(Interval(0, 5), Interval(1, 4), evaluate=False)
assert -1 in Complement(S.Reals, S.Naturals, evaluate=False)
assert not 1 in Complement(S.Reals, S.Naturals, evaluate=False)
assert Complement(S.Integers, S.UniversalSet) == EmptySet()
assert S.UniversalSet.complement(S.Integers) == EmptySet()
assert (not 0 in S.Reals.intersect(S.Integers - FiniteSet(0)))
assert S.EmptySet - S.Integers == S.EmptySet
assert (S.Integers - FiniteSet(0)) - FiniteSet(1) == S.Integers - FiniteSet(0, 1)
assert S.Reals - Union(S.Naturals, FiniteSet(pi)) == \
Intersection(S.Reals - S.Naturals, S.Reals - FiniteSet(pi))
# issue 12712
assert Complement(FiniteSet(x, y, 2), Interval(-10, 10)) == \
Complement(FiniteSet(x, y), Interval(-10, 10))
A = FiniteSet(*symbols('a:c'))
B = FiniteSet(*symbols('d:f'))
assert unchanged(Complement, ProductSet(A, A), B)
A2 = ProductSet(A, A)
B3 = ProductSet(B, B, B)
assert A2 - B3 == A2
assert B3 - A2 == B3
def test_complement():
assert Interval(0, 1).complement(S.Reals) == \
Union(Interval(-oo, 0, True, True), Interval(1, oo, True, True))
assert Interval(0, 1, True, False).complement(S.Reals) == \
Union(Interval(-oo, 0, True, False), Interval(1, oo, True, True))
assert Interval(0, 1, False, True).complement(S.Reals) == \
Union(Interval(-oo, 0, True, True), Interval(1, oo, False, True))
assert Interval(0, 1, True, True).complement(S.Reals) == \
Union(Interval(-oo, 0, True, False), Interval(1, oo, False, True))
assert S.UniversalSet.complement(S.EmptySet) == S.EmptySet
assert S.UniversalSet.complement(S.Reals) == S.EmptySet
assert S.UniversalSet.complement(S.UniversalSet) == S.EmptySet
assert S.EmptySet.complement(S.Reals) == S.Reals
assert Union(Interval(0, 1), Interval(2, 3)).complement(S.Reals) == \
Union(Interval(-oo, 0, True, True), Interval(1, 2, True, True),
Interval(3, oo, True, True))
assert FiniteSet(0).complement(S.Reals) == \
Union(Interval(-oo, 0, True, True), Interval(0, oo, True, True))
assert (FiniteSet(5) + Interval(S.NegativeInfinity,
0)).complement(S.Reals) == \
Interval(0, 5, True, True) + Interval(5, S.Infinity, True, True)
assert FiniteSet(1, 2, 3).complement(S.Reals) == \
Interval(S.NegativeInfinity, 1, True, True) + \
Interval(1, 2, True, True) + Interval(2, 3, True, True) +\
Interval(3, S.Infinity, True, True)
assert FiniteSet(x).complement(S.Reals) == Complement(S.Reals, FiniteSet(x))
assert FiniteSet(0, x).complement(S.Reals) == Complement(Interval(-oo, 0, True, True) +
Interval(0, oo, True, True)
,FiniteSet(x), evaluate=False)
square = Interval(0, 1) * Interval(0, 1)
notsquare = square.complement(S.Reals*S.Reals)
assert all(pt in square for pt in [(0, 0), (.5, .5), (1, 0), (1, 1)])
assert not any(
pt in notsquare for pt in [(0, 0), (.5, .5), (1, 0), (1, 1)])
assert not any(pt in square for pt in [(-1, 0), (1.5, .5), (10, 10)])
assert all(pt in notsquare for pt in [(-1, 0), (1.5, .5), (10, 10)])
def test_intersect1():
assert all(S.Integers.intersection(i) is i for i in
(S.Naturals, S.Naturals0))
assert all(i.intersection(S.Integers) is i for i in
(S.Naturals, S.Naturals0))
s = S.Naturals0
assert S.Naturals.intersection(s) is S.Naturals
assert s.intersection(S.Naturals) is S.Naturals
x = Symbol('x')
assert Interval(0, 2).intersect(Interval(1, 2)) == Interval(1, 2)
assert Interval(0, 2).intersect(Interval(1, 2, True)) == \
Interval(1, 2, True)
assert Interval(0, 2, True).intersect(Interval(1, 2)) == \
Interval(1, 2, False, False)
assert Interval(0, 2, True, True).intersect(Interval(1, 2)) == \
Interval(1, 2, False, True)
assert Interval(0, 2).intersect(Union(Interval(0, 1), Interval(2, 3))) == \
Union(Interval(0, 1), Interval(2, 2))
assert FiniteSet(1, 2).intersect(FiniteSet(1, 2, 3)) == FiniteSet(1, 2)
assert FiniteSet(1, 2, x).intersect(FiniteSet(x)) == FiniteSet(x)
assert FiniteSet('ham', 'eggs').intersect(FiniteSet('ham')) == \
FiniteSet('ham')
assert FiniteSet(1, 2, 3, 4, 5).intersect(S.EmptySet) == S.EmptySet
assert Interval(0, 5).intersect(FiniteSet(1, 3)) == FiniteSet(1, 3)
assert Interval(0, 1, True, True).intersect(FiniteSet(1)) == S.EmptySet
assert Union(Interval(0, 1), Interval(2, 3)).intersect(Interval(1, 2)) == \
Union(Interval(1, 1), Interval(2, 2))
assert Union(Interval(0, 1), Interval(2, 3)).intersect(Interval(0, 2)) == \
Union(Interval(0, 1), Interval(2, 2))
assert Union(Interval(0, 1), Interval(2, 3)).intersect(Interval(1, 2, True, True)) == \
S.EmptySet
assert Union(Interval(0, 1), Interval(2, 3)).intersect(S.EmptySet) == \
S.EmptySet
assert Union(Interval(0, 5), FiniteSet('ham')).intersect(FiniteSet(2, 3, 4, 5, 6)) == \
Intersection(FiniteSet(2, 3, 4, 5, 6), Union(FiniteSet('ham'), Interval(0, 5)))
assert Intersection(FiniteSet(1, 2, 3), Interval(2, x), Interval(3, y)) == \
Intersection(FiniteSet(3), Interval(2, x), Interval(3, y), evaluate=False)
assert Intersection(FiniteSet(1, 2), Interval(0, 3), Interval(x, y)) == \
Intersection({1, 2}, Interval(x, y), evaluate=False)
assert Intersection(FiniteSet(1, 2, 4), Interval(0, 3), Interval(x, y)) == \
Intersection({1, 2}, Interval(x, y), evaluate=False)
# XXX: Is the real=True necessary here?
# https://github.com/sympy/sympy/issues/17532
m, n = symbols('m, n', real=True)
assert Intersection(FiniteSet(m), FiniteSet(m, n), Interval(m, m+1)) == \
FiniteSet(m)
# issue 8217
assert Intersection(FiniteSet(x), FiniteSet(y)) == \
Intersection(FiniteSet(x), FiniteSet(y), evaluate=False)
assert FiniteSet(x).intersect(S.Reals) == \
Intersection(S.Reals, FiniteSet(x), evaluate=False)
# tests for the intersection alias
assert Interval(0, 5).intersection(FiniteSet(1, 3)) == FiniteSet(1, 3)
assert Interval(0, 1, True, True).intersection(FiniteSet(1)) == S.EmptySet
assert Union(Interval(0, 1), Interval(2, 3)).intersection(Interval(1, 2)) == \
Union(Interval(1, 1), Interval(2, 2))
def test_intersection():
# iterable
i = Intersection(FiniteSet(1, 2, 3), Interval(2, 5), evaluate=False)
assert i.is_iterable
assert set(i) == {S(2), S(3)}
# challenging intervals
x = Symbol('x', real=True)
i = Intersection(Interval(0, 3), Interval(x, 6))
assert (5 in i) is False
raises(TypeError, lambda: 2 in i)
# Singleton special cases
assert Intersection(Interval(0, 1), S.EmptySet) == S.EmptySet
assert Intersection(Interval(-oo, oo), Interval(-oo, x)) == Interval(-oo, x)
# Products
line = Interval(0, 5)
i = Intersection(line**2, line**3, evaluate=False)
assert (2, 2) not in i
assert (2, 2, 2) not in i
raises(ValueError, lambda: list(i))
a = Intersection(Intersection(S.Integers, S.Naturals, evaluate=False), S.Reals, evaluate=False)
assert a._argset == frozenset([Intersection(S.Naturals, S.Integers, evaluate=False), S.Reals])
assert Intersection(S.Complexes, FiniteSet(S.ComplexInfinity)) == S.EmptySet
# issue 12178
assert Intersection() == S.UniversalSet
# issue 16987
assert Intersection({1}, {1}, {x}) == Intersection({1}, {x})
def test_issue_9623():
n = Symbol('n')
a = S.Reals
b = Interval(0, oo)
c = FiniteSet(n)
assert Intersection(a, b, c) == Intersection(b, c)
assert Intersection(Interval(1, 2), Interval(3, 4), FiniteSet(n)) == EmptySet()
def test_is_disjoint():
assert Interval(0, 2).is_disjoint(Interval(1, 2)) == False
assert Interval(0, 2).is_disjoint(Interval(3, 4)) == True
def test_ProductSet():
# ProductSet is always a set of Tuples
assert ProductSet(S.Reals) == S.Reals ** 1
assert ProductSet(S.Reals, S.Reals) == S.Reals ** 2
assert ProductSet(S.Reals, S.Reals, S.Reals) == S.Reals ** 3
assert ProductSet(S.Reals) != S.Reals
assert ProductSet(S.Reals, S.Reals) == S.Reals * S.Reals
assert ProductSet(S.Reals, S.Reals, S.Reals) != S.Reals * S.Reals * S.Reals
assert ProductSet(S.Reals, S.Reals, S.Reals) == (S.Reals * S.Reals * S.Reals).flatten()
assert 1 not in ProductSet(S.Reals)
assert (1,) in ProductSet(S.Reals)
assert 1 not in ProductSet(S.Reals, S.Reals)
assert (1, 2) in ProductSet(S.Reals, S.Reals)
assert (1, I) not in ProductSet(S.Reals, S.Reals)
assert (1, 2, 3) in ProductSet(S.Reals, S.Reals, S.Reals)
assert (1, 2, 3) in S.Reals ** 3
assert (1, 2, 3) not in S.Reals * S.Reals * S.Reals
assert ((1, 2), 3) in S.Reals * S.Reals * S.Reals
assert (1, (2, 3)) not in S.Reals * S.Reals * S.Reals
assert (1, (2, 3)) in S.Reals * (S.Reals * S.Reals)
assert ProductSet() == FiniteSet(())
assert ProductSet(S.Reals, S.EmptySet) == S.EmptySet
# See GH-17458
for n in range(5):
Rn = ProductSet(*(S.Reals,) * n)
assert (1,) * n in Rn
assert 1 not in Rn
assert (S.Reals * S.Reals) * S.Reals != S.Reals * (S.Reals * S.Reals)
S1 = S.Reals
S2 = S.Integers
x1 = pi
x2 = 3
assert x1 in S1
assert x2 in S2
assert (x1, x2) in S1 * S2
S3 = S1 * S2
x3 = (x1, x2)
assert x3 in S3
assert (x3, x3) in S3 * S3
assert x3 + x3 not in S3 * S3
raises(ValueError, lambda: S.Reals**-1)
with warns_deprecated_sympy():
ProductSet(FiniteSet(s) for s in range(2))
raises(TypeError, lambda: ProductSet(None))
S1 = FiniteSet(1, 2)
S2 = FiniteSet(3, 4)
S3 = ProductSet(S1, S2)
assert (S3.as_relational(x, y)
== And(S1.as_relational(x), S2.as_relational(y))
== And(Or(Eq(x, 1), Eq(x, 2)), Or(Eq(y, 3), Eq(y, 4))))
raises(ValueError, lambda: S3.as_relational(x))
raises(ValueError, lambda: S3.as_relational(x, 1))
raises(ValueError, lambda: ProductSet(Interval(0, 1)).as_relational(x, y))
Z2 = ProductSet(S.Integers, S.Integers)
assert Z2.contains((1, 2)) is S.true
assert Z2.contains((1,)) is S.false
assert Z2.contains(x) == Contains(x, Z2, evaluate=False)
assert Z2.contains(x).subs(x, 1) is S.false
assert Z2.contains((x, 1)).subs(x, 2) is S.true
assert Z2.contains((x, y)) == Contains((x, y), Z2, evaluate=False)
assert unchanged(Contains, (x, y), Z2)
assert Contains((1, 2), Z2) is S.true
def test_ProductSet_of_single_arg_is_not_arg():
assert unchanged(ProductSet, Interval(0, 1))
assert ProductSet(Interval(0, 1)) != Interval(0, 1)
def test_ProductSet_is_empty():
assert ProductSet(S.Integers, S.Reals).is_empty == False
assert ProductSet(Interval(x, 1), S.Reals).is_empty == None
def test_interval_subs():
a = Symbol('a', real=True)
assert Interval(0, a).subs(a, 2) == Interval(0, 2)
assert Interval(a, 0).subs(a, 2) == S.EmptySet
def test_interval_to_mpi():
assert Interval(0, 1).to_mpi() == mpi(0, 1)
assert Interval(0, 1, True, False).to_mpi() == mpi(0, 1)
assert type(Interval(0, 1).to_mpi()) == type(mpi(0, 1))
def test_measure():
a = Symbol('a', real=True)
assert Interval(1, 3).measure == 2
assert Interval(0, a).measure == a
assert Interval(1, a).measure == a - 1
assert Union(Interval(1, 2), Interval(3, 4)).measure == 2
assert Union(Interval(1, 2), Interval(3, 4), FiniteSet(5, 6, 7)).measure \
== 2
assert FiniteSet(1, 2, oo, a, -oo, -5).measure == 0
assert S.EmptySet.measure == 0
square = Interval(0, 10) * Interval(0, 10)
offsetsquare = Interval(5, 15) * Interval(5, 15)
band = Interval(-oo, oo) * Interval(2, 4)
assert square.measure == offsetsquare.measure == 100
assert (square + offsetsquare).measure == 175 # there is some overlap
assert (square - offsetsquare).measure == 75
assert (square * FiniteSet(1, 2, 3)).measure == 0
assert (square.intersect(band)).measure == 20
assert (square + band).measure == oo
assert (band * FiniteSet(1, 2, 3)).measure == nan
def test_is_subset():
assert Interval(0, 1).is_subset(Interval(0, 2)) is True
assert Interval(0, 3).is_subset(Interval(0, 2)) is False
assert FiniteSet(1, 2).is_subset(FiniteSet(1, 2, 3, 4))
assert FiniteSet(4, 5).is_subset(FiniteSet(1, 2, 3, 4)) is False
assert FiniteSet(1).is_subset(Interval(0, 2))
assert FiniteSet(1, 2).is_subset(Interval(0, 2, True, True)) is False
assert (Interval(1, 2) + FiniteSet(3)).is_subset(
(Interval(0, 2, False, True) + FiniteSet(2, 3)))
assert Interval(3, 4).is_subset(Union(Interval(0, 1), Interval(2, 5))) is True
assert Interval(3, 6).is_subset(Union(Interval(0, 1), Interval(2, 5))) is False
assert FiniteSet(1, 2, 3, 4).is_subset(Interval(0, 5)) is True
assert S.EmptySet.is_subset(FiniteSet(1, 2, 3)) is True
assert Interval(0, 1).is_subset(S.EmptySet) is False
assert S.EmptySet.is_subset(S.EmptySet) is True
raises(ValueError, lambda: S.EmptySet.is_subset(1))
# tests for the issubset alias
assert FiniteSet(1, 2, 3, 4).issubset(Interval(0, 5)) is True
assert S.EmptySet.issubset(FiniteSet(1, 2, 3)) is True
assert S.Naturals.is_subset(S.Integers)
assert S.Naturals0.is_subset(S.Integers)
assert FiniteSet(x).is_subset(FiniteSet(y)) is None
assert FiniteSet(x).is_subset(FiniteSet(y).subs(y, x)) is True
assert FiniteSet(x).is_subset(FiniteSet(y).subs(y, x+1)) is False
def test_is_proper_subset():
assert Interval(0, 1).is_proper_subset(Interval(0, 2)) is True
assert Interval(0, 3).is_proper_subset(Interval(0, 2)) is False
assert S.EmptySet.is_proper_subset(FiniteSet(1, 2, 3)) is True
raises(ValueError, lambda: Interval(0, 1).is_proper_subset(0))
def test_is_superset():
assert Interval(0, 1).is_superset(Interval(0, 2)) == False
assert Interval(0, 3).is_superset(Interval(0, 2))
assert FiniteSet(1, 2).is_superset(FiniteSet(1, 2, 3, 4)) == False
assert FiniteSet(4, 5).is_superset(FiniteSet(1, 2, 3, 4)) == False
assert FiniteSet(1).is_superset(Interval(0, 2)) == False
assert FiniteSet(1, 2).is_superset(Interval(0, 2, True, True)) == False
assert (Interval(1, 2) + FiniteSet(3)).is_superset(
(Interval(0, 2, False, True) + FiniteSet(2, 3))) == False
assert Interval(3, 4).is_superset(Union(Interval(0, 1), Interval(2, 5))) == False
assert FiniteSet(1, 2, 3, 4).is_superset(Interval(0, 5)) == False
assert S.EmptySet.is_superset(FiniteSet(1, 2, 3)) == False
assert Interval(0, 1).is_superset(S.EmptySet) == True
assert S.EmptySet.is_superset(S.EmptySet) == True
raises(ValueError, lambda: S.EmptySet.is_superset(1))
# tests for the issuperset alias
assert Interval(0, 1).issuperset(S.EmptySet) == True
assert S.EmptySet.issuperset(S.EmptySet) == True
def test_is_proper_superset():
assert Interval(0, 1).is_proper_superset(Interval(0, 2)) is False
assert Interval(0, 3).is_proper_superset(Interval(0, 2)) is True
assert FiniteSet(1, 2, 3).is_proper_superset(S.EmptySet) is True
raises(ValueError, lambda: Interval(0, 1).is_proper_superset(0))
def test_contains():
assert Interval(0, 2).contains(1) is S.true
assert Interval(0, 2).contains(3) is S.false
assert Interval(0, 2, True, False).contains(0) is S.false
assert Interval(0, 2, True, False).contains(2) is S.true
assert Interval(0, 2, False, True).contains(0) is S.true
assert Interval(0, 2, False, True).contains(2) is S.false
assert Interval(0, 2, True, True).contains(0) is S.false
assert Interval(0, 2, True, True).contains(2) is S.false
assert (Interval(0, 2) in Interval(0, 2)) is False
assert FiniteSet(1, 2, 3).contains(2) is S.true
assert FiniteSet(1, 2, Symbol('x')).contains(Symbol('x')) is S.true
assert FiniteSet(y)._contains(x) is None
raises(TypeError, lambda: x in FiniteSet(y))
assert FiniteSet({x, y})._contains({x}) is None
assert FiniteSet({x, y}).subs(y, x)._contains({x}) is True
assert FiniteSet({x, y}).subs(y, x+1)._contains({x}) is False
# issue 8197
from sympy.abc import a, b
assert isinstance(FiniteSet(b).contains(-a), Contains)
assert isinstance(FiniteSet(b).contains(a), Contains)
assert isinstance(FiniteSet(a).contains(1), Contains)
raises(TypeError, lambda: 1 in FiniteSet(a))
# issue 8209
rad1 = Pow(Pow(2, S(1)/3) - 1, S(1)/3)
rad2 = Pow(S(1)/9, S(1)/3) - Pow(S(2)/9, S(1)/3) + Pow(S(4)/9, S(1)/3)
s1 = FiniteSet(rad1)
s2 = FiniteSet(rad2)
assert s1 - s2 == S.EmptySet
items = [1, 2, S.Infinity, S('ham'), -1.1]
fset = FiniteSet(*items)
assert all(item in fset for item in items)
assert all(fset.contains(item) is S.true for item in items)
assert Union(Interval(0, 1), Interval(2, 5)).contains(3) is S.true
assert Union(Interval(0, 1), Interval(2, 5)).contains(6) is S.false
assert Union(Interval(0, 1), FiniteSet(2, 5)).contains(3) is S.false
assert S.EmptySet.contains(1) is S.false
assert FiniteSet(rootof(x**3 + x - 1, 0)).contains(S.Infinity) is S.false
assert rootof(x**5 + x**3 + 1, 0) in S.Reals
assert not rootof(x**5 + x**3 + 1, 1) in S.Reals
# non-bool results
assert Union(Interval(1, 2), Interval(3, 4)).contains(x) == \
Or(And(S(1) <= x, x <= 2), And(S(3) <= x, x <= 4))
assert Intersection(Interval(1, x), Interval(2, 3)).contains(y) == \
And(y <= 3, y <= x, S(1) <= y, S(2) <= y)
assert (S.Complexes).contains(S.ComplexInfinity) == S.false
def test_interval_symbolic():
x = Symbol('x')
e = Interval(0, 1)
assert e.contains(x) == And(S(0) <= x, x <= 1)
raises(TypeError, lambda: x in e)
e = Interval(0, 1, True, True)
assert e.contains(x) == And(S(0) < x, x < 1)
def test_union_contains():
x = Symbol('x')
i1 = Interval(0, 1)
i2 = Interval(2, 3)
i3 = Union(i1, i2)
assert i3.as_relational(x) == Or(And(S(0) <= x, x <= 1), And(S(2) <= x, x <= 3))
raises(TypeError, lambda: x in i3)
e = i3.contains(x)
assert e == i3.as_relational(x)
assert e.subs(x, -0.5) is false
assert e.subs(x, 0.5) is true
assert e.subs(x, 1.5) is false
assert e.subs(x, 2.5) is true
assert e.subs(x, 3.5) is false
U = Interval(0, 2, True, True) + Interval(10, oo) + FiniteSet(-1, 2, 5, 6)
assert all(el not in U for el in [0, 4, -oo])
assert all(el in U for el in [2, 5, 10])
def test_is_number():
assert Interval(0, 1).is_number is False
assert Set().is_number is False
def test_Interval_is_left_unbounded():
assert Interval(3, 4).is_left_unbounded is False
assert Interval(-oo, 3).is_left_unbounded is True
assert Interval(Float("-inf"), 3).is_left_unbounded is True
def test_Interval_is_right_unbounded():
assert Interval(3, 4).is_right_unbounded is False
assert Interval(3, oo).is_right_unbounded is True
assert Interval(3, Float("+inf")).is_right_unbounded is True
def test_Interval_as_relational():
x = Symbol('x')
assert Interval(-1, 2, False, False).as_relational(x) == \
And(Le(-1, x), Le(x, 2))
assert Interval(-1, 2, True, False).as_relational(x) == \
And(Lt(-1, x), Le(x, 2))
assert Interval(-1, 2, False, True).as_relational(x) == \
And(Le(-1, x), Lt(x, 2))
assert Interval(-1, 2, True, True).as_relational(x) == \
And(Lt(-1, x), Lt(x, 2))
assert Interval(-oo, 2, right_open=False).as_relational(x) == And(Lt(-oo, x), Le(x, 2))
assert Interval(-oo, 2, right_open=True).as_relational(x) == And(Lt(-oo, x), Lt(x, 2))
assert Interval(-2, oo, left_open=False).as_relational(x) == And(Le(-2, x), Lt(x, oo))
assert Interval(-2, oo, left_open=True).as_relational(x) == And(Lt(-2, x), Lt(x, oo))
assert Interval(-oo, oo).as_relational(x) == And(Lt(-oo, x), Lt(x, oo))
x = Symbol('x', real=True)
y = Symbol('y', real=True)
assert Interval(x, y).as_relational(x) == (x <= y)
assert Interval(y, x).as_relational(x) == (y <= x)
def test_Finite_as_relational():
x = Symbol('x')
y = Symbol('y')
assert FiniteSet(1, 2).as_relational(x) == Or(Eq(x, 1), Eq(x, 2))
assert FiniteSet(y, -5).as_relational(x) == Or(Eq(x, y), Eq(x, -5))
def test_Union_as_relational():
x = Symbol('x')
assert (Interval(0, 1) + FiniteSet(2)).as_relational(x) == \
Or(And(Le(0, x), Le(x, 1)), Eq(x, 2))
assert (Interval(0, 1, True, True) + FiniteSet(1)).as_relational(x) == \
And(Lt(0, x), Le(x, 1))
def test_Intersection_as_relational():
x = Symbol('x')
assert (Intersection(Interval(0, 1), FiniteSet(2),
evaluate=False).as_relational(x)
== And(And(Le(0, x), Le(x, 1)), Eq(x, 2)))
def test_Complement_as_relational():
x = Symbol('x')
expr = Complement(Interval(0, 1), FiniteSet(2), evaluate=False)
assert expr.as_relational(x) == \
And(Le(0, x), Le(x, 1), Ne(x, 2))
@XFAIL
def test_Complement_as_relational_fail():
x = Symbol('x')
expr = Complement(Interval(0, 1), FiniteSet(2), evaluate=False)
# XXX This example fails because 0 <= x changes to x >= 0
# during the evaluation.
assert expr.as_relational(x) == \
(0 <= x) & (x <= 1) & Ne(x, 2)
def test_SymmetricDifference_as_relational():
x = Symbol('x')
expr = SymmetricDifference(Interval(0, 1), FiniteSet(2), evaluate=False)
assert expr.as_relational(x) == Xor(Eq(x, 2), Le(0, x) & Le(x, 1))
def test_EmptySet():
assert S.EmptySet.as_relational(Symbol('x')) is S.false
assert S.EmptySet.intersect(S.UniversalSet) == S.EmptySet
assert S.EmptySet.boundary == S.EmptySet
def test_finite_basic():
x = Symbol('x')
A = FiniteSet(1, 2, 3)
B = FiniteSet(3, 4, 5)
AorB = Union(A, B)
AandB = A.intersect(B)
assert A.is_subset(AorB) and B.is_subset(AorB)
assert AandB.is_subset(A)
assert AandB == FiniteSet(3)
assert A.inf == 1 and A.sup == 3
assert AorB.inf == 1 and AorB.sup == 5
assert FiniteSet(x, 1, 5).sup == Max(x, 5)
assert FiniteSet(x, 1, 5).inf == Min(x, 1)
# issue 7335
assert FiniteSet(S.EmptySet) != S.EmptySet
assert FiniteSet(FiniteSet(1, 2, 3)) != FiniteSet(1, 2, 3)
assert FiniteSet((1, 2, 3)) != FiniteSet(1, 2, 3)
# Ensure a variety of types can exist in a FiniteSet
s = FiniteSet((1, 2), Float, A, -5, x, 'eggs', x**2, Interval)
assert (A > B) is False
assert (A >= B) is False
assert (A < B) is False
assert (A <= B) is False
assert AorB > A and AorB > B
assert AorB >= A and AorB >= B
assert A >= A and A <= A
assert A >= AandB and B >= AandB
assert A > AandB and B > AandB
assert FiniteSet(1.0) == FiniteSet(1)
def test_powerset():
# EmptySet
A = FiniteSet()
pset = A.powerset()
assert len(pset) == 1
assert pset == FiniteSet(S.EmptySet)
# FiniteSets
A = FiniteSet(1, 2)
pset = A.powerset()
assert len(pset) == 2**len(A)
assert pset == FiniteSet(FiniteSet(), FiniteSet(1),
FiniteSet(2), A)
# Not finite sets
I = Interval(0, 1)
raises(NotImplementedError, I.powerset)
def test_product_basic():
H, T = 'H', 'T'
unit_line = Interval(0, 1)
d6 = FiniteSet(1, 2, 3, 4, 5, 6)
d4 = FiniteSet(1, 2, 3, 4)
coin = FiniteSet(H, T)
square = unit_line * unit_line
assert (0, 0) in square
assert 0 not in square
assert (H, T) in coin ** 2
assert (.5, .5, .5) in (square * unit_line).flatten()
assert ((.5, .5), .5) in square * unit_line
assert (H, 3, 3) in (coin * d6 * d6).flatten()
assert ((H, 3), 3) in coin * d6 * d6
HH, TT = sympify(H), sympify(T)
assert set(coin**2) == set(((HH, HH), (HH, TT), (TT, HH), (TT, TT)))
assert (d4*d4).is_subset(d6*d6)
assert square.complement(Interval(-oo, oo)*Interval(-oo, oo)) == Union(
(Interval(-oo, 0, True, True) +
Interval(1, oo, True, True))*Interval(-oo, oo),
Interval(-oo, oo)*(Interval(-oo, 0, True, True) +
Interval(1, oo, True, True)))
assert (Interval(-5, 5)**3).is_subset(Interval(-10, 10)**3)
assert not (Interval(-10, 10)**3).is_subset(Interval(-5, 5)**3)
assert not (Interval(-5, 5)**2).is_subset(Interval(-10, 10)**3)
assert (Interval(.2, .5)*FiniteSet(.5)).is_subset(square) # segment in square
assert len(coin*coin*coin) == 8
assert len(S.EmptySet*S.EmptySet) == 0
assert len(S.EmptySet*coin) == 0
raises(TypeError, lambda: len(coin*Interval(0, 2)))
def test_real():
x = Symbol('x', real=True, finite=True)
I = Interval(0, 5)
J = Interval(10, 20)
A = FiniteSet(1, 2, 30, x, S.Pi)
B = FiniteSet(-4, 0)
C = FiniteSet(100)
D = FiniteSet('Ham', 'Eggs')
assert all(s.is_subset(S.Reals) for s in [I, J, A, B, C])
assert not D.is_subset(S.Reals)
assert all((a + b).is_subset(S.Reals) for a in [I, J, A, B, C] for b in [I, J, A, B, C])
assert not any((a + D).is_subset(S.Reals) for a in [I, J, A, B, C, D])
assert not (I + A + D).is_subset(S.Reals)
def test_supinf():
x = Symbol('x', real=True)
y = Symbol('y', real=True)
assert (Interval(0, 1) + FiniteSet(2)).sup == 2
assert (Interval(0, 1) + FiniteSet(2)).inf == 0
assert (Interval(0, 1) + FiniteSet(x)).sup == Max(1, x)
assert (Interval(0, 1) + FiniteSet(x)).inf == Min(0, x)
assert FiniteSet(5, 1, x).sup == Max(5, x)
assert FiniteSet(5, 1, x).inf == Min(1, x)
assert FiniteSet(5, 1, x, y).sup == Max(5, x, y)
assert FiniteSet(5, 1, x, y).inf == Min(1, x, y)
assert FiniteSet(5, 1, x, y, S.Infinity, S.NegativeInfinity).sup == \
S.Infinity
assert FiniteSet(5, 1, x, y, S.Infinity, S.NegativeInfinity).inf == \
S.NegativeInfinity
assert FiniteSet('Ham', 'Eggs').sup == Max('Ham', 'Eggs')
def test_universalset():
U = S.UniversalSet
x = Symbol('x')
assert U.as_relational(x) is S.true
assert U.union(Interval(2, 4)) == U
assert U.intersect(Interval(2, 4)) == Interval(2, 4)
assert U.measure == S.Infinity
assert U.boundary == S.EmptySet
assert U.contains(0) is S.true
def test_Union_of_ProductSets_shares():
line = Interval(0, 2)
points = FiniteSet(0, 1, 2)
assert Union(line * line, line * points) == line * line
def test_Interval_free_symbols():
# issue 6211
assert Interval(0, 1).free_symbols == set()
x = Symbol('x', real=True)
assert Interval(0, x).free_symbols == {x}
def test_image_interval():
from sympy.core.numbers import Rational
x = Symbol('x', real=True)
a = Symbol('a', real=True)
assert imageset(x, 2*x, Interval(-2, 1)) == Interval(-4, 2)
assert imageset(x, 2*x, Interval(-2, 1, True, False)) == \
Interval(-4, 2, True, False)
assert imageset(x, x**2, Interval(-2, 1, True, False)) == \
Interval(0, 4, False, True)
assert imageset(x, x**2, Interval(-2, 1)) == Interval(0, 4)
assert imageset(x, x**2, Interval(-2, 1, True, False)) == \
Interval(0, 4, False, True)
assert imageset(x, x**2, Interval(-2, 1, True, True)) == \
Interval(0, 4, False, True)
assert imageset(x, (x - 2)**2, Interval(1, 3)) == Interval(0, 1)
assert imageset(x, 3*x**4 - 26*x**3 + 78*x**2 - 90*x, Interval(0, 4)) == \
Interval(-35, 0) # Multiple Maxima
assert imageset(x, x + 1/x, Interval(-oo, oo)) == Interval(-oo, -2) \
+ Interval(2, oo) # Single Infinite discontinuity
assert imageset(x, 1/x + 1/(x-1)**2, Interval(0, 2, True, False)) == \
Interval(Rational(3, 2), oo, False) # Multiple Infinite discontinuities
# Test for Python lambda
assert imageset(lambda x: 2*x, Interval(-2, 1)) == Interval(-4, 2)
assert imageset(Lambda(x, a*x), Interval(0, 1)) == \
ImageSet(Lambda(x, a*x), Interval(0, 1))
assert imageset(Lambda(x, sin(cos(x))), Interval(0, 1)) == \
ImageSet(Lambda(x, sin(cos(x))), Interval(0, 1))
def test_image_piecewise():
f = Piecewise((x, x <= -1), (1/x**2, x <= 5), (x**3, True))
f1 = Piecewise((0, x <= 1), (1, x <= 2), (2, True))
assert imageset(x, f, Interval(-5, 5)) == Union(Interval(-5, -1), Interval(S(1)/25, oo))
assert imageset(x, f1, Interval(1, 2)) == FiniteSet(0, 1)
@XFAIL # See: https://github.com/sympy/sympy/pull/2723#discussion_r8659826
def test_image_Intersection():
x = Symbol('x', real=True)
y = Symbol('y', real=True)
assert imageset(x, x**2, Interval(-2, 0).intersect(Interval(x, y))) == \
Interval(0, 4).intersect(Interval(Min(x**2, y**2), Max(x**2, y**2)))
def test_image_FiniteSet():
x = Symbol('x', real=True)
assert imageset(x, 2*x, FiniteSet(1, 2, 3)) == FiniteSet(2, 4, 6)
def test_image_Union():
x = Symbol('x', real=True)
assert imageset(x, x**2, Interval(-2, 0) + FiniteSet(1, 2, 3)) == \
(Interval(0, 4) + FiniteSet(9))
def test_image_EmptySet():
x = Symbol('x', real=True)
assert imageset(x, 2*x, S.EmptySet) == S.EmptySet
def test_issue_5724_7680():
assert I not in S.Reals # issue 7680
assert Interval(-oo, oo).contains(I) is S.false
def test_boundary():
assert FiniteSet(1).boundary == FiniteSet(1)
assert all(Interval(0, 1, left_open, right_open).boundary == FiniteSet(0, 1)
for left_open in (true, false) for right_open in (true, false))
def test_boundary_Union():
assert (Interval(0, 1) + Interval(2, 3)).boundary == FiniteSet(0, 1, 2, 3)
assert ((Interval(0, 1, False, True)
+ Interval(1, 2, True, False)).boundary == FiniteSet(0, 1, 2))
assert (Interval(0, 1) + FiniteSet(2)).boundary == FiniteSet(0, 1, 2)
assert Union(Interval(0, 10), Interval(5, 15), evaluate=False).boundary \
== FiniteSet(0, 15)
assert Union(Interval(0, 10), Interval(0, 1), evaluate=False).boundary \
== FiniteSet(0, 10)
assert Union(Interval(0, 10, True, True),
Interval(10, 15, True, True), evaluate=False).boundary \
== FiniteSet(0, 10, 15)
@XFAIL
def test_union_boundary_of_joining_sets():
""" Testing the boundary of unions is a hard problem """
assert Union(Interval(0, 10), Interval(10, 15), evaluate=False).boundary \
== FiniteSet(0, 15)
def test_boundary_ProductSet():
open_square = Interval(0, 1, True, True) ** 2
assert open_square.boundary == (FiniteSet(0, 1) * Interval(0, 1)
+ Interval(0, 1) * FiniteSet(0, 1))
second_square = Interval(1, 2, True, True) * Interval(0, 1, True, True)
assert (open_square + second_square).boundary == (
FiniteSet(0, 1) * Interval(0, 1)
+ FiniteSet(1, 2) * Interval(0, 1)
+ Interval(0, 1) * FiniteSet(0, 1)
+ Interval(1, 2) * FiniteSet(0, 1))
def test_boundary_ProductSet_line():
line_in_r2 = Interval(0, 1) * FiniteSet(0)
assert line_in_r2.boundary == line_in_r2
def test_is_open():
assert not Interval(0, 1, False, False).is_open
assert not Interval(0, 1, True, False).is_open
assert Interval(0, 1, True, True).is_open
assert not FiniteSet(1, 2, 3).is_open
def test_is_closed():
assert Interval(0, 1, False, False).is_closed
assert not Interval(0, 1, True, False).is_closed
assert FiniteSet(1, 2, 3).is_closed
def test_closure():
assert Interval(0, 1, False, True).closure == Interval(0, 1, False, False)
def test_interior():
assert Interval(0, 1, False, True).interior == Interval(0, 1, True, True)
def test_issue_7841():
raises(TypeError, lambda: x in S.Reals)
def test_Eq():
assert Eq(Interval(0, 1), Interval(0, 1))
assert Eq(Interval(0, 1), Interval(0, 2)) == False
s1 = FiniteSet(0, 1)
s2 = FiniteSet(1, 2)
assert Eq(s1, s1)
assert Eq(s1, s2) == False
assert Eq(s1*s2, s1*s2)
assert Eq(s1*s2, s2*s1) == False
assert unchanged(Eq, FiniteSet({x, y}), FiniteSet({x}))
assert Eq(FiniteSet({x, y}).subs(y, x), FiniteSet({x})) is S.true
assert Eq(FiniteSet({x, y}), FiniteSet({x})).subs(y, x) is S.true
assert Eq(FiniteSet({x, y}).subs(y, x+1), FiniteSet({x})) is S.false
assert Eq(FiniteSet({x, y}), FiniteSet({x})).subs(y, x+1) is S.false
assert Eq(ProductSet({1}, {2}), Interval(1, 2)) not in (S.true, S.false)
assert Eq(ProductSet({1}), ProductSet({1}, {2})) is S.false
assert Eq(FiniteSet(()), FiniteSet(1)) is S.false
assert Eq(ProductSet(), FiniteSet(1)) is S.false
i1 = Interval(0, 1)
i2 = Interval(x, y)
assert unchanged(Eq, ProductSet(i1, i1), ProductSet(i2, i2))
def test_SymmetricDifference():
assert SymmetricDifference(FiniteSet(0, 1, 2, 3, 4, 5), \
FiniteSet(2, 4, 6, 8, 10)) == FiniteSet(0, 1, 3, 5, 6, 8, 10)
assert SymmetricDifference(FiniteSet(2, 3, 4), FiniteSet(2, 3 ,4 ,5 )) \
== FiniteSet(5)
assert FiniteSet(1, 2, 3, 4, 5) ^ FiniteSet(1, 2, 5, 6) == \
FiniteSet(3, 4, 6)
assert Set(1, 2 ,3) ^ Set(2, 3, 4) == Union(Set(1, 2, 3) - Set(2, 3, 4), \
Set(2, 3, 4) - Set(1, 2, 3))
assert Interval(0, 4) ^ Interval(2, 5) == Union(Interval(0, 4) - \
Interval(2, 5), Interval(2, 5) - Interval(0, 4))
def test_issue_9536():
from sympy.functions.elementary.exponential import log
a = Symbol('a', real=True)
assert FiniteSet(log(a)).intersect(S.Reals) == Intersection(S.Reals, FiniteSet(log(a)))
def test_issue_9637():
n = Symbol('n')
a = FiniteSet(n)
b = FiniteSet(2, n)
assert Complement(S.Reals, a) == Complement(S.Reals, a, evaluate=False)
assert Complement(Interval(1, 3), a) == Complement(Interval(1, 3), a, evaluate=False)
assert Complement(Interval(1, 3), b) == \
Complement(Union(Interval(1, 2, False, True), Interval(2, 3, True, False)), a)
assert Complement(a, S.Reals) == Complement(a, S.Reals, evaluate=False)
assert Complement(a, Interval(1, 3)) == Complement(a, Interval(1, 3), evaluate=False)
def test_issue_9808():
# See https://github.com/sympy/sympy/issues/16342
assert Complement(FiniteSet(y), FiniteSet(1)) == Complement(FiniteSet(y), FiniteSet(1), evaluate=False)
assert Complement(FiniteSet(1, 2, x), FiniteSet(x, y, 2, 3)) == \
Complement(FiniteSet(1), FiniteSet(y), evaluate=False)
def test_issue_9956():
assert Union(Interval(-oo, oo), FiniteSet(1)) == Interval(-oo, oo)
assert Interval(-oo, oo).contains(1) is S.true
def test_issue_Symbol_inter():
i = Interval(0, oo)
r = S.Reals
mat = Matrix([0, 0, 0])
assert Intersection(r, i, FiniteSet(m), FiniteSet(m, n)) == \
Intersection(i, FiniteSet(m))
assert Intersection(FiniteSet(1, m, n), FiniteSet(m, n, 2), i) == \
Intersection(i, FiniteSet(m, n))
assert Intersection(FiniteSet(m, n, x), FiniteSet(m, z), r) == \
Intersection(Intersection({m, z}, {m, n, x}), r)
assert Intersection(FiniteSet(m, n, 3), FiniteSet(m, n, x), r) == \
Intersection(FiniteSet(3, m, n), FiniteSet(m, n, x), r, evaluate=False)
assert Intersection(FiniteSet(m, n, 3), FiniteSet(m, n, 2, 3), r) == \
Intersection(FiniteSet(3, m, n), r)
assert Intersection(r, FiniteSet(mat, 2, n), FiniteSet(0, mat, n)) == \
Intersection(r, FiniteSet(n))
assert Intersection(FiniteSet(sin(x), cos(x)), FiniteSet(sin(x), cos(x), 1), r) == \
Intersection(r, FiniteSet(sin(x), cos(x)))
assert Intersection(FiniteSet(x**2, 1, sin(x)), FiniteSet(x**2, 2, sin(x)), r) == \
Intersection(r, FiniteSet(x**2, sin(x)))
def test_issue_11827():
assert S.Naturals0**4
def test_issue_10113():
f = x**2/(x**2 - 4)
assert imageset(x, f, S.Reals) == Union(Interval(-oo, 0), Interval(1, oo, True, True))
assert imageset(x, f, Interval(-2, 2)) == Interval(-oo, 0)
assert imageset(x, f, Interval(-2, 3)) == Union(Interval(-oo, 0), Interval(S(9)/5, oo))
def test_issue_10248():
assert list(Intersection(S.Reals, FiniteSet(x))) == [
(-oo < x) & (x < oo)]
def test_issue_9447():
a = Interval(0, 1) + Interval(2, 3)
assert Complement(S.UniversalSet, a) == Complement(
S.UniversalSet, Union(Interval(0, 1), Interval(2, 3)), evaluate=False)
assert Complement(S.Naturals, a) == Complement(
S.Naturals, Union(Interval(0, 1), Interval(2, 3)), evaluate=False)
def test_issue_10337():
assert (FiniteSet(2) == 3) is False
assert (FiniteSet(2) != 3) is True
raises(TypeError, lambda: FiniteSet(2) < 3)
raises(TypeError, lambda: FiniteSet(2) <= 3)
raises(TypeError, lambda: FiniteSet(2) > 3)
raises(TypeError, lambda: FiniteSet(2) >= 3)
def test_issue_10326():
bad = [
EmptySet(),
FiniteSet(1),
Interval(1, 2),
S.ComplexInfinity,
S.ImaginaryUnit,
S.Infinity,
S.NaN,
S.NegativeInfinity,
]
interval = Interval(0, 5)
for i in bad:
assert i not in interval
x = Symbol('x', real=True)
nr = Symbol('nr', extended_real=False)
assert x + 1 in Interval(x, x + 4)
assert nr not in Interval(x, x + 4)
assert Interval(1, 2) in FiniteSet(Interval(0, 5), Interval(1, 2))
assert Interval(-oo, oo).contains(oo) is S.false
assert Interval(-oo, oo).contains(-oo) is S.false
def test_issue_2799():
U = S.UniversalSet
a = Symbol('a', real=True)
inf_interval = Interval(a, oo)
R = S.Reals
assert U + inf_interval == inf_interval + U
assert U + R == R + U
assert R + inf_interval == inf_interval + R
def test_issue_9706():
assert Interval(-oo, 0).closure == Interval(-oo, 0, True, False)
assert Interval(0, oo).closure == Interval(0, oo, False, True)
assert Interval(-oo, oo).closure == Interval(-oo, oo)
def test_issue_8257():
reals_plus_infinity = Union(Interval(-oo, oo), FiniteSet(oo))
reals_plus_negativeinfinity = Union(Interval(-oo, oo), FiniteSet(-oo))
assert Interval(-oo, oo) + FiniteSet(oo) == reals_plus_infinity
assert FiniteSet(oo) + Interval(-oo, oo) == reals_plus_infinity
assert Interval(-oo, oo) + FiniteSet(-oo) == reals_plus_negativeinfinity
assert FiniteSet(-oo) + Interval(-oo, oo) == reals_plus_negativeinfinity
def test_issue_10931():
assert S.Integers - S.Integers == EmptySet()
assert S.Integers - S.Reals == EmptySet()
def test_issue_11174():
soln = Intersection(Interval(-oo, oo), FiniteSet(-x), evaluate=False)
assert Intersection(FiniteSet(-x), S.Reals) == soln
soln = Intersection(S.Reals, FiniteSet(x), evaluate=False)
assert Intersection(FiniteSet(x), S.Reals) == soln
def test_finite_set_intersection():
# The following should not produce recursion errors
# Note: some of these are not completely correct. See
# https://github.com/sympy/sympy/issues/16342.
assert Intersection(FiniteSet(-oo, x), FiniteSet(x)) == FiniteSet(x)
assert Intersection._handle_finite_sets([FiniteSet(-oo, x), FiniteSet(0, x)]) == FiniteSet(x)
assert Intersection._handle_finite_sets([FiniteSet(-oo, x), FiniteSet(x)]) == FiniteSet(x)
assert Intersection._handle_finite_sets([FiniteSet(2, 3, x, y), FiniteSet(1, 2, x)]) == \
Intersection._handle_finite_sets([FiniteSet(1, 2, x), FiniteSet(2, 3, x, y)]) == \
Intersection(FiniteSet(1, 2, x), FiniteSet(2, 3, x, y)) == \
Intersection(FiniteSet(1, 2, x), FiniteSet(2, x, y))
assert FiniteSet(1+x-y) & FiniteSet(1) == \
FiniteSet(1) & FiniteSet(1+x-y) == \
Intersection(FiniteSet(1+x-y), FiniteSet(1), evaluate=False)
assert FiniteSet(1) & FiniteSet(x) == FiniteSet(x) & FiniteSet(1) == \
Intersection(FiniteSet(1), FiniteSet(x), evaluate=False)
assert FiniteSet({x}) & FiniteSet({x, y}) == \
Intersection(FiniteSet({x}), FiniteSet({x, y}), evaluate=False)
def test_union_intersection_constructor():
# The actual exception does not matter here, so long as these fail
sets = [FiniteSet(1), FiniteSet(2)]
raises(Exception, lambda: Union(sets))
raises(Exception, lambda: Intersection(sets))
raises(Exception, lambda: Union(tuple(sets)))
raises(Exception, lambda: Intersection(tuple(sets)))
raises(Exception, lambda: Union(i for i in sets))
raises(Exception, lambda: Intersection(i for i in sets))
# Python sets are treated the same as FiniteSet
# The union of a single set (of sets) is the set (of sets) itself
assert Union(set(sets)) == FiniteSet(*sets)
assert Intersection(set(sets)) == FiniteSet(*sets)
assert Union({1}, {2}) == FiniteSet(1, 2)
assert Intersection({1, 2}, {2, 3}) == FiniteSet(2)
def test_Union_contains():
assert zoo not in Union(
Interval.open(-oo, 0), Interval.open(0, oo))
@XFAIL
def test_issue_16878b():
# in intersection_sets for (ImageSet, Set) there is no code
# that handles the base_set of S.Reals like there is
# for Integers
assert imageset(x, (x, x), S.Reals).is_subset(S.Reals**2) is True
|
99bc89fdec3c1d9becfee7569f4d7328d85afed3b5981eef0584a4b02894000a | from sympy import (pi, sin, cos, Symbol, Integral, Sum, sqrt, log, exp, Ne,
oo, LambertW, I, meijerg, exp_polar, Max, Piecewise, And,
real_root)
from sympy.plotting import (plot, plot_parametric, plot3d_parametric_line,
plot3d, plot3d_parametric_surface)
from sympy.plotting.plot import unset_show, plot_contour, PlotGrid
from sympy.utilities import lambdify as lambdify_
from sympy.utilities.pytest import skip, raises, warns
from sympy.plotting.experimental_lambdify import lambdify
from sympy.external import import_module
from tempfile import NamedTemporaryFile
import os
unset_show()
# XXX: We could implement this as a context manager instead
# That would need rewriting the plot_and_save() function
# entirely
class TmpFileManager:
tmp_files = []
@classmethod
def tmp_file(cls, name=''):
cls.tmp_files.append(NamedTemporaryFile(prefix=name, suffix='.png').name)
return cls.tmp_files[-1]
@classmethod
def cleanup(cls):
for file in cls.tmp_files:
try:
os.remove(file)
except OSError:
# If the file doesn't exist, for instance, if the test failed.
pass
def plot_and_save_1(name):
tmp_file = TmpFileManager.tmp_file
x = Symbol('x')
y = Symbol('y')
###
# Examples from the 'introduction' notebook
###
p = plot(x)
p = plot(x*sin(x), x*cos(x))
p.extend(p)
p[0].line_color = lambda a: a
p[1].line_color = 'b'
p.title = 'Big title'
p.xlabel = 'the x axis'
p[1].label = 'straight line'
p.legend = True
p.aspect_ratio = (1, 1)
p.xlim = (-15, 20)
p.save(tmp_file('%s_basic_options_and_colors' % name))
p._backend.close()
p.extend(plot(x + 1))
p.append(plot(x + 3, x**2)[1])
p.save(tmp_file('%s_plot_extend_append' % name))
p[2] = plot(x**2, (x, -2, 3))
p.save(tmp_file('%s_plot_setitem' % name))
p._backend.close()
p = plot(sin(x), (x, -2*pi, 4*pi))
p.save(tmp_file('%s_line_explicit' % name))
p._backend.close()
p = plot(sin(x))
p.save(tmp_file('%s_line_default_range' % name))
p._backend.close()
p = plot((x**2, (x, -5, 5)), (x**3, (x, -3, 3)))
p.save(tmp_file('%s_line_multiple_range' % name))
p._backend.close()
raises(ValueError, lambda: plot(x, y))
#Piecewise plots
p = plot(Piecewise((1, x > 0), (0, True)), (x, -1, 1))
p.save(tmp_file('%s_plot_piecewise' % name))
p._backend.close()
p = plot(Piecewise((x, x < 1), (x**2, True)), (x, -3, 3))
p.save(tmp_file('%s_plot_piecewise_2' % name))
p._backend.close()
# test issue 7471
p1 = plot(x)
p2 = plot(3)
p1.extend(p2)
p.save(tmp_file('%s_horizontal_line' % name))
p._backend.close()
# test issue 10925
f = Piecewise((-1, x < -1), (x, And(-1 <= x, x < 0)), \
(x**2, And(0 <= x, x < 1)), (x**3, x >= 1))
p = plot(f, (x, -3, 3))
p.save(tmp_file('%s_plot_piecewise_3' % name))
p._backend.close()
def plot_and_save_2(name):
tmp_file = TmpFileManager.tmp_file
x = Symbol('x')
y = Symbol('y')
z = Symbol('z')
#parametric 2d plots.
#Single plot with default range.
plot_parametric(sin(x), cos(x)).save(tmp_file())
#Single plot with range.
p = plot_parametric(sin(x), cos(x), (x, -5, 5))
p.save(tmp_file('%s_parametric_range' % name))
p._backend.close()
#Multiple plots with same range.
p = plot_parametric((sin(x), cos(x)), (x, sin(x)))
p.save(tmp_file('%s_parametric_multiple' % name))
p._backend.close()
#Multiple plots with different ranges.
p = plot_parametric((sin(x), cos(x), (x, -3, 3)), (x, sin(x), (x, -5, 5)))
p.save(tmp_file('%s_parametric_multiple_ranges' % name))
p._backend.close()
#depth of recursion specified.
p = plot_parametric(x, sin(x), depth=13)
p.save(tmp_file('%s_recursion_depth' % name))
p._backend.close()
#No adaptive sampling.
p = plot_parametric(cos(x), sin(x), adaptive=False, nb_of_points=500)
p.save(tmp_file('%s_adaptive' % name))
p._backend.close()
#3d parametric plots
p = plot3d_parametric_line(sin(x), cos(x), x)
p.save(tmp_file('%s_3d_line' % name))
p._backend.close()
p = plot3d_parametric_line(
(sin(x), cos(x), x, (x, -5, 5)), (cos(x), sin(x), x, (x, -3, 3)))
p.save(tmp_file('%s_3d_line_multiple' % name))
p._backend.close()
p = plot3d_parametric_line(sin(x), cos(x), x, nb_of_points=30)
p.save(tmp_file('%s_3d_line_points' % name))
p._backend.close()
# 3d surface single plot.
p = plot3d(x * y)
p.save(tmp_file('%s_surface' % name))
p._backend.close()
# Multiple 3D plots with same range.
p = plot3d(-x * y, x * y, (x, -5, 5))
p.save(tmp_file('%s_surface_multiple' % name))
p._backend.close()
# Multiple 3D plots with different ranges.
p = plot3d(
(x * y, (x, -3, 3), (y, -3, 3)), (-x * y, (x, -3, 3), (y, -3, 3)))
p.save(tmp_file('%s_surface_multiple_ranges' % name))
p._backend.close()
# Single Parametric 3D plot
p = plot3d_parametric_surface(sin(x + y), cos(x - y), x - y)
p.save(tmp_file('%s_parametric_surface' % name))
p._backend.close()
# Multiple Parametric 3D plots.
p = plot3d_parametric_surface(
(x*sin(z), x*cos(z), z, (x, -5, 5), (z, -5, 5)),
(sin(x + y), cos(x - y), x - y, (x, -5, 5), (y, -5, 5)))
p.save(tmp_file('%s_parametric_surface' % name))
p._backend.close()
# Single Contour plot.
p = plot_contour(sin(x)*sin(y), (x, -5, 5), (y, -5, 5))
p.save(tmp_file('%s_contour_plot' % name))
p._backend.close()
# Multiple Contour plots with same range.
p = plot_contour(x**2 + y**2, x**3 + y**3, (x, -5, 5), (y, -5, 5))
p.save(tmp_file('%s_contour_plot' % name))
p._backend.close()
# Multiple Contour plots with different range.
p = plot_contour((x**2 + y**2, (x, -5, 5), (y, -5, 5)), (x**3 + y**3, (x, -3, 3), (y, -3, 3)))
p.save(tmp_file('%s_contour_plot' % name))
p._backend.close()
def plot_and_save_3(name):
tmp_file = TmpFileManager.tmp_file
x = Symbol('x')
y = Symbol('y')
z = Symbol('z')
###
# Examples from the 'colors' notebook
###
p = plot(sin(x))
p[0].line_color = lambda a: a
p.save(tmp_file('%s_colors_line_arity1' % name))
p[0].line_color = lambda a, b: b
p.save(tmp_file('%s_colors_line_arity2' % name))
p._backend.close()
p = plot(x*sin(x), x*cos(x), (x, 0, 10))
p[0].line_color = lambda a: a
p.save(tmp_file('%s_colors_param_line_arity1' % name))
p[0].line_color = lambda a, b: a
p.save(tmp_file('%s_colors_param_line_arity2a' % name))
p[0].line_color = lambda a, b: b
p.save(tmp_file('%s_colors_param_line_arity2b' % name))
p._backend.close()
p = plot3d_parametric_line(sin(x) + 0.1*sin(x)*cos(7*x),
cos(x) + 0.1*cos(x)*cos(7*x),
0.1*sin(7*x),
(x, 0, 2*pi))
p[0].line_color = lambdify_(x, sin(4*x))
p.save(tmp_file('%s_colors_3d_line_arity1' % name))
p[0].line_color = lambda a, b: b
p.save(tmp_file('%s_colors_3d_line_arity2' % name))
p[0].line_color = lambda a, b, c: c
p.save(tmp_file('%s_colors_3d_line_arity3' % name))
p._backend.close()
p = plot3d(sin(x)*y, (x, 0, 6*pi), (y, -5, 5))
p[0].surface_color = lambda a: a
p.save(tmp_file('%s_colors_surface_arity1' % name))
p[0].surface_color = lambda a, b: b
p.save(tmp_file('%s_colors_surface_arity2' % name))
p[0].surface_color = lambda a, b, c: c
p.save(tmp_file('%s_colors_surface_arity3a' % name))
p[0].surface_color = lambdify_((x, y, z), sqrt((x - 3*pi)**2 + y**2))
p.save(tmp_file('%s_colors_surface_arity3b' % name))
p._backend.close()
p = plot3d_parametric_surface(x * cos(4 * y), x * sin(4 * y), y,
(x, -1, 1), (y, -1, 1))
p[0].surface_color = lambda a: a
p.save(tmp_file('%s_colors_param_surf_arity1' % name))
p[0].surface_color = lambda a, b: a*b
p.save(tmp_file('%s_colors_param_surf_arity2' % name))
p[0].surface_color = lambdify_((x, y, z), sqrt(x**2 + y**2 + z**2))
p.save(tmp_file('%s_colors_param_surf_arity3' % name))
p._backend.close()
def plot_and_save_4(name):
tmp_file = TmpFileManager.tmp_file
x = Symbol('x')
y = Symbol('y')
###
# Examples from the 'advanced' notebook
###
# XXX: This raises the warning "The evaluation of the expression is
# problematic. We are trying a failback method that may still work. Please
# report this as a bug." It has to use the fallback because using evalf()
# is the only way to evaluate the integral. We should perhaps just remove
# that warning.
with warns(UserWarning, match="The evaluation of the expression is problematic"):
i = Integral(log((sin(x)**2 + 1)*sqrt(x**2 + 1)), (x, 0, y))
p = plot(i, (y, 1, 5))
p.save(tmp_file('%s_advanced_integral' % name))
p._backend.close()
def plot_and_save_5(name):
tmp_file = TmpFileManager.tmp_file
x = Symbol('x')
y = Symbol('y')
s = Sum(1/x**y, (x, 1, oo))
p = plot(s, (y, 2, 10))
p.save(tmp_file('%s_advanced_inf_sum' % name))
p._backend.close()
p = plot(Sum(1/x, (x, 1, y)), (y, 2, 10), show=False)
p[0].only_integers = True
p[0].steps = True
p.save(tmp_file('%s_advanced_fin_sum' % name))
p._backend.close()
def plot_and_save_6(name):
tmp_file = TmpFileManager.tmp_file
x = Symbol('x')
###
# Test expressions that can not be translated to np and generate complex
# results.
###
plot(sin(x) + I*cos(x)).save(tmp_file())
plot(sqrt(sqrt(-x))).save(tmp_file())
plot(LambertW(x)).save(tmp_file())
plot(sqrt(LambertW(x))).save(tmp_file())
#Characteristic function of a StudentT distribution with nu=10
plot((meijerg(((1 / 2,), ()), ((5, 0, 1 / 2), ()), 5 * x**2 * exp_polar(-I*pi)/2)
+ meijerg(((1/2,), ()), ((5, 0, 1/2), ()),
5*x**2 * exp_polar(I*pi)/2)) / (48 * pi), (x, 1e-6, 1e-2)).save(tmp_file())
def plotgrid_and_save(name):
tmp_file = TmpFileManager.tmp_file
x = Symbol('x')
y = Symbol('y')
p1 = plot(x)
p2 = plot_parametric((sin(x), cos(x)), (x, sin(x)), show=False)
p3 = plot_parametric(cos(x), sin(x), adaptive=False, nb_of_points=500, show=False)
p4 = plot3d_parametric_line(sin(x), cos(x), x, show=False)
# symmetric grid
p = PlotGrid(2, 2, p1, p2, p3, p4)
p.save(tmp_file('%s_grid1' % name))
p._backend.close()
# grid size greater than the number of subplots
p = PlotGrid(3, 4, p1, p2, p3, p4)
p.save(tmp_file('%s_grid2' % name))
p._backend.close()
p5 = plot(cos(x),(x, -pi, pi), show=False)
p5[0].line_color = lambda a: a
p6 = plot(Piecewise((1, x > 0), (0, True)), (x, -1, 1), show=False)
p7 = plot_contour((x**2 + y**2, (x, -5, 5), (y, -5, 5)), (x**3 + y**3, (x, -3, 3), (y, -3, 3)), show=False)
# unsymmetric grid (subplots in one line)
p = PlotGrid(1, 3, p5, p6, p7)
p.save(tmp_file('%s_grid3' % name))
p._backend.close()
def test_matplotlib_1():
matplotlib = import_module('matplotlib', min_module_version='1.1.0', catch=(RuntimeError,))
if matplotlib:
try:
plot_and_save_1('test')
finally:
# clean up
TmpFileManager.cleanup()
else:
skip("Matplotlib not the default backend")
def test_matplotlib_2():
matplotlib = import_module('matplotlib', min_module_version='1.1.0', catch=(RuntimeError,))
if matplotlib:
try:
plot_and_save_2('test')
finally:
# clean up
TmpFileManager.cleanup()
else:
skip("Matplotlib not the default backend")
def test_matplotlib_3():
matplotlib = import_module('matplotlib', min_module_version='1.1.0', catch=(RuntimeError,))
if matplotlib:
try:
plot_and_save_3('test')
finally:
# clean up
TmpFileManager.cleanup()
else:
skip("Matplotlib not the default backend")
def test_matplotlib_4():
matplotlib = import_module('matplotlib', min_module_version='1.1.0', catch=(RuntimeError,))
if matplotlib:
try:
plot_and_save_4('test')
finally:
# clean up
TmpFileManager.cleanup()
else:
skip("Matplotlib not the default backend")
def test_matplotlib_5():
matplotlib = import_module('matplotlib', min_module_version='1.1.0', catch=(RuntimeError,))
if matplotlib:
try:
plot_and_save_5('test')
finally:
# clean up
TmpFileManager.cleanup()
else:
skip("Matplotlib not the default backend")
def test_matplotlib_6():
matplotlib = import_module('matplotlib', min_module_version='1.1.0', catch=(RuntimeError,))
if matplotlib:
try:
plot_and_save_6('test')
finally:
# clean up
TmpFileManager.cleanup()
else:
skip("Matplotlib not the default backend")
def test_matplotlib_7():
matplotlib = import_module('matplotlib', min_module_version='1.1.0', catch=(RuntimeError,))
if matplotlib:
try:
plotgrid_and_save('test')
finally:
# clean up
TmpFileManager.cleanup()
else:
skip("Matplotlib not the default backend")
# Tests for exception handling in experimental_lambdify
def test_experimental_lambify():
x = Symbol('x')
f = lambdify([x], Max(x, 5))
# XXX should f be tested? If f(2) is attempted, an
# error is raised because a complex produced during wrapping of the arg
# is being compared with an int.
assert Max(2, 5) == 5
assert Max(5, 7) == 7
x = Symbol('x-3')
f = lambdify([x], x + 1)
assert f(1) == 2
def test_append_issue_7140():
matplotlib = import_module('matplotlib', min_module_version='1.1.0', catch=(RuntimeError,))
if not matplotlib:
skip("Matplotlib not the default backend")
x = Symbol('x')
p1 = plot(x)
p2 = plot(x**2)
p3 = plot(x + 2)
# append a series
p2.append(p1[0])
assert len(p2._series) == 2
with raises(TypeError):
p1.append(p2)
with raises(TypeError):
p1.append(p2._series)
def test_issue_15265():
from sympy.core.sympify import sympify
from sympy.core.singleton import S
matplotlib = import_module('matplotlib', min_module_version='1.1.0', catch=(RuntimeError,))
if not matplotlib:
skip("Matplotlib not the default backend")
x = Symbol('x')
eqn = sin(x)
p = plot(eqn, xlim=(-S.Pi, S.Pi), ylim=(-1, 1))
p._backend.close()
p = plot(eqn, xlim=(-1, 1), ylim=(-S.Pi, S.Pi))
p._backend.close()
p = plot(eqn, xlim=(-1, 1), ylim=(sympify('-3.14'), sympify('3.14')))
p._backend.close()
p = plot(eqn, xlim=(sympify('-3.14'), sympify('3.14')), ylim=(-1, 1))
p._backend.close()
raises(ValueError,
lambda: plot(eqn, xlim=(-S.ImaginaryUnit, 1), ylim=(-1, 1)))
raises(ValueError,
lambda: plot(eqn, xlim=(-1, 1), ylim=(-1, S.ImaginaryUnit)))
raises(ValueError,
lambda: plot(eqn, xlim=(-S.Infinity, 1), ylim=(-1, 1)))
raises(ValueError,
lambda: plot(eqn, xlim=(-1, 1), ylim=(-1, S.Infinity)))
def test_empty_Plot():
matplotlib = import_module('matplotlib', min_module_version='1.1.0', catch=(RuntimeError,))
if not matplotlib:
skip("Matplotlib not the default backend")
from sympy.plotting.plot import Plot
p = Plot()
# No exception showing an empty plot
p.show()
def test_empty_plot():
matplotlib = import_module('matplotlib', min_module_version='1.1.0', catch=(RuntimeError,))
if not matplotlib:
skip("Matplotlib not the default backend")
# No exception showing an empty plot
plot()
def test_issue_17405():
matplotlib = import_module('matplotlib', min_module_version='1.1.0', catch=(RuntimeError,))
if not matplotlib:
skip("Matplotlib not the default backend")
x = Symbol('x')
f = x**0.3 - 10*x**3 + x**2
p = plot(f, (x, -10, 10), show=False)
# Random number of segments, probably more than 100, but we want to see
# that there are segments generated, as opposed to when the bug was present
assert len(p[0].get_segments()) >= 30
def test_logplot_PR_16796():
matplotlib = import_module('matplotlib', min_module_version='1.1.0', catch=(RuntimeError,))
if not matplotlib:
skip("Matplotlib not the default backend")
x = Symbol('x')
p = plot(x, (x, .001, 100), xscale='log', show=False)
# Random number of segments, probably more than 100, but we want to see
# that there are segments generated, as opposed to when the bug was present
assert len(p[0].get_segments()) >= 30
assert p[0].end == 100.0
assert p[0].start == .001
def test_issue_16572():
matplotlib = import_module('matplotlib', min_module_version='1.1.0', catch=(RuntimeError,))
if not matplotlib:
skip("Matplotlib not the default backend")
x = Symbol('x')
p = plot(LambertW(x), show=False)
# Random number of segments, probably more than 50, but we want to see
# that there are segments generated, as opposed to when the bug was present
assert len(p[0].get_segments()) >= 30
def test_issue_11865():
matplotlib = import_module('matplotlib', min_module_version='1.1.0', catch=(RuntimeError,))
if not matplotlib:
skip("Matplotlib not the default backend")
k = Symbol('k', integer=True)
f = Piecewise((-I*exp(I*pi*k)/k + I*exp(-I*pi*k)/k, Ne(k, 0)), (2*pi, True))
p = plot(f, show=False)
# Random number of segments, probably more than 100, but we want to see
# that there are segments generated, as opposed to when the bug was present
# and that there are no exceptions.
assert len(p[0].get_segments()) >= 30
def test_issue_11461():
matplotlib = import_module('matplotlib', min_module_version='1.1.0', catch=(RuntimeError,))
if not matplotlib:
skip("Matplotlib not the default backend")
x = Symbol('x')
p = plot(real_root((log(x/(x-2))), 3), show=False)
# Random number of segments, probably more than 100, but we want to see
# that there are segments generated, as opposed to when the bug was present
# and that there are no exceptions.
assert len(p[0].get_segments()) >= 30
|
de34ce7bb5d1a548ef762d116c0a340e640219cac55621aa221636a1ffe62054 | """
Continuous Random Variables - Prebuilt variables
Contains
========
Arcsin
Benini
Beta
BetaNoncentral
BetaPrime
Cauchy
Chi
ChiNoncentral
ChiSquared
Dagum
Erlang
ExGaussian
Exponential
ExponentialPower
FDistribution
FisherZ
Frechet
Gamma
GammaInverse
Gumbel
Gompertz
Kumaraswamy
Laplace
Logistic
LogLogistic
LogNormal
Maxwell
Nakagami
Normal
Pareto
QuadraticU
RaisedCosine
Rayleigh
ShiftedGompertz
StudentT
Trapezoidal
Triangular
Uniform
UniformSum
VonMises
Weibull
WignerSemicircle
"""
from __future__ import print_function, division
import random
from sympy import beta as beta_fn
from sympy import cos, sin, tan, atan, exp, besseli, besselj, besselk
from sympy import (log, sqrt, pi, S, Dummy, Interval, sympify, gamma, sign,
Piecewise, And, Eq, binomial, factorial, Sum, floor, Abs,
Lambda, Basic, lowergamma, erf, erfc, erfi, erfinv, I,
hyper, uppergamma, sinh, Ne, expint, Rational)
from sympy.external import import_module
from sympy.matrices import MatrixBase, MatrixExpr
from sympy.stats.crv import (SingleContinuousPSpace, SingleContinuousDistribution,
ContinuousDistributionHandmade)
from sympy.stats.joint_rv import JointPSpace, CompoundDistribution
from sympy.stats.joint_rv_types import multivariate_rv
from sympy.stats.rv import _value_check, RandomSymbol
oo = S.Infinity
__all__ = ['ContinuousRV',
'Arcsin',
'Benini',
'Beta',
'BetaNoncentral',
'BetaPrime',
'Cauchy',
'Chi',
'ChiNoncentral',
'ChiSquared',
'Dagum',
'Erlang',
'ExGaussian',
'Exponential',
'ExponentialPower',
'FDistribution',
'FisherZ',
'Frechet',
'Gamma',
'GammaInverse',
'Gompertz',
'Gumbel',
'Kumaraswamy',
'Laplace',
'Logistic',
'LogLogistic',
'LogNormal',
'Maxwell',
'Nakagami',
'Normal',
'GaussianInverse',
'Pareto',
'QuadraticU',
'RaisedCosine',
'Rayleigh',
'StudentT',
'ShiftedGompertz',
'Trapezoidal',
'Triangular',
'Uniform',
'UniformSum',
'VonMises',
'Weibull',
'WignerSemicircle'
]
def ContinuousRV(symbol, density, set=Interval(-oo, oo)):
"""
Create a Continuous Random Variable given the following:
-- a symbol
-- a probability density function
-- set on which the pdf is valid (defaults to entire real line)
Returns a RandomSymbol.
Many common continuous random variable types are already implemented.
This function should be necessary only very rarely.
Examples
========
>>> from sympy import Symbol, sqrt, exp, pi
>>> from sympy.stats import ContinuousRV, P, E
>>> x = Symbol("x")
>>> pdf = sqrt(2)*exp(-x**2/2)/(2*sqrt(pi)) # Normal distribution
>>> X = ContinuousRV(x, pdf)
>>> E(X)
0
>>> P(X>0)
1/2
"""
pdf = Piecewise((density, set.as_relational(symbol)), (0, True))
pdf = Lambda(symbol, pdf)
dist = ContinuousDistributionHandmade(pdf, set)
return SingleContinuousPSpace(symbol, dist).value
def rv(symbol, cls, args):
args = list(map(sympify, args))
dist = cls(*args)
dist.check(*args)
pspace = SingleContinuousPSpace(symbol, dist)
if any(isinstance(arg, RandomSymbol) for arg in args):
pspace = JointPSpace(symbol, CompoundDistribution(dist))
return pspace.value
########################################
# Continuous Probability Distributions #
########################################
#-------------------------------------------------------------------------------
# Arcsin distribution ----------------------------------------------------------
class ArcsinDistribution(SingleContinuousDistribution):
_argnames = ('a', 'b')
def set(self):
return Interval(self.a, self.b)
def pdf(self, x):
return 1/(pi*sqrt((x - self.a)*(self.b - x)))
def _cdf(self, x):
from sympy import asin
a, b = self.a, self.b
return Piecewise(
(S.Zero, x < a),
(2*asin(sqrt((x - a)/(b - a)))/pi, x <= b),
(S.One, True))
def Arcsin(name, a=0, b=1):
r"""
Create a Continuous Random Variable with an arcsin distribution.
The density of the arcsin distribution is given by
.. math::
f(x) := \frac{1}{\pi\sqrt{(x-a)(b-x)}}
with :math:`x \in (a,b)`. It must hold that :math:`-\infty < a < b < \infty`.
Parameters
==========
a : Real number, the left interval boundary
b : Real number, the right interval boundary
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Arcsin, density, cdf
>>> from sympy import Symbol, simplify
>>> a = Symbol("a", real=True)
>>> b = Symbol("b", real=True)
>>> z = Symbol("z")
>>> X = Arcsin("x", a, b)
>>> density(X)(z)
1/(pi*sqrt((-a + z)*(b - z)))
>>> cdf(X)(z)
Piecewise((0, a > z),
(2*asin(sqrt((-a + z)/(-a + b)))/pi, b >= z),
(1, True))
References
==========
.. [1] https://en.wikipedia.org/wiki/Arcsine_distribution
"""
return rv(name, ArcsinDistribution, (a, b))
#-------------------------------------------------------------------------------
# Benini distribution ----------------------------------------------------------
class BeniniDistribution(SingleContinuousDistribution):
_argnames = ('alpha', 'beta', 'sigma')
@staticmethod
def check(alpha, beta, sigma):
_value_check(alpha > 0, "Shape parameter Alpha must be positive.")
_value_check(beta > 0, "Shape parameter Beta must be positive.")
_value_check(sigma > 0, "Scale parameter Sigma must be positive.")
@property
def set(self):
return Interval(self.sigma, oo)
def pdf(self, x):
alpha, beta, sigma = self.alpha, self.beta, self.sigma
return (exp(-alpha*log(x/sigma) - beta*log(x/sigma)**2)
*(alpha/x + 2*beta*log(x/sigma)/x))
def _moment_generating_function(self, t):
raise NotImplementedError('The moment generating function of the '
'Benini distribution does not exist.')
def Benini(name, alpha, beta, sigma):
r"""
Create a Continuous Random Variable with a Benini distribution.
The density of the Benini distribution is given by
.. math::
f(x) := e^{-\alpha\log{\frac{x}{\sigma}}
-\beta\log^2\left[{\frac{x}{\sigma}}\right]}
\left(\frac{\alpha}{x}+\frac{2\beta\log{\frac{x}{\sigma}}}{x}\right)
This is a heavy-tailed distribution and is also known as the log-Rayleigh
distribution.
Parameters
==========
alpha : Real number, `\alpha > 0`, a shape
beta : Real number, `\beta > 0`, a shape
sigma : Real number, `\sigma > 0`, a scale
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Benini, density, cdf
>>> from sympy import Symbol, simplify, pprint
>>> alpha = Symbol("alpha", positive=True)
>>> beta = Symbol("beta", positive=True)
>>> sigma = Symbol("sigma", positive=True)
>>> z = Symbol("z")
>>> X = Benini("x", alpha, beta, sigma)
>>> D = density(X)(z)
>>> pprint(D, use_unicode=False)
/ / z \\ / z \ 2/ z \
| 2*beta*log|-----|| - alpha*log|-----| - beta*log |-----|
|alpha \sigma/| \sigma/ \sigma/
|----- + -----------------|*e
\ z z /
>>> cdf(X)(z)
Piecewise((1 - exp(-alpha*log(z/sigma) - beta*log(z/sigma)**2), sigma <= z),
(0, True))
References
==========
.. [1] https://en.wikipedia.org/wiki/Benini_distribution
.. [2] http://reference.wolfram.com/legacy/v8/ref/BeniniDistribution.html
"""
return rv(name, BeniniDistribution, (alpha, beta, sigma))
#-------------------------------------------------------------------------------
# Beta distribution ------------------------------------------------------------
class BetaDistribution(SingleContinuousDistribution):
_argnames = ('alpha', 'beta')
set = Interval(0, 1)
@staticmethod
def check(alpha, beta):
_value_check(alpha > 0, "Shape parameter Alpha must be positive.")
_value_check(beta > 0, "Shape parameter Beta must be positive.")
def pdf(self, x):
alpha, beta = self.alpha, self.beta
return x**(alpha - 1) * (1 - x)**(beta - 1) / beta_fn(alpha, beta)
def sample(self):
return random.betavariate(self.alpha, self.beta)
def _characteristic_function(self, t):
return hyper((self.alpha,), (self.alpha + self.beta,), I*t)
def _moment_generating_function(self, t):
return hyper((self.alpha,), (self.alpha + self.beta,), t)
def Beta(name, alpha, beta):
r"""
Create a Continuous Random Variable with a Beta distribution.
The density of the Beta distribution is given by
.. math::
f(x) := \frac{x^{\alpha-1}(1-x)^{\beta-1}} {\mathrm{B}(\alpha,\beta)}
with :math:`x \in [0,1]`.
Parameters
==========
alpha : Real number, `\alpha > 0`, a shape
beta : Real number, `\beta > 0`, a shape
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Beta, density, E, variance
>>> from sympy import Symbol, simplify, pprint, factor
>>> alpha = Symbol("alpha", positive=True)
>>> beta = Symbol("beta", positive=True)
>>> z = Symbol("z")
>>> X = Beta("x", alpha, beta)
>>> D = density(X)(z)
>>> pprint(D, use_unicode=False)
alpha - 1 beta - 1
z *(1 - z)
--------------------------
B(alpha, beta)
>>> simplify(E(X))
alpha/(alpha + beta)
>>> factor(simplify(variance(X)))
alpha*beta/((alpha + beta)**2*(alpha + beta + 1))
References
==========
.. [1] https://en.wikipedia.org/wiki/Beta_distribution
.. [2] http://mathworld.wolfram.com/BetaDistribution.html
"""
return rv(name, BetaDistribution, (alpha, beta))
#-------------------------------------------------------------------------------
# Noncentral Beta distribution ------------------------------------------------------------
class BetaNoncentralDistribution(SingleContinuousDistribution):
_argnames = ('alpha', 'beta', 'lamda')
set = Interval(0, 1)
@staticmethod
def check(alpha, beta, lamda):
_value_check(alpha > 0, "Shape parameter Alpha must be positive.")
_value_check(beta > 0, "Shape parameter Beta must be positive.")
_value_check(lamda >= 0, "Noncentrality parameter Lambda must be positive")
def pdf(self, x):
alpha, beta, lamda = self.alpha, self.beta, self.lamda
k = Dummy("k")
return Sum(exp(-lamda / 2) * (lamda / 2)**k * x**(alpha + k - 1) *(
1 - x)**(beta - 1) / (factorial(k) * beta_fn(alpha + k, beta)), (k, 0, oo))
def BetaNoncentral(name, alpha, beta, lamda):
r"""
Create a Continuous Random Variable with a Type I Noncentral Beta distribution.
The density of the Noncentral Beta distribution is given by
.. math::
f(x) := \sum_{k=0}^\infty e^{-\lambda/2}\frac{(\lambda/2)^k}{k!}
\frac{x^{\alpha+k-1}(1-x)^{\beta-1}}{\mathrm{B}(\alpha+k,\beta)}
with :math:`x \in [0,1]`.
Parameters
==========
alpha : Real number, `\alpha > 0`, a shape
beta : Real number, `\beta > 0`, a shape
lamda: Real number, `\lambda >= 0`, noncentrality parameter
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import BetaNoncentral, density, cdf
>>> from sympy import Symbol, pprint
>>> alpha = Symbol("alpha", positive=True)
>>> beta = Symbol("beta", positive=True)
>>> lamda = Symbol("lamda", nonnegative=True)
>>> z = Symbol("z")
>>> X = BetaNoncentral("x", alpha, beta, lamda)
>>> D = density(X)(z)
>>> pprint(D, use_unicode=False)
oo
_____
\ `
\ -lamda
\ k -------
\ k + alpha - 1 /lamda\ beta - 1 2
) z *|-----| *(1 - z) *e
/ \ 2 /
/ ------------------------------------------------
/ B(k + alpha, beta)*k!
/____,
k = 0
Compute cdf with specific 'x', 'alpha', 'beta' and 'lamda' values as follows :
>>> cdf(BetaNoncentral("x", 1, 1, 1), evaluate=False)(2).doit()
2*exp(1/2)
The argument evaluate=False prevents an attempt at evaluation
of the sum for general x, before the argument 2 is passed.
References
==========
.. [1] https://en.wikipedia.org/wiki/Noncentral_beta_distribution
.. [2] https://reference.wolfram.com/language/ref/NoncentralBetaDistribution.html
"""
return rv(name, BetaNoncentralDistribution, (alpha, beta, lamda))
#-------------------------------------------------------------------------------
# Beta prime distribution ------------------------------------------------------
class BetaPrimeDistribution(SingleContinuousDistribution):
_argnames = ('alpha', 'beta')
@staticmethod
def check(alpha, beta):
_value_check(alpha > 0, "Shape parameter Alpha must be positive.")
_value_check(beta > 0, "Shape parameter Beta must be positive.")
set = Interval(0, oo)
def pdf(self, x):
alpha, beta = self.alpha, self.beta
return x**(alpha - 1)*(1 + x)**(-alpha - beta)/beta_fn(alpha, beta)
def BetaPrime(name, alpha, beta):
r"""
Create a continuous random variable with a Beta prime distribution.
The density of the Beta prime distribution is given by
.. math::
f(x) := \frac{x^{\alpha-1} (1+x)^{-\alpha -\beta}}{B(\alpha,\beta)}
with :math:`x > 0`.
Parameters
==========
alpha : Real number, `\alpha > 0`, a shape
beta : Real number, `\beta > 0`, a shape
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import BetaPrime, density
>>> from sympy import Symbol, pprint
>>> alpha = Symbol("alpha", positive=True)
>>> beta = Symbol("beta", positive=True)
>>> z = Symbol("z")
>>> X = BetaPrime("x", alpha, beta)
>>> D = density(X)(z)
>>> pprint(D, use_unicode=False)
alpha - 1 -alpha - beta
z *(z + 1)
-------------------------------
B(alpha, beta)
References
==========
.. [1] https://en.wikipedia.org/wiki/Beta_prime_distribution
.. [2] http://mathworld.wolfram.com/BetaPrimeDistribution.html
"""
return rv(name, BetaPrimeDistribution, (alpha, beta))
#-------------------------------------------------------------------------------
# Cauchy distribution ----------------------------------------------------------
class CauchyDistribution(SingleContinuousDistribution):
_argnames = ('x0', 'gamma')
@staticmethod
def check(x0, gamma):
_value_check(gamma > 0, "Scale parameter Gamma must be positive.")
def pdf(self, x):
return 1/(pi*self.gamma*(1 + ((x - self.x0)/self.gamma)**2))
def _cdf(self, x):
x0, gamma = self.x0, self.gamma
return (1/pi)*atan((x - x0)/gamma) + S.Half
def _characteristic_function(self, t):
return exp(self.x0 * I * t - self.gamma * Abs(t))
def _moment_generating_function(self, t):
raise NotImplementedError("The moment generating function for the "
"Cauchy distribution does not exist.")
def _quantile(self, p):
return self.x0 + self.gamma*tan(pi*(p - S.Half))
def Cauchy(name, x0, gamma):
r"""
Create a continuous random variable with a Cauchy distribution.
The density of the Cauchy distribution is given by
.. math::
f(x) := \frac{1}{\pi \gamma [1 + {(\frac{x-x_0}{\gamma})}^2]}
Parameters
==========
x0 : Real number, the location
gamma : Real number, `\gamma > 0`, a scale
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Cauchy, density
>>> from sympy import Symbol
>>> x0 = Symbol("x0")
>>> gamma = Symbol("gamma", positive=True)
>>> z = Symbol("z")
>>> X = Cauchy("x", x0, gamma)
>>> density(X)(z)
1/(pi*gamma*(1 + (-x0 + z)**2/gamma**2))
References
==========
.. [1] https://en.wikipedia.org/wiki/Cauchy_distribution
.. [2] http://mathworld.wolfram.com/CauchyDistribution.html
"""
return rv(name, CauchyDistribution, (x0, gamma))
#-------------------------------------------------------------------------------
# Chi distribution -------------------------------------------------------------
class ChiDistribution(SingleContinuousDistribution):
_argnames = ('k',)
@staticmethod
def check(k):
_value_check(k > 0, "Number of degrees of freedom (k) must be positive.")
_value_check(k.is_integer, "Number of degrees of freedom (k) must be an integer.")
set = Interval(0, oo)
def pdf(self, x):
return 2**(1 - self.k/2)*x**(self.k - 1)*exp(-x**2/2)/gamma(self.k/2)
def _characteristic_function(self, t):
k = self.k
part_1 = hyper((k/2,), (S.Half,), -t**2/2)
part_2 = I*t*sqrt(2)*gamma((k+1)/2)/gamma(k/2)
part_3 = hyper(((k+1)/2,), (Rational(3, 2),), -t**2/2)
return part_1 + part_2*part_3
def _moment_generating_function(self, t):
k = self.k
part_1 = hyper((k / 2,), (S.Half,), t ** 2 / 2)
part_2 = t * sqrt(2) * gamma((k + 1) / 2) / gamma(k / 2)
part_3 = hyper(((k + 1) / 2,), (S(3) / 2,), t ** 2 / 2)
return part_1 + part_2 * part_3
def Chi(name, k):
r"""
Create a continuous random variable with a Chi distribution.
The density of the Chi distribution is given by
.. math::
f(x) := \frac{2^{1-k/2}x^{k-1}e^{-x^2/2}}{\Gamma(k/2)}
with :math:`x \geq 0`.
Parameters
==========
k : Positive integer, The number of degrees of freedom
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Chi, density, E
>>> from sympy import Symbol, simplify
>>> k = Symbol("k", integer=True)
>>> z = Symbol("z")
>>> X = Chi("x", k)
>>> density(X)(z)
2**(1 - k/2)*z**(k - 1)*exp(-z**2/2)/gamma(k/2)
>>> simplify(E(X))
sqrt(2)*gamma(k/2 + 1/2)/gamma(k/2)
References
==========
.. [1] https://en.wikipedia.org/wiki/Chi_distribution
.. [2] http://mathworld.wolfram.com/ChiDistribution.html
"""
return rv(name, ChiDistribution, (k,))
#-------------------------------------------------------------------------------
# Non-central Chi distribution -------------------------------------------------
class ChiNoncentralDistribution(SingleContinuousDistribution):
_argnames = ('k', 'l')
@staticmethod
def check(k, l):
_value_check(k > 0, "Number of degrees of freedom (k) must be positive.")
_value_check(k.is_integer, "Number of degrees of freedom (k) must be an integer.")
_value_check(l > 0, "Shift parameter Lambda must be positive.")
set = Interval(0, oo)
def pdf(self, x):
k, l = self.k, self.l
return exp(-(x**2+l**2)/2)*x**k*l / (l*x)**(k/2) * besseli(k/2-1, l*x)
def ChiNoncentral(name, k, l):
r"""
Create a continuous random variable with a non-central Chi distribution.
The density of the non-central Chi distribution is given by
.. math::
f(x) := \frac{e^{-(x^2+\lambda^2)/2} x^k\lambda}
{(\lambda x)^{k/2}} I_{k/2-1}(\lambda x)
with `x \geq 0`. Here, `I_\nu (x)` is the
:ref:`modified Bessel function of the first kind <besseli>`.
Parameters
==========
k : A positive Integer, `k > 0`, the number of degrees of freedom
lambda : Real number, `\lambda > 0`, Shift parameter
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import ChiNoncentral, density
>>> from sympy import Symbol
>>> k = Symbol("k", integer=True)
>>> l = Symbol("l")
>>> z = Symbol("z")
>>> X = ChiNoncentral("x", k, l)
>>> density(X)(z)
l*z**k*(l*z)**(-k/2)*exp(-l**2/2 - z**2/2)*besseli(k/2 - 1, l*z)
References
==========
.. [1] https://en.wikipedia.org/wiki/Noncentral_chi_distribution
"""
return rv(name, ChiNoncentralDistribution, (k, l))
#-------------------------------------------------------------------------------
# Chi squared distribution -----------------------------------------------------
class ChiSquaredDistribution(SingleContinuousDistribution):
_argnames = ('k',)
@staticmethod
def check(k):
_value_check(k > 0, "Number of degrees of freedom (k) must be positive.")
_value_check(k.is_integer, "Number of degrees of freedom (k) must be an integer.")
set = Interval(0, oo)
def pdf(self, x):
k = self.k
return 1/(2**(k/2)*gamma(k/2))*x**(k/2 - 1)*exp(-x/2)
def _cdf(self, x):
k = self.k
return Piecewise(
(S.One/gamma(k/2)*lowergamma(k/2, x/2), x >= 0),
(0, True)
)
def _characteristic_function(self, t):
return (1 - 2*I*t)**(-self.k/2)
def _moment_generating_function(self, t):
return (1 - 2*t)**(-self.k/2)
def ChiSquared(name, k):
r"""
Create a continuous random variable with a Chi-squared distribution.
The density of the Chi-squared distribution is given by
.. math::
f(x) := \frac{1}{2^{\frac{k}{2}}\Gamma\left(\frac{k}{2}\right)}
x^{\frac{k}{2}-1} e^{-\frac{x}{2}}
with :math:`x \geq 0`.
Parameters
==========
k : Positive integer, The number of degrees of freedom
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import ChiSquared, density, E, variance, moment
>>> from sympy import Symbol
>>> k = Symbol("k", integer=True, positive=True)
>>> z = Symbol("z")
>>> X = ChiSquared("x", k)
>>> density(X)(z)
2**(-k/2)*z**(k/2 - 1)*exp(-z/2)/gamma(k/2)
>>> E(X)
k
>>> variance(X)
2*k
>>> moment(X, 3)
k**3 + 6*k**2 + 8*k
References
==========
.. [1] https://en.wikipedia.org/wiki/Chi_squared_distribution
.. [2] http://mathworld.wolfram.com/Chi-SquaredDistribution.html
"""
return rv(name, ChiSquaredDistribution, (k, ))
#-------------------------------------------------------------------------------
# Dagum distribution -----------------------------------------------------------
class DagumDistribution(SingleContinuousDistribution):
_argnames = ('p', 'a', 'b')
set = Interval(0, oo)
@staticmethod
def check(p, a, b):
_value_check(p > 0, "Shape parameter p must be positive.")
_value_check(a > 0, "Shape parameter a must be positive.")
_value_check(b > 0, "Scale parameter b must be positive.")
def pdf(self, x):
p, a, b = self.p, self.a, self.b
return a*p/x*((x/b)**(a*p)/(((x/b)**a + 1)**(p + 1)))
def _cdf(self, x):
p, a, b = self.p, self.a, self.b
return Piecewise(((S.One + (S(x)/b)**-a)**-p, x>=0),
(S.Zero, True))
def Dagum(name, p, a, b):
r"""
Create a continuous random variable with a Dagum distribution.
The density of the Dagum distribution is given by
.. math::
f(x) := \frac{a p}{x} \left( \frac{\left(\tfrac{x}{b}\right)^{a p}}
{\left(\left(\tfrac{x}{b}\right)^a + 1 \right)^{p+1}} \right)
with :math:`x > 0`.
Parameters
==========
p : Real number, `p > 0`, a shape
a : Real number, `a > 0`, a shape
b : Real number, `b > 0`, a scale
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Dagum, density, cdf
>>> from sympy import Symbol
>>> p = Symbol("p", positive=True)
>>> a = Symbol("a", positive=True)
>>> b = Symbol("b", positive=True)
>>> z = Symbol("z")
>>> X = Dagum("x", p, a, b)
>>> density(X)(z)
a*p*(z/b)**(a*p)*((z/b)**a + 1)**(-p - 1)/z
>>> cdf(X)(z)
Piecewise(((1 + (z/b)**(-a))**(-p), z >= 0), (0, True))
References
==========
.. [1] https://en.wikipedia.org/wiki/Dagum_distribution
"""
return rv(name, DagumDistribution, (p, a, b))
#-------------------------------------------------------------------------------
# Erlang distribution ----------------------------------------------------------
def Erlang(name, k, l):
r"""
Create a continuous random variable with an Erlang distribution.
The density of the Erlang distribution is given by
.. math::
f(x) := \frac{\lambda^k x^{k-1} e^{-\lambda x}}{(k-1)!}
with :math:`x \in [0,\infty]`.
Parameters
==========
k : Positive integer
l : Real number, `\lambda > 0`, the rate
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Erlang, density, cdf, E, variance
>>> from sympy import Symbol, simplify, pprint
>>> k = Symbol("k", integer=True, positive=True)
>>> l = Symbol("l", positive=True)
>>> z = Symbol("z")
>>> X = Erlang("x", k, l)
>>> D = density(X)(z)
>>> pprint(D, use_unicode=False)
k k - 1 -l*z
l *z *e
---------------
Gamma(k)
>>> C = cdf(X)(z)
>>> pprint(C, use_unicode=False)
/lowergamma(k, l*z)
|------------------ for z > 0
< Gamma(k)
|
\ 0 otherwise
>>> E(X)
k/l
>>> simplify(variance(X))
k/l**2
References
==========
.. [1] https://en.wikipedia.org/wiki/Erlang_distribution
.. [2] http://mathworld.wolfram.com/ErlangDistribution.html
"""
return rv(name, GammaDistribution, (k, S.One/l))
# -------------------------------------------------------------------------------
# ExGaussian distribution -----------------------------------------------------
class ExGaussianDistribution(SingleContinuousDistribution):
_argnames = ('mean', 'std', 'rate')
set = Interval(-oo, oo)
@staticmethod
def check(mean, std, rate):
_value_check(
std > 0, "Standard deviation of ExGaussian must be positive.")
_value_check(rate > 0, "Rate of ExGaussian must be positive.")
def pdf(self, x):
mean, std, rate = self.mean, self.std, self.rate
term1 = rate/2
term2 = exp(rate * (2 * mean + rate * std**2 - 2*x)/2)
term3 = erfc((mean + rate*std**2 - x)/(sqrt(2)*std))
return term1*term2*term3
def _cdf(self, x):
from sympy.stats import cdf
mean, std, rate = self.mean, self.std, self.rate
u = rate*(x - mean)
v = rate*std
GaussianCDF1 = cdf(Normal('x', 0, v))(u)
GaussianCDF2 = cdf(Normal('x', v**2, v))(u)
return GaussianCDF1 - exp(-u + (v**2/2) + log(GaussianCDF2))
def _characteristic_function(self, t):
mean, std, rate = self.mean, self.std, self.rate
term1 = (1 - I*t/rate)**(-1)
term2 = exp(I*mean*t - std**2*t**2/2)
return term1 * term2
def _moment_generating_function(self, t):
mean, std, rate = self.mean, self.std, self.rate
term1 = (1 - t/rate)**(-1)
term2 = exp(mean*t + std**2*t**2/2)
return term1*term2
def ExGaussian(name, mean, std, rate):
r"""
Create a continuous random variable with an Exponentially modified
Gaussian (EMG) distribution.
The density of the exponentially modified Gaussian distribution is given by
.. math::
f(x) := \frac{\lambda}{2}e^{\frac{\lambda}{2}(2\mu+\lambda\sigma^2-2x)}
\text{erfc}(\frac{\mu + \lambda\sigma^2 - x}{\sqrt{2}\sigma})
with `x > 0`. Note that the expected value is `1/\lambda`.
Parameters
==========
mu : A Real number, the mean of Gaussian component
std: A positive Real number,
:math: `\sigma^2 > 0` the variance of Gaussian component
lambda: A positive Real number,
:math: `\lambda > 0` the rate of Exponential component
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import ExGaussian, density, cdf, E
>>> from sympy.stats import variance, skewness
>>> from sympy import Symbol, pprint, simplify
>>> mean = Symbol("mu")
>>> std = Symbol("sigma", positive=True)
>>> rate = Symbol("lamda", positive=True)
>>> z = Symbol("z")
>>> X = ExGaussian("x", mean, std, rate)
>>> pprint(density(X)(z), use_unicode=False)
/ 2 \
lamda*\lamda*sigma + 2*mu - 2*z/
--------------------------------- / ___ / 2 \\
2 |\/ 2 *\lamda*sigma + mu - z/|
lamda*e *erfc|-----------------------------|
\ 2*sigma /
----------------------------------------------------------------------------
2
>>> cdf(X)(z)
-(erf(sqrt(2)*(-lamda**2*sigma**2 + lamda*(-mu + z))/(2*lamda*sigma))/2 + 1/2)*exp(lamda**2*sigma**2/2 - lamda*(-mu + z)) + erf(sqrt(2)*(-mu + z)/(2*sigma))/2 + 1/2
>>> E(X)
(lamda*mu + 1)/lamda
>>> simplify(variance(X))
sigma**2 + lamda**(-2)
>>> simplify(skewness(X))
2/(lamda**2*sigma**2 + 1)**(3/2)
References
==========
.. [1] https://en.wikipedia.org/wiki/Exponentially_modified_Gaussian_distribution
"""
return rv(name, ExGaussianDistribution, (mean, std, rate))
#-------------------------------------------------------------------------------
# Exponential distribution -----------------------------------------------------
class ExponentialDistribution(SingleContinuousDistribution):
_argnames = ('rate',)
set = Interval(0, oo)
@staticmethod
def check(rate):
_value_check(rate > 0, "Rate must be positive.")
def pdf(self, x):
return self.rate * exp(-self.rate*x)
def sample(self):
return random.expovariate(self.rate)
def _cdf(self, x):
return Piecewise(
(S.One - exp(-self.rate*x), x >= 0),
(0, True),
)
def _characteristic_function(self, t):
rate = self.rate
return rate / (rate - I*t)
def _moment_generating_function(self, t):
rate = self.rate
return rate / (rate - t)
def _quantile(self, p):
return -log(1-p)/self.rate
def Exponential(name, rate):
r"""
Create a continuous random variable with an Exponential distribution.
The density of the exponential distribution is given by
.. math::
f(x) := \lambda \exp(-\lambda x)
with `x > 0`. Note that the expected value is `1/\lambda`.
Parameters
==========
rate : A positive Real number, `\lambda > 0`, the rate (or inverse scale/inverse mean)
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Exponential, density, cdf, E
>>> from sympy.stats import variance, std, skewness, quantile
>>> from sympy import Symbol
>>> l = Symbol("lambda", positive=True)
>>> z = Symbol("z")
>>> p = Symbol("p")
>>> X = Exponential("x", l)
>>> density(X)(z)
lambda*exp(-lambda*z)
>>> cdf(X)(z)
Piecewise((1 - exp(-lambda*z), z >= 0), (0, True))
>>> quantile(X)(p)
-log(1 - p)/lambda
>>> E(X)
1/lambda
>>> variance(X)
lambda**(-2)
>>> skewness(X)
2
>>> X = Exponential('x', 10)
>>> density(X)(z)
10*exp(-10*z)
>>> E(X)
1/10
>>> std(X)
1/10
References
==========
.. [1] https://en.wikipedia.org/wiki/Exponential_distribution
.. [2] http://mathworld.wolfram.com/ExponentialDistribution.html
"""
return rv(name, ExponentialDistribution, (rate, ))
# -------------------------------------------------------------------------------
# Exponential Power distribution -----------------------------------------------------
class ExponentialPowerDistribution(SingleContinuousDistribution):
_argnames = ('mu', 'alpha', 'beta')
set = Interval(-oo, oo)
@staticmethod
def check(mu, alpha, beta):
_value_check(alpha > 0, "Scale parameter alpha must be positive.")
_value_check(beta > 0, "Shape parameter beta must be positive.")
def pdf(self, x):
mu, alpha, beta = self.mu, self.alpha, self.beta
num = beta*exp(-(Abs(x - mu)/alpha)**beta)
den = 2*alpha*gamma(1/beta)
return num/den
def _cdf(self, x):
mu, alpha, beta = self.mu, self.alpha, self.beta
num = lowergamma(1/beta, (Abs(x - mu) / alpha)**beta)
den = 2*gamma(1/beta)
return sign(x - mu)*num/den + S.Half
def ExponentialPower(name, mu, alpha, beta):
r"""
Create a Continuous Random Variable with Exponential Power distribution.
This distribution is known also as Generalized Normal
distribution version 1
The density of the Exponential Power distribution is given by
.. math::
f(x) := \frac{\beta}{2\alpha\Gamma(\frac{1}{\beta})}
e^{{-(\frac{|x - \mu|}{\alpha})^{\beta}}}
with :math:`x \in [ - \infty, \infty ]`.
Parameters
==========
mu : Real number, 'mu' is a location
alpha : Real number, 'alpha > 0' is a scale
beta : Real number, 'beta > 0' is a shape
Returns
=======
A RandomSymbol
Examples
========
>>> from sympy.stats import ExponentialPower, density, E, variance, cdf
>>> from sympy import Symbol, simplify, pprint
>>> z = Symbol("z")
>>> mu = Symbol("mu")
>>> alpha = Symbol("alpha", positive=True)
>>> beta = Symbol("beta", positive=True)
>>> X = ExponentialPower("x", mu, alpha, beta)
>>> pprint(density(X)(z), use_unicode=False)
beta
/|mu - z|\
-|--------|
\ alpha /
beta*e
---------------------
/ 1 \
2*alpha*Gamma|----|
\beta/
>>> cdf(X)(z)
1/2 + lowergamma(1/beta, (Abs(mu - z)/alpha)**beta)*sign(-mu + z)/(2*gamma(1/beta))
References
==========
.. [1] https://reference.wolfram.com/language/ref/ExponentialPowerDistribution.html
.. [2] https://en.wikipedia.org/wiki/Generalized_normal_distribution#Version_1
"""
return rv(name, ExponentialPowerDistribution, (mu, alpha, beta))
#-------------------------------------------------------------------------------
# F distribution ---------------------------------------------------------------
class FDistributionDistribution(SingleContinuousDistribution):
_argnames = ('d1', 'd2')
set = Interval(0, oo)
@staticmethod
def check(d1, d2):
_value_check((d1 > 0, d1.is_integer),
"Degrees of freedom d1 must be positive integer.")
_value_check((d2 > 0, d2.is_integer),
"Degrees of freedom d2 must be positive integer.")
def pdf(self, x):
d1, d2 = self.d1, self.d2
return (sqrt((d1*x)**d1*d2**d2 / (d1*x+d2)**(d1+d2))
/ (x * beta_fn(d1/2, d2/2)))
def _moment_generating_function(self, t):
raise NotImplementedError('The moment generating function for the '
'F-distribution does not exist.')
def FDistribution(name, d1, d2):
r"""
Create a continuous random variable with a F distribution.
The density of the F distribution is given by
.. math::
f(x) := \frac{\sqrt{\frac{(d_1 x)^{d_1} d_2^{d_2}}
{(d_1 x + d_2)^{d_1 + d_2}}}}
{x \mathrm{B} \left(\frac{d_1}{2}, \frac{d_2}{2}\right)}
with :math:`x > 0`.
Parameters
==========
d1 : `d_1 > 0`, where d_1 is the degrees of freedom (n_1 - 1)
d2 : `d_2 > 0`, where d_2 is the degrees of freedom (n_2 - 1)
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import FDistribution, density
>>> from sympy import Symbol, simplify, pprint
>>> d1 = Symbol("d1", positive=True)
>>> d2 = Symbol("d2", positive=True)
>>> z = Symbol("z")
>>> X = FDistribution("x", d1, d2)
>>> D = density(X)(z)
>>> pprint(D, use_unicode=False)
d2
-- ______________________________
2 / d1 -d1 - d2
d2 *\/ (d1*z) *(d1*z + d2)
--------------------------------------
/d1 d2\
z*B|--, --|
\2 2 /
References
==========
.. [1] https://en.wikipedia.org/wiki/F-distribution
.. [2] http://mathworld.wolfram.com/F-Distribution.html
"""
return rv(name, FDistributionDistribution, (d1, d2))
#-------------------------------------------------------------------------------
# Fisher Z distribution --------------------------------------------------------
class FisherZDistribution(SingleContinuousDistribution):
_argnames = ('d1', 'd2')
set = Interval(-oo, oo)
@staticmethod
def check(d1, d2):
_value_check(d1 > 0, "Degree of freedom d1 must be positive.")
_value_check(d2 > 0, "Degree of freedom d2 must be positive.")
def pdf(self, x):
d1, d2 = self.d1, self.d2
return (2*d1**(d1/2)*d2**(d2/2) / beta_fn(d1/2, d2/2) *
exp(d1*x) / (d1*exp(2*x)+d2)**((d1+d2)/2))
def FisherZ(name, d1, d2):
r"""
Create a Continuous Random Variable with an Fisher's Z distribution.
The density of the Fisher's Z distribution is given by
.. math::
f(x) := \frac{2d_1^{d_1/2} d_2^{d_2/2}} {\mathrm{B}(d_1/2, d_2/2)}
\frac{e^{d_1z}}{\left(d_1e^{2z}+d_2\right)^{\left(d_1+d_2\right)/2}}
.. TODO - What is the difference between these degrees of freedom?
Parameters
==========
d1 : `d_1 > 0`, degree of freedom
d2 : `d_2 > 0`, degree of freedom
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import FisherZ, density
>>> from sympy import Symbol, simplify, pprint
>>> d1 = Symbol("d1", positive=True)
>>> d2 = Symbol("d2", positive=True)
>>> z = Symbol("z")
>>> X = FisherZ("x", d1, d2)
>>> D = density(X)(z)
>>> pprint(D, use_unicode=False)
d1 d2
d1 d2 - -- - --
-- -- 2 2
2 2 / 2*z \ d1*z
2*d1 *d2 *\d1*e + d2/ *e
-----------------------------------------
/d1 d2\
B|--, --|
\2 2 /
References
==========
.. [1] https://en.wikipedia.org/wiki/Fisher%27s_z-distribution
.. [2] http://mathworld.wolfram.com/Fishersz-Distribution.html
"""
return rv(name, FisherZDistribution, (d1, d2))
#-------------------------------------------------------------------------------
# Frechet distribution ---------------------------------------------------------
class FrechetDistribution(SingleContinuousDistribution):
_argnames = ('a', 's', 'm')
set = Interval(0, oo)
@staticmethod
def check(a, s, m):
_value_check(a > 0, "Shape parameter alpha must be positive.")
_value_check(s > 0, "Scale parameter s must be positive.")
def __new__(cls, a, s=1, m=0):
a, s, m = list(map(sympify, (a, s, m)))
return Basic.__new__(cls, a, s, m)
def pdf(self, x):
a, s, m = self.a, self.s, self.m
return a/s * ((x-m)/s)**(-1-a) * exp(-((x-m)/s)**(-a))
def _cdf(self, x):
a, s, m = self.a, self.s, self.m
return Piecewise((exp(-((x-m)/s)**(-a)), x >= m),
(S.Zero, True))
def Frechet(name, a, s=1, m=0):
r"""
Create a continuous random variable with a Frechet distribution.
The density of the Frechet distribution is given by
.. math::
f(x) := \frac{\alpha}{s} \left(\frac{x-m}{s}\right)^{-1-\alpha}
e^{-(\frac{x-m}{s})^{-\alpha}}
with :math:`x \geq m`.
Parameters
==========
a : Real number, :math:`a \in \left(0, \infty\right)` the shape
s : Real number, :math:`s \in \left(0, \infty\right)` the scale
m : Real number, :math:`m \in \left(-\infty, \infty\right)` the minimum
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Frechet, density, E, std, cdf
>>> from sympy import Symbol, simplify
>>> a = Symbol("a", positive=True)
>>> s = Symbol("s", positive=True)
>>> m = Symbol("m", real=True)
>>> z = Symbol("z")
>>> X = Frechet("x", a, s, m)
>>> density(X)(z)
a*((-m + z)/s)**(-a - 1)*exp(-((-m + z)/s)**(-a))/s
>>> cdf(X)(z)
Piecewise((exp(-((-m + z)/s)**(-a)), m <= z), (0, True))
References
==========
.. [1] https://en.wikipedia.org/wiki/Fr%C3%A9chet_distribution
"""
return rv(name, FrechetDistribution, (a, s, m))
#-------------------------------------------------------------------------------
# Gamma distribution -----------------------------------------------------------
class GammaDistribution(SingleContinuousDistribution):
_argnames = ('k', 'theta')
set = Interval(0, oo)
@staticmethod
def check(k, theta):
_value_check(k > 0, "k must be positive")
_value_check(theta > 0, "Theta must be positive")
def pdf(self, x):
k, theta = self.k, self.theta
return x**(k - 1) * exp(-x/theta) / (gamma(k)*theta**k)
def sample(self):
return random.gammavariate(self.k, self.theta)
def _cdf(self, x):
k, theta = self.k, self.theta
return Piecewise(
(lowergamma(k, S(x)/theta)/gamma(k), x > 0),
(S.Zero, True))
def _characteristic_function(self, t):
return (1 - self.theta*I*t)**(-self.k)
def _moment_generating_function(self, t):
return (1- self.theta*t)**(-self.k)
def Gamma(name, k, theta):
r"""
Create a continuous random variable with a Gamma distribution.
The density of the Gamma distribution is given by
.. math::
f(x) := \frac{1}{\Gamma(k) \theta^k} x^{k - 1} e^{-\frac{x}{\theta}}
with :math:`x \in [0,1]`.
Parameters
==========
k : Real number, `k > 0`, a shape
theta : Real number, `\theta > 0`, a scale
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Gamma, density, cdf, E, variance
>>> from sympy import Symbol, pprint, simplify
>>> k = Symbol("k", positive=True)
>>> theta = Symbol("theta", positive=True)
>>> z = Symbol("z")
>>> X = Gamma("x", k, theta)
>>> D = density(X)(z)
>>> pprint(D, use_unicode=False)
-z
-----
-k k - 1 theta
theta *z *e
---------------------
Gamma(k)
>>> C = cdf(X, meijerg=True)(z)
>>> pprint(C, use_unicode=False)
/ / z \
|k*lowergamma|k, -----|
| \ theta/
<---------------------- for z >= 0
| Gamma(k + 1)
|
\ 0 otherwise
>>> E(X)
k*theta
>>> V = simplify(variance(X))
>>> pprint(V, use_unicode=False)
2
k*theta
References
==========
.. [1] https://en.wikipedia.org/wiki/Gamma_distribution
.. [2] http://mathworld.wolfram.com/GammaDistribution.html
"""
return rv(name, GammaDistribution, (k, theta))
#-------------------------------------------------------------------------------
# Inverse Gamma distribution ---------------------------------------------------
class GammaInverseDistribution(SingleContinuousDistribution):
_argnames = ('a', 'b')
set = Interval(0, oo)
@staticmethod
def check(a, b):
_value_check(a > 0, "alpha must be positive")
_value_check(b > 0, "beta must be positive")
def pdf(self, x):
a, b = self.a, self.b
return b**a/gamma(a) * x**(-a-1) * exp(-b/x)
def _cdf(self, x):
a, b = self.a, self.b
return Piecewise((uppergamma(a,b/x)/gamma(a), x > 0),
(S.Zero, True))
def sample(self):
scipy = import_module('scipy')
if scipy:
from scipy.stats import invgamma
return invgamma.rvs(float(self.a), 0, float(self.b))
else:
raise NotImplementedError('Sampling the Inverse Gamma Distribution requires Scipy.')
def _characteristic_function(self, t):
a, b = self.a, self.b
return 2 * (-I*b*t)**(a/2) * besselk(sqrt(-4*I*b*t)) / gamma(a)
def _moment_generating_function(self, t):
raise NotImplementedError('The moment generating function for the '
'gamma inverse distribution does not exist.')
def GammaInverse(name, a, b):
r"""
Create a continuous random variable with an inverse Gamma distribution.
The density of the inverse Gamma distribution is given by
.. math::
f(x) := \frac{\beta^\alpha}{\Gamma(\alpha)} x^{-\alpha - 1}
\exp\left(\frac{-\beta}{x}\right)
with :math:`x > 0`.
Parameters
==========
a : Real number, `a > 0` a shape
b : Real number, `b > 0` a scale
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import GammaInverse, density, cdf, E, variance
>>> from sympy import Symbol, pprint
>>> a = Symbol("a", positive=True)
>>> b = Symbol("b", positive=True)
>>> z = Symbol("z")
>>> X = GammaInverse("x", a, b)
>>> D = density(X)(z)
>>> pprint(D, use_unicode=False)
-b
---
a -a - 1 z
b *z *e
---------------
Gamma(a)
>>> cdf(X)(z)
Piecewise((uppergamma(a, b/z)/gamma(a), z > 0), (0, True))
References
==========
.. [1] https://en.wikipedia.org/wiki/Inverse-gamma_distribution
"""
return rv(name, GammaInverseDistribution, (a, b))
#-------------------------------------------------------------------------------
# Gumbel distribution (Maximum and Minimum) --------------------------------------------------------
class GumbelDistribution(SingleContinuousDistribution):
_argnames = ('beta', 'mu', 'minimum')
set = Interval(-oo, oo)
@staticmethod
def check(beta, mu, minimum):
_value_check(beta > 0, "Scale parameter beta must be positive.")
def pdf(self, x):
beta, mu = self.beta, self.mu
z = (x - mu)/beta
f_max = (1/beta)*exp(-z - exp(-z))
f_min = (1/beta)*exp(z - exp(z))
return Piecewise((f_min, self.minimum), (f_max, not self.minimum))
def _cdf(self, x):
beta, mu = self.beta, self.mu
z = (x - mu)/beta
F_max = exp(-exp(-z))
F_min = 1 - exp(-exp(z))
return Piecewise((F_min, self.minimum), (F_max, not self.minimum))
def _characteristic_function(self, t):
cf_max = gamma(1 - I*self.beta*t) * exp(I*self.mu*t)
cf_min = gamma(1 + I*self.beta*t) * exp(I*self.mu*t)
return Piecewise((cf_min, self.minimum), (cf_max, not self.minimum))
def _moment_generating_function(self, t):
mgf_max = gamma(1 - self.beta*t) * exp(self.mu*t)
mgf_min = gamma(1 + self.beta*t) * exp(self.mu*t)
return Piecewise((mgf_min, self.minimum), (mgf_max, not self.minimum))
def Gumbel(name, beta, mu, minimum=False):
r"""
Create a Continuous Random Variable with Gumbel distribution.
The density of the Gumbel distribution is given by
For Maximum
.. math::
f(x) := \dfrac{1}{\beta} \exp \left( -\dfrac{x-\mu}{\beta}
- \exp \left( -\dfrac{x - \mu}{\beta} \right) \right)
with :math:`x \in [ - \infty, \infty ]`.
For Minimum
.. math::
f(x) := \frac{e^{- e^{\frac{- \mu + x}{\beta}} + \frac{- \mu + x}{\beta}}}{\beta}
with :math:`x \in [ - \infty, \infty ]`.
Parameters
==========
mu : Real number, 'mu' is a location
beta : Real number, 'beta > 0' is a scale
minimum : Boolean, by default, False, set to True for enabling minimum distribution
Returns
=======
A RandomSymbol
Examples
========
>>> from sympy.stats import Gumbel, density, E, variance, cdf
>>> from sympy import Symbol, simplify, pprint
>>> x = Symbol("x")
>>> mu = Symbol("mu")
>>> beta = Symbol("beta", positive=True)
>>> X = Gumbel("x", beta, mu)
>>> density(X)(x)
exp(-exp(-(-mu + x)/beta) - (-mu + x)/beta)/beta
>>> cdf(X)(x)
exp(-exp(-(-mu + x)/beta))
References
==========
.. [1] http://mathworld.wolfram.com/GumbelDistribution.html
.. [2] https://en.wikipedia.org/wiki/Gumbel_distribution
.. [3] http://www.mathwave.com/help/easyfit/html/analyses/distributions/gumbel_max.html
.. [4] http://www.mathwave.com/help/easyfit/html/analyses/distributions/gumbel_min.html
"""
return rv(name, GumbelDistribution, (beta, mu, minimum))
#-------------------------------------------------------------------------------
# Gompertz distribution --------------------------------------------------------
class GompertzDistribution(SingleContinuousDistribution):
_argnames = ('b', 'eta')
set = Interval(0, oo)
@staticmethod
def check(b, eta):
_value_check(b > 0, "b must be positive")
_value_check(eta > 0, "eta must be positive")
def pdf(self, x):
eta, b = self.eta, self.b
return b*eta*exp(b*x)*exp(eta)*exp(-eta*exp(b*x))
def _cdf(self, x):
eta, b = self.eta, self.b
return 1 - exp(eta)*exp(-eta*exp(b*x))
def _moment_generating_function(self, t):
eta, b = self.eta, self.b
return eta * exp(eta) * expint(t/b, eta)
def Gompertz(name, b, eta):
r"""
Create a Continuous Random Variable with Gompertz distribution.
The density of the Gompertz distribution is given by
.. math::
f(x) := b \eta e^{b x} e^{\eta} \exp \left(-\eta e^{bx} \right)
with :math: 'x \in [0, \inf)'.
Parameters
==========
b: Real number, 'b > 0' a scale
eta: Real number, 'eta > 0' a shape
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Gompertz, density, E, variance
>>> from sympy import Symbol, simplify, pprint
>>> b = Symbol("b", positive=True)
>>> eta = Symbol("eta", positive=True)
>>> z = Symbol("z")
>>> X = Gompertz("x", b, eta)
>>> density(X)(z)
b*eta*exp(eta)*exp(b*z)*exp(-eta*exp(b*z))
References
==========
.. [1] https://en.wikipedia.org/wiki/Gompertz_distribution
"""
return rv(name, GompertzDistribution, (b, eta))
#-------------------------------------------------------------------------------
# Kumaraswamy distribution -----------------------------------------------------
class KumaraswamyDistribution(SingleContinuousDistribution):
_argnames = ('a', 'b')
set = Interval(0, oo)
@staticmethod
def check(a, b):
_value_check(a > 0, "a must be positive")
_value_check(b > 0, "b must be positive")
def pdf(self, x):
a, b = self.a, self.b
return a * b * x**(a-1) * (1-x**a)**(b-1)
def _cdf(self, x):
a, b = self.a, self.b
return Piecewise(
(S.Zero, x < S.Zero),
(1 - (1 - x**a)**b, x <= S.One),
(S.One, True))
def Kumaraswamy(name, a, b):
r"""
Create a Continuous Random Variable with a Kumaraswamy distribution.
The density of the Kumaraswamy distribution is given by
.. math::
f(x) := a b x^{a-1} (1-x^a)^{b-1}
with :math:`x \in [0,1]`.
Parameters
==========
a : Real number, `a > 0` a shape
b : Real number, `b > 0` a shape
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Kumaraswamy, density, E, variance, cdf
>>> from sympy import Symbol, simplify, pprint
>>> a = Symbol("a", positive=True)
>>> b = Symbol("b", positive=True)
>>> z = Symbol("z")
>>> X = Kumaraswamy("x", a, b)
>>> D = density(X)(z)
>>> pprint(D, use_unicode=False)
b - 1
a - 1 / a\
a*b*z *\1 - z /
>>> cdf(X)(z)
Piecewise((0, z < 0), (1 - (1 - z**a)**b, z <= 1), (1, True))
References
==========
.. [1] https://en.wikipedia.org/wiki/Kumaraswamy_distribution
"""
return rv(name, KumaraswamyDistribution, (a, b))
#-------------------------------------------------------------------------------
# Laplace distribution ---------------------------------------------------------
class LaplaceDistribution(SingleContinuousDistribution):
_argnames = ('mu', 'b')
set = Interval(-oo, oo)
@staticmethod
def check(mu, b):
_value_check(b > 0, "Scale parameter b must be positive.")
_value_check(mu.is_real, "Location parameter mu should be real")
def pdf(self, x):
mu, b = self.mu, self.b
return 1/(2*b)*exp(-Abs(x - mu)/b)
def _cdf(self, x):
mu, b = self.mu, self.b
return Piecewise(
(S.Half*exp((x - mu)/b), x < mu),
(S.One - S.Half*exp(-(x - mu)/b), x >= mu)
)
def _characteristic_function(self, t):
return exp(self.mu*I*t) / (1 + self.b**2*t**2)
def _moment_generating_function(self, t):
return exp(self.mu*t) / (1 - self.b**2*t**2)
def Laplace(name, mu, b):
r"""
Create a continuous random variable with a Laplace distribution.
The density of the Laplace distribution is given by
.. math::
f(x) := \frac{1}{2 b} \exp \left(-\frac{|x-\mu|}b \right)
Parameters
==========
mu : Real number or a list/matrix, the location (mean) or the
location vector
b : Real number or a positive definite matrix, representing a scale
or the covariance matrix.
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Laplace, density, cdf
>>> from sympy import Symbol, pprint
>>> mu = Symbol("mu")
>>> b = Symbol("b", positive=True)
>>> z = Symbol("z")
>>> X = Laplace("x", mu, b)
>>> density(X)(z)
exp(-Abs(mu - z)/b)/(2*b)
>>> cdf(X)(z)
Piecewise((exp((-mu + z)/b)/2, mu > z), (1 - exp((mu - z)/b)/2, True))
>>> L = Laplace('L', [1, 2], [[1, 0], [0, 1]])
>>> pprint(density(L)(1, 2), use_unicode=False)
5 / ____\
e *besselk\0, \/ 35 /
---------------------
pi
References
==========
.. [1] https://en.wikipedia.org/wiki/Laplace_distribution
.. [2] http://mathworld.wolfram.com/LaplaceDistribution.html
"""
if isinstance(mu, (list, MatrixBase)) and\
isinstance(b, (list, MatrixBase)):
from sympy.stats.joint_rv_types import MultivariateLaplaceDistribution
return multivariate_rv(
MultivariateLaplaceDistribution, name, mu, b)
return rv(name, LaplaceDistribution, (mu, b))
#-------------------------------------------------------------------------------
# Logistic distribution --------------------------------------------------------
class LogisticDistribution(SingleContinuousDistribution):
_argnames = ('mu', 's')
set = Interval(-oo, oo)
@staticmethod
def check(mu, s):
_value_check(s > 0, "Scale parameter s must be positive.")
def pdf(self, x):
mu, s = self.mu, self.s
return exp(-(x - mu)/s)/(s*(1 + exp(-(x - mu)/s))**2)
def _cdf(self, x):
mu, s = self.mu, self.s
return S.One/(1 + exp(-(x - mu)/s))
def _characteristic_function(self, t):
return Piecewise((exp(I*t*self.mu) * pi*self.s*t / sinh(pi*self.s*t), Ne(t, 0)), (S.One, True))
def _moment_generating_function(self, t):
return exp(self.mu*t) * beta_fn(1 - self.s*t, 1 + self.s*t)
def _quantile(self, p):
return self.mu - self.s*log(-S.One + S.One/p)
def Logistic(name, mu, s):
r"""
Create a continuous random variable with a logistic distribution.
The density of the logistic distribution is given by
.. math::
f(x) := \frac{e^{-(x-\mu)/s}} {s\left(1+e^{-(x-\mu)/s}\right)^2}
Parameters
==========
mu : Real number, the location (mean)
s : Real number, `s > 0` a scale
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Logistic, density, cdf
>>> from sympy import Symbol
>>> mu = Symbol("mu", real=True)
>>> s = Symbol("s", positive=True)
>>> z = Symbol("z")
>>> X = Logistic("x", mu, s)
>>> density(X)(z)
exp((mu - z)/s)/(s*(exp((mu - z)/s) + 1)**2)
>>> cdf(X)(z)
1/(exp((mu - z)/s) + 1)
References
==========
.. [1] https://en.wikipedia.org/wiki/Logistic_distribution
.. [2] http://mathworld.wolfram.com/LogisticDistribution.html
"""
return rv(name, LogisticDistribution, (mu, s))
#-------------------------------------------------------------------------------
# Log-logistic distribution --------------------------------------------------------
class LogLogisticDistribution(SingleContinuousDistribution):
_argnames = ('alpha', 'beta')
set = Interval(0, oo)
@staticmethod
def check(alpha, beta):
_value_check(alpha > 0, "Scale parameter Alpha must be positive.")
_value_check(beta > 0, "Shape parameter Beta must be positive.")
def pdf(self, x):
a, b = self.alpha, self.beta
return ((b/a)*(x/a)**(b - 1))/(1 + (x/a)**b)**2
def _cdf(self, x):
a, b = self.alpha, self.beta
return 1/(1 + (x/a)**(-b))
def _quantile(self, p):
a, b = self.alpha, self.beta
return a*((p/(1 - p))**(1/b))
def expectation(self, expr, var, **kwargs):
a, b = self.args
return Piecewise((S.NaN, b <= 1), (pi*a/(b*sin(pi/b)), True))
def LogLogistic(name, alpha, beta):
r"""
Create a continuous random variable with a log-logistic distribution.
The distribution is unimodal when `beta > 1`.
The density of the log-logistic distribution is given by
.. math::
f(x) := \frac{(\frac{\beta}{\alpha})(\frac{x}{\alpha})^{\beta - 1}}
{(1 + (\frac{x}{\alpha})^{\beta})^2}
Parameters
==========
alpha : Real number, `\alpha > 0`, scale parameter and median of distribution
beta : Real number, `\beta > 0` a shape parameter
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import LogLogistic, density, cdf, quantile
>>> from sympy import Symbol, pprint
>>> alpha = Symbol("alpha", real=True, positive=True)
>>> beta = Symbol("beta", real=True, positive=True)
>>> p = Symbol("p")
>>> z = Symbol("z", positive=True)
>>> X = LogLogistic("x", alpha, beta)
>>> D = density(X)(z)
>>> pprint(D, use_unicode=False)
beta - 1
/ z \
beta*|-----|
\alpha/
------------------------
2
/ beta \
|/ z \ |
alpha*||-----| + 1|
\\alpha/ /
>>> cdf(X)(z)
1/(1 + (z/alpha)**(-beta))
>>> quantile(X)(p)
alpha*(p/(1 - p))**(1/beta)
References
==========
.. [1] https://en.wikipedia.org/wiki/Log-logistic_distribution
"""
return rv(name, LogLogisticDistribution, (alpha, beta))
#-------------------------------------------------------------------------------
# Log Normal distribution ------------------------------------------------------
class LogNormalDistribution(SingleContinuousDistribution):
_argnames = ('mean', 'std')
set = Interval(0, oo)
@staticmethod
def check(mean, std):
_value_check(std > 0, "Parameter std must be positive.")
def pdf(self, x):
mean, std = self.mean, self.std
return exp(-(log(x) - mean)**2 / (2*std**2)) / (x*sqrt(2*pi)*std)
def sample(self):
return random.lognormvariate(self.mean, self.std)
def _cdf(self, x):
mean, std = self.mean, self.std
return Piecewise(
(S.Half + S.Half*erf((log(x) - mean)/sqrt(2)/std), x > 0),
(S.Zero, True)
)
def _moment_generating_function(self, t):
raise NotImplementedError('Moment generating function of the log-normal distribution is not defined.')
def LogNormal(name, mean, std):
r"""
Create a continuous random variable with a log-normal distribution.
The density of the log-normal distribution is given by
.. math::
f(x) := \frac{1}{x\sqrt{2\pi\sigma^2}}
e^{-\frac{\left(\ln x-\mu\right)^2}{2\sigma^2}}
with :math:`x \geq 0`.
Parameters
==========
mu : Real number, the log-scale
sigma : Real number, :math:`\sigma^2 > 0` a shape
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import LogNormal, density
>>> from sympy import Symbol, simplify, pprint
>>> mu = Symbol("mu", real=True)
>>> sigma = Symbol("sigma", positive=True)
>>> z = Symbol("z")
>>> X = LogNormal("x", mu, sigma)
>>> D = density(X)(z)
>>> pprint(D, use_unicode=False)
2
-(-mu + log(z))
-----------------
2
___ 2*sigma
\/ 2 *e
------------------------
____
2*\/ pi *sigma*z
>>> X = LogNormal('x', 0, 1) # Mean 0, standard deviation 1
>>> density(X)(z)
sqrt(2)*exp(-log(z)**2/2)/(2*sqrt(pi)*z)
References
==========
.. [1] https://en.wikipedia.org/wiki/Lognormal
.. [2] http://mathworld.wolfram.com/LogNormalDistribution.html
"""
return rv(name, LogNormalDistribution, (mean, std))
#-------------------------------------------------------------------------------
# Maxwell distribution ---------------------------------------------------------
class MaxwellDistribution(SingleContinuousDistribution):
_argnames = ('a',)
set = Interval(0, oo)
@staticmethod
def check(a):
_value_check(a > 0, "Parameter a must be positive.")
def pdf(self, x):
a = self.a
return sqrt(2/pi)*x**2*exp(-x**2/(2*a**2))/a**3
def _cdf(self, x):
a = self.a
return erf(sqrt(2)*x/(2*a)) - sqrt(2)*x*exp(-x**2/(2*a**2))/(sqrt(pi)*a)
def Maxwell(name, a):
r"""
Create a continuous random variable with a Maxwell distribution.
The density of the Maxwell distribution is given by
.. math::
f(x) := \sqrt{\frac{2}{\pi}} \frac{x^2 e^{-x^2/(2a^2)}}{a^3}
with :math:`x \geq 0`.
.. TODO - what does the parameter mean?
Parameters
==========
a : Real number, `a > 0`
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Maxwell, density, E, variance
>>> from sympy import Symbol, simplify
>>> a = Symbol("a", positive=True)
>>> z = Symbol("z")
>>> X = Maxwell("x", a)
>>> density(X)(z)
sqrt(2)*z**2*exp(-z**2/(2*a**2))/(sqrt(pi)*a**3)
>>> E(X)
2*sqrt(2)*a/sqrt(pi)
>>> simplify(variance(X))
a**2*(-8 + 3*pi)/pi
References
==========
.. [1] https://en.wikipedia.org/wiki/Maxwell_distribution
.. [2] http://mathworld.wolfram.com/MaxwellDistribution.html
"""
return rv(name, MaxwellDistribution, (a, ))
#-------------------------------------------------------------------------------
# Nakagami distribution --------------------------------------------------------
class NakagamiDistribution(SingleContinuousDistribution):
_argnames = ('mu', 'omega')
set = Interval(0, oo)
@staticmethod
def check(mu, omega):
_value_check(mu >= S.Half, "Shape parameter mu must be greater than equal to 1/2.")
_value_check(omega > 0, "Spread parameter omega must be positive.")
def pdf(self, x):
mu, omega = self.mu, self.omega
return 2*mu**mu/(gamma(mu)*omega**mu)*x**(2*mu - 1)*exp(-mu/omega*x**2)
def _cdf(self, x):
mu, omega = self.mu, self.omega
return Piecewise(
(lowergamma(mu, (mu/omega)*x**2)/gamma(mu), x > 0),
(S.Zero, True))
def Nakagami(name, mu, omega):
r"""
Create a continuous random variable with a Nakagami distribution.
The density of the Nakagami distribution is given by
.. math::
f(x) := \frac{2\mu^\mu}{\Gamma(\mu)\omega^\mu} x^{2\mu-1}
\exp\left(-\frac{\mu}{\omega}x^2 \right)
with :math:`x > 0`.
Parameters
==========
mu : Real number, `\mu \geq \frac{1}{2}` a shape
omega : Real number, `\omega > 0`, the spread
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Nakagami, density, E, variance, cdf
>>> from sympy import Symbol, simplify, pprint
>>> mu = Symbol("mu", positive=True)
>>> omega = Symbol("omega", positive=True)
>>> z = Symbol("z")
>>> X = Nakagami("x", mu, omega)
>>> D = density(X)(z)
>>> pprint(D, use_unicode=False)
2
-mu*z
-------
mu -mu 2*mu - 1 omega
2*mu *omega *z *e
----------------------------------
Gamma(mu)
>>> simplify(E(X))
sqrt(mu)*sqrt(omega)*gamma(mu + 1/2)/gamma(mu + 1)
>>> V = simplify(variance(X))
>>> pprint(V, use_unicode=False)
2
omega*Gamma (mu + 1/2)
omega - -----------------------
Gamma(mu)*Gamma(mu + 1)
>>> cdf(X)(z)
Piecewise((lowergamma(mu, mu*z**2/omega)/gamma(mu), z > 0),
(0, True))
References
==========
.. [1] https://en.wikipedia.org/wiki/Nakagami_distribution
"""
return rv(name, NakagamiDistribution, (mu, omega))
#-------------------------------------------------------------------------------
# Normal distribution ----------------------------------------------------------
class NormalDistribution(SingleContinuousDistribution):
_argnames = ('mean', 'std')
@staticmethod
def check(mean, std):
_value_check(std > 0, "Standard deviation must be positive")
def pdf(self, x):
return exp(-(x - self.mean)**2 / (2*self.std**2)) / (sqrt(2*pi)*self.std)
def sample(self):
return random.normalvariate(self.mean, self.std)
def _cdf(self, x):
mean, std = self.mean, self.std
return erf(sqrt(2)*(-mean + x)/(2*std))/2 + S.Half
def _characteristic_function(self, t):
mean, std = self.mean, self.std
return exp(I*mean*t - std**2*t**2/2)
def _moment_generating_function(self, t):
mean, std = self.mean, self.std
return exp(mean*t + std**2*t**2/2)
def _quantile(self, p):
mean, std = self.mean, self.std
return mean + std*sqrt(2)*erfinv(2*p - 1)
def Normal(name, mean, std):
r"""
Create a continuous random variable with a Normal distribution.
The density of the Normal distribution is given by
.. math::
f(x) := \frac{1}{\sigma\sqrt{2\pi}} e^{ -\frac{(x-\mu)^2}{2\sigma^2} }
Parameters
==========
mu : Real number or a list representing the mean or the mean vector
sigma : Real number or a positive definite square matrix,
:math:`\sigma^2 > 0` the variance
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Normal, density, E, std, cdf, skewness, quantile
>>> from sympy import Symbol, simplify, pprint, factor, together, factor_terms
>>> mu = Symbol("mu")
>>> sigma = Symbol("sigma", positive=True)
>>> z = Symbol("z")
>>> y = Symbol("y")
>>> p = Symbol("p")
>>> X = Normal("x", mu, sigma)
>>> density(X)(z)
sqrt(2)*exp(-(-mu + z)**2/(2*sigma**2))/(2*sqrt(pi)*sigma)
>>> C = simplify(cdf(X))(z) # it needs a little more help...
>>> pprint(C, use_unicode=False)
/ ___ \
|\/ 2 *(-mu + z)|
erf|---------------|
\ 2*sigma / 1
-------------------- + -
2 2
>>> quantile(X)(p)
mu + sqrt(2)*sigma*erfinv(2*p - 1)
>>> simplify(skewness(X))
0
>>> X = Normal("x", 0, 1) # Mean 0, standard deviation 1
>>> density(X)(z)
sqrt(2)*exp(-z**2/2)/(2*sqrt(pi))
>>> E(2*X + 1)
1
>>> simplify(std(2*X + 1))
2
>>> m = Normal('X', [1, 2], [[2, 1], [1, 2]])
>>> from sympy.stats.joint_rv import marginal_distribution
>>> pprint(density(m)(y, z), use_unicode=False)
/1 y\ /2*y z\ / z\ / y 2*z \
|- - -|*|--- - -| + |1 - -|*|- - + --- - 1|
___ \2 2/ \ 3 3/ \ 2/ \ 3 3 /
\/ 3 *e
--------------------------------------------------
6*pi
>>> marginal_distribution(m, m[0])(1)
1/(2*sqrt(pi))
References
==========
.. [1] https://en.wikipedia.org/wiki/Normal_distribution
.. [2] http://mathworld.wolfram.com/NormalDistributionFunction.html
"""
if isinstance(mean, (list, MatrixBase, MatrixExpr)) and\
isinstance(std, (list, MatrixBase, MatrixExpr)):
from sympy.stats.joint_rv_types import MultivariateNormalDistribution
return multivariate_rv(
MultivariateNormalDistribution, name, mean, std)
return rv(name, NormalDistribution, (mean, std))
#-------------------------------------------------------------------------------
# Inverse Gaussian distribution ----------------------------------------------------------
class GaussianInverseDistribution(SingleContinuousDistribution):
_argnames = ('mean', 'shape')
@property
def set(self):
return Interval(0, oo)
@staticmethod
def check(mean, shape):
_value_check(shape > 0, "Shape parameter must be positive")
_value_check(mean > 0, "Mean must be positive")
def pdf(self, x):
mu, s = self.mean, self.shape
return exp(-s*(x - mu)**2 / (2*x*mu**2)) * sqrt(s/((2*pi*x**3)))
def sample(self):
scipy = import_module('scipy')
if scipy:
from scipy.stats import invgauss
return invgauss.rvs(float(self.mean/self.shape), 0, float(self.shape))
else:
raise NotImplementedError(
'Sampling the Inverse Gaussian Distribution requires Scipy.')
def _cdf(self, x):
from sympy.stats import cdf
mu, s = self.mean, self.shape
stdNormalcdf = cdf(Normal('x', 0, 1))
first_term = stdNormalcdf(sqrt(s/x) * ((x/mu) - S.One))
second_term = exp(2*s/mu) * stdNormalcdf(-sqrt(s/x)*(x/mu + S.One))
return first_term + second_term
def _characteristic_function(self, t):
mu, s = self.mean, self.shape
return exp((s/mu)*(1 - sqrt(1 - (2*mu**2*I*t)/s)))
def _moment_generating_function(self, t):
mu, s = self.mean, self.shape
return exp((s/mu)*(1 - sqrt(1 - (2*mu**2*t)/s)))
def GaussianInverse(name, mean, shape):
r"""
Create a continuous random variable with an Inverse Gaussian distribution.
Inverse Gaussian distribution is also known as Wald distribution.
The density of the Inverse Gaussian distribution is given by
.. math::
f(x) := \sqrt{\frac{\lambda}{2\pi x^3}} e^{-\frac{\lambda(x-\mu)^2}{2x\mu^2}}
Parameters
==========
mu : Positive number representing the mean
lambda : Positive number representing the shape parameter
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import GaussianInverse, density, cdf, E, std, skewness
>>> from sympy import Symbol, pprint
>>> mu = Symbol("mu", positive=True)
>>> lamda = Symbol("lambda", positive=True)
>>> z = Symbol("z", positive=True)
>>> X = GaussianInverse("x", mu, lamda)
>>> D = density(X)(z)
>>> pprint(D, use_unicode=False)
2
-lambda*(-mu + z)
-------------------
2
___ ________ 2*mu *z
\/ 2 *\/ lambda *e
-------------------------------------
____ 3/2
2*\/ pi *z
>>> E(X)
mu
>>> std(X).expand()
mu**(3/2)/sqrt(lambda)
>>> skewness(X).expand()
3*sqrt(mu)/sqrt(lambda)
References
==========
.. [1] https://en.wikipedia.org/wiki/Inverse_Gaussian_distribution
.. [2] http://mathworld.wolfram.com/InverseGaussianDistribution.html
"""
return rv(name, GaussianInverseDistribution, (mean, shape))
Wald = GaussianInverse
#-------------------------------------------------------------------------------
# Pareto distribution ----------------------------------------------------------
class ParetoDistribution(SingleContinuousDistribution):
_argnames = ('xm', 'alpha')
@property
def set(self):
return Interval(self.xm, oo)
@staticmethod
def check(xm, alpha):
_value_check(xm > 0, "Xm must be positive")
_value_check(alpha > 0, "Alpha must be positive")
def pdf(self, x):
xm, alpha = self.xm, self.alpha
return alpha * xm**alpha / x**(alpha + 1)
def sample(self):
return random.paretovariate(self.alpha)
def _cdf(self, x):
xm, alpha = self.xm, self.alpha
return Piecewise(
(S.One - xm**alpha/x**alpha, x>=xm),
(0, True),
)
def _moment_generating_function(self, t):
xm, alpha = self.xm, self.alpha
return alpha * (-xm*t)**alpha * uppergamma(-alpha, -xm*t)
def _characteristic_function(self, t):
xm, alpha = self.xm, self.alpha
return alpha * (-I * xm * t) ** alpha * uppergamma(-alpha, -I * xm * t)
def Pareto(name, xm, alpha):
r"""
Create a continuous random variable with the Pareto distribution.
The density of the Pareto distribution is given by
.. math::
f(x) := \frac{\alpha\,x_m^\alpha}{x^{\alpha+1}}
with :math:`x \in [x_m,\infty]`.
Parameters
==========
xm : Real number, `x_m > 0`, a scale
alpha : Real number, `\alpha > 0`, a shape
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Pareto, density
>>> from sympy import Symbol
>>> xm = Symbol("xm", positive=True)
>>> beta = Symbol("beta", positive=True)
>>> z = Symbol("z")
>>> X = Pareto("x", xm, beta)
>>> density(X)(z)
beta*xm**beta*z**(-beta - 1)
References
==========
.. [1] https://en.wikipedia.org/wiki/Pareto_distribution
.. [2] http://mathworld.wolfram.com/ParetoDistribution.html
"""
return rv(name, ParetoDistribution, (xm, alpha))
#-------------------------------------------------------------------------------
# QuadraticU distribution ------------------------------------------------------
class QuadraticUDistribution(SingleContinuousDistribution):
_argnames = ('a', 'b')
@property
def set(self):
return Interval(self.a, self.b)
@staticmethod
def check(a, b):
_value_check(b > a, "Parameter b must be in range (%s, oo)."%(a))
def pdf(self, x):
a, b = self.a, self.b
alpha = 12 / (b-a)**3
beta = (a+b) / 2
return Piecewise(
(alpha * (x-beta)**2, And(a<=x, x<=b)),
(S.Zero, True))
def _moment_generating_function(self, t):
a, b = self.a, self.b
return -3 * (exp(a*t) * (4 + (a**2 + 2*a*(-2 + b) + b**2) * t) - exp(b*t) * (4 + (-4*b + (a + b)**2) * t)) / ((a-b)**3 * t**2)
def _characteristic_function(self, t):
def _moment_generating_function(self, t):
a, b = self.a, self.b
return -3*I*(exp(I*a*t*exp(I*b*t)) * (4*I - (-4*b + (a+b)**2)*t)) / ((a-b)**3 * t**2)
def QuadraticU(name, a, b):
r"""
Create a Continuous Random Variable with a U-quadratic distribution.
The density of the U-quadratic distribution is given by
.. math::
f(x) := \alpha (x-\beta)^2
with :math:`x \in [a,b]`.
Parameters
==========
a : Real number
b : Real number, :math:`a < b`
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import QuadraticU, density, E, variance
>>> from sympy import Symbol, simplify, factor, pprint
>>> a = Symbol("a", real=True)
>>> b = Symbol("b", real=True)
>>> z = Symbol("z")
>>> X = QuadraticU("x", a, b)
>>> D = density(X)(z)
>>> pprint(D, use_unicode=False)
/ 2
| / a b \
|12*|- - - - + z|
| \ 2 2 /
<----------------- for And(b >= z, a <= z)
| 3
| (-a + b)
|
\ 0 otherwise
References
==========
.. [1] https://en.wikipedia.org/wiki/U-quadratic_distribution
"""
return rv(name, QuadraticUDistribution, (a, b))
#-------------------------------------------------------------------------------
# RaisedCosine distribution ----------------------------------------------------
class RaisedCosineDistribution(SingleContinuousDistribution):
_argnames = ('mu', 's')
@property
def set(self):
return Interval(self.mu - self.s, self.mu + self.s)
@staticmethod
def check(mu, s):
_value_check(s > 0, "s must be positive")
def pdf(self, x):
mu, s = self.mu, self.s
return Piecewise(
((1+cos(pi*(x-mu)/s)) / (2*s), And(mu-s<=x, x<=mu+s)),
(S.Zero, True))
def _characteristic_function(self, t):
mu, s = self.mu, self.s
return Piecewise((exp(-I*pi*mu/s)/2, Eq(t, -pi/s)),
(exp(I*pi*mu/s)/2, Eq(t, pi/s)),
(pi**2*sin(s*t)*exp(I*mu*t) / (s*t*(pi**2 - s**2*t**2)), True))
def _moment_generating_function(self, t):
mu, s = self.mu, self.s
return pi**2 * sinh(s*t) * exp(mu*t) / (s*t*(pi**2 + s**2*t**2))
def RaisedCosine(name, mu, s):
r"""
Create a Continuous Random Variable with a raised cosine distribution.
The density of the raised cosine distribution is given by
.. math::
f(x) := \frac{1}{2s}\left(1+\cos\left(\frac{x-\mu}{s}\pi\right)\right)
with :math:`x \in [\mu-s,\mu+s]`.
Parameters
==========
mu : Real number
s : Real number, `s > 0`
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import RaisedCosine, density, E, variance
>>> from sympy import Symbol, simplify, pprint
>>> mu = Symbol("mu", real=True)
>>> s = Symbol("s", positive=True)
>>> z = Symbol("z")
>>> X = RaisedCosine("x", mu, s)
>>> D = density(X)(z)
>>> pprint(D, use_unicode=False)
/ /pi*(-mu + z)\
|cos|------------| + 1
| \ s /
<--------------------- for And(z >= mu - s, z <= mu + s)
| 2*s
|
\ 0 otherwise
References
==========
.. [1] https://en.wikipedia.org/wiki/Raised_cosine_distribution
"""
return rv(name, RaisedCosineDistribution, (mu, s))
#-------------------------------------------------------------------------------
# Rayleigh distribution --------------------------------------------------------
class RayleighDistribution(SingleContinuousDistribution):
_argnames = ('sigma',)
set = Interval(0, oo)
@staticmethod
def check(sigma):
_value_check(sigma > 0, "Scale parameter sigma must be positive.")
def pdf(self, x):
sigma = self.sigma
return x/sigma**2*exp(-x**2/(2*sigma**2))
def _cdf(self, x):
sigma = self.sigma
return 1 - exp(-(x**2/(2*sigma**2)))
def _characteristic_function(self, t):
sigma = self.sigma
return 1 - sigma*t*exp(-sigma**2*t**2/2) * sqrt(pi/2) * (erfi(sigma*t/sqrt(2)) - I)
def _moment_generating_function(self, t):
sigma = self.sigma
return 1 + sigma*t*exp(sigma**2*t**2/2) * sqrt(pi/2) * (erf(sigma*t/sqrt(2)) + 1)
def Rayleigh(name, sigma):
r"""
Create a continuous random variable with a Rayleigh distribution.
The density of the Rayleigh distribution is given by
.. math ::
f(x) := \frac{x}{\sigma^2} e^{-x^2/2\sigma^2}
with :math:`x > 0`.
Parameters
==========
sigma : Real number, `\sigma > 0`
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Rayleigh, density, E, variance
>>> from sympy import Symbol, simplify
>>> sigma = Symbol("sigma", positive=True)
>>> z = Symbol("z")
>>> X = Rayleigh("x", sigma)
>>> density(X)(z)
z*exp(-z**2/(2*sigma**2))/sigma**2
>>> E(X)
sqrt(2)*sqrt(pi)*sigma/2
>>> variance(X)
-pi*sigma**2/2 + 2*sigma**2
References
==========
.. [1] https://en.wikipedia.org/wiki/Rayleigh_distribution
.. [2] http://mathworld.wolfram.com/RayleighDistribution.html
"""
return rv(name, RayleighDistribution, (sigma, ))
#-------------------------------------------------------------------------------
# Shifted Gompertz distribution ------------------------------------------------
class ShiftedGompertzDistribution(SingleContinuousDistribution):
_argnames = ('b', 'eta')
set = Interval(0, oo)
@staticmethod
def check(b, eta):
_value_check(b > 0, "b must be positive")
_value_check(eta > 0, "eta must be positive")
def pdf(self, x):
b, eta = self.b, self.eta
return b*exp(-b*x)*exp(-eta*exp(-b*x))*(1+eta*(1-exp(-b*x)))
def ShiftedGompertz(name, b, eta):
r"""
Create a continuous random variable with a Shifted Gompertz distribution.
The density of the Shifted Gompertz distribution is given by
.. math::
f(x) := b e^{-b x} e^{-\eta \exp(-b x)} \left[1 + \eta(1 - e^(-bx)) \right]
with :math: 'x \in [0, \inf)'.
Parameters
==========
b: Real number, 'b > 0' a scale
eta: Real number, 'eta > 0' a shape
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import ShiftedGompertz, density, E, variance
>>> from sympy import Symbol
>>> b = Symbol("b", positive=True)
>>> eta = Symbol("eta", positive=True)
>>> x = Symbol("x")
>>> X = ShiftedGompertz("x", b, eta)
>>> density(X)(x)
b*(eta*(1 - exp(-b*x)) + 1)*exp(-b*x)*exp(-eta*exp(-b*x))
References
==========
.. [1] https://en.wikipedia.org/wiki/Shifted_Gompertz_distribution
"""
return rv(name, ShiftedGompertzDistribution, (b, eta))
#-------------------------------------------------------------------------------
# StudentT distribution --------------------------------------------------------
class StudentTDistribution(SingleContinuousDistribution):
_argnames = ('nu',)
set = Interval(-oo, oo)
@staticmethod
def check(nu):
_value_check(nu > 0, "Degrees of freedom nu must be positive.")
def pdf(self, x):
nu = self.nu
return 1/(sqrt(nu)*beta_fn(S.Half, nu/2))*(1 + x**2/nu)**(-(nu + 1)/2)
def _cdf(self, x):
nu = self.nu
return S.Half + x*gamma((nu+1)/2)*hyper((S.Half, (nu+1)/2),
(Rational(3, 2),), -x**2/nu)/(sqrt(pi*nu)*gamma(nu/2))
def _moment_generating_function(self, t):
raise NotImplementedError('The moment generating function for the Student-T distribution is undefined.')
def StudentT(name, nu):
r"""
Create a continuous random variable with a student's t distribution.
The density of the student's t distribution is given by
.. math::
f(x) := \frac{\Gamma \left(\frac{\nu+1}{2} \right)}
{\sqrt{\nu\pi}\Gamma \left(\frac{\nu}{2} \right)}
\left(1+\frac{x^2}{\nu} \right)^{-\frac{\nu+1}{2}}
Parameters
==========
nu : Real number, `\nu > 0`, the degrees of freedom
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import StudentT, density, E, variance, cdf
>>> from sympy import Symbol, simplify, pprint
>>> nu = Symbol("nu", positive=True)
>>> z = Symbol("z")
>>> X = StudentT("x", nu)
>>> D = density(X)(z)
>>> pprint(D, use_unicode=False)
nu 1
- -- - -
2 2
/ 2\
| z |
|1 + --|
\ nu/
-----------------
____ / nu\
\/ nu *B|1/2, --|
\ 2 /
>>> cdf(X)(z)
1/2 + z*gamma(nu/2 + 1/2)*hyper((1/2, nu/2 + 1/2), (3/2,),
-z**2/nu)/(sqrt(pi)*sqrt(nu)*gamma(nu/2))
References
==========
.. [1] https://en.wikipedia.org/wiki/Student_t-distribution
.. [2] http://mathworld.wolfram.com/Studentst-Distribution.html
"""
return rv(name, StudentTDistribution, (nu, ))
#-------------------------------------------------------------------------------
# Trapezoidal distribution ------------------------------------------------------
class TrapezoidalDistribution(SingleContinuousDistribution):
_argnames = ('a', 'b', 'c', 'd')
@property
def set(self):
return Interval(self.a, self.d)
@staticmethod
def check(a, b, c, d):
_value_check(a < d, "Lower bound parameter a < %s. a = %s"%(d, a))
_value_check((a <= b, b < c),
"Level start parameter b must be in range [%s, %s). b = %s"%(a, c, b))
_value_check((b < c, c <= d),
"Level end parameter c must be in range (%s, %s]. c = %s"%(b, d, c))
_value_check(d >= c, "Upper bound parameter d > %s. d = %s"%(c, d))
def pdf(self, x):
a, b, c, d = self.a, self.b, self.c, self.d
return Piecewise(
(2*(x-a) / ((b-a)*(d+c-a-b)), And(a <= x, x < b)),
(2 / (d+c-a-b), And(b <= x, x < c)),
(2*(d-x) / ((d-c)*(d+c-a-b)), And(c <= x, x <= d)),
(S.Zero, True))
def Trapezoidal(name, a, b, c, d):
r"""
Create a continuous random variable with a trapezoidal distribution.
The density of the trapezoidal distribution is given by
.. math::
f(x) := \begin{cases}
0 & \mathrm{for\ } x < a, \\
\frac{2(x-a)}{(b-a)(d+c-a-b)} & \mathrm{for\ } a \le x < b, \\
\frac{2}{d+c-a-b} & \mathrm{for\ } b \le x < c, \\
\frac{2(d-x)}{(d-c)(d+c-a-b)} & \mathrm{for\ } c \le x < d, \\
0 & \mathrm{for\ } d < x.
\end{cases}
Parameters
==========
a : Real number, :math:`a < d`
b : Real number, :math:`a <= b < c`
c : Real number, :math:`b < c <= d`
d : Real number
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Trapezoidal, density, E
>>> from sympy import Symbol, pprint
>>> a = Symbol("a")
>>> b = Symbol("b")
>>> c = Symbol("c")
>>> d = Symbol("d")
>>> z = Symbol("z")
>>> X = Trapezoidal("x", a,b,c,d)
>>> pprint(density(X)(z), use_unicode=False)
/ -2*a + 2*z
|------------------------- for And(a <= z, b > z)
|(-a + b)*(-a - b + c + d)
|
| 2
| -------------- for And(b <= z, c > z)
< -a - b + c + d
|
| 2*d - 2*z
|------------------------- for And(d >= z, c <= z)
|(-c + d)*(-a - b + c + d)
|
\ 0 otherwise
References
==========
.. [1] https://en.wikipedia.org/wiki/Trapezoidal_distribution
"""
return rv(name, TrapezoidalDistribution, (a, b, c, d))
#-------------------------------------------------------------------------------
# Triangular distribution ------------------------------------------------------
class TriangularDistribution(SingleContinuousDistribution):
_argnames = ('a', 'b', 'c')
@property
def set(self):
return Interval(self.a, self.b)
@staticmethod
def check(a, b, c):
_value_check(b > a, "Parameter b > %s. b = %s"%(a, b))
_value_check((a <= c, c <= b),
"Parameter c must be in range [%s, %s]. c = %s"%(a, b, c))
def pdf(self, x):
a, b, c = self.a, self.b, self.c
return Piecewise(
(2*(x - a)/((b - a)*(c - a)), And(a <= x, x < c)),
(2/(b - a), Eq(x, c)),
(2*(b - x)/((b - a)*(b - c)), And(c < x, x <= b)),
(S.Zero, True))
def _characteristic_function(self, t):
a, b, c = self.a, self.b, self.c
return -2 *((b-c) * exp(I*a*t) - (b-a) * exp(I*c*t) + (c-a) * exp(I*b*t)) / ((b-a)*(c-a)*(b-c)*t**2)
def _moment_generating_function(self, t):
a, b, c = self.a, self.b, self.c
return 2 * ((b - c) * exp(a * t) - (b - a) * exp(c * t) + (c - a) * exp(b * t)) / (
(b - a) * (c - a) * (b - c) * t ** 2)
def Triangular(name, a, b, c):
r"""
Create a continuous random variable with a triangular distribution.
The density of the triangular distribution is given by
.. math::
f(x) := \begin{cases}
0 & \mathrm{for\ } x < a, \\
\frac{2(x-a)}{(b-a)(c-a)} & \mathrm{for\ } a \le x < c, \\
\frac{2}{b-a} & \mathrm{for\ } x = c, \\
\frac{2(b-x)}{(b-a)(b-c)} & \mathrm{for\ } c < x \le b, \\
0 & \mathrm{for\ } b < x.
\end{cases}
Parameters
==========
a : Real number, :math:`a \in \left(-\infty, \infty\right)`
b : Real number, :math:`a < b`
c : Real number, :math:`a \leq c \leq b`
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Triangular, density, E
>>> from sympy import Symbol, pprint
>>> a = Symbol("a")
>>> b = Symbol("b")
>>> c = Symbol("c")
>>> z = Symbol("z")
>>> X = Triangular("x", a,b,c)
>>> pprint(density(X)(z), use_unicode=False)
/ -2*a + 2*z
|----------------- for And(a <= z, c > z)
|(-a + b)*(-a + c)
|
| 2
| ------ for c = z
< -a + b
|
| 2*b - 2*z
|---------------- for And(b >= z, c < z)
|(-a + b)*(b - c)
|
\ 0 otherwise
References
==========
.. [1] https://en.wikipedia.org/wiki/Triangular_distribution
.. [2] http://mathworld.wolfram.com/TriangularDistribution.html
"""
return rv(name, TriangularDistribution, (a, b, c))
#-------------------------------------------------------------------------------
# Uniform distribution ---------------------------------------------------------
class UniformDistribution(SingleContinuousDistribution):
_argnames = ('left', 'right')
@property
def set(self):
return Interval(self.left, self.right)
@staticmethod
def check(left, right):
_value_check(left < right, "Lower limit should be less than Upper limit.")
def pdf(self, x):
left, right = self.left, self.right
return Piecewise(
(S.One/(right - left), And(left <= x, x <= right)),
(S.Zero, True)
)
def _cdf(self, x):
left, right = self.left, self.right
return Piecewise(
(S.Zero, x < left),
((x - left)/(right - left), x <= right),
(S.One, True)
)
def _characteristic_function(self, t):
left, right = self.left, self.right
return Piecewise(((exp(I*t*right) - exp(I*t*left)) / (I*t*(right - left)), Ne(t, 0)),
(S.One, True))
def _moment_generating_function(self, t):
left, right = self.left, self.right
return Piecewise(((exp(t*right) - exp(t*left)) / (t * (right - left)), Ne(t, 0)),
(S.One, True))
def expectation(self, expr, var, **kwargs):
from sympy import Max, Min
kwargs['evaluate'] = True
result = SingleContinuousDistribution.expectation(self, expr, var, **kwargs)
result = result.subs({Max(self.left, self.right): self.right,
Min(self.left, self.right): self.left})
return result
def sample(self):
return random.uniform(self.left, self.right)
def Uniform(name, left, right):
r"""
Create a continuous random variable with a uniform distribution.
The density of the uniform distribution is given by
.. math::
f(x) := \begin{cases}
\frac{1}{b - a} & \text{for } x \in [a,b] \\
0 & \text{otherwise}
\end{cases}
with :math:`x \in [a,b]`.
Parameters
==========
a : Real number, :math:`-\infty < a` the left boundary
b : Real number, :math:`a < b < \infty` the right boundary
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Uniform, density, cdf, E, variance, skewness
>>> from sympy import Symbol, simplify
>>> a = Symbol("a", negative=True)
>>> b = Symbol("b", positive=True)
>>> z = Symbol("z")
>>> X = Uniform("x", a, b)
>>> density(X)(z)
Piecewise((1/(-a + b), (b >= z) & (a <= z)), (0, True))
>>> cdf(X)(z)
Piecewise((0, a > z), ((-a + z)/(-a + b), b >= z), (1, True))
>>> E(X)
a/2 + b/2
>>> simplify(variance(X))
a**2/12 - a*b/6 + b**2/12
References
==========
.. [1] https://en.wikipedia.org/wiki/Uniform_distribution_%28continuous%29
.. [2] http://mathworld.wolfram.com/UniformDistribution.html
"""
return rv(name, UniformDistribution, (left, right))
#-------------------------------------------------------------------------------
# UniformSum distribution ------------------------------------------------------
class UniformSumDistribution(SingleContinuousDistribution):
_argnames = ('n',)
@property
def set(self):
return Interval(0, self.n)
@staticmethod
def check(n):
_value_check((n > 0, n.is_integer),
"Parameter n must be positive integer.")
def pdf(self, x):
n = self.n
k = Dummy("k")
return 1/factorial(
n - 1)*Sum((-1)**k*binomial(n, k)*(x - k)**(n - 1), (k, 0, floor(x)))
def _cdf(self, x):
n = self.n
k = Dummy("k")
return Piecewise((S.Zero, x < 0),
(1/factorial(n)*Sum((-1)**k*binomial(n, k)*(x - k)**(n),
(k, 0, floor(x))), x <= n),
(S.One, True))
def _characteristic_function(self, t):
return ((exp(I*t) - 1) / (I*t))**self.n
def _moment_generating_function(self, t):
return ((exp(t) - 1) / t)**self.n
def UniformSum(name, n):
r"""
Create a continuous random variable with an Irwin-Hall distribution.
The probability distribution function depends on a single parameter
`n` which is an integer.
The density of the Irwin-Hall distribution is given by
.. math ::
f(x) := \frac{1}{(n-1)!}\sum_{k=0}^{\left\lfloor x\right\rfloor}(-1)^k
\binom{n}{k}(x-k)^{n-1}
Parameters
==========
n : A positive Integer, `n > 0`
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import UniformSum, density, cdf
>>> from sympy import Symbol, pprint
>>> n = Symbol("n", integer=True)
>>> z = Symbol("z")
>>> X = UniformSum("x", n)
>>> D = density(X)(z)
>>> pprint(D, use_unicode=False)
floor(z)
___
\ `
\ k n - 1 /n\
) (-1) *(-k + z) *| |
/ \k/
/__,
k = 0
--------------------------------
(n - 1)!
>>> cdf(X)(z)
Piecewise((0, z < 0), (Sum((-1)**_k*(-_k + z)**n*binomial(n, _k),
(_k, 0, floor(z)))/factorial(n), n >= z), (1, True))
Compute cdf with specific 'x' and 'n' values as follows :
>>> cdf(UniformSum("x", 5), evaluate=False)(2).doit()
9/40
The argument evaluate=False prevents an attempt at evaluation
of the sum for general n, before the argument 2 is passed.
References
==========
.. [1] https://en.wikipedia.org/wiki/Uniform_sum_distribution
.. [2] http://mathworld.wolfram.com/UniformSumDistribution.html
"""
return rv(name, UniformSumDistribution, (n, ))
#-------------------------------------------------------------------------------
# VonMises distribution --------------------------------------------------------
class VonMisesDistribution(SingleContinuousDistribution):
_argnames = ('mu', 'k')
set = Interval(0, 2*pi)
@staticmethod
def check(mu, k):
_value_check(k > 0, "k must be positive")
def pdf(self, x):
mu, k = self.mu, self.k
return exp(k*cos(x-mu)) / (2*pi*besseli(0, k))
def VonMises(name, mu, k):
r"""
Create a Continuous Random Variable with a von Mises distribution.
The density of the von Mises distribution is given by
.. math::
f(x) := \frac{e^{\kappa\cos(x-\mu)}}{2\pi I_0(\kappa)}
with :math:`x \in [0,2\pi]`.
Parameters
==========
mu : Real number, measure of location
k : Real number, measure of concentration
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import VonMises, density, E, variance
>>> from sympy import Symbol, simplify, pprint
>>> mu = Symbol("mu")
>>> k = Symbol("k", positive=True)
>>> z = Symbol("z")
>>> X = VonMises("x", mu, k)
>>> D = density(X)(z)
>>> pprint(D, use_unicode=False)
k*cos(mu - z)
e
------------------
2*pi*besseli(0, k)
References
==========
.. [1] https://en.wikipedia.org/wiki/Von_Mises_distribution
.. [2] http://mathworld.wolfram.com/vonMisesDistribution.html
"""
return rv(name, VonMisesDistribution, (mu, k))
#-------------------------------------------------------------------------------
# Weibull distribution ---------------------------------------------------------
class WeibullDistribution(SingleContinuousDistribution):
_argnames = ('alpha', 'beta')
set = Interval(0, oo)
@staticmethod
def check(alpha, beta):
_value_check(alpha > 0, "Alpha must be positive")
_value_check(beta > 0, "Beta must be positive")
def pdf(self, x):
alpha, beta = self.alpha, self.beta
return beta * (x/alpha)**(beta - 1) * exp(-(x/alpha)**beta) / alpha
def sample(self):
return random.weibullvariate(self.alpha, self.beta)
def Weibull(name, alpha, beta):
r"""
Create a continuous random variable with a Weibull distribution.
The density of the Weibull distribution is given by
.. math::
f(x) := \begin{cases}
\frac{k}{\lambda}\left(\frac{x}{\lambda}\right)^{k-1}
e^{-(x/\lambda)^{k}} & x\geq0\\
0 & x<0
\end{cases}
Parameters
==========
lambda : Real number, :math:`\lambda > 0` a scale
k : Real number, `k > 0` a shape
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import Weibull, density, E, variance
>>> from sympy import Symbol, simplify
>>> l = Symbol("lambda", positive=True)
>>> k = Symbol("k", positive=True)
>>> z = Symbol("z")
>>> X = Weibull("x", l, k)
>>> density(X)(z)
k*(z/lambda)**(k - 1)*exp(-(z/lambda)**k)/lambda
>>> simplify(E(X))
lambda*gamma(1 + 1/k)
>>> simplify(variance(X))
lambda**2*(-gamma(1 + 1/k)**2 + gamma(1 + 2/k))
References
==========
.. [1] https://en.wikipedia.org/wiki/Weibull_distribution
.. [2] http://mathworld.wolfram.com/WeibullDistribution.html
"""
return rv(name, WeibullDistribution, (alpha, beta))
#-------------------------------------------------------------------------------
# Wigner semicircle distribution -----------------------------------------------
class WignerSemicircleDistribution(SingleContinuousDistribution):
_argnames = ('R',)
@property
def set(self):
return Interval(-self.R, self.R)
@staticmethod
def check(R):
_value_check(R > 0, "Radius R must be positive.")
def pdf(self, x):
R = self.R
return 2/(pi*R**2)*sqrt(R**2 - x**2)
def _characteristic_function(self, t):
return Piecewise((2 * besselj(1, self.R*t) / (self.R*t), Ne(t, 0)),
(S.One, True))
def _moment_generating_function(self, t):
return Piecewise((2 * besseli(1, self.R*t) / (self.R*t), Ne(t, 0)),
(S.One, True))
def WignerSemicircle(name, R):
r"""
Create a continuous random variable with a Wigner semicircle distribution.
The density of the Wigner semicircle distribution is given by
.. math::
f(x) := \frac2{\pi R^2}\,\sqrt{R^2-x^2}
with :math:`x \in [-R,R]`.
Parameters
==========
R : Real number, `R > 0`, the radius
Returns
=======
A `RandomSymbol`.
Examples
========
>>> from sympy.stats import WignerSemicircle, density, E
>>> from sympy import Symbol, simplify
>>> R = Symbol("R", positive=True)
>>> z = Symbol("z")
>>> X = WignerSemicircle("x", R)
>>> density(X)(z)
2*sqrt(R**2 - z**2)/(pi*R**2)
>>> E(X)
0
References
==========
.. [1] https://en.wikipedia.org/wiki/Wigner_semicircle_distribution
.. [2] http://mathworld.wolfram.com/WignersSemicircleLaw.html
"""
return rv(name, WignerSemicircleDistribution, (R,))
|
89cc9ca1e42cacd7f2ae85c480085e1b9c882569715d69f353adbd528f47cff9 | """
Finite Discrete Random Variables - Prebuilt variable types
Contains
========
FiniteRV
DiscreteUniform
Die
Bernoulli
Coin
Binomial
BetaBinomial
Hypergeometric
Rademacher
"""
from __future__ import print_function, division
import random
from sympy import (S, sympify, Rational, binomial, cacheit, Integer,
Dummy, Eq, Intersection, Interval,
Symbol, Lambda, Piecewise, Or, Gt, Lt, Ge, Le, Contains)
from sympy import beta as beta_fn
from sympy.external import import_module
from sympy.core.compatibility import range
from sympy.tensor.array import ArrayComprehensionMap
from sympy.stats.frv import (SingleFiniteDistribution,
SingleFinitePSpace)
from sympy.stats.rv import _value_check, Density, RandomSymbol
numpy = import_module('numpy')
scipy = import_module('scipy')
pymc3 = import_module('pymc3')
__all__ = ['FiniteRV',
'DiscreteUniform',
'Die',
'Bernoulli',
'Coin',
'Binomial',
'BetaBinomial',
'Hypergeometric',
'Rademacher'
]
def rv(name, cls, *args):
args = list(map(sympify, args))
dist = cls(*args)
dist.check(*args)
return SingleFinitePSpace(name, dist).value
class FiniteDistributionHandmade(SingleFiniteDistribution):
@property
def dict(self):
return self.args[0]
def pmf(self, x):
x = Symbol('x')
return Lambda(x, Piecewise(*(
[(v, Eq(k, x)) for k, v in self.dict.items()] + [(S.Zero, True)])))
@property
def set(self):
return set(self.dict.keys())
@staticmethod
def check(density):
for p in density.values():
_value_check((p >= 0, p <= 1),
"Probability at a point must be between 0 and 1.")
_value_check(Eq(sum(density.values()), 1), "Total Probability must be 1.")
def FiniteRV(name, density):
"""
Create a Finite Random Variable given a dict representing the density.
Returns a RandomSymbol.
>>> from sympy.stats import FiniteRV, P, E
>>> density = {0: .1, 1: .2, 2: .3, 3: .4}
>>> X = FiniteRV('X', density)
>>> E(X)
2.00000000000000
>>> P(X >= 2)
0.700000000000000
"""
return rv(name, FiniteDistributionHandmade, density)
class DiscreteUniformDistribution(SingleFiniteDistribution):
@property
def p(self):
return Rational(1, len(self.args))
@property
@cacheit
def dict(self):
return dict((k, self.p) for k in self.set)
@property
def set(self):
return set(self.args)
def pmf(self, x):
if x in self.args:
return self.p
else:
return S.Zero
def _sample_random(self, size):
x = Symbol('x')
return ArrayComprehensionMap(lambda: self.args[random.randint(0, len(self.args)-1)], (x, 0, size)).doit()
def DiscreteUniform(name, items):
"""
Create a Finite Random Variable representing a uniform distribution over
the input set.
Returns a RandomSymbol.
Examples
========
>>> from sympy.stats import DiscreteUniform, density
>>> from sympy import symbols
>>> X = DiscreteUniform('X', symbols('a b c')) # equally likely over a, b, c
>>> density(X).dict
{a: 1/3, b: 1/3, c: 1/3}
>>> Y = DiscreteUniform('Y', list(range(5))) # distribution over a range
>>> density(Y).dict
{0: 1/5, 1: 1/5, 2: 1/5, 3: 1/5, 4: 1/5}
References
==========
.. [1] https://en.wikipedia.org/wiki/Discrete_uniform_distribution
.. [2] http://mathworld.wolfram.com/DiscreteUniformDistribution.html
"""
return rv(name, DiscreteUniformDistribution, *items)
class DieDistribution(SingleFiniteDistribution):
_argnames = ('sides',)
@staticmethod
def check(sides):
_value_check((sides.is_positive, sides.is_integer),
"number of sides must be a positive integer.")
@property
def is_symbolic(self):
return not self.sides.is_number
@property
def high(self):
return self.sides
@property
def low(self):
return S.One
@property
def set(self):
if self.is_symbolic:
return Intersection(S.Naturals0, Interval(0, self.sides))
return set(map(Integer, list(range(1, self.sides + 1))))
def pmf(self, x):
x = sympify(x)
if not (x.is_number or x.is_Symbol or isinstance(x, RandomSymbol)):
raise ValueError("'x' expected as an argument of type 'number' or 'Symbol' or , "
"'RandomSymbol' not %s" % (type(x)))
cond = Ge(x, 1) & Le(x, self.sides) & Contains(x, S.Integers)
return Piecewise((S.One/self.sides, cond), (S.Zero, True))
def Die(name, sides=6):
"""
Create a Finite Random Variable representing a fair die.
Returns a RandomSymbol.
Examples
========
>>> from sympy.stats import Die, density
>>> from sympy import Symbol
>>> D6 = Die('D6', 6) # Six sided Die
>>> density(D6).dict
{1: 1/6, 2: 1/6, 3: 1/6, 4: 1/6, 5: 1/6, 6: 1/6}
>>> D4 = Die('D4', 4) # Four sided Die
>>> density(D4).dict
{1: 1/4, 2: 1/4, 3: 1/4, 4: 1/4}
>>> n = Symbol('n', positive=True, integer=True)
>>> Dn = Die('Dn', n) # n sided Die
>>> density(Dn).dict
Density(DieDistribution(n))
>>> density(Dn).dict.subs(n, 4).doit()
{1: 1/4, 2: 1/4, 3: 1/4, 4: 1/4}
"""
return rv(name, DieDistribution, sides)
class BernoulliDistribution(SingleFiniteDistribution):
_argnames = ('p', 'succ', 'fail')
@staticmethod
def check(p, succ, fail):
_value_check((p >= 0, p <= 1),
"p should be in range [0, 1].")
@property
def set(self):
return set([self.succ, self.fail])
def pmf(self, x):
return Piecewise((self.p, x == self.succ),
(1 - self.p, x == self.fail),
(S.Zero, True))
def Bernoulli(name, p, succ=1, fail=0):
"""
Create a Finite Random Variable representing a Bernoulli process.
Returns a RandomSymbol
Examples
========
>>> from sympy.stats import Bernoulli, density
>>> from sympy import S
>>> X = Bernoulli('X', S(3)/4) # 1-0 Bernoulli variable, probability = 3/4
>>> density(X).dict
{0: 1/4, 1: 3/4}
>>> X = Bernoulli('X', S.Half, 'Heads', 'Tails') # A fair coin toss
>>> density(X).dict
{Heads: 1/2, Tails: 1/2}
References
==========
.. [1] https://en.wikipedia.org/wiki/Bernoulli_distribution
.. [2] http://mathworld.wolfram.com/BernoulliDistribution.html
"""
return rv(name, BernoulliDistribution, p, succ, fail)
def Coin(name, p=S.Half):
"""
Create a Finite Random Variable representing a Coin toss.
Probability p is the chance of gettings "Heads." Half by default
Returns a RandomSymbol.
Examples
========
>>> from sympy.stats import Coin, density
>>> from sympy import Rational
>>> C = Coin('C') # A fair coin toss
>>> density(C).dict
{H: 1/2, T: 1/2}
>>> C2 = Coin('C2', Rational(3, 5)) # An unfair coin
>>> density(C2).dict
{H: 3/5, T: 2/5}
See Also
========
sympy.stats.Binomial
References
==========
.. [1] https://en.wikipedia.org/wiki/Coin_flipping
"""
return rv(name, BernoulliDistribution, p, 'H', 'T')
class BinomialDistribution(SingleFiniteDistribution):
_argnames = ('n', 'p', 'succ', 'fail')
@staticmethod
def check(n, p, succ, fail):
_value_check((n.is_integer, n.is_nonnegative),
"'n' must be nonnegative integer.")
_value_check((p <= 1, p >= 0),
"p should be in range [0, 1].")
@property
def high(self):
return self.n
@property
def low(self):
return S.Zero
@property
def is_symbolic(self):
return not self.n.is_number
@property
def set(self):
if self.is_symbolic:
return Intersection(S.Naturals0, Interval(0, self.n))
return set(self.dict.keys())
def pmf(self, x):
n, p = self.n, self.p
x = sympify(x)
if not (x.is_number or x.is_Symbol or isinstance(x, RandomSymbol)):
raise ValueError("'x' expected as an argument of type 'number' or 'Symbol' or , "
"'RandomSymbol' not %s" % (type(x)))
cond = Ge(x, 0) & Le(x, n) & Contains(x, S.Integers)
return Piecewise((binomial(n, x) * p**x * (1 - p)**(n - x), cond), (S.Zero, True))
@property
@cacheit
def dict(self):
if self.is_symbolic:
return Density(self)
return dict((k*self.succ + (self.n-k)*self.fail, self.pmf(k))
for k in range(0, self.n + 1))
def Binomial(name, n, p, succ=1, fail=0):
"""
Create a Finite Random Variable representing a binomial distribution.
Returns a RandomSymbol.
Examples
========
>>> from sympy.stats import Binomial, density
>>> from sympy import S, Symbol
>>> X = Binomial('X', 4, S.Half) # Four "coin flips"
>>> density(X).dict
{0: 1/16, 1: 1/4, 2: 3/8, 3: 1/4, 4: 1/16}
>>> n = Symbol('n', positive=True, integer=True)
>>> p = Symbol('p', positive=True)
>>> X = Binomial('X', n, S.Half) # n "coin flips"
>>> density(X).dict
Density(BinomialDistribution(n, 1/2, 1, 0))
>>> density(X).dict.subs(n, 4).doit()
{0: 1/16, 1: 1/4, 2: 3/8, 3: 1/4, 4: 1/16}
References
==========
.. [1] https://en.wikipedia.org/wiki/Binomial_distribution
.. [2] http://mathworld.wolfram.com/BinomialDistribution.html
"""
return rv(name, BinomialDistribution, n, p, succ, fail)
#-------------------------------------------------------------------------------
# Beta-binomial distribution ----------------------------------------------------------
class BetaBinomialDistribution(SingleFiniteDistribution):
_argnames = ('n', 'alpha', 'beta')
@staticmethod
def check(n, alpha, beta):
_value_check((n.is_integer, n.is_nonnegative),
"'n' must be nonnegative integer. n = %s." % str(n))
_value_check((alpha > 0),
"'alpha' must be: alpha > 0 . alpha = %s" % str(alpha))
_value_check((beta > 0),
"'beta' must be: beta > 0 . beta = %s" % str(beta))
@property
def high(self):
return self.n
@property
def low(self):
return S.Zero
@property
def is_symbolic(self):
return not self.n.is_number
@property
def set(self):
if self.is_symbolic:
return Intersection(S.Naturals0, Interval(0, self.n))
return set(map(Integer, list(range(0, self.n + 1))))
def pmf(self, k):
n, a, b = self.n, self.alpha, self.beta
return binomial(n, k) * beta_fn(k + a, n - k + b) / beta_fn(a, b)
def _sample_pymc3(self, size):
n, a, b = int(self.n), float(self.alpha), float(self.beta)
with pymc3.Model():
pymc3.BetaBinomial('X', alpha=a, beta=b, n=n)
return pymc3.sample(size, chains=1, progressbar=False)[:]['X']
def BetaBinomial(name, n, alpha, beta):
"""
Create a Finite Random Variable representing a Beta-binomial distribution.
Returns a RandomSymbol.
Examples
========
>>> from sympy.stats import BetaBinomial, density
>>> from sympy import S
>>> X = BetaBinomial('X', 2, 1, 1)
>>> density(X).dict
{0: beta(1, 3)/beta(1, 1), 1: 2*beta(2, 2)/beta(1, 1), 2: beta(3, 1)/beta(1, 1)}
References
==========
.. [1] https://en.wikipedia.org/wiki/Beta-binomial_distribution
.. [2] http://mathworld.wolfram.com/BetaBinomialDistribution.html
"""
return rv(name, BetaBinomialDistribution, n, alpha, beta)
class HypergeometricDistribution(SingleFiniteDistribution):
_argnames = ('N', 'm', 'n')
@staticmethod
def check(n, N, m):
_value_check((N.is_integer, N.is_nonnegative),
"'N' must be nonnegative integer. N = %s." % str(n))
_value_check((n.is_integer, n.is_nonnegative),
"'n' must be nonnegative integer. n = %s." % str(n))
_value_check((m.is_integer, m.is_nonnegative),
"'m' must be nonnegative integer. m = %s." % str(n))
@property
def is_symbolic(self):
return any(not x.is_number for x in (self.N, self.m, self.n))
@property
def high(self):
return Piecewise((self.n, Lt(self.n, self.m) != False), (self.m, True))
@property
def low(self):
return Piecewise((0, Gt(0, self.n + self.m - self.N) != False), (self.n + self.m - self.N, True))
@property
def set(self):
N, m, n = self.N, self.m, self.n
if self.is_symbolic:
return Intersection(S.Naturals0, Interval(self.low, self.high))
return set([i for i in range(max(0, n + m - N), min(n, m) + 1)])
def pmf(self, k):
N, m, n = self.N, self.m, self.n
return S(binomial(m, k) * binomial(N - m, n - k))/binomial(N, n)
def _sample_scipy(self, size):
N, m, n = int(self.N), int(self.m), int(self.n)
return scipy.stats.hypergeom.rvs(M=m, n=n, N=N, size=size)
def Hypergeometric(name, N, m, n):
"""
Create a Finite Random Variable representing a hypergeometric distribution.
Returns a RandomSymbol.
Examples
========
>>> from sympy.stats import Hypergeometric, density
>>> from sympy import S
>>> X = Hypergeometric('X', 10, 5, 3) # 10 marbles, 5 white (success), 3 draws
>>> density(X).dict
{0: 1/12, 1: 5/12, 2: 5/12, 3: 1/12}
References
==========
.. [1] https://en.wikipedia.org/wiki/Hypergeometric_distribution
.. [2] http://mathworld.wolfram.com/HypergeometricDistribution.html
"""
return rv(name, HypergeometricDistribution, N, m, n)
class RademacherDistribution(SingleFiniteDistribution):
@property
def set(self):
return set([-1, 1])
@property
def pmf(self):
k = Dummy('k')
return Lambda(k, Piecewise((S.Half, Or(Eq(k, -1), Eq(k, 1))), (S.Zero, True)))
def Rademacher(name):
"""
Create a Finite Random Variable representing a Rademacher distribution.
Return a RandomSymbol.
Examples
========
>>> from sympy.stats import Rademacher, density
>>> X = Rademacher('X')
>>> density(X).dict
{-1: 1/2, 1: 1/2}
See Also
========
sympy.stats.Bernoulli
References
==========
.. [1] https://en.wikipedia.org/wiki/Rademacher_distribution
"""
return rv(name, RademacherDistribution)
|
f1134a6a1524183ef1b81f2f7083a2bf7547d58addf5f321fdae57543f8b72ac | from __future__ import print_function, division
from sympy import (Matrix, MatrixSymbol, S, Indexed, Basic,
Set, And, Eq, FiniteSet, ImmutableMatrix,
Lambda, Mul, Dummy, IndexedBase,
linsolve, eye, Or, Not, Intersection,
Union, Expr, Function, exp, cacheit,
Ge)
from sympy.core.relational import Relational
from sympy.logic.boolalg import Boolean
from sympy.stats.joint_rv import JointDistributionHandmade, JointDistribution
from sympy.stats.rv import (RandomIndexedSymbol, random_symbols, RandomSymbol,
_symbol_converter)
from sympy.stats.stochastic_process import StochasticPSpace
from sympy.stats.symbolic_probability import Probability, Expectation
__all__ = [
'StochasticProcess',
'DiscreteTimeStochasticProcess',
'DiscreteMarkovChain',
'TransitionMatrixOf',
'StochasticStateSpaceOf',
'GeneratorMatrixOf',
'ContinuousMarkovChain'
]
def _set_converter(itr):
"""
Helper function for converting list/tuple/set to Set.
If parameter is not an instance of list/tuple/set then
no operation is performed.
Returns
=======
Set
The argument converted to Set.
Raises
======
TypeError
If the argument is not an instance of list/tuple/set.
"""
if isinstance(itr, (list, tuple, set)):
itr = FiniteSet(*itr)
if not isinstance(itr, Set):
raise TypeError("%s is not an instance of list/tuple/set."%(itr))
return itr
def _matrix_checks(matrix):
if not isinstance(matrix, (Matrix, MatrixSymbol, ImmutableMatrix)):
raise TypeError("Transition probabilities either should "
"be a Matrix or a MatrixSymbol.")
if matrix.shape[0] != matrix.shape[1]:
raise ValueError("%s is not a square matrix"%(matrix))
if isinstance(matrix, Matrix):
matrix = ImmutableMatrix(matrix.tolist())
return matrix
class StochasticProcess(Basic):
"""
Base class for all the stochastic processes whether
discrete or continuous.
Parameters
==========
sym: Symbol or string_types
state_space: Set
The state space of the stochastic process, by default S.Reals.
For discrete sets it is zero indexed.
See Also
========
DiscreteTimeStochasticProcess
"""
index_set = S.Reals
def __new__(cls, sym, state_space=S.Reals, **kwargs):
sym = _symbol_converter(sym)
state_space = _set_converter(state_space)
return Basic.__new__(cls, sym, state_space)
@property
def symbol(self):
return self.args[0]
@property
def state_space(self):
return self.args[1]
def __call__(self, time):
"""
Overridden in ContinuousTimeStochasticProcess.
"""
raise NotImplementedError("Use [] for indexing discrete time stochastic process.")
def __getitem__(self, time):
"""
Overridden in DiscreteTimeStochasticProcess.
"""
raise NotImplementedError("Use () for indexing continuous time stochastic process.")
def probability(self, condition):
raise NotImplementedError()
def joint_distribution(self, *args):
"""
Computes the joint distribution of the random indexed variables.
Parameters
==========
args: iterable
The finite list of random indexed variables/the key of a stochastic
process whose joint distribution has to be computed.
Returns
=======
JointDistribution
The joint distribution of the list of random indexed variables.
An unevaluated object is returned if it is not possible to
compute the joint distribution.
Raises
======
ValueError: When the arguments passed are not of type RandomIndexSymbol
or Number.
"""
args = list(args)
for i, arg in enumerate(args):
if S(arg).is_Number:
if self.index_set.is_subset(S.Integers):
args[i] = self.__getitem__(arg)
else:
args[i] = self.__call__(arg)
elif not isinstance(arg, RandomIndexedSymbol):
raise ValueError("Expected a RandomIndexedSymbol or "
"key not %s"%(type(arg)))
if args[0].pspace.distribution == None: # checks if there is any distribution available
return JointDistribution(*args)
# TODO: Add tests for the below part of the method, when implementation of Bernoulli Process
# is completed
pdf = Lambda(*[arg.name for arg in args],
expr=Mul.fromiter(arg.pspace.distribution.pdf(arg) for arg in args))
return JointDistributionHandmade(pdf)
def expectation(self, condition, given_condition):
raise NotImplementedError("Abstract method for expectation queries.")
class DiscreteTimeStochasticProcess(StochasticProcess):
"""
Base class for all discrete stochastic processes.
"""
def __getitem__(self, time):
"""
For indexing discrete time stochastic processes.
Returns
=======
RandomIndexedSymbol
"""
if time not in self.index_set:
raise IndexError("%s is not in the index set of %s"%(time, self.symbol))
idx_obj = Indexed(self.symbol, time)
pspace_obj = StochasticPSpace(self.symbol, self)
return RandomIndexedSymbol(idx_obj, pspace_obj)
class ContinuousTimeStochasticProcess(StochasticProcess):
"""
Base class for all continuous time stochastic process.
"""
def __call__(self, time):
"""
For indexing continuous time stochastic processes.
Returns
=======
RandomIndexedSymbol
"""
if time not in self.index_set:
raise IndexError("%s is not in the index set of %s"%(time, self.symbol))
func_obj = Function(self.symbol)(time)
pspace_obj = StochasticPSpace(self.symbol, self)
return RandomIndexedSymbol(func_obj, pspace_obj)
class TransitionMatrixOf(Boolean):
"""
Assumes that the matrix is the transition matrix
of the process.
"""
def __new__(cls, process, matrix):
if not isinstance(process, DiscreteMarkovChain):
raise ValueError("Currently only DiscreteMarkovChain "
"support TransitionMatrixOf.")
matrix = _matrix_checks(matrix)
return Basic.__new__(cls, process, matrix)
process = property(lambda self: self.args[0])
matrix = property(lambda self: self.args[1])
class GeneratorMatrixOf(TransitionMatrixOf):
"""
Assumes that the matrix is the generator matrix
of the process.
"""
def __new__(cls, process, matrix):
if not isinstance(process, ContinuousMarkovChain):
raise ValueError("Currently only ContinuousMarkovChain "
"support GeneratorMatrixOf.")
matrix = _matrix_checks(matrix)
return Basic.__new__(cls, process, matrix)
class StochasticStateSpaceOf(Boolean):
def __new__(cls, process, state_space):
if not isinstance(process, (DiscreteMarkovChain, ContinuousMarkovChain)):
raise ValueError("Currently only DiscreteMarkovChain and ContinuousMarkovChain "
"support StochasticStateSpaceOf.")
state_space = _set_converter(state_space)
return Basic.__new__(cls, process, state_space)
process = property(lambda self: self.args[0])
state_space = property(lambda self: self.args[1])
class MarkovProcess(StochasticProcess):
"""
Contains methods that handle queries
common to Markov processes.
"""
def _extract_information(self, given_condition):
"""
Helper function to extract information, like,
transition matrix/generator matrix, state space, etc.
"""
if isinstance(self, DiscreteMarkovChain):
trans_probs = self.transition_probabilities
elif isinstance(self, ContinuousMarkovChain):
trans_probs = self.generator_matrix
state_space = self.state_space
if isinstance(given_condition, And):
gcs = given_condition.args
given_condition = S.true
for gc in gcs:
if isinstance(gc, TransitionMatrixOf):
trans_probs = gc.matrix
if isinstance(gc, StochasticStateSpaceOf):
state_space = gc.state_space
if isinstance(gc, Relational):
given_condition = given_condition & gc
if isinstance(given_condition, TransitionMatrixOf):
trans_probs = given_condition.matrix
given_condition = S.true
if isinstance(given_condition, StochasticStateSpaceOf):
state_space = given_condition.state_space
given_condition = S.true
return trans_probs, state_space, given_condition
def _check_trans_probs(self, trans_probs, row_sum=1):
"""
Helper function for checking the validity of transition
probabilities.
"""
if not isinstance(trans_probs, MatrixSymbol):
rows = trans_probs.tolist()
for row in rows:
if (sum(row) - row_sum) != 0:
raise ValueError("Values in a row must sum to %s. "
"If you are using Float or floats then please use Rational."%(row_sum))
def _work_out_state_space(self, state_space, given_condition, trans_probs):
"""
Helper function to extract state space if there
is a random symbol in the given condition.
"""
# if given condition is None, then there is no need to work out
# state_space from random variables
if given_condition != None:
rand_var = list(given_condition.atoms(RandomSymbol) -
given_condition.atoms(RandomIndexedSymbol))
if len(rand_var) == 1:
state_space = rand_var[0].pspace.set
if not FiniteSet(*[i for i in range(trans_probs.shape[0])]).is_subset(state_space):
raise ValueError("state space is not compatible with the transition probabilites.")
state_space = FiniteSet(*[i for i in range(trans_probs.shape[0])])
return state_space
@cacheit
def _preprocess(self, given_condition, evaluate):
"""
Helper function for pre-processing the information.
"""
is_insufficient = False
if not evaluate: # avoid pre-processing if the result is not to be evaluated
return (True, None, None, None)
# extracting transition matrix and state space
trans_probs, state_space, given_condition = self._extract_information(given_condition)
# given_condition does not have sufficient information
# for computations
if trans_probs == None or \
given_condition == None:
is_insufficient = True
else:
# checking transition probabilities
if isinstance(self, DiscreteMarkovChain):
self._check_trans_probs(trans_probs, row_sum=1)
elif isinstance(self, ContinuousMarkovChain):
self._check_trans_probs(trans_probs, row_sum=0)
# working out state space
state_space = self._work_out_state_space(state_space, given_condition, trans_probs)
return is_insufficient, trans_probs, state_space, given_condition
def probability(self, condition, given_condition=None, evaluate=True, **kwargs):
"""
Handles probability queries for Markov process.
Parameters
==========
condition: Relational
given_condition: Relational/And
Returns
=======
Probability
If the information is not sufficient.
Expr
In all other cases.
Note
====
Any information passed at the time of query overrides
any information passed at the time of object creation like
transition probabilities, state space.
Pass the transition matrix using TransitionMatrixOf,
generator matrix using GeneratorMatrixOf and state space
using StochasticStateSpaceOf in given_condition using & or And.
"""
check, mat, state_space, new_given_condition = \
self._preprocess(given_condition, evaluate)
if check:
return Probability(condition, new_given_condition)
if isinstance(self, ContinuousMarkovChain):
trans_probs = self.transition_probabilities(mat)
elif isinstance(self, DiscreteMarkovChain):
trans_probs = mat
if isinstance(condition, Relational):
rv, states = (list(condition.atoms(RandomIndexedSymbol))[0], condition.as_set())
if isinstance(new_given_condition, And):
gcs = new_given_condition.args
else:
gcs = (new_given_condition, )
grvs = new_given_condition.atoms(RandomIndexedSymbol)
min_key_rv = None
for grv in grvs:
if grv.key <= rv.key:
min_key_rv = grv
if min_key_rv == None:
return Probability(condition)
prob, gstate = dict(), None
for gc in gcs:
if gc.has(min_key_rv):
if gc.has(Probability):
p, gp = (gc.rhs, gc.lhs) if isinstance(gc.lhs, Probability) \
else (gc.lhs, gc.rhs)
gr = gp.args[0]
gset = Intersection(gr.as_set(), state_space)
gstate = list(gset)[0]
prob[gset] = p
else:
_, gstate = (gc.lhs.key, gc.rhs) if isinstance(gc.lhs, RandomIndexedSymbol) \
else (gc.rhs.key, gc.lhs)
if any((k not in self.index_set) for k in (rv.key, min_key_rv.key)):
raise IndexError("The timestamps of the process are not in it's index set.")
states = Intersection(states, state_space)
for state in Union(states, FiniteSet(gstate)):
if Ge(state, mat.shape[0]) == True:
raise IndexError("No information is available for (%s, %s) in "
"transition probabilities of shape, (%s, %s). "
"State space is zero indexed."
%(gstate, state, mat.shape[0], mat.shape[1]))
if prob:
gstates = Union(*prob.keys())
if len(gstates) == 1:
gstate = list(gstates)[0]
gprob = list(prob.values())[0]
prob[gstates] = gprob
elif len(gstates) == len(state_space) - 1:
gstate = list(state_space - gstates)[0]
gprob = S.One - sum(prob.values())
prob[state_space - gstates] = gprob
else:
raise ValueError("Conflicting information.")
else:
gprob = S.One
if min_key_rv == rv:
return sum([prob[FiniteSet(state)] for state in states])
if isinstance(self, ContinuousMarkovChain):
return gprob * sum([trans_probs(rv.key - min_key_rv.key).__getitem__((gstate, state))
for state in states])
if isinstance(self, DiscreteMarkovChain):
return gprob * sum([(trans_probs**(rv.key - min_key_rv.key)).__getitem__((gstate, state))
for state in states])
if isinstance(condition, Not):
expr = condition.args[0]
return S.One - self.probability(expr, given_condition, evaluate, **kwargs)
if isinstance(condition, And):
compute_later, state2cond, conds = [], dict(), condition.args
for expr in conds:
if isinstance(expr, Relational):
ris = list(expr.atoms(RandomIndexedSymbol))[0]
if state2cond.get(ris, None) is None:
state2cond[ris] = S.true
state2cond[ris] &= expr
else:
compute_later.append(expr)
ris = []
for ri in state2cond:
ris.append(ri)
cset = Intersection(state2cond[ri].as_set(), state_space)
if len(cset) == 0:
return S.Zero
state2cond[ri] = cset.as_relational(ri)
sorted_ris = sorted(ris, key=lambda ri: ri.key)
prod = self.probability(state2cond[sorted_ris[0]], given_condition, evaluate, **kwargs)
for i in range(1, len(sorted_ris)):
ri, prev_ri = sorted_ris[i], sorted_ris[i-1]
if not isinstance(state2cond[ri], Eq):
raise ValueError("The process is in multiple states at %s, unable to determine the probability."%(ri))
mat_of = TransitionMatrixOf(self, mat) if isinstance(self, DiscreteMarkovChain) else GeneratorMatrixOf(self, mat)
prod *= self.probability(state2cond[ri], state2cond[prev_ri]
& mat_of
& StochasticStateSpaceOf(self, state_space),
evaluate, **kwargs)
for expr in compute_later:
prod *= self.probability(expr, given_condition, evaluate, **kwargs)
return prod
if isinstance(condition, Or):
return sum([self.probability(expr, given_condition, evaluate, **kwargs)
for expr in condition.args])
raise NotImplementedError("Mechanism for handling (%s, %s) queries hasn't been "
"implemented yet."%(expr, condition))
def expectation(self, expr, condition=None, evaluate=True, **kwargs):
"""
Handles expectation queries for markov process.
Parameters
==========
expr: RandomIndexedSymbol, Relational, Logic
Condition for which expectation has to be computed. Must
contain a RandomIndexedSymbol of the process.
condition: Relational, Logic
The given conditions under which computations should be done.
Returns
=======
Expectation
Unevaluated object if computations cannot be done due to
insufficient information.
Expr
In all other cases when the computations are successful.
Note
====
Any information passed at the time of query overrides
any information passed at the time of object creation like
transition probabilities, state space.
Pass the transition matrix using TransitionMatrixOf,
generator matrix using GeneratorMatrixOf and state space
using StochasticStateSpaceOf in given_condition using & or And.
"""
check, mat, state_space, condition = \
self._preprocess(condition, evaluate)
if check:
return Expectation(expr, condition)
rvs = random_symbols(expr)
if isinstance(expr, Expr) and isinstance(condition, Eq) \
and len(rvs) == 1:
# handle queries similar to E(f(X[i]), Eq(X[i-m], <some-state>))
rv = list(rvs)[0]
lhsg, rhsg = condition.lhs, condition.rhs
if not isinstance(lhsg, RandomIndexedSymbol):
lhsg, rhsg = (rhsg, lhsg)
if rhsg not in self.state_space:
raise ValueError("%s state is not in the state space."%(rhsg))
if rv.key < lhsg.key:
raise ValueError("Incorrect given condition is given, expectation "
"time %s < time %s"%(rv.key, rv.key))
mat_of = TransitionMatrixOf(self, mat) if isinstance(self, DiscreteMarkovChain) else GeneratorMatrixOf(self, mat)
cond = condition & mat_of & \
StochasticStateSpaceOf(self, state_space)
func = lambda s: self.probability(Eq(rv, s), cond)*expr.subs(rv, s)
return sum([func(s) for s in state_space])
raise NotImplementedError("Mechanism for handling (%s, %s) queries hasn't been "
"implemented yet."%(expr, condition))
class DiscreteMarkovChain(DiscreteTimeStochasticProcess, MarkovProcess):
"""
Represents discrete time Markov chain.
Parameters
==========
sym: Symbol/string_types
state_space: Set
Optional, by default, S.Reals
trans_probs: Matrix/ImmutableMatrix/MatrixSymbol
Optional, by default, None
Examples
========
>>> from sympy.stats import DiscreteMarkovChain, TransitionMatrixOf
>>> from sympy import Matrix, MatrixSymbol, Eq
>>> from sympy.stats import P
>>> T = Matrix([[0.5, 0.2, 0.3],[0.2, 0.5, 0.3],[0.2, 0.3, 0.5]])
>>> Y = DiscreteMarkovChain("Y", [0, 1, 2], T)
>>> YS = DiscreteMarkovChain("Y")
>>> Y.state_space
{0, 1, 2}
>>> Y.transition_probabilities
Matrix([
[0.5, 0.2, 0.3],
[0.2, 0.5, 0.3],
[0.2, 0.3, 0.5]])
>>> TS = MatrixSymbol('T', 3, 3)
>>> P(Eq(YS[3], 2), Eq(YS[1], 1) & TransitionMatrixOf(YS, TS))
T[0, 2]*T[1, 0] + T[1, 1]*T[1, 2] + T[1, 2]*T[2, 2]
>>> P(Eq(Y[3], 2), Eq(Y[1], 1)).round(2)
0.36
References
==========
.. [1] https://en.wikipedia.org/wiki/Markov_chain#Discrete-time_Markov_chain
.. [2] https://www.dartmouth.edu/~chance/teaching_aids/books_articles/probability_book/Chapter11.pdf
"""
index_set = S.Naturals0
def __new__(cls, sym, state_space=S.Reals, trans_probs=None):
sym = _symbol_converter(sym)
state_space = _set_converter(state_space)
if trans_probs != None:
trans_probs = _matrix_checks(trans_probs)
return Basic.__new__(cls, sym, state_space, trans_probs)
@property
def transition_probabilities(self):
"""
Transition probabilities of discrete Markov chain,
either an instance of Matrix or MatrixSymbol.
"""
return self.args[2]
def _transient2transient(self):
"""
Computes the one step probabilities of transient
states to transient states. Used in finding
fundamental matrix, absorbing probabilties.
"""
trans_probs = self.transition_probabilities
if not isinstance(trans_probs, ImmutableMatrix):
return None
m = trans_probs.shape[0]
trans_states = [i for i in range(m) if trans_probs[i, i] != 1]
t2t = [[trans_probs[si, sj] for sj in trans_states] for si in trans_states]
return ImmutableMatrix(t2t)
def _transient2absorbing(self):
"""
Computes the one step probabilities of transient
states to absorbing states. Used in finding
fundamental matrix, absorbing probabilties.
"""
trans_probs = self.transition_probabilities
if not isinstance(trans_probs, ImmutableMatrix):
return None
m, trans_states, absorb_states = \
trans_probs.shape[0], [], []
for i in range(m):
if trans_probs[i, i] == 1:
absorb_states.append(i)
else:
trans_states.append(i)
if not absorb_states or not trans_states:
return None
t2a = [[trans_probs[si, sj] for sj in absorb_states]
for si in trans_states]
return ImmutableMatrix(t2a)
def fundamental_matrix(self):
Q = self._transient2transient()
if Q == None:
return None
I = eye(Q.shape[0])
if (I - Q).det() == 0:
raise ValueError("Fundamental matrix doesn't exists.")
return ImmutableMatrix((I - Q).inv().tolist())
def absorbing_probabilites(self):
"""
Computes the absorbing probabilities, i.e.,
the ij-th entry of the matrix denotes the
probability of Markov chain being absorbed
in state j starting from state i.
"""
R = self._transient2absorbing()
N = self.fundamental_matrix()
if R == None or N == None:
return None
return N*R
def is_regular(self):
w = self.fixed_row_vector()
if w is None or isinstance(w, (Lambda)):
return None
return all((wi > 0) == True for wi in w.row(0))
def is_absorbing_state(self, state):
trans_probs = self.transition_probabilities
if isinstance(trans_probs, ImmutableMatrix) and \
state < trans_probs.shape[0]:
return S(trans_probs[state, state]) is S.One
def is_absorbing_chain(self):
trans_probs = self.transition_probabilities
return any(self.is_absorbing_state(state) == True
for state in range(trans_probs.shape[0]))
def fixed_row_vector(self):
trans_probs = self.transition_probabilities
if trans_probs == None:
return None
if isinstance(trans_probs, MatrixSymbol):
wm = MatrixSymbol('wm', 1, trans_probs.shape[0])
return Lambda((wm, trans_probs), Eq(wm*trans_probs, wm))
w = IndexedBase('w')
wi = [w[i] for i in range(trans_probs.shape[0])]
wm = Matrix([wi])
eqs = (wm*trans_probs - wm).tolist()[0]
eqs.append(sum(wi) - 1)
soln = list(linsolve(eqs, wi))[0]
return ImmutableMatrix([[sol for sol in soln]])
@property
def limiting_distribution(self):
"""
The fixed row vector is the limiting
distribution of a discrete Markov chain.
"""
return self.fixed_row_vector()
class ContinuousMarkovChain(ContinuousTimeStochasticProcess, MarkovProcess):
"""
Represents continuous time Markov chain.
Parameters
==========
sym: Symbol/string_types
state_space: Set
Optional, by default, S.Reals
gen_mat: Matrix/ImmutableMatrix/MatrixSymbol
Optional, by default, None
Examples
========
>>> from sympy.stats import ContinuousMarkovChain
>>> from sympy import Matrix, S, MatrixSymbol
>>> G = Matrix([[-S(1), S(1)], [S(1), -S(1)]])
>>> C = ContinuousMarkovChain('C', state_space=[0, 1], gen_mat=G)
>>> C.limiting_distribution()
Matrix([[1/2, 1/2]])
References
==========
.. [1] https://en.wikipedia.org/wiki/Markov_chain#Continuous-time_Markov_chain
.. [2] http://u.math.biu.ac.il/~amirgi/CTMCnotes.pdf
"""
index_set = S.Reals
def __new__(cls, sym, state_space=S.Reals, gen_mat=None):
sym = _symbol_converter(sym)
state_space = _set_converter(state_space)
if gen_mat != None:
gen_mat = _matrix_checks(gen_mat)
return Basic.__new__(cls, sym, state_space, gen_mat)
@property
def generator_matrix(self):
return self.args[2]
@cacheit
def transition_probabilities(self, gen_mat=None):
t = Dummy('t')
if isinstance(gen_mat, (Matrix, ImmutableMatrix)) and \
gen_mat.is_diagonalizable():
# for faster computation use diagonalized generator matrix
Q, D = gen_mat.diagonalize()
return Lambda(t, Q*exp(t*D)*Q.inv())
if gen_mat != None:
return Lambda(t, exp(t*gen_mat))
def limiting_distribution(self):
gen_mat = self.generator_matrix
if gen_mat == None:
return None
if isinstance(gen_mat, MatrixSymbol):
wm = MatrixSymbol('wm', 1, gen_mat.shape[0])
return Lambda((wm, gen_mat), Eq(wm*gen_mat, wm))
w = IndexedBase('w')
wi = [w[i] for i in range(gen_mat.shape[0])]
wm = Matrix([wi])
eqs = (wm*gen_mat).tolist()[0]
eqs.append(sum(wi) - 1)
soln = list(linsolve(eqs, wi))[0]
return ImmutableMatrix([[sol for sol in soln]])
|
0ed018dcc045ef748c9c8aa5d4527ea959f77e442ac1b7089ce342fd23d4b3b8 | from sympy import (sympify, S, pi, sqrt, exp, Lambda, Indexed, besselk, gamma, Interval,
Range, factorial, Mul, Integer,
Add, rf, Eq, Piecewise, ones, Symbol, Pow, Rational, Sum,
Intersection, Matrix, symbols, Product, IndexedBase)
from sympy.matrices import ImmutableMatrix, MatrixSymbol
from sympy.matrices.expressions.determinant import det
from sympy.stats.joint_rv import (JointDistribution, JointPSpace,
JointDistributionHandmade, MarginalDistribution)
from sympy.stats.rv import _value_check, random_symbols
__all__ = ['JointRV',
'Dirichlet',
'GeneralizedMultivariateLogGamma',
'GeneralizedMultivariateLogGammaOmega',
'Multinomial',
'MultivariateBeta',
'MultivariateEwens',
'MultivariateT',
'NegativeMultinomial',
'NormalGamma'
]
def multivariate_rv(cls, sym, *args):
args = list(map(sympify, args))
dist = cls(*args)
args = dist.args
dist.check(*args)
return JointPSpace(sym, dist).value
def JointRV(symbol, pdf, _set=None):
"""
Create a Joint Random Variable where each of its component is conitinuous,
given the following:
-- a symbol
-- a PDF in terms of indexed symbols of the symbol given
as the first argument
NOTE: As of now, the set for each component for a `JointRV` is
equal to the set of all integers, which can not be changed.
Returns a RandomSymbol.
Examples
========
>>> from sympy import symbols, exp, pi, Indexed, S
>>> from sympy.stats import density
>>> from sympy.stats.joint_rv_types import JointRV
>>> x1, x2 = (Indexed('x', i) for i in (1, 2))
>>> pdf = exp(-x1**2/2 + x1 - x2**2/2 - S(1)/2)/(2*pi)
>>> N1 = JointRV('x', pdf) #Multivariate Normal distribution
>>> density(N1)(1, 2)
exp(-2)/(2*pi)
"""
#TODO: Add support for sets provided by the user
symbol = sympify(symbol)
syms = list(i for i in pdf.free_symbols if isinstance(i, Indexed)
and i.base == IndexedBase(symbol))
syms = tuple(sorted(syms, key = lambda index: index.args[1]))
_set = S.Reals**len(syms)
pdf = Lambda(syms, pdf)
dist = JointDistributionHandmade(pdf, _set)
jrv = JointPSpace(symbol, dist).value
rvs = random_symbols(pdf)
if len(rvs) != 0:
dist = MarginalDistribution(dist, (jrv,))
return JointPSpace(symbol, dist).value
return jrv
#-------------------------------------------------------------------------------
# Multivariate Normal distribution ---------------------------------------------------------
class MultivariateNormalDistribution(JointDistribution):
_argnames = ['mu', 'sigma']
is_Continuous=True
@property
def set(self):
k = self.mu.shape[0]
return S.Reals**k
@staticmethod
def check(mu, sigma):
_value_check(mu.shape[0] == sigma.shape[0],
"Size of the mean vector and covariance matrix are incorrect.")
#check if covariance matrix is positive definite or not.
if not isinstance(sigma, MatrixSymbol):
_value_check(sigma.is_positive_definite,
"The covariance matrix must be positive definite. ")
def pdf(self, *args):
mu, sigma = self.mu, self.sigma
k = mu.shape[0]
args = ImmutableMatrix(args)
x = args - mu
return S.One/sqrt((2*pi)**(k)*det(sigma))*exp(
Rational(-1, 2)*x.transpose()*(sigma.inv()*\
x))[0]
def marginal_distribution(self, indices, sym):
sym = ImmutableMatrix([Indexed(sym, i) for i in indices])
_mu, _sigma = self.mu, self.sigma
k = self.mu.shape[0]
for i in range(k):
if i not in indices:
_mu = _mu.row_del(i)
_sigma = _sigma.col_del(i)
_sigma = _sigma.row_del(i)
return Lambda(tuple(sym), S.One/sqrt((2*pi)**(len(_mu))*det(_sigma))*exp(
Rational(-1, 2)*(_mu - sym).transpose()*(_sigma.inv()*\
(_mu - sym)))[0])
#-------------------------------------------------------------------------------
# Multivariate Laplace distribution ---------------------------------------------------------
class MultivariateLaplaceDistribution(JointDistribution):
_argnames = ['mu', 'sigma']
is_Continuous=True
@property
def set(self):
k = self.mu.shape[0]
return S.Reals**k
@staticmethod
def check(mu, sigma):
_value_check(mu.shape[0] == sigma.shape[0],
"Size of the mean vector and covariance matrix are incorrect.")
# check if covariance matrix is positive definite or not.
if not isinstance(sigma, MatrixSymbol):
_value_check(sigma.is_positive_definite,
"The covariance matrix must be positive definite. ")
def pdf(self, *args):
mu, sigma = self.mu, self.sigma
mu_T = mu.transpose()
k = S(mu.shape[0])
sigma_inv = sigma.inv()
args = ImmutableMatrix(args)
args_T = args.transpose()
x = (mu_T*sigma_inv*mu)[0]
y = (args_T*sigma_inv*args)[0]
v = 1 - k/2
return S(2)/((2*pi)**(S(k)/2)*sqrt(det(sigma)))\
*(y/(2 + x))**(S(v)/2)*besselk(v, sqrt((2 + x)*(y)))\
*exp((args_T*sigma_inv*mu)[0])
#-------------------------------------------------------------------------------
# Multivariate StudentT distribution ---------------------------------------------------------
class MultivariateTDistribution(JointDistribution):
_argnames = ['mu', 'shape_mat', 'dof']
is_Continuous=True
@property
def set(self):
k = self.mu.shape[0]
return S.Reals**k
@staticmethod
def check(mu, sigma, v):
_value_check(mu.shape[0] == sigma.shape[0],
"Size of the location vector and shape matrix are incorrect.")
# check if covariance matrix is positive definite or not.
if not isinstance(sigma, MatrixSymbol):
_value_check(sigma.is_positive_definite,
"The shape matrix must be positive definite. ")
def pdf(self, *args):
mu, sigma = self.mu, self.shape_mat
v = S(self.dof)
k = S(mu.shape[0])
sigma_inv = sigma.inv()
args = ImmutableMatrix(args)
x = args - mu
return gamma((k + v)/2)/(gamma(v/2)*(v*pi)**(k/2)*sqrt(det(sigma)))\
*(1 + 1/v*(x.transpose()*sigma_inv*x)[0])**((-v - k)/2)
def MultivariateT(syms, mu, sigma, v):
"""
Creates a joint random variable with multivariate T-distribution.
Parameters
==========
syms: list/tuple/set of symbols for identifying each component
mu: A list/tuple/set consisting of k means,represents a k
dimensional location vector
sigma: The shape matrix for the distribution
Returns
=======
A random symbol
"""
return multivariate_rv(MultivariateTDistribution, syms, mu, sigma, v)
#-------------------------------------------------------------------------------
# Multivariate Normal Gamma distribution ---------------------------------------------------------
class NormalGammaDistribution(JointDistribution):
_argnames = ['mu', 'lamda', 'alpha', 'beta']
is_Continuous=True
@staticmethod
def check(mu, lamda, alpha, beta):
_value_check(mu.is_real, "Location must be real.")
_value_check(lamda > 0, "Lambda must be positive")
_value_check(alpha > 0, "alpha must be positive")
_value_check(beta > 0, "beta must be positive")
@property
def set(self):
return S.Reals*Interval(0, S.Infinity)
def pdf(self, x, tau):
beta, alpha, lamda = self.beta, self.alpha, self.lamda
mu = self.mu
return beta**alpha*sqrt(lamda)/(gamma(alpha)*sqrt(2*pi))*\
tau**(alpha - S.Half)*exp(-1*beta*tau)*\
exp(-1*(lamda*tau*(x - mu)**2)/S(2))
def marginal_distribution(self, indices, *sym):
if len(indices) == 2:
return self.pdf(*sym)
if indices[0] == 0:
#For marginal over `x`, return non-standardized Student-T's
#distribution
x = sym[0]
v, mu, sigma = self.alpha - S.Half, self.mu, \
S(self.beta)/(self.lamda * self.alpha)
return Lambda(sym, gamma((v + 1)/2)/(gamma(v/2)*sqrt(pi*v)*sigma)*\
(1 + 1/v*((x - mu)/sigma)**2)**((-v -1)/2))
#For marginal over `tau`, return Gamma distribution as per construction
from sympy.stats.crv_types import GammaDistribution
return Lambda(sym, GammaDistribution(self.alpha, self.beta)(sym[0]))
def NormalGamma(syms, mu, lamda, alpha, beta):
"""
Creates a bivariate joint random variable with multivariate Normal gamma
distribution.
Parameters
==========
syms: list/tuple/set of two symbols for identifying each component
mu: A real number, as the mean of the normal distribution
alpha: a positive integer
beta: a positive integer
lamda: a positive integer
Returns
=======
A random symbol
"""
return multivariate_rv(NormalGammaDistribution, syms, mu, lamda, alpha, beta)
#-------------------------------------------------------------------------------
# Multivariate Beta/Dirichlet distribution ---------------------------------------------------------
class MultivariateBetaDistribution(JointDistribution):
_argnames = ['alpha']
is_Continuous = True
@staticmethod
def check(alpha):
_value_check(len(alpha) >= 2, "At least two categories should be passed.")
for a_k in alpha:
_value_check((a_k > 0) != False, "Each concentration parameter"
" should be positive.")
@property
def set(self):
k = len(self.alpha)
return Interval(0, 1)**k
def pdf(self, *syms):
alpha = self.alpha
B = Mul.fromiter(map(gamma, alpha))/gamma(Add(*alpha))
return Mul.fromiter([sym**(a_k - 1) for a_k, sym in zip(alpha, syms)])/B
def MultivariateBeta(syms, *alpha):
"""
Creates a continuous random variable with Dirichlet/Multivariate Beta
Distribution.
The density of the dirichlet distribution can be found at [1].
Parameters
==========
alpha: positive real numbers signifying concentration numbers.
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import density
>>> from sympy.stats.joint_rv import marginal_distribution
>>> from sympy.stats.joint_rv_types import MultivariateBeta
>>> from sympy import Symbol
>>> a1 = Symbol('a1', positive=True)
>>> a2 = Symbol('a2', positive=True)
>>> B = MultivariateBeta('B', [a1, a2])
>>> C = MultivariateBeta('C', a1, a2)
>>> x = Symbol('x')
>>> y = Symbol('y')
>>> density(B)(x, y)
x**(a1 - 1)*y**(a2 - 1)*gamma(a1 + a2)/(gamma(a1)*gamma(a2))
>>> marginal_distribution(C, C[0])(x)
x**(a1 - 1)*gamma(a1 + a2)/(a2*gamma(a1)*gamma(a2))
References
==========
.. [1] https://en.wikipedia.org/wiki/Dirichlet_distribution
.. [2] http://mathworld.wolfram.com/DirichletDistribution.html
"""
if not isinstance(alpha[0], list):
alpha = (list(alpha),)
return multivariate_rv(MultivariateBetaDistribution, syms, alpha[0])
Dirichlet = MultivariateBeta
#-------------------------------------------------------------------------------
# Multivariate Ewens distribution ---------------------------------------------------------
class MultivariateEwensDistribution(JointDistribution):
_argnames = ['n', 'theta']
is_Discrete = True
is_Continuous = False
@staticmethod
def check(n, theta):
_value_check((n > 0),
"sample size should be positive integer.")
_value_check(theta.is_positive, "mutation rate should be positive.")
@property
def set(self):
if not isinstance(self.n, Integer):
i = Symbol('i', integer=True, positive=True)
return Product(Intersection(S.Naturals0, Interval(0, self.n//i)),
(i, 1, self.n))
prod_set = Range(0, self.n + 1)
for i in range(2, self.n + 1):
prod_set *= Range(0, self.n//i + 1)
return prod_set.flatten()
def pdf(self, *syms):
n, theta = self.n, self.theta
condi = isinstance(self.n, Integer)
if not (isinstance(syms[0], IndexedBase) or condi):
raise ValueError("Please use IndexedBase object for syms as "
"the dimension is symbolic")
term_1 = factorial(n)/rf(theta, n)
if condi:
term_2 = Mul.fromiter([theta**syms[j]/((j+1)**syms[j]*factorial(syms[j]))
for j in range(n)])
cond = Eq(sum([(k + 1)*syms[k] for k in range(n)]), n)
return Piecewise((term_1 * term_2, cond), (0, True))
syms = syms[0]
j, k = symbols('j, k', positive=True, integer=True)
term_2 = Product(theta**syms[j]/((j+1)**syms[j]*factorial(syms[j])),
(j, 0, n - 1))
cond = Eq(Sum((k + 1)*syms[k], (k, 0, n - 1)), n)
return Piecewise((term_1 * term_2, cond), (0, True))
def MultivariateEwens(syms, n, theta):
"""
Creates a discrete random variable with Multivariate Ewens
Distribution.
The density of the said distribution can be found at [1].
Parameters
==========
n: positive integer of class Integer,
size of the sample or the integer whose partitions are considered
theta: mutation rate, must be positive real number.
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import density
>>> from sympy.stats.joint_rv import marginal_distribution
>>> from sympy.stats.joint_rv_types import MultivariateEwens
>>> from sympy import Symbol
>>> a1 = Symbol('a1', positive=True)
>>> a2 = Symbol('a2', positive=True)
>>> ed = MultivariateEwens('E', 2, 1)
>>> density(ed)(a1, a2)
Piecewise((2**(-a2)/(factorial(a1)*factorial(a2)), Eq(a1 + 2*a2, 2)), (0, True))
>>> marginal_distribution(ed, ed[0])(a1)
Piecewise((1/factorial(a1), Eq(a1, 2)), (0, True))
References
==========
.. [1] https://en.wikipedia.org/wiki/Ewens%27s_sampling_formula
.. [2] http://www.stat.rutgers.edu/home/hcrane/Papers/STS529.pdf
"""
return multivariate_rv(MultivariateEwensDistribution, syms, n, theta)
#-------------------------------------------------------------------------------
# Generalized Multivariate Log Gamma distribution ---------------------------------------------------------
class GeneralizedMultivariateLogGammaDistribution(JointDistribution):
_argnames = ['delta', 'v', 'lamda', 'mu']
is_Continuous=True
def check(self, delta, v, l, mu):
_value_check((delta >= 0, delta <= 1), "delta must be in range [0, 1].")
_value_check((v > 0), "v must be positive")
for lk in l:
_value_check((lk > 0), "lamda must be a positive vector.")
for muk in mu:
_value_check((muk > 0), "mu must be a positive vector.")
_value_check(len(l) > 1,"the distribution should have at least"
" two random variables.")
@property
def set(self):
return S.Reals**len(self.lamda)
def pdf(self, *y):
from sympy.functions.special.gamma_functions import gamma
d, v, l, mu = self.delta, self.v, self.lamda, self.mu
n = Symbol('n', negative=False, integer=True)
k = len(l)
sterm1 = Pow((1 - d), n)/\
((gamma(v + n)**(k - 1))*gamma(v)*gamma(n + 1))
sterm2 = Mul.fromiter([mui*li**(-v - n) for mui, li in zip(mu, l)])
term1 = sterm1 * sterm2
sterm3 = (v + n) * sum([mui * yi for mui, yi in zip(mu, y)])
sterm4 = sum([exp(mui * yi)/li for (mui, yi, li) in zip(mu, y, l)])
term2 = exp(sterm3 - sterm4)
return Pow(d, v) * Sum(term1 * term2, (n, 0, S.Infinity))
def GeneralizedMultivariateLogGamma(syms, delta, v, lamda, mu):
"""
Creates a joint random variable with generalized multivariate log gamma
distribution.
The joint pdf can be found at [1].
Parameters
==========
syms: list/tuple/set of symbols for identifying each component
delta: A constant in range [0, 1]
v: positive real
lamda: a list of positive reals
mu: a list of positive reals
Returns
=======
A Random Symbol
Examples
========
>>> from sympy.stats import density
>>> from sympy.stats.joint_rv import marginal_distribution
>>> from sympy.stats.joint_rv_types import GeneralizedMultivariateLogGamma
>>> from sympy import symbols, S
>>> v = 1
>>> l, mu = [1, 1, 1], [1, 1, 1]
>>> d = S.Half
>>> y = symbols('y_1:4', positive=True)
>>> Gd = GeneralizedMultivariateLogGamma('G', d, v, l, mu)
>>> density(Gd)(y[0], y[1], y[2])
Sum(2**(-n)*exp((n + 1)*(y_1 + y_2 + y_3) - exp(y_1) - exp(y_2) -
exp(y_3))/gamma(n + 1)**3, (n, 0, oo))/2
References
==========
.. [1] https://en.wikipedia.org/wiki/Generalized_multivariate_log-gamma_distribution
.. [2] https://www.researchgate.net/publication/234137346_On_a_multivariate_log-gamma_distribution_and_the_use_of_the_distribution_in_the_Bayesian_analysis
Note
====
If the GeneralizedMultivariateLogGamma is too long to type use,
`from sympy.stats.joint_rv_types import GeneralizedMultivariateLogGamma as GMVLG`
If you want to pass the matrix omega instead of the constant delta, then use,
GeneralizedMultivariateLogGammaOmega.
"""
return multivariate_rv(GeneralizedMultivariateLogGammaDistribution,
syms, delta, v, lamda, mu)
def GeneralizedMultivariateLogGammaOmega(syms, omega, v, lamda, mu):
"""
Extends GeneralizedMultivariateLogGamma.
Parameters
==========
syms: list/tuple/set of symbols for identifying each component
omega: A square matrix
Every element of square matrix must be absolute value of
square root of correlation coefficient
v: positive real
lamda: a list of positive reals
mu: a list of positive reals
Returns
=======
A Random Symbol
Examples
========
>>> from sympy.stats import density
>>> from sympy.stats.joint_rv import marginal_distribution
>>> from sympy.stats.joint_rv_types import GeneralizedMultivariateLogGammaOmega
>>> from sympy import Matrix, symbols, S
>>> omega = Matrix([[1, S.Half, S.Half], [S.Half, 1, S.Half], [S.Half, S.Half, 1]])
>>> v = 1
>>> l, mu = [1, 1, 1], [1, 1, 1]
>>> G = GeneralizedMultivariateLogGammaOmega('G', omega, v, l, mu)
>>> y = symbols('y_1:4', positive=True)
>>> density(G)(y[0], y[1], y[2])
sqrt(2)*Sum((1 - sqrt(2)/2)**n*exp((n + 1)*(y_1 + y_2 + y_3) - exp(y_1) -
exp(y_2) - exp(y_3))/gamma(n + 1)**3, (n, 0, oo))/2
References
==========
See references of GeneralizedMultivariateLogGamma.
Notes
=====
If the GeneralizedMultivariateLogGammaOmega is too long to type use,
`from sympy.stats.joint_rv_types import GeneralizedMultivariateLogGammaOmega as GMVLGO`
"""
_value_check((omega.is_square, isinstance(omega, Matrix)), "omega must be a"
" square matrix")
for val in omega.values():
_value_check((val >= 0, val <= 1),
"all values in matrix must be between 0 and 1(both inclusive).")
_value_check(omega.diagonal().equals(ones(1, omega.shape[0])),
"all the elements of diagonal should be 1.")
_value_check((omega.shape[0] == len(lamda), len(lamda) == len(mu)),
"lamda, mu should be of same length and omega should "
" be of shape (length of lamda, length of mu)")
_value_check(len(lamda) > 1,"the distribution should have at least"
" two random variables.")
delta = Pow(Rational(omega.det()), Rational(1, len(lamda) - 1))
return GeneralizedMultivariateLogGamma(syms, delta, v, lamda, mu)
#-------------------------------------------------------------------------------
# Multinomial distribution ---------------------------------------------------------
class MultinomialDistribution(JointDistribution):
_argnames = ['n', 'p']
is_Continuous=False
is_Discrete = True
@staticmethod
def check(n, p):
_value_check(n > 0,
"number of trials must be a positive integer")
for p_k in p:
_value_check((p_k >= 0, p_k <= 1),
"probability must be in range [0, 1]")
_value_check(Eq(sum(p), 1),
"probabilities must sum to 1")
@property
def set(self):
return Intersection(S.Naturals0, Interval(0, self.n))**len(self.p)
def pdf(self, *x):
n, p = self.n, self.p
term_1 = factorial(n)/Mul.fromiter([factorial(x_k) for x_k in x])
term_2 = Mul.fromiter([p_k**x_k for p_k, x_k in zip(p, x)])
return Piecewise((term_1 * term_2, Eq(sum(x), n)), (0, True))
def Multinomial(syms, n, *p):
"""
Creates a discrete random variable with Multinomial Distribution.
The density of the said distribution can be found at [1].
Parameters
==========
n: positive integer of class Integer,
number of trials
p: event probabilites, >= 0 and <= 1
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import density
>>> from sympy.stats.joint_rv import marginal_distribution
>>> from sympy.stats.joint_rv_types import Multinomial
>>> from sympy import symbols
>>> x1, x2, x3 = symbols('x1, x2, x3', nonnegative=True, integer=True)
>>> p1, p2, p3 = symbols('p1, p2, p3', positive=True)
>>> M = Multinomial('M', 3, p1, p2, p3)
>>> density(M)(x1, x2, x3)
Piecewise((6*p1**x1*p2**x2*p3**x3/(factorial(x1)*factorial(x2)*factorial(x3)),
Eq(x1 + x2 + x3, 3)), (0, True))
>>> marginal_distribution(M, M[0])(x1).subs(x1, 1)
3*p1*p2**2 + 6*p1*p2*p3 + 3*p1*p3**2
References
==========
.. [1] https://en.wikipedia.org/wiki/Multinomial_distribution
.. [2] http://mathworld.wolfram.com/MultinomialDistribution.html
"""
if not isinstance(p[0], list):
p = (list(p), )
return multivariate_rv(MultinomialDistribution, syms, n, p[0])
#-------------------------------------------------------------------------------
# Negative Multinomial Distribution ---------------------------------------------------------
class NegativeMultinomialDistribution(JointDistribution):
_argnames = ['k0', 'p']
is_Continuous=False
is_Discrete = True
@staticmethod
def check(k0, p):
_value_check(k0 > 0,
"number of failures must be a positive integer")
for p_k in p:
_value_check((p_k >= 0, p_k <= 1),
"probability must be in range [0, 1].")
_value_check(sum(p) <= 1,
"success probabilities must not be greater than 1.")
@property
def set(self):
return Range(0, S.Infinity)**len(self.p)
def pdf(self, *k):
k0, p = self.k0, self.p
term_1 = (gamma(k0 + sum(k))*(1 - sum(p))**k0)/gamma(k0)
term_2 = Mul.fromiter([pi**ki/factorial(ki) for pi, ki in zip(p, k)])
return term_1 * term_2
def NegativeMultinomial(syms, k0, *p):
"""
Creates a discrete random variable with Negative Multinomial Distribution.
The density of the said distribution can be found at [1].
Parameters
==========
k0: positive integer of class Integer,
number of failures before the experiment is stopped
p: event probabilites, >= 0 and <= 1
Returns
=======
A RandomSymbol.
Examples
========
>>> from sympy.stats import density
>>> from sympy.stats.joint_rv import marginal_distribution
>>> from sympy.stats.joint_rv_types import NegativeMultinomial
>>> from sympy import symbols
>>> x1, x2, x3 = symbols('x1, x2, x3', nonnegative=True, integer=True)
>>> p1, p2, p3 = symbols('p1, p2, p3', positive=True)
>>> N = NegativeMultinomial('M', 3, p1, p2, p3)
>>> N_c = NegativeMultinomial('M', 3, 0.1, 0.1, 0.1)
>>> density(N)(x1, x2, x3)
p1**x1*p2**x2*p3**x3*(-p1 - p2 - p3 + 1)**3*gamma(x1 + x2 +
x3 + 3)/(2*factorial(x1)*factorial(x2)*factorial(x3))
>>> marginal_distribution(N_c, N_c[0])(1).evalf().round(2)
0.25
References
==========
.. [1] https://en.wikipedia.org/wiki/Negative_multinomial_distribution
.. [2] http://mathworld.wolfram.com/NegativeBinomialDistribution.html
"""
if not isinstance(p[0], list):
p = (list(p), )
return multivariate_rv(NegativeMultinomialDistribution, syms, k0, p[0])
|
94036eccc7f5b56b9eb28c3edb5fcae7183a6aa056a4a7875f019cf027f4b9e1 | """Tools for arithmetic error propagation."""
from __future__ import print_function, division
from itertools import repeat, combinations
from sympy import S, Symbol, Add, Mul, simplify, Pow, exp
from sympy.stats.symbolic_probability import RandomSymbol, Variance, Covariance
_arg0_or_var = lambda var: var.args[0] if len(var.args) > 0 else var
def variance_prop(expr, consts=(), include_covar=False):
r"""Symbolically propagates variance (`\sigma^2`) for expressions.
This is computed as as seen in [1]_.
Parameters
==========
expr : Expr
A sympy expression to compute the variance for.
consts : sequence of Symbols, optional
Represents symbols that are known constants in the expr,
and thus have zero variance. All symbols not in consts are
assumed to be variant.
include_covar : bool, optional
Flag for whether or not to include covariances, default=False.
Returns
=======
var_expr : Expr
An expression for the total variance of the expr.
The variance for the original symbols (e.g. x) are represented
via instance of the Variance symbol (e.g. Variance(x)).
Examples
========
>>> from sympy import symbols, exp
>>> from sympy.stats.error_prop import variance_prop
>>> x, y = symbols('x y')
>>> variance_prop(x + y)
Variance(x) + Variance(y)
>>> variance_prop(x * y)
x**2*Variance(y) + y**2*Variance(x)
>>> variance_prop(exp(2*x))
4*exp(4*x)*Variance(x)
References
==========
.. [1] https://en.wikipedia.org/wiki/Propagation_of_uncertainty
"""
args = expr.args
if len(args) == 0:
if expr in consts:
return S.Zero
elif isinstance(expr, RandomSymbol):
return Variance(expr).doit()
elif isinstance(expr, Symbol):
return Variance(RandomSymbol(expr)).doit()
else:
return S.Zero
nargs = len(args)
var_args = list(map(variance_prop, args, repeat(consts, nargs),
repeat(include_covar, nargs)))
if isinstance(expr, Add):
var_expr = Add(*var_args)
if include_covar:
terms = [2 * Covariance(_arg0_or_var(x), _arg0_or_var(y)).doit() \
for x, y in combinations(var_args, 2)]
var_expr += Add(*terms)
elif isinstance(expr, Mul):
terms = [v/a**2 for a, v in zip(args, var_args)]
var_expr = simplify(expr**2 * Add(*terms))
if include_covar:
terms = [2*Covariance(_arg0_or_var(x), _arg0_or_var(y)).doit()/(a*b) \
for (a, b), (x, y) in zip(combinations(args, 2),
combinations(var_args, 2))]
var_expr += Add(*terms)
elif isinstance(expr, Pow):
b = args[1]
v = var_args[0] * (expr * b / args[0])**2
var_expr = simplify(v)
elif isinstance(expr, exp):
var_expr = simplify(var_args[0] * expr**2)
else:
# unknown how to proceed, return variance of whole expr.
var_expr = Variance(expr)
return var_expr
|
90686784ac3fad096fc2026cb233e8c0d61d9927acaa7728d4f227d3bafc2685 | """
Joint Random Variables Module
See Also
========
sympy.stats.rv
sympy.stats.frv
sympy.stats.crv
sympy.stats.drv
"""
from __future__ import print_function, division
from sympy import (Basic, Lambda, sympify, Indexed, Symbol, ProductSet, S,
Dummy)
from sympy.concrete.products import Product
from sympy.concrete.summations import Sum, summation
from sympy.core.compatibility import string_types, iterable
from sympy.core.containers import Tuple
from sympy.integrals.integrals import Integral, integrate
from sympy.matrices import ImmutableMatrix
from sympy.stats.crv import (ContinuousDistribution,
SingleContinuousDistribution, SingleContinuousPSpace)
from sympy.stats.drv import (DiscreteDistribution,
SingleDiscreteDistribution, SingleDiscretePSpace)
from sympy.stats.rv import (ProductPSpace, NamedArgsMixin,
ProductDomain, RandomSymbol, random_symbols, SingleDomain)
from sympy.utilities.misc import filldedent
# __all__ = ['marginal_distribution']
class JointPSpace(ProductPSpace):
"""
Represents a joint probability space. Represented using symbols for
each component and a distribution.
"""
def __new__(cls, sym, dist):
if isinstance(dist, SingleContinuousDistribution):
return SingleContinuousPSpace(sym, dist)
if isinstance(dist, SingleDiscreteDistribution):
return SingleDiscretePSpace(sym, dist)
if isinstance(sym, string_types):
sym = Symbol(sym)
if not isinstance(sym, Symbol):
raise TypeError("s should have been string or Symbol")
return Basic.__new__(cls, sym, dist)
@property
def set(self):
return self.domain.set
@property
def symbol(self):
return self.args[0]
@property
def distribution(self):
return self.args[1]
@property
def value(self):
return JointRandomSymbol(self.symbol, self)
@property
def component_count(self):
_set = self.distribution.set
if isinstance(_set, ProductSet):
return S(len(_set.args))
elif isinstance(_set, Product):
return _set.limits[0][-1]
return S.One
@property
def pdf(self):
sym = [Indexed(self.symbol, i) for i in range(self.component_count)]
return self.distribution(*sym)
@property
def domain(self):
rvs = random_symbols(self.distribution)
if not rvs:
return SingleDomain(self.symbol, self.distribution.set)
return ProductDomain(*[rv.pspace.domain for rv in rvs])
def component_domain(self, index):
return self.set.args[index]
def marginal_distribution(self, *indices):
count = self.component_count
if count.atoms(Symbol):
raise ValueError("Marginal distributions cannot be computed "
"for symbolic dimensions. It is a work under progress.")
orig = [Indexed(self.symbol, i) for i in range(count)]
all_syms = [Symbol(str(i)) for i in orig]
replace_dict = dict(zip(all_syms, orig))
sym = tuple(Symbol(str(Indexed(self.symbol, i))) for i in indices)
limits = list([i,] for i in all_syms if i not in sym)
index = 0
for i in range(count):
if i not in indices:
limits[index].append(self.distribution.set.args[i])
limits[index] = tuple(limits[index])
index += 1
if self.distribution.is_Continuous:
f = Lambda(sym, integrate(self.distribution(*all_syms), *limits))
elif self.distribution.is_Discrete:
f = Lambda(sym, summation(self.distribution(*all_syms), *limits))
return f.xreplace(replace_dict)
def compute_expectation(self, expr, rvs=None, evaluate=False, **kwargs):
syms = tuple(self.value[i] for i in range(self.component_count))
rvs = rvs or syms
if not any([i in rvs for i in syms]):
return expr
expr = expr*self.pdf
for rv in rvs:
if isinstance(rv, Indexed):
expr = expr.xreplace({rv: Indexed(str(rv.base), rv.args[1])})
elif isinstance(rv, RandomSymbol):
expr = expr.xreplace({rv: rv.symbol})
if self.value in random_symbols(expr):
raise NotImplementedError(filldedent('''
Expectations of expression with unindexed joint random symbols
cannot be calculated yet.'''))
limits = tuple((Indexed(str(rv.base),rv.args[1]),
self.distribution.set.args[rv.args[1]]) for rv in syms)
return Integral(expr, *limits)
def where(self, condition):
raise NotImplementedError()
def compute_density(self, expr):
raise NotImplementedError()
def sample(self):
raise NotImplementedError()
def probability(self, condition):
raise NotImplementedError()
class JointDistribution(Basic, NamedArgsMixin):
"""
Represented by the random variables part of the joint distribution.
Contains methods for PDF, CDF, sampling, marginal densities, etc.
"""
_argnames = ('pdf', )
def __new__(cls, *args):
args = list(map(sympify, args))
for i in range(len(args)):
if isinstance(args[i], list):
args[i] = ImmutableMatrix(args[i])
return Basic.__new__(cls, *args)
@property
def domain(self):
return ProductDomain(self.symbols)
@property
def pdf(self, *args):
return self.density.args[1]
def cdf(self, other):
if not isinstance(other, dict):
raise ValueError("%s should be of type dict, got %s"%(other, type(other)))
rvs = other.keys()
_set = self.domain.set.sets
expr = self.pdf(tuple(i.args[0] for i in self.symbols))
for i in range(len(other)):
if rvs[i].is_Continuous:
density = Integral(expr, (rvs[i], _set[i].inf,
other[rvs[i]]))
elif rvs[i].is_Discrete:
density = Sum(expr, (rvs[i], _set[i].inf,
other[rvs[i]]))
return density
def __call__(self, *args):
return self.pdf(*args)
class JointRandomSymbol(RandomSymbol):
"""
Representation of random symbols with joint probability distributions
to allow indexing."
"""
def __getitem__(self, key):
if isinstance(self.pspace, JointPSpace):
if (self.pspace.component_count <= key) == True:
raise ValueError("Index keys for %s can only up to %s." %
(self.name, self.pspace.component_count - 1))
return Indexed(self, key)
class JointDistributionHandmade(JointDistribution, NamedArgsMixin):
_argnames = ('pdf',)
is_Continuous = True
@property
def set(self):
return self.args[1]
def marginal_distribution(rv, *indices):
"""
Marginal distribution function of a joint random variable.
Parameters
==========
rv: A random variable with a joint probability distribution.
indices: component indices or the indexed random symbol
for whom the joint distribution is to be calculated
Returns
=======
A Lambda expression n `sym`.
Examples
========
>>> from sympy.stats.crv_types import Normal
>>> from sympy.stats.joint_rv import marginal_distribution
>>> m = Normal('X', [1, 2], [[2, 1], [1, 2]])
>>> marginal_distribution(m, m[0])(1)
1/(2*sqrt(pi))
"""
indices = list(indices)
for i in range(len(indices)):
if isinstance(indices[i], Indexed):
indices[i] = indices[i].args[1]
prob_space = rv.pspace
if not indices:
raise ValueError(
"At least one component for marginal density is needed.")
if hasattr(prob_space.distribution, 'marginal_distribution'):
return prob_space.distribution.marginal_distribution(indices, rv.symbol)
return prob_space.marginal_distribution(*indices)
class CompoundDistribution(Basic, NamedArgsMixin):
"""
Represents a compound probability distribution.
Constructed using a single probability distribution with a parameter
distributed according to some given distribution.
"""
def __new__(cls, dist):
if not isinstance(dist, (ContinuousDistribution, DiscreteDistribution)):
raise ValueError(filldedent('''CompoundDistribution can only be
initialized from ContinuousDistribution or DiscreteDistribution
'''))
_args = dist.args
if not any([isinstance(i, RandomSymbol) for i in _args]):
return dist
return Basic.__new__(cls, dist)
@property
def latent_distributions(self):
return random_symbols(self.args[0])
def pdf(self, *x):
dist = self.args[0]
z = Dummy('z')
if isinstance(dist, ContinuousDistribution):
rv = SingleContinuousPSpace(z, dist).value
elif isinstance(dist, DiscreteDistribution):
rv = SingleDiscretePSpace(z, dist).value
return MarginalDistribution(self, (rv,)).pdf(*x)
def set(self):
return self.args[0].set
def __call__(self, *args):
return self.pdf(*args)
class MarginalDistribution(Basic):
"""
Represents the marginal distribution of a joint probability space.
Initialised using a probability distribution and random variables(or
their indexed components) which should be a part of the resultant
distribution.
"""
def __new__(cls, dist, *rvs):
if len(rvs) == 1 and iterable(rvs[0]):
rvs = tuple(rvs[0])
if not all([isinstance(rv, (Indexed, RandomSymbol))] for rv in rvs):
raise ValueError(filldedent('''Marginal distribution can be
intitialised only in terms of random variables or indexed random
variables'''))
rvs = Tuple.fromiter(rv for rv in rvs)
if not isinstance(dist, JointDistribution) and len(random_symbols(dist)) == 0:
return dist
return Basic.__new__(cls, dist, rvs)
def check(self):
pass
@property
def set(self):
rvs = [i for i in self.args[1] if isinstance(i, RandomSymbol)]
return ProductSet(*[rv.pspace.set for rv in rvs])
@property
def symbols(self):
rvs = self.args[1]
return set([rv.pspace.symbol for rv in rvs])
def pdf(self, *x):
expr, rvs = self.args[0], self.args[1]
marginalise_out = [i for i in random_symbols(expr) if i not in rvs]
if isinstance(expr, CompoundDistribution):
syms = Dummy('x', real=True)
expr = expr.args[0].pdf(syms)
elif isinstance(expr, JointDistribution):
count = len(expr.domain.args)
x = Dummy('x', real=True, finite=True)
syms = tuple(Indexed(x, i) for i in count)
expr = expr.pdf(syms)
else:
syms = tuple(rv.pspace.symbol if isinstance(rv, RandomSymbol) else rv.args[0] for rv in rvs)
return Lambda(syms, self.compute_pdf(expr, marginalise_out))(*x)
def compute_pdf(self, expr, rvs):
for rv in rvs:
lpdf = 1
if isinstance(rv, RandomSymbol):
lpdf = rv.pspace.pdf
expr = self.marginalise_out(expr*lpdf, rv)
return expr
def marginalise_out(self, expr, rv):
from sympy.concrete.summations import Sum
if isinstance(rv, RandomSymbol):
dom = rv.pspace.set
elif isinstance(rv, Indexed):
dom = rv.base.component_domain(
rv.pspace.component_domain(rv.args[1]))
expr = expr.xreplace({rv: rv.pspace.symbol})
if rv.pspace.is_Continuous:
#TODO: Modify to support integration
#for all kinds of sets.
expr = Integral(expr, (rv.pspace.symbol, dom))
elif rv.pspace.is_Discrete:
#incorporate this into `Sum`/`summation`
if dom in (S.Integers, S.Naturals, S.Naturals0):
dom = (dom.inf, dom.sup)
expr = Sum(expr, (rv.pspace.symbol, dom))
return expr
def __call__(self, *args):
return self.pdf(*args)
|
86d1527a98b921a613ce30b0cf4f50e2d842fa83034dfef46d4aac28864f730b | from __future__ import print_function, division
from sympy import (Basic, exp, pi, Lambda, Trace, S, MatrixSymbol, Integral,
gamma, Product, Dummy, Sum, Abs, IndexedBase, I)
from sympy.core.sympify import _sympify
from sympy.stats.rv import (_symbol_converter, Density, RandomMatrixSymbol,
RandomSymbol)
from sympy.stats.joint_rv_types import JointDistributionHandmade
from sympy.stats.random_matrix import RandomMatrixPSpace
from sympy.tensor.array import ArrayComprehension
__all__ = [
'CircularEnsemble',
'CircularUnitaryEnsemble',
'CircularOrthogonalEnsemble',
'CircularSymplecticEnsemble',
'GaussianEnsemble',
'GaussianUnitaryEnsemble',
'GaussianOrthogonalEnsemble',
'GaussianSymplecticEnsemble',
'joint_eigen_distribution',
'JointEigenDistribution',
'level_spacing_distribution'
]
class RandomMatrixEnsemble(Basic):
"""
Base class for random matrix ensembles.
It acts as an umbrella and contains
the methods common to all the ensembles
defined in sympy.stats.random_matrix_models.
"""
def __new__(cls, sym, dim=None):
sym, dim = _symbol_converter(sym), _sympify(dim)
if dim.is_integer == False:
raise ValueError("Dimension of the random matrices must be "
"integers, received %s instead."%(dim))
self = Basic.__new__(cls, sym, dim)
rmp = RandomMatrixPSpace(sym, model=self)
return RandomMatrixSymbol(sym, dim, dim, pspace=rmp)
symbol = property(lambda self: self.args[0])
dimension = property(lambda self: self.args[1])
def density(self, expr):
return Density(expr)
class GaussianEnsemble(RandomMatrixEnsemble):
"""
Abstract class for Gaussian ensembles.
Contains the properties common to all the
gaussian ensembles.
References
==========
.. [1] https://en.wikipedia.org/wiki/Random_matrix#Gaussian_ensembles
.. [2] https://arxiv.org/pdf/1712.07903.pdf
"""
def _compute_normalization_constant(self, beta, n):
"""
Helper function for computing normalization
constant for joint probability density of eigen
values of Gaussian ensembles.
References
==========
.. [1] https://en.wikipedia.org/wiki/Selberg_integral#Mehta's_integral
"""
n = S(n)
prod_term = lambda j: gamma(1 + beta*S(j)/2)/gamma(S.One + beta/S(2))
j = Dummy('j', integer=True, positive=True)
term1 = Product(prod_term(j), (j, 1, n)).doit()
term2 = (2/(beta*n))**(beta*n*(n - 1)/4 + n/2)
term3 = (2*pi)**(n/2)
return term1 * term2 * term3
def _compute_joint_eigen_distribution(self, beta):
"""
Helper function for computing the joint
probability distribution of eigen values
of the random matrix.
"""
n = self.dimension
Zbn = self._compute_normalization_constant(beta, n)
l = IndexedBase('l')
i = Dummy('i', integer=True, positive=True)
j = Dummy('j', integer=True, positive=True)
k = Dummy('k', integer=True, positive=True)
term1 = exp((-S(n)/2) * Sum(l[k]**2, (k, 1, n)).doit())
sub_term = Lambda(i, Product(Abs(l[j] - l[i])**beta, (j, i + 1, n)))
term2 = Product(sub_term(i).doit(), (i, 1, n - 1)).doit()
syms = ArrayComprehension(l[k], (k, 1, n)).doit()
return Lambda(tuple(syms), (term1 * term2)/Zbn)
class GaussianUnitaryEnsemble(GaussianEnsemble):
"""
Represents Gaussian Unitary Ensembles.
Examples
========
>>> from sympy.stats import GaussianUnitaryEnsemble as GUE, density
>>> G = GUE('U', 2)
>>> density(G)
Lambda(H, exp(-Trace(H**2))/(2*pi**2))
"""
@property
def normalization_constant(self):
n = self.dimension
return 2**(S(n)/2) * pi**(S(n**2)/2)
def density(self, expr):
n, ZGUE = self.dimension, self.normalization_constant
h_pspace = RandomMatrixPSpace('P', model=self)
H = RandomMatrixSymbol('H', n, n, pspace=h_pspace)
return Lambda(H, exp(-S(n)/2 * Trace(H**2))/ZGUE)
def joint_eigen_distribution(self):
return self._compute_joint_eigen_distribution(S(2))
def level_spacing_distribution(self):
s = Dummy('s')
f = (32/pi**2)*(s**2)*exp((-4/pi)*s**2)
return Lambda(s, f)
class GaussianOrthogonalEnsemble(GaussianEnsemble):
"""
Represents Gaussian Orthogonal Ensembles.
Examples
========
>>> from sympy.stats import GaussianOrthogonalEnsemble as GOE, density
>>> G = GOE('U', 2)
>>> density(G)
Lambda(H, exp(-Trace(H**2)/2)/Integral(exp(-Trace(_H**2)/2), _H))
"""
@property
def normalization_constant(self):
n = self.dimension
_H = MatrixSymbol('_H', n, n)
return Integral(exp(-S(n)/4 * Trace(_H**2)))
def density(self, expr):
n, ZGOE = self.dimension, self.normalization_constant
h_pspace = RandomMatrixPSpace('P', model=self)
H = RandomMatrixSymbol('H', n, n, pspace=h_pspace)
return Lambda(H, exp(-S(n)/4 * Trace(H**2))/ZGOE)
def joint_eigen_distribution(self):
return self._compute_joint_eigen_distribution(S.One)
def level_spacing_distribution(self):
s = Dummy('s')
f = (pi/2)*s*exp((-pi/4)*s**2)
return Lambda(s, f)
class GaussianSymplecticEnsemble(GaussianEnsemble):
"""
Represents Gaussian Symplectic Ensembles.
Examples
========
>>> from sympy.stats import GaussianSymplecticEnsemble as GSE, density
>>> G = GSE('U', 2)
>>> density(G)
Lambda(H, exp(-2*Trace(H**2))/Integral(exp(-2*Trace(_H**2)), _H))
"""
@property
def normalization_constant(self):
n = self.dimension
_H = MatrixSymbol('_H', n, n)
return Integral(exp(-S(n) * Trace(_H**2)))
def density(self, expr):
n, ZGSE = self.dimension, self.normalization_constant
h_pspace = RandomMatrixPSpace('P', model=self)
H = RandomMatrixSymbol('H', n, n, pspace=h_pspace)
return Lambda(H, exp(-S(n) * Trace(H**2))/ZGSE)
def joint_eigen_distribution(self):
return self._compute_joint_eigen_distribution(S(4))
def level_spacing_distribution(self):
s = Dummy('s')
f = ((S(2)**18)/((S(3)**6)*(pi**3)))*(s**4)*exp((-64/(9*pi))*s**2)
return Lambda(s, f)
class CircularEnsemble(RandomMatrixEnsemble):
"""
Abstract class for Circular ensembles.
Contains the properties and methods
common to all the circular ensembles.
References
==========
.. [1] https://en.wikipedia.org/wiki/Circular_ensemble
"""
def density(self, expr):
# TODO : Add support for Lie groups(as extensions of sympy.diffgeom)
# and define measures on them
raise NotImplementedError("Support for Haar measure hasn't been "
"implemented yet, therefore the density of "
"%s cannot be computed."%(self))
def _compute_joint_eigen_distribution(self, beta):
"""
Helper function to compute the joint distribution of phases
of the complex eigen values of matrices belonging to any
circular ensembles.
"""
n = self.dimension
Zbn = ((2*pi)**n)*(gamma(beta*n/2 + 1)/S((gamma(beta/2 + 1)))**n)
t = IndexedBase('t')
i, j, k = (Dummy('i', integer=True), Dummy('j', integer=True),
Dummy('k', integer=True))
syms = ArrayComprehension(t[i], (i, 1, n)).doit()
f = Product(Product(Abs(exp(I*t[k]) - exp(I*t[j]))**beta, (j, k + 1, n)).doit(),
(k, 1, n - 1)).doit()
return Lambda(tuple(syms), f/Zbn)
class CircularUnitaryEnsemble(CircularEnsemble):
"""
Represents Cicular Unitary Ensembles.
Examples
========
>>> from sympy.stats import CircularUnitaryEnsemble as CUE, density
>>> from sympy.stats import joint_eigen_distribution
>>> C = CUE('U', 1)
>>> joint_eigen_distribution(C)
Lambda(t[1], Product(Abs(exp(I*t[_j]) - exp(I*t[_k]))**2, (_j, _k + 1, 1), (_k, 1, 0))/(2*pi))
Note
====
As can be seen above in the example, density of CiruclarUnitaryEnsemble
is not evaluated becuase the exact definition is based on haar measure of
unitary group which is not unique.
"""
def joint_eigen_distribution(self):
return self._compute_joint_eigen_distribution(S(2))
class CircularOrthogonalEnsemble(CircularEnsemble):
"""
Represents Cicular Orthogonal Ensembles.
Examples
========
>>> from sympy.stats import CircularOrthogonalEnsemble as COE, density
>>> from sympy.stats import joint_eigen_distribution
>>> C = COE('O', 1)
>>> joint_eigen_distribution(C)
Lambda(t[1], Product(Abs(exp(I*t[_j]) - exp(I*t[_k])), (_j, _k + 1, 1), (_k, 1, 0))/(2*pi))
Note
====
As can be seen above in the example, density of CiruclarOrthogonalEnsemble
is not evaluated becuase the exact definition is based on haar measure of
unitary group which is not unique.
"""
def joint_eigen_distribution(self):
return self._compute_joint_eigen_distribution(S.One)
class CircularSymplecticEnsemble(CircularEnsemble):
"""
Represents Cicular Symplectic Ensembles.
Examples
========
>>> from sympy.stats import CircularSymplecticEnsemble as CSE, density
>>> from sympy.stats import joint_eigen_distribution
>>> C = CSE('S', 1)
>>> joint_eigen_distribution(C)
Lambda(t[1], Product(Abs(exp(I*t[_j]) - exp(I*t[_k]))**4, (_j, _k + 1, 1), (_k, 1, 0))/(2*pi))
Note
====
As can be seen above in the example, density of CiruclarSymplecticEnsemble
is not evaluated becuase the exact definition is based on haar measure of
unitary group which is not unique.
"""
def joint_eigen_distribution(self):
return self._compute_joint_eigen_distribution(S(4))
def joint_eigen_distribution(mat):
"""
For obtaining joint probability distribution
of eigen values of random matrix.
Parameters
==========
mat: RandomMatrixSymbol
The matrix symbol whose eigen values are to be considered.
Returns
=======
Lambda
Examples
========
>>> from sympy.stats import GaussianUnitaryEnsemble as GUE
>>> from sympy.stats import joint_eigen_distribution
>>> U = GUE('U', 2)
>>> joint_eigen_distribution(U)
Lambda((l[1], l[2]), exp(-l[1]**2 - l[2]**2)*Product(Abs(l[_i] - l[_j])**2, (_j, _i + 1, 2), (_i, 1, 1))/pi)
"""
if not isinstance(mat, RandomMatrixSymbol):
raise ValueError("%s is not of type, RandomMatrixSymbol."%(mat))
return mat.pspace.model.joint_eigen_distribution()
def JointEigenDistribution(mat):
"""
Creates joint distribution of eigen values of matrices with random
expressions.
Parameters
==========
mat: Matrix
The matrix under consideration
Returns
=======
JointDistributionHandmade
Examples
========
>>> from sympy.stats import Normal, JointEigenDistribution
>>> from sympy import Matrix
>>> A = [[Normal('A00', 0, 1), Normal('A01', 0, 1)],
... [Normal('A10', 0, 1), Normal('A11', 0, 1)]]
>>> JointEigenDistribution(Matrix(A))
JointDistributionHandmade(-sqrt(A00**2 - 2*A00*A11 + 4*A01*A10 + A11**2)/2
+ A00/2 + A11/2, sqrt(A00**2 - 2*A00*A11 + 4*A01*A10 + A11**2)/2 + A00/2 + A11/2)
"""
eigenvals = mat.eigenvals(multiple=True)
if any(not eigenval.has(RandomSymbol) for eigenval in set(eigenvals)):
raise ValueError("Eigen values don't have any random expression, "
"joint distribution cannot be generated.")
return JointDistributionHandmade(*eigenvals)
def level_spacing_distribution(mat):
"""
For obtaining distribution of level spacings.
Parameters
==========
mat: RandomMatrixSymbol
The random matrix symbol whose eigen values are
to be considered for finding the level spacings.
Returns
=======
Lambda
Examples
========
>>> from sympy.stats import GaussianUnitaryEnsemble as GUE
>>> from sympy.stats import level_spacing_distribution
>>> U = GUE('U', 2)
>>> level_spacing_distribution(U)
Lambda(_s, 32*_s**2*exp(-4*_s**2/pi)/pi**2)
References
==========
.. [1] https://en.wikipedia.org/wiki/Random_matrix#Distribution_of_level_spacings
"""
return mat.pspace.model.level_spacing_distribution()
|
c070ce7392e10648918e44c5f5ae26a5691dfa7e4fa59d016c8164507fd85700 | """
Finite Discrete Random Variables Module
See Also
========
sympy.stats.frv_types
sympy.stats.rv
sympy.stats.crv
"""
from __future__ import print_function, division
import random
from itertools import product
from sympy import (Basic, Symbol, cacheit, sympify, Mul,
And, Or, Tuple, Piecewise, Eq, Lambda, exp, I, Dummy, nan,
Sum, Intersection, S)
from sympy.core.containers import Dict
from sympy.core.logic import Logic
from sympy.core.relational import Relational
from sympy.sets.sets import FiniteSet
from sympy.stats.rv import (RandomDomain, ProductDomain, ConditionalDomain,
PSpace, IndependentProductPSpace, SinglePSpace, random_symbols,
sumsets, rv_subs, NamedArgsMixin, Density)
class FiniteDensity(dict):
"""
A domain with Finite Density.
"""
def __call__(self, item):
"""
Make instance of a class callable.
If item belongs to current instance of a class, return it.
Otherwise, return 0.
"""
item = sympify(item)
if item in self:
return self[item]
else:
return 0
@property
def dict(self):
"""
Return item as dictionary.
"""
return dict(self)
class FiniteDomain(RandomDomain):
"""
A domain with discrete finite support
Represented using a FiniteSet.
"""
is_Finite = True
@property
def symbols(self):
return FiniteSet(sym for sym, val in self.elements)
@property
def elements(self):
return self.args[0]
@property
def dict(self):
return FiniteSet(*[Dict(dict(el)) for el in self.elements])
def __contains__(self, other):
return other in self.elements
def __iter__(self):
return self.elements.__iter__()
def as_boolean(self):
return Or(*[And(*[Eq(sym, val) for sym, val in item]) for item in self])
class SingleFiniteDomain(FiniteDomain):
"""
A FiniteDomain over a single symbol/set
Example: The possibilities of a *single* die roll.
"""
def __new__(cls, symbol, set):
if not isinstance(set, FiniteSet) and \
not isinstance(set, Intersection):
set = FiniteSet(*set)
return Basic.__new__(cls, symbol, set)
@property
def symbol(self):
return self.args[0]
@property
def symbols(self):
return FiniteSet(self.symbol)
@property
def set(self):
return self.args[1]
@property
def elements(self):
return FiniteSet(*[frozenset(((self.symbol, elem), )) for elem in self.set])
def __iter__(self):
return (frozenset(((self.symbol, elem),)) for elem in self.set)
def __contains__(self, other):
sym, val = tuple(other)[0]
return sym == self.symbol and val in self.set
class ProductFiniteDomain(ProductDomain, FiniteDomain):
"""
A Finite domain consisting of several other FiniteDomains
Example: The possibilities of the rolls of three independent dice
"""
def __iter__(self):
proditer = product(*self.domains)
return (sumsets(items) for items in proditer)
@property
def elements(self):
return FiniteSet(*self)
class ConditionalFiniteDomain(ConditionalDomain, ProductFiniteDomain):
"""
A FiniteDomain that has been restricted by a condition
Example: The possibilities of a die roll under the condition that the
roll is even.
"""
def __new__(cls, domain, condition):
"""
Create a new instance of ConditionalFiniteDomain class
"""
if condition is True:
return domain
cond = rv_subs(condition)
return Basic.__new__(cls, domain, cond)
def _test(self, elem):
"""
Test the value. If value is boolean, return it. If value is equality
relational (two objects are equal), return it with left-hand side
being equal to right-hand side. Otherwise, raise ValueError exception.
"""
val = self.condition.xreplace(dict(elem))
if val in [True, False]:
return val
elif val.is_Equality:
return val.lhs == val.rhs
raise ValueError("Undecidable if %s" % str(val))
def __contains__(self, other):
return other in self.fulldomain and self._test(other)
def __iter__(self):
return (elem for elem in self.fulldomain if self._test(elem))
@property
def set(self):
if isinstance(self.fulldomain, SingleFiniteDomain):
return FiniteSet(*[elem for elem in self.fulldomain.set
if frozenset(((self.fulldomain.symbol, elem),)) in self])
else:
raise NotImplementedError(
"Not implemented on multi-dimensional conditional domain")
def as_boolean(self):
return FiniteDomain.as_boolean(self)
class SingleFiniteDistribution(Basic, NamedArgsMixin):
def __new__(cls, *args):
args = list(map(sympify, args))
return Basic.__new__(cls, *args)
@staticmethod
def check(*args):
pass
@property
@cacheit
def dict(self):
if self.is_symbolic:
return Density(self)
return dict((k, self.pmf(k)) for k in self.set)
def pmf(self, *args): # to be overridden by specific distribution
raise NotImplementedError()
@property
def set(self): # to be overridden by specific distribution
raise NotImplementedError()
values = property(lambda self: self.dict.values)
items = property(lambda self: self.dict.items)
is_symbolic = property(lambda self: False)
__iter__ = property(lambda self: self.dict.__iter__)
__getitem__ = property(lambda self: self.dict.__getitem__)
def __call__(self, *args):
return self.pmf(*args)
def __contains__(self, other):
return other in self.set
#=============================================
#========= Probability Space ===============
#=============================================
class FinitePSpace(PSpace):
"""
A Finite Probability Space
Represents the probabilities of a finite number of events.
"""
is_Finite = True
def __new__(cls, domain, density):
density = dict((sympify(key), sympify(val))
for key, val in density.items())
public_density = Dict(density)
obj = PSpace.__new__(cls, domain, public_density)
obj._density = density
return obj
def prob_of(self, elem):
elem = sympify(elem)
density = self._density
if isinstance(list(density.keys())[0], FiniteSet):
return density.get(elem, S.Zero)
return density.get(tuple(elem)[0][1], S.Zero)
def where(self, condition):
assert all(r.symbol in self.symbols for r in random_symbols(condition))
return ConditionalFiniteDomain(self.domain, condition)
def compute_density(self, expr):
expr = rv_subs(expr, self.values)
d = FiniteDensity()
for elem in self.domain:
val = expr.xreplace(dict(elem))
prob = self.prob_of(elem)
d[val] = d.get(val, S.Zero) + prob
return d
@cacheit
def compute_cdf(self, expr):
d = self.compute_density(expr)
cum_prob = S.Zero
cdf = []
for key in sorted(d):
prob = d[key]
cum_prob += prob
cdf.append((key, cum_prob))
return dict(cdf)
@cacheit
def sorted_cdf(self, expr, python_float=False):
cdf = self.compute_cdf(expr)
items = list(cdf.items())
sorted_items = sorted(items, key=lambda val_cumprob: val_cumprob[1])
if python_float:
sorted_items = [(v, float(cum_prob))
for v, cum_prob in sorted_items]
return sorted_items
@cacheit
def compute_characteristic_function(self, expr):
d = self.compute_density(expr)
t = Dummy('t', real=True)
return Lambda(t, sum(exp(I*k*t)*v for k,v in d.items()))
@cacheit
def compute_moment_generating_function(self, expr):
d = self.compute_density(expr)
t = Dummy('t', real=True)
return Lambda(t, sum(exp(k*t)*v for k,v in d.items()))
def compute_expectation(self, expr, rvs=None, **kwargs):
rvs = rvs or self.values
expr = rv_subs(expr, rvs)
probs = [self.prob_of(elem) for elem in self.domain]
if isinstance(expr, (Logic, Relational)):
parse_domain = [tuple(elem)[0][1] for elem in self.domain]
bools = [expr.xreplace(dict(elem)) for elem in self.domain]
else:
parse_domain = [expr.xreplace(dict(elem)) for elem in self.domain]
bools = [True for elem in self.domain]
return sum([Piecewise((prob * elem, blv), (S.Zero, True))
for prob, elem, blv in zip(probs, parse_domain, bools)])
def compute_quantile(self, expr):
cdf = self.compute_cdf(expr)
p = Dummy('p', real=True)
set = ((nan, (p < 0) | (p > 1)),)
for key, value in cdf.items():
set = set + ((key, p <= value), )
return Lambda(p, Piecewise(*set))
def probability(self, condition):
cond_symbols = frozenset(rs.symbol for rs in random_symbols(condition))
cond = rv_subs(condition)
if not cond_symbols.issubset(self.symbols):
raise ValueError("Cannot compare foreign random symbols, %s"
%(str(cond_symbols - self.symbols)))
if isinstance(condition, Relational) and \
(not cond.free_symbols.issubset(self.domain.free_symbols)):
rv = condition.lhs if isinstance(condition.rhs, Symbol) else condition.rhs
return sum(Piecewise(
(self.prob_of(elem), condition.subs(rv, list(elem)[0][1])),
(S.Zero, True)) for elem in self.domain)
return sympify(sum(self.prob_of(elem) for elem in self.where(condition)))
def conditional_space(self, condition):
domain = self.where(condition)
prob = self.probability(condition)
density = dict((key, val / prob)
for key, val in self._density.items() if domain._test(key))
return FinitePSpace(domain, density)
def sample(self):
"""
Internal sample method
Returns dictionary mapping RandomSymbol to realization value.
"""
expr = Tuple(*self.values)
cdf = self.sorted_cdf(expr, python_float=True)
x = random.uniform(0, 1)
# Find first occurrence with cumulative probability less than x
# This should be replaced with binary search
for value, cum_prob in cdf:
if x < cum_prob:
# return dictionary mapping RandomSymbols to values
return dict(list(zip(expr, value)))
assert False, "We should never have gotten to this point"
class SingleFinitePSpace(SinglePSpace, FinitePSpace):
"""
A single finite probability space
Represents the probabilities of a set of random events that can be
attributed to a single variable/symbol.
This class is implemented by many of the standard FiniteRV types such as
Die, Bernoulli, Coin, etc....
"""
@property
def domain(self):
return SingleFiniteDomain(self.symbol, self.distribution.set)
@property
def _is_symbolic(self):
"""
Helper property to check if the distribution
of the random variable is having symbolic
dimension.
"""
return self.distribution.is_symbolic
@property
def distribution(self):
return self.args[1]
def pmf(self, expr):
return self.distribution.pmf(expr)
@property
@cacheit
def _density(self):
return dict((FiniteSet((self.symbol, val)), prob)
for val, prob in self.distribution.dict.items())
@cacheit
def compute_characteristic_function(self, expr):
if self._is_symbolic:
d = self.compute_density(expr)
t = Dummy('t', real=True)
ki = Dummy('ki')
return Lambda(t, Sum(d(ki)*exp(I*ki*t), (ki, self.args[1].low, self.args[1].high)))
expr = rv_subs(expr, self.values)
return FinitePSpace(self.domain, self.distribution).compute_characteristic_function(expr)
@cacheit
def compute_moment_generating_function(self, expr):
if self._is_symbolic:
d = self.compute_density(expr)
t = Dummy('t', real=True)
ki = Dummy('ki')
return Lambda(t, Sum(d(ki)*exp(ki*t), (ki, self.args[1].low, self.args[1].high)))
expr = rv_subs(expr, self.values)
return FinitePSpace(self.domain, self.distribution).compute_moment_generating_function(expr)
def compute_quantile(self, expr):
if self._is_symbolic:
raise NotImplementedError("Computing quantile for random variables "
"with symbolic dimension because the bounds of searching the required "
"value is undetermined.")
expr = rv_subs(expr, self.values)
return FinitePSpace(self.domain, self.distribution).compute_quantile(expr)
def compute_density(self, expr):
if self._is_symbolic:
rv = list(random_symbols(expr))[0]
k = Dummy('k', integer=True)
cond = True if not isinstance(expr, (Relational, Logic)) \
else expr.subs(rv, k)
return Lambda(k,
Piecewise((self.pmf(k), And(k >= self.args[1].low,
k <= self.args[1].high, cond)), (S.Zero, True)))
expr = rv_subs(expr, self.values)
return FinitePSpace(self.domain, self.distribution).compute_density(expr)
def compute_cdf(self, expr):
if self._is_symbolic:
d = self.compute_density(expr)
k = Dummy('k')
ki = Dummy('ki')
return Lambda(k, Sum(d(ki), (ki, self.args[1].low, k)))
expr = rv_subs(expr, self.values)
return FinitePSpace(self.domain, self.distribution).compute_cdf(expr)
def compute_expectation(self, expr, rvs=None, **kwargs):
if self._is_symbolic:
rv = random_symbols(expr)[0]
k = Dummy('k', integer=True)
expr = expr.subs(rv, k)
cond = True if not isinstance(expr, (Relational, Logic)) \
else expr
func = self.pmf(k) * k if cond != True else self.pmf(k) * expr
return Sum(Piecewise((func, cond), (S.Zero, True)),
(k, self.distribution.low, self.distribution.high)).doit()
expr = rv_subs(expr, rvs)
return FinitePSpace(self.domain, self.distribution).compute_expectation(expr, rvs, **kwargs)
def probability(self, condition):
if self._is_symbolic:
#TODO: Implement the mechanism for handling queries for symbolic sized distributions.
raise NotImplementedError("Currently, probability queries are not "
"supported for random variables with symbolic sized distributions.")
condition = rv_subs(condition)
return FinitePSpace(self.domain, self.distribution).probability(condition)
def conditional_space(self, condition):
"""
This method is used for transferring the
computation to probability method because
conditional space of random variables with
symbolic dimensions is currently not possible.
"""
if self._is_symbolic:
self
domain = self.where(condition)
prob = self.probability(condition)
density = dict((key, val / prob)
for key, val in self._density.items() if domain._test(key))
return FinitePSpace(domain, density)
class ProductFinitePSpace(IndependentProductPSpace, FinitePSpace):
"""
A collection of several independent finite probability spaces
"""
@property
def domain(self):
return ProductFiniteDomain(*[space.domain for space in self.spaces])
@property
@cacheit
def _density(self):
proditer = product(*[iter(space._density.items())
for space in self.spaces])
d = {}
for items in proditer:
elems, probs = list(zip(*items))
elem = sumsets(elems)
prob = Mul(*probs)
d[elem] = d.get(elem, S.Zero) + prob
return Dict(d)
@property
@cacheit
def density(self):
return Dict(self._density)
def probability(self, condition):
return FinitePSpace.probability(self, condition)
def compute_density(self, expr):
return FinitePSpace.compute_density(self, expr)
|
31eb7f82404b1a421e1229d59cfc3866819e7f77ea25dd7cb14b827b89ac6a5b | """
Integer factorization
"""
from __future__ import print_function, division
import random
import math
from sympy.core import sympify
from sympy.core.compatibility import as_int, SYMPY_INTS, range, string_types
from sympy.core.containers import Dict
from sympy.core.evalf import bitcount
from sympy.core.expr import Expr
from sympy.core.function import Function
from sympy.core.logic import fuzzy_and
from sympy.core.mul import Mul
from sympy.core.numbers import igcd, ilcm, Rational
from sympy.core.power import integer_nthroot, Pow
from sympy.core.singleton import S
from .primetest import isprime
from .generate import sieve, primerange, nextprime
# Note: This list should be updated whenever new Mersenne primes are found.
# Refer: https://www.mersenne.org/
MERSENNE_PRIME_EXPONENTS = (2, 3, 5, 7, 13, 17, 19, 31, 61, 89, 107, 127, 521, 607, 1279, 2203,
2281, 3217, 4253, 4423, 9689, 9941, 11213, 19937, 21701, 23209, 44497, 86243, 110503, 132049,
216091, 756839, 859433, 1257787, 1398269, 2976221, 3021377, 6972593, 13466917, 20996011, 24036583,
25964951, 30402457, 32582657, 37156667, 42643801, 43112609, 57885161, 74207281, 77232917, 82589933)
small_trailing = [0] * 256
for j in range(1,8):
small_trailing[1<<j::1<<(j+1)] = [j] * (1<<(7-j))
def smoothness(n):
"""
Return the B-smooth and B-power smooth values of n.
The smoothness of n is the largest prime factor of n; the power-
smoothness is the largest divisor raised to its multiplicity.
Examples
========
>>> from sympy.ntheory.factor_ import smoothness
>>> smoothness(2**7*3**2)
(3, 128)
>>> smoothness(2**4*13)
(13, 16)
>>> smoothness(2)
(2, 2)
See Also
========
factorint, smoothness_p
"""
if n == 1:
return (1, 1) # not prime, but otherwise this causes headaches
facs = factorint(n)
return max(facs), max(m**facs[m] for m in facs)
def smoothness_p(n, m=-1, power=0, visual=None):
"""
Return a list of [m, (p, (M, sm(p + m), psm(p + m)))...]
where:
1. p**M is the base-p divisor of n
2. sm(p + m) is the smoothness of p + m (m = -1 by default)
3. psm(p + m) is the power smoothness of p + m
The list is sorted according to smoothness (default) or by power smoothness
if power=1.
The smoothness of the numbers to the left (m = -1) or right (m = 1) of a
factor govern the results that are obtained from the p +/- 1 type factoring
methods.
>>> from sympy.ntheory.factor_ import smoothness_p, factorint
>>> smoothness_p(10431, m=1)
(1, [(3, (2, 2, 4)), (19, (1, 5, 5)), (61, (1, 31, 31))])
>>> smoothness_p(10431)
(-1, [(3, (2, 2, 2)), (19, (1, 3, 9)), (61, (1, 5, 5))])
>>> smoothness_p(10431, power=1)
(-1, [(3, (2, 2, 2)), (61, (1, 5, 5)), (19, (1, 3, 9))])
If visual=True then an annotated string will be returned:
>>> print(smoothness_p(21477639576571, visual=1))
p**i=4410317**1 has p-1 B=1787, B-pow=1787
p**i=4869863**1 has p-1 B=2434931, B-pow=2434931
This string can also be generated directly from a factorization dictionary
and vice versa:
>>> factorint(17*9)
{3: 2, 17: 1}
>>> smoothness_p(_)
'p**i=3**2 has p-1 B=2, B-pow=2\\np**i=17**1 has p-1 B=2, B-pow=16'
>>> smoothness_p(_)
{3: 2, 17: 1}
The table of the output logic is:
====== ====== ======= =======
| Visual
------ ----------------------
Input True False other
====== ====== ======= =======
dict str tuple str
str str tuple dict
tuple str tuple str
n str tuple tuple
mul str tuple tuple
====== ====== ======= =======
See Also
========
factorint, smoothness
"""
from sympy.utilities import flatten
# visual must be True, False or other (stored as None)
if visual in (1, 0):
visual = bool(visual)
elif visual not in (True, False):
visual = None
if isinstance(n, string_types):
if visual:
return n
d = {}
for li in n.splitlines():
k, v = [int(i) for i in
li.split('has')[0].split('=')[1].split('**')]
d[k] = v
if visual is not True and visual is not False:
return d
return smoothness_p(d, visual=False)
elif type(n) is not tuple:
facs = factorint(n, visual=False)
if power:
k = -1
else:
k = 1
if type(n) is not tuple:
rv = (m, sorted([(f,
tuple([M] + list(smoothness(f + m))))
for f, M in [i for i in facs.items()]],
key=lambda x: (x[1][k], x[0])))
else:
rv = n
if visual is False or (visual is not True) and (type(n) in [int, Mul]):
return rv
lines = []
for dat in rv[1]:
dat = flatten(dat)
dat.insert(2, m)
lines.append('p**i=%i**%i has p%+i B=%i, B-pow=%i' % tuple(dat))
return '\n'.join(lines)
def trailing(n):
"""Count the number of trailing zero digits in the binary
representation of n, i.e. determine the largest power of 2
that divides n.
Examples
========
>>> from sympy import trailing
>>> trailing(128)
7
>>> trailing(63)
0
"""
n = abs(int(n))
if not n:
return 0
low_byte = n & 0xff
if low_byte:
return small_trailing[low_byte]
# 2**m is quick for z up through 2**30
z = bitcount(n) - 1
if isinstance(z, SYMPY_INTS):
if n == 1 << z:
return z
if z < 300:
# fixed 8-byte reduction
t = 8
n >>= 8
while not n & 0xff:
n >>= 8
t += 8
return t + small_trailing[n & 0xff]
# binary reduction important when there might be a large
# number of trailing 0s
t = 0
p = 8
while not n & 1:
while not n & ((1 << p) - 1):
n >>= p
t += p
p *= 2
p //= 2
return t
def multiplicity(p, n):
"""
Find the greatest integer m such that p**m divides n.
Examples
========
>>> from sympy.ntheory import multiplicity
>>> from sympy.core.numbers import Rational as R
>>> [multiplicity(5, n) for n in [8, 5, 25, 125, 250]]
[0, 1, 2, 3, 3]
>>> multiplicity(3, R(1, 9))
-2
"""
try:
p, n = as_int(p), as_int(n)
except ValueError:
if all(isinstance(i, (SYMPY_INTS, Rational)) for i in (p, n)):
p = Rational(p)
n = Rational(n)
if p.q == 1:
if n.p == 1:
return -multiplicity(p.p, n.q)
return multiplicity(p.p, n.p) - multiplicity(p.p, n.q)
elif p.p == 1:
return multiplicity(p.q, n.q)
else:
like = min(
multiplicity(p.p, n.p),
multiplicity(p.q, n.q))
cross = min(
multiplicity(p.q, n.p),
multiplicity(p.p, n.q))
return like - cross
raise ValueError('expecting ints or fractions, got %s and %s' % (p, n))
if n == 0:
raise ValueError('no such integer exists: multiplicity of %s is not-defined' %(n))
if p == 2:
return trailing(n)
if p < 2:
raise ValueError('p must be an integer, 2 or larger, but got %s' % p)
if p == n:
return 1
m = 0
n, rem = divmod(n, p)
while not rem:
m += 1
if m > 5:
# The multiplicity could be very large. Better
# to increment in powers of two
e = 2
while 1:
ppow = p**e
if ppow < n:
nnew, rem = divmod(n, ppow)
if not rem:
m += e
e *= 2
n = nnew
continue
return m + multiplicity(p, n)
n, rem = divmod(n, p)
return m
def perfect_power(n, candidates=None, big=True, factor=True):
"""
Return ``(b, e)`` such that ``n`` == ``b**e`` if ``n`` is a
perfect power with ``e > 1``, else ``False``. A ValueError is
raised if ``n`` is not an integer or is not positive.
By default, the base is recursively decomposed and the exponents
collected so the largest possible ``e`` is sought. If ``big=False``
then the smallest possible ``e`` (thus prime) will be chosen.
If ``factor=True`` then simultaneous factorization of ``n`` is
attempted since finding a factor indicates the only possible root
for ``n``. This is True by default since only a few small factors will
be tested in the course of searching for the perfect power.
The use of ``candidates`` is primarily for internal use; if provided,
False will be returned if ``n`` cannot be written as a power with one
of the candidates as an exponent and factoring (beyond testing for
a factor of 2) will not be attempted.
Examples
========
>>> from sympy import perfect_power
>>> perfect_power(16)
(2, 4)
>>> perfect_power(16, big=False)
(4, 2)
Notes
=====
To know whether an integer is a perfect power of 2 use
>>> is2pow = lambda n: bool(n and not n & (n - 1))
>>> [(i, is2pow(i)) for i in range(5)]
[(0, False), (1, True), (2, True), (3, False), (4, True)]
It is not necessary to provide ``candidates``. When provided
it will be assumed that they are ints. The first one that is
larger than the computed maximum possible exponent will signal
failure for the routine.
>>> perfect_power(3**8, [9])
False
>>> perfect_power(3**8, [2, 4, 8])
(3, 8)
>>> perfect_power(3**8, [4, 8], big=False)
(9, 4)
See Also
========
sympy.core.power.integer_nthroot
primetest.is_square
"""
from sympy.core.power import integer_nthroot
n = as_int(n)
if n < 3:
if n < 1:
raise ValueError('expecting positive n')
return False
logn = math.log(n, 2)
max_possible = int(logn) + 2 # only check values less than this
not_square = n % 10 in [2, 3, 7, 8] # squares cannot end in 2, 3, 7, 8
min_possible = 2 + not_square
if not candidates:
candidates = primerange(min_possible, max_possible)
else:
candidates = sorted([i for i in candidates
if min_possible <= i < max_possible])
if n%2 == 0:
e = trailing(n)
candidates = [i for i in candidates if e%i == 0]
if big:
candidates = reversed(candidates)
for e in candidates:
r, ok = integer_nthroot(n, e)
if ok:
return (r, e)
return False
def _factors():
rv = 2 + n % 2
while True:
yield rv
rv = nextprime(rv)
for fac, e in zip(_factors(), candidates):
# see if there is a factor present
if factor and n % fac == 0:
# find what the potential power is
if fac == 2:
e = trailing(n)
else:
e = multiplicity(fac, n)
# if it's a trivial power we are done
if e == 1:
return False
# maybe the e-th root of n is exact
r, exact = integer_nthroot(n, e)
if not exact:
# Having a factor, we know that e is the maximal
# possible value for a root of n.
# If n = fac**e*m can be written as a perfect
# power then see if m can be written as r**E where
# gcd(e, E) != 1 so n = (fac**(e//E)*r)**E
m = n//fac**e
rE = perfect_power(m, candidates=divisors(e, generator=True))
if not rE:
return False
else:
r, E = rE
r, e = fac**(e//E)*r, E
if not big:
e0 = primefactors(e)
if e0[0] != e:
r, e = r**(e//e0[0]), e0[0]
return r, e
# Weed out downright impossible candidates
if logn/e < 40:
b = 2.0**(logn/e)
if abs(int(b + 0.5) - b) > 0.01:
continue
# now see if the plausible e makes a perfect power
r, exact = integer_nthroot(n, e)
if exact:
if big:
m = perfect_power(r, big=big, factor=factor)
if m:
r, e = m[0], e*m[1]
return int(r), e
return False
def pollard_rho(n, s=2, a=1, retries=5, seed=1234, max_steps=None, F=None):
r"""
Use Pollard's rho method to try to extract a nontrivial factor
of ``n``. The returned factor may be a composite number. If no
factor is found, ``None`` is returned.
The algorithm generates pseudo-random values of x with a generator
function, replacing x with F(x). If F is not supplied then the
function x**2 + ``a`` is used. The first value supplied to F(x) is ``s``.
Upon failure (if ``retries`` is > 0) a new ``a`` and ``s`` will be
supplied; the ``a`` will be ignored if F was supplied.
The sequence of numbers generated by such functions generally have a
a lead-up to some number and then loop around back to that number and
begin to repeat the sequence, e.g. 1, 2, 3, 4, 5, 3, 4, 5 -- this leader
and loop look a bit like the Greek letter rho, and thus the name, 'rho'.
For a given function, very different leader-loop values can be obtained
so it is a good idea to allow for retries:
>>> from sympy.ntheory.generate import cycle_length
>>> n = 16843009
>>> F = lambda x:(2048*pow(x, 2, n) + 32767) % n
>>> for s in range(5):
... print('loop length = %4i; leader length = %3i' % next(cycle_length(F, s)))
...
loop length = 2489; leader length = 42
loop length = 78; leader length = 120
loop length = 1482; leader length = 99
loop length = 1482; leader length = 285
loop length = 1482; leader length = 100
Here is an explicit example where there is a two element leadup to
a sequence of 3 numbers (11, 14, 4) that then repeat:
>>> x=2
>>> for i in range(9):
... x=(x**2+12)%17
... print(x)
...
16
13
11
14
4
11
14
4
11
>>> next(cycle_length(lambda x: (x**2+12)%17, 2))
(3, 2)
>>> list(cycle_length(lambda x: (x**2+12)%17, 2, values=True))
[16, 13, 11, 14, 4]
Instead of checking the differences of all generated values for a gcd
with n, only the kth and 2*kth numbers are checked, e.g. 1st and 2nd,
2nd and 4th, 3rd and 6th until it has been detected that the loop has been
traversed. Loops may be many thousands of steps long before rho finds a
factor or reports failure. If ``max_steps`` is specified, the iteration
is cancelled with a failure after the specified number of steps.
Examples
========
>>> from sympy import pollard_rho
>>> n=16843009
>>> F=lambda x:(2048*pow(x,2,n) + 32767) % n
>>> pollard_rho(n, F=F)
257
Use the default setting with a bad value of ``a`` and no retries:
>>> pollard_rho(n, a=n-2, retries=0)
If retries is > 0 then perhaps the problem will correct itself when
new values are generated for a:
>>> pollard_rho(n, a=n-2, retries=1)
257
References
==========
.. [1] Richard Crandall & Carl Pomerance (2005), "Prime Numbers:
A Computational Perspective", Springer, 2nd edition, 229-231
"""
n = int(n)
if n < 5:
raise ValueError('pollard_rho should receive n > 4')
prng = random.Random(seed + retries)
V = s
for i in range(retries + 1):
U = V
if not F:
F = lambda x: (pow(x, 2, n) + a) % n
j = 0
while 1:
if max_steps and (j > max_steps):
break
j += 1
U = F(U)
V = F(F(V)) # V is 2x further along than U
g = igcd(U - V, n)
if g == 1:
continue
if g == n:
break
return int(g)
V = prng.randint(0, n - 1)
a = prng.randint(1, n - 3) # for x**2 + a, a%n should not be 0 or -2
F = None
return None
def pollard_pm1(n, B=10, a=2, retries=0, seed=1234):
"""
Use Pollard's p-1 method to try to extract a nontrivial factor
of ``n``. Either a divisor (perhaps composite) or ``None`` is returned.
The value of ``a`` is the base that is used in the test gcd(a**M - 1, n).
The default is 2. If ``retries`` > 0 then if no factor is found after the
first attempt, a new ``a`` will be generated randomly (using the ``seed``)
and the process repeated.
Note: the value of M is lcm(1..B) = reduce(ilcm, range(2, B + 1)).
A search is made for factors next to even numbers having a power smoothness
less than ``B``. Choosing a larger B increases the likelihood of finding a
larger factor but takes longer. Whether a factor of n is found or not
depends on ``a`` and the power smoothness of the even number just less than
the factor p (hence the name p - 1).
Although some discussion of what constitutes a good ``a`` some
descriptions are hard to interpret. At the modular.math site referenced
below it is stated that if gcd(a**M - 1, n) = N then a**M % q**r is 1
for every prime power divisor of N. But consider the following:
>>> from sympy.ntheory.factor_ import smoothness_p, pollard_pm1
>>> n=257*1009
>>> smoothness_p(n)
(-1, [(257, (1, 2, 256)), (1009, (1, 7, 16))])
So we should (and can) find a root with B=16:
>>> pollard_pm1(n, B=16, a=3)
1009
If we attempt to increase B to 256 we find that it doesn't work:
>>> pollard_pm1(n, B=256)
>>>
But if the value of ``a`` is changed we find that only multiples of
257 work, e.g.:
>>> pollard_pm1(n, B=256, a=257)
1009
Checking different ``a`` values shows that all the ones that didn't
work had a gcd value not equal to ``n`` but equal to one of the
factors:
>>> from sympy.core.numbers import ilcm, igcd
>>> from sympy import factorint, Pow
>>> M = 1
>>> for i in range(2, 256):
... M = ilcm(M, i)
...
>>> set([igcd(pow(a, M, n) - 1, n) for a in range(2, 256) if
... igcd(pow(a, M, n) - 1, n) != n])
{1009}
But does aM % d for every divisor of n give 1?
>>> aM = pow(255, M, n)
>>> [(d, aM%Pow(*d.args)) for d in factorint(n, visual=True).args]
[(257**1, 1), (1009**1, 1)]
No, only one of them. So perhaps the principle is that a root will
be found for a given value of B provided that:
1) the power smoothness of the p - 1 value next to the root
does not exceed B
2) a**M % p != 1 for any of the divisors of n.
By trying more than one ``a`` it is possible that one of them
will yield a factor.
Examples
========
With the default smoothness bound, this number can't be cracked:
>>> from sympy.ntheory import pollard_pm1, primefactors
>>> pollard_pm1(21477639576571)
Increasing the smoothness bound helps:
>>> pollard_pm1(21477639576571, B=2000)
4410317
Looking at the smoothness of the factors of this number we find:
>>> from sympy.utilities import flatten
>>> from sympy.ntheory.factor_ import smoothness_p, factorint
>>> print(smoothness_p(21477639576571, visual=1))
p**i=4410317**1 has p-1 B=1787, B-pow=1787
p**i=4869863**1 has p-1 B=2434931, B-pow=2434931
The B and B-pow are the same for the p - 1 factorizations of the divisors
because those factorizations had a very large prime factor:
>>> factorint(4410317 - 1)
{2: 2, 617: 1, 1787: 1}
>>> factorint(4869863-1)
{2: 1, 2434931: 1}
Note that until B reaches the B-pow value of 1787, the number is not cracked;
>>> pollard_pm1(21477639576571, B=1786)
>>> pollard_pm1(21477639576571, B=1787)
4410317
The B value has to do with the factors of the number next to the divisor,
not the divisors themselves. A worst case scenario is that the number next
to the factor p has a large prime divisisor or is a perfect power. If these
conditions apply then the power-smoothness will be about p/2 or p. The more
realistic is that there will be a large prime factor next to p requiring
a B value on the order of p/2. Although primes may have been searched for
up to this level, the p/2 is a factor of p - 1, something that we don't
know. The modular.math reference below states that 15% of numbers in the
range of 10**15 to 15**15 + 10**4 are 10**6 power smooth so a B of 10**6
will fail 85% of the time in that range. From 10**8 to 10**8 + 10**3 the
percentages are nearly reversed...but in that range the simple trial
division is quite fast.
References
==========
.. [1] Richard Crandall & Carl Pomerance (2005), "Prime Numbers:
A Computational Perspective", Springer, 2nd edition, 236-238
.. [2] http://modular.math.washington.edu/edu/2007/spring/ent/ent-html/node81.html
.. [3] https://www.cs.toronto.edu/~yuvalf/Factorization.pdf
"""
n = int(n)
if n < 4 or B < 3:
raise ValueError('pollard_pm1 should receive n > 3 and B > 2')
prng = random.Random(seed + B)
# computing a**lcm(1,2,3,..B) % n for B > 2
# it looks weird, but it's right: primes run [2, B]
# and the answer's not right until the loop is done.
for i in range(retries + 1):
aM = a
for p in sieve.primerange(2, B + 1):
e = int(math.log(B, p))
aM = pow(aM, pow(p, e), n)
g = igcd(aM - 1, n)
if 1 < g < n:
return int(g)
# get a new a:
# since the exponent, lcm(1..B), is even, if we allow 'a' to be 'n-1'
# then (n - 1)**even % n will be 1 which will give a g of 0 and 1 will
# give a zero, too, so we set the range as [2, n-2]. Some references
# say 'a' should be coprime to n, but either will detect factors.
a = prng.randint(2, n - 2)
def _trial(factors, n, candidates, verbose=False):
"""
Helper function for integer factorization. Trial factors ``n`
against all integers given in the sequence ``candidates``
and updates the dict ``factors`` in-place. Returns the reduced
value of ``n`` and a flag indicating whether any factors were found.
"""
if verbose:
factors0 = list(factors.keys())
nfactors = len(factors)
for d in candidates:
if n % d == 0:
m = multiplicity(d, n)
n //= d**m
factors[d] = m
if verbose:
for k in sorted(set(factors).difference(set(factors0))):
print(factor_msg % (k, factors[k]))
return int(n), len(factors) != nfactors
def _check_termination(factors, n, limitp1, use_trial, use_rho, use_pm1,
verbose):
"""
Helper function for integer factorization. Checks if ``n``
is a prime or a perfect power, and in those cases updates
the factorization and raises ``StopIteration``.
"""
if verbose:
print('Check for termination')
# since we've already been factoring there is no need to do
# simultaneous factoring with the power check
p = perfect_power(n, factor=False)
if p is not False:
base, exp = p
if limitp1:
limit = limitp1 - 1
else:
limit = limitp1
facs = factorint(base, limit, use_trial, use_rho, use_pm1,
verbose=False)
for b, e in facs.items():
if verbose:
print(factor_msg % (b, e))
factors[b] = exp*e
raise StopIteration
if isprime(n):
factors[int(n)] = 1
raise StopIteration
if n == 1:
raise StopIteration
trial_int_msg = "Trial division with ints [%i ... %i] and fail_max=%i"
trial_msg = "Trial division with primes [%i ... %i]"
rho_msg = "Pollard's rho with retries %i, max_steps %i and seed %i"
pm1_msg = "Pollard's p-1 with smoothness bound %i and seed %i"
factor_msg = '\t%i ** %i'
fermat_msg = 'Close factors satisying Fermat condition found.'
complete_msg = 'Factorization is complete.'
def _factorint_small(factors, n, limit, fail_max):
"""
Return the value of n and either a 0 (indicating that factorization up
to the limit was complete) or else the next near-prime that would have
been tested.
Factoring stops if there are fail_max unsuccessful tests in a row.
If factors of n were found they will be in the factors dictionary as
{factor: multiplicity} and the returned value of n will have had those
factors removed. The factors dictionary is modified in-place.
"""
def done(n, d):
"""return n, d if the sqrt(n) wasn't reached yet, else
n, 0 indicating that factoring is done.
"""
if d*d <= n:
return n, d
return n, 0
d = 2
m = trailing(n)
if m:
factors[d] = m
n >>= m
d = 3
if limit < d:
if n > 1:
factors[n] = 1
return done(n, d)
# reduce
m = 0
while n % d == 0:
n //= d
m += 1
if m == 20:
mm = multiplicity(d, n)
m += mm
n //= d**mm
break
if m:
factors[d] = m
# when d*d exceeds maxx or n we are done; if limit**2 is greater
# than n then maxx is set to zero so the value of n will flag the finish
if limit*limit > n:
maxx = 0
else:
maxx = limit*limit
dd = maxx or n
d = 5
fails = 0
while fails < fail_max:
if d*d > dd:
break
# d = 6*i - 1
# reduce
m = 0
while n % d == 0:
n //= d
m += 1
if m == 20:
mm = multiplicity(d, n)
m += mm
n //= d**mm
break
if m:
factors[d] = m
dd = maxx or n
fails = 0
else:
fails += 1
d += 2
if d*d > dd:
break
# d = 6*i - 1
# reduce
m = 0
while n % d == 0:
n //= d
m += 1
if m == 20:
mm = multiplicity(d, n)
m += mm
n //= d**mm
break
if m:
factors[d] = m
dd = maxx or n
fails = 0
else:
fails += 1
# d = 6*(i + 1) - 1
d += 4
return done(n, d)
def factorint(n, limit=None, use_trial=True, use_rho=True, use_pm1=True,
verbose=False, visual=None, multiple=False):
r"""
Given a positive integer ``n``, ``factorint(n)`` returns a dict containing
the prime factors of ``n`` as keys and their respective multiplicities
as values. For example:
>>> from sympy.ntheory import factorint
>>> factorint(2000) # 2000 = (2**4) * (5**3)
{2: 4, 5: 3}
>>> factorint(65537) # This number is prime
{65537: 1}
For input less than 2, factorint behaves as follows:
- ``factorint(1)`` returns the empty factorization, ``{}``
- ``factorint(0)`` returns ``{0:1}``
- ``factorint(-n)`` adds ``-1:1`` to the factors and then factors ``n``
Partial Factorization:
If ``limit`` (> 3) is specified, the search is stopped after performing
trial division up to (and including) the limit (or taking a
corresponding number of rho/p-1 steps). This is useful if one has
a large number and only is interested in finding small factors (if
any). Note that setting a limit does not prevent larger factors
from being found early; it simply means that the largest factor may
be composite. Since checking for perfect power is relatively cheap, it is
done regardless of the limit setting.
This number, for example, has two small factors and a huge
semi-prime factor that cannot be reduced easily:
>>> from sympy.ntheory import isprime
>>> from sympy.core.compatibility import long
>>> a = 1407633717262338957430697921446883
>>> f = factorint(a, limit=10000)
>>> f == {991: 1, long(202916782076162456022877024859): 1, 7: 1}
True
>>> isprime(max(f))
False
This number has a small factor and a residual perfect power whose
base is greater than the limit:
>>> factorint(3*101**7, limit=5)
{3: 1, 101: 7}
List of Factors:
If ``multiple`` is set to ``True`` then a list containing the
prime factors including multiplicities is returned.
>>> factorint(24, multiple=True)
[2, 2, 2, 3]
Visual Factorization:
If ``visual`` is set to ``True``, then it will return a visual
factorization of the integer. For example:
>>> from sympy import pprint
>>> pprint(factorint(4200, visual=True))
3 1 2 1
2 *3 *5 *7
Note that this is achieved by using the evaluate=False flag in Mul
and Pow. If you do other manipulations with an expression where
evaluate=False, it may evaluate. Therefore, you should use the
visual option only for visualization, and use the normal dictionary
returned by visual=False if you want to perform operations on the
factors.
You can easily switch between the two forms by sending them back to
factorint:
>>> from sympy import Mul, Pow
>>> regular = factorint(1764); regular
{2: 2, 3: 2, 7: 2}
>>> pprint(factorint(regular))
2 2 2
2 *3 *7
>>> visual = factorint(1764, visual=True); pprint(visual)
2 2 2
2 *3 *7
>>> print(factorint(visual))
{2: 2, 3: 2, 7: 2}
If you want to send a number to be factored in a partially factored form
you can do so with a dictionary or unevaluated expression:
>>> factorint(factorint({4: 2, 12: 3})) # twice to toggle to dict form
{2: 10, 3: 3}
>>> factorint(Mul(4, 12, evaluate=False))
{2: 4, 3: 1}
The table of the output logic is:
====== ====== ======= =======
Visual
------ ----------------------
Input True False other
====== ====== ======= =======
dict mul dict mul
n mul dict dict
mul mul dict dict
====== ====== ======= =======
Notes
=====
Algorithm:
The function switches between multiple algorithms. Trial division
quickly finds small factors (of the order 1-5 digits), and finds
all large factors if given enough time. The Pollard rho and p-1
algorithms are used to find large factors ahead of time; they
will often find factors of the order of 10 digits within a few
seconds:
>>> factors = factorint(12345678910111213141516)
>>> for base, exp in sorted(factors.items()):
... print('%s %s' % (base, exp))
...
2 2
2507191691 1
1231026625769 1
Any of these methods can optionally be disabled with the following
boolean parameters:
- ``use_trial``: Toggle use of trial division
- ``use_rho``: Toggle use of Pollard's rho method
- ``use_pm1``: Toggle use of Pollard's p-1 method
``factorint`` also periodically checks if the remaining part is
a prime number or a perfect power, and in those cases stops.
For unevaluated factorial, it uses Legendre's formula(theorem).
If ``verbose`` is set to ``True``, detailed progress is printed.
See Also
========
smoothness, smoothness_p, divisors
"""
if isinstance(n, Dict):
n = dict(n)
if multiple:
fac = factorint(n, limit=limit, use_trial=use_trial,
use_rho=use_rho, use_pm1=use_pm1,
verbose=verbose, visual=False, multiple=False)
factorlist = sum(([p] * fac[p] if fac[p] > 0 else [S.One/p]*(-fac[p])
for p in sorted(fac)), [])
return factorlist
factordict = {}
if visual and not isinstance(n, Mul) and not isinstance(n, dict):
factordict = factorint(n, limit=limit, use_trial=use_trial,
use_rho=use_rho, use_pm1=use_pm1,
verbose=verbose, visual=False)
elif isinstance(n, Mul):
factordict = {int(k): int(v) for k, v in
n.as_powers_dict().items()}
elif isinstance(n, dict):
factordict = n
if factordict and (isinstance(n, Mul) or isinstance(n, dict)):
# check it
for key in list(factordict.keys()):
if isprime(key):
continue
e = factordict.pop(key)
d = factorint(key, limit=limit, use_trial=use_trial, use_rho=use_rho,
use_pm1=use_pm1, verbose=verbose, visual=False)
for k, v in d.items():
if k in factordict:
factordict[k] += v*e
else:
factordict[k] = v*e
if visual or (type(n) is dict and
visual is not True and
visual is not False):
if factordict == {}:
return S.One
if -1 in factordict:
factordict.pop(-1)
args = [S.NegativeOne]
else:
args = []
args.extend([Pow(*i, evaluate=False)
for i in sorted(factordict.items())])
return Mul(*args, evaluate=False)
elif isinstance(n, dict) or isinstance(n, Mul):
return factordict
assert use_trial or use_rho or use_pm1
from sympy.functions.combinatorial.factorials import factorial
if isinstance(n, factorial):
x = as_int(n.args[0])
if x >= 20:
factors = {}
m = 2 # to initialize the if condition below
for p in sieve.primerange(2, x + 1):
if m > 1:
m, q = 0, x // p
while q != 0:
m += q
q //= p
factors[p] = m
if factors and verbose:
for k in sorted(factors):
print(factor_msg % (k, factors[k]))
if verbose:
print(complete_msg)
return factors
else:
# if n < 20!, direct computation is faster
# since it uses a lookup table
n = n.func(x)
n = as_int(n)
if limit:
limit = int(limit)
# special cases
if n < 0:
factors = factorint(
-n, limit=limit, use_trial=use_trial, use_rho=use_rho,
use_pm1=use_pm1, verbose=verbose, visual=False)
factors[-1] = 1
return factors
if limit and limit < 2:
if n == 1:
return {}
return {n: 1}
elif n < 10:
# doing this we are assured of getting a limit > 2
# when we have to compute it later
return [{0: 1}, {}, {2: 1}, {3: 1}, {2: 2}, {5: 1},
{2: 1, 3: 1}, {7: 1}, {2: 3}, {3: 2}][n]
factors = {}
# do simplistic factorization
if verbose:
sn = str(n)
if len(sn) > 50:
print('Factoring %s' % sn[:5] + \
'..(%i other digits)..' % (len(sn) - 10) + sn[-5:])
else:
print('Factoring', n)
if use_trial:
# this is the preliminary factorization for small factors
small = 2**15
fail_max = 600
small = min(small, limit or small)
if verbose:
print(trial_int_msg % (2, small, fail_max))
n, next_p = _factorint_small(factors, n, small, fail_max)
else:
next_p = 2
if factors and verbose:
for k in sorted(factors):
print(factor_msg % (k, factors[k]))
if next_p == 0:
if n > 1:
factors[int(n)] = 1
if verbose:
print(complete_msg)
return factors
# continue with more advanced factorization methods
# first check if the simplistic run didn't finish
# because of the limit and check for a perfect
# power before exiting
try:
if limit and next_p > limit:
if verbose:
print('Exceeded limit:', limit)
_check_termination(factors, n, limit, use_trial, use_rho, use_pm1,
verbose)
if n > 1:
factors[int(n)] = 1
return factors
else:
# Before quitting (or continuing on)...
# ...do a Fermat test since it's so easy and we need the
# square root anyway. Finding 2 factors is easy if they are
# "close enough." This is the big root equivalent of dividing by
# 2, 3, 5.
sqrt_n = integer_nthroot(n, 2)[0]
a = sqrt_n + 1
a2 = a**2
b2 = a2 - n
for i in range(3):
b, fermat = integer_nthroot(b2, 2)
if fermat:
break
b2 += 2*a + 1 # equiv to (a + 1)**2 - n
a += 1
if fermat:
if verbose:
print(fermat_msg)
if limit:
limit -= 1
for r in [a - b, a + b]:
facs = factorint(r, limit=limit, use_trial=use_trial,
use_rho=use_rho, use_pm1=use_pm1,
verbose=verbose)
factors.update(facs)
raise StopIteration
# ...see if factorization can be terminated
_check_termination(factors, n, limit, use_trial, use_rho, use_pm1,
verbose)
except StopIteration:
if verbose:
print(complete_msg)
return factors
# these are the limits for trial division which will
# be attempted in parallel with pollard methods
low, high = next_p, 2*next_p
limit = limit or sqrt_n
# add 1 to make sure limit is reached in primerange calls
limit += 1
while 1:
try:
high_ = high
if limit < high_:
high_ = limit
# Trial division
if use_trial:
if verbose:
print(trial_msg % (low, high_))
ps = sieve.primerange(low, high_)
n, found_trial = _trial(factors, n, ps, verbose)
if found_trial:
_check_termination(factors, n, limit, use_trial, use_rho,
use_pm1, verbose)
else:
found_trial = False
if high > limit:
if verbose:
print('Exceeded limit:', limit)
if n > 1:
factors[int(n)] = 1
raise StopIteration
# Only used advanced methods when no small factors were found
if not found_trial:
if (use_pm1 or use_rho):
high_root = max(int(math.log(high_**0.7)), low, 3)
# Pollard p-1
if use_pm1:
if verbose:
print(pm1_msg % (high_root, high_))
c = pollard_pm1(n, B=high_root, seed=high_)
if c:
# factor it and let _trial do the update
ps = factorint(c, limit=limit - 1,
use_trial=use_trial,
use_rho=use_rho,
use_pm1=use_pm1,
verbose=verbose)
n, _ = _trial(factors, n, ps, verbose=False)
_check_termination(factors, n, limit, use_trial,
use_rho, use_pm1, verbose)
# Pollard rho
if use_rho:
max_steps = high_root
if verbose:
print(rho_msg % (1, max_steps, high_))
c = pollard_rho(n, retries=1, max_steps=max_steps,
seed=high_)
if c:
# factor it and let _trial do the update
ps = factorint(c, limit=limit - 1,
use_trial=use_trial,
use_rho=use_rho,
use_pm1=use_pm1,
verbose=verbose)
n, _ = _trial(factors, n, ps, verbose=False)
_check_termination(factors, n, limit, use_trial,
use_rho, use_pm1, verbose)
except StopIteration:
if verbose:
print(complete_msg)
return factors
low, high = high, high*2
def factorrat(rat, limit=None, use_trial=True, use_rho=True, use_pm1=True,
verbose=False, visual=None, multiple=False):
r"""
Given a Rational ``r``, ``factorrat(r)`` returns a dict containing
the prime factors of ``r`` as keys and their respective multiplicities
as values. For example:
>>> from sympy.ntheory import factorrat
>>> from sympy.core.symbol import S
>>> factorrat(S(8)/9) # 8/9 = (2**3) * (3**-2)
{2: 3, 3: -2}
>>> factorrat(S(-1)/987) # -1/789 = -1 * (3**-1) * (7**-1) * (47**-1)
{-1: 1, 3: -1, 7: -1, 47: -1}
Please see the docstring for ``factorint`` for detailed explanations
and examples of the following keywords:
- ``limit``: Integer limit up to which trial division is done
- ``use_trial``: Toggle use of trial division
- ``use_rho``: Toggle use of Pollard's rho method
- ``use_pm1``: Toggle use of Pollard's p-1 method
- ``verbose``: Toggle detailed printing of progress
- ``multiple``: Toggle returning a list of factors or dict
- ``visual``: Toggle product form of output
"""
from collections import defaultdict
if multiple:
fac = factorrat(rat, limit=limit, use_trial=use_trial,
use_rho=use_rho, use_pm1=use_pm1,
verbose=verbose, visual=False, multiple=False)
factorlist = sum(([p] * fac[p] if fac[p] > 0 else [S.One/p]*(-fac[p])
for p, _ in sorted(fac.items(),
key=lambda elem: elem[0]
if elem[1] > 0
else 1/elem[0])), [])
return factorlist
f = factorint(rat.p, limit=limit, use_trial=use_trial,
use_rho=use_rho, use_pm1=use_pm1,
verbose=verbose).copy()
f = defaultdict(int, f)
for p, e in factorint(rat.q, limit=limit,
use_trial=use_trial,
use_rho=use_rho,
use_pm1=use_pm1,
verbose=verbose).items():
f[p] += -e
if len(f) > 1 and 1 in f:
del f[1]
if not visual:
return dict(f)
else:
if -1 in f:
f.pop(-1)
args = [S.NegativeOne]
else:
args = []
args.extend([Pow(*i, evaluate=False)
for i in sorted(f.items())])
return Mul(*args, evaluate=False)
def primefactors(n, limit=None, verbose=False):
"""Return a sorted list of n's prime factors, ignoring multiplicity
and any composite factor that remains if the limit was set too low
for complete factorization. Unlike factorint(), primefactors() does
not return -1 or 0.
Examples
========
>>> from sympy.ntheory import primefactors, factorint, isprime
>>> primefactors(6)
[2, 3]
>>> primefactors(-5)
[5]
>>> sorted(factorint(123456).items())
[(2, 6), (3, 1), (643, 1)]
>>> primefactors(123456)
[2, 3, 643]
>>> sorted(factorint(10000000001, limit=200).items())
[(101, 1), (99009901, 1)]
>>> isprime(99009901)
False
>>> primefactors(10000000001, limit=300)
[101]
See Also
========
divisors
"""
n = int(n)
factors = sorted(factorint(n, limit=limit, verbose=verbose).keys())
s = [f for f in factors[:-1:] if f not in [-1, 0, 1]]
if factors and isprime(factors[-1]):
s += [factors[-1]]
return s
def _divisors(n):
"""Helper function for divisors which generates the divisors."""
factordict = factorint(n)
ps = sorted(factordict.keys())
def rec_gen(n=0):
if n == len(ps):
yield 1
else:
pows = [1]
for j in range(factordict[ps[n]]):
pows.append(pows[-1] * ps[n])
for q in rec_gen(n + 1):
for p in pows:
yield p * q
for p in rec_gen():
yield p
def divisors(n, generator=False):
r"""
Return all divisors of n sorted from 1..n by default.
If generator is ``True`` an unordered generator is returned.
The number of divisors of n can be quite large if there are many
prime factors (counting repeated factors). If only the number of
factors is desired use divisor_count(n).
Examples
========
>>> from sympy import divisors, divisor_count
>>> divisors(24)
[1, 2, 3, 4, 6, 8, 12, 24]
>>> divisor_count(24)
8
>>> list(divisors(120, generator=True))
[1, 2, 4, 8, 3, 6, 12, 24, 5, 10, 20, 40, 15, 30, 60, 120]
Notes
=====
This is a slightly modified version of Tim Peters referenced at:
https://stackoverflow.com/questions/1010381/python-factorization
See Also
========
primefactors, factorint, divisor_count
"""
n = as_int(abs(n))
if isprime(n):
return [1, n]
if n == 1:
return [1]
if n == 0:
return []
rv = _divisors(n)
if not generator:
return sorted(rv)
return rv
def divisor_count(n, modulus=1):
"""
Return the number of divisors of ``n``. If ``modulus`` is not 1 then only
those that are divisible by ``modulus`` are counted.
Examples
========
>>> from sympy import divisor_count
>>> divisor_count(6)
4
See Also
========
factorint, divisors, totient
"""
if not modulus:
return 0
elif modulus != 1:
n, r = divmod(n, modulus)
if r:
return 0
if n == 0:
return 0
return Mul(*[v + 1 for k, v in factorint(n).items() if k > 1])
def _udivisors(n):
"""Helper function for udivisors which generates the unitary divisors."""
factorpows = [p**e for p, e in factorint(n).items()]
for i in range(2**len(factorpows)):
d, j, k = 1, i, 0
while j:
if (j & 1):
d *= factorpows[k]
j >>= 1
k += 1
yield d
def udivisors(n, generator=False):
r"""
Return all unitary divisors of n sorted from 1..n by default.
If generator is ``True`` an unordered generator is returned.
The number of unitary divisors of n can be quite large if there are many
prime factors. If only the number of unitary divisors is desired use
udivisor_count(n).
Examples
========
>>> from sympy.ntheory.factor_ import udivisors, udivisor_count
>>> udivisors(15)
[1, 3, 5, 15]
>>> udivisor_count(15)
4
>>> sorted(udivisors(120, generator=True))
[1, 3, 5, 8, 15, 24, 40, 120]
See Also
========
primefactors, factorint, divisors, divisor_count, udivisor_count
References
==========
.. [1] https://en.wikipedia.org/wiki/Unitary_divisor
.. [2] http://mathworld.wolfram.com/UnitaryDivisor.html
"""
n = as_int(abs(n))
if isprime(n):
return [1, n]
if n == 1:
return [1]
if n == 0:
return []
rv = _udivisors(n)
if not generator:
return sorted(rv)
return rv
def udivisor_count(n):
"""
Return the number of unitary divisors of ``n``.
Parameters
==========
n : integer
Examples
========
>>> from sympy.ntheory.factor_ import udivisor_count
>>> udivisor_count(120)
8
See Also
========
factorint, divisors, udivisors, divisor_count, totient
References
==========
.. [1] http://mathworld.wolfram.com/UnitaryDivisorFunction.html
"""
if n == 0:
return 0
return 2**len([p for p in factorint(n) if p > 1])
def _antidivisors(n):
"""Helper function for antidivisors which generates the antidivisors."""
for d in _divisors(n):
y = 2*d
if n > y and n % y:
yield y
for d in _divisors(2*n-1):
if n > d >= 2 and n % d:
yield d
for d in _divisors(2*n+1):
if n > d >= 2 and n % d:
yield d
def antidivisors(n, generator=False):
r"""
Return all antidivisors of n sorted from 1..n by default.
Antidivisors [1]_ of n are numbers that do not divide n by the largest
possible margin. If generator is True an unordered generator is returned.
Examples
========
>>> from sympy.ntheory.factor_ import antidivisors
>>> antidivisors(24)
[7, 16]
>>> sorted(antidivisors(128, generator=True))
[3, 5, 15, 17, 51, 85]
See Also
========
primefactors, factorint, divisors, divisor_count, antidivisor_count
References
==========
.. [1] definition is described in https://oeis.org/A066272/a066272a.html
"""
n = as_int(abs(n))
if n <= 2:
return []
rv = _antidivisors(n)
if not generator:
return sorted(rv)
return rv
def antidivisor_count(n):
"""
Return the number of antidivisors [1]_ of ``n``.
Parameters
==========
n : integer
Examples
========
>>> from sympy.ntheory.factor_ import antidivisor_count
>>> antidivisor_count(13)
4
>>> antidivisor_count(27)
5
See Also
========
factorint, divisors, antidivisors, divisor_count, totient
References
==========
.. [1] formula from https://oeis.org/A066272
"""
n = as_int(abs(n))
if n <= 2:
return 0
return divisor_count(2*n - 1) + divisor_count(2*n + 1) + \
divisor_count(n) - divisor_count(n, 2) - 5
class totient(Function):
r"""
Calculate the Euler totient function phi(n)
``totient(n)`` or `\phi(n)` is the number of positive integers `\leq` n
that are relatively prime to n.
Parameters
==========
n : integer
Examples
========
>>> from sympy.ntheory import totient
>>> totient(1)
1
>>> totient(25)
20
See Also
========
divisor_count
References
==========
.. [1] https://en.wikipedia.org/wiki/Euler%27s_totient_function
.. [2] http://mathworld.wolfram.com/TotientFunction.html
"""
@classmethod
def eval(cls, n):
n = sympify(n)
if n.is_Integer:
if n < 1:
raise ValueError("n must be a positive integer")
factors = factorint(n)
return cls._from_factors(factors)
elif not isinstance(n, Expr) or (n.is_integer is False) or (n.is_positive is False):
raise ValueError("n must be a positive integer")
def _eval_is_integer(self):
return fuzzy_and([self.args[0].is_integer, self.args[0].is_positive])
@classmethod
def _from_distinct_primes(self, *args):
"""Subroutine to compute totient from the list of assumed
distinct primes
Examples
========
>>> from sympy.ntheory.factor_ import totient
>>> totient._from_distinct_primes(5, 7)
24
"""
from functools import reduce
return reduce(lambda i, j: i * (j-1), args, 1)
@classmethod
def _from_factors(self, factors):
"""Subroutine to compute totient from already-computed factors
Examples
========
>>> from sympy.ntheory.factor_ import totient
>>> totient._from_factors({5: 2})
20
"""
t = 1
for p, k in factors.items():
t *= (p - 1) * p**(k - 1)
return t
class reduced_totient(Function):
r"""
Calculate the Carmichael reduced totient function lambda(n)
``reduced_totient(n)`` or `\lambda(n)` is the smallest m > 0 such that
`k^m \equiv 1 \mod n` for all k relatively prime to n.
Examples
========
>>> from sympy.ntheory import reduced_totient
>>> reduced_totient(1)
1
>>> reduced_totient(8)
2
>>> reduced_totient(30)
4
See Also
========
totient
References
==========
.. [1] https://en.wikipedia.org/wiki/Carmichael_function
.. [2] http://mathworld.wolfram.com/CarmichaelFunction.html
"""
@classmethod
def eval(cls, n):
n = sympify(n)
if n.is_Integer:
if n < 1:
raise ValueError("n must be a positive integer")
factors = factorint(n)
return cls._from_factors(factors)
@classmethod
def _from_factors(self, factors):
"""Subroutine to compute totient from already-computed factors
"""
t = 1
for p, k in factors.items():
if p == 2 and k > 2:
t = ilcm(t, 2**(k - 2))
else:
t = ilcm(t, (p - 1) * p**(k - 1))
return t
@classmethod
def _from_distinct_primes(self, *args):
"""Subroutine to compute totient from the list of assumed
distinct primes
"""
args = [p - 1 for p in args]
return ilcm(*args)
def _eval_is_integer(self):
return fuzzy_and([self.args[0].is_integer, self.args[0].is_positive])
class divisor_sigma(Function):
r"""
Calculate the divisor function `\sigma_k(n)` for positive integer n
``divisor_sigma(n, k)`` is equal to ``sum([x**k for x in divisors(n)])``
If n's prime factorization is:
.. math ::
n = \prod_{i=1}^\omega p_i^{m_i},
then
.. math ::
\sigma_k(n) = \prod_{i=1}^\omega (1+p_i^k+p_i^{2k}+\cdots
+ p_i^{m_ik}).
Parameters
==========
n : integer
k : integer, optional
power of divisors in the sum
for k = 0, 1:
``divisor_sigma(n, 0)`` is equal to ``divisor_count(n)``
``divisor_sigma(n, 1)`` is equal to ``sum(divisors(n))``
Default for k is 1.
Examples
========
>>> from sympy.ntheory import divisor_sigma
>>> divisor_sigma(18, 0)
6
>>> divisor_sigma(39, 1)
56
>>> divisor_sigma(12, 2)
210
>>> divisor_sigma(37)
38
See Also
========
divisor_count, totient, divisors, factorint
References
==========
.. [1] https://en.wikipedia.org/wiki/Divisor_function
"""
@classmethod
def eval(cls, n, k=1):
n = sympify(n)
k = sympify(k)
if n.is_prime:
return 1 + n**k
if n.is_Integer:
if n <= 0:
raise ValueError("n must be a positive integer")
else:
return Mul(*[(p**(k*(e + 1)) - 1)/(p**k - 1) if k != 0
else e + 1 for p, e in factorint(n).items()])
def core(n, t=2):
r"""
Calculate core(n, t) = `core_t(n)` of a positive integer n
``core_2(n)`` is equal to the squarefree part of n
If n's prime factorization is:
.. math ::
n = \prod_{i=1}^\omega p_i^{m_i},
then
.. math ::
core_t(n) = \prod_{i=1}^\omega p_i^{m_i \mod t}.
Parameters
==========
n : integer
t : integer
core(n, t) calculates the t-th power free part of n
``core(n, 2)`` is the squarefree part of ``n``
``core(n, 3)`` is the cubefree part of ``n``
Default for t is 2.
Examples
========
>>> from sympy.ntheory.factor_ import core
>>> core(24, 2)
6
>>> core(9424, 3)
1178
>>> core(379238)
379238
>>> core(15**11, 10)
15
See Also
========
factorint, sympy.solvers.diophantine.square_factor
References
==========
.. [1] https://en.wikipedia.org/wiki/Square-free_integer#Squarefree_core
"""
n = as_int(n)
t = as_int(t)
if n <= 0:
raise ValueError("n must be a positive integer")
elif t <= 1:
raise ValueError("t must be >= 2")
else:
y = 1
for p, e in factorint(n).items():
y *= p**(e % t)
return y
def digits(n, b=10):
"""
Return a list of the digits of n in base b. The first element in the list
is b (or -b if n is negative).
Examples
========
>>> from sympy.ntheory.factor_ import digits
>>> digits(35)
[10, 3, 5]
>>> digits(27, 2)
[2, 1, 1, 0, 1, 1]
>>> digits(65536, 256)
[256, 1, 0, 0]
>>> digits(-3958, 27)
[-27, 5, 11, 16]
"""
b = as_int(b)
n = as_int(n)
if b <= 1:
raise ValueError("b must be >= 2")
else:
x, y = abs(n), []
while x >= b:
x, r = divmod(x, b)
y.append(r)
y.append(x)
y.append(-b if n < 0 else b)
y.reverse()
return y
class udivisor_sigma(Function):
r"""
Calculate the unitary divisor function `\sigma_k^*(n)` for positive integer n
``udivisor_sigma(n, k)`` is equal to ``sum([x**k for x in udivisors(n)])``
If n's prime factorization is:
.. math ::
n = \prod_{i=1}^\omega p_i^{m_i},
then
.. math ::
\sigma_k^*(n) = \prod_{i=1}^\omega (1+ p_i^{m_ik}).
Parameters
==========
k : power of divisors in the sum
for k = 0, 1:
``udivisor_sigma(n, 0)`` is equal to ``udivisor_count(n)``
``udivisor_sigma(n, 1)`` is equal to ``sum(udivisors(n))``
Default for k is 1.
Examples
========
>>> from sympy.ntheory.factor_ import udivisor_sigma
>>> udivisor_sigma(18, 0)
4
>>> udivisor_sigma(74, 1)
114
>>> udivisor_sigma(36, 3)
47450
>>> udivisor_sigma(111)
152
See Also
========
divisor_count, totient, divisors, udivisors, udivisor_count, divisor_sigma,
factorint
References
==========
.. [1] http://mathworld.wolfram.com/UnitaryDivisorFunction.html
"""
@classmethod
def eval(cls, n, k=1):
n = sympify(n)
k = sympify(k)
if n.is_prime:
return 1 + n**k
if n.is_Integer:
if n <= 0:
raise ValueError("n must be a positive integer")
else:
return Mul(*[1+p**(k*e) for p, e in factorint(n).items()])
class primenu(Function):
r"""
Calculate the number of distinct prime factors for a positive integer n.
If n's prime factorization is:
.. math ::
n = \prod_{i=1}^k p_i^{m_i},
then ``primenu(n)`` or `\nu(n)` is:
.. math ::
\nu(n) = k.
Examples
========
>>> from sympy.ntheory.factor_ import primenu
>>> primenu(1)
0
>>> primenu(30)
3
See Also
========
factorint
References
==========
.. [1] http://mathworld.wolfram.com/PrimeFactor.html
"""
@classmethod
def eval(cls, n):
n = sympify(n)
if n.is_Integer:
if n <= 0:
raise ValueError("n must be a positive integer")
else:
return len(factorint(n).keys())
class primeomega(Function):
r"""
Calculate the number of prime factors counting multiplicities for a
positive integer n.
If n's prime factorization is:
.. math ::
n = \prod_{i=1}^k p_i^{m_i},
then ``primeomega(n)`` or `\Omega(n)` is:
.. math ::
\Omega(n) = \sum_{i=1}^k m_i.
Examples
========
>>> from sympy.ntheory.factor_ import primeomega
>>> primeomega(1)
0
>>> primeomega(20)
3
See Also
========
factorint
References
==========
.. [1] http://mathworld.wolfram.com/PrimeFactor.html
"""
@classmethod
def eval(cls, n):
n = sympify(n)
if n.is_Integer:
if n <= 0:
raise ValueError("n must be a positive integer")
else:
return sum(factorint(n).values())
def mersenne_prime_exponent(nth):
"""Returns the exponent ``i`` for the nth Mersenne prime (which
has the form `2^i - 1`).
Examples
========
>>> from sympy.ntheory.factor_ import mersenne_prime_exponent
>>> mersenne_prime_exponent(1)
2
>>> mersenne_prime_exponent(20)
4423
"""
n = as_int(nth)
if n < 1:
raise ValueError("nth must be a positive integer; mersenne_prime_exponent(1) == 2")
if n > 51:
raise ValueError("There are only 51 perfect numbers; nth must be less than or equal to 51")
return MERSENNE_PRIME_EXPONENTS[n - 1]
def is_perfect(n):
"""Returns True if ``n`` is a perfect number, else False.
A perfect number is equal to the sum of its positive, proper divisors.
Examples
========
>>> from sympy.ntheory.factor_ import is_perfect, divisors
>>> is_perfect(20)
False
>>> is_perfect(6)
True
>>> sum(divisors(6)[:-1])
6
References
==========
.. [1] http://mathworld.wolfram.com/PerfectNumber.html
"""
from sympy.core.power import integer_log
r, b = integer_nthroot(1 + 8*n, 2)
if not b:
return False
n, x = divmod(1 + r, 4)
if x:
return False
e, b = integer_log(n, 2)
return b and (e + 1) in MERSENNE_PRIME_EXPONENTS
def is_mersenne_prime(n):
"""Returns True if ``n`` is a Mersenne prime, else False.
A Mersenne prime is a prime number having the form `2^i - 1`.
Examples
========
>>> from sympy.ntheory.factor_ import is_mersenne_prime
>>> is_mersenne_prime(6)
False
>>> is_mersenne_prime(127)
True
References
==========
.. [1] http://mathworld.wolfram.com/MersennePrime.html
"""
from sympy.core.power import integer_log
r, b = integer_log(n + 1, 2)
return b and r in MERSENNE_PRIME_EXPONENTS
def abundance(n):
"""Returns the difference between the sum of the positive
proper divisors of a number and the number.
Examples
========
>>> from sympy.ntheory import abundance, is_perfect, is_abundant
>>> abundance(6)
0
>>> is_perfect(6)
True
>>> abundance(10)
-2
>>> is_abundant(10)
False
"""
return divisor_sigma(n, 1) - 2 * n
def is_abundant(n):
"""Returns True if ``n`` is an abundant number, else False.
A abundant number is smaller than the sum of its positive proper divisors.
Examples
========
>>> from sympy.ntheory.factor_ import is_abundant
>>> is_abundant(20)
True
>>> is_abundant(15)
False
References
==========
.. [1] http://mathworld.wolfram.com/AbundantNumber.html
"""
n = as_int(n)
if is_perfect(n):
return False
return n % 6 == 0 or bool(abundance(n) > 0)
def is_deficient(n):
"""Returns True if ``n`` is a deficient number, else False.
A deficient number is greater than the sum of its positive proper divisors.
Examples
========
>>> from sympy.ntheory.factor_ import is_deficient
>>> is_deficient(20)
False
>>> is_deficient(15)
True
References
==========
.. [1] http://mathworld.wolfram.com/DeficientNumber.html
"""
n = as_int(n)
if is_perfect(n):
return False
return bool(abundance(n) < 0)
def is_amicable(m, n):
"""Returns True if the numbers `m` and `n` are "amicable", else False.
Amicable numbers are two different numbers so related that the sum
of the proper divisors of each is equal to that of the other.
Examples
========
>>> from sympy.ntheory.factor_ import is_amicable, divisor_sigma
>>> is_amicable(220, 284)
True
>>> divisor_sigma(220) == divisor_sigma(284)
True
References
==========
.. [1] https://en.wikipedia.org/wiki/Amicable_numbers
"""
if m == n:
return False
a, b = map(lambda i: divisor_sigma(i), (m, n))
return a == b == (m + n)
|
ecd149345b7845bb9ecd47e19d1d0c1dce2ee2e6a8b43abe55a2d3ed48cd7d5c | from __future__ import print_function, division
import itertools
from sympy.combinatorics.fp_groups import FpGroup, FpSubgroup, simplify_presentation
from sympy.combinatorics.free_groups import FreeGroup
from sympy.combinatorics.perm_groups import PermutationGroup
from sympy.core.numbers import igcd
from sympy.ntheory.factor_ import totient
from sympy import S
class GroupHomomorphism(object):
'''
A class representing group homomorphisms. Instantiate using `homomorphism()`.
References
==========
.. [1] Holt, D., Eick, B. and O'Brien, E. (2005). Handbook of computational group theory.
'''
def __init__(self, domain, codomain, images):
self.domain = domain
self.codomain = codomain
self.images = images
self._inverses = None
self._kernel = None
self._image = None
def _invs(self):
'''
Return a dictionary with `{gen: inverse}` where `gen` is a rewriting
generator of `codomain` (e.g. strong generator for permutation groups)
and `inverse` is an element of its preimage
'''
image = self.image()
inverses = {}
for k in list(self.images.keys()):
v = self.images[k]
if not (v in inverses
or v.is_identity):
inverses[v] = k
if isinstance(self.codomain, PermutationGroup):
gens = image.strong_gens
else:
gens = image.generators
for g in gens:
if g in inverses or g.is_identity:
continue
w = self.domain.identity
if isinstance(self.codomain, PermutationGroup):
parts = image._strong_gens_slp[g][::-1]
else:
parts = g
for s in parts:
if s in inverses:
w = w*inverses[s]
else:
w = w*inverses[s**-1]**-1
inverses[g] = w
return inverses
def invert(self, g):
'''
Return an element of the preimage of `g` or of each element
of `g` if `g` is a list.
NOTE: If the codomain is an FpGroup, the inverse for equal
elements might not always be the same unless the FpGroup's
rewriting system is confluent. However, making a system
confluent can be time-consuming. If it's important, try
`self.codomain.make_confluent()` first.
'''
from sympy.combinatorics import Permutation
from sympy.combinatorics.free_groups import FreeGroupElement
if isinstance(g, (Permutation, FreeGroupElement)):
if isinstance(self.codomain, FpGroup):
g = self.codomain.reduce(g)
if self._inverses is None:
self._inverses = self._invs()
image = self.image()
w = self.domain.identity
if isinstance(self.codomain, PermutationGroup):
gens = image.generator_product(g)[::-1]
else:
gens = g
# the following can't be "for s in gens:"
# because that would be equivalent to
# "for s in gens.array_form:" when g is
# a FreeGroupElement. On the other hand,
# when you call gens by index, the generator
# (or inverse) at position i is returned.
for i in range(len(gens)):
s = gens[i]
if s.is_identity:
continue
if s in self._inverses:
w = w*self._inverses[s]
else:
w = w*self._inverses[s**-1]**-1
return w
elif isinstance(g, list):
return [self.invert(e) for e in g]
def kernel(self):
'''
Compute the kernel of `self`.
'''
if self._kernel is None:
self._kernel = self._compute_kernel()
return self._kernel
def _compute_kernel(self):
from sympy import S
G = self.domain
G_order = G.order()
if G_order is S.Infinity:
raise NotImplementedError(
"Kernel computation is not implemented for infinite groups")
gens = []
if isinstance(G, PermutationGroup):
K = PermutationGroup(G.identity)
else:
K = FpSubgroup(G, gens, normal=True)
i = self.image().order()
while K.order()*i != G_order:
r = G.random()
k = r*self.invert(self(r))**-1
if not k in K:
gens.append(k)
if isinstance(G, PermutationGroup):
K = PermutationGroup(gens)
else:
K = FpSubgroup(G, gens, normal=True)
return K
def image(self):
'''
Compute the image of `self`.
'''
if self._image is None:
values = list(set(self.images.values()))
if isinstance(self.codomain, PermutationGroup):
self._image = self.codomain.subgroup(values)
else:
self._image = FpSubgroup(self.codomain, values)
return self._image
def _apply(self, elem):
'''
Apply `self` to `elem`.
'''
if not elem in self.domain:
if isinstance(elem, (list, tuple)):
return [self._apply(e) for e in elem]
raise ValueError("The supplied element doesn't belong to the domain")
if elem.is_identity:
return self.codomain.identity
else:
images = self.images
value = self.codomain.identity
if isinstance(self.domain, PermutationGroup):
gens = self.domain.generator_product(elem, original=True)
for g in gens:
if g in self.images:
value = images[g]*value
else:
value = images[g**-1]**-1*value
else:
i = 0
for _, p in elem.array_form:
if p < 0:
g = elem[i]**-1
else:
g = elem[i]
value = value*images[g]**p
i += abs(p)
return value
def __call__(self, elem):
return self._apply(elem)
def is_injective(self):
'''
Check if the homomorphism is injective
'''
return self.kernel().order() == 1
def is_surjective(self):
'''
Check if the homomorphism is surjective
'''
from sympy import S
im = self.image().order()
oth = self.codomain.order()
if im is S.Infinity and oth is S.Infinity:
return None
else:
return im == oth
def is_isomorphism(self):
'''
Check if `self` is an isomorphism.
'''
return self.is_injective() and self.is_surjective()
def is_trivial(self):
'''
Check is `self` is a trivial homomorphism, i.e. all elements
are mapped to the identity.
'''
return self.image().order() == 1
def compose(self, other):
'''
Return the composition of `self` and `other`, i.e.
the homomorphism phi such that for all g in the domain
of `other`, phi(g) = self(other(g))
'''
if not other.image().is_subgroup(self.domain):
raise ValueError("The image of `other` must be a subgroup of "
"the domain of `self`")
images = {g: self(other(g)) for g in other.images}
return GroupHomomorphism(other.domain, self.codomain, images)
def restrict_to(self, H):
'''
Return the restriction of the homomorphism to the subgroup `H`
of the domain.
'''
if not isinstance(H, PermutationGroup) or not H.is_subgroup(self.domain):
raise ValueError("Given H is not a subgroup of the domain")
domain = H
images = {g: self(g) for g in H.generators}
return GroupHomomorphism(domain, self.codomain, images)
def invert_subgroup(self, H):
'''
Return the subgroup of the domain that is the inverse image
of the subgroup `H` of the homomorphism image
'''
if not H.is_subgroup(self.image()):
raise ValueError("Given H is not a subgroup of the image")
gens = []
P = PermutationGroup(self.image().identity)
for h in H.generators:
h_i = self.invert(h)
if h_i not in P:
gens.append(h_i)
P = PermutationGroup(gens)
for k in self.kernel().generators:
if k*h_i not in P:
gens.append(k*h_i)
P = PermutationGroup(gens)
return P
def homomorphism(domain, codomain, gens, images=[], check=True):
'''
Create (if possible) a group homomorphism from the group `domain`
to the group `codomain` defined by the images of the domain's
generators `gens`. `gens` and `images` can be either lists or tuples
of equal sizes. If `gens` is a proper subset of the group's generators,
the unspecified generators will be mapped to the identity. If the
images are not specified, a trivial homomorphism will be created.
If the given images of the generators do not define a homomorphism,
an exception is raised.
If `check` is `False`, don't check whether the given images actually
define a homomorphism.
'''
if not isinstance(domain, (PermutationGroup, FpGroup, FreeGroup)):
raise TypeError("The domain must be a group")
if not isinstance(codomain, (PermutationGroup, FpGroup, FreeGroup)):
raise TypeError("The codomain must be a group")
generators = domain.generators
if any([g not in generators for g in gens]):
raise ValueError("The supplied generators must be a subset of the domain's generators")
if any([g not in codomain for g in images]):
raise ValueError("The images must be elements of the codomain")
if images and len(images) != len(gens):
raise ValueError("The number of images must be equal to the number of generators")
gens = list(gens)
images = list(images)
images.extend([codomain.identity]*(len(generators)-len(images)))
gens.extend([g for g in generators if g not in gens])
images = dict(zip(gens,images))
if check and not _check_homomorphism(domain, codomain, images):
raise ValueError("The given images do not define a homomorphism")
return GroupHomomorphism(domain, codomain, images)
def _check_homomorphism(domain, codomain, images):
if hasattr(domain, 'relators'):
rels = domain.relators
else:
gens = domain.presentation().generators
rels = domain.presentation().relators
identity = codomain.identity
def _image(r):
if r.is_identity:
return identity
else:
w = identity
r_arr = r.array_form
i = 0
j = 0
# i is the index for r and j is for
# r_arr. r_arr[j] is the tuple (sym, p)
# where sym is the generator symbol
# and p is the power to which it is
# raised while r[i] is a generator
# (not just its symbol) or the inverse of
# a generator - hence the need for
# both indices
while i < len(r):
power = r_arr[j][1]
if isinstance(domain, PermutationGroup) and r[i] in gens:
s = domain.generators[gens.index(r[i])]
else:
s = r[i]
if s in images:
w = w*images[s]**power
elif s**-1 in images:
w = w*images[s**-1]**power
i += abs(power)
j += 1
return w
for r in rels:
if isinstance(codomain, FpGroup):
s = codomain.equals(_image(r), identity)
if s is None:
# only try to make the rewriting system
# confluent when it can't determine the
# truth of equality otherwise
success = codomain.make_confluent()
s = codomain.equals(_image(r), identity)
if s is None and not success:
raise RuntimeError("Can't determine if the images "
"define a homomorphism. Try increasing "
"the maximum number of rewriting rules "
"(group._rewriting_system.set_max(new_value); "
"the current value is stored in group._rewriting"
"_system.maxeqns)")
else:
s = _image(r).is_identity
if not s:
return False
return True
def orbit_homomorphism(group, omega):
'''
Return the homomorphism induced by the action of the permutation
group `group` on the set `omega` that is closed under the action.
'''
from sympy.combinatorics import Permutation
from sympy.combinatorics.named_groups import SymmetricGroup
codomain = SymmetricGroup(len(omega))
identity = codomain.identity
omega = list(omega)
images = {g: identity*Permutation([omega.index(o^g) for o in omega]) for g in group.generators}
group._schreier_sims(base=omega)
H = GroupHomomorphism(group, codomain, images)
if len(group.basic_stabilizers) > len(omega):
H._kernel = group.basic_stabilizers[len(omega)]
else:
H._kernel = PermutationGroup([group.identity])
return H
def block_homomorphism(group, blocks):
'''
Return the homomorphism induced by the action of the permutation
group `group` on the block system `blocks`. The latter should be
of the same form as returned by the `minimal_block` method for
permutation groups, namely a list of length `group.degree` where
the i-th entry is a representative of the block i belongs to.
'''
from sympy.combinatorics import Permutation
from sympy.combinatorics.named_groups import SymmetricGroup
n = len(blocks)
# number the blocks; m is the total number,
# b is such that b[i] is the number of the block i belongs to,
# p is the list of length m such that p[i] is the representative
# of the i-th block
m = 0
p = []
b = [None]*n
for i in range(n):
if blocks[i] == i:
p.append(i)
b[i] = m
m += 1
for i in range(n):
b[i] = b[blocks[i]]
codomain = SymmetricGroup(m)
# the list corresponding to the identity permutation in codomain
identity = range(m)
images = {g: Permutation([b[p[i]^g] for i in identity]) for g in group.generators}
H = GroupHomomorphism(group, codomain, images)
return H
def group_isomorphism(G, H, isomorphism=True):
'''
Compute an isomorphism between 2 given groups.
Parameters
==========
G (a finite `FpGroup` or a `PermutationGroup`) -- First group
H (a finite `FpGroup` or a `PermutationGroup`) -- Second group
isomorphism (boolean) -- This is used to avoid the computation of homomorphism
when the user only wants to check if there exists
an isomorphism between the groups.
Returns
=======
If isomorphism = False -- Returns a boolean.
If isomorphism = True -- Returns a boolean and an isomorphism between `G` and `H`.
Examples
========
>>> from sympy.combinatorics import Permutation
>>> Permutation.print_cyclic = True
>>> from sympy.combinatorics.perm_groups import PermutationGroup
>>> from sympy.combinatorics.free_groups import free_group
>>> from sympy.combinatorics.fp_groups import FpGroup
>>> from sympy.combinatorics.homomorphisms import homomorphism, group_isomorphism
>>> from sympy.combinatorics.named_groups import DihedralGroup, AlternatingGroup
>>> D = DihedralGroup(8)
>>> p = Permutation(0, 1, 2, 3, 4, 5, 6, 7)
>>> P = PermutationGroup(p)
>>> group_isomorphism(D, P)
(False, None)
>>> F, a, b = free_group("a, b")
>>> G = FpGroup(F, [a**3, b**3, (a*b)**2])
>>> H = AlternatingGroup(4)
>>> (check, T) = group_isomorphism(G, H)
>>> check
True
>>> T(b*a*b**-1*a**-1*b**-1)
(0 2 3)
Notes
=====
Uses the approach suggested by Robert Tarjan to compute the isomorphism between two groups.
First, the generators of `G` are mapped to the elements of `H` and
we check if the mapping induces an isomorphism.
'''
if not isinstance(G, (PermutationGroup, FpGroup)):
raise TypeError("The group must be a PermutationGroup or an FpGroup")
if not isinstance(H, (PermutationGroup, FpGroup)):
raise TypeError("The group must be a PermutationGroup or an FpGroup")
if isinstance(G, FpGroup) and isinstance(H, FpGroup):
G = simplify_presentation(G)
H = simplify_presentation(H)
# Two infinite FpGroups with the same generators are isomorphic
# when the relators are same but are ordered differently.
if G.generators == H.generators and (G.relators).sort() == (H.relators).sort():
if not isomorphism:
return True
return (True, homomorphism(G, H, G.generators, H.generators))
# `_H` is the permutation group isomorphic to `H`.
_H = H
g_order = G.order()
h_order = H.order()
if g_order is S.Infinity:
raise NotImplementedError("Isomorphism methods are not implemented for infinite groups.")
if isinstance(H, FpGroup):
if h_order is S.Infinity:
raise NotImplementedError("Isomorphism methods are not implemented for infinite groups.")
_H, h_isomorphism = H._to_perm_group()
if (g_order != h_order) or (G.is_abelian != H.is_abelian):
if not isomorphism:
return False
return (False, None)
if not isomorphism:
# Two groups of the same cyclic numbered order
# are isomorphic to each other.
n = g_order
if (igcd(n, totient(n))) == 1:
return True
# Match the generators of `G` with subsets of `_H`
gens = list(G.generators)
for subset in itertools.permutations(_H, len(gens)):
images = list(subset)
images.extend([_H.identity]*(len(G.generators)-len(images)))
_images = dict(zip(gens,images))
if _check_homomorphism(G, _H, _images):
if isinstance(H, FpGroup):
images = h_isomorphism.invert(images)
T = homomorphism(G, H, G.generators, images, check=False)
if T.is_isomorphism():
# It is a valid isomorphism
if not isomorphism:
return True
return (True, T)
if not isomorphism:
return False
return (False, None)
def is_isomorphic(G, H):
'''
Check if the groups are isomorphic to each other
Parameters
==========
G (a finite `FpGroup` or a `PermutationGroup`) -- First group
H (a finite `FpGroup` or a `PermutationGroup`) -- Second group
Returns
=======
boolean
'''
return group_isomorphism(G, H, isomorphism=False)
|
3e9e6873ed112135f0109d5dbb83aaeb82e580fa75553765f153765c9c9f937f | """Finitely Presented Groups and its algorithms. """
from __future__ import print_function, division
from sympy import S
from sympy.combinatorics.free_groups import (FreeGroup, FreeGroupElement,
free_group)
from sympy.combinatorics.rewritingsystem import RewritingSystem
from sympy.combinatorics.coset_table import (CosetTable,
coset_enumeration_r,
coset_enumeration_c)
from sympy.combinatorics import PermutationGroup
from sympy.printing.defaults import DefaultPrinting
from sympy.utilities import public
from sympy.core.compatibility import string_types
from itertools import product
@public
def fp_group(fr_grp, relators=[]):
_fp_group = FpGroup(fr_grp, relators)
return (_fp_group,) + tuple(_fp_group._generators)
@public
def xfp_group(fr_grp, relators=[]):
_fp_group = FpGroup(fr_grp, relators)
return (_fp_group, _fp_group._generators)
# Does not work. Both symbols and pollute are undefined. Never tested.
@public
def vfp_group(fr_grpm, relators):
_fp_group = FpGroup(symbols, relators)
pollute([sym.name for sym in _fp_group.symbols], _fp_group.generators)
return _fp_group
def _parse_relators(rels):
"""Parse the passed relators."""
return rels
###############################################################################
# FINITELY PRESENTED GROUPS #
###############################################################################
class FpGroup(DefaultPrinting):
"""
The FpGroup would take a FreeGroup and a list/tuple of relators, the
relators would be specified in such a way that each of them be equal to the
identity of the provided free group.
"""
is_group = True
is_FpGroup = True
is_PermutationGroup = False
def __init__(self, fr_grp, relators):
relators = _parse_relators(relators)
self.free_group = fr_grp
self.relators = relators
self.generators = self._generators()
self.dtype = type("FpGroupElement", (FpGroupElement,), {"group": self})
# CosetTable instance on identity subgroup
self._coset_table = None
# returns whether coset table on identity subgroup
# has been standardized
self._is_standardized = False
self._order = None
self._center = None
self._rewriting_system = RewritingSystem(self)
self._perm_isomorphism = None
return
def _generators(self):
return self.free_group.generators
def make_confluent(self):
'''
Try to make the group's rewriting system confluent
'''
self._rewriting_system.make_confluent()
return
def reduce(self, word):
'''
Return the reduced form of `word` in `self` according to the group's
rewriting system. If it's confluent, the reduced form is the unique normal
form of the word in the group.
'''
return self._rewriting_system.reduce(word)
def equals(self, word1, word2):
'''
Compare `word1` and `word2` for equality in the group
using the group's rewriting system. If the system is
confluent, the returned answer is necessarily correct.
(If it isn't, `False` could be returned in some cases
where in fact `word1 == word2`)
'''
if self.reduce(word1*word2**-1) == self.identity:
return True
elif self._rewriting_system.is_confluent:
return False
return None
@property
def identity(self):
return self.free_group.identity
def __contains__(self, g):
return g in self.free_group
def subgroup(self, gens, C=None, homomorphism=False):
'''
Return the subgroup generated by `gens` using the
Reidemeister-Schreier algorithm
homomorphism -- When set to True, return a dictionary containing the images
of the presentation generators in the original group.
Examples
========
>>> from sympy.combinatorics.fp_groups import (FpGroup, FpSubgroup)
>>> from sympy.combinatorics.free_groups import free_group
>>> F, x, y = free_group("x, y")
>>> f = FpGroup(F, [x**3, y**5, (x*y)**2])
>>> H = [x*y, x**-1*y**-1*x*y*x]
>>> K, T = f.subgroup(H, homomorphism=True)
>>> T(K.generators)
[x*y, x**-1*y**2*x**-1]
'''
if not all([isinstance(g, FreeGroupElement) for g in gens]):
raise ValueError("Generators must be `FreeGroupElement`s")
if not all([g.group == self.free_group for g in gens]):
raise ValueError("Given generators are not members of the group")
if homomorphism:
g, rels, _gens = reidemeister_presentation(self, gens, C=C, homomorphism=True)
else:
g, rels = reidemeister_presentation(self, gens, C=C)
if g:
g = FpGroup(g[0].group, rels)
else:
g = FpGroup(free_group('')[0], [])
if homomorphism:
from sympy.combinatorics.homomorphisms import homomorphism
return g, homomorphism(g, self, g.generators, _gens, check=False)
return g
def coset_enumeration(self, H, strategy="relator_based", max_cosets=None,
draft=None, incomplete=False):
"""
Return an instance of ``coset table``, when Todd-Coxeter algorithm is
run over the ``self`` with ``H`` as subgroup, using ``strategy``
argument as strategy. The returned coset table is compressed but not
standardized.
An instance of `CosetTable` for `fp_grp` can be passed as the keyword
argument `draft` in which case the coset enumeration will start with
that instance and attempt to complete it.
When `incomplete` is `True` and the function is unable to complete for
some reason, the partially complete table will be returned.
"""
if not max_cosets:
max_cosets = CosetTable.coset_table_max_limit
if strategy == 'relator_based':
C = coset_enumeration_r(self, H, max_cosets=max_cosets,
draft=draft, incomplete=incomplete)
else:
C = coset_enumeration_c(self, H, max_cosets=max_cosets,
draft=draft, incomplete=incomplete)
if C.is_complete():
C.compress()
return C
def standardize_coset_table(self):
"""
Standardized the coset table ``self`` and makes the internal variable
``_is_standardized`` equal to ``True``.
"""
self._coset_table.standardize()
self._is_standardized = True
def coset_table(self, H, strategy="relator_based", max_cosets=None,
draft=None, incomplete=False):
"""
Return the mathematical coset table of ``self`` in ``H``.
"""
if not H:
if self._coset_table is not None:
if not self._is_standardized:
self.standardize_coset_table()
else:
C = self.coset_enumeration([], strategy, max_cosets=max_cosets,
draft=draft, incomplete=incomplete)
self._coset_table = C
self.standardize_coset_table()
return self._coset_table.table
else:
C = self.coset_enumeration(H, strategy, max_cosets=max_cosets,
draft=draft, incomplete=incomplete)
C.standardize()
return C.table
def order(self, strategy="relator_based"):
"""
Returns the order of the finitely presented group ``self``. It uses
the coset enumeration with identity group as subgroup, i.e ``H=[]``.
Examples
========
>>> from sympy.combinatorics.free_groups import free_group
>>> from sympy.combinatorics.fp_groups import FpGroup
>>> F, x, y = free_group("x, y")
>>> f = FpGroup(F, [x, y**2])
>>> f.order(strategy="coset_table_based")
2
"""
from sympy import S, gcd
if self._order is not None:
return self._order
if self._coset_table is not None:
self._order = len(self._coset_table.table)
elif len(self.relators) == 0:
self._order = self.free_group.order()
elif len(self.generators) == 1:
self._order = abs(gcd([r.array_form[0][1] for r in self.relators]))
elif self._is_infinite():
self._order = S.Infinity
else:
gens, C = self._finite_index_subgroup()
if C:
ind = len(C.table)
self._order = ind*self.subgroup(gens, C=C).order()
else:
self._order = self.index([])
return self._order
def _is_infinite(self):
'''
Test if the group is infinite. Return `True` if the test succeeds
and `None` otherwise
'''
used_gens = set()
for r in self.relators:
used_gens.update(r.contains_generators())
if any([g not in used_gens for g in self.generators]):
return True
# Abelianisation test: check is the abelianisation is infinite
abelian_rels = []
from sympy.polys.solvers import RawMatrix as Matrix
from sympy.polys.domains import ZZ
from sympy.matrices.normalforms import invariant_factors
for rel in self.relators:
abelian_rels.append([rel.exponent_sum(g) for g in self.generators])
m = Matrix(abelian_rels)
setattr(m, "ring", ZZ)
if 0 in invariant_factors(m):
return True
else:
return None
def _finite_index_subgroup(self, s=[]):
'''
Find the elements of `self` that generate a finite index subgroup
and, if found, return the list of elements and the coset table of `self` by
the subgroup, otherwise return `(None, None)`
'''
gen = self.most_frequent_generator()
rels = list(self.generators)
rels.extend(self.relators)
if not s:
if len(self.generators) == 2:
s = [gen] + [g for g in self.generators if g != gen]
else:
rand = self.free_group.identity
i = 0
while ((rand in rels or rand**-1 in rels or rand.is_identity)
and i<10):
rand = self.random()
i += 1
s = [gen, rand] + [g for g in self.generators if g != gen]
mid = (len(s)+1)//2
half1 = s[:mid]
half2 = s[mid:]
draft1 = None
draft2 = None
m = 200
C = None
while not C and (m/2 < CosetTable.coset_table_max_limit):
m = min(m, CosetTable.coset_table_max_limit)
draft1 = self.coset_enumeration(half1, max_cosets=m,
draft=draft1, incomplete=True)
if draft1.is_complete():
C = draft1
half = half1
else:
draft2 = self.coset_enumeration(half2, max_cosets=m,
draft=draft2, incomplete=True)
if draft2.is_complete():
C = draft2
half = half2
if not C:
m *= 2
if not C:
return None, None
C.compress()
return half, C
def most_frequent_generator(self):
gens = self.generators
rels = self.relators
freqs = [sum([r.generator_count(g) for r in rels]) for g in gens]
return gens[freqs.index(max(freqs))]
def random(self):
import random
r = self.free_group.identity
for i in range(random.randint(2,3)):
r = r*random.choice(self.generators)**random.choice([1,-1])
return r
def index(self, H, strategy="relator_based"):
"""
Return the index of subgroup ``H`` in group ``self``.
Examples
========
>>> from sympy.combinatorics.free_groups import free_group
>>> from sympy.combinatorics.fp_groups import FpGroup
>>> F, x, y = free_group("x, y")
>>> f = FpGroup(F, [x**5, y**4, y*x*y**3*x**3])
>>> f.index([x])
4
"""
# TODO: use |G:H| = |G|/|H| (currently H can't be made into a group)
# when we know |G| and |H|
if H == []:
return self.order()
else:
C = self.coset_enumeration(H, strategy)
return len(C.table)
def __str__(self):
if self.free_group.rank > 30:
str_form = "<fp group with %s generators>" % self.free_group.rank
else:
str_form = "<fp group on the generators %s>" % str(self.generators)
return str_form
__repr__ = __str__
#==============================================================================
# PERMUTATION GROUP METHODS
#==============================================================================
def _to_perm_group(self):
'''
Return an isomorphic permutation group and the isomorphism.
The implementation is dependent on coset enumeration so
will only terminate for finite groups.
'''
from sympy.combinatorics import Permutation, PermutationGroup
from sympy.combinatorics.homomorphisms import homomorphism
if self.order() is S.Infinity:
raise NotImplementedError("Permutation presentation of infinite "
"groups is not implemented")
if self._perm_isomorphism:
T = self._perm_isomorphism
P = T.image()
else:
C = self.coset_table([])
gens = self.generators
images = [[C[i][2*gens.index(g)] for i in range(len(C))] for g in gens]
images = [Permutation(i) for i in images]
P = PermutationGroup(images)
T = homomorphism(self, P, gens, images, check=False)
self._perm_isomorphism = T
return P, T
def _perm_group_list(self, method_name, *args):
'''
Given the name of a `PermutationGroup` method (returning a subgroup
or a list of subgroups) and (optionally) additional arguments it takes,
return a list or a list of lists containing the generators of this (or
these) subgroups in terms of the generators of `self`.
'''
P, T = self._to_perm_group()
perm_result = getattr(P, method_name)(*args)
single = False
if isinstance(perm_result, PermutationGroup):
perm_result, single = [perm_result], True
result = []
for group in perm_result:
gens = group.generators
result.append(T.invert(gens))
return result[0] if single else result
def derived_series(self):
'''
Return the list of lists containing the generators
of the subgroups in the derived series of `self`.
'''
return self._perm_group_list('derived_series')
def lower_central_series(self):
'''
Return the list of lists containing the generators
of the subgroups in the lower central series of `self`.
'''
return self._perm_group_list('lower_central_series')
def center(self):
'''
Return the list of generators of the center of `self`.
'''
return self._perm_group_list('center')
def derived_subgroup(self):
'''
Return the list of generators of the derived subgroup of `self`.
'''
return self._perm_group_list('derived_subgroup')
def centralizer(self, other):
'''
Return the list of generators of the centralizer of `other`
(a list of elements of `self`) in `self`.
'''
T = self._to_perm_group()[1]
other = T(other)
return self._perm_group_list('centralizer', other)
def normal_closure(self, other):
'''
Return the list of generators of the normal closure of `other`
(a list of elements of `self`) in `self`.
'''
T = self._to_perm_group()[1]
other = T(other)
return self._perm_group_list('normal_closure', other)
def _perm_property(self, attr):
'''
Given an attribute of a `PermutationGroup`, return
its value for a permutation group isomorphic to `self`.
'''
P = self._to_perm_group()[0]
return getattr(P, attr)
@property
def is_abelian(self):
'''
Check if `self` is abelian.
'''
return self._perm_property("is_abelian")
@property
def is_nilpotent(self):
'''
Check if `self` is nilpotent.
'''
return self._perm_property("is_nilpotent")
@property
def is_solvable(self):
'''
Check if `self` is solvable.
'''
return self._perm_property("is_solvable")
@property
def elements(self):
'''
List the elements of `self`.
'''
P, T = self._to_perm_group()
return T.invert(P._elements)
@property
def is_cyclic(self):
"""
Return ``True`` if group is Cyclic.
"""
if len(self.generators) <= 1:
return True
try:
P, T = self._to_perm_group()
except NotImplementedError:
raise NotImplementedError("Check for infinite Cyclic group "
"is not implemented")
return P.is_cyclic
def abelian_invariants(self):
"""
Return Abelian Invariants of a group.
"""
try:
P, T = self._to_perm_group()
except NotImplementedError:
raise NotImplementedError("abelian invariants is not implemented"
"for infinite group")
return P.abelian_invariants()
def composition_series(self):
"""
Return subnormal series of maximum length for a group.
"""
try:
P, T = self._to_perm_group()
except NotImplementedError:
raise NotImplementedError("composition series is not implemented"
"for infinite group")
return P.composition_series()
class FpSubgroup(DefaultPrinting):
'''
The class implementing a subgroup of an FpGroup or a FreeGroup
(only finite index subgroups are supported at this point). This
is to be used if one wishes to check if an element of the original
group belongs to the subgroup
'''
def __init__(self, G, gens, normal=False):
super(FpSubgroup,self).__init__()
self.parent = G
self.generators = list(set([g for g in gens if g != G.identity]))
self._min_words = None #for use in __contains__
self.C = None
self.normal = normal
def __contains__(self, g):
if isinstance(self.parent, FreeGroup):
if self._min_words is None:
# make _min_words - a list of subwords such that
# g is in the subgroup if and only if it can be
# partitioned into these subwords. Infinite families of
# subwords are presented by tuples, e.g. (r, w)
# stands for the family of subwords r*w**n*r**-1
def _process(w):
# this is to be used before adding new words
# into _min_words; if the word w is not cyclically
# reduced, it will generate an infinite family of
# subwords so should be written as a tuple;
# if it is, w**-1 should be added to the list
# as well
p, r = w.cyclic_reduction(removed=True)
if not r.is_identity:
return [(r, p)]
else:
return [w, w**-1]
# make the initial list
gens = []
for w in self.generators:
if self.normal:
w = w.cyclic_reduction()
gens.extend(_process(w))
for w1 in gens:
for w2 in gens:
# if w1 and w2 are equal or are inverses, continue
if w1 == w2 or (not isinstance(w1, tuple)
and w1**-1 == w2):
continue
# if the start of one word is the inverse of the
# end of the other, their multiple should be added
# to _min_words because of cancellation
if isinstance(w1, tuple):
# start, end
s1, s2 = w1[0][0], w1[0][0]**-1
else:
s1, s2 = w1[0], w1[len(w1)-1]
if isinstance(w2, tuple):
# start, end
r1, r2 = w2[0][0], w2[0][0]**-1
else:
r1, r2 = w2[0], w2[len(w1)-1]
# p1 and p2 are w1 and w2 or, in case when
# w1 or w2 is an infinite family, a representative
p1, p2 = w1, w2
if isinstance(w1, tuple):
p1 = w1[0]*w1[1]*w1[0]**-1
if isinstance(w2, tuple):
p2 = w2[0]*w2[1]*w2[0]**-1
# add the product of the words to the list is necessary
if r1**-1 == s2 and not (p1*p2).is_identity:
new = _process(p1*p2)
if not new in gens:
gens.extend(new)
if r2**-1 == s1 and not (p2*p1).is_identity:
new = _process(p2*p1)
if not new in gens:
gens.extend(new)
self._min_words = gens
min_words = self._min_words
def _is_subword(w):
# check if w is a word in _min_words or one of
# the infinite families in it
w, r = w.cyclic_reduction(removed=True)
if r.is_identity or self.normal:
return w in min_words
else:
t = [s[1] for s in min_words if isinstance(s, tuple)
and s[0] == r]
return [s for s in t if w.power_of(s)] != []
# store the solution of words for which the result of
# _word_break (below) is known
known = {}
def _word_break(w):
# check if w can be written as a product of words
# in min_words
if len(w) == 0:
return True
i = 0
while i < len(w):
i += 1
prefix = w.subword(0, i)
if not _is_subword(prefix):
continue
rest = w.subword(i, len(w))
if rest not in known:
known[rest] = _word_break(rest)
if known[rest]:
return True
return False
if self.normal:
g = g.cyclic_reduction()
return _word_break(g)
else:
if self.C is None:
C = self.parent.coset_enumeration(self.generators)
self.C = C
i = 0
C = self.C
for j in range(len(g)):
i = C.table[i][C.A_dict[g[j]]]
return i == 0
def order(self):
from sympy import S
if not self.generators:
return 1
if isinstance(self.parent, FreeGroup):
return S.Infinity
if self.C is None:
C = self.parent.coset_enumeration(self.generators)
self.C = C
# This is valid because `len(self.C.table)` (the index of the subgroup)
# will always be finite - otherwise coset enumeration doesn't terminate
return self.parent.order()/len(self.C.table)
def to_FpGroup(self):
if isinstance(self.parent, FreeGroup):
gen_syms = [('x_%d'%i) for i in range(len(self.generators))]
return free_group(', '.join(gen_syms))[0]
return self.parent.subgroup(C=self.C)
def __str__(self):
if len(self.generators) > 30:
str_form = "<fp subgroup with %s generators>" % len(self.generators)
else:
str_form = "<fp subgroup on the generators %s>" % str(self.generators)
return str_form
__repr__ = __str__
###############################################################################
# LOW INDEX SUBGROUPS #
###############################################################################
def low_index_subgroups(G, N, Y=[]):
"""
Implements the Low Index Subgroups algorithm, i.e find all subgroups of
``G`` upto a given index ``N``. This implements the method described in
[Sim94]. This procedure involves a backtrack search over incomplete Coset
Tables, rather than over forced coincidences.
Parameters
==========
G: An FpGroup < X|R >
N: positive integer, representing the maximum index value for subgroups
Y: (an optional argument) specifying a list of subgroup generators, such
that each of the resulting subgroup contains the subgroup generated by Y.
Examples
========
>>> from sympy.combinatorics.free_groups import free_group
>>> from sympy.combinatorics.fp_groups import FpGroup, low_index_subgroups
>>> F, x, y = free_group("x, y")
>>> f = FpGroup(F, [x**2, y**3, (x*y)**4])
>>> L = low_index_subgroups(f, 4)
>>> for coset_table in L:
... print(coset_table.table)
[[0, 0, 0, 0]]
[[0, 0, 1, 2], [1, 1, 2, 0], [3, 3, 0, 1], [2, 2, 3, 3]]
[[0, 0, 1, 2], [2, 2, 2, 0], [1, 1, 0, 1]]
[[1, 1, 0, 0], [0, 0, 1, 1]]
References
==========
.. [1] Holt, D., Eick, B., O'Brien, E.
"Handbook of Computational Group Theory"
Section 5.4
.. [2] Marston Conder and Peter Dobcsanyi
"Applications and Adaptions of the Low Index Subgroups Procedure"
"""
C = CosetTable(G, [])
R = G.relators
# length chosen for the length of the short relators
len_short_rel = 5
# elements of R2 only checked at the last step for complete
# coset tables
R2 = set([rel for rel in R if len(rel) > len_short_rel])
# elements of R1 are used in inner parts of the process to prune
# branches of the search tree,
R1 = set([rel.identity_cyclic_reduction() for rel in set(R) - R2])
R1_c_list = C.conjugates(R1)
S = []
descendant_subgroups(S, C, R1_c_list, C.A[0], R2, N, Y)
return S
def descendant_subgroups(S, C, R1_c_list, x, R2, N, Y):
A_dict = C.A_dict
A_dict_inv = C.A_dict_inv
if C.is_complete():
# if C is complete then it only needs to test
# whether the relators in R2 are satisfied
for w, alpha in product(R2, C.omega):
if not C.scan_check(alpha, w):
return
# relators in R2 are satisfied, append the table to list
S.append(C)
else:
# find the first undefined entry in Coset Table
for alpha, x in product(range(len(C.table)), C.A):
if C.table[alpha][A_dict[x]] is None:
# this is "x" in pseudo-code (using "y" makes it clear)
undefined_coset, undefined_gen = alpha, x
break
# for filling up the undefine entry we try all possible values
# of beta in Omega or beta = n where beta^(undefined_gen^-1) is undefined
reach = C.omega + [C.n]
for beta in reach:
if beta < N:
if beta == C.n or C.table[beta][A_dict_inv[undefined_gen]] is None:
try_descendant(S, C, R1_c_list, R2, N, undefined_coset, \
undefined_gen, beta, Y)
def try_descendant(S, C, R1_c_list, R2, N, alpha, x, beta, Y):
r"""
Solves the problem of trying out each individual possibility
for `\alpha^x.
"""
D = C.copy()
if beta == D.n and beta < N:
D.table.append([None]*len(D.A))
D.p.append(beta)
D.table[alpha][D.A_dict[x]] = beta
D.table[beta][D.A_dict_inv[x]] = alpha
D.deduction_stack.append((alpha, x))
if not D.process_deductions_check(R1_c_list[D.A_dict[x]], \
R1_c_list[D.A_dict_inv[x]]):
return
for w in Y:
if not D.scan_check(0, w):
return
if first_in_class(D, Y):
descendant_subgroups(S, D, R1_c_list, x, R2, N, Y)
def first_in_class(C, Y=[]):
"""
Checks whether the subgroup ``H=G1`` corresponding to the Coset Table
could possibly be the canonical representative of its conjugacy class.
Parameters
==========
C: CosetTable
Returns
=======
bool: True/False
If this returns False, then no descendant of C can have that property, and
so we can abandon C. If it returns True, then we need to process further
the node of the search tree corresponding to C, and so we call
``descendant_subgroups`` recursively on C.
Examples
========
>>> from sympy.combinatorics.free_groups import free_group
>>> from sympy.combinatorics.fp_groups import FpGroup, CosetTable, first_in_class
>>> F, x, y = free_group("x, y")
>>> f = FpGroup(F, [x**2, y**3, (x*y)**4])
>>> C = CosetTable(f, [])
>>> C.table = [[0, 0, None, None]]
>>> first_in_class(C)
True
>>> C.table = [[1, 1, 1, None], [0, 0, None, 1]]; C.p = [0, 1]
>>> first_in_class(C)
True
>>> C.table = [[1, 1, 2, 1], [0, 0, 0, None], [None, None, None, 0]]
>>> C.p = [0, 1, 2]
>>> first_in_class(C)
False
>>> C.table = [[1, 1, 1, 2], [0, 0, 2, 0], [2, None, 0, 1]]
>>> first_in_class(C)
False
# TODO:: Sims points out in [Sim94] that performance can be improved by
# remembering some of the information computed by ``first_in_class``. If
# the ``continue alpha`` statement is executed at line 14, then the same thing
# will happen for that value of alpha in any descendant of the table C, and so
# the values the values of alpha for which this occurs could profitably be
# stored and passed through to the descendants of C. Of course this would
# make the code more complicated.
# The code below is taken directly from the function on page 208 of [Sim94]
# nu[alpha]
"""
n = C.n
# lamda is the largest numbered point in Omega_c_alpha which is currently defined
lamda = -1
# for alpha in Omega_c, nu[alpha] is the point in Omega_c_alpha corresponding to alpha
nu = [None]*n
# for alpha in Omega_c_alpha, mu[alpha] is the point in Omega_c corresponding to alpha
mu = [None]*n
# mutually nu and mu are the mutually-inverse equivalence maps between
# Omega_c_alpha and Omega_c
next_alpha = False
# For each 0!=alpha in [0 .. nc-1], we start by constructing the equivalent
# standardized coset table C_alpha corresponding to H_alpha
for alpha in range(1, n):
# reset nu to "None" after previous value of alpha
for beta in range(lamda+1):
nu[mu[beta]] = None
# we only want to reject our current table in favour of a preceding
# table in the ordering in which 1 is replaced by alpha, if the subgroup
# G_alpha corresponding to this preceding table definitely contains the
# given subgroup
for w in Y:
# TODO: this should support input of a list of general words
# not just the words which are in "A" (i.e gen and gen^-1)
if C.table[alpha][C.A_dict[w]] != alpha:
# continue with alpha
next_alpha = True
break
if next_alpha:
next_alpha = False
continue
# try alpha as the new point 0 in Omega_C_alpha
mu[0] = alpha
nu[alpha] = 0
# compare corresponding entries in C and C_alpha
lamda = 0
for beta in range(n):
for x in C.A:
gamma = C.table[beta][C.A_dict[x]]
delta = C.table[mu[beta]][C.A_dict[x]]
# if either of the entries is undefined,
# we move with next alpha
if gamma is None or delta is None:
# continue with alpha
next_alpha = True
break
if nu[delta] is None:
# delta becomes the next point in Omega_C_alpha
lamda += 1
nu[delta] = lamda
mu[lamda] = delta
if nu[delta] < gamma:
return False
if nu[delta] > gamma:
# continue with alpha
next_alpha = True
break
if next_alpha:
next_alpha = False
break
return True
#========================================================================
# Simplifying Presentation
#========================================================================
def simplify_presentation(*args, **kwargs):
'''
For an instance of `FpGroup`, return a simplified isomorphic copy of
the group (e.g. remove redundant generators or relators). Alternatively,
a list of generators and relators can be passed in which case the
simplified lists will be returned.
By default, the generators of the group are unchanged. If you would
like to remove redundant generators, set the keyword argument
`change_gens = True`.
'''
change_gens = kwargs.get("change_gens", False)
if len(args) == 1:
if not isinstance(args[0], FpGroup):
raise TypeError("The argument must be an instance of FpGroup")
G = args[0]
gens, rels = simplify_presentation(G.generators, G.relators,
change_gens=change_gens)
if gens:
return FpGroup(gens[0].group, rels)
return FpGroup(FreeGroup([]), [])
elif len(args) == 2:
gens, rels = args[0][:], args[1][:]
if not gens:
return gens, rels
identity = gens[0].group.identity
else:
if len(args) == 0:
m = "Not enough arguments"
else:
m = "Too many arguments"
raise RuntimeError(m)
prev_gens = []
prev_rels = []
while not set(prev_rels) == set(rels):
prev_rels = rels
while change_gens and not set(prev_gens) == set(gens):
prev_gens = gens
gens, rels = elimination_technique_1(gens, rels, identity)
rels = _simplify_relators(rels, identity)
if change_gens:
syms = [g.array_form[0][0] for g in gens]
F = free_group(syms)[0]
identity = F.identity
gens = F.generators
subs = dict(zip(syms, gens))
for j, r in enumerate(rels):
a = r.array_form
rel = identity
for sym, p in a:
rel = rel*subs[sym]**p
rels[j] = rel
return gens, rels
def _simplify_relators(rels, identity):
"""Relies upon ``_simplification_technique_1`` for its functioning. """
rels = rels[:]
rels = list(set(_simplification_technique_1(rels)))
rels.sort()
rels = [r.identity_cyclic_reduction() for r in rels]
try:
rels.remove(identity)
except ValueError:
pass
return rels
# Pg 350, section 2.5.1 from [2]
def elimination_technique_1(gens, rels, identity):
rels = rels[:]
# the shorter relators are examined first so that generators selected for
# elimination will have shorter strings as equivalent
rels.sort()
gens = gens[:]
redundant_gens = {}
redundant_rels = []
used_gens = set()
# examine each relator in relator list for any generator occurring exactly
# once
for rel in rels:
# don't look for a redundant generator in a relator which
# depends on previously found ones
contained_gens = rel.contains_generators()
if any([g in contained_gens for g in redundant_gens]):
continue
contained_gens = list(contained_gens)
contained_gens.sort(reverse = True)
for gen in contained_gens:
if rel.generator_count(gen) == 1 and gen not in used_gens:
k = rel.exponent_sum(gen)
gen_index = rel.index(gen**k)
bk = rel.subword(gen_index + 1, len(rel))
fw = rel.subword(0, gen_index)
chi = bk*fw
redundant_gens[gen] = chi**(-1*k)
used_gens.update(chi.contains_generators())
redundant_rels.append(rel)
break
rels = [r for r in rels if r not in redundant_rels]
# eliminate the redundant generators from remaining relators
rels = [r.eliminate_words(redundant_gens, _all = True).identity_cyclic_reduction() for r in rels]
rels = list(set(rels))
try:
rels.remove(identity)
except ValueError:
pass
gens = [g for g in gens if g not in redundant_gens]
return gens, rels
def _simplification_technique_1(rels):
"""
All relators are checked to see if they are of the form `gen^n`. If any
such relators are found then all other relators are processed for strings
in the `gen` known order.
Examples
========
>>> from sympy.combinatorics.free_groups import free_group
>>> from sympy.combinatorics.fp_groups import _simplification_technique_1
>>> F, x, y = free_group("x, y")
>>> w1 = [x**2*y**4, x**3]
>>> _simplification_technique_1(w1)
[x**-1*y**4, x**3]
>>> w2 = [x**2*y**-4*x**5, x**3, x**2*y**8, y**5]
>>> _simplification_technique_1(w2)
[x**-1*y*x**-1, x**3, x**-1*y**-2, y**5]
>>> w3 = [x**6*y**4, x**4]
>>> _simplification_technique_1(w3)
[x**2*y**4, x**4]
"""
from sympy import gcd
rels = rels[:]
# dictionary with "gen: n" where gen^n is one of the relators
exps = {}
for i in range(len(rels)):
rel = rels[i]
if rel.number_syllables() == 1:
g = rel[0]
exp = abs(rel.array_form[0][1])
if rel.array_form[0][1] < 0:
rels[i] = rels[i]**-1
g = g**-1
if g in exps:
exp = gcd(exp, exps[g].array_form[0][1])
exps[g] = g**exp
one_syllables_words = exps.values()
# decrease some of the exponents in relators, making use of the single
# syllable relators
for i in range(len(rels)):
rel = rels[i]
if rel in one_syllables_words:
continue
rel = rel.eliminate_words(one_syllables_words, _all = True)
# if rels[i] contains g**n where abs(n) is greater than half of the power p
# of g in exps, g**n can be replaced by g**(n-p) (or g**(p-n) if n<0)
for g in rel.contains_generators():
if g in exps:
exp = exps[g].array_form[0][1]
max_exp = (exp + 1)//2
rel = rel.eliminate_word(g**(max_exp), g**(max_exp-exp), _all = True)
rel = rel.eliminate_word(g**(-max_exp), g**(-(max_exp-exp)), _all = True)
rels[i] = rel
rels = [r.identity_cyclic_reduction() for r in rels]
return rels
###############################################################################
# SUBGROUP PRESENTATIONS #
###############################################################################
# Pg 175 [1]
def define_schreier_generators(C, homomorphism=False):
'''
Parameters
==========
C -- Coset table.
homomorphism -- When set to True, return a dictionary containing the images
of the presentation generators in the original group.
'''
y = []
gamma = 1
f = C.fp_group
X = f.generators
if homomorphism:
# `_gens` stores the elements of the parent group to
# to which the schreier generators correspond to.
_gens = {}
# compute the schreier Traversal
tau = {}
tau[0] = f.identity
C.P = [[None]*len(C.A) for i in range(C.n)]
for alpha, x in product(C.omega, C.A):
beta = C.table[alpha][C.A_dict[x]]
if beta == gamma:
C.P[alpha][C.A_dict[x]] = "<identity>"
C.P[beta][C.A_dict_inv[x]] = "<identity>"
gamma += 1
if homomorphism:
tau[beta] = tau[alpha]*x
elif x in X and C.P[alpha][C.A_dict[x]] is None:
y_alpha_x = '%s_%s' % (x, alpha)
y.append(y_alpha_x)
C.P[alpha][C.A_dict[x]] = y_alpha_x
if homomorphism:
_gens[y_alpha_x] = tau[alpha]*x*tau[beta]**-1
grp_gens = list(free_group(', '.join(y)))
C._schreier_free_group = grp_gens.pop(0)
C._schreier_generators = grp_gens
if homomorphism:
C._schreier_gen_elem = _gens
# replace all elements of P by, free group elements
for i, j in product(range(len(C.P)), range(len(C.A))):
# if equals "<identity>", replace by identity element
if C.P[i][j] == "<identity>":
C.P[i][j] = C._schreier_free_group.identity
elif isinstance(C.P[i][j], string_types):
r = C._schreier_generators[y.index(C.P[i][j])]
C.P[i][j] = r
beta = C.table[i][j]
C.P[beta][j + 1] = r**-1
def reidemeister_relators(C):
R = C.fp_group.relators
rels = [rewrite(C, coset, word) for word in R for coset in range(C.n)]
order_1_gens = set([i for i in rels if len(i) == 1])
# remove all the order 1 generators from relators
rels = list(filter(lambda rel: rel not in order_1_gens, rels))
# replace order 1 generators by identity element in reidemeister relators
for i in range(len(rels)):
w = rels[i]
w = w.eliminate_words(order_1_gens, _all=True)
rels[i] = w
C._schreier_generators = [i for i in C._schreier_generators
if not (i in order_1_gens or i**-1 in order_1_gens)]
# Tietze transformation 1 i.e TT_1
# remove cyclic conjugate elements from relators
i = 0
while i < len(rels):
w = rels[i]
j = i + 1
while j < len(rels):
if w.is_cyclic_conjugate(rels[j]):
del rels[j]
else:
j += 1
i += 1
C._reidemeister_relators = rels
def rewrite(C, alpha, w):
"""
Parameters
==========
C: CosetTable
alpha: A live coset
w: A word in `A*`
Returns
=======
rho(tau(alpha), w)
Examples
========
>>> from sympy.combinatorics.fp_groups import FpGroup, CosetTable, define_schreier_generators, rewrite
>>> from sympy.combinatorics.free_groups import free_group
>>> F, x, y = free_group("x ,y")
>>> f = FpGroup(F, [x**2, y**3, (x*y)**6])
>>> C = CosetTable(f, [])
>>> C.table = [[1, 1, 2, 3], [0, 0, 4, 5], [4, 4, 3, 0], [5, 5, 0, 2], [2, 2, 5, 1], [3, 3, 1, 4]]
>>> C.p = [0, 1, 2, 3, 4, 5]
>>> define_schreier_generators(C)
>>> rewrite(C, 0, (x*y)**6)
x_4*y_2*x_3*x_1*x_2*y_4*x_5
"""
v = C._schreier_free_group.identity
for i in range(len(w)):
x_i = w[i]
v = v*C.P[alpha][C.A_dict[x_i]]
alpha = C.table[alpha][C.A_dict[x_i]]
return v
# Pg 350, section 2.5.2 from [2]
def elimination_technique_2(C):
"""
This technique eliminates one generator at a time. Heuristically this
seems superior in that we may select for elimination the generator with
shortest equivalent string at each stage.
>>> from sympy.combinatorics.free_groups import free_group
>>> from sympy.combinatorics.fp_groups import FpGroup, coset_enumeration_r, \
reidemeister_relators, define_schreier_generators, elimination_technique_2
>>> F, x, y = free_group("x, y")
>>> f = FpGroup(F, [x**3, y**5, (x*y)**2]); H = [x*y, x**-1*y**-1*x*y*x]
>>> C = coset_enumeration_r(f, H)
>>> C.compress(); C.standardize()
>>> define_schreier_generators(C)
>>> reidemeister_relators(C)
>>> elimination_technique_2(C)
([y_1, y_2], [y_2**-3, y_2*y_1*y_2*y_1*y_2*y_1, y_1**2])
"""
rels = C._reidemeister_relators
rels.sort(reverse=True)
gens = C._schreier_generators
for i in range(len(gens) - 1, -1, -1):
rel = rels[i]
for j in range(len(gens) - 1, -1, -1):
gen = gens[j]
if rel.generator_count(gen) == 1:
k = rel.exponent_sum(gen)
gen_index = rel.index(gen**k)
bk = rel.subword(gen_index + 1, len(rel))
fw = rel.subword(0, gen_index)
rep_by = (bk*fw)**(-1*k)
del rels[i]; del gens[j]
for l in range(len(rels)):
rels[l] = rels[l].eliminate_word(gen, rep_by)
break
C._reidemeister_relators = rels
C._schreier_generators = gens
return C._schreier_generators, C._reidemeister_relators
def reidemeister_presentation(fp_grp, H, C=None, homomorphism=False):
"""
Parameters
==========
fp_group: A finitely presented group, an instance of FpGroup
H: A subgroup whose presentation is to be found, given as a list
of words in generators of `fp_grp`
homomorphism: When set to True, return a homomorphism from the subgroup
to the parent group
Examples
========
>>> from sympy.combinatorics.free_groups import free_group
>>> from sympy.combinatorics.fp_groups import FpGroup, reidemeister_presentation
>>> F, x, y = free_group("x, y")
Example 5.6 Pg. 177 from [1]
>>> f = FpGroup(F, [x**3, y**5, (x*y)**2])
>>> H = [x*y, x**-1*y**-1*x*y*x]
>>> reidemeister_presentation(f, H)
((y_1, y_2), (y_1**2, y_2**3, y_2*y_1*y_2*y_1*y_2*y_1))
Example 5.8 Pg. 183 from [1]
>>> f = FpGroup(F, [x**3, y**3, (x*y)**3])
>>> H = [x*y, x*y**-1]
>>> reidemeister_presentation(f, H)
((x_0, y_0), (x_0**3, y_0**3, x_0*y_0*x_0*y_0*x_0*y_0))
Exercises Q2. Pg 187 from [1]
>>> f = FpGroup(F, [x**2*y**2, y**-1*x*y*x**-3])
>>> H = [x]
>>> reidemeister_presentation(f, H)
((x_0,), (x_0**4,))
Example 5.9 Pg. 183 from [1]
>>> f = FpGroup(F, [x**3*y**-3, (x*y)**3, (x*y**-1)**2])
>>> H = [x]
>>> reidemeister_presentation(f, H)
((x_0,), (x_0**6,))
"""
if not C:
C = coset_enumeration_r(fp_grp, H)
C.compress(); C.standardize()
define_schreier_generators(C, homomorphism=homomorphism)
reidemeister_relators(C)
gens, rels = C._schreier_generators, C._reidemeister_relators
gens, rels = simplify_presentation(gens, rels, change_gens=True)
C.schreier_generators = tuple(gens)
C.reidemeister_relators = tuple(rels)
if homomorphism:
_gens = []
for gen in gens:
_gens.append(C._schreier_gen_elem[str(gen)])
return C.schreier_generators, C.reidemeister_relators, _gens
return C.schreier_generators, C.reidemeister_relators
FpGroupElement = FreeGroupElement
|
9ffa86e67736608508e59975ffba4e089343243698461bfbcab6e940b612123c | """
This module implements sums and products containing the Kronecker Delta function.
References
==========
- http://mathworld.wolfram.com/KroneckerDelta.html
"""
from __future__ import print_function, division
from sympy.core import Add, Mul, S, Dummy
from sympy.core.cache import cacheit
from sympy.core.compatibility import default_sort_key, range
from sympy.functions import KroneckerDelta, Piecewise, piecewise_fold
from sympy.sets import Interval
@cacheit
def _expand_delta(expr, index):
"""
Expand the first Add containing a simple KroneckerDelta.
"""
if not expr.is_Mul:
return expr
delta = None
func = Add
terms = [S.One]
for h in expr.args:
if delta is None and h.is_Add and _has_simple_delta(h, index):
delta = True
func = h.func
terms = [terms[0]*t for t in h.args]
else:
terms = [t*h for t in terms]
return func(*terms)
@cacheit
def _extract_delta(expr, index):
"""
Extract a simple KroneckerDelta from the expression.
Returns the tuple ``(delta, newexpr)`` where:
- ``delta`` is a simple KroneckerDelta expression if one was found,
or ``None`` if no simple KroneckerDelta expression was found.
- ``newexpr`` is a Mul containing the remaining terms; ``expr`` is
returned unchanged if no simple KroneckerDelta expression was found.
Examples
========
>>> from sympy import KroneckerDelta
>>> from sympy.concrete.delta import _extract_delta
>>> from sympy.abc import x, y, i, j, k
>>> _extract_delta(4*x*y*KroneckerDelta(i, j), i)
(KroneckerDelta(i, j), 4*x*y)
>>> _extract_delta(4*x*y*KroneckerDelta(i, j), k)
(None, 4*x*y*KroneckerDelta(i, j))
See Also
========
sympy.functions.special.tensor_functions.KroneckerDelta
deltaproduct
deltasummation
"""
if not _has_simple_delta(expr, index):
return (None, expr)
if isinstance(expr, KroneckerDelta):
return (expr, S.One)
if not expr.is_Mul:
raise ValueError("Incorrect expr")
delta = None
terms = []
for arg in expr.args:
if delta is None and _is_simple_delta(arg, index):
delta = arg
else:
terms.append(arg)
return (delta, expr.func(*terms))
@cacheit
def _has_simple_delta(expr, index):
"""
Returns True if ``expr`` is an expression that contains a KroneckerDelta
that is simple in the index ``index``, meaning that this KroneckerDelta
is nonzero for a single value of the index ``index``.
"""
if expr.has(KroneckerDelta):
if _is_simple_delta(expr, index):
return True
if expr.is_Add or expr.is_Mul:
for arg in expr.args:
if _has_simple_delta(arg, index):
return True
return False
@cacheit
def _is_simple_delta(delta, index):
"""
Returns True if ``delta`` is a KroneckerDelta and is nonzero for a single
value of the index ``index``.
"""
if isinstance(delta, KroneckerDelta) and delta.has(index):
p = (delta.args[0] - delta.args[1]).as_poly(index)
if p:
return p.degree() == 1
return False
@cacheit
def _remove_multiple_delta(expr):
"""
Evaluate products of KroneckerDelta's.
"""
from sympy.solvers import solve
if expr.is_Add:
return expr.func(*list(map(_remove_multiple_delta, expr.args)))
if not expr.is_Mul:
return expr
eqs = []
newargs = []
for arg in expr.args:
if isinstance(arg, KroneckerDelta):
eqs.append(arg.args[0] - arg.args[1])
else:
newargs.append(arg)
if not eqs:
return expr
solns = solve(eqs, dict=True)
if len(solns) == 0:
return S.Zero
elif len(solns) == 1:
for key in solns[0].keys():
newargs.append(KroneckerDelta(key, solns[0][key]))
expr2 = expr.func(*newargs)
if expr != expr2:
return _remove_multiple_delta(expr2)
return expr
@cacheit
def _simplify_delta(expr):
"""
Rewrite a KroneckerDelta's indices in its simplest form.
"""
from sympy.solvers import solve
if isinstance(expr, KroneckerDelta):
try:
slns = solve(expr.args[0] - expr.args[1], dict=True)
if slns and len(slns) == 1:
return Mul(*[KroneckerDelta(*(key, value))
for key, value in slns[0].items()])
except NotImplementedError:
pass
return expr
@cacheit
def deltaproduct(f, limit):
"""
Handle products containing a KroneckerDelta.
See Also
========
deltasummation
sympy.functions.special.tensor_functions.KroneckerDelta
sympy.concrete.products.product
"""
from sympy.concrete.products import product
if ((limit[2] - limit[1]) < 0) == True:
return S.One
if not f.has(KroneckerDelta):
return product(f, limit)
if f.is_Add:
# Identify the term in the Add that has a simple KroneckerDelta
delta = None
terms = []
for arg in sorted(f.args, key=default_sort_key):
if delta is None and _has_simple_delta(arg, limit[0]):
delta = arg
else:
terms.append(arg)
newexpr = f.func(*terms)
k = Dummy("kprime", integer=True)
if isinstance(limit[1], int) and isinstance(limit[2], int):
result = deltaproduct(newexpr, limit) + sum([
deltaproduct(newexpr, (limit[0], limit[1], ik - 1)) *
delta.subs(limit[0], ik) *
deltaproduct(newexpr, (limit[0], ik + 1, limit[2])) for ik in range(int(limit[1]), int(limit[2] + 1))]
)
else:
result = deltaproduct(newexpr, limit) + deltasummation(
deltaproduct(newexpr, (limit[0], limit[1], k - 1)) *
delta.subs(limit[0], k) *
deltaproduct(newexpr, (limit[0], k + 1, limit[2])),
(k, limit[1], limit[2]),
no_piecewise=_has_simple_delta(newexpr, limit[0])
)
return _remove_multiple_delta(result)
delta, _ = _extract_delta(f, limit[0])
if not delta:
g = _expand_delta(f, limit[0])
if f != g:
from sympy import factor
try:
return factor(deltaproduct(g, limit))
except AssertionError:
return deltaproduct(g, limit)
return product(f, limit)
return _remove_multiple_delta(f.subs(limit[0], limit[1])*KroneckerDelta(limit[2], limit[1])) + \
S.One*_simplify_delta(KroneckerDelta(limit[2], limit[1] - 1))
@cacheit
def deltasummation(f, limit, no_piecewise=False):
"""
Handle summations containing a KroneckerDelta.
The idea for summation is the following:
- If we are dealing with a KroneckerDelta expression, i.e. KroneckerDelta(g(x), j),
we try to simplify it.
If we could simplify it, then we sum the resulting expression.
We already know we can sum a simplified expression, because only
simple KroneckerDelta expressions are involved.
If we couldn't simplify it, there are two cases:
1) The expression is a simple expression: we return the summation,
taking care if we are dealing with a Derivative or with a proper
KroneckerDelta.
2) The expression is not simple (i.e. KroneckerDelta(cos(x))): we can do
nothing at all.
- If the expr is a multiplication expr having a KroneckerDelta term:
First we expand it.
If the expansion did work, then we try to sum the expansion.
If not, we try to extract a simple KroneckerDelta term, then we have two
cases:
1) We have a simple KroneckerDelta term, so we return the summation.
2) We didn't have a simple term, but we do have an expression with
simplified KroneckerDelta terms, so we sum this expression.
Examples
========
>>> from sympy import oo, symbols
>>> from sympy.abc import k
>>> i, j = symbols('i, j', integer=True, finite=True)
>>> from sympy.concrete.delta import deltasummation
>>> from sympy import KroneckerDelta, Piecewise
>>> deltasummation(KroneckerDelta(i, k), (k, -oo, oo))
1
>>> deltasummation(KroneckerDelta(i, k), (k, 0, oo))
Piecewise((1, i >= 0), (0, True))
>>> deltasummation(KroneckerDelta(i, k), (k, 1, 3))
Piecewise((1, (i >= 1) & (i <= 3)), (0, True))
>>> deltasummation(k*KroneckerDelta(i, j)*KroneckerDelta(j, k), (k, -oo, oo))
j*KroneckerDelta(i, j)
>>> deltasummation(j*KroneckerDelta(i, j), (j, -oo, oo))
i
>>> deltasummation(i*KroneckerDelta(i, j), (i, -oo, oo))
j
See Also
========
deltaproduct
sympy.functions.special.tensor_functions.KroneckerDelta
sympy.concrete.sums.summation
"""
from sympy.concrete.summations import summation
from sympy.solvers import solve
if ((limit[2] - limit[1]) < 0) == True:
return S.Zero
if not f.has(KroneckerDelta):
return summation(f, limit)
x = limit[0]
g = _expand_delta(f, x)
if g.is_Add:
return piecewise_fold(
g.func(*[deltasummation(h, limit, no_piecewise) for h in g.args]))
# try to extract a simple KroneckerDelta term
delta, expr = _extract_delta(g, x)
if (delta is not None) and (delta.delta_range is not None):
dinf, dsup = delta.delta_range
if (limit[1] - dinf <= 0) == True and (limit[2] - dsup >= 0) == True:
no_piecewise = True
if not delta:
return summation(f, limit)
solns = solve(delta.args[0] - delta.args[1], x)
if len(solns) == 0:
return S.Zero
elif len(solns) != 1:
from sympy.concrete.summations import Sum
return Sum(f, limit)
value = solns[0]
if no_piecewise:
return expr.subs(x, value)
return Piecewise(
(expr.subs(x, value), Interval(*limit[1:3]).as_relational(value)),
(S.Zero, True)
)
|
6db6ad703dbc7f11c58504bebb4f1d509bc5c4a799df3e00794c7cdd478d3a32 | """Gosper's algorithm for hypergeometric summation. """
from __future__ import print_function, division
from sympy.core import S, Dummy, symbols
from sympy.core.compatibility import is_sequence, range
from sympy.polys import Poly, parallel_poly_from_expr, factor
from sympy.solvers import solve
from sympy.simplify import hypersimp
def gosper_normal(f, g, n, polys=True):
r"""
Compute the Gosper's normal form of ``f`` and ``g``.
Given relatively prime univariate polynomials ``f`` and ``g``,
rewrite their quotient to a normal form defined as follows:
.. math::
\frac{f(n)}{g(n)} = Z \cdot \frac{A(n) C(n+1)}{B(n) C(n)}
where ``Z`` is an arbitrary constant and ``A``, ``B``, ``C`` are
monic polynomials in ``n`` with the following properties:
1. `\gcd(A(n), B(n+h)) = 1 \forall h \in \mathbb{N}`
2. `\gcd(B(n), C(n+1)) = 1`
3. `\gcd(A(n), C(n)) = 1`
This normal form, or rational factorization in other words, is a
crucial step in Gosper's algorithm and in solving of difference
equations. It can be also used to decide if two hypergeometric
terms are similar or not.
This procedure will return a tuple containing elements of this
factorization in the form ``(Z*A, B, C)``.
Examples
========
>>> from sympy.concrete.gosper import gosper_normal
>>> from sympy.abc import n
>>> gosper_normal(4*n+5, 2*(4*n+1)*(2*n+3), n, polys=False)
(1/4, n + 3/2, n + 1/4)
"""
(p, q), opt = parallel_poly_from_expr(
(f, g), n, field=True, extension=True)
a, A = p.LC(), p.monic()
b, B = q.LC(), q.monic()
C, Z = A.one, a/b
h = Dummy('h')
D = Poly(n + h, n, h, domain=opt.domain)
R = A.resultant(B.compose(D))
roots = set(R.ground_roots().keys())
for r in set(roots):
if not r.is_Integer or r < 0:
roots.remove(r)
for i in sorted(roots):
d = A.gcd(B.shift(+i))
A = A.quo(d)
B = B.quo(d.shift(-i))
for j in range(1, i + 1):
C *= d.shift(-j)
A = A.mul_ground(Z)
if not polys:
A = A.as_expr()
B = B.as_expr()
C = C.as_expr()
return A, B, C
def gosper_term(f, n):
r"""
Compute Gosper's hypergeometric term for ``f``.
Suppose ``f`` is a hypergeometric term such that:
.. math::
s_n = \sum_{k=0}^{n-1} f_k
and `f_k` doesn't depend on `n`. Returns a hypergeometric
term `g_n` such that `g_{n+1} - g_n = f_n`.
Examples
========
>>> from sympy.concrete.gosper import gosper_term
>>> from sympy.functions import factorial
>>> from sympy.abc import n
>>> gosper_term((4*n + 1)*factorial(n)/factorial(2*n + 1), n)
(-n - 1/2)/(n + 1/4)
"""
r = hypersimp(f, n)
if r is None:
return None # 'f' is *not* a hypergeometric term
p, q = r.as_numer_denom()
A, B, C = gosper_normal(p, q, n)
B = B.shift(-1)
N = S(A.degree())
M = S(B.degree())
K = S(C.degree())
if (N != M) or (A.LC() != B.LC()):
D = {K - max(N, M)}
elif not N:
D = {K - N + 1, S.Zero}
else:
D = {K - N + 1, (B.nth(N - 1) - A.nth(N - 1))/A.LC()}
for d in set(D):
if not d.is_Integer or d < 0:
D.remove(d)
if not D:
return None # 'f(n)' is *not* Gosper-summable
d = max(D)
coeffs = symbols('c:%s' % (d + 1), cls=Dummy)
domain = A.get_domain().inject(*coeffs)
x = Poly(coeffs, n, domain=domain)
H = A*x.shift(1) - B*x - C
solution = solve(H.coeffs(), coeffs)
if solution is None:
return None # 'f(n)' is *not* Gosper-summable
x = x.as_expr().subs(solution)
for coeff in coeffs:
if coeff not in solution:
x = x.subs(coeff, 0)
if x.is_zero:
return None # 'f(n)' is *not* Gosper-summable
else:
return B.as_expr()*x/C.as_expr()
def gosper_sum(f, k):
r"""
Gosper's hypergeometric summation algorithm.
Given a hypergeometric term ``f`` such that:
.. math ::
s_n = \sum_{k=0}^{n-1} f_k
and `f(n)` doesn't depend on `n`, returns `g_{n} - g(0)` where
`g_{n+1} - g_n = f_n`, or ``None`` if `s_n` can not be expressed
in closed form as a sum of hypergeometric terms.
Examples
========
>>> from sympy.concrete.gosper import gosper_sum
>>> from sympy.functions import factorial
>>> from sympy.abc import i, n, k
>>> f = (4*k + 1)*factorial(k)/factorial(2*k + 1)
>>> gosper_sum(f, (k, 0, n))
(-factorial(n) + 2*factorial(2*n + 1))/factorial(2*n + 1)
>>> _.subs(n, 2) == sum(f.subs(k, i) for i in [0, 1, 2])
True
>>> gosper_sum(f, (k, 3, n))
(-60*factorial(n) + factorial(2*n + 1))/(60*factorial(2*n + 1))
>>> _.subs(n, 5) == sum(f.subs(k, i) for i in [3, 4, 5])
True
References
==========
.. [1] Marko Petkovsek, Herbert S. Wilf, Doron Zeilberger, A = B,
AK Peters, Ltd., Wellesley, MA, USA, 1997, pp. 73--100
"""
indefinite = False
if is_sequence(k):
k, a, b = k
else:
indefinite = True
g = gosper_term(f, k)
if g is None:
return None
if indefinite:
result = f*g
else:
result = (f*(g + 1)).subs(k, b) - (f*g).subs(k, a)
if result is S.NaN:
try:
result = (f*(g + 1)).limit(k, b) - (f*g).limit(k, a)
except NotImplementedError:
result = None
return factor(result)
|
e5fcfef9f59e26a42bf422636445c496c939e22cec761462bba93c147dcc9644 | from __future__ import print_function, division
from sympy.calculus.singularities import is_decreasing
from sympy.calculus.util import AccumulationBounds
from sympy.concrete.expr_with_limits import AddWithLimits
from sympy.concrete.expr_with_intlimits import ExprWithIntLimits
from sympy.concrete.gosper import gosper_sum
from sympy.core.add import Add
from sympy.core.compatibility import range
from sympy.core.function import Derivative
from sympy.core.mul import Mul
from sympy.core.relational import Eq
from sympy.core.singleton import S
from sympy.core.symbol import Dummy, Wild, Symbol
from sympy.functions.special.zeta_functions import zeta
from sympy.functions.elementary.piecewise import Piecewise
from sympy.logic.boolalg import And
from sympy.polys import apart, PolynomialError, together
from sympy.series.limitseq import limit_seq
from sympy.series.order import O
from sympy.sets.sets import FiniteSet
from sympy.simplify import denom
from sympy.simplify.combsimp import combsimp
from sympy.simplify.powsimp import powsimp
from sympy.solvers import solve
from sympy.solvers.solveset import solveset
import itertools
class Sum(AddWithLimits, ExprWithIntLimits):
r"""Represents unevaluated summation.
``Sum`` represents a finite or infinite series, with the first argument
being the general form of terms in the series, and the second argument
being ``(dummy_variable, start, end)``, with ``dummy_variable`` taking
all integer values from ``start`` through ``end``. In accordance with
long-standing mathematical convention, the end term is included in the
summation.
Finite sums
===========
For finite sums (and sums with symbolic limits assumed to be finite) we
follow the summation convention described by Karr [1], especially
definition 3 of section 1.4. The sum:
.. math::
\sum_{m \leq i < n} f(i)
has *the obvious meaning* for `m < n`, namely:
.. math::
\sum_{m \leq i < n} f(i) = f(m) + f(m+1) + \ldots + f(n-2) + f(n-1)
with the upper limit value `f(n)` excluded. The sum over an empty set is
zero if and only if `m = n`:
.. math::
\sum_{m \leq i < n} f(i) = 0 \quad \mathrm{for} \quad m = n
Finally, for all other sums over empty sets we assume the following
definition:
.. math::
\sum_{m \leq i < n} f(i) = - \sum_{n \leq i < m} f(i) \quad \mathrm{for} \quad m > n
It is important to note that Karr defines all sums with the upper
limit being exclusive. This is in contrast to the usual mathematical notation,
but does not affect the summation convention. Indeed we have:
.. math::
\sum_{m \leq i < n} f(i) = \sum_{i = m}^{n - 1} f(i)
where the difference in notation is intentional to emphasize the meaning,
with limits typeset on the top being inclusive.
Examples
========
>>> from sympy.abc import i, k, m, n, x
>>> from sympy import Sum, factorial, oo, IndexedBase, Function
>>> Sum(k, (k, 1, m))
Sum(k, (k, 1, m))
>>> Sum(k, (k, 1, m)).doit()
m**2/2 + m/2
>>> Sum(k**2, (k, 1, m))
Sum(k**2, (k, 1, m))
>>> Sum(k**2, (k, 1, m)).doit()
m**3/3 + m**2/2 + m/6
>>> Sum(x**k, (k, 0, oo))
Sum(x**k, (k, 0, oo))
>>> Sum(x**k, (k, 0, oo)).doit()
Piecewise((1/(1 - x), Abs(x) < 1), (Sum(x**k, (k, 0, oo)), True))
>>> Sum(x**k/factorial(k), (k, 0, oo)).doit()
exp(x)
Here are examples to do summation with symbolic indices. You
can use either Function of IndexedBase classes:
>>> f = Function('f')
>>> Sum(f(n), (n, 0, 3)).doit()
f(0) + f(1) + f(2) + f(3)
>>> Sum(f(n), (n, 0, oo)).doit()
Sum(f(n), (n, 0, oo))
>>> f = IndexedBase('f')
>>> Sum(f[n]**2, (n, 0, 3)).doit()
f[0]**2 + f[1]**2 + f[2]**2 + f[3]**2
An example showing that the symbolic result of a summation is still
valid for seemingly nonsensical values of the limits. Then the Karr
convention allows us to give a perfectly valid interpretation to
those sums by interchanging the limits according to the above rules:
>>> S = Sum(i, (i, 1, n)).doit()
>>> S
n**2/2 + n/2
>>> S.subs(n, -4)
6
>>> Sum(i, (i, 1, -4)).doit()
6
>>> Sum(-i, (i, -3, 0)).doit()
6
An explicit example of the Karr summation convention:
>>> S1 = Sum(i**2, (i, m, m+n-1)).doit()
>>> S1
m**2*n + m*n**2 - m*n + n**3/3 - n**2/2 + n/6
>>> S2 = Sum(i**2, (i, m+n, m-1)).doit()
>>> S2
-m**2*n - m*n**2 + m*n - n**3/3 + n**2/2 - n/6
>>> S1 + S2
0
>>> S3 = Sum(i, (i, m, m-1)).doit()
>>> S3
0
See Also
========
summation
Product, product
References
==========
.. [1] Michael Karr, "Summation in Finite Terms", Journal of the ACM,
Volume 28 Issue 2, April 1981, Pages 305-350
http://dl.acm.org/citation.cfm?doid=322248.322255
.. [2] https://en.wikipedia.org/wiki/Summation#Capital-sigma_notation
.. [3] https://en.wikipedia.org/wiki/Empty_sum
"""
__slots__ = ['is_commutative']
def __new__(cls, function, *symbols, **assumptions):
obj = AddWithLimits.__new__(cls, function, *symbols, **assumptions)
if not hasattr(obj, 'limits'):
return obj
if any(len(l) != 3 or None in l for l in obj.limits):
raise ValueError('Sum requires values for lower and upper bounds.')
return obj
def _eval_is_zero(self):
# a Sum is only zero if its function is zero or if all terms
# cancel out. This only answers whether the summand is zero; if
# not then None is returned since we don't analyze whether all
# terms cancel out.
if self.function.is_zero or self.has_empty_sequence:
return True
def _eval_is_extended_real(self):
if self.has_empty_sequence:
return True
return self.function.is_extended_real
def _eval_is_positive(self):
if self.has_finite_limits and self.has_reversed_limits is False:
return self.function.is_positive
def _eval_is_negative(self):
if self.has_finite_limits and self.has_reversed_limits is False:
return self.function.is_negative
def _eval_is_finite(self):
if self.has_finite_limits and self.function.is_finite:
return True
def doit(self, **hints):
if hints.get('deep', True):
f = self.function.doit(**hints)
else:
f = self.function
# first make sure any definite limits have summation
# variables with matching assumptions
reps = {}
for xab in self.limits:
d = _dummy_with_inherited_properties_concrete(xab)
if d:
reps[xab[0]] = d
if reps:
undo = dict([(v, k) for k, v in reps.items()])
did = self.xreplace(reps).doit(**hints)
if type(did) is tuple: # when separate=True
did = tuple([i.xreplace(undo) for i in did])
elif did is not None:
did = did.xreplace(undo)
else:
did = self
return did
if self.function.is_Matrix:
expanded = self.expand()
if self != expanded:
return expanded.doit()
return _eval_matrix_sum(self)
for n, limit in enumerate(self.limits):
i, a, b = limit
dif = b - a
if dif == -1:
# Any summation over an empty set is zero
return S.Zero
if dif.is_integer and dif.is_negative:
a, b = b + 1, a - 1
f = -f
newf = eval_sum(f, (i, a, b))
if newf is None:
if f == self.function:
zeta_function = self.eval_zeta_function(f, (i, a, b))
if zeta_function is not None:
return zeta_function
return self
else:
return self.func(f, *self.limits[n:])
f = newf
if hints.get('deep', True):
# eval_sum could return partially unevaluated
# result with Piecewise. In this case we won't
# doit() recursively.
if not isinstance(f, Piecewise):
return f.doit(**hints)
return f
def eval_zeta_function(self, f, limits):
"""
Check whether the function matches with the zeta function.
If it matches, then return a `Piecewise` expression because
zeta function does not converge unless `s > 1` and `q > 0`
"""
i, a, b = limits
w, y, z = Wild('w', exclude=[i]), Wild('y', exclude=[i]), Wild('z', exclude=[i])
result = f.match((w * i + y) ** (-z))
if result is not None and b is S.Infinity:
coeff = 1 / result[w] ** result[z]
s = result[z]
q = result[y] / result[w] + a
return Piecewise((coeff * zeta(s, q), And(q > 0, s > 1)), (self, True))
def _eval_derivative(self, x):
"""
Differentiate wrt x as long as x is not in the free symbols of any of
the upper or lower limits.
Sum(a*b*x, (x, 1, a)) can be differentiated wrt x or b but not `a`
since the value of the sum is discontinuous in `a`. In a case
involving a limit variable, the unevaluated derivative is returned.
"""
# diff already confirmed that x is in the free symbols of self, but we
# don't want to differentiate wrt any free symbol in the upper or lower
# limits
# XXX remove this test for free_symbols when the default _eval_derivative is in
if isinstance(x, Symbol) and x not in self.free_symbols:
return S.Zero
# get limits and the function
f, limits = self.function, list(self.limits)
limit = limits.pop(-1)
if limits: # f is the argument to a Sum
f = self.func(f, *limits)
_, a, b = limit
if x in a.free_symbols or x in b.free_symbols:
return None
df = Derivative(f, x, evaluate=True)
rv = self.func(df, limit)
return rv
def _eval_difference_delta(self, n, step):
k, _, upper = self.args[-1]
new_upper = upper.subs(n, n + step)
if len(self.args) == 2:
f = self.args[0]
else:
f = self.func(*self.args[:-1])
return Sum(f, (k, upper + 1, new_upper)).doit()
def _eval_simplify(self, **kwargs):
from sympy.simplify.simplify import factor_sum, sum_combine
from sympy.core.function import expand
from sympy.core.mul import Mul
# split the function into adds
terms = Add.make_args(expand(self.function))
s_t = [] # Sum Terms
o_t = [] # Other Terms
for term in terms:
if term.has(Sum):
# if there is an embedded sum here
# it is of the form x * (Sum(whatever))
# hence we make a Mul out of it, and simplify all interior sum terms
subterms = Mul.make_args(expand(term))
out_terms = []
for subterm in subterms:
# go through each term
if isinstance(subterm, Sum):
# if it's a sum, simplify it
out_terms.append(subterm._eval_simplify())
else:
# otherwise, add it as is
out_terms.append(subterm)
# turn it back into a Mul
s_t.append(Mul(*out_terms))
else:
o_t.append(term)
# next try to combine any interior sums for further simplification
result = Add(sum_combine(s_t), *o_t)
return factor_sum(result, limits=self.limits)
def is_convergent(self):
r"""Checks for the convergence of a Sum.
We divide the study of convergence of infinite sums and products in
two parts.
First Part:
One part is the question whether all the terms are well defined, i.e.,
they are finite in a sum and also non-zero in a product. Zero
is the analogy of (minus) infinity in products as
:math:`e^{-\infty} = 0`.
Second Part:
The second part is the question of convergence after infinities,
and zeros in products, have been omitted assuming that their number
is finite. This means that we only consider the tail of the sum or
product, starting from some point after which all terms are well
defined.
For example, in a sum of the form:
.. math::
\sum_{1 \leq i < \infty} \frac{1}{n^2 + an + b}
where a and b are numbers. The routine will return true, even if there
are infinities in the term sequence (at most two). An analogous
product would be:
.. math::
\prod_{1 \leq i < \infty} e^{\frac{1}{n^2 + an + b}}
This is how convergence is interpreted. It is concerned with what
happens at the limit. Finding the bad terms is another independent
matter.
Note: It is responsibility of user to see that the sum or product
is well defined.
There are various tests employed to check the convergence like
divergence test, root test, integral test, alternating series test,
comparison tests, Dirichlet tests. It returns true if Sum is convergent
and false if divergent and NotImplementedError if it can not be checked.
References
==========
.. [1] https://en.wikipedia.org/wiki/Convergence_tests
Examples
========
>>> from sympy import factorial, S, Sum, Symbol, oo
>>> n = Symbol('n', integer=True)
>>> Sum(n/(n - 1), (n, 4, 7)).is_convergent()
True
>>> Sum(n/(2*n + 1), (n, 1, oo)).is_convergent()
False
>>> Sum(factorial(n)/5**n, (n, 1, oo)).is_convergent()
False
>>> Sum(1/n**(S(6)/5), (n, 1, oo)).is_convergent()
True
See Also
========
Sum.is_absolutely_convergent()
Product.is_convergent()
"""
from sympy import Interval, Integral, log, symbols, simplify
p, q, r = symbols('p q r', cls=Wild)
sym = self.limits[0][0]
lower_limit = self.limits[0][1]
upper_limit = self.limits[0][2]
sequence_term = self.function
if len(sequence_term.free_symbols) > 1:
raise NotImplementedError("convergence checking for more than one symbol "
"containing series is not handled")
if lower_limit.is_finite and upper_limit.is_finite:
return S.true
# transform sym -> -sym and swap the upper_limit = S.Infinity
# and lower_limit = - upper_limit
if lower_limit is S.NegativeInfinity:
if upper_limit is S.Infinity:
return Sum(sequence_term, (sym, 0, S.Infinity)).is_convergent() and \
Sum(sequence_term, (sym, S.NegativeInfinity, 0)).is_convergent()
sequence_term = simplify(sequence_term.xreplace({sym: -sym}))
lower_limit = -upper_limit
upper_limit = S.Infinity
sym_ = Dummy(sym.name, integer=True, positive=True)
sequence_term = sequence_term.xreplace({sym: sym_})
sym = sym_
interval = Interval(lower_limit, upper_limit)
# Piecewise function handle
if sequence_term.is_Piecewise:
for func, cond in sequence_term.args:
# see if it represents something going to oo
if cond == True or cond.as_set().sup is S.Infinity:
s = Sum(func, (sym, lower_limit, upper_limit))
return s.is_convergent()
return S.true
### -------- Divergence test ----------- ###
try:
lim_val = limit_seq(sequence_term, sym)
if lim_val is not None and lim_val.is_zero is False:
return S.false
except NotImplementedError:
pass
try:
lim_val_abs = limit_seq(abs(sequence_term), sym)
if lim_val_abs is not None and lim_val_abs.is_zero is False:
return S.false
except NotImplementedError:
pass
order = O(sequence_term, (sym, S.Infinity))
### --------- p-series test (1/n**p) ---------- ###
p_series_test = order.expr.match(sym**p)
if p_series_test is not None:
if p_series_test[p] < -1:
return S.true
if p_series_test[p] >= -1:
return S.false
### ------------- comparison test ------------- ###
# 1/(n**p*log(n)**q*log(log(n))**r) comparison
n_log_test = order.expr.match(1/(sym**p*log(sym)**q*log(log(sym))**r))
if n_log_test is not None:
if (n_log_test[p] > 1 or
(n_log_test[p] == 1 and n_log_test[q] > 1) or
(n_log_test[p] == n_log_test[q] == 1 and n_log_test[r] > 1)):
return S.true
return S.false
### ------------- Limit comparison test -----------###
# (1/n) comparison
try:
lim_comp = limit_seq(sym*sequence_term, sym)
if lim_comp is not None and lim_comp.is_number and lim_comp > 0:
return S.false
except NotImplementedError:
pass
### ----------- ratio test ---------------- ###
next_sequence_term = sequence_term.xreplace({sym: sym + 1})
ratio = combsimp(powsimp(next_sequence_term/sequence_term))
try:
lim_ratio = limit_seq(ratio, sym)
if lim_ratio is not None and lim_ratio.is_number:
if abs(lim_ratio) > 1:
return S.false
if abs(lim_ratio) < 1:
return S.true
except NotImplementedError:
pass
### ----------- root test ---------------- ###
# lim = Limit(abs(sequence_term)**(1/sym), sym, S.Infinity)
try:
lim_evaluated = limit_seq(abs(sequence_term)**(1/sym), sym)
if lim_evaluated is not None and lim_evaluated.is_number:
if lim_evaluated < 1:
return S.true
if lim_evaluated > 1:
return S.false
except NotImplementedError:
pass
### ------------- alternating series test ----------- ###
dict_val = sequence_term.match((-1)**(sym + p)*q)
if not dict_val[p].has(sym) and is_decreasing(dict_val[q], interval):
return S.true
### ------------- integral test -------------- ###
check_interval = None
maxima = solveset(sequence_term.diff(sym), sym, interval)
if not maxima:
check_interval = interval
elif isinstance(maxima, FiniteSet) and maxima.sup.is_number:
check_interval = Interval(maxima.sup, interval.sup)
if (check_interval is not None and
(is_decreasing(sequence_term, check_interval) or
is_decreasing(-sequence_term, check_interval))):
integral_val = Integral(
sequence_term, (sym, lower_limit, upper_limit))
try:
integral_val_evaluated = integral_val.doit()
if integral_val_evaluated.is_number:
return S(integral_val_evaluated.is_finite)
except NotImplementedError:
pass
### ----- Dirichlet and bounded times convergent tests ----- ###
# TODO
#
# Dirichlet_test
# https://en.wikipedia.org/wiki/Dirichlet%27s_test
#
# Bounded times convergent test
# It is based on comparison theorems for series.
# In particular, if the general term of a series can
# be written as a product of two terms a_n and b_n
# and if a_n is bounded and if Sum(b_n) is absolutely
# convergent, then the original series Sum(a_n * b_n)
# is absolutely convergent and so convergent.
#
# The following code can grows like 2**n where n is the
# number of args in order.expr
# Possibly combined with the potentially slow checks
# inside the loop, could make this test extremely slow
# for larger summation expressions.
if order.expr.is_Mul:
args = order.expr.args
argset = set(args)
### -------------- Dirichlet tests -------------- ###
m = Dummy('m', integer=True)
def _dirichlet_test(g_n):
try:
ing_val = limit_seq(Sum(g_n, (sym, interval.inf, m)).doit(), m)
if ing_val is not None and ing_val.is_finite:
return S.true
except NotImplementedError:
pass
### -------- bounded times convergent test ---------###
def _bounded_convergent_test(g1_n, g2_n):
try:
lim_val = limit_seq(g1_n, sym)
if lim_val is not None and (lim_val.is_finite or (
isinstance(lim_val, AccumulationBounds)
and (lim_val.max - lim_val.min).is_finite)):
if Sum(g2_n, (sym, lower_limit, upper_limit)).is_absolutely_convergent():
return S.true
except NotImplementedError:
pass
for n in range(1, len(argset)):
for a_tuple in itertools.combinations(args, n):
b_set = argset - set(a_tuple)
a_n = Mul(*a_tuple)
b_n = Mul(*b_set)
if is_decreasing(a_n, interval):
dirich = _dirichlet_test(b_n)
if dirich is not None:
return dirich
bc_test = _bounded_convergent_test(a_n, b_n)
if bc_test is not None:
return bc_test
_sym = self.limits[0][0]
sequence_term = sequence_term.xreplace({sym: _sym})
raise NotImplementedError("The algorithm to find the Sum convergence of %s "
"is not yet implemented" % (sequence_term))
def is_absolutely_convergent(self):
"""
Checks for the absolute convergence of an infinite series.
Same as checking convergence of absolute value of sequence_term of
an infinite series.
References
==========
.. [1] https://en.wikipedia.org/wiki/Absolute_convergence
Examples
========
>>> from sympy import Sum, Symbol, sin, oo
>>> n = Symbol('n', integer=True)
>>> Sum((-1)**n, (n, 1, oo)).is_absolutely_convergent()
False
>>> Sum((-1)**n/n**2, (n, 1, oo)).is_absolutely_convergent()
True
See Also
========
Sum.is_convergent()
"""
return Sum(abs(self.function), self.limits).is_convergent()
def euler_maclaurin(self, m=0, n=0, eps=0, eval_integral=True):
"""
Return an Euler-Maclaurin approximation of self, where m is the
number of leading terms to sum directly and n is the number of
terms in the tail.
With m = n = 0, this is simply the corresponding integral
plus a first-order endpoint correction.
Returns (s, e) where s is the Euler-Maclaurin approximation
and e is the estimated error (taken to be the magnitude of
the first omitted term in the tail):
>>> from sympy.abc import k, a, b
>>> from sympy import Sum
>>> Sum(1/k, (k, 2, 5)).doit().evalf()
1.28333333333333
>>> s, e = Sum(1/k, (k, 2, 5)).euler_maclaurin()
>>> s
-log(2) + 7/20 + log(5)
>>> from sympy import sstr
>>> print(sstr((s.evalf(), e.evalf()), full_prec=True))
(1.26629073187415, 0.0175000000000000)
The endpoints may be symbolic:
>>> s, e = Sum(1/k, (k, a, b)).euler_maclaurin()
>>> s
-log(a) + log(b) + 1/(2*b) + 1/(2*a)
>>> e
Abs(1/(12*b**2) - 1/(12*a**2))
If the function is a polynomial of degree at most 2n+1, the
Euler-Maclaurin formula becomes exact (and e = 0 is returned):
>>> Sum(k, (k, 2, b)).euler_maclaurin()
(b**2/2 + b/2 - 1, 0)
>>> Sum(k, (k, 2, b)).doit()
b**2/2 + b/2 - 1
With a nonzero eps specified, the summation is ended
as soon as the remainder term is less than the epsilon.
"""
from sympy.functions import bernoulli, factorial
from sympy.integrals import Integral
m = int(m)
n = int(n)
f = self.function
if len(self.limits) != 1:
raise ValueError("More than 1 limit")
i, a, b = self.limits[0]
if (a > b) == True:
if a - b == 1:
return S.Zero, S.Zero
a, b = b + 1, a - 1
f = -f
s = S.Zero
if m:
if b.is_Integer and a.is_Integer:
m = min(m, b - a + 1)
if not eps or f.is_polynomial(i):
for k in range(m):
s += f.subs(i, a + k)
else:
term = f.subs(i, a)
if term:
test = abs(term.evalf(3)) < eps
if test == True:
return s, abs(term)
elif not (test == False):
# a symbolic Relational class, can't go further
return term, S.Zero
s += term
for k in range(1, m):
term = f.subs(i, a + k)
if abs(term.evalf(3)) < eps and term != 0:
return s, abs(term)
s += term
if b - a + 1 == m:
return s, S.Zero
a += m
x = Dummy('x')
I = Integral(f.subs(i, x), (x, a, b))
if eval_integral:
I = I.doit()
s += I
def fpoint(expr):
if b is S.Infinity:
return expr.subs(i, a), 0
return expr.subs(i, a), expr.subs(i, b)
fa, fb = fpoint(f)
iterm = (fa + fb)/2
g = f.diff(i)
for k in range(1, n + 2):
ga, gb = fpoint(g)
term = bernoulli(2*k)/factorial(2*k)*(gb - ga)
if (eps and term and abs(term.evalf(3)) < eps) or (k > n):
break
s += term
g = g.diff(i, 2, simplify=False)
return s + iterm, abs(term)
def reverse_order(self, *indices):
"""
Reverse the order of a limit in a Sum.
Usage
=====
``reverse_order(self, *indices)`` reverses some limits in the expression
``self`` which can be either a ``Sum`` or a ``Product``. The selectors in
the argument ``indices`` specify some indices whose limits get reversed.
These selectors are either variable names or numerical indices counted
starting from the inner-most limit tuple.
Examples
========
>>> from sympy import Sum
>>> from sympy.abc import x, y, a, b, c, d
>>> Sum(x, (x, 0, 3)).reverse_order(x)
Sum(-x, (x, 4, -1))
>>> Sum(x*y, (x, 1, 5), (y, 0, 6)).reverse_order(x, y)
Sum(x*y, (x, 6, 0), (y, 7, -1))
>>> Sum(x, (x, a, b)).reverse_order(x)
Sum(-x, (x, b + 1, a - 1))
>>> Sum(x, (x, a, b)).reverse_order(0)
Sum(-x, (x, b + 1, a - 1))
While one should prefer variable names when specifying which limits
to reverse, the index counting notation comes in handy in case there
are several symbols with the same name.
>>> S = Sum(x**2, (x, a, b), (x, c, d))
>>> S
Sum(x**2, (x, a, b), (x, c, d))
>>> S0 = S.reverse_order(0)
>>> S0
Sum(-x**2, (x, b + 1, a - 1), (x, c, d))
>>> S1 = S0.reverse_order(1)
>>> S1
Sum(x**2, (x, b + 1, a - 1), (x, d + 1, c - 1))
Of course we can mix both notations:
>>> Sum(x*y, (x, a, b), (y, 2, 5)).reverse_order(x, 1)
Sum(x*y, (x, b + 1, a - 1), (y, 6, 1))
>>> Sum(x*y, (x, a, b), (y, 2, 5)).reverse_order(y, x)
Sum(x*y, (x, b + 1, a - 1), (y, 6, 1))
See Also
========
index, reorder_limit, reorder
References
==========
.. [1] Michael Karr, "Summation in Finite Terms", Journal of the ACM,
Volume 28 Issue 2, April 1981, Pages 305-350
http://dl.acm.org/citation.cfm?doid=322248.322255
"""
l_indices = list(indices)
for i, indx in enumerate(l_indices):
if not isinstance(indx, int):
l_indices[i] = self.index(indx)
e = 1
limits = []
for i, limit in enumerate(self.limits):
l = limit
if i in l_indices:
e = -e
l = (limit[0], limit[2] + 1, limit[1] - 1)
limits.append(l)
return Sum(e * self.function, *limits)
def summation(f, *symbols, **kwargs):
r"""
Compute the summation of f with respect to symbols.
The notation for symbols is similar to the notation used in Integral.
summation(f, (i, a, b)) computes the sum of f with respect to i from a to b,
i.e.,
::
b
____
\ `
summation(f, (i, a, b)) = ) f
/___,
i = a
If it cannot compute the sum, it returns an unevaluated Sum object.
Repeated sums can be computed by introducing additional symbols tuples::
>>> from sympy import summation, oo, symbols, log
>>> i, n, m = symbols('i n m', integer=True)
>>> summation(2*i - 1, (i, 1, n))
n**2
>>> summation(1/2**i, (i, 0, oo))
2
>>> summation(1/log(n)**n, (n, 2, oo))
Sum(log(n)**(-n), (n, 2, oo))
>>> summation(i, (i, 0, n), (n, 0, m))
m**3/6 + m**2/2 + m/3
>>> from sympy.abc import x
>>> from sympy import factorial
>>> summation(x**n/factorial(n), (n, 0, oo))
exp(x)
See Also
========
Sum
Product, product
"""
return Sum(f, *symbols, **kwargs).doit(deep=False)
def telescopic_direct(L, R, n, limits):
"""Returns the direct summation of the terms of a telescopic sum
L is the term with lower index
R is the term with higher index
n difference between the indexes of L and R
For example:
>>> from sympy.concrete.summations import telescopic_direct
>>> from sympy.abc import k, a, b
>>> telescopic_direct(1/k, -1/(k+2), 2, (k, a, b))
-1/(b + 2) - 1/(b + 1) + 1/(a + 1) + 1/a
"""
(i, a, b) = limits
s = 0
for m in range(n):
s += L.subs(i, a + m) + R.subs(i, b - m)
return s
def telescopic(L, R, limits):
'''Tries to perform the summation using the telescopic property
return None if not possible
'''
(i, a, b) = limits
if L.is_Add or R.is_Add:
return None
# We want to solve(L.subs(i, i + m) + R, m)
# First we try a simple match since this does things that
# solve doesn't do, e.g. solve(f(k+m)-f(k), m) fails
k = Wild("k")
sol = (-R).match(L.subs(i, i + k))
s = None
if sol and k in sol:
s = sol[k]
if not (s.is_Integer and L.subs(i, i + s) == -R):
# sometimes match fail(f(x+2).match(-f(x+k))->{k: -2 - 2x}))
s = None
# But there are things that match doesn't do that solve
# can do, e.g. determine that 1/(x + m) = 1/(1 - x) when m = 1
if s is None:
m = Dummy('m')
try:
sol = solve(L.subs(i, i + m) + R, m) or []
except NotImplementedError:
return None
sol = [si for si in sol if si.is_Integer and
(L.subs(i, i + si) + R).expand().is_zero]
if len(sol) != 1:
return None
s = sol[0]
if s < 0:
return telescopic_direct(R, L, abs(s), (i, a, b))
elif s > 0:
return telescopic_direct(L, R, s, (i, a, b))
def eval_sum(f, limits):
from sympy.concrete.delta import deltasummation, _has_simple_delta
from sympy.functions import KroneckerDelta
(i, a, b) = limits
if f.is_zero:
return S.Zero
if i not in f.free_symbols:
return f*(b - a + 1)
if a == b:
return f.subs(i, a)
if isinstance(f, Piecewise):
if not any(i in arg.args[1].free_symbols for arg in f.args):
# Piecewise conditions do not depend on the dummy summation variable,
# therefore we can fold: Sum(Piecewise((e, c), ...), limits)
# --> Piecewise((Sum(e, limits), c), ...)
newargs = []
for arg in f.args:
newexpr = eval_sum(arg.expr, limits)
if newexpr is None:
return None
newargs.append((newexpr, arg.cond))
return f.func(*newargs)
if f.has(KroneckerDelta):
f = f.replace(
lambda x: isinstance(x, Sum),
lambda x: x.factor()
)
if _has_simple_delta(f, limits[0]):
return deltasummation(f, limits)
dif = b - a
definite = dif.is_Integer
# Doing it directly may be faster if there are very few terms.
if definite and (dif < 100):
return eval_sum_direct(f, (i, a, b))
if isinstance(f, Piecewise):
return None
# Try to do it symbolically. Even when the number of terms is known,
# this can save time when b-a is big.
# We should try to transform to partial fractions
value = eval_sum_symbolic(f.expand(), (i, a, b))
if value is not None:
return value
# Do it directly
if definite:
return eval_sum_direct(f, (i, a, b))
def eval_sum_direct(expr, limits):
"""
Evaluate expression directly, but perform some simple checks first
to possibly result in a smaller expression and faster execution.
"""
from sympy.core import Add
(i, a, b) = limits
dif = b - a
# Linearity
if expr.is_Mul:
# Try factor out everything not including i
without_i, with_i = expr.as_independent(i)
if without_i != 1:
s = eval_sum_direct(with_i, (i, a, b))
if s:
r = without_i*s
if r is not S.NaN:
return r
else:
# Try term by term
L, R = expr.as_two_terms()
if not L.has(i):
sR = eval_sum_direct(R, (i, a, b))
if sR:
return L*sR
if not R.has(i):
sL = eval_sum_direct(L, (i, a, b))
if sL:
return sL*R
try:
expr = apart(expr, i) # see if it becomes an Add
except PolynomialError:
pass
if expr.is_Add:
# Try factor out everything not including i
without_i, with_i = expr.as_independent(i)
if without_i != 0:
s = eval_sum_direct(with_i, (i, a, b))
if s:
r = without_i*(dif + 1) + s
if r is not S.NaN:
return r
else:
# Try term by term
L, R = expr.as_two_terms()
lsum = eval_sum_direct(L, (i, a, b))
rsum = eval_sum_direct(R, (i, a, b))
if None not in (lsum, rsum):
r = lsum + rsum
if r is not S.NaN:
return r
return Add(*[expr.subs(i, a + j) for j in range(dif + 1)])
def eval_sum_symbolic(f, limits):
from sympy.functions import harmonic, bernoulli
f_orig = f
(i, a, b) = limits
if not f.has(i):
return f*(b - a + 1)
# Linearity
if f.is_Mul:
# Try factor out everything not including i
without_i, with_i = f.as_independent(i)
if without_i != 1:
s = eval_sum_symbolic(with_i, (i, a, b))
if s:
r = without_i*s
if r is not S.NaN:
return r
else:
# Try term by term
L, R = f.as_two_terms()
if not L.has(i):
sR = eval_sum_symbolic(R, (i, a, b))
if sR:
return L*sR
if not R.has(i):
sL = eval_sum_symbolic(L, (i, a, b))
if sL:
return sL*R
try:
f = apart(f, i) # see if it becomes an Add
except PolynomialError:
pass
if f.is_Add:
L, R = f.as_two_terms()
lrsum = telescopic(L, R, (i, a, b))
if lrsum:
return lrsum
# Try factor out everything not including i
without_i, with_i = f.as_independent(i)
if without_i != 0:
s = eval_sum_symbolic(with_i, (i, a, b))
if s:
r = without_i*(b - a + 1) + s
if r is not S.NaN:
return r
else:
# Try term by term
lsum = eval_sum_symbolic(L, (i, a, b))
rsum = eval_sum_symbolic(R, (i, a, b))
if None not in (lsum, rsum):
r = lsum + rsum
if r is not S.NaN:
return r
# Polynomial terms with Faulhaber's formula
n = Wild('n')
result = f.match(i**n)
if result is not None:
n = result[n]
if n.is_Integer:
if n >= 0:
if (b is S.Infinity and not a is S.NegativeInfinity) or \
(a is S.NegativeInfinity and not b is S.Infinity):
return S.Infinity
return ((bernoulli(n + 1, b + 1) - bernoulli(n + 1, a))/(n + 1)).expand()
elif a.is_Integer and a >= 1:
if n == -1:
return harmonic(b) - harmonic(a - 1)
else:
return harmonic(b, abs(n)) - harmonic(a - 1, abs(n))
if not (a.has(S.Infinity, S.NegativeInfinity) or
b.has(S.Infinity, S.NegativeInfinity)):
# Geometric terms
c1 = Wild('c1', exclude=[i])
c2 = Wild('c2', exclude=[i])
c3 = Wild('c3', exclude=[i])
wexp = Wild('wexp')
# Here we first attempt powsimp on f for easier matching with the
# exponential pattern, and attempt expansion on the exponent for easier
# matching with the linear pattern.
e = f.powsimp().match(c1 ** wexp)
if e is not None:
e_exp = e.pop(wexp).expand().match(c2*i + c3)
if e_exp is not None:
e.update(e_exp)
if e is not None:
p = (c1**c3).subs(e)
q = (c1**c2).subs(e)
r = p*(q**a - q**(b + 1))/(1 - q)
l = p*(b - a + 1)
return Piecewise((l, Eq(q, S.One)), (r, True))
r = gosper_sum(f, (i, a, b))
if isinstance(r, (Mul,Add)):
from sympy import ordered, Tuple
non_limit = r.free_symbols - Tuple(*limits[1:]).free_symbols
den = denom(together(r))
den_sym = non_limit & den.free_symbols
args = []
for v in ordered(den_sym):
try:
s = solve(den, v)
m = Eq(v, s[0]) if s else S.false
if m != False:
args.append((Sum(f_orig.subs(*m.args), limits).doit(), m))
break
except NotImplementedError:
continue
args.append((r, True))
return Piecewise(*args)
if not r in (None, S.NaN):
return r
h = eval_sum_hyper(f_orig, (i, a, b))
if h is not None:
return h
factored = f_orig.factor()
if factored != f_orig:
return eval_sum_symbolic(factored, (i, a, b))
def _eval_sum_hyper(f, i, a):
""" Returns (res, cond). Sums from a to oo. """
from sympy.functions import hyper
from sympy.simplify import hyperexpand, hypersimp, fraction, simplify
from sympy.polys.polytools import Poly, factor
from sympy.core.numbers import Float
if a != 0:
return _eval_sum_hyper(f.subs(i, i + a), i, 0)
if f.subs(i, 0) == 0:
if simplify(f.subs(i, Dummy('i', integer=True, positive=True))) == 0:
return S.Zero, True
return _eval_sum_hyper(f.subs(i, i + 1), i, 0)
hs = hypersimp(f, i)
if hs is None:
return None
if isinstance(hs, Float):
from sympy.simplify.simplify import nsimplify
hs = nsimplify(hs)
numer, denom = fraction(factor(hs))
top, topl = numer.as_coeff_mul(i)
bot, botl = denom.as_coeff_mul(i)
ab = [top, bot]
factors = [topl, botl]
params = [[], []]
for k in range(2):
for fac in factors[k]:
mul = 1
if fac.is_Pow:
mul = fac.exp
fac = fac.base
if not mul.is_Integer:
return None
p = Poly(fac, i)
if p.degree() != 1:
return None
m, n = p.all_coeffs()
ab[k] *= m**mul
params[k] += [n/m]*mul
# Add "1" to numerator parameters, to account for implicit n! in
# hypergeometric series.
ap = params[0] + [1]
bq = params[1]
x = ab[0]/ab[1]
h = hyper(ap, bq, x)
f = combsimp(f)
return f.subs(i, 0)*hyperexpand(h), h.convergence_statement
def eval_sum_hyper(f, i_a_b):
from sympy.logic.boolalg import And
i, a, b = i_a_b
if (b - a).is_Integer:
# We are never going to do better than doing the sum in the obvious way
return None
old_sum = Sum(f, (i, a, b))
if b != S.Infinity:
if a is S.NegativeInfinity:
res = _eval_sum_hyper(f.subs(i, -i), i, -b)
if res is not None:
return Piecewise(res, (old_sum, True))
else:
res1 = _eval_sum_hyper(f, i, a)
res2 = _eval_sum_hyper(f, i, b + 1)
if res1 is None or res2 is None:
return None
(res1, cond1), (res2, cond2) = res1, res2
cond = And(cond1, cond2)
if cond == False:
return None
return Piecewise((res1 - res2, cond), (old_sum, True))
if a is S.NegativeInfinity:
res1 = _eval_sum_hyper(f.subs(i, -i), i, 1)
res2 = _eval_sum_hyper(f, i, 0)
if res1 is None or res2 is None:
return None
res1, cond1 = res1
res2, cond2 = res2
cond = And(cond1, cond2)
if cond == False or cond.as_set() == S.EmptySet:
return None
return Piecewise((res1 + res2, cond), (old_sum, True))
# Now b == oo, a != -oo
res = _eval_sum_hyper(f, i, a)
if res is not None:
r, c = res
if c == False:
if r.is_number:
f = f.subs(i, Dummy('i', integer=True, positive=True) + a)
if f.is_positive or f.is_zero:
return S.Infinity
elif f.is_negative:
return S.NegativeInfinity
return None
return Piecewise(res, (old_sum, True))
def _eval_matrix_sum(expression):
f = expression.function
for n, limit in enumerate(expression.limits):
i, a, b = limit
dif = b - a
if dif.is_Integer:
if (dif < 0) == True:
a, b = b + 1, a - 1
f = -f
newf = eval_sum_direct(f, (i, a, b))
if newf is not None:
return newf.doit()
def _dummy_with_inherited_properties_concrete(limits):
"""
Return a Dummy symbol that inherits as much assumptions based on the
provided symbol and limits as possible.
If the symbol already has all possible assumptions, return None.
"""
x, a, b = limits
l = [a, b]
assumptions_to_consider = ['extended_nonnegative', 'nonnegative',
'extended_nonpositive', 'nonpositive',
'extended_positive', 'positive',
'extended_negative', 'negative',
'integer', 'rational', 'finite',
'zero', 'real', 'extended_real']
assumptions_to_keep = {}
assumptions_to_add = {}
for assum in assumptions_to_consider:
assum_true = x._assumptions.get(assum, None)
if assum_true:
assumptions_to_keep[assum] = True
elif all([getattr(i, 'is_' + assum) for i in l]):
assumptions_to_add[assum] = True
if assumptions_to_add:
assumptions_to_keep.update(assumptions_to_add)
return Dummy('d', **assumptions_to_keep)
else:
return None
|
f5e657b33e58040332981bad9c502ce664f9d897621542cff22dae51ae820b0f | """
Limits
======
Implemented according to the PhD thesis
http://www.cybertester.com/data/gruntz.pdf, which contains very thorough
descriptions of the algorithm including many examples. We summarize here
the gist of it.
All functions are sorted according to how rapidly varying they are at
infinity using the following rules. Any two functions f and g can be
compared using the properties of L:
L=lim log|f(x)| / log|g(x)| (for x -> oo)
We define >, < ~ according to::
1. f > g .... L=+-oo
we say that:
- f is greater than any power of g
- f is more rapidly varying than g
- f goes to infinity/zero faster than g
2. f < g .... L=0
we say that:
- f is lower than any power of g
3. f ~ g .... L!=0, +-oo
we say that:
- both f and g are bounded from above and below by suitable integral
powers of the other
Examples
========
::
2 < x < exp(x) < exp(x**2) < exp(exp(x))
2 ~ 3 ~ -5
x ~ x**2 ~ x**3 ~ 1/x ~ x**m ~ -x
exp(x) ~ exp(-x) ~ exp(2x) ~ exp(x)**2 ~ exp(x+exp(-x))
f ~ 1/f
So we can divide all the functions into comparability classes (x and x^2
belong to one class, exp(x) and exp(-x) belong to some other class). In
principle, we could compare any two functions, but in our algorithm, we
don't compare anything below the class 2~3~-5 (for example log(x) is
below this), so we set 2~3~-5 as the lowest comparability class.
Given the function f, we find the list of most rapidly varying (mrv set)
subexpressions of it. This list belongs to the same comparability class.
Let's say it is {exp(x), exp(2x)}. Using the rule f ~ 1/f we find an
element "w" (either from the list or a new one) from the same
comparability class which goes to zero at infinity. In our example we
set w=exp(-x) (but we could also set w=exp(-2x) or w=exp(-3x) ...). We
rewrite the mrv set using w, in our case {1/w, 1/w^2}, and substitute it
into f. Then we expand f into a series in w::
f = c0*w^e0 + c1*w^e1 + ... + O(w^en), where e0<e1<...<en, c0!=0
but for x->oo, lim f = lim c0*w^e0, because all the other terms go to zero,
because w goes to zero faster than the ci and ei. So::
for e0>0, lim f = 0
for e0<0, lim f = +-oo (the sign depends on the sign of c0)
for e0=0, lim f = lim c0
We need to recursively compute limits at several places of the algorithm, but
as is shown in the PhD thesis, it always finishes.
Important functions from the implementation:
compare(a, b, x) compares "a" and "b" by computing the limit L.
mrv(e, x) returns list of most rapidly varying (mrv) subexpressions of "e"
rewrite(e, Omega, x, wsym) rewrites "e" in terms of w
leadterm(f, x) returns the lowest power term in the series of f
mrv_leadterm(e, x) returns the lead term (c0, e0) for e
limitinf(e, x) computes lim e (for x->oo)
limit(e, z, z0) computes any limit by converting it to the case x->oo
All the functions are really simple and straightforward except
rewrite(), which is the most difficult/complex part of the algorithm.
When the algorithm fails, the bugs are usually in the series expansion
(i.e. in SymPy) or in rewrite.
This code is almost exact rewrite of the Maple code inside the Gruntz
thesis.
Debugging
---------
Because the gruntz algorithm is highly recursive, it's difficult to
figure out what went wrong inside a debugger. Instead, turn on nice
debug prints by defining the environment variable SYMPY_DEBUG. For
example:
[user@localhost]: SYMPY_DEBUG=True ./bin/isympy
In [1]: limit(sin(x)/x, x, 0)
limitinf(_x*sin(1/_x), _x) = 1
+-mrv_leadterm(_x*sin(1/_x), _x) = (1, 0)
| +-mrv(_x*sin(1/_x), _x) = set([_x])
| | +-mrv(_x, _x) = set([_x])
| | +-mrv(sin(1/_x), _x) = set([_x])
| | +-mrv(1/_x, _x) = set([_x])
| | +-mrv(_x, _x) = set([_x])
| +-mrv_leadterm(exp(_x)*sin(exp(-_x)), _x, set([exp(_x)])) = (1, 0)
| +-rewrite(exp(_x)*sin(exp(-_x)), set([exp(_x)]), _x, _w) = (1/_w*sin(_w), -_x)
| +-sign(_x, _x) = 1
| +-mrv_leadterm(1, _x) = (1, 0)
+-sign(0, _x) = 0
+-limitinf(1, _x) = 1
And check manually which line is wrong. Then go to the source code and
debug this function to figure out the exact problem.
"""
from __future__ import print_function, division
from sympy import cacheit
from sympy.core import Basic, S, oo, I, Dummy, Wild, Mul
from sympy.core.compatibility import reduce
from sympy.functions import log, exp
from sympy.series.order import Order
from sympy.simplify.powsimp import powsimp, powdenest
from sympy.utilities.misc import debug_decorator as debug
from sympy.utilities.timeutils import timethis
timeit = timethis('gruntz')
def compare(a, b, x):
"""Returns "<" if a<b, "=" for a == b, ">" for a>b"""
# log(exp(...)) must always be simplified here for termination
la, lb = log(a), log(b)
if isinstance(a, Basic) and isinstance(a, exp):
la = a.args[0]
if isinstance(b, Basic) and isinstance(b, exp):
lb = b.args[0]
c = limitinf(la/lb, x)
if c == 0:
return "<"
elif c.is_infinite:
return ">"
else:
return "="
class SubsSet(dict):
"""
Stores (expr, dummy) pairs, and how to rewrite expr-s.
The gruntz algorithm needs to rewrite certain expressions in term of a new
variable w. We cannot use subs, because it is just too smart for us. For
example::
> Omega=[exp(exp(_p - exp(-_p))/(1 - 1/_p)), exp(exp(_p))]
> O2=[exp(-exp(_p) + exp(-exp(-_p))*exp(_p)/(1 - 1/_p))/_w, 1/_w]
> e = exp(exp(_p - exp(-_p))/(1 - 1/_p)) - exp(exp(_p))
> e.subs(Omega[0],O2[0]).subs(Omega[1],O2[1])
-1/w + exp(exp(p)*exp(-exp(-p))/(1 - 1/p))
is really not what we want!
So we do it the hard way and keep track of all the things we potentially
want to substitute by dummy variables. Consider the expression::
exp(x - exp(-x)) + exp(x) + x.
The mrv set is {exp(x), exp(-x), exp(x - exp(-x))}.
We introduce corresponding dummy variables d1, d2, d3 and rewrite::
d3 + d1 + x.
This class first of all keeps track of the mapping expr->variable, i.e.
will at this stage be a dictionary::
{exp(x): d1, exp(-x): d2, exp(x - exp(-x)): d3}.
[It turns out to be more convenient this way round.]
But sometimes expressions in the mrv set have other expressions from the
mrv set as subexpressions, and we need to keep track of that as well. In
this case, d3 is really exp(x - d2), so rewrites at this stage is::
{d3: exp(x-d2)}.
The function rewrite uses all this information to correctly rewrite our
expression in terms of w. In this case w can be chosen to be exp(-x),
i.e. d2. The correct rewriting then is::
exp(-w)/w + 1/w + x.
"""
def __init__(self):
self.rewrites = {}
def __repr__(self):
return super(SubsSet, self).__repr__() + ', ' + self.rewrites.__repr__()
def __getitem__(self, key):
if not key in self:
self[key] = Dummy()
return dict.__getitem__(self, key)
def do_subs(self, e):
"""Substitute the variables with expressions"""
for expr, var in self.items():
e = e.xreplace({var: expr})
return e
def meets(self, s2):
"""Tell whether or not self and s2 have non-empty intersection"""
return set(self.keys()).intersection(list(s2.keys())) != set()
def union(self, s2, exps=None):
"""Compute the union of self and s2, adjusting exps"""
res = self.copy()
tr = {}
for expr, var in s2.items():
if expr in self:
if exps:
exps = exps.xreplace({var: res[expr]})
tr[var] = res[expr]
else:
res[expr] = var
for var, rewr in s2.rewrites.items():
res.rewrites[var] = rewr.xreplace(tr)
return res, exps
def copy(self):
"""Create a shallow copy of SubsSet"""
r = SubsSet()
r.rewrites = self.rewrites.copy()
for expr, var in self.items():
r[expr] = var
return r
@debug
def mrv(e, x):
"""Returns a SubsSet of most rapidly varying (mrv) subexpressions of 'e',
and e rewritten in terms of these"""
e = powsimp(e, deep=True, combine='exp')
if not isinstance(e, Basic):
raise TypeError("e should be an instance of Basic")
if not e.has(x):
return SubsSet(), e
elif e == x:
s = SubsSet()
return s, s[x]
elif e.is_Mul or e.is_Add:
i, d = e.as_independent(x) # throw away x-independent terms
if d.func != e.func:
s, expr = mrv(d, x)
return s, e.func(i, expr)
a, b = d.as_two_terms()
s1, e1 = mrv(a, x)
s2, e2 = mrv(b, x)
return mrv_max1(s1, s2, e.func(i, e1, e2), x)
elif e.is_Pow:
b, e = e.as_base_exp()
if b == 1:
return SubsSet(), b
if e.has(x):
return mrv(exp(e * log(b)), x)
else:
s, expr = mrv(b, x)
return s, expr**e
elif isinstance(e, log):
s, expr = mrv(e.args[0], x)
return s, log(expr)
elif isinstance(e, exp):
# We know from the theory of this algorithm that exp(log(...)) may always
# be simplified here, and doing so is vital for termination.
if isinstance(e.args[0], log):
return mrv(e.args[0].args[0], x)
# if a product has an infinite factor the result will be
# infinite if there is no zero, otherwise NaN; here, we
# consider the result infinite if any factor is infinite
li = limitinf(e.args[0], x)
if any(_.is_infinite for _ in Mul.make_args(li)):
s1 = SubsSet()
e1 = s1[e]
s2, e2 = mrv(e.args[0], x)
su = s1.union(s2)[0]
su.rewrites[e1] = exp(e2)
return mrv_max3(s1, e1, s2, exp(e2), su, e1, x)
else:
s, expr = mrv(e.args[0], x)
return s, exp(expr)
elif e.is_Function:
l = [mrv(a, x) for a in e.args]
l2 = [s for (s, _) in l if s != SubsSet()]
if len(l2) != 1:
# e.g. something like BesselJ(x, x)
raise NotImplementedError("MRV set computation for functions in"
" several variables not implemented.")
s, ss = l2[0], SubsSet()
args = [ss.do_subs(x[1]) for x in l]
return s, e.func(*args)
elif e.is_Derivative:
raise NotImplementedError("MRV set computation for derviatives"
" not implemented yet.")
return mrv(e.args[0], x)
raise NotImplementedError(
"Don't know how to calculate the mrv of '%s'" % e)
def mrv_max3(f, expsf, g, expsg, union, expsboth, x):
"""Computes the maximum of two sets of expressions f and g, which
are in the same comparability class, i.e. max() compares (two elements of)
f and g and returns either (f, expsf) [if f is larger], (g, expsg)
[if g is larger] or (union, expsboth) [if f, g are of the same class].
"""
if not isinstance(f, SubsSet):
raise TypeError("f should be an instance of SubsSet")
if not isinstance(g, SubsSet):
raise TypeError("g should be an instance of SubsSet")
if f == SubsSet():
return g, expsg
elif g == SubsSet():
return f, expsf
elif f.meets(g):
return union, expsboth
c = compare(list(f.keys())[0], list(g.keys())[0], x)
if c == ">":
return f, expsf
elif c == "<":
return g, expsg
else:
if c != "=":
raise ValueError("c should be =")
return union, expsboth
def mrv_max1(f, g, exps, x):
"""Computes the maximum of two sets of expressions f and g, which
are in the same comparability class, i.e. mrv_max1() compares (two elements of)
f and g and returns the set, which is in the higher comparability class
of the union of both, if they have the same order of variation.
Also returns exps, with the appropriate substitutions made.
"""
u, b = f.union(g, exps)
return mrv_max3(f, g.do_subs(exps), g, f.do_subs(exps),
u, b, x)
@debug
@cacheit
@timeit
def sign(e, x):
"""
Returns a sign of an expression e(x) for x->oo.
::
e > 0 for x sufficiently large ... 1
e == 0 for x sufficiently large ... 0
e < 0 for x sufficiently large ... -1
The result of this function is currently undefined if e changes sign
arbitrarily often for arbitrarily large x (e.g. sin(x)).
Note that this returns zero only if e is *constantly* zero
for x sufficiently large. [If e is constant, of course, this is just
the same thing as the sign of e.]
"""
from sympy import sign as _sign
if not isinstance(e, Basic):
raise TypeError("e should be an instance of Basic")
if e.is_positive:
return 1
elif e.is_negative:
return -1
elif e.is_zero:
return 0
elif not e.has(x):
return _sign(e)
elif e == x:
return 1
elif e.is_Mul:
a, b = e.as_two_terms()
sa = sign(a, x)
if not sa:
return 0
return sa * sign(b, x)
elif isinstance(e, exp):
return 1
elif e.is_Pow:
s = sign(e.base, x)
if s == 1:
return 1
if e.exp.is_Integer:
return s**e.exp
elif isinstance(e, log):
return sign(e.args[0] - 1, x)
# if all else fails, do it the hard way
c0, e0 = mrv_leadterm(e, x)
return sign(c0, x)
@debug
@timeit
@cacheit
def limitinf(e, x):
"""Limit e(x) for x-> oo"""
# rewrite e in terms of tractable functions only
e = e.rewrite('tractable', deep=True)
if not e.has(x):
return e # e is a constant
if e.has(Order):
e = e.expand().removeO()
if not x.is_positive:
# We make sure that x.is_positive is True so we
# get all the correct mathematical behavior from the expression.
# We need a fresh variable.
p = Dummy('p', positive=True, finite=True)
e = e.subs(x, p)
x = p
c0, e0 = mrv_leadterm(e, x)
sig = sign(e0, x)
if sig == 1:
return S.Zero # e0>0: lim f = 0
elif sig == -1: # e0<0: lim f = +-oo (the sign depends on the sign of c0)
if c0.match(I*Wild("a", exclude=[I])):
return c0*oo
s = sign(c0, x)
# the leading term shouldn't be 0:
if s == 0:
raise ValueError("Leading term should not be 0")
return s*oo
elif sig == 0:
return limitinf(c0, x) # e0=0: lim f = lim c0
def moveup2(s, x):
r = SubsSet()
for expr, var in s.items():
r[expr.xreplace({x: exp(x)})] = var
for var, expr in s.rewrites.items():
r.rewrites[var] = s.rewrites[var].xreplace({x: exp(x)})
return r
def moveup(l, x):
return [e.xreplace({x: exp(x)}) for e in l]
@debug
@timeit
def calculate_series(e, x, logx=None):
""" Calculates at least one term of the series of "e" in "x".
This is a place that fails most often, so it is in its own function.
"""
from sympy.polys import cancel
for t in e.lseries(x, logx=logx):
t = cancel(t)
if t.has(exp) and t.has(log):
t = powdenest(t)
if t.simplify():
break
return t
@debug
@timeit
@cacheit
def mrv_leadterm(e, x):
"""Returns (c0, e0) for e."""
Omega = SubsSet()
if not e.has(x):
return (e, S.Zero)
if Omega == SubsSet():
Omega, exps = mrv(e, x)
if not Omega:
# e really does not depend on x after simplification
series = calculate_series(e, x)
c0, e0 = series.leadterm(x)
if e0 != 0:
raise ValueError("e0 should be 0")
return c0, e0
if x in Omega:
# move the whole omega up (exponentiate each term):
Omega_up = moveup2(Omega, x)
e_up = moveup([e], x)[0]
exps_up = moveup([exps], x)[0]
# NOTE: there is no need to move this down!
e = e_up
Omega = Omega_up
exps = exps_up
#
# The positive dummy, w, is used here so log(w*2) etc. will expand;
# a unique dummy is needed in this algorithm
#
# For limits of complex functions, the algorithm would have to be
# improved, or just find limits of Re and Im components separately.
#
w = Dummy("w", real=True, positive=True, finite=True)
f, logw = rewrite(exps, Omega, x, w)
series = calculate_series(f, w, logx=logw)
return series.leadterm(w)
def build_expression_tree(Omega, rewrites):
r""" Helper function for rewrite.
We need to sort Omega (mrv set) so that we replace an expression before
we replace any expression in terms of which it has to be rewritten::
e1 ---> e2 ---> e3
\
-> e4
Here we can do e1, e2, e3, e4 or e1, e2, e4, e3.
To do this we assemble the nodes into a tree, and sort them by height.
This function builds the tree, rewrites then sorts the nodes.
"""
class Node:
def ht(self):
return reduce(lambda x, y: x + y,
[x.ht() for x in self.before], 1)
nodes = {}
for expr, v in Omega:
n = Node()
n.before = []
n.var = v
n.expr = expr
nodes[v] = n
for _, v in Omega:
if v in rewrites:
n = nodes[v]
r = rewrites[v]
for _, v2 in Omega:
if r.has(v2):
n.before.append(nodes[v2])
return nodes
@debug
@timeit
def rewrite(e, Omega, x, wsym):
"""e(x) ... the function
Omega ... the mrv set
wsym ... the symbol which is going to be used for w
Returns the rewritten e in terms of w and log(w). See test_rewrite1()
for examples and correct results.
"""
from sympy import ilcm
if not isinstance(Omega, SubsSet):
raise TypeError("Omega should be an instance of SubsSet")
if len(Omega) == 0:
raise ValueError("Length can not be 0")
# all items in Omega must be exponentials
for t in Omega.keys():
if not isinstance(t, exp):
raise ValueError("Value should be exp")
rewrites = Omega.rewrites
Omega = list(Omega.items())
nodes = build_expression_tree(Omega, rewrites)
Omega.sort(key=lambda x: nodes[x[1]].ht(), reverse=True)
# make sure we know the sign of each exp() term; after the loop,
# g is going to be the "w" - the simplest one in the mrv set
for g, _ in Omega:
sig = sign(g.args[0], x)
if sig != 1 and sig != -1:
raise NotImplementedError('Result depends on the sign of %s' % sig)
if sig == 1:
wsym = 1/wsym # if g goes to oo, substitute 1/w
# O2 is a list, which results by rewriting each item in Omega using "w"
O2 = []
denominators = []
for f, var in Omega:
c = limitinf(f.args[0]/g.args[0], x)
if c.is_Rational:
denominators.append(c.q)
arg = f.args[0]
if var in rewrites:
if not isinstance(rewrites[var], exp):
raise ValueError("Value should be exp")
arg = rewrites[var].args[0]
O2.append((var, exp((arg - c*g.args[0]).expand())*wsym**c))
# Remember that Omega contains subexpressions of "e". So now we find
# them in "e" and substitute them for our rewriting, stored in O2
# the following powsimp is necessary to automatically combine exponentials,
# so that the .xreplace() below succeeds:
# TODO this should not be necessary
f = powsimp(e, deep=True, combine='exp')
for a, b in O2:
f = f.xreplace({a: b})
for _, var in Omega:
assert not f.has(var)
# finally compute the logarithm of w (logw).
logw = g.args[0]
if sig == 1:
logw = -logw # log(w)->log(1/w)=-log(w)
# Some parts of sympy have difficulty computing series expansions with
# non-integral exponents. The following heuristic improves the situation:
exponent = reduce(ilcm, denominators, 1)
f = f.xreplace({wsym: wsym**exponent})
logw /= exponent
return f, logw
def gruntz(e, z, z0, dir="+"):
"""
Compute the limit of e(z) at the point z0 using the Gruntz algorithm.
z0 can be any expression, including oo and -oo.
For dir="+" (default) it calculates the limit from the right
(z->z0+) and for dir="-" the limit from the left (z->z0-). For infinite z0
(oo or -oo), the dir argument doesn't matter.
This algorithm is fully described in the module docstring in the gruntz.py
file. It relies heavily on the series expansion. Most frequently, gruntz()
is only used if the faster limit() function (which uses heuristics) fails.
"""
if not z.is_symbol:
raise NotImplementedError("Second argument must be a Symbol")
# convert all limits to the limit z->oo; sign of z is handled in limitinf
r = None
if z0 is oo:
r = limitinf(e, z)
elif z0 is -oo:
r = limitinf(e.subs(z, -z), z)
else:
if str(dir) == "-":
e0 = e.subs(z, z0 - 1/z)
elif str(dir) == "+":
e0 = e.subs(z, z0 + 1/z)
else:
raise NotImplementedError("dir must be '+' or '-'")
r = limitinf(e0, z)
# This is a bit of a heuristic for nice results... we always rewrite
# tractable functions in terms of familiar intractable ones.
# It might be nicer to rewrite the exactly to what they were initially,
# but that would take some work to implement.
return r.rewrite('intractable', deep=True)
|
4029dff30778e8a08f6fd6b2322aae5c8c96d7c6ab93a164fc61eea5267d2330 | """Limits of sequences"""
from __future__ import print_function, division
from sympy.core.add import Add
from sympy.core.function import PoleError
from sympy.core.power import Pow
from sympy.core.singleton import S
from sympy.core.symbol import Dummy
from sympy.core.sympify import sympify
from sympy.functions.combinatorial.numbers import fibonacci
from sympy.functions.elementary.complexes import Abs
from sympy.functions.elementary.miscellaneous import Max, Min
from sympy.functions.elementary.trigonometric import cos, sin
from sympy.series.limits import Limit
def difference_delta(expr, n=None, step=1):
"""Difference Operator.
Discrete analog of differential operator. Given a sequence x[n],
returns the sequence x[n + step] - x[n].
Examples
========
>>> from sympy import difference_delta as dd
>>> from sympy.abc import n
>>> dd(n*(n + 1), n)
2*n + 2
>>> dd(n*(n + 1), n, 2)
4*n + 6
References
==========
.. [1] https://reference.wolfram.com/language/ref/DifferenceDelta.html
"""
expr = sympify(expr)
if n is None:
f = expr.free_symbols
if len(f) == 1:
n = f.pop()
elif len(f) == 0:
return S.Zero
else:
raise ValueError("Since there is more than one variable in the"
" expression, a variable must be supplied to"
" take the difference of %s" % expr)
step = sympify(step)
if step.is_number is False or step.is_finite is False:
raise ValueError("Step should be a finite number.")
if hasattr(expr, '_eval_difference_delta'):
result = expr._eval_difference_delta(n, step)
if result:
return result
return expr.subs(n, n + step) - expr
def dominant(expr, n):
"""Finds the dominant term in a sum, that is a term that dominates
every other term.
If limit(a/b, n, oo) is oo then a dominates b.
If limit(a/b, n, oo) is 0 then b dominates a.
Otherwise, a and b are comparable.
If there is no unique dominant term, then returns ``None``.
Examples
========
>>> from sympy import Sum
>>> from sympy.series.limitseq import dominant
>>> from sympy.abc import n, k
>>> dominant(5*n**3 + 4*n**2 + n + 1, n)
5*n**3
>>> dominant(2**n + Sum(k, (k, 0, n)), n)
2**n
See Also
========
sympy.series.limitseq.dominant
"""
terms = Add.make_args(expr.expand(func=True))
term0 = terms[-1]
comp = [term0] # comparable terms
for t in terms[:-1]:
e = (term0 / t).gammasimp()
l = limit_seq(e, n)
if l is None:
return None
elif l.is_zero:
term0 = t
comp = [term0]
elif l not in [S.Infinity, S.NegativeInfinity]:
comp.append(t)
if len(comp) > 1:
return None
return term0
def _limit_inf(expr, n):
try:
return Limit(expr, n, S.Infinity).doit(deep=False)
except (NotImplementedError, PoleError):
return None
def _limit_seq(expr, n, trials):
from sympy.concrete.summations import Sum
for i in range(trials):
if not expr.has(Sum):
result = _limit_inf(expr, n)
if result is not None:
return result
num, den = expr.as_numer_denom()
if not den.has(n) or not num.has(n):
result = _limit_inf(expr.doit(), n)
if result is not None:
return result
return None
num, den = (difference_delta(t.expand(), n) for t in [num, den])
expr = (num / den).gammasimp()
if not expr.has(Sum):
result = _limit_inf(expr, n)
if result is not None:
return result
num, den = expr.as_numer_denom()
num = dominant(num, n)
if num is None:
return None
den = dominant(den, n)
if den is None:
return None
expr = (num / den).gammasimp()
def limit_seq(expr, n=None, trials=5):
"""Finds the limit of a sequence as index n tends to infinity.
Parameters
==========
expr : Expr
SymPy expression for the n-th term of the sequence
n : Symbol, optional
The index of the sequence, an integer that tends to positive
infinity. If None, inferred from the expression unless it has
multiple symbols.
trials: int, optional
The algorithm is highly recursive. ``trials`` is a safeguard from
infinite recursion in case the limit is not easily computed by the
algorithm. Try increasing ``trials`` if the algorithm returns ``None``.
Admissible Terms
================
The algorithm is designed for sequences built from rational functions,
indefinite sums, and indefinite products over an indeterminate n. Terms of
alternating sign are also allowed, but more complex oscillatory behavior is
not supported.
Examples
========
>>> from sympy import limit_seq, Sum, binomial
>>> from sympy.abc import n, k, m
>>> limit_seq((5*n**3 + 3*n**2 + 4) / (3*n**3 + 4*n - 5), n)
5/3
>>> limit_seq(binomial(2*n, n) / Sum(binomial(2*k, k), (k, 1, n)), n)
3/4
>>> limit_seq(Sum(k**2 * Sum(2**m/m, (m, 1, k)), (k, 1, n)) / (2**n*n), n)
4
See Also
========
sympy.series.limitseq.dominant
References
==========
.. [1] Computing Limits of Sequences - Manuel Kauers
"""
from sympy.concrete.summations import Sum
from sympy.calculus.util import AccumulationBounds
if n is None:
free = expr.free_symbols
if len(free) == 1:
n = free.pop()
elif not free:
return expr
else:
raise ValueError("Expression has more than one variable. "
"Please specify a variable.")
elif n not in expr.free_symbols:
return expr
expr = expr.rewrite(fibonacci, S.GoldenRatio)
n_ = Dummy("n", integer=True, positive=True)
n1 = Dummy("n", odd=True, positive=True)
n2 = Dummy("n", even=True, positive=True)
# If there is a negative term raised to a power involving n, or a
# trigonometric function, then consider even and odd n separately.
powers = (p.as_base_exp() for p in expr.atoms(Pow))
if (any(b.is_negative and e.has(n) for b, e in powers) or
expr.has(cos, sin)):
L1 = _limit_seq(expr.xreplace({n: n1}), n1, trials)
if L1 is not None:
L2 = _limit_seq(expr.xreplace({n: n2}), n2, trials)
if L1 != L2:
if L1.is_comparable and L2.is_comparable:
return AccumulationBounds(Min(L1, L2), Max(L1, L2))
else:
return None
else:
L1 = _limit_seq(expr.xreplace({n: n_}), n_, trials)
if L1 is not None:
return L1
else:
if expr.is_Add:
limits = [limit_seq(term, n, trials) for term in expr.args]
if any(result is None for result in limits):
return None
else:
return Add(*limits)
# Maybe the absolute value is easier to deal with (though not if
# it has a Sum). If it tends to 0, the limit is 0.
elif not expr.has(Sum):
if _limit_seq(Abs(expr.xreplace({n: n_})), n_, trials).is_zero:
return S.Zero
|
81a1247c28b5a1ecb517584e5c0473ac8a021707ad96a78931f39c9d18294ea4 | """
This module implements the Residue function and related tools for working
with residues.
"""
from __future__ import print_function, division
from sympy import sympify
from sympy.utilities.timeutils import timethis
@timethis('residue')
def residue(expr, x, x0):
"""
Finds the residue of ``expr`` at the point x=x0.
The residue is defined as the coefficient of 1/(x-x0) in the power series
expansion about x=x0.
Examples
========
>>> from sympy import Symbol, residue, sin
>>> x = Symbol("x")
>>> residue(1/x, x, 0)
1
>>> residue(1/x**2, x, 0)
0
>>> residue(2/sin(x), x, 0)
2
This function is essential for the Residue Theorem [1].
References
==========
.. [1] https://en.wikipedia.org/wiki/Residue_theorem
"""
# The current implementation uses series expansion to
# calculate it. A more general implementation is explained in
# the section 5.6 of the Bronstein's book {M. Bronstein:
# Symbolic Integration I, Springer Verlag (2005)}. For purely
# rational functions, the algorithm is much easier. See
# sections 2.4, 2.5, and 2.7 (this section actually gives an
# algorithm for computing any Laurent series coefficient for
# a rational function). The theory in section 2.4 will help to
# understand why the resultant works in the general algorithm.
# For the definition of a resultant, see section 1.4 (and any
# previous sections for more review).
from sympy import collect, Mul, Order, S
expr = sympify(expr)
if x0 != 0:
expr = expr.subs(x, x + x0)
for n in [0, 1, 2, 4, 8, 16, 32]:
if n == 0:
s = expr.series(x, n=0)
else:
s = expr.nseries(x, n=n)
if not s.has(Order) or s.getn() >= 0:
break
s = collect(s.removeO(), x)
if s.is_Add:
args = s.args
else:
args = [s]
res = S.Zero
for arg in args:
c, m = arg.as_coeff_mul(x)
m = Mul(*m)
if not (m == 1 or m == x or (m.is_Pow and m.exp.is_Integer)):
raise NotImplementedError('term of unexpected form: %s' % m)
if m == 1/x:
res += c
return res
|
d53224e0a704d781ab614cce0a89df759a2e2d5bcc4b5f1bfb9fe5f284ef335d | """Formal Power Series"""
from __future__ import print_function, division
from collections import defaultdict
from sympy import oo, zoo, nan
from sympy.core.add import Add
from sympy.core.compatibility import iterable
from sympy.core.expr import Expr
from sympy.core.function import Derivative, Function, expand
from sympy.core.mul import Mul
from sympy.core.numbers import Rational
from sympy.core.relational import Eq
from sympy.sets.sets import Interval
from sympy.core.singleton import S
from sympy.core.symbol import Wild, Dummy, symbols, Symbol
from sympy.core.sympify import sympify
from sympy.discrete.convolutions import convolution
from sympy.functions.combinatorial.factorials import binomial, factorial, rf
from sympy.functions.combinatorial.numbers import bell
from sympy.functions.elementary.integers import floor, frac, ceiling
from sympy.functions.elementary.miscellaneous import Min, Max
from sympy.functions.elementary.piecewise import Piecewise
from sympy.series.limits import Limit
from sympy.series.order import Order
from sympy.simplify.powsimp import powsimp
from sympy.series.sequences import sequence
from sympy.series.series_class import SeriesBase
def rational_algorithm(f, x, k, order=4, full=False):
"""Rational algorithm for computing
formula of coefficients of Formal Power Series
of a function.
Applicable when f(x) or some derivative of f(x)
is a rational function in x.
:func:`rational_algorithm` uses :func:`apart` function for partial fraction
decomposition. :func:`apart` by default uses 'undetermined coefficients
method'. By setting ``full=True``, 'Bronstein's algorithm' can be used
instead.
Looks for derivative of a function up to 4'th order (by default).
This can be overridden using order option.
Returns
=======
formula : Expr
ind : Expr
Independent terms.
order : int
Examples
========
>>> from sympy import log, atan, I
>>> from sympy.series.formal import rational_algorithm as ra
>>> from sympy.abc import x, k
>>> ra(1 / (1 - x), x, k)
(1, 0, 0)
>>> ra(log(1 + x), x, k)
(-(-1)**(-k)/k, 0, 1)
>>> ra(atan(x), x, k, full=True)
((-I*(-I)**(-k)/2 + I*I**(-k)/2)/k, 0, 1)
Notes
=====
By setting ``full=True``, range of admissible functions to be solved using
``rational_algorithm`` can be increased. This option should be used
carefully as it can significantly slow down the computation as ``doit`` is
performed on the :class:`RootSum` object returned by the ``apart`` function.
Use ``full=False`` whenever possible.
See Also
========
sympy.polys.partfrac.apart
References
==========
.. [1] Formal Power Series - Dominik Gruntz, Wolfram Koepf
.. [2] Power Series in Computer Algebra - Wolfram Koepf
"""
from sympy.polys import RootSum, apart
from sympy.integrals import integrate
diff = f
ds = [] # list of diff
for i in range(order + 1):
if i:
diff = diff.diff(x)
if diff.is_rational_function(x):
coeff, sep = S.Zero, S.Zero
terms = apart(diff, x, full=full)
if terms.has(RootSum):
terms = terms.doit()
for t in Add.make_args(terms):
num, den = t.as_numer_denom()
if not den.has(x):
sep += t
else:
if isinstance(den, Mul):
# m*(n*x - a)**j -> (n*x - a)**j
ind = den.as_independent(x)
den = ind[1]
num /= ind[0]
# (n*x - a)**j -> (x - b)
den, j = den.as_base_exp()
a, xterm = den.as_coeff_add(x)
# term -> m/x**n
if not a:
sep += t
continue
xc = xterm[0].coeff(x)
a /= -xc
num /= xc**j
ak = ((-1)**j * num *
binomial(j + k - 1, k).rewrite(factorial) /
a**(j + k))
coeff += ak
# Hacky, better way?
if coeff.is_zero:
return None
if (coeff.has(x) or coeff.has(zoo) or coeff.has(oo) or
coeff.has(nan)):
return None
for j in range(i):
coeff = (coeff / (k + j + 1))
sep = integrate(sep, x)
sep += (ds.pop() - sep).limit(x, 0) # constant of integration
return (coeff.subs(k, k - i), sep, i)
else:
ds.append(diff)
return None
def rational_independent(terms, x):
"""Returns a list of all the rationally independent terms.
Examples
========
>>> from sympy import sin, cos
>>> from sympy.series.formal import rational_independent
>>> from sympy.abc import x
>>> rational_independent([cos(x), sin(x)], x)
[cos(x), sin(x)]
>>> rational_independent([x**2, sin(x), x*sin(x), x**3], x)
[x**3 + x**2, x*sin(x) + sin(x)]
"""
if not terms:
return []
ind = terms[0:1]
for t in terms[1:]:
n = t.as_independent(x)[1]
for i, term in enumerate(ind):
d = term.as_independent(x)[1]
q = (n / d).cancel()
if q.is_rational_function(x):
ind[i] += t
break
else:
ind.append(t)
return ind
def simpleDE(f, x, g, order=4):
r"""Generates simple DE.
DE is of the form
.. math::
f^k(x) + \sum\limits_{j=0}^{k-1} A_j f^j(x) = 0
where :math:`A_j` should be rational function in x.
Generates DE's upto order 4 (default). DE's can also have free parameters.
By increasing order, higher order DE's can be found.
Yields a tuple of (DE, order).
"""
from sympy.solvers.solveset import linsolve
a = symbols('a:%d' % (order))
def _makeDE(k):
eq = f.diff(x, k) + Add(*[a[i]*f.diff(x, i) for i in range(0, k)])
DE = g(x).diff(x, k) + Add(*[a[i]*g(x).diff(x, i) for i in range(0, k)])
return eq, DE
found = False
for k in range(1, order + 1):
eq, DE = _makeDE(k)
eq = eq.expand()
terms = eq.as_ordered_terms()
ind = rational_independent(terms, x)
if found or len(ind) == k:
sol = dict(zip(a, (i for s in linsolve(ind, a[:k]) for i in s)))
if sol:
found = True
DE = DE.subs(sol)
DE = DE.as_numer_denom()[0]
DE = DE.factor().as_coeff_mul(Derivative)[1][0]
yield DE.collect(Derivative(g(x))), k
def exp_re(DE, r, k):
"""Converts a DE with constant coefficients (explike) into a RE.
Performs the substitution:
.. math::
f^j(x) \\to r(k + j)
Normalises the terms so that lowest order of a term is always r(k).
Examples
========
>>> from sympy import Function, Derivative
>>> from sympy.series.formal import exp_re
>>> from sympy.abc import x, k
>>> f, r = Function('f'), Function('r')
>>> exp_re(-f(x) + Derivative(f(x)), r, k)
-r(k) + r(k + 1)
>>> exp_re(Derivative(f(x), x) + Derivative(f(x), (x, 2)), r, k)
r(k) + r(k + 1)
See Also
========
sympy.series.formal.hyper_re
"""
RE = S.Zero
g = DE.atoms(Function).pop()
mini = None
for t in Add.make_args(DE):
coeff, d = t.as_independent(g)
if isinstance(d, Derivative):
j = d.derivative_count
else:
j = 0
if mini is None or j < mini:
mini = j
RE += coeff * r(k + j)
if mini:
RE = RE.subs(k, k - mini)
return RE
def hyper_re(DE, r, k):
"""Converts a DE into a RE.
Performs the substitution:
.. math::
x^l f^j(x) \\to (k + 1 - l)_j . a_{k + j - l}
Normalises the terms so that lowest order of a term is always r(k).
Examples
========
>>> from sympy import Function, Derivative
>>> from sympy.series.formal import hyper_re
>>> from sympy.abc import x, k
>>> f, r = Function('f'), Function('r')
>>> hyper_re(-f(x) + Derivative(f(x)), r, k)
(k + 1)*r(k + 1) - r(k)
>>> hyper_re(-x*f(x) + Derivative(f(x), (x, 2)), r, k)
(k + 2)*(k + 3)*r(k + 3) - r(k)
See Also
========
sympy.series.formal.exp_re
"""
RE = S.Zero
g = DE.atoms(Function).pop()
x = g.atoms(Symbol).pop()
mini = None
for t in Add.make_args(DE.expand()):
coeff, d = t.as_independent(g)
c, v = coeff.as_independent(x)
l = v.as_coeff_exponent(x)[1]
if isinstance(d, Derivative):
j = d.derivative_count
else:
j = 0
RE += c * rf(k + 1 - l, j) * r(k + j - l)
if mini is None or j - l < mini:
mini = j - l
RE = RE.subs(k, k - mini)
m = Wild('m')
return RE.collect(r(k + m))
def _transformation_a(f, x, P, Q, k, m, shift):
f *= x**(-shift)
P = P.subs(k, k + shift)
Q = Q.subs(k, k + shift)
return f, P, Q, m
def _transformation_c(f, x, P, Q, k, m, scale):
f = f.subs(x, x**scale)
P = P.subs(k, k / scale)
Q = Q.subs(k, k / scale)
m *= scale
return f, P, Q, m
def _transformation_e(f, x, P, Q, k, m):
f = f.diff(x)
P = P.subs(k, k + 1) * (k + m + 1)
Q = Q.subs(k, k + 1) * (k + 1)
return f, P, Q, m
def _apply_shift(sol, shift):
return [(res, cond + shift) for res, cond in sol]
def _apply_scale(sol, scale):
return [(res, cond / scale) for res, cond in sol]
def _apply_integrate(sol, x, k):
return [(res / ((cond + 1)*(cond.as_coeff_Add()[1].coeff(k))), cond + 1)
for res, cond in sol]
def _compute_formula(f, x, P, Q, k, m, k_max):
"""Computes the formula for f."""
from sympy.polys import roots
sol = []
for i in range(k_max + 1, k_max + m + 1):
if (i < 0) == True:
continue
r = f.diff(x, i).limit(x, 0) / factorial(i)
if r.is_zero:
continue
kterm = m*k + i
res = r
p = P.subs(k, kterm)
q = Q.subs(k, kterm)
c1 = p.subs(k, 1/k).leadterm(k)[0]
c2 = q.subs(k, 1/k).leadterm(k)[0]
res *= (-c1 / c2)**k
for r, mul in roots(p, k).items():
res *= rf(-r, k)**mul
for r, mul in roots(q, k).items():
res /= rf(-r, k)**mul
sol.append((res, kterm))
return sol
def _rsolve_hypergeometric(f, x, P, Q, k, m):
"""Recursive wrapper to rsolve_hypergeometric.
Returns a Tuple of (formula, series independent terms,
maximum power of x in independent terms) if successful
otherwise ``None``.
See :func:`rsolve_hypergeometric` for details.
"""
from sympy.polys import lcm, roots
from sympy.integrals import integrate
# transformation - c
proots, qroots = roots(P, k), roots(Q, k)
all_roots = dict(proots)
all_roots.update(qroots)
scale = lcm([r.as_numer_denom()[1] for r, t in all_roots.items()
if r.is_rational])
f, P, Q, m = _transformation_c(f, x, P, Q, k, m, scale)
# transformation - a
qroots = roots(Q, k)
if qroots:
k_min = Min(*qroots.keys())
else:
k_min = S.Zero
shift = k_min + m
f, P, Q, m = _transformation_a(f, x, P, Q, k, m, shift)
l = (x*f).limit(x, 0)
if not isinstance(l, Limit) and l != 0: # Ideally should only be l != 0
return None
qroots = roots(Q, k)
if qroots:
k_max = Max(*qroots.keys())
else:
k_max = S.Zero
ind, mp = S.Zero, -oo
for i in range(k_max + m + 1):
r = f.diff(x, i).limit(x, 0) / factorial(i)
if r.is_finite is False:
old_f = f
f, P, Q, m = _transformation_a(f, x, P, Q, k, m, i)
f, P, Q, m = _transformation_e(f, x, P, Q, k, m)
sol, ind, mp = _rsolve_hypergeometric(f, x, P, Q, k, m)
sol = _apply_integrate(sol, x, k)
sol = _apply_shift(sol, i)
ind = integrate(ind, x)
ind += (old_f - ind).limit(x, 0) # constant of integration
mp += 1
return sol, ind, mp
elif r:
ind += r*x**(i + shift)
pow_x = Rational((i + shift), scale)
if pow_x > mp:
mp = pow_x # maximum power of x
ind = ind.subs(x, x**(1/scale))
sol = _compute_formula(f, x, P, Q, k, m, k_max)
sol = _apply_shift(sol, shift)
sol = _apply_scale(sol, scale)
return sol, ind, mp
def rsolve_hypergeometric(f, x, P, Q, k, m):
"""Solves RE of hypergeometric type.
Attempts to solve RE of the form
Q(k)*a(k + m) - P(k)*a(k)
Transformations that preserve Hypergeometric type:
a. x**n*f(x): b(k + m) = R(k - n)*b(k)
b. f(A*x): b(k + m) = A**m*R(k)*b(k)
c. f(x**n): b(k + n*m) = R(k/n)*b(k)
d. f(x**(1/m)): b(k + 1) = R(k*m)*b(k)
e. f'(x): b(k + m) = ((k + m + 1)/(k + 1))*R(k + 1)*b(k)
Some of these transformations have been used to solve the RE.
Returns
=======
formula : Expr
ind : Expr
Independent terms.
order : int
Examples
========
>>> from sympy import exp, ln, S
>>> from sympy.series.formal import rsolve_hypergeometric as rh
>>> from sympy.abc import x, k
>>> rh(exp(x), x, -S.One, (k + 1), k, 1)
(Piecewise((1/factorial(k), Eq(Mod(k, 1), 0)), (0, True)), 1, 1)
>>> rh(ln(1 + x), x, k**2, k*(k + 1), k, 1)
(Piecewise(((-1)**(k - 1)*factorial(k - 1)/RisingFactorial(2, k - 1),
Eq(Mod(k, 1), 0)), (0, True)), x, 2)
References
==========
.. [1] Formal Power Series - Dominik Gruntz, Wolfram Koepf
.. [2] Power Series in Computer Algebra - Wolfram Koepf
"""
result = _rsolve_hypergeometric(f, x, P, Q, k, m)
if result is None:
return None
sol_list, ind, mp = result
sol_dict = defaultdict(lambda: S.Zero)
for res, cond in sol_list:
j, mk = cond.as_coeff_Add()
c = mk.coeff(k)
if j.is_integer is False:
res *= x**frac(j)
j = floor(j)
res = res.subs(k, (k - j) / c)
cond = Eq(k % c, j % c)
sol_dict[cond] += res # Group together formula for same conditions
sol = []
for cond, res in sol_dict.items():
sol.append((res, cond))
sol.append((S.Zero, True))
sol = Piecewise(*sol)
if mp is -oo:
s = S.Zero
elif mp.is_integer is False:
s = ceiling(mp)
else:
s = mp + 1
# save all the terms of
# form 1/x**k in ind
if s < 0:
ind += sum(sequence(sol * x**k, (k, s, -1)))
s = S.Zero
return (sol, ind, s)
def _solve_hyper_RE(f, x, RE, g, k):
"""See docstring of :func:`rsolve_hypergeometric` for details."""
terms = Add.make_args(RE)
if len(terms) == 2:
gs = list(RE.atoms(Function))
P, Q = map(RE.coeff, gs)
m = gs[1].args[0] - gs[0].args[0]
if m < 0:
P, Q = Q, P
m = abs(m)
return rsolve_hypergeometric(f, x, P, Q, k, m)
def _solve_explike_DE(f, x, DE, g, k):
"""Solves DE with constant coefficients."""
from sympy.solvers import rsolve
for t in Add.make_args(DE):
coeff, d = t.as_independent(g)
if coeff.free_symbols:
return
RE = exp_re(DE, g, k)
init = {}
for i in range(len(Add.make_args(RE))):
if i:
f = f.diff(x)
init[g(k).subs(k, i)] = f.limit(x, 0)
sol = rsolve(RE, g(k), init)
if sol:
return (sol / factorial(k), S.Zero, S.Zero)
def _solve_simple(f, x, DE, g, k):
"""Converts DE into RE and solves using :func:`rsolve`."""
from sympy.solvers import rsolve
RE = hyper_re(DE, g, k)
init = {}
for i in range(len(Add.make_args(RE))):
if i:
f = f.diff(x)
init[g(k).subs(k, i)] = f.limit(x, 0) / factorial(i)
sol = rsolve(RE, g(k), init)
if sol:
return (sol, S.Zero, S.Zero)
def _transform_explike_DE(DE, g, x, order, syms):
"""Converts DE with free parameters into DE with constant coefficients."""
from sympy.solvers.solveset import linsolve
eq = []
highest_coeff = DE.coeff(Derivative(g(x), x, order))
for i in range(order):
coeff = DE.coeff(Derivative(g(x), x, i))
coeff = (coeff / highest_coeff).expand().collect(x)
for t in Add.make_args(coeff):
eq.append(t)
temp = []
for e in eq:
if e.has(x):
break
elif e.has(Symbol):
temp.append(e)
else:
eq = temp
if eq:
sol = dict(zip(syms, (i for s in linsolve(eq, list(syms)) for i in s)))
if sol:
DE = DE.subs(sol)
DE = DE.factor().as_coeff_mul(Derivative)[1][0]
DE = DE.collect(Derivative(g(x)))
return DE
def _transform_DE_RE(DE, g, k, order, syms):
"""Converts DE with free parameters into RE of hypergeometric type."""
from sympy.solvers.solveset import linsolve
RE = hyper_re(DE, g, k)
eq = []
for i in range(1, order):
coeff = RE.coeff(g(k + i))
eq.append(coeff)
sol = dict(zip(syms, (i for s in linsolve(eq, list(syms)) for i in s)))
if sol:
m = Wild('m')
RE = RE.subs(sol)
RE = RE.factor().as_numer_denom()[0].collect(g(k + m))
RE = RE.as_coeff_mul(g)[1][0]
for i in range(order): # smallest order should be g(k)
if RE.coeff(g(k + i)) and i:
RE = RE.subs(k, k - i)
break
return RE
def solve_de(f, x, DE, order, g, k):
"""Solves the DE.
Tries to solve DE by either converting into a RE containing two terms or
converting into a DE having constant coefficients.
Returns
=======
formula : Expr
ind : Expr
Independent terms.
order : int
Examples
========
>>> from sympy import Derivative as D, Function
>>> from sympy import exp, ln
>>> from sympy.series.formal import solve_de
>>> from sympy.abc import x, k
>>> f = Function('f')
>>> solve_de(exp(x), x, D(f(x), x) - f(x), 1, f, k)
(Piecewise((1/factorial(k), Eq(Mod(k, 1), 0)), (0, True)), 1, 1)
>>> solve_de(ln(1 + x), x, (x + 1)*D(f(x), x, 2) + D(f(x)), 2, f, k)
(Piecewise(((-1)**(k - 1)*factorial(k - 1)/RisingFactorial(2, k - 1),
Eq(Mod(k, 1), 0)), (0, True)), x, 2)
"""
sol = None
syms = DE.free_symbols.difference({g, x})
if syms:
RE = _transform_DE_RE(DE, g, k, order, syms)
else:
RE = hyper_re(DE, g, k)
if not RE.free_symbols.difference({k}):
sol = _solve_hyper_RE(f, x, RE, g, k)
if sol:
return sol
if syms:
DE = _transform_explike_DE(DE, g, x, order, syms)
if not DE.free_symbols.difference({x}):
sol = _solve_explike_DE(f, x, DE, g, k)
if sol:
return sol
def hyper_algorithm(f, x, k, order=4):
"""Hypergeometric algorithm for computing Formal Power Series.
Steps:
* Generates DE
* Convert the DE into RE
* Solves the RE
Examples
========
>>> from sympy import exp, ln
>>> from sympy.series.formal import hyper_algorithm
>>> from sympy.abc import x, k
>>> hyper_algorithm(exp(x), x, k)
(Piecewise((1/factorial(k), Eq(Mod(k, 1), 0)), (0, True)), 1, 1)
>>> hyper_algorithm(ln(1 + x), x, k)
(Piecewise(((-1)**(k - 1)*factorial(k - 1)/RisingFactorial(2, k - 1),
Eq(Mod(k, 1), 0)), (0, True)), x, 2)
See Also
========
sympy.series.formal.simpleDE
sympy.series.formal.solve_de
"""
g = Function('g')
des = [] # list of DE's
sol = None
for DE, i in simpleDE(f, x, g, order):
if DE is not None:
sol = solve_de(f, x, DE, i, g, k)
if sol:
return sol
if not DE.free_symbols.difference({x}):
des.append(DE)
# If nothing works
# Try plain rsolve
for DE in des:
sol = _solve_simple(f, x, DE, g, k)
if sol:
return sol
def _compute_fps(f, x, x0, dir, hyper, order, rational, full):
"""Recursive wrapper to compute fps.
See :func:`compute_fps` for details.
"""
if x0 in [S.Infinity, S.NegativeInfinity]:
dir = S.One if x0 is S.Infinity else -S.One
temp = f.subs(x, 1/x)
result = _compute_fps(temp, x, 0, dir, hyper, order, rational, full)
if result is None:
return None
return (result[0], result[1].subs(x, 1/x), result[2].subs(x, 1/x))
elif x0 or dir == -S.One:
if dir == -S.One:
rep = -x + x0
rep2 = -x
rep2b = x0
else:
rep = x + x0
rep2 = x
rep2b = -x0
temp = f.subs(x, rep)
result = _compute_fps(temp, x, 0, S.One, hyper, order, rational, full)
if result is None:
return None
return (result[0], result[1].subs(x, rep2 + rep2b),
result[2].subs(x, rep2 + rep2b))
if f.is_polynomial(x):
k = Dummy('k')
ak = sequence(Coeff(f, x, k), (k, 1, oo))
xk = sequence(x**k, (k, 0, oo))
ind = f.coeff(x, 0)
return ak, xk, ind
# Break instances of Add
# this allows application of different
# algorithms on different terms increasing the
# range of admissible functions.
if isinstance(f, Add):
result = False
ak = sequence(S.Zero, (0, oo))
ind, xk = S.Zero, None
for t in Add.make_args(f):
res = _compute_fps(t, x, 0, S.One, hyper, order, rational, full)
if res:
if not result:
result = True
xk = res[1]
if res[0].start > ak.start:
seq = ak
s, f = ak.start, res[0].start
else:
seq = res[0]
s, f = res[0].start, ak.start
save = Add(*[z[0]*z[1] for z in zip(seq[0:(f - s)], xk[s:f])])
ak += res[0]
ind += res[2] + save
else:
ind += t
if result:
return ak, xk, ind
return None
# The symbolic term - symb, if present, is being separated from the function
# Otherwise symb is being set to S.One
syms = f.free_symbols.difference({x})
(f, symb) = expand(f).as_independent(*syms)
if symb.is_zero:
symb = S.One
symb = powsimp(symb)
result = None
# from here on it's x0=0 and dir=1 handling
k = Dummy('k')
if rational:
result = rational_algorithm(f, x, k, order, full)
if result is None and hyper:
result = hyper_algorithm(f, x, k, order)
if result is None:
return None
ak = sequence(result[0], (k, result[2], oo))
xk_formula = powsimp(x**k * symb)
xk = sequence(xk_formula, (k, 0, oo))
ind = powsimp(result[1] * symb)
return ak, xk, ind
def compute_fps(f, x, x0=0, dir=1, hyper=True, order=4, rational=True,
full=False):
"""Computes the formula for Formal Power Series of a function.
Tries to compute the formula by applying the following techniques
(in order):
* rational_algorithm
* Hypergeometric algorithm
Parameters
==========
x : Symbol
x0 : number, optional
Point to perform series expansion about. Default is 0.
dir : {1, -1, '+', '-'}, optional
If dir is 1 or '+' the series is calculated from the right and
for -1 or '-' the series is calculated from the left. For smooth
functions this flag will not alter the results. Default is 1.
hyper : {True, False}, optional
Set hyper to False to skip the hypergeometric algorithm.
By default it is set to False.
order : int, optional
Order of the derivative of ``f``, Default is 4.
rational : {True, False}, optional
Set rational to False to skip rational algorithm. By default it is set
to True.
full : {True, False}, optional
Set full to True to increase the range of rational algorithm.
See :func:`rational_algorithm` for details. By default it is set to
False.
Returns
=======
ak : sequence
Sequence of coefficients.
xk : sequence
Sequence of powers of x.
ind : Expr
Independent terms.
mul : Pow
Common terms.
See Also
========
sympy.series.formal.rational_algorithm
sympy.series.formal.hyper_algorithm
"""
f = sympify(f)
x = sympify(x)
if not f.has(x):
return None
x0 = sympify(x0)
if dir == '+':
dir = S.One
elif dir == '-':
dir = -S.One
elif dir not in [S.One, -S.One]:
raise ValueError("Dir must be '+' or '-'")
else:
dir = sympify(dir)
return _compute_fps(f, x, x0, dir, hyper, order, rational, full)
class Coeff(Function):
"""
Coeff(p, x, n) represents the nth coefficient of the polynomial p in x
"""
@classmethod
def eval(cls, p, x, n):
if p.is_polynomial(x) and n.is_integer:
return p.coeff(x, n)
class FormalPowerSeries(SeriesBase):
"""Represents Formal Power Series of a function.
No computation is performed. This class should only to be used to represent
a series. No checks are performed.
For computing a series use :func:`fps`.
See Also
========
sympy.series.formal.fps
"""
def __new__(cls, *args):
args = map(sympify, args)
return Expr.__new__(cls, *args)
def __init__(self, *args):
ak = args[4][0]
k = ak.variables[0]
self.ak_seq = sequence(ak.formula, (k, 1, oo))
self.fact_seq = sequence(factorial(k), (k, 1, oo))
self.bell_coeff_seq = self.ak_seq * self.fact_seq
self.sign_seq = sequence((-1, 1), (k, 1, oo))
@property
def function(self):
return self.args[0]
@property
def x(self):
return self.args[1]
@property
def x0(self):
return self.args[2]
@property
def dir(self):
return self.args[3]
@property
def ak(self):
return self.args[4][0]
@property
def xk(self):
return self.args[4][1]
@property
def ind(self):
return self.args[4][2]
@property
def interval(self):
return Interval(0, oo)
@property
def start(self):
return self.interval.inf
@property
def stop(self):
return self.interval.sup
@property
def length(self):
return oo
@property
def infinite(self):
"""Returns an infinite representation of the series"""
from sympy.concrete import Sum
ak, xk = self.ak, self.xk
k = ak.variables[0]
inf_sum = Sum(ak.formula * xk.formula, (k, ak.start, ak.stop))
return self.ind + inf_sum
def _get_pow_x(self, term):
"""Returns the power of x in a term."""
xterm, pow_x = term.as_independent(self.x)[1].as_base_exp()
if not xterm.has(self.x):
return S.Zero
return pow_x
def polynomial(self, n=6):
"""Truncated series as polynomial.
Returns series expansion of ``f`` upto order ``O(x**n)``
as a polynomial(without ``O`` term).
"""
terms = []
sym = self.free_symbols
for i, t in enumerate(self):
xp = self._get_pow_x(t)
if xp.has(*sym):
xp = xp.as_coeff_add(*sym)[0]
if xp >= n:
break
elif xp.is_integer is True and i == n + 1:
break
elif t is not S.Zero:
terms.append(t)
return Add(*terms)
def truncate(self, n=6):
"""Truncated series.
Returns truncated series expansion of f upto
order ``O(x**n)``.
If n is ``None``, returns an infinite iterator.
"""
if n is None:
return iter(self)
x, x0 = self.x, self.x0
pt_xk = self.xk.coeff(n)
if x0 is S.NegativeInfinity:
x0 = S.Infinity
return self.polynomial(n) + Order(pt_xk, (x, x0))
def zero_coeff(self):
return self._eval_term(0)
def _eval_term(self, pt):
try:
pt_xk = self.xk.coeff(pt)
pt_ak = self.ak.coeff(pt).simplify() # Simplify the coefficients
except IndexError:
term = S.Zero
else:
term = (pt_ak * pt_xk)
if self.ind:
ind = S.Zero
sym = self.free_symbols
for t in Add.make_args(self.ind):
pow_x = self._get_pow_x(t)
if pow_x.has(*sym):
pow_x = pow_x.as_coeff_add(*sym)[0]
if pt == 0 and pow_x < 1:
ind += t
elif pow_x >= pt and pow_x < pt + 1:
ind += t
term += ind
return term.collect(self.x)
def _eval_subs(self, old, new):
x = self.x
if old.has(x):
return self
def _eval_as_leading_term(self, x):
for t in self:
if t is not S.Zero:
return t
def _eval_derivative(self, x):
f = self.function.diff(x)
ind = self.ind.diff(x)
pow_xk = self._get_pow_x(self.xk.formula)
ak = self.ak
k = ak.variables[0]
if ak.formula.has(x):
form = []
for e, c in ak.formula.args:
temp = S.Zero
for t in Add.make_args(e):
pow_x = self._get_pow_x(t)
temp += t * (pow_xk + pow_x)
form.append((temp, c))
form = Piecewise(*form)
ak = sequence(form.subs(k, k + 1), (k, ak.start - 1, ak.stop))
else:
ak = sequence((ak.formula * pow_xk).subs(k, k + 1),
(k, ak.start - 1, ak.stop))
return self.func(f, self.x, self.x0, self.dir, (ak, self.xk, ind))
def integrate(self, x=None, **kwargs):
"""Integrate Formal Power Series.
Examples
========
>>> from sympy import fps, sin, integrate
>>> from sympy.abc import x
>>> f = fps(sin(x))
>>> f.integrate(x).truncate()
-1 + x**2/2 - x**4/24 + O(x**6)
>>> integrate(f, (x, 0, 1))
1 - cos(1)
"""
from sympy.integrals import integrate
if x is None:
x = self.x
elif iterable(x):
return integrate(self.function, x)
f = integrate(self.function, x)
ind = integrate(self.ind, x)
ind += (f - ind).limit(x, 0) # constant of integration
pow_xk = self._get_pow_x(self.xk.formula)
ak = self.ak
k = ak.variables[0]
if ak.formula.has(x):
form = []
for e, c in ak.formula.args:
temp = S.Zero
for t in Add.make_args(e):
pow_x = self._get_pow_x(t)
temp += t / (pow_xk + pow_x + 1)
form.append((temp, c))
form = Piecewise(*form)
ak = sequence(form.subs(k, k - 1), (k, ak.start + 1, ak.stop))
else:
ak = sequence((ak.formula / (pow_xk + 1)).subs(k, k - 1),
(k, ak.start + 1, ak.stop))
return self.func(f, self.x, self.x0, self.dir, (ak, self.xk, ind))
def product(self, other, x=None, n=6):
"""Multiplies two Formal Power Series, using discrete convolution and
return the truncated terms upto specified order.
Parameters
==========
n : Number, optional
Specifies the order of the term up to which the polynomial should
be truncated.
Examples
========
>>> from sympy import fps, sin, exp, convolution
>>> from sympy.abc import x
>>> f1 = fps(sin(x))
>>> f2 = fps(exp(x))
>>> f1.product(f2, x).truncate(4)
x + x**2 + x**3/3 + O(x**4)
See Also
========
sympy.discrete.convolutions
sympy.series.formal.FormalPowerSeriesProduct
"""
if x is None:
x = self.x
if n is None:
return iter(self)
other = sympify(other)
if not isinstance(other, FormalPowerSeries):
raise ValueError("Both series should be an instance of FormalPowerSeries"
" class.")
if self.dir != other.dir:
raise ValueError("Both series should be calculated from the"
" same direction.")
elif self.x0 != other.x0:
raise ValueError("Both series should be calculated about the"
" same point.")
elif self.x != other.x:
raise ValueError("Both series should have the same symbol.")
return FormalPowerSeriesProduct(self, other)
def coeff_bell(self, n):
r"""
self.coeff_bell(n) returns a sequence of Bell polynomials of the second kind.
Note that ``n`` should be a integer.
The second kind of Bell polynomials (are sometimes called "partial" Bell
polynomials or incomplete Bell polynomials) are defined as
.. math:: B_{n,k}(x_1, x_2,\dotsc x_{n-k+1}) =
\sum_{j_1+j_2+j_2+\dotsb=k \atop j_1+2j_2+3j_2+\dotsb=n}
\frac{n!}{j_1!j_2!\dotsb j_{n-k+1}!}
\left(\frac{x_1}{1!} \right)^{j_1}
\left(\frac{x_2}{2!} \right)^{j_2} \dotsb
\left(\frac{x_{n-k+1}}{(n-k+1)!} \right) ^{j_{n-k+1}}.
* ``bell(n, k, (x1, x2, ...))`` gives Bell polynomials of the second kind,
`B_{n,k}(x_1, x_2, \dotsc, x_{n-k+1})`.
See Also
========
sympy.functions.combinatorial.numbers.bell
"""
inner_coeffs = [bell(n, j, tuple(self.bell_coeff_seq[:n-j+1])) for j in range(1, n+1)]
k = Dummy('k')
return sequence(tuple(inner_coeffs), (k, 1, oo))
def compose(self, other, x=None, n=6):
r"""
Returns the truncated terms of the formal power series of the composed function,
up to specified `n`.
If `f` and `g` are two formal power series of two different functions,
then the coefficient sequence ``ak`` of the composed formal power series `fp`
will be as follows.
.. math::
\sum\limits_{k=0}^{n} b_k B_{n,k}(x_1, x_2, \dotsc, x_{n-k+1})
Parameters
==========
n : Number, optional
Specifies the order of the term up to which the polynomial should
be truncated.
Examples
========
>>> from sympy import fps, sin, exp, bell
>>> from sympy.abc import x
>>> f1 = fps(exp(x))
>>> f2 = fps(sin(x))
>>> f1.compose(f2, x).truncate()
1 + x + x**2/2 - x**4/8 - x**5/15 + O(x**6)
>>> f1.compose(f2, x).truncate(8)
1 + x + x**2/2 - x**4/8 - x**5/15 - x**6/240 + x**7/90 + O(x**8)
See Also
========
sympy.functions.combinatorial.numbers.bell
sympy.series.formal.FormalPowerSeriesCompose
References
==========
.. [1] Comtet, Louis: Advanced combinatorics; the art of finite and infinite expansions. Reidel, 1974.
"""
if x is None:
x = self.x
if n is None:
return iter(self)
other = sympify(other)
if not isinstance(other, FormalPowerSeries):
raise ValueError("Both series should be an instance of FormalPowerSeries"
" class.")
if self.dir != other.dir:
raise ValueError("Both series should be calculated from the"
" same direction.")
elif self.x0 != other.x0:
raise ValueError("Both series should be calculated about the"
" same point.")
elif self.x != other.x:
raise ValueError("Both series should have the same symbol.")
if other._eval_term(0).as_coeff_mul(other.x)[0] is not S.Zero:
raise ValueError("The formal power series of the inner function should not have any "
"constant coefficient term.")
return FormalPowerSeriesCompose(self, other)
def inverse(self, x=None, n=6):
r"""
Returns the truncated terms of the inverse of the formal power series,
up to specified `n`.
If `f` and `g` are two formal power series of two different functions,
then the coefficient sequence ``ak`` of the composed formal power series `fp`
will be as follows.
.. math::
\sum\limits_{k=0}^{n} (-1)^{k} x_0^{-k-1} B_{n,k}(x_1, x_2, \dotsc, x_{n-k+1})
Parameters
==========
n : Number, optional
Specifies the order of the term up to which the polynomial should
be truncated.
Examples
========
>>> from sympy import fps, exp, cos, bell
>>> from sympy.abc import x
>>> f1 = fps(exp(x))
>>> f2 = fps(cos(x))
>>> f1.inverse(x).truncate()
1 - x + x**2/2 - x**3/6 + x**4/24 - x**5/120 + O(x**6)
>>> f2.inverse(x).truncate(8)
1 + x**2/2 + 5*x**4/24 + 61*x**6/720 + O(x**8)
See Also
========
sympy.functions.combinatorial.numbers.bell
sympy.series.formal.FormalPowerSeriesInverse
References
==========
.. [1] Comtet, Louis: Advanced combinatorics; the art of finite and infinite expansions. Reidel, 1974.
"""
if x is None:
x = self.x
if n is None:
return iter(self)
if self._eval_term(0).is_zero:
raise ValueError("Constant coefficient should exist for an inverse of a formal"
" power series to exist.")
return FormalPowerSeriesInverse(self)
def __add__(self, other):
other = sympify(other)
if isinstance(other, FormalPowerSeries):
if self.dir != other.dir:
raise ValueError("Both series should be calculated from the"
" same direction.")
elif self.x0 != other.x0:
raise ValueError("Both series should be calculated about the"
" same point.")
x, y = self.x, other.x
f = self.function + other.function.subs(y, x)
if self.x not in f.free_symbols:
return f
ak = self.ak + other.ak
if self.ak.start > other.ak.start:
seq = other.ak
s, e = other.ak.start, self.ak.start
else:
seq = self.ak
s, e = self.ak.start, other.ak.start
save = Add(*[z[0]*z[1] for z in zip(seq[0:(e - s)], self.xk[s:e])])
ind = self.ind + other.ind + save
return self.func(f, x, self.x0, self.dir, (ak, self.xk, ind))
elif not other.has(self.x):
f = self.function + other
ind = self.ind + other
return self.func(f, self.x, self.x0, self.dir,
(self.ak, self.xk, ind))
return Add(self, other)
def __radd__(self, other):
return self.__add__(other)
def __neg__(self):
return self.func(-self.function, self.x, self.x0, self.dir,
(-self.ak, self.xk, -self.ind))
def __sub__(self, other):
return self.__add__(-other)
def __rsub__(self, other):
return (-self).__add__(other)
def __mul__(self, other):
other = sympify(other)
if other.has(self.x):
return Mul(self, other)
f = self.function * other
ak = self.ak.coeff_mul(other)
ind = self.ind * other
return self.func(f, self.x, self.x0, self.dir, (ak, self.xk, ind))
def __rmul__(self, other):
return self.__mul__(other)
class FiniteFormalPowerSeries(FormalPowerSeries):
"""Base Class for Product, Compose and Inverse classes"""
def __init__(self, *args):
pass
@property
def ffps(self):
return self.args[0]
@property
def gfps(self):
return self.args[1]
@property
def f(self):
return self.ffps.function
@property
def g(self):
return self.gfps.function
@property
def infinite(self):
raise NotImplementedError("No infinite version for an object of"
" FiniteFormalPowerSeries class.")
def _eval_terms(self, n):
raise NotImplementedError("(%s)._eval_terms()" % self)
def _eval_term(self, pt):
raise NotImplementedError("By the current logic, one can get terms"
"upto a certain order, instead of getting term by term.")
def polynomial(self, n):
return self._eval_terms(n)
def truncate(self, n=6):
ffps = self.ffps
pt_xk = ffps.xk.coeff(n)
x, x0 = ffps.x, ffps.x0
return self.polynomial(n) + Order(pt_xk, (x, x0))
def _eval_derivative(self, x):
raise NotImplementedError
def integrate(self, x):
raise NotImplementedError
class FormalPowerSeriesProduct(FiniteFormalPowerSeries):
"""Represents the product of two formal power series of two functions.
No computation is performed. Terms are calculated using a term by term logic,
instead of a point by point logic.
There are two differences between a `FormalPowerSeries` object and a
`FormalPowerSeriesProduct` object. The first argument contains the two
functions involved in the product. Also, the coefficient sequence contains
both the coefficient sequence of the formal power series of the involved functions.
See Also
========
sympy.series.formal.FormalPowerSeries
sympy.series.formal.FiniteFormalPowerSeries
"""
def __init__(self, *args):
ffps, gfps = self.ffps, self.gfps
k = ffps.ak.variables[0]
self.coeff1 = sequence(ffps.ak.formula, (k, 0, oo))
k = gfps.ak.variables[0]
self.coeff2 = sequence(gfps.ak.formula, (k, 0, oo))
@property
def function(self):
"""Function of the product of two formal power series."""
return self.f * self.g
def _eval_terms(self, n):
"""
Returns the first `n` terms of the product formal power series.
Term by term logic is implemented here.
Examples
========
>>> from sympy import fps, sin, exp, convolution
>>> from sympy.abc import x
>>> f1 = fps(sin(x))
>>> f2 = fps(exp(x))
>>> fprod = f1.product(f2, x)
>>> fprod._eval_terms(4)
x**3/3 + x**2 + x
See Also
========
sympy.series.formal.FormalPowerSeries.product
"""
coeff1, coeff2 = self.coeff1, self.coeff2
aks = convolution(coeff1[:n], coeff2[:n])
terms = []
for i in range(0, n):
terms.append(aks[i] * self.ffps.xk.coeff(i))
return Add(*terms)
class FormalPowerSeriesCompose(FiniteFormalPowerSeries):
"""Represents the composed formal power series of two functions.
No computation is performed. Terms are calculated using a term by term logic,
instead of a point by point logic.
There are two differences between a `FormalPowerSeries` object and a
`FormalPowerSeriesCompose` object. The first argument contains the outer
function and the inner function involved in the omposition. Also, the
coefficient sequence contains the generic sequence which is to be multiplied
by a custom `bell_seq` finite sequence. The finite terms will then be added up to
get the final terms.
See Also
========
sympy.series.formal.FormalPowerSeries
sympy.series.formal.FiniteFormalPowerSeries
"""
@property
def function(self):
"""Function for the composed formal power series."""
f, g, x = self.f, self.g, self.ffps.x
return f.subs(x, g)
def _eval_terms(self, n):
"""
Returns the first `n` terms of the composed formal power series.
Term by term logic is implemented here.
The coefficient sequence of the `FormalPowerSeriesCompose` object is the generic sequence.
It is multiplied by `bell_seq` to get a sequence, whose terms are added up to get
the final terms for the polynomial.
Examples
========
>>> from sympy import fps, sin, exp, bell
>>> from sympy.abc import x
>>> f1 = fps(exp(x))
>>> f2 = fps(sin(x))
>>> fcomp = f1.compose(f2, x)
>>> fcomp._eval_terms(6)
-x**5/15 - x**4/8 + x**2/2 + x + 1
>>> fcomp._eval_terms(8)
x**7/90 - x**6/240 - x**5/15 - x**4/8 + x**2/2 + x + 1
See Also
========
sympy.series.formal.FormalPowerSeries.compose
sympy.series.formal.FormalPowerSeries.coeff_bell
"""
ffps, gfps = self.ffps, self.gfps
terms = [ffps.zero_coeff()]
for i in range(1, n):
bell_seq = gfps.coeff_bell(i)
seq = (ffps.bell_coeff_seq * bell_seq)
terms.append(Add(*(seq[:i])) / ffps.fact_seq[i-1] * ffps.xk.coeff(i))
return Add(*terms)
class FormalPowerSeriesInverse(FiniteFormalPowerSeries):
"""Represents the Inverse of a formal power series.
No computation is performed. Terms are calculated using a term by term logic,
instead of a point by point logic.
There is a single difference between a `FormalPowerSeries` object and a
`FormalPowerSeriesInverse` object. The coefficient sequence contains the
generic sequence which is to be multiplied by a custom `bell_seq` finite sequence.
The finite terms will then be added up to get the final terms.
See Also
========
sympy.series.formal.FormalPowerSeries
sympy.series.formal.FiniteFormalPowerSeries
"""
def __init__(self, *args):
ffps = self.ffps
k = ffps.xk.variables[0]
inv = ffps.zero_coeff()
inv_seq = sequence(inv ** (-(k + 1)), (k, 1, oo))
self.aux_seq = ffps.sign_seq * ffps.fact_seq * inv_seq
@property
def function(self):
"""Function for the inverse of a formal power series."""
f = self.f
return 1 / f
@property
def g(self):
raise ValueError("Only one function is considered while performing"
"inverse of a formal power series.")
@property
def gfps(self):
raise ValueError("Only one function is considered while performing"
"inverse of a formal power series.")
def _eval_terms(self, n):
"""
Returns the first `n` terms of the composed formal power series.
Term by term logic is implemented here.
The coefficient sequence of the `FormalPowerSeriesInverse` object is the generic sequence.
It is multiplied by `bell_seq` to get a sequence, whose terms are added up to get
the final terms for the polynomial.
Examples
========
>>> from sympy import fps, exp, cos, bell
>>> from sympy.abc import x
>>> f1 = fps(exp(x))
>>> f2 = fps(cos(x))
>>> finv1, finv2 = f1.inverse(), f2.inverse()
>>> finv1._eval_terms(6)
-x**5/120 + x**4/24 - x**3/6 + x**2/2 - x + 1
>>> finv2._eval_terms(8)
61*x**6/720 + 5*x**4/24 + x**2/2 + 1
See Also
========
sympy.series.formal.FormalPowerSeries.inverse
sympy.series.formal.FormalPowerSeries.coeff_bell
"""
ffps = self.ffps
terms = [ffps.zero_coeff()]
for i in range(1, n):
bell_seq = ffps.coeff_bell(i)
seq = (self.aux_seq * bell_seq)
terms.append(Add(*(seq[:i])) / ffps.fact_seq[i-1] * ffps.xk.coeff(i))
return Add(*terms)
def fps(f, x=None, x0=0, dir=1, hyper=True, order=4, rational=True, full=False):
"""Generates Formal Power Series of f.
Returns the formal series expansion of ``f`` around ``x = x0``
with respect to ``x`` in the form of a ``FormalPowerSeries`` object.
Formal Power Series is represented using an explicit formula
computed using different algorithms.
See :func:`compute_fps` for the more details regarding the computation
of formula.
Parameters
==========
x : Symbol, optional
If x is None and ``f`` is univariate, the univariate symbols will be
supplied, otherwise an error will be raised.
x0 : number, optional
Point to perform series expansion about. Default is 0.
dir : {1, -1, '+', '-'}, optional
If dir is 1 or '+' the series is calculated from the right and
for -1 or '-' the series is calculated from the left. For smooth
functions this flag will not alter the results. Default is 1.
hyper : {True, False}, optional
Set hyper to False to skip the hypergeometric algorithm.
By default it is set to False.
order : int, optional
Order of the derivative of ``f``, Default is 4.
rational : {True, False}, optional
Set rational to False to skip rational algorithm. By default it is set
to True.
full : {True, False}, optional
Set full to True to increase the range of rational algorithm.
See :func:`rational_algorithm` for details. By default it is set to
False.
Examples
========
>>> from sympy import fps, O, ln, atan, sin
>>> from sympy.abc import x, n
Rational Functions
>>> fps(ln(1 + x)).truncate()
x - x**2/2 + x**3/3 - x**4/4 + x**5/5 + O(x**6)
>>> fps(atan(x), full=True).truncate()
x - x**3/3 + x**5/5 + O(x**6)
Symbolic Functions
>>> fps(x**n*sin(x**2), x).truncate(8)
-x**(n + 6)/6 + x**(n + 2) + O(x**(n + 8))
See Also
========
sympy.series.formal.FormalPowerSeries
sympy.series.formal.compute_fps
"""
f = sympify(f)
if x is None:
free = f.free_symbols
if len(free) == 1:
x = free.pop()
elif not free:
return f
else:
raise NotImplementedError("multivariate formal power series")
result = compute_fps(f, x, x0, dir, hyper, order, rational, full)
if result is None:
return f
return FormalPowerSeries(f, x, x0, dir, result)
|
f7ea3feddbd80f4a925fc72911a3e8b9dbd375c9e23fcd91915cbbeda88e8f88 | from __future__ import print_function, division
from sympy.core import S, sympify, Expr, Rational, Dummy
from sympy.core import Add, Mul, expand_power_base, expand_log
from sympy.core.cache import cacheit
from sympy.core.compatibility import default_sort_key, is_sequence
from sympy.core.containers import Tuple
from sympy.sets.sets import Complement
from sympy.utilities.iterables import uniq
class Order(Expr):
r""" Represents the limiting behavior of some function
The order of a function characterizes the function based on the limiting
behavior of the function as it goes to some limit. Only taking the limit
point to be a number is currently supported. This is expressed in
big O notation [1]_.
The formal definition for the order of a function `g(x)` about a point `a`
is such that `g(x) = O(f(x))` as `x \rightarrow a` if and only if for any
`\delta > 0` there exists a `M > 0` such that `|g(x)| \leq M|f(x)|` for
`|x-a| < \delta`. This is equivalent to `\lim_{x \rightarrow a}
\sup |g(x)/f(x)| < \infty`.
Let's illustrate it on the following example by taking the expansion of
`\sin(x)` about 0:
.. math ::
\sin(x) = x - x^3/3! + O(x^5)
where in this case `O(x^5) = x^5/5! - x^7/7! + \cdots`. By the definition
of `O`, for any `\delta > 0` there is an `M` such that:
.. math ::
|x^5/5! - x^7/7! + ....| <= M|x^5| \text{ for } |x| < \delta
or by the alternate definition:
.. math ::
\lim_{x \rightarrow 0} | (x^5/5! - x^7/7! + ....) / x^5| < \infty
which surely is true, because
.. math ::
\lim_{x \rightarrow 0} | (x^5/5! - x^7/7! + ....) / x^5| = 1/5!
As it is usually used, the order of a function can be intuitively thought
of representing all terms of powers greater than the one specified. For
example, `O(x^3)` corresponds to any terms proportional to `x^3,
x^4,\ldots` and any higher power. For a polynomial, this leaves terms
proportional to `x^2`, `x` and constants.
Examples
========
>>> from sympy import O, oo, cos, pi
>>> from sympy.abc import x, y
>>> O(x + x**2)
O(x)
>>> O(x + x**2, (x, 0))
O(x)
>>> O(x + x**2, (x, oo))
O(x**2, (x, oo))
>>> O(1 + x*y)
O(1, x, y)
>>> O(1 + x*y, (x, 0), (y, 0))
O(1, x, y)
>>> O(1 + x*y, (x, oo), (y, oo))
O(x*y, (x, oo), (y, oo))
>>> O(1) in O(1, x)
True
>>> O(1, x) in O(1)
False
>>> O(x) in O(1, x)
True
>>> O(x**2) in O(x)
True
>>> O(x)*x
O(x**2)
>>> O(x) - O(x)
O(x)
>>> O(cos(x))
O(1)
>>> O(cos(x), (x, pi/2))
O(x - pi/2, (x, pi/2))
References
==========
.. [1] `Big O notation <https://en.wikipedia.org/wiki/Big_O_notation>`_
Notes
=====
In ``O(f(x), x)`` the expression ``f(x)`` is assumed to have a leading
term. ``O(f(x), x)`` is automatically transformed to
``O(f(x).as_leading_term(x),x)``.
``O(expr*f(x), x)`` is ``O(f(x), x)``
``O(expr, x)`` is ``O(1)``
``O(0, x)`` is 0.
Multivariate O is also supported:
``O(f(x, y), x, y)`` is transformed to
``O(f(x, y).as_leading_term(x,y).as_leading_term(y), x, y)``
In the multivariate case, it is assumed the limits w.r.t. the various
symbols commute.
If no symbols are passed then all symbols in the expression are used
and the limit point is assumed to be zero.
"""
is_Order = True
__slots__ = []
@cacheit
def __new__(cls, expr, *args, **kwargs):
expr = sympify(expr)
if not args:
if expr.is_Order:
variables = expr.variables
point = expr.point
else:
variables = list(expr.free_symbols)
point = [S.Zero]*len(variables)
else:
args = list(args if is_sequence(args) else [args])
variables, point = [], []
if is_sequence(args[0]):
for a in args:
v, p = list(map(sympify, a))
variables.append(v)
point.append(p)
else:
variables = list(map(sympify, args))
point = [S.Zero]*len(variables)
if not all(v.is_symbol for v in variables):
raise TypeError('Variables are not symbols, got %s' % variables)
if len(list(uniq(variables))) != len(variables):
raise ValueError('Variables are supposed to be unique symbols, got %s' % variables)
if expr.is_Order:
expr_vp = dict(expr.args[1:])
new_vp = dict(expr_vp)
vp = dict(zip(variables, point))
for v, p in vp.items():
if v in new_vp.keys():
if p != new_vp[v]:
raise NotImplementedError(
"Mixing Order at different points is not supported.")
else:
new_vp[v] = p
if set(expr_vp.keys()) == set(new_vp.keys()):
return expr
else:
variables = list(new_vp.keys())
point = [new_vp[v] for v in variables]
if expr is S.NaN:
return S.NaN
if any(x in p.free_symbols for x in variables for p in point):
raise ValueError('Got %s as a point.' % point)
if variables:
if any(p != point[0] for p in point):
raise NotImplementedError(
"Multivariable orders at different points are not supported.")
if point[0] is S.Infinity:
s = {k: 1/Dummy() for k in variables}
rs = {1/v: 1/k for k, v in s.items()}
elif point[0] is S.NegativeInfinity:
s = {k: -1/Dummy() for k in variables}
rs = {-1/v: -1/k for k, v in s.items()}
elif point[0] is not S.Zero:
s = dict((k, Dummy() + point[0]) for k in variables)
rs = dict((v - point[0], k - point[0]) for k, v in s.items())
else:
s = ()
rs = ()
expr = expr.subs(s)
if expr.is_Add:
from sympy import expand_multinomial
expr = expand_multinomial(expr)
if s:
args = tuple([r[0] for r in rs.items()])
else:
args = tuple(variables)
if len(variables) > 1:
# XXX: better way? We need this expand() to
# workaround e.g: expr = x*(x + y).
# (x*(x + y)).as_leading_term(x, y) currently returns
# x*y (wrong order term!). That's why we want to deal with
# expand()'ed expr (handled in "if expr.is_Add" branch below).
expr = expr.expand()
old_expr = None
while old_expr != expr:
old_expr = expr
if expr.is_Add:
lst = expr.extract_leading_order(args)
expr = Add(*[f.expr for (e, f) in lst])
elif expr:
expr = expr.as_leading_term(*args)
expr = expr.as_independent(*args, as_Add=False)[1]
expr = expand_power_base(expr)
expr = expand_log(expr)
if len(args) == 1:
# The definition of O(f(x)) symbol explicitly stated that
# the argument of f(x) is irrelevant. That's why we can
# combine some power exponents (only "on top" of the
# expression tree for f(x)), e.g.:
# x**p * (-x)**q -> x**(p+q) for real p, q.
x = args[0]
margs = list(Mul.make_args(
expr.as_independent(x, as_Add=False)[1]))
for i, t in enumerate(margs):
if t.is_Pow:
b, q = t.args
if b in (x, -x) and q.is_real and not q.has(x):
margs[i] = x**q
elif b.is_Pow and not b.exp.has(x):
b, r = b.args
if b in (x, -x) and r.is_real:
margs[i] = x**(r*q)
elif b.is_Mul and b.args[0] is S.NegativeOne:
b = -b
if b.is_Pow and not b.exp.has(x):
b, r = b.args
if b in (x, -x) and r.is_real:
margs[i] = x**(r*q)
expr = Mul(*margs)
expr = expr.subs(rs)
if expr.is_zero:
return expr
if expr.is_Order:
expr = expr.expr
if not expr.has(*variables):
expr = S.One
# create Order instance:
vp = dict(zip(variables, point))
variables.sort(key=default_sort_key)
point = [vp[v] for v in variables]
args = (expr,) + Tuple(*zip(variables, point))
obj = Expr.__new__(cls, *args)
return obj
def _eval_nseries(self, x, n, logx):
return self
@property
def expr(self):
return self.args[0]
@property
def variables(self):
if self.args[1:]:
return tuple(x[0] for x in self.args[1:])
else:
return ()
@property
def point(self):
if self.args[1:]:
return tuple(x[1] for x in self.args[1:])
else:
return ()
@property
def free_symbols(self):
return self.expr.free_symbols | set(self.variables)
def _eval_power(b, e):
if e.is_Number and e.is_nonnegative:
return b.func(b.expr ** e, *b.args[1:])
if e == O(1):
return b
return
def as_expr_variables(self, order_symbols):
if order_symbols is None:
order_symbols = self.args[1:]
else:
if (not all(o[1] == order_symbols[0][1] for o in order_symbols) and
not all(p == self.point[0] for p in self.point)): # pragma: no cover
raise NotImplementedError('Order at points other than 0 '
'or oo not supported, got %s as a point.' % self.point)
if order_symbols and order_symbols[0][1] != self.point[0]:
raise NotImplementedError(
"Multiplying Order at different points is not supported.")
order_symbols = dict(order_symbols)
for s, p in dict(self.args[1:]).items():
if s not in order_symbols.keys():
order_symbols[s] = p
order_symbols = sorted(order_symbols.items(), key=lambda x: default_sort_key(x[0]))
return self.expr, tuple(order_symbols)
def removeO(self):
return S.Zero
def getO(self):
return self
@cacheit
def contains(self, expr):
r"""
Return True if expr belongs to Order(self.expr, \*self.variables).
Return False if self belongs to expr.
Return None if the inclusion relation cannot be determined
(e.g. when self and expr have different symbols).
"""
from sympy import powsimp
if expr.is_zero:
return True
if expr is S.NaN:
return False
point = self.point[0] if self.point else S.Zero
if expr.is_Order:
if (any(p != point for p in expr.point) or
any(p != point for p in self.point)):
return None
if expr.expr == self.expr:
# O(1) + O(1), O(1) + O(1, x), etc.
return all([x in self.args[1:] for x in expr.args[1:]])
if expr.expr.is_Add:
return all([self.contains(x) for x in expr.expr.args])
if self.expr.is_Add and point.is_zero:
return any([self.func(x, *self.args[1:]).contains(expr)
for x in self.expr.args])
if self.variables and expr.variables:
common_symbols = tuple(
[s for s in self.variables if s in expr.variables])
elif self.variables:
common_symbols = self.variables
else:
common_symbols = expr.variables
if not common_symbols:
return None
if (self.expr.is_Pow and len(self.variables) == 1
and self.variables == expr.variables):
symbol = self.variables[0]
other = expr.expr.as_independent(symbol, as_Add=False)[1]
if (other.is_Pow and other.base == symbol and
self.expr.base == symbol):
if point.is_zero:
rv = (self.expr.exp - other.exp).is_nonpositive
if point.is_infinite:
rv = (self.expr.exp - other.exp).is_nonnegative
if rv is not None:
return rv
r = None
ratio = self.expr/expr.expr
ratio = powsimp(ratio, deep=True, combine='exp')
for s in common_symbols:
from sympy.series.limits import Limit
l = Limit(ratio, s, point).doit(heuristics=False)
if not isinstance(l, Limit):
l = l != 0
else:
l = None
if r is None:
r = l
else:
if r != l:
return
return r
if self.expr.is_Pow and len(self.variables) == 1:
symbol = self.variables[0]
other = expr.as_independent(symbol, as_Add=False)[1]
if (other.is_Pow and other.base == symbol and
self.expr.base == symbol):
if point.is_zero:
rv = (self.expr.exp - other.exp).is_nonpositive
if point.is_infinite:
rv = (self.expr.exp - other.exp).is_nonnegative
if rv is not None:
return rv
obj = self.func(expr, *self.args[1:])
return self.contains(obj)
def __contains__(self, other):
result = self.contains(other)
if result is None:
raise TypeError('contains did not evaluate to a bool')
return result
def _eval_subs(self, old, new):
if old in self.variables:
newexpr = self.expr.subs(old, new)
i = self.variables.index(old)
newvars = list(self.variables)
newpt = list(self.point)
if new.is_symbol:
newvars[i] = new
else:
syms = new.free_symbols
if len(syms) == 1 or old in syms:
if old in syms:
var = self.variables[i]
else:
var = syms.pop()
# First, try to substitute self.point in the "new"
# expr to see if this is a fixed point.
# E.g. O(y).subs(y, sin(x))
point = new.subs(var, self.point[i])
if point != self.point[i]:
from sympy.solvers.solveset import solveset
d = Dummy()
sol = solveset(old - new.subs(var, d), d)
if isinstance(sol, Complement):
e1 = sol.args[0]
e2 = sol.args[1]
sol = set(e1) - set(e2)
res = [dict(zip((d, ), sol))]
point = d.subs(res[0]).limit(old, self.point[i])
newvars[i] = var
newpt[i] = point
elif old not in syms:
del newvars[i], newpt[i]
if not syms and new == self.point[i]:
newvars.extend(syms)
newpt.extend([S.Zero]*len(syms))
else:
return
return Order(newexpr, *zip(newvars, newpt))
def _eval_conjugate(self):
expr = self.expr._eval_conjugate()
if expr is not None:
return self.func(expr, *self.args[1:])
def _eval_derivative(self, x):
return self.func(self.expr.diff(x), *self.args[1:]) or self
def _eval_transpose(self):
expr = self.expr._eval_transpose()
if expr is not None:
return self.func(expr, *self.args[1:])
def _sage_(self):
#XXX: SAGE doesn't have Order yet. Let's return 0 instead.
return Rational(0)._sage_()
def __neg__(self):
return self
O = Order
|
63ff231b90820896f28adb9a81e52955c546652df9d4c4c7f5e0e55173040b43 | """
Expand Hypergeometric (and Meijer G) functions into named
special functions.
The algorithm for doing this uses a collection of lookup tables of
hypergeometric functions, and various of their properties, to expand
many hypergeometric functions in terms of special functions.
It is based on the following paper:
Kelly B. Roach. Meijer G Function Representations.
In: Proceedings of the 1997 International Symposium on Symbolic and
Algebraic Computation, pages 205-211, New York, 1997. ACM.
It is described in great(er) detail in the Sphinx documentation.
"""
# SUMMARY OF EXTENSIONS FOR MEIJER G FUNCTIONS
#
# o z**rho G(ap, bq; z) = G(ap + rho, bq + rho; z)
#
# o denote z*d/dz by D
#
# o It is helpful to keep in mind that ap and bq play essentially symmetric
# roles: G(1/z) has slightly altered parameters, with ap and bq interchanged.
#
# o There are four shift operators:
# A_J = b_J - D, J = 1, ..., n
# B_J = 1 - a_j + D, J = 1, ..., m
# C_J = -b_J + D, J = m+1, ..., q
# D_J = a_J - 1 - D, J = n+1, ..., p
#
# A_J, C_J increment b_J
# B_J, D_J decrement a_J
#
# o The corresponding four inverse-shift operators are defined if there
# is no cancellation. Thus e.g. an index a_J (upper or lower) can be
# incremented if a_J != b_i for i = 1, ..., q.
#
# o Order reduction: if b_j - a_i is a non-negative integer, where
# j <= m and i > n, the corresponding quotient of gamma functions reduces
# to a polynomial. Hence the G function can be expressed using a G-function
# of lower order.
# Similarly if j > m and i <= n.
#
# Secondly, there are paired index theorems [Adamchik, The evaluation of
# integrals of Bessel functions via G-function identities]. Suppose there
# are three parameters a, b, c, where a is an a_i, i <= n, b is a b_j,
# j <= m and c is a denominator parameter (i.e. a_i, i > n or b_j, j > m).
# Suppose further all three differ by integers.
# Then the order can be reduced.
# TODO work this out in detail.
#
# o An index quadruple is called suitable if its order cannot be reduced.
# If there exists a sequence of shift operators transforming one index
# quadruple into another, we say one is reachable from the other.
#
# o Deciding if one index quadruple is reachable from another is tricky. For
# this reason, we use hand-built routines to match and instantiate formulas.
#
from __future__ import print_function, division
from collections import defaultdict
from itertools import product
from sympy import SYMPY_DEBUG
from sympy.core import (S, Dummy, symbols, sympify, Tuple, expand, I, pi, Mul,
EulerGamma, oo, zoo, expand_func, Add, nan, Expr, Rational)
from sympy.core.compatibility import default_sort_key, range, reduce
from sympy.core.mod import Mod
from sympy.functions import (exp, sqrt, root, log, lowergamma, cos,
besseli, gamma, uppergamma, expint, erf, sin, besselj, Ei, Ci, Si, Shi,
sinh, cosh, Chi, fresnels, fresnelc, polar_lift, exp_polar, floor, ceiling,
rf, factorial, lerchphi, Piecewise, re, elliptic_k, elliptic_e)
from sympy.functions.elementary.complexes import polarify, unpolarify
from sympy.functions.special.hyper import (hyper, HyperRep_atanh,
HyperRep_power1, HyperRep_power2, HyperRep_log1, HyperRep_asin1,
HyperRep_asin2, HyperRep_sqrts1, HyperRep_sqrts2, HyperRep_log2,
HyperRep_cosasin, HyperRep_sinasin, meijerg)
from sympy.polys import poly, Poly
from sympy.series import residue
from sympy.simplify import simplify
from sympy.simplify.powsimp import powdenest
from sympy.utilities.iterables import sift
# function to define "buckets"
def _mod1(x):
# TODO see if this can work as Mod(x, 1); this will require
# different handling of the "buckets" since these need to
# be sorted and that fails when there is a mixture of
# integers and expressions with parameters. With the current
# Mod behavior, Mod(k, 1) == Mod(1, 1) == 0 if k is an integer.
# Although the sorting can be done with Basic.compare, this may
# still require different handling of the sorted buckets.
if x.is_Number:
return Mod(x, 1)
c, x = x.as_coeff_Add()
return Mod(c, 1) + x
# leave add formulae at the top for easy reference
def add_formulae(formulae):
""" Create our knowledge base. """
from sympy.matrices import Matrix
a, b, c, z = symbols('a b c, z', cls=Dummy)
def add(ap, bq, res):
func = Hyper_Function(ap, bq)
formulae.append(Formula(func, z, res, (a, b, c)))
def addb(ap, bq, B, C, M):
func = Hyper_Function(ap, bq)
formulae.append(Formula(func, z, None, (a, b, c), B, C, M))
# Luke, Y. L. (1969), The Special Functions and Their Approximations,
# Volume 1, section 6.2
# 0F0
add((), (), exp(z))
# 1F0
add((a, ), (), HyperRep_power1(-a, z))
# 2F1
addb((a, a - S.Half), (2*a, ),
Matrix([HyperRep_power2(a, z),
HyperRep_power2(a + S.Half, z)/2]),
Matrix([[1, 0]]),
Matrix([[(a - S.Half)*z/(1 - z), (S.Half - a)*z/(1 - z)],
[a/(1 - z), a*(z - 2)/(1 - z)]]))
addb((1, 1), (2, ),
Matrix([HyperRep_log1(z), 1]), Matrix([[-1/z, 0]]),
Matrix([[0, z/(z - 1)], [0, 0]]))
addb((S.Half, 1), (S('3/2'), ),
Matrix([HyperRep_atanh(z), 1]),
Matrix([[1, 0]]),
Matrix([[Rational(-1, 2), 1/(1 - z)/2], [0, 0]]))
addb((S.Half, S.Half), (S('3/2'), ),
Matrix([HyperRep_asin1(z), HyperRep_power1(Rational(-1, 2), z)]),
Matrix([[1, 0]]),
Matrix([[Rational(-1, 2), S.Half], [0, z/(1 - z)/2]]))
addb((a, S.Half + a), (S.Half, ),
Matrix([HyperRep_sqrts1(-a, z), -HyperRep_sqrts2(-a - S.Half, z)]),
Matrix([[1, 0]]),
Matrix([[0, -a],
[z*(-2*a - 1)/2/(1 - z), S.Half - z*(-2*a - 1)/(1 - z)]]))
# A. P. Prudnikov, Yu. A. Brychkov and O. I. Marichev (1990).
# Integrals and Series: More Special Functions, Vol. 3,.
# Gordon and Breach Science Publisher
addb([a, -a], [S.Half],
Matrix([HyperRep_cosasin(a, z), HyperRep_sinasin(a, z)]),
Matrix([[1, 0]]),
Matrix([[0, -a], [a*z/(1 - z), 1/(1 - z)/2]]))
addb([1, 1], [3*S.Half],
Matrix([HyperRep_asin2(z), 1]), Matrix([[1, 0]]),
Matrix([[(z - S.Half)/(1 - z), 1/(1 - z)/2], [0, 0]]))
# Complete elliptic integrals K(z) and E(z), both a 2F1 function
addb([S.Half, S.Half], [S.One],
Matrix([elliptic_k(z), elliptic_e(z)]),
Matrix([[2/pi, 0]]),
Matrix([[Rational(-1, 2), -1/(2*z-2)],
[Rational(-1, 2), S.Half]]))
addb([Rational(-1, 2), S.Half], [S.One],
Matrix([elliptic_k(z), elliptic_e(z)]),
Matrix([[0, 2/pi]]),
Matrix([[Rational(-1, 2), -1/(2*z-2)],
[Rational(-1, 2), S.Half]]))
# 3F2
addb([Rational(-1, 2), 1, 1], [S.Half, 2],
Matrix([z*HyperRep_atanh(z), HyperRep_log1(z), 1]),
Matrix([[Rational(-2, 3), -S.One/(3*z), Rational(2, 3)]]),
Matrix([[S.Half, 0, z/(1 - z)/2],
[0, 0, z/(z - 1)],
[0, 0, 0]]))
# actually the formula for 3/2 is much nicer ...
addb([Rational(-1, 2), 1, 1], [2, 2],
Matrix([HyperRep_power1(S.Half, z), HyperRep_log2(z), 1]),
Matrix([[Rational(4, 9) - 16/(9*z), 4/(3*z), 16/(9*z)]]),
Matrix([[z/2/(z - 1), 0, 0], [1/(2*(z - 1)), 0, S.Half], [0, 0, 0]]))
# 1F1
addb([1], [b], Matrix([z**(1 - b) * exp(z) * lowergamma(b - 1, z), 1]),
Matrix([[b - 1, 0]]), Matrix([[1 - b + z, 1], [0, 0]]))
addb([a], [2*a],
Matrix([z**(S.Half - a)*exp(z/2)*besseli(a - S.Half, z/2)
* gamma(a + S.Half)/4**(S.Half - a),
z**(S.Half - a)*exp(z/2)*besseli(a + S.Half, z/2)
* gamma(a + S.Half)/4**(S.Half - a)]),
Matrix([[1, 0]]),
Matrix([[z/2, z/2], [z/2, (z/2 - 2*a)]]))
mz = polar_lift(-1)*z
addb([a], [a + 1],
Matrix([mz**(-a)*a*lowergamma(a, mz), a*exp(z)]),
Matrix([[1, 0]]),
Matrix([[-a, 1], [0, z]]))
# This one is redundant.
add([Rational(-1, 2)], [S.Half], exp(z) - sqrt(pi*z)*(-I)*erf(I*sqrt(z)))
# Added to get nice results for Laplace transform of Fresnel functions
# http://functions.wolfram.com/07.22.03.6437.01
# Basic rule
#add([1], [Rational(3, 4), Rational(5, 4)],
# sqrt(pi) * (cos(2*sqrt(polar_lift(-1)*z))*fresnelc(2*root(polar_lift(-1)*z,4)/sqrt(pi)) +
# sin(2*sqrt(polar_lift(-1)*z))*fresnels(2*root(polar_lift(-1)*z,4)/sqrt(pi)))
# / (2*root(polar_lift(-1)*z,4)))
# Manually tuned rule
addb([1], [Rational(3, 4), Rational(5, 4)],
Matrix([ sqrt(pi)*(I*sinh(2*sqrt(z))*fresnels(2*root(z, 4)*exp(I*pi/4)/sqrt(pi))
+ cosh(2*sqrt(z))*fresnelc(2*root(z, 4)*exp(I*pi/4)/sqrt(pi)))
* exp(-I*pi/4)/(2*root(z, 4)),
sqrt(pi)*root(z, 4)*(sinh(2*sqrt(z))*fresnelc(2*root(z, 4)*exp(I*pi/4)/sqrt(pi))
+ I*cosh(2*sqrt(z))*fresnels(2*root(z, 4)*exp(I*pi/4)/sqrt(pi)))
*exp(-I*pi/4)/2,
1 ]),
Matrix([[1, 0, 0]]),
Matrix([[Rational(-1, 4), 1, Rational(1, 4)],
[ z, Rational(1, 4), 0],
[ 0, 0, 0]]))
# 2F2
addb([S.Half, a], [Rational(3, 2), a + 1],
Matrix([a/(2*a - 1)*(-I)*sqrt(pi/z)*erf(I*sqrt(z)),
a/(2*a - 1)*(polar_lift(-1)*z)**(-a)*
lowergamma(a, polar_lift(-1)*z),
a/(2*a - 1)*exp(z)]),
Matrix([[1, -1, 0]]),
Matrix([[Rational(-1, 2), 0, 1], [0, -a, 1], [0, 0, z]]))
# We make a "basis" of four functions instead of three, and give EulerGamma
# an extra slot (it could just be a coefficient to 1). The advantage is
# that this way Polys will not see multivariate polynomials (it treats
# EulerGamma as an indeterminate), which is *way* faster.
addb([1, 1], [2, 2],
Matrix([Ei(z) - log(z), exp(z), 1, EulerGamma]),
Matrix([[1/z, 0, 0, -1/z]]),
Matrix([[0, 1, -1, 0], [0, z, 0, 0], [0, 0, 0, 0], [0, 0, 0, 0]]))
# 0F1
add((), (S.Half, ), cosh(2*sqrt(z)))
addb([], [b],
Matrix([gamma(b)*z**((1 - b)/2)*besseli(b - 1, 2*sqrt(z)),
gamma(b)*z**(1 - b/2)*besseli(b, 2*sqrt(z))]),
Matrix([[1, 0]]), Matrix([[0, 1], [z, (1 - b)]]))
# 0F3
x = 4*z**Rational(1, 4)
def fp(a, z):
return besseli(a, x) + besselj(a, x)
def fm(a, z):
return besseli(a, x) - besselj(a, x)
# TODO branching
addb([], [S.Half, a, a + S.Half],
Matrix([fp(2*a - 1, z), fm(2*a, z)*z**Rational(1, 4),
fm(2*a - 1, z)*sqrt(z), fp(2*a, z)*z**Rational(3, 4)])
* 2**(-2*a)*gamma(2*a)*z**((1 - 2*a)/4),
Matrix([[1, 0, 0, 0]]),
Matrix([[0, 1, 0, 0],
[0, S.Half - a, 1, 0],
[0, 0, S.Half, 1],
[z, 0, 0, 1 - a]]))
x = 2*(4*z)**Rational(1, 4)*exp_polar(I*pi/4)
addb([], [a, a + S.Half, 2*a],
(2*sqrt(polar_lift(-1)*z))**(1 - 2*a)*gamma(2*a)**2 *
Matrix([besselj(2*a - 1, x)*besseli(2*a - 1, x),
x*(besseli(2*a, x)*besselj(2*a - 1, x)
- besseli(2*a - 1, x)*besselj(2*a, x)),
x**2*besseli(2*a, x)*besselj(2*a, x),
x**3*(besseli(2*a, x)*besselj(2*a - 1, x)
+ besseli(2*a - 1, x)*besselj(2*a, x))]),
Matrix([[1, 0, 0, 0]]),
Matrix([[0, Rational(1, 4), 0, 0],
[0, (1 - 2*a)/2, Rational(-1, 2), 0],
[0, 0, 1 - 2*a, Rational(1, 4)],
[-32*z, 0, 0, 1 - a]]))
# 1F2
addb([a], [a - S.Half, 2*a],
Matrix([z**(S.Half - a)*besseli(a - S.Half, sqrt(z))**2,
z**(1 - a)*besseli(a - S.Half, sqrt(z))
*besseli(a - Rational(3, 2), sqrt(z)),
z**(Rational(3, 2) - a)*besseli(a - Rational(3, 2), sqrt(z))**2]),
Matrix([[-gamma(a + S.Half)**2/4**(S.Half - a),
2*gamma(a - S.Half)*gamma(a + S.Half)/4**(1 - a),
0]]),
Matrix([[1 - 2*a, 1, 0], [z/2, S.Half - a, S.Half], [0, z, 0]]))
addb([S.Half], [b, 2 - b],
pi*(1 - b)/sin(pi*b)*
Matrix([besseli(1 - b, sqrt(z))*besseli(b - 1, sqrt(z)),
sqrt(z)*(besseli(-b, sqrt(z))*besseli(b - 1, sqrt(z))
+ besseli(1 - b, sqrt(z))*besseli(b, sqrt(z))),
besseli(-b, sqrt(z))*besseli(b, sqrt(z))]),
Matrix([[1, 0, 0]]),
Matrix([[b - 1, S.Half, 0],
[z, 0, z],
[0, S.Half, -b]]))
addb([S.Half], [Rational(3, 2), Rational(3, 2)],
Matrix([Shi(2*sqrt(z))/2/sqrt(z), sinh(2*sqrt(z))/2/sqrt(z),
cosh(2*sqrt(z))]),
Matrix([[1, 0, 0]]),
Matrix([[Rational(-1, 2), S.Half, 0], [0, Rational(-1, 2), S.Half], [0, 2*z, 0]]))
# FresnelS
# Basic rule
#add([Rational(3, 4)], [Rational(3, 2),Rational(7, 4)], 6*fresnels( exp(pi*I/4)*root(z,4)*2/sqrt(pi) ) / ( pi * (exp(pi*I/4)*root(z,4)*2/sqrt(pi))**3 ) )
# Manually tuned rule
addb([Rational(3, 4)], [Rational(3, 2), Rational(7, 4)],
Matrix(
[ fresnels(
exp(
pi*I/4)*root(
z, 4)*2/sqrt(
pi) ) / (
pi * (exp(pi*I/4)*root(z, 4)*2/sqrt(pi))**3 ),
sinh(2*sqrt(z))/sqrt(z),
cosh(2*sqrt(z)) ]),
Matrix([[6, 0, 0]]),
Matrix([[Rational(-3, 4), Rational(1, 16), 0],
[ 0, Rational(-1, 2), 1],
[ 0, z, 0]]))
# FresnelC
# Basic rule
#add([Rational(1, 4)], [S.Half,Rational(5, 4)], fresnelc( exp(pi*I/4)*root(z,4)*2/sqrt(pi) ) / ( exp(pi*I/4)*root(z,4)*2/sqrt(pi) ) )
# Manually tuned rule
addb([Rational(1, 4)], [S.Half, Rational(5, 4)],
Matrix(
[ sqrt(
pi)*exp(
-I*pi/4)*fresnelc(
2*root(z, 4)*exp(I*pi/4)/sqrt(pi))/(2*root(z, 4)),
cosh(2*sqrt(z)),
sinh(2*sqrt(z))*sqrt(z) ]),
Matrix([[1, 0, 0]]),
Matrix([[Rational(-1, 4), Rational(1, 4), 0 ],
[ 0, 0, 1 ],
[ 0, z, S.Half]]))
# 2F3
# XXX with this five-parameter formula is pretty slow with the current
# Formula.find_instantiations (creates 2!*3!*3**(2+3) ~ 3000
# instantiations ... But it's not too bad.
addb([a, a + S.Half], [2*a, b, 2*a - b + 1],
gamma(b)*gamma(2*a - b + 1) * (sqrt(z)/2)**(1 - 2*a) *
Matrix([besseli(b - 1, sqrt(z))*besseli(2*a - b, sqrt(z)),
sqrt(z)*besseli(b, sqrt(z))*besseli(2*a - b, sqrt(z)),
sqrt(z)*besseli(b - 1, sqrt(z))*besseli(2*a - b + 1, sqrt(z)),
besseli(b, sqrt(z))*besseli(2*a - b + 1, sqrt(z))]),
Matrix([[1, 0, 0, 0]]),
Matrix([[0, S.Half, S.Half, 0],
[z/2, 1 - b, 0, z/2],
[z/2, 0, b - 2*a, z/2],
[0, S.Half, S.Half, -2*a]]))
# (C/f above comment about eulergamma in the basis).
addb([1, 1], [2, 2, Rational(3, 2)],
Matrix([Chi(2*sqrt(z)) - log(2*sqrt(z)),
cosh(2*sqrt(z)), sqrt(z)*sinh(2*sqrt(z)), 1, EulerGamma]),
Matrix([[1/z, 0, 0, 0, -1/z]]),
Matrix([[0, S.Half, 0, Rational(-1, 2), 0],
[0, 0, 1, 0, 0],
[0, z, S.Half, 0, 0],
[0, 0, 0, 0, 0],
[0, 0, 0, 0, 0]]))
# 3F3
# This is rule: http://functions.wolfram.com/07.31.03.0134.01
# Initial reason to add it was a nice solution for
# integrate(erf(a*z)/z**2, z) and same for erfc and erfi.
# Basic rule
# add([1, 1, a], [2, 2, a+1], (a/(z*(a-1)**2)) *
# (1 - (-z)**(1-a) * (gamma(a) - uppergamma(a,-z))
# - (a-1) * (EulerGamma + uppergamma(0,-z) + log(-z))
# - exp(z)))
# Manually tuned rule
addb([1, 1, a], [2, 2, a+1],
Matrix([a*(log(-z) + expint(1, -z) + EulerGamma)/(z*(a**2 - 2*a + 1)),
a*(-z)**(-a)*(gamma(a) - uppergamma(a, -z))/(a - 1)**2,
a*exp(z)/(a**2 - 2*a + 1),
a/(z*(a**2 - 2*a + 1))]),
Matrix([[1-a, 1, -1/z, 1]]),
Matrix([[-1,0,-1/z,1],
[0,-a,1,0],
[0,0,z,0],
[0,0,0,-1]]))
def add_meijerg_formulae(formulae):
from sympy.matrices import Matrix
a, b, c, z = list(map(Dummy, 'abcz'))
rho = Dummy('rho')
def add(an, ap, bm, bq, B, C, M, matcher):
formulae.append(MeijerFormula(an, ap, bm, bq, z, [a, b, c, rho],
B, C, M, matcher))
def detect_uppergamma(func):
x = func.an[0]
y, z = func.bm
swapped = False
if not _mod1((x - y).simplify()):
swapped = True
(y, z) = (z, y)
if _mod1((x - z).simplify()) or x - z > 0:
return None
l = [y, x]
if swapped:
l = [x, y]
return {rho: y, a: x - y}, G_Function([x], [], l, [])
add([a + rho], [], [rho, a + rho], [],
Matrix([gamma(1 - a)*z**rho*exp(z)*uppergamma(a, z),
gamma(1 - a)*z**(a + rho)]),
Matrix([[1, 0]]),
Matrix([[rho + z, -1], [0, a + rho]]),
detect_uppergamma)
def detect_3113(func):
"""http://functions.wolfram.com/07.34.03.0984.01"""
x = func.an[0]
u, v, w = func.bm
if _mod1((u - v).simplify()) == 0:
if _mod1((v - w).simplify()) == 0:
return
sig = (S.Half, S.Half, S.Zero)
x1, x2, y = u, v, w
else:
if _mod1((x - u).simplify()) == 0:
sig = (S.Half, S.Zero, S.Half)
x1, y, x2 = u, v, w
else:
sig = (S.Zero, S.Half, S.Half)
y, x1, x2 = u, v, w
if (_mod1((x - x1).simplify()) != 0 or
_mod1((x - x2).simplify()) != 0 or
_mod1((x - y).simplify()) != S.Half or
x - x1 > 0 or x - x2 > 0):
return
return {a: x}, G_Function([x], [], [x - S.Half + t for t in sig], [])
s = sin(2*sqrt(z))
c_ = cos(2*sqrt(z))
S_ = Si(2*sqrt(z)) - pi/2
C = Ci(2*sqrt(z))
add([a], [], [a, a, a - S.Half], [],
Matrix([sqrt(pi)*z**(a - S.Half)*(c_*S_ - s*C),
sqrt(pi)*z**a*(s*S_ + c_*C),
sqrt(pi)*z**a]),
Matrix([[-2, 0, 0]]),
Matrix([[a - S.Half, -1, 0], [z, a, S.Half], [0, 0, a]]),
detect_3113)
def make_simp(z):
""" Create a function that simplifies rational functions in ``z``. """
def simp(expr):
""" Efficiently simplify the rational function ``expr``. """
numer, denom = expr.as_numer_denom()
numer = numer.expand()
# denom = denom.expand() # is this needed?
c, numer, denom = poly(numer, z).cancel(poly(denom, z))
return c * numer.as_expr() / denom.as_expr()
return simp
def debug(*args):
if SYMPY_DEBUG:
for a in args:
print(a, end="")
print()
class Hyper_Function(Expr):
""" A generalized hypergeometric function. """
def __new__(cls, ap, bq):
obj = super(Hyper_Function, cls).__new__(cls)
obj.ap = Tuple(*list(map(expand, ap)))
obj.bq = Tuple(*list(map(expand, bq)))
return obj
@property
def args(self):
return (self.ap, self.bq)
@property
def sizes(self):
return (len(self.ap), len(self.bq))
@property
def gamma(self):
"""
Number of upper parameters that are negative integers
This is a transformation invariant.
"""
return sum(bool(x.is_integer and x.is_negative) for x in self.ap)
def _hashable_content(self):
return super(Hyper_Function, self)._hashable_content() + (self.ap,
self.bq)
def __call__(self, arg):
return hyper(self.ap, self.bq, arg)
def build_invariants(self):
"""
Compute the invariant vector.
The invariant vector is:
(gamma, ((s1, n1), ..., (sk, nk)), ((t1, m1), ..., (tr, mr)))
where gamma is the number of integer a < 0,
s1 < ... < sk
nl is the number of parameters a_i congruent to sl mod 1
t1 < ... < tr
ml is the number of parameters b_i congruent to tl mod 1
If the index pair contains parameters, then this is not truly an
invariant, since the parameters cannot be sorted uniquely mod1.
Examples
========
>>> from sympy.simplify.hyperexpand import Hyper_Function
>>> from sympy import S
>>> ap = (S.Half, S.One/3, S(-1)/2, -2)
>>> bq = (1, 2)
Here gamma = 1,
k = 3, s1 = 0, s2 = 1/3, s3 = 1/2
n1 = 1, n2 = 1, n2 = 2
r = 1, t1 = 0
m1 = 2:
>>> Hyper_Function(ap, bq).build_invariants()
(1, ((0, 1), (1/3, 1), (1/2, 2)), ((0, 2),))
"""
abuckets, bbuckets = sift(self.ap, _mod1), sift(self.bq, _mod1)
def tr(bucket):
bucket = list(bucket.items())
if not any(isinstance(x[0], Mod) for x in bucket):
bucket.sort(key=lambda x: default_sort_key(x[0]))
bucket = tuple([(mod, len(values)) for mod, values in bucket if
values])
return bucket
return (self.gamma, tr(abuckets), tr(bbuckets))
def difficulty(self, func):
""" Estimate how many steps it takes to reach ``func`` from self.
Return -1 if impossible. """
if self.gamma != func.gamma:
return -1
oabuckets, obbuckets, abuckets, bbuckets = [sift(params, _mod1) for
params in (self.ap, self.bq, func.ap, func.bq)]
diff = 0
for bucket, obucket in [(abuckets, oabuckets), (bbuckets, obbuckets)]:
for mod in set(list(bucket.keys()) + list(obucket.keys())):
if (not mod in bucket) or (not mod in obucket) \
or len(bucket[mod]) != len(obucket[mod]):
return -1
l1 = list(bucket[mod])
l2 = list(obucket[mod])
l1.sort()
l2.sort()
for i, j in zip(l1, l2):
diff += abs(i - j)
return diff
def _is_suitable_origin(self):
"""
Decide if ``self`` is a suitable origin.
A function is a suitable origin iff:
* none of the ai equals bj + n, with n a non-negative integer
* none of the ai is zero
* none of the bj is a non-positive integer
Note that this gives meaningful results only when none of the indices
are symbolic.
"""
for a in self.ap:
for b in self.bq:
if (a - b).is_integer and (a - b).is_negative is False:
return False
for a in self.ap:
if a == 0:
return False
for b in self.bq:
if b.is_integer and b.is_nonpositive:
return False
return True
class G_Function(Expr):
""" A Meijer G-function. """
def __new__(cls, an, ap, bm, bq):
obj = super(G_Function, cls).__new__(cls)
obj.an = Tuple(*list(map(expand, an)))
obj.ap = Tuple(*list(map(expand, ap)))
obj.bm = Tuple(*list(map(expand, bm)))
obj.bq = Tuple(*list(map(expand, bq)))
return obj
@property
def args(self):
return (self.an, self.ap, self.bm, self.bq)
def _hashable_content(self):
return super(G_Function, self)._hashable_content() + self.args
def __call__(self, z):
return meijerg(self.an, self.ap, self.bm, self.bq, z)
def compute_buckets(self):
"""
Compute buckets for the fours sets of parameters.
We guarantee that any two equal Mod objects returned are actually the
same, and that the buckets are sorted by real part (an and bq
descendending, bm and ap ascending).
Examples
========
>>> from sympy.simplify.hyperexpand import G_Function
>>> from sympy.abc import y
>>> from sympy import S, symbols
>>> a, b = [1, 3, 2, S(3)/2], [1 + y, y, 2, y + 3]
>>> G_Function(a, b, [2], [y]).compute_buckets()
({0: [3, 2, 1], 1/2: [3/2]},
{0: [2], y: [y, y + 1, y + 3]}, {0: [2]}, {y: [y]})
"""
dicts = pan, pap, pbm, pbq = [defaultdict(list) for i in range(4)]
for dic, lis in zip(dicts, (self.an, self.ap, self.bm, self.bq)):
for x in lis:
dic[_mod1(x)].append(x)
for dic, flip in zip(dicts, (True, False, False, True)):
for m, items in dic.items():
x0 = items[0]
items.sort(key=lambda x: x - x0, reverse=flip)
dic[m] = items
return tuple([dict(w) for w in dicts])
@property
def signature(self):
return (len(self.an), len(self.ap), len(self.bm), len(self.bq))
# Dummy variable.
_x = Dummy('x')
class Formula(object):
"""
This class represents hypergeometric formulae.
Its data members are:
- z, the argument
- closed_form, the closed form expression
- symbols, the free symbols (parameters) in the formula
- func, the function
- B, C, M (see _compute_basis)
Examples
========
>>> from sympy.abc import a, b, z
>>> from sympy.simplify.hyperexpand import Formula, Hyper_Function
>>> func = Hyper_Function((a/2, a/3 + b, (1+a)/2), (a, b, (a+b)/7))
>>> f = Formula(func, z, None, [a, b])
"""
def _compute_basis(self, closed_form):
"""
Compute a set of functions B=(f1, ..., fn), a nxn matrix M
and a 1xn matrix C such that:
closed_form = C B
z d/dz B = M B.
"""
from sympy.matrices import Matrix, eye, zeros
afactors = [_x + a for a in self.func.ap]
bfactors = [_x + b - 1 for b in self.func.bq]
expr = _x*Mul(*bfactors) - self.z*Mul(*afactors)
poly = Poly(expr, _x)
n = poly.degree() - 1
b = [closed_form]
for _ in range(n):
b.append(self.z*b[-1].diff(self.z))
self.B = Matrix(b)
self.C = Matrix([[1] + [0]*n])
m = eye(n)
m = m.col_insert(0, zeros(n, 1))
l = poly.all_coeffs()[1:]
l.reverse()
self.M = m.row_insert(n, -Matrix([l])/poly.all_coeffs()[0])
def __init__(self, func, z, res, symbols, B=None, C=None, M=None):
z = sympify(z)
res = sympify(res)
symbols = [x for x in sympify(symbols) if func.has(x)]
self.z = z
self.symbols = symbols
self.B = B
self.C = C
self.M = M
self.func = func
# TODO with symbolic parameters, it could be advantageous
# (for prettier answers) to compute a basis only *after*
# instantiation
if res is not None:
self._compute_basis(res)
@property
def closed_form(self):
return reduce(lambda s,m: s+m[0]*m[1], zip(self.C, self.B), S.Zero)
def find_instantiations(self, func):
"""
Find substitutions of the free symbols that match ``func``.
Return the substitution dictionaries as a list. Note that the returned
instantiations need not actually match, or be valid!
"""
from sympy.solvers import solve
ap = func.ap
bq = func.bq
if len(ap) != len(self.func.ap) or len(bq) != len(self.func.bq):
raise TypeError('Cannot instantiate other number of parameters')
symbol_values = []
for a in self.symbols:
if a in self.func.ap.args:
symbol_values.append(ap)
elif a in self.func.bq.args:
symbol_values.append(bq)
else:
raise ValueError("At least one of the parameters of the "
"formula must be equal to %s" % (a,))
base_repl = [dict(list(zip(self.symbols, values)))
for values in product(*symbol_values)]
abuckets, bbuckets = [sift(params, _mod1) for params in [ap, bq]]
a_inv, b_inv = [dict((a, len(vals)) for a, vals in bucket.items())
for bucket in [abuckets, bbuckets]]
critical_values = [[0] for _ in self.symbols]
result = []
_n = Dummy()
for repl in base_repl:
symb_a, symb_b = [sift(params, lambda x: _mod1(x.xreplace(repl)))
for params in [self.func.ap, self.func.bq]]
for bucket, obucket in [(abuckets, symb_a), (bbuckets, symb_b)]:
for mod in set(list(bucket.keys()) + list(obucket.keys())):
if (not mod in bucket) or (not mod in obucket) \
or len(bucket[mod]) != len(obucket[mod]):
break
for a, vals in zip(self.symbols, critical_values):
if repl[a].free_symbols:
continue
exprs = [expr for expr in obucket[mod] if expr.has(a)]
repl0 = repl.copy()
repl0[a] += _n
for expr in exprs:
for target in bucket[mod]:
n0, = solve(expr.xreplace(repl0) - target, _n)
if n0.free_symbols:
raise ValueError("Value should not be true")
vals.append(n0)
else:
values = []
for a, vals in zip(self.symbols, critical_values):
a0 = repl[a]
min_ = floor(min(vals))
max_ = ceiling(max(vals))
values.append([a0 + n for n in range(min_, max_ + 1)])
result.extend(dict(list(zip(self.symbols, l))) for l in product(*values))
return result
class FormulaCollection(object):
""" A collection of formulae to use as origins. """
def __init__(self):
""" Doing this globally at module init time is a pain ... """
self.symbolic_formulae = {}
self.concrete_formulae = {}
self.formulae = []
add_formulae(self.formulae)
# Now process the formulae into a helpful form.
# These dicts are indexed by (p, q).
for f in self.formulae:
sizes = f.func.sizes
if len(f.symbols) > 0:
self.symbolic_formulae.setdefault(sizes, []).append(f)
else:
inv = f.func.build_invariants()
self.concrete_formulae.setdefault(sizes, {})[inv] = f
def lookup_origin(self, func):
"""
Given the suitable target ``func``, try to find an origin in our
knowledge base.
Examples
========
>>> from sympy.simplify.hyperexpand import (FormulaCollection,
... Hyper_Function)
>>> f = FormulaCollection()
>>> f.lookup_origin(Hyper_Function((), ())).closed_form
exp(_z)
>>> f.lookup_origin(Hyper_Function([1], ())).closed_form
HyperRep_power1(-1, _z)
>>> from sympy import S
>>> i = Hyper_Function([S('1/4'), S('3/4 + 4')], [S.Half])
>>> f.lookup_origin(i).closed_form
HyperRep_sqrts1(-1/4, _z)
"""
inv = func.build_invariants()
sizes = func.sizes
if sizes in self.concrete_formulae and \
inv in self.concrete_formulae[sizes]:
return self.concrete_formulae[sizes][inv]
# We don't have a concrete formula. Try to instantiate.
if not sizes in self.symbolic_formulae:
return None # Too bad...
possible = []
for f in self.symbolic_formulae[sizes]:
repls = f.find_instantiations(func)
for repl in repls:
func2 = f.func.xreplace(repl)
if not func2._is_suitable_origin():
continue
diff = func2.difficulty(func)
if diff == -1:
continue
possible.append((diff, repl, f, func2))
# find the nearest origin
possible.sort(key=lambda x: x[0])
for _, repl, f, func2 in possible:
f2 = Formula(func2, f.z, None, [], f.B.subs(repl),
f.C.subs(repl), f.M.subs(repl))
if not any(e.has(S.NaN, oo, -oo, zoo) for e in [f2.B, f2.M, f2.C]):
return f2
return None
class MeijerFormula(object):
"""
This class represents a Meijer G-function formula.
Its data members are:
- z, the argument
- symbols, the free symbols (parameters) in the formula
- func, the function
- B, C, M (c/f ordinary Formula)
"""
def __init__(self, an, ap, bm, bq, z, symbols, B, C, M, matcher):
an, ap, bm, bq = [Tuple(*list(map(expand, w))) for w in [an, ap, bm, bq]]
self.func = G_Function(an, ap, bm, bq)
self.z = z
self.symbols = symbols
self._matcher = matcher
self.B = B
self.C = C
self.M = M
@property
def closed_form(self):
return reduce(lambda s,m: s+m[0]*m[1], zip(self.C, self.B), S.Zero)
def try_instantiate(self, func):
"""
Try to instantiate the current formula to (almost) match func.
This uses the _matcher passed on init.
"""
if func.signature != self.func.signature:
return None
res = self._matcher(func)
if res is not None:
subs, newfunc = res
return MeijerFormula(newfunc.an, newfunc.ap, newfunc.bm, newfunc.bq,
self.z, [],
self.B.subs(subs), self.C.subs(subs),
self.M.subs(subs), None)
class MeijerFormulaCollection(object):
"""
This class holds a collection of meijer g formulae.
"""
def __init__(self):
formulae = []
add_meijerg_formulae(formulae)
self.formulae = defaultdict(list)
for formula in formulae:
self.formulae[formula.func.signature].append(formula)
self.formulae = dict(self.formulae)
def lookup_origin(self, func):
""" Try to find a formula that matches func. """
if not func.signature in self.formulae:
return None
for formula in self.formulae[func.signature]:
res = formula.try_instantiate(func)
if res is not None:
return res
class Operator(object):
"""
Base class for operators to be applied to our functions.
These operators are differential operators. They are by convention
expressed in the variable D = z*d/dz (although this base class does
not actually care).
Note that when the operator is applied to an object, we typically do
*not* blindly differentiate but instead use a different representation
of the z*d/dz operator (see make_derivative_operator).
To subclass from this, define a __init__ method that initializes a
self._poly variable. This variable stores a polynomial. By convention
the generator is z*d/dz, and acts to the right of all coefficients.
Thus this poly
x**2 + 2*z*x + 1
represents the differential operator
(z*d/dz)**2 + 2*z**2*d/dz.
This class is used only in the implementation of the hypergeometric
function expansion algorithm.
"""
def apply(self, obj, op):
"""
Apply ``self`` to the object ``obj``, where the generator is ``op``.
Examples
========
>>> from sympy.simplify.hyperexpand import Operator
>>> from sympy.polys.polytools import Poly
>>> from sympy.abc import x, y, z
>>> op = Operator()
>>> op._poly = Poly(x**2 + z*x + y, x)
>>> op.apply(z**7, lambda f: f.diff(z))
y*z**7 + 7*z**7 + 42*z**5
"""
coeffs = self._poly.all_coeffs()
coeffs.reverse()
diffs = [obj]
for c in coeffs[1:]:
diffs.append(op(diffs[-1]))
r = coeffs[0]*diffs[0]
for c, d in zip(coeffs[1:], diffs[1:]):
r += c*d
return r
class MultOperator(Operator):
""" Simply multiply by a "constant" """
def __init__(self, p):
self._poly = Poly(p, _x)
class ShiftA(Operator):
""" Increment an upper index. """
def __init__(self, ai):
ai = sympify(ai)
if ai == 0:
raise ValueError('Cannot increment zero upper index.')
self._poly = Poly(_x/ai + 1, _x)
def __str__(self):
return '<Increment upper %s.>' % (1/self._poly.all_coeffs()[0])
class ShiftB(Operator):
""" Decrement a lower index. """
def __init__(self, bi):
bi = sympify(bi)
if bi == 1:
raise ValueError('Cannot decrement unit lower index.')
self._poly = Poly(_x/(bi - 1) + 1, _x)
def __str__(self):
return '<Decrement lower %s.>' % (1/self._poly.all_coeffs()[0] + 1)
class UnShiftA(Operator):
""" Decrement an upper index. """
def __init__(self, ap, bq, i, z):
""" Note: i counts from zero! """
ap, bq, i = list(map(sympify, [ap, bq, i]))
self._ap = ap
self._bq = bq
self._i = i
ap = list(ap)
bq = list(bq)
ai = ap.pop(i) - 1
if ai == 0:
raise ValueError('Cannot decrement unit upper index.')
m = Poly(z*ai, _x)
for a in ap:
m *= Poly(_x + a, _x)
A = Dummy('A')
n = D = Poly(ai*A - ai, A)
for b in bq:
n *= (D + b - 1)
b0 = -n.nth(0)
if b0 == 0:
raise ValueError('Cannot decrement upper index: '
'cancels with lower')
n = Poly(Poly(n.all_coeffs()[:-1], A).as_expr().subs(A, _x/ai + 1), _x)
self._poly = Poly((n - m)/b0, _x)
def __str__(self):
return '<Decrement upper index #%s of %s, %s.>' % (self._i,
self._ap, self._bq)
class UnShiftB(Operator):
""" Increment a lower index. """
def __init__(self, ap, bq, i, z):
""" Note: i counts from zero! """
ap, bq, i = list(map(sympify, [ap, bq, i]))
self._ap = ap
self._bq = bq
self._i = i
ap = list(ap)
bq = list(bq)
bi = bq.pop(i) + 1
if bi == 0:
raise ValueError('Cannot increment -1 lower index.')
m = Poly(_x*(bi - 1), _x)
for b in bq:
m *= Poly(_x + b - 1, _x)
B = Dummy('B')
D = Poly((bi - 1)*B - bi + 1, B)
n = Poly(z, B)
for a in ap:
n *= (D + a)
b0 = n.nth(0)
if b0 == 0:
raise ValueError('Cannot increment index: cancels with upper')
n = Poly(Poly(n.all_coeffs()[:-1], B).as_expr().subs(
B, _x/(bi - 1) + 1), _x)
self._poly = Poly((m - n)/b0, _x)
def __str__(self):
return '<Increment lower index #%s of %s, %s.>' % (self._i,
self._ap, self._bq)
class MeijerShiftA(Operator):
""" Increment an upper b index. """
def __init__(self, bi):
bi = sympify(bi)
self._poly = Poly(bi - _x, _x)
def __str__(self):
return '<Increment upper b=%s.>' % (self._poly.all_coeffs()[1])
class MeijerShiftB(Operator):
""" Decrement an upper a index. """
def __init__(self, bi):
bi = sympify(bi)
self._poly = Poly(1 - bi + _x, _x)
def __str__(self):
return '<Decrement upper a=%s.>' % (1 - self._poly.all_coeffs()[1])
class MeijerShiftC(Operator):
""" Increment a lower b index. """
def __init__(self, bi):
bi = sympify(bi)
self._poly = Poly(-bi + _x, _x)
def __str__(self):
return '<Increment lower b=%s.>' % (-self._poly.all_coeffs()[1])
class MeijerShiftD(Operator):
""" Decrement a lower a index. """
def __init__(self, bi):
bi = sympify(bi)
self._poly = Poly(bi - 1 - _x, _x)
def __str__(self):
return '<Decrement lower a=%s.>' % (self._poly.all_coeffs()[1] + 1)
class MeijerUnShiftA(Operator):
""" Decrement an upper b index. """
def __init__(self, an, ap, bm, bq, i, z):
""" Note: i counts from zero! """
an, ap, bm, bq, i = list(map(sympify, [an, ap, bm, bq, i]))
self._an = an
self._ap = ap
self._bm = bm
self._bq = bq
self._i = i
an = list(an)
ap = list(ap)
bm = list(bm)
bq = list(bq)
bi = bm.pop(i) - 1
m = Poly(1, _x)
for b in bm:
m *= Poly(b - _x, _x)
for b in bq:
m *= Poly(_x - b, _x)
A = Dummy('A')
D = Poly(bi - A, A)
n = Poly(z, A)
for a in an:
n *= (D + 1 - a)
for a in ap:
n *= (-D + a - 1)
b0 = n.nth(0)
if b0 == 0:
raise ValueError('Cannot decrement upper b index (cancels)')
n = Poly(Poly(n.all_coeffs()[:-1], A).as_expr().subs(A, bi - _x), _x)
self._poly = Poly((m - n)/b0, _x)
def __str__(self):
return '<Decrement upper b index #%s of %s, %s, %s, %s.>' % (self._i,
self._an, self._ap, self._bm, self._bq)
class MeijerUnShiftB(Operator):
""" Increment an upper a index. """
def __init__(self, an, ap, bm, bq, i, z):
""" Note: i counts from zero! """
an, ap, bm, bq, i = list(map(sympify, [an, ap, bm, bq, i]))
self._an = an
self._ap = ap
self._bm = bm
self._bq = bq
self._i = i
an = list(an)
ap = list(ap)
bm = list(bm)
bq = list(bq)
ai = an.pop(i) + 1
m = Poly(z, _x)
for a in an:
m *= Poly(1 - a + _x, _x)
for a in ap:
m *= Poly(a - 1 - _x, _x)
B = Dummy('B')
D = Poly(B + ai - 1, B)
n = Poly(1, B)
for b in bm:
n *= (-D + b)
for b in bq:
n *= (D - b)
b0 = n.nth(0)
if b0 == 0:
raise ValueError('Cannot increment upper a index (cancels)')
n = Poly(Poly(n.all_coeffs()[:-1], B).as_expr().subs(
B, 1 - ai + _x), _x)
self._poly = Poly((m - n)/b0, _x)
def __str__(self):
return '<Increment upper a index #%s of %s, %s, %s, %s.>' % (self._i,
self._an, self._ap, self._bm, self._bq)
class MeijerUnShiftC(Operator):
""" Decrement a lower b index. """
# XXX this is "essentially" the same as MeijerUnShiftA. This "essentially"
# can be made rigorous using the functional equation G(1/z) = G'(z),
# where G' denotes a G function of slightly altered parameters.
# However, sorting out the details seems harder than just coding it
# again.
def __init__(self, an, ap, bm, bq, i, z):
""" Note: i counts from zero! """
an, ap, bm, bq, i = list(map(sympify, [an, ap, bm, bq, i]))
self._an = an
self._ap = ap
self._bm = bm
self._bq = bq
self._i = i
an = list(an)
ap = list(ap)
bm = list(bm)
bq = list(bq)
bi = bq.pop(i) - 1
m = Poly(1, _x)
for b in bm:
m *= Poly(b - _x, _x)
for b in bq:
m *= Poly(_x - b, _x)
C = Dummy('C')
D = Poly(bi + C, C)
n = Poly(z, C)
for a in an:
n *= (D + 1 - a)
for a in ap:
n *= (-D + a - 1)
b0 = n.nth(0)
if b0 == 0:
raise ValueError('Cannot decrement lower b index (cancels)')
n = Poly(Poly(n.all_coeffs()[:-1], C).as_expr().subs(C, _x - bi), _x)
self._poly = Poly((m - n)/b0, _x)
def __str__(self):
return '<Decrement lower b index #%s of %s, %s, %s, %s.>' % (self._i,
self._an, self._ap, self._bm, self._bq)
class MeijerUnShiftD(Operator):
""" Increment a lower a index. """
# XXX This is essentially the same as MeijerUnShiftA.
# See comment at MeijerUnShiftC.
def __init__(self, an, ap, bm, bq, i, z):
""" Note: i counts from zero! """
an, ap, bm, bq, i = list(map(sympify, [an, ap, bm, bq, i]))
self._an = an
self._ap = ap
self._bm = bm
self._bq = bq
self._i = i
an = list(an)
ap = list(ap)
bm = list(bm)
bq = list(bq)
ai = ap.pop(i) + 1
m = Poly(z, _x)
for a in an:
m *= Poly(1 - a + _x, _x)
for a in ap:
m *= Poly(a - 1 - _x, _x)
B = Dummy('B') # - this is the shift operator `D_I`
D = Poly(ai - 1 - B, B)
n = Poly(1, B)
for b in bm:
n *= (-D + b)
for b in bq:
n *= (D - b)
b0 = n.nth(0)
if b0 == 0:
raise ValueError('Cannot increment lower a index (cancels)')
n = Poly(Poly(n.all_coeffs()[:-1], B).as_expr().subs(
B, ai - 1 - _x), _x)
self._poly = Poly((m - n)/b0, _x)
def __str__(self):
return '<Increment lower a index #%s of %s, %s, %s, %s.>' % (self._i,
self._an, self._ap, self._bm, self._bq)
class ReduceOrder(Operator):
""" Reduce Order by cancelling an upper and a lower index. """
def __new__(cls, ai, bj):
""" For convenience if reduction is not possible, return None. """
ai = sympify(ai)
bj = sympify(bj)
n = ai - bj
if not n.is_Integer or n < 0:
return None
if bj.is_integer and bj.is_nonpositive:
return None
expr = Operator.__new__(cls)
p = S.One
for k in range(n):
p *= (_x + bj + k)/(bj + k)
expr._poly = Poly(p, _x)
expr._a = ai
expr._b = bj
return expr
@classmethod
def _meijer(cls, b, a, sign):
""" Cancel b + sign*s and a + sign*s
This is for meijer G functions. """
b = sympify(b)
a = sympify(a)
n = b - a
if n.is_negative or not n.is_Integer:
return None
expr = Operator.__new__(cls)
p = S.One
for k in range(n):
p *= (sign*_x + a + k)
expr._poly = Poly(p, _x)
if sign == -1:
expr._a = b
expr._b = a
else:
expr._b = Add(1, a - 1, evaluate=False)
expr._a = Add(1, b - 1, evaluate=False)
return expr
@classmethod
def meijer_minus(cls, b, a):
return cls._meijer(b, a, -1)
@classmethod
def meijer_plus(cls, a, b):
return cls._meijer(1 - a, 1 - b, 1)
def __str__(self):
return '<Reduce order by cancelling upper %s with lower %s.>' % \
(self._a, self._b)
def _reduce_order(ap, bq, gen, key):
""" Order reduction algorithm used in Hypergeometric and Meijer G """
ap = list(ap)
bq = list(bq)
ap.sort(key=key)
bq.sort(key=key)
nap = []
# we will edit bq in place
operators = []
for a in ap:
op = None
for i in range(len(bq)):
op = gen(a, bq[i])
if op is not None:
bq.pop(i)
break
if op is None:
nap.append(a)
else:
operators.append(op)
return nap, bq, operators
def reduce_order(func):
"""
Given the hypergeometric function ``func``, find a sequence of operators to
reduces order as much as possible.
Return (newfunc, [operators]), where applying the operators to the
hypergeometric function newfunc yields func.
Examples
========
>>> from sympy.simplify.hyperexpand import reduce_order, Hyper_Function
>>> reduce_order(Hyper_Function((1, 2), (3, 4)))
(Hyper_Function((1, 2), (3, 4)), [])
>>> reduce_order(Hyper_Function((1,), (1,)))
(Hyper_Function((), ()), [<Reduce order by cancelling upper 1 with lower 1.>])
>>> reduce_order(Hyper_Function((2, 4), (3, 3)))
(Hyper_Function((2,), (3,)), [<Reduce order by cancelling
upper 4 with lower 3.>])
"""
nap, nbq, operators = _reduce_order(func.ap, func.bq, ReduceOrder, default_sort_key)
return Hyper_Function(Tuple(*nap), Tuple(*nbq)), operators
def reduce_order_meijer(func):
"""
Given the Meijer G function parameters, ``func``, find a sequence of
operators that reduces order as much as possible.
Return newfunc, [operators].
Examples
========
>>> from sympy.simplify.hyperexpand import (reduce_order_meijer,
... G_Function)
>>> reduce_order_meijer(G_Function([3, 4], [5, 6], [3, 4], [1, 2]))[0]
G_Function((4, 3), (5, 6), (3, 4), (2, 1))
>>> reduce_order_meijer(G_Function([3, 4], [5, 6], [3, 4], [1, 8]))[0]
G_Function((3,), (5, 6), (3, 4), (1,))
>>> reduce_order_meijer(G_Function([3, 4], [5, 6], [7, 5], [1, 5]))[0]
G_Function((3,), (), (), (1,))
>>> reduce_order_meijer(G_Function([3, 4], [5, 6], [7, 5], [5, 3]))[0]
G_Function((), (), (), ())
"""
nan, nbq, ops1 = _reduce_order(func.an, func.bq, ReduceOrder.meijer_plus,
lambda x: default_sort_key(-x))
nbm, nap, ops2 = _reduce_order(func.bm, func.ap, ReduceOrder.meijer_minus,
default_sort_key)
return G_Function(nan, nap, nbm, nbq), ops1 + ops2
def make_derivative_operator(M, z):
""" Create a derivative operator, to be passed to Operator.apply. """
def doit(C):
r = z*C.diff(z) + C*M
r = r.applyfunc(make_simp(z))
return r
return doit
def apply_operators(obj, ops, op):
"""
Apply the list of operators ``ops`` to object ``obj``, substituting
``op`` for the generator.
"""
res = obj
for o in reversed(ops):
res = o.apply(res, op)
return res
def devise_plan(target, origin, z):
"""
Devise a plan (consisting of shift and un-shift operators) to be applied
to the hypergeometric function ``target`` to yield ``origin``.
Returns a list of operators.
Examples
========
>>> from sympy.simplify.hyperexpand import devise_plan, Hyper_Function
>>> from sympy.abc import z
Nothing to do:
>>> devise_plan(Hyper_Function((1, 2), ()), Hyper_Function((1, 2), ()), z)
[]
>>> devise_plan(Hyper_Function((), (1, 2)), Hyper_Function((), (1, 2)), z)
[]
Very simple plans:
>>> devise_plan(Hyper_Function((2,), ()), Hyper_Function((1,), ()), z)
[<Increment upper 1.>]
>>> devise_plan(Hyper_Function((), (2,)), Hyper_Function((), (1,)), z)
[<Increment lower index #0 of [], [1].>]
Several buckets:
>>> from sympy import S
>>> devise_plan(Hyper_Function((1, S.Half), ()),
... Hyper_Function((2, S('3/2')), ()), z) #doctest: +NORMALIZE_WHITESPACE
[<Decrement upper index #0 of [3/2, 1], [].>,
<Decrement upper index #0 of [2, 3/2], [].>]
A slightly more complicated plan:
>>> devise_plan(Hyper_Function((1, 3), ()), Hyper_Function((2, 2), ()), z)
[<Increment upper 2.>, <Decrement upper index #0 of [2, 2], [].>]
Another more complicated plan: (note that the ap have to be shifted first!)
>>> devise_plan(Hyper_Function((1, -1), (2,)), Hyper_Function((3, -2), (4,)), z)
[<Decrement lower 3.>, <Decrement lower 4.>,
<Decrement upper index #1 of [-1, 2], [4].>,
<Decrement upper index #1 of [-1, 3], [4].>, <Increment upper -2.>]
"""
abuckets, bbuckets, nabuckets, nbbuckets = [sift(params, _mod1) for
params in (target.ap, target.bq, origin.ap, origin.bq)]
if len(list(abuckets.keys())) != len(list(nabuckets.keys())) or \
len(list(bbuckets.keys())) != len(list(nbbuckets.keys())):
raise ValueError('%s not reachable from %s' % (target, origin))
ops = []
def do_shifts(fro, to, inc, dec):
ops = []
for i in range(len(fro)):
if to[i] - fro[i] > 0:
sh = inc
ch = 1
else:
sh = dec
ch = -1
while to[i] != fro[i]:
ops += [sh(fro, i)]
fro[i] += ch
return ops
def do_shifts_a(nal, nbk, al, aother, bother):
""" Shift us from (nal, nbk) to (al, nbk). """
return do_shifts(nal, al, lambda p, i: ShiftA(p[i]),
lambda p, i: UnShiftA(p + aother, nbk + bother, i, z))
def do_shifts_b(nal, nbk, bk, aother, bother):
""" Shift us from (nal, nbk) to (nal, bk). """
return do_shifts(nbk, bk,
lambda p, i: UnShiftB(nal + aother, p + bother, i, z),
lambda p, i: ShiftB(p[i]))
for r in sorted(list(abuckets.keys()) + list(bbuckets.keys()), key=default_sort_key):
al = ()
nal = ()
bk = ()
nbk = ()
if r in abuckets:
al = abuckets[r]
nal = nabuckets[r]
if r in bbuckets:
bk = bbuckets[r]
nbk = nbbuckets[r]
if len(al) != len(nal) or len(bk) != len(nbk):
raise ValueError('%s not reachable from %s' % (target, origin))
al, nal, bk, nbk = [sorted(list(w), key=default_sort_key)
for w in [al, nal, bk, nbk]]
def others(dic, key):
l = []
for k, value in dic.items():
if k != key:
l += list(dic[k])
return l
aother = others(nabuckets, r)
bother = others(nbbuckets, r)
if len(al) == 0:
# there can be no complications, just shift the bs as we please
ops += do_shifts_b([], nbk, bk, aother, bother)
elif len(bk) == 0:
# there can be no complications, just shift the as as we please
ops += do_shifts_a(nal, [], al, aother, bother)
else:
namax = nal[-1]
amax = al[-1]
if nbk[0] - namax <= 0 or bk[0] - amax <= 0:
raise ValueError('Non-suitable parameters.')
if namax - amax > 0:
# we are going to shift down - first do the as, then the bs
ops += do_shifts_a(nal, nbk, al, aother, bother)
ops += do_shifts_b(al, nbk, bk, aother, bother)
else:
# we are going to shift up - first do the bs, then the as
ops += do_shifts_b(nal, nbk, bk, aother, bother)
ops += do_shifts_a(nal, bk, al, aother, bother)
nabuckets[r] = al
nbbuckets[r] = bk
ops.reverse()
return ops
def try_shifted_sum(func, z):
""" Try to recognise a hypergeometric sum that starts from k > 0. """
abuckets, bbuckets = sift(func.ap, _mod1), sift(func.bq, _mod1)
if len(abuckets[S.Zero]) != 1:
return None
r = abuckets[S.Zero][0]
if r <= 0:
return None
if not S.Zero in bbuckets:
return None
l = list(bbuckets[S.Zero])
l.sort()
k = l[0]
if k <= 0:
return None
nap = list(func.ap)
nap.remove(r)
nbq = list(func.bq)
nbq.remove(k)
k -= 1
nap = [x - k for x in nap]
nbq = [x - k for x in nbq]
ops = []
for n in range(r - 1):
ops.append(ShiftA(n + 1))
ops.reverse()
fac = factorial(k)/z**k
for a in nap:
fac /= rf(a, k)
for b in nbq:
fac *= rf(b, k)
ops += [MultOperator(fac)]
p = 0
for n in range(k):
m = z**n/factorial(n)
for a in nap:
m *= rf(a, n)
for b in nbq:
m /= rf(b, n)
p += m
return Hyper_Function(nap, nbq), ops, -p
def try_polynomial(func, z):
""" Recognise polynomial cases. Returns None if not such a case.
Requires order to be fully reduced. """
abuckets, bbuckets = sift(func.ap, _mod1), sift(func.bq, _mod1)
a0 = abuckets[S.Zero]
b0 = bbuckets[S.Zero]
a0.sort()
b0.sort()
al0 = [x for x in a0 if x <= 0]
bl0 = [x for x in b0 if x <= 0]
if bl0 and all(a < bl0[-1] for a in al0):
return oo
if not al0:
return None
a = al0[-1]
fac = 1
res = S.One
for n in Tuple(*list(range(-a))):
fac *= z
fac /= n + 1
for a in func.ap:
fac *= a + n
for b in func.bq:
fac /= b + n
res += fac
return res
def try_lerchphi(func):
"""
Try to find an expression for Hyper_Function ``func`` in terms of Lerch
Transcendents.
Return None if no such expression can be found.
"""
# This is actually quite simple, and is described in Roach's paper,
# section 18.
# We don't need to implement the reduction to polylog here, this
# is handled by expand_func.
from sympy.matrices import Matrix, zeros
from sympy.polys import apart
# First we need to figure out if the summation coefficient is a rational
# function of the summation index, and construct that rational function.
abuckets, bbuckets = sift(func.ap, _mod1), sift(func.bq, _mod1)
paired = {}
for key, value in abuckets.items():
if key != 0 and not key in bbuckets:
return None
bvalue = bbuckets[key]
paired[key] = (list(value), list(bvalue))
bbuckets.pop(key, None)
if bbuckets != {}:
return None
if not S.Zero in abuckets:
return None
aints, bints = paired[S.Zero]
# Account for the additional n! in denominator
paired[S.Zero] = (aints, bints + [1])
t = Dummy('t')
numer = S.One
denom = S.One
for key, (avalue, bvalue) in paired.items():
if len(avalue) != len(bvalue):
return None
# Note that since order has been reduced fully, all the b are
# bigger than all the a they differ from by an integer. In particular
# if there are any negative b left, this function is not well-defined.
for a, b in zip(avalue, bvalue):
if (a - b).is_positive:
k = a - b
numer *= rf(b + t, k)
denom *= rf(b, k)
else:
k = b - a
numer *= rf(a, k)
denom *= rf(a + t, k)
# Now do a partial fraction decomposition.
# We assemble two structures: a list monomials of pairs (a, b) representing
# a*t**b (b a non-negative integer), and a dict terms, where
# terms[a] = [(b, c)] means that there is a term b/(t-a)**c.
part = apart(numer/denom, t)
args = Add.make_args(part)
monomials = []
terms = {}
for arg in args:
numer, denom = arg.as_numer_denom()
if not denom.has(t):
p = Poly(numer, t)
if not p.is_monomial:
raise TypeError("p should be monomial")
((b, ), a) = p.LT()
monomials += [(a/denom, b)]
continue
if numer.has(t):
raise NotImplementedError('Need partial fraction decomposition'
' with linear denominators')
indep, [dep] = denom.as_coeff_mul(t)
n = 1
if dep.is_Pow:
n = dep.exp
dep = dep.base
if dep == t:
a == 0
elif dep.is_Add:
a, tmp = dep.as_independent(t)
b = 1
if tmp != t:
b, _ = tmp.as_independent(t)
if dep != b*t + a:
raise NotImplementedError('unrecognised form %s' % dep)
a /= b
indep *= b**n
else:
raise NotImplementedError('unrecognised form of partial fraction')
terms.setdefault(a, []).append((numer/indep, n))
# Now that we have this information, assemble our formula. All the
# monomials yield rational functions and go into one basis element.
# The terms[a] are related by differentiation. If the largest exponent is
# n, we need lerchphi(z, k, a) for k = 1, 2, ..., n.
# deriv maps a basis to its derivative, expressed as a C(z)-linear
# combination of other basis elements.
deriv = {}
coeffs = {}
z = Dummy('z')
monomials.sort(key=lambda x: x[1])
mon = {0: 1/(1 - z)}
if monomials:
for k in range(monomials[-1][1]):
mon[k + 1] = z*mon[k].diff(z)
for a, n in monomials:
coeffs.setdefault(S.One, []).append(a*mon[n])
for a, l in terms.items():
for c, k in l:
coeffs.setdefault(lerchphi(z, k, a), []).append(c)
l.sort(key=lambda x: x[1])
for k in range(2, l[-1][1] + 1):
deriv[lerchphi(z, k, a)] = [(-a, lerchphi(z, k, a)),
(1, lerchphi(z, k - 1, a))]
deriv[lerchphi(z, 1, a)] = [(-a, lerchphi(z, 1, a)),
(1/(1 - z), S.One)]
trans = {}
for n, b in enumerate([S.One] + list(deriv.keys())):
trans[b] = n
basis = [expand_func(b) for (b, _) in sorted(list(trans.items()),
key=lambda x:x[1])]
B = Matrix(basis)
C = Matrix([[0]*len(B)])
for b, c in coeffs.items():
C[trans[b]] = Add(*c)
M = zeros(len(B))
for b, l in deriv.items():
for c, b2 in l:
M[trans[b], trans[b2]] = c
return Formula(func, z, None, [], B, C, M)
def build_hypergeometric_formula(func):
"""
Create a formula object representing the hypergeometric function ``func``.
"""
# We know that no `ap` are negative integers, otherwise "detect poly"
# would have kicked in. However, `ap` could be empty. In this case we can
# use a different basis.
# I'm not aware of a basis that works in all cases.
from sympy import zeros, Matrix, eye
z = Dummy('z')
if func.ap:
afactors = [_x + a for a in func.ap]
bfactors = [_x + b - 1 for b in func.bq]
expr = _x*Mul(*bfactors) - z*Mul(*afactors)
poly = Poly(expr, _x)
n = poly.degree()
basis = []
M = zeros(n)
for k in range(n):
a = func.ap[0] + k
basis += [hyper([a] + list(func.ap[1:]), func.bq, z)]
if k < n - 1:
M[k, k] = -a
M[k, k + 1] = a
B = Matrix(basis)
C = Matrix([[1] + [0]*(n - 1)])
derivs = [eye(n)]
for k in range(n):
derivs.append(M*derivs[k])
l = poly.all_coeffs()
l.reverse()
res = [0]*n
for k, c in enumerate(l):
for r, d in enumerate(C*derivs[k]):
res[r] += c*d
for k, c in enumerate(res):
M[n - 1, k] = -c/derivs[n - 1][0, n - 1]/poly.all_coeffs()[0]
return Formula(func, z, None, [], B, C, M)
else:
# Since there are no `ap`, none of the `bq` can be non-positive
# integers.
basis = []
bq = list(func.bq[:])
for i in range(len(bq)):
basis += [hyper([], bq, z)]
bq[i] += 1
basis += [hyper([], bq, z)]
B = Matrix(basis)
n = len(B)
C = Matrix([[1] + [0]*(n - 1)])
M = zeros(n)
M[0, n - 1] = z/Mul(*func.bq)
for k in range(1, n):
M[k, k - 1] = func.bq[k - 1]
M[k, k] = -func.bq[k - 1]
return Formula(func, z, None, [], B, C, M)
def hyperexpand_special(ap, bq, z):
"""
Try to find a closed-form expression for hyper(ap, bq, z), where ``z``
is supposed to be a "special" value, e.g. 1.
This function tries various of the classical summation formulae
(Gauss, Saalschuetz, etc).
"""
# This code is very ad-hoc. There are many clever algorithms
# (notably Zeilberger's) related to this problem.
# For now we just want a few simple cases to work.
p, q = len(ap), len(bq)
z_ = z
z = unpolarify(z)
if z == 0:
return S.One
if p == 2 and q == 1:
# 2F1
a, b, c = ap + bq
if z == 1:
# Gauss
return gamma(c - a - b)*gamma(c)/gamma(c - a)/gamma(c - b)
if z == -1 and simplify(b - a + c) == 1:
b, a = a, b
if z == -1 and simplify(a - b + c) == 1:
# Kummer
if b.is_integer and b.is_negative:
return 2*cos(pi*b/2)*gamma(-b)*gamma(b - a + 1) \
/gamma(-b/2)/gamma(b/2 - a + 1)
else:
return gamma(b/2 + 1)*gamma(b - a + 1) \
/gamma(b + 1)/gamma(b/2 - a + 1)
# TODO tons of more formulae
# investigate what algorithms exist
return hyper(ap, bq, z_)
_collection = None
def _hyperexpand(func, z, ops0=[], z0=Dummy('z0'), premult=1, prem=0,
rewrite='default'):
"""
Try to find an expression for the hypergeometric function ``func``.
The result is expressed in terms of a dummy variable z0. Then it
is multiplied by premult. Then ops0 is applied.
premult must be a*z**prem for some a independent of z.
"""
if z.is_zero:
return S.One
z = polarify(z, subs=False)
if rewrite == 'default':
rewrite = 'nonrepsmall'
def carryout_plan(f, ops):
C = apply_operators(f.C.subs(f.z, z0), ops,
make_derivative_operator(f.M.subs(f.z, z0), z0))
from sympy import eye
C = apply_operators(C, ops0,
make_derivative_operator(f.M.subs(f.z, z0)
+ prem*eye(f.M.shape[0]), z0))
if premult == 1:
C = C.applyfunc(make_simp(z0))
r = reduce(lambda s,m: s+m[0]*m[1], zip(C, f.B.subs(f.z, z0)), S.Zero)*premult
res = r.subs(z0, z)
if rewrite:
res = res.rewrite(rewrite)
return res
# TODO
# The following would be possible:
# *) PFD Duplication (see Kelly Roach's paper)
# *) In a similar spirit, try_lerchphi() can be generalised considerably.
global _collection
if _collection is None:
_collection = FormulaCollection()
debug('Trying to expand hypergeometric function ', func)
# First reduce order as much as possible.
func, ops = reduce_order(func)
if ops:
debug(' Reduced order to ', func)
else:
debug(' Could not reduce order.')
# Now try polynomial cases
res = try_polynomial(func, z0)
if res is not None:
debug(' Recognised polynomial.')
p = apply_operators(res, ops, lambda f: z0*f.diff(z0))
p = apply_operators(p*premult, ops0, lambda f: z0*f.diff(z0))
return unpolarify(simplify(p).subs(z0, z))
# Try to recognise a shifted sum.
p = S.Zero
res = try_shifted_sum(func, z0)
if res is not None:
func, nops, p = res
debug(' Recognised shifted sum, reduced order to ', func)
ops += nops
# apply the plan for poly
p = apply_operators(p, ops, lambda f: z0*f.diff(z0))
p = apply_operators(p*premult, ops0, lambda f: z0*f.diff(z0))
p = simplify(p).subs(z0, z)
# Try special expansions early.
if unpolarify(z) in [1, -1] and (len(func.ap), len(func.bq)) == (2, 1):
f = build_hypergeometric_formula(func)
r = carryout_plan(f, ops).replace(hyper, hyperexpand_special)
if not r.has(hyper):
return r + p
# Try to find a formula in our collection
formula = _collection.lookup_origin(func)
# Now try a lerch phi formula
if formula is None:
formula = try_lerchphi(func)
if formula is None:
debug(' Could not find an origin. ',
'Will return answer in terms of '
'simpler hypergeometric functions.')
formula = build_hypergeometric_formula(func)
debug(' Found an origin: ', formula.closed_form, ' ', formula.func)
# We need to find the operators that convert formula into func.
ops += devise_plan(func, formula.func, z0)
# Now carry out the plan.
r = carryout_plan(formula, ops) + p
return powdenest(r, polar=True).replace(hyper, hyperexpand_special)
def devise_plan_meijer(fro, to, z):
"""
Find operators to convert G-function ``fro`` into G-function ``to``.
It is assumed that fro and to have the same signatures, and that in fact
any corresponding pair of parameters differs by integers, and a direct path
is possible. I.e. if there are parameters a1 b1 c1 and a2 b2 c2 it is
assumed that a1 can be shifted to a2, etc. The only thing this routine
determines is the order of shifts to apply, nothing clever will be tried.
It is also assumed that fro is suitable.
Examples
========
>>> from sympy.simplify.hyperexpand import (devise_plan_meijer,
... G_Function)
>>> from sympy.abc import z
Empty plan:
>>> devise_plan_meijer(G_Function([1], [2], [3], [4]),
... G_Function([1], [2], [3], [4]), z)
[]
Very simple plans:
>>> devise_plan_meijer(G_Function([0], [], [], []),
... G_Function([1], [], [], []), z)
[<Increment upper a index #0 of [0], [], [], [].>]
>>> devise_plan_meijer(G_Function([0], [], [], []),
... G_Function([-1], [], [], []), z)
[<Decrement upper a=0.>]
>>> devise_plan_meijer(G_Function([], [1], [], []),
... G_Function([], [2], [], []), z)
[<Increment lower a index #0 of [], [1], [], [].>]
Slightly more complicated plans:
>>> devise_plan_meijer(G_Function([0], [], [], []),
... G_Function([2], [], [], []), z)
[<Increment upper a index #0 of [1], [], [], [].>,
<Increment upper a index #0 of [0], [], [], [].>]
>>> devise_plan_meijer(G_Function([0], [], [0], []),
... G_Function([-1], [], [1], []), z)
[<Increment upper b=0.>, <Decrement upper a=0.>]
Order matters:
>>> devise_plan_meijer(G_Function([0], [], [0], []),
... G_Function([1], [], [1], []), z)
[<Increment upper a index #0 of [0], [], [1], [].>, <Increment upper b=0.>]
"""
# TODO for now, we use the following simple heuristic: inverse-shift
# when possible, shift otherwise. Give up if we cannot make progress.
def try_shift(f, t, shifter, diff, counter):
""" Try to apply ``shifter`` in order to bring some element in ``f``
nearer to its counterpart in ``to``. ``diff`` is +/- 1 and
determines the effect of ``shifter``. Counter is a list of elements
blocking the shift.
Return an operator if change was possible, else None.
"""
for idx, (a, b) in enumerate(zip(f, t)):
if (
(a - b).is_integer and (b - a)/diff > 0 and
all(a != x for x in counter)):
sh = shifter(idx)
f[idx] += diff
return sh
fan = list(fro.an)
fap = list(fro.ap)
fbm = list(fro.bm)
fbq = list(fro.bq)
ops = []
change = True
while change:
change = False
op = try_shift(fan, to.an,
lambda i: MeijerUnShiftB(fan, fap, fbm, fbq, i, z),
1, fbm + fbq)
if op is not None:
ops += [op]
change = True
continue
op = try_shift(fap, to.ap,
lambda i: MeijerUnShiftD(fan, fap, fbm, fbq, i, z),
1, fbm + fbq)
if op is not None:
ops += [op]
change = True
continue
op = try_shift(fbm, to.bm,
lambda i: MeijerUnShiftA(fan, fap, fbm, fbq, i, z),
-1, fan + fap)
if op is not None:
ops += [op]
change = True
continue
op = try_shift(fbq, to.bq,
lambda i: MeijerUnShiftC(fan, fap, fbm, fbq, i, z),
-1, fan + fap)
if op is not None:
ops += [op]
change = True
continue
op = try_shift(fan, to.an, lambda i: MeijerShiftB(fan[i]), -1, [])
if op is not None:
ops += [op]
change = True
continue
op = try_shift(fap, to.ap, lambda i: MeijerShiftD(fap[i]), -1, [])
if op is not None:
ops += [op]
change = True
continue
op = try_shift(fbm, to.bm, lambda i: MeijerShiftA(fbm[i]), 1, [])
if op is not None:
ops += [op]
change = True
continue
op = try_shift(fbq, to.bq, lambda i: MeijerShiftC(fbq[i]), 1, [])
if op is not None:
ops += [op]
change = True
continue
if fan != list(to.an) or fap != list(to.ap) or fbm != list(to.bm) or \
fbq != list(to.bq):
raise NotImplementedError('Could not devise plan.')
ops.reverse()
return ops
_meijercollection = None
def _meijergexpand(func, z0, allow_hyper=False, rewrite='default',
place=None):
"""
Try to find an expression for the Meijer G function specified
by the G_Function ``func``. If ``allow_hyper`` is True, then returning
an expression in terms of hypergeometric functions is allowed.
Currently this just does Slater's theorem.
If expansions exist both at zero and at infinity, ``place``
can be set to ``0`` or ``zoo`` for the preferred choice.
"""
global _meijercollection
if _meijercollection is None:
_meijercollection = MeijerFormulaCollection()
if rewrite == 'default':
rewrite = None
func0 = func
debug('Try to expand Meijer G function corresponding to ', func)
# We will play games with analytic continuation - rather use a fresh symbol
z = Dummy('z')
func, ops = reduce_order_meijer(func)
if ops:
debug(' Reduced order to ', func)
else:
debug(' Could not reduce order.')
# Try to find a direct formula
f = _meijercollection.lookup_origin(func)
if f is not None:
debug(' Found a Meijer G formula: ', f.func)
ops += devise_plan_meijer(f.func, func, z)
# Now carry out the plan.
C = apply_operators(f.C.subs(f.z, z), ops,
make_derivative_operator(f.M.subs(f.z, z), z))
C = C.applyfunc(make_simp(z))
r = C*f.B.subs(f.z, z)
r = r[0].subs(z, z0)
return powdenest(r, polar=True)
debug(" Could not find a direct formula. Trying Slater's theorem.")
# TODO the following would be possible:
# *) Paired Index Theorems
# *) PFD Duplication
# (See Kelly Roach's paper for details on either.)
#
# TODO Also, we tend to create combinations of gamma functions that can be
# simplified.
def can_do(pbm, pap):
""" Test if slater applies. """
for i in pbm:
if len(pbm[i]) > 1:
l = 0
if i in pap:
l = len(pap[i])
if l + 1 < len(pbm[i]):
return False
return True
def do_slater(an, bm, ap, bq, z, zfinal):
# zfinal is the value that will eventually be substituted for z.
# We pass it to _hyperexpand to improve performance.
func = G_Function(an, bm, ap, bq)
_, pbm, pap, _ = func.compute_buckets()
if not can_do(pbm, pap):
return S.Zero, False
cond = len(an) + len(ap) < len(bm) + len(bq)
if len(an) + len(ap) == len(bm) + len(bq):
cond = abs(z) < 1
if cond is False:
return S.Zero, False
res = S.Zero
for m in pbm:
if len(pbm[m]) == 1:
bh = pbm[m][0]
fac = 1
bo = list(bm)
bo.remove(bh)
for bj in bo:
fac *= gamma(bj - bh)
for aj in an:
fac *= gamma(1 + bh - aj)
for bj in bq:
fac /= gamma(1 + bh - bj)
for aj in ap:
fac /= gamma(aj - bh)
nap = [1 + bh - a for a in list(an) + list(ap)]
nbq = [1 + bh - b for b in list(bo) + list(bq)]
k = polar_lift(S.NegativeOne**(len(ap) - len(bm)))
harg = k*zfinal
# NOTE even though k "is" +-1, this has to be t/k instead of
# t*k ... we are using polar numbers for consistency!
premult = (t/k)**bh
hyp = _hyperexpand(Hyper_Function(nap, nbq), harg, ops,
t, premult, bh, rewrite=None)
res += fac * hyp
else:
b_ = pbm[m][0]
ki = [bi - b_ for bi in pbm[m][1:]]
u = len(ki)
li = [ai - b_ for ai in pap[m][:u + 1]]
bo = list(bm)
for b in pbm[m]:
bo.remove(b)
ao = list(ap)
for a in pap[m][:u]:
ao.remove(a)
lu = li[-1]
di = [l - k for (l, k) in zip(li, ki)]
# We first work out the integrand:
s = Dummy('s')
integrand = z**s
for b in bm:
if not Mod(b, 1) and b.is_Number:
b = int(round(b))
integrand *= gamma(b - s)
for a in an:
integrand *= gamma(1 - a + s)
for b in bq:
integrand /= gamma(1 - b + s)
for a in ap:
integrand /= gamma(a - s)
# Now sum the finitely many residues:
# XXX This speeds up some cases - is it a good idea?
integrand = expand_func(integrand)
for r in range(int(round(lu))):
resid = residue(integrand, s, b_ + r)
resid = apply_operators(resid, ops, lambda f: z*f.diff(z))
res -= resid
# Now the hypergeometric term.
au = b_ + lu
k = polar_lift(S.NegativeOne**(len(ao) + len(bo) + 1))
harg = k*zfinal
premult = (t/k)**au
nap = [1 + au - a for a in list(an) + list(ap)] + [1]
nbq = [1 + au - b for b in list(bm) + list(bq)]
hyp = _hyperexpand(Hyper_Function(nap, nbq), harg, ops,
t, premult, au, rewrite=None)
C = S.NegativeOne**(lu)/factorial(lu)
for i in range(u):
C *= S.NegativeOne**di[i]/rf(lu - li[i] + 1, di[i])
for a in an:
C *= gamma(1 - a + au)
for b in bo:
C *= gamma(b - au)
for a in ao:
C /= gamma(a - au)
for b in bq:
C /= gamma(1 - b + au)
res += C*hyp
return res, cond
t = Dummy('t')
slater1, cond1 = do_slater(func.an, func.bm, func.ap, func.bq, z, z0)
def tr(l):
return [1 - x for x in l]
for op in ops:
op._poly = Poly(op._poly.subs({z: 1/t, _x: -_x}), _x)
slater2, cond2 = do_slater(tr(func.bm), tr(func.an), tr(func.bq), tr(func.ap),
t, 1/z0)
slater1 = powdenest(slater1.subs(z, z0), polar=True)
slater2 = powdenest(slater2.subs(t, 1/z0), polar=True)
if not isinstance(cond2, bool):
cond2 = cond2.subs(t, 1/z)
m = func(z)
if m.delta > 0 or \
(m.delta == 0 and len(m.ap) == len(m.bq) and
(re(m.nu) < -1) is not False and polar_lift(z0) == polar_lift(1)):
# The condition delta > 0 means that the convergence region is
# connected. Any expression we find can be continued analytically
# to the entire convergence region.
# The conditions delta==0, p==q, re(nu) < -1 imply that G is continuous
# on the positive reals, so the values at z=1 agree.
if cond1 is not False:
cond1 = True
if cond2 is not False:
cond2 = True
if cond1 is True:
slater1 = slater1.rewrite(rewrite or 'nonrep')
else:
slater1 = slater1.rewrite(rewrite or 'nonrepsmall')
if cond2 is True:
slater2 = slater2.rewrite(rewrite or 'nonrep')
else:
slater2 = slater2.rewrite(rewrite or 'nonrepsmall')
if cond1 is not False and cond2 is not False:
# If one condition is False, there is no choice.
if place == 0:
cond2 = False
if place == zoo:
cond1 = False
if not isinstance(cond1, bool):
cond1 = cond1.subs(z, z0)
if not isinstance(cond2, bool):
cond2 = cond2.subs(z, z0)
def weight(expr, cond):
if cond is True:
c0 = 0
elif cond is False:
c0 = 1
else:
c0 = 2
if expr.has(oo, zoo, -oo, nan):
# XXX this actually should not happen, but consider
# S('meijerg(((0, -1/2, 0, -1/2, 1/2), ()), ((0,),
# (-1/2, -1/2, -1/2, -1)), exp_polar(I*pi))/4')
c0 = 3
return (c0, expr.count(hyper), expr.count_ops())
w1 = weight(slater1, cond1)
w2 = weight(slater2, cond2)
if min(w1, w2) <= (0, 1, oo):
if w1 < w2:
return slater1
else:
return slater2
if max(w1[0], w2[0]) <= 1 and max(w1[1], w2[1]) <= 1:
return Piecewise((slater1, cond1), (slater2, cond2), (func0(z0), True))
# We couldn't find an expression without hypergeometric functions.
# TODO it would be helpful to give conditions under which the integral
# is known to diverge.
r = Piecewise((slater1, cond1), (slater2, cond2), (func0(z0), True))
if r.has(hyper) and not allow_hyper:
debug(' Could express using hypergeometric functions, '
'but not allowed.')
if not r.has(hyper) or allow_hyper:
return r
return func0(z0)
def hyperexpand(f, allow_hyper=False, rewrite='default', place=None):
"""
Expand hypergeometric functions. If allow_hyper is True, allow partial
simplification (that is a result different from input,
but still containing hypergeometric functions).
If a G-function has expansions both at zero and at infinity,
``place`` can be set to ``0`` or ``zoo`` to indicate the
preferred choice.
Examples
========
>>> from sympy.simplify.hyperexpand import hyperexpand
>>> from sympy.functions import hyper
>>> from sympy.abc import z
>>> hyperexpand(hyper([], [], z))
exp(z)
Non-hyperegeometric parts of the expression and hypergeometric expressions
that are not recognised are left unchanged:
>>> hyperexpand(1 + hyper([1, 1, 1], [], z))
hyper((1, 1, 1), (), z) + 1
"""
f = sympify(f)
def do_replace(ap, bq, z):
r = _hyperexpand(Hyper_Function(ap, bq), z, rewrite=rewrite)
if r is None:
return hyper(ap, bq, z)
else:
return r
def do_meijer(ap, bq, z):
r = _meijergexpand(G_Function(ap[0], ap[1], bq[0], bq[1]), z,
allow_hyper, rewrite=rewrite, place=place)
if not r.has(nan, zoo, oo, -oo):
return r
return f.replace(hyper, do_replace).replace(meijerg, do_meijer)
|
201ce58c5badcdfc582f24fa8d6d89ed278141af264e2dba9887af25bb72ffac | from __future__ import print_function, division
from collections import defaultdict
from sympy.core import (Basic, S, Add, Mul, Pow, Symbol, sympify, expand_mul,
expand_func, Function, Dummy, Expr, factor_terms,
expand_power_exp, Eq)
from sympy.core.compatibility import iterable, ordered, range, as_int
from sympy.core.evaluate import global_evaluate
from sympy.core.function import expand_log, count_ops, _mexpand, _coeff_isneg, nfloat
from sympy.core.numbers import Float, I, pi, Rational, Integer
from sympy.core.rules import Transform
from sympy.core.sympify import _sympify
from sympy.functions import gamma, exp, sqrt, log, exp_polar, piecewise_fold, re
from sympy.functions.combinatorial.factorials import CombinatorialFunction
from sympy.functions.elementary.complexes import unpolarify
from sympy.functions.elementary.exponential import ExpBase
from sympy.functions.elementary.hyperbolic import HyperbolicFunction
from sympy.functions.elementary.integers import ceiling
from sympy.functions.elementary.piecewise import Piecewise, piecewise_fold
from sympy.functions.elementary.trigonometric import TrigonometricFunction
from sympy.functions.special.bessel import besselj, besseli, besselk, jn, bessely
from sympy.functions.special.tensor_functions import KroneckerDelta
from sympy.polys import together, cancel, factor
from sympy.simplify.combsimp import combsimp
from sympy.simplify.cse_opts import sub_pre, sub_post
from sympy.simplify.powsimp import powsimp
from sympy.simplify.radsimp import radsimp, fraction, collect_abs
from sympy.simplify.sqrtdenest import sqrtdenest
from sympy.simplify.trigsimp import trigsimp, exptrigsimp
from sympy.utilities.iterables import has_variety, sift
import mpmath
def separatevars(expr, symbols=[], dict=False, force=False):
"""
Separates variables in an expression, if possible. By
default, it separates with respect to all symbols in an
expression and collects constant coefficients that are
independent of symbols.
If dict=True then the separated terms will be returned
in a dictionary keyed to their corresponding symbols.
By default, all symbols in the expression will appear as
keys; if symbols are provided, then all those symbols will
be used as keys, and any terms in the expression containing
other symbols or non-symbols will be returned keyed to the
string 'coeff'. (Passing None for symbols will return the
expression in a dictionary keyed to 'coeff'.)
If force=True, then bases of powers will be separated regardless
of assumptions on the symbols involved.
Notes
=====
The order of the factors is determined by Mul, so that the
separated expressions may not necessarily be grouped together.
Although factoring is necessary to separate variables in some
expressions, it is not necessary in all cases, so one should not
count on the returned factors being factored.
Examples
========
>>> from sympy.abc import x, y, z, alpha
>>> from sympy import separatevars, sin
>>> separatevars((x*y)**y)
(x*y)**y
>>> separatevars((x*y)**y, force=True)
x**y*y**y
>>> e = 2*x**2*z*sin(y)+2*z*x**2
>>> separatevars(e)
2*x**2*z*(sin(y) + 1)
>>> separatevars(e, symbols=(x, y), dict=True)
{'coeff': 2*z, x: x**2, y: sin(y) + 1}
>>> separatevars(e, [x, y, alpha], dict=True)
{'coeff': 2*z, alpha: 1, x: x**2, y: sin(y) + 1}
If the expression is not really separable, or is only partially
separable, separatevars will do the best it can to separate it
by using factoring.
>>> separatevars(x + x*y - 3*x**2)
-x*(3*x - y - 1)
If the expression is not separable then expr is returned unchanged
or (if dict=True) then None is returned.
>>> eq = 2*x + y*sin(x)
>>> separatevars(eq) == eq
True
>>> separatevars(2*x + y*sin(x), symbols=(x, y), dict=True) == None
True
"""
expr = sympify(expr)
if dict:
return _separatevars_dict(_separatevars(expr, force), symbols)
else:
return _separatevars(expr, force)
def _separatevars(expr, force):
from sympy.functions.elementary.complexes import Abs
if isinstance(expr, Abs):
arg = expr.args[0]
if arg.is_Mul and not arg.is_number:
s = separatevars(arg, dict=True, force=force)
if s is not None:
return Mul(*map(expr.func, s.values()))
else:
return expr
if len(expr.free_symbols) < 2:
return expr
# don't destroy a Mul since much of the work may already be done
if expr.is_Mul:
args = list(expr.args)
changed = False
for i, a in enumerate(args):
args[i] = separatevars(a, force)
changed = changed or args[i] != a
if changed:
expr = expr.func(*args)
return expr
# get a Pow ready for expansion
if expr.is_Pow:
expr = Pow(separatevars(expr.base, force=force), expr.exp)
# First try other expansion methods
expr = expr.expand(mul=False, multinomial=False, force=force)
_expr, reps = posify(expr) if force else (expr, {})
expr = factor(_expr).subs(reps)
if not expr.is_Add:
return expr
# Find any common coefficients to pull out
args = list(expr.args)
commonc = args[0].args_cnc(cset=True, warn=False)[0]
for i in args[1:]:
commonc &= i.args_cnc(cset=True, warn=False)[0]
commonc = Mul(*commonc)
commonc = commonc.as_coeff_Mul()[1] # ignore constants
commonc_set = commonc.args_cnc(cset=True, warn=False)[0]
# remove them
for i, a in enumerate(args):
c, nc = a.args_cnc(cset=True, warn=False)
c = c - commonc_set
args[i] = Mul(*c)*Mul(*nc)
nonsepar = Add(*args)
if len(nonsepar.free_symbols) > 1:
_expr = nonsepar
_expr, reps = posify(_expr) if force else (_expr, {})
_expr = (factor(_expr)).subs(reps)
if not _expr.is_Add:
nonsepar = _expr
return commonc*nonsepar
def _separatevars_dict(expr, symbols):
if symbols:
if not all((t.is_Atom for t in symbols)):
raise ValueError("symbols must be Atoms.")
symbols = list(symbols)
elif symbols is None:
return {'coeff': expr}
else:
symbols = list(expr.free_symbols)
if not symbols:
return None
ret = dict(((i, []) for i in symbols + ['coeff']))
for i in Mul.make_args(expr):
expsym = i.free_symbols
intersection = set(symbols).intersection(expsym)
if len(intersection) > 1:
return None
if len(intersection) == 0:
# There are no symbols, so it is part of the coefficient
ret['coeff'].append(i)
else:
ret[intersection.pop()].append(i)
# rebuild
for k, v in ret.items():
ret[k] = Mul(*v)
return ret
def _is_sum_surds(p):
args = p.args if p.is_Add else [p]
for y in args:
if not ((y**2).is_Rational and y.is_extended_real):
return False
return True
def posify(eq):
"""Return eq (with generic symbols made positive) and a
dictionary containing the mapping between the old and new
symbols.
Any symbol that has positive=None will be replaced with a positive dummy
symbol having the same name. This replacement will allow more symbolic
processing of expressions, especially those involving powers and
logarithms.
A dictionary that can be sent to subs to restore eq to its original
symbols is also returned.
>>> from sympy import posify, Symbol, log, solve
>>> from sympy.abc import x
>>> posify(x + Symbol('p', positive=True) + Symbol('n', negative=True))
(_x + n + p, {_x: x})
>>> eq = 1/x
>>> log(eq).expand()
log(1/x)
>>> log(posify(eq)[0]).expand()
-log(_x)
>>> p, rep = posify(eq)
>>> log(p).expand().subs(rep)
-log(x)
It is possible to apply the same transformations to an iterable
of expressions:
>>> eq = x**2 - 4
>>> solve(eq, x)
[-2, 2]
>>> eq_x, reps = posify([eq, x]); eq_x
[_x**2 - 4, _x]
>>> solve(*eq_x)
[2]
"""
eq = sympify(eq)
if iterable(eq):
f = type(eq)
eq = list(eq)
syms = set()
for e in eq:
syms = syms.union(e.atoms(Symbol))
reps = {}
for s in syms:
reps.update(dict((v, k) for k, v in posify(s)[1].items()))
for i, e in enumerate(eq):
eq[i] = e.subs(reps)
return f(eq), {r: s for s, r in reps.items()}
reps = {s: Dummy(s.name, positive=True, **s.assumptions0)
for s in eq.free_symbols if s.is_positive is None}
eq = eq.subs(reps)
return eq, {r: s for s, r in reps.items()}
def hypersimp(f, k):
"""Given combinatorial term f(k) simplify its consecutive term ratio
i.e. f(k+1)/f(k). The input term can be composed of functions and
integer sequences which have equivalent representation in terms
of gamma special function.
The algorithm performs three basic steps:
1. Rewrite all functions in terms of gamma, if possible.
2. Rewrite all occurrences of gamma in terms of products
of gamma and rising factorial with integer, absolute
constant exponent.
3. Perform simplification of nested fractions, powers
and if the resulting expression is a quotient of
polynomials, reduce their total degree.
If f(k) is hypergeometric then as result we arrive with a
quotient of polynomials of minimal degree. Otherwise None
is returned.
For more information on the implemented algorithm refer to:
1. W. Koepf, Algorithms for m-fold Hypergeometric Summation,
Journal of Symbolic Computation (1995) 20, 399-417
"""
f = sympify(f)
g = f.subs(k, k + 1) / f
g = g.rewrite(gamma)
g = expand_func(g)
g = powsimp(g, deep=True, combine='exp')
if g.is_rational_function(k):
return simplify(g, ratio=S.Infinity)
else:
return None
def hypersimilar(f, g, k):
"""Returns True if 'f' and 'g' are hyper-similar.
Similarity in hypergeometric sense means that a quotient of
f(k) and g(k) is a rational function in k. This procedure
is useful in solving recurrence relations.
For more information see hypersimp().
"""
f, g = list(map(sympify, (f, g)))
h = (f/g).rewrite(gamma)
h = h.expand(func=True, basic=False)
return h.is_rational_function(k)
def signsimp(expr, evaluate=None):
"""Make all Add sub-expressions canonical wrt sign.
If an Add subexpression, ``a``, can have a sign extracted,
as determined by could_extract_minus_sign, it is replaced
with Mul(-1, a, evaluate=False). This allows signs to be
extracted from powers and products.
Examples
========
>>> from sympy import signsimp, exp, symbols
>>> from sympy.abc import x, y
>>> i = symbols('i', odd=True)
>>> n = -1 + 1/x
>>> n/x/(-n)**2 - 1/n/x
(-1 + 1/x)/(x*(1 - 1/x)**2) - 1/(x*(-1 + 1/x))
>>> signsimp(_)
0
>>> x*n + x*-n
x*(-1 + 1/x) + x*(1 - 1/x)
>>> signsimp(_)
0
Since powers automatically handle leading signs
>>> (-2)**i
-2**i
signsimp can be used to put the base of a power with an integer
exponent into canonical form:
>>> n**i
(-1 + 1/x)**i
By default, signsimp doesn't leave behind any hollow simplification:
if making an Add canonical wrt sign didn't change the expression, the
original Add is restored. If this is not desired then the keyword
``evaluate`` can be set to False:
>>> e = exp(y - x)
>>> signsimp(e) == e
True
>>> signsimp(e, evaluate=False)
exp(-(x - y))
"""
if evaluate is None:
evaluate = global_evaluate[0]
expr = sympify(expr)
if not isinstance(expr, Expr) or expr.is_Atom:
return expr
e = sub_post(sub_pre(expr))
if not isinstance(e, Expr) or e.is_Atom:
return e
if e.is_Add:
return e.func(*[signsimp(a, evaluate) for a in e.args])
if evaluate:
e = e.xreplace({m: -(-m) for m in e.atoms(Mul) if -(-m) != m})
return e
def simplify(expr, ratio=1.7, measure=count_ops, rational=False, inverse=False, doit=True, **kwargs):
"""Simplifies the given expression.
Simplification is not a well defined term and the exact strategies
this function tries can change in the future versions of SymPy. If
your algorithm relies on "simplification" (whatever it is), try to
determine what you need exactly - is it powsimp()?, radsimp()?,
together()?, logcombine()?, or something else? And use this particular
function directly, because those are well defined and thus your algorithm
will be robust.
Nonetheless, especially for interactive use, or when you don't know
anything about the structure of the expression, simplify() tries to apply
intelligent heuristics to make the input expression "simpler". For
example:
>>> from sympy import simplify, cos, sin
>>> from sympy.abc import x, y
>>> a = (x + x**2)/(x*sin(y)**2 + x*cos(y)**2)
>>> a
(x**2 + x)/(x*sin(y)**2 + x*cos(y)**2)
>>> simplify(a)
x + 1
Note that we could have obtained the same result by using specific
simplification functions:
>>> from sympy import trigsimp, cancel
>>> trigsimp(a)
(x**2 + x)/x
>>> cancel(_)
x + 1
In some cases, applying :func:`simplify` may actually result in some more
complicated expression. The default ``ratio=1.7`` prevents more extreme
cases: if (result length)/(input length) > ratio, then input is returned
unmodified. The ``measure`` parameter lets you specify the function used
to determine how complex an expression is. The function should take a
single argument as an expression and return a number such that if
expression ``a`` is more complex than expression ``b``, then
``measure(a) > measure(b)``. The default measure function is
:func:`count_ops`, which returns the total number of operations in the
expression.
For example, if ``ratio=1``, ``simplify`` output can't be longer
than input.
::
>>> from sympy import sqrt, simplify, count_ops, oo
>>> root = 1/(sqrt(2)+3)
Since ``simplify(root)`` would result in a slightly longer expression,
root is returned unchanged instead::
>>> simplify(root, ratio=1) == root
True
If ``ratio=oo``, simplify will be applied anyway::
>>> count_ops(simplify(root, ratio=oo)) > count_ops(root)
True
Note that the shortest expression is not necessary the simplest, so
setting ``ratio`` to 1 may not be a good idea.
Heuristically, the default value ``ratio=1.7`` seems like a reasonable
choice.
You can easily define your own measure function based on what you feel
should represent the "size" or "complexity" of the input expression. Note
that some choices, such as ``lambda expr: len(str(expr))`` may appear to be
good metrics, but have other problems (in this case, the measure function
may slow down simplify too much for very large expressions). If you don't
know what a good metric would be, the default, ``count_ops``, is a good
one.
For example:
>>> from sympy import symbols, log
>>> a, b = symbols('a b', positive=True)
>>> g = log(a) + log(b) + log(a)*log(1/b)
>>> h = simplify(g)
>>> h
log(a*b**(1 - log(a)))
>>> count_ops(g)
8
>>> count_ops(h)
5
So you can see that ``h`` is simpler than ``g`` using the count_ops metric.
However, we may not like how ``simplify`` (in this case, using
``logcombine``) has created the ``b**(log(1/a) + 1)`` term. A simple way
to reduce this would be to give more weight to powers as operations in
``count_ops``. We can do this by using the ``visual=True`` option:
>>> print(count_ops(g, visual=True))
2*ADD + DIV + 4*LOG + MUL
>>> print(count_ops(h, visual=True))
2*LOG + MUL + POW + SUB
>>> from sympy import Symbol, S
>>> def my_measure(expr):
... POW = Symbol('POW')
... # Discourage powers by giving POW a weight of 10
... count = count_ops(expr, visual=True).subs(POW, 10)
... # Every other operation gets a weight of 1 (the default)
... count = count.replace(Symbol, type(S.One))
... return count
>>> my_measure(g)
8
>>> my_measure(h)
14
>>> 15./8 > 1.7 # 1.7 is the default ratio
True
>>> simplify(g, measure=my_measure)
-log(a)*log(b) + log(a) + log(b)
Note that because ``simplify()`` internally tries many different
simplification strategies and then compares them using the measure
function, we get a completely different result that is still different
from the input expression by doing this.
If rational=True, Floats will be recast as Rationals before simplification.
If rational=None, Floats will be recast as Rationals but the result will
be recast as Floats. If rational=False(default) then nothing will be done
to the Floats.
If inverse=True, it will be assumed that a composition of inverse
functions, such as sin and asin, can be cancelled in any order.
For example, ``asin(sin(x))`` will yield ``x`` without checking whether
x belongs to the set where this relation is true. The default is
False.
Note that ``simplify()`` automatically calls ``doit()`` on the final
expression. You can avoid this behavior by passing ``doit=False`` as
an argument.
"""
def shorter(*choices):
"""
Return the choice that has the fewest ops. In case of a tie,
the expression listed first is selected.
"""
if not has_variety(choices):
return choices[0]
return min(choices, key=measure)
def done(e):
rv = e.doit() if doit else e
return shorter(rv, collect_abs(rv))
expr = sympify(expr)
kwargs = dict(
ratio=kwargs.get('ratio', ratio),
measure=kwargs.get('measure', measure),
rational=kwargs.get('rational', rational),
inverse=kwargs.get('inverse', inverse),
doit=kwargs.get('doit', doit))
# no routine for Expr needs to check for is_zero
if isinstance(expr, Expr) and expr.is_zero and expr*0 == S.Zero:
return S.Zero
_eval_simplify = getattr(expr, '_eval_simplify', None)
if _eval_simplify is not None:
return _eval_simplify(**kwargs)
original_expr = expr = collect_abs(signsimp(expr))
if not isinstance(expr, Basic) or not expr.args: # XXX: temporary hack
return expr
if inverse and expr.has(Function):
expr = inversecombine(expr)
if not expr.args: # simplified to atomic
return expr
# do deep simplification
handled = Add, Mul, Pow, ExpBase
expr = expr.replace(
# here, checking for x.args is not enough because Basic has
# args but Basic does not always play well with replace, e.g.
# when simultaneous is True found expressions will be masked
# off with a Dummy but not all Basic objects in an expression
# can be replaced with a Dummy
lambda x: isinstance(x, Expr) and x.args and not isinstance(
x, handled),
lambda x: x.func(*[simplify(i, **kwargs) for i in x.args]),
simultaneous=False)
if not isinstance(expr, handled):
return done(expr)
if not expr.is_commutative:
expr = nc_simplify(expr)
# TODO: Apply different strategies, considering expression pattern:
# is it a purely rational function? Is there any trigonometric function?...
# See also https://github.com/sympy/sympy/pull/185.
# rationalize Floats
floats = False
if rational is not False and expr.has(Float):
floats = True
expr = nsimplify(expr, rational=True)
expr = bottom_up(expr, lambda w: getattr(w, 'normal', lambda: w)())
expr = Mul(*powsimp(expr).as_content_primitive())
_e = cancel(expr)
expr1 = shorter(_e, _mexpand(_e).cancel()) # issue 6829
expr2 = shorter(together(expr, deep=True), together(expr1, deep=True))
if ratio is S.Infinity:
expr = expr2
else:
expr = shorter(expr2, expr1, expr)
if not isinstance(expr, Basic): # XXX: temporary hack
return expr
expr = factor_terms(expr, sign=False)
from sympy.simplify.hyperexpand import hyperexpand
from sympy.functions.special.bessel import BesselBase
from sympy import Sum, Product, Integral
# hyperexpand automatically only works on hypergeometric terms
expr = hyperexpand(expr)
# Deal with Piecewise separately to avoid recursive growth of expressions
if expr.has(Piecewise):
# Fold into a single Piecewise
expr = piecewise_fold(expr)
# Apply doit, if doit=True
expr = done(expr)
# Still a Piecewise?
if expr.has(Piecewise):
# Fold into a single Piecewise, in case doit lead to some
# expressions being Piecewise
expr = piecewise_fold(expr)
# kroneckersimp also affects Piecewise
if expr.has(KroneckerDelta):
expr = kroneckersimp(expr)
# Still a Piecewise?
if expr.has(Piecewise):
from sympy.functions.elementary.piecewise import piecewise_simplify
# Do not apply doit on the segments as it has already
# been done above, but simplify
expr = piecewise_simplify(expr, deep=True, doit=False)
# Still a Piecewise?
if expr.has(Piecewise):
# Try factor common terms
expr = shorter(expr, factor_terms(expr))
# As all expressions have been simplified above with the
# complete simplify, nothing more needs to be done here
return expr
if expr.has(KroneckerDelta):
expr = kroneckersimp(expr)
if expr.has(BesselBase):
expr = besselsimp(expr)
if expr.has(TrigonometricFunction, HyperbolicFunction):
expr = trigsimp(expr, deep=True)
if expr.has(log):
expr = shorter(expand_log(expr, deep=True), logcombine(expr))
if expr.has(CombinatorialFunction, gamma):
# expression with gamma functions or non-integer arguments is
# automatically passed to gammasimp
expr = combsimp(expr)
if expr.has(Sum):
expr = sum_simplify(expr, **kwargs)
if expr.has(Integral):
expr = expr.xreplace(dict([
(i, factor_terms(i)) for i in expr.atoms(Integral)]))
if expr.has(Product):
expr = product_simplify(expr)
from sympy.physics.units import Quantity
from sympy.physics.units.util import quantity_simplify
if expr.has(Quantity):
expr = quantity_simplify(expr)
short = shorter(powsimp(expr, combine='exp', deep=True), powsimp(expr), expr)
short = shorter(short, cancel(short))
short = shorter(short, factor_terms(short), expand_power_exp(expand_mul(short)))
if short.has(TrigonometricFunction, HyperbolicFunction, ExpBase):
short = exptrigsimp(short)
# get rid of hollow 2-arg Mul factorization
hollow_mul = Transform(
lambda x: Mul(*x.args),
lambda x:
x.is_Mul and
len(x.args) == 2 and
x.args[0].is_Number and
x.args[1].is_Add and
x.is_commutative)
expr = short.xreplace(hollow_mul)
numer, denom = expr.as_numer_denom()
if denom.is_Add:
n, d = fraction(radsimp(1/denom, symbolic=False, max_terms=1))
if n is not S.One:
expr = (numer*n).expand()/d
if expr.could_extract_minus_sign():
n, d = fraction(expr)
if d != 0:
expr = signsimp(-n/(-d))
if measure(expr) > ratio*measure(original_expr):
expr = original_expr
# restore floats
if floats and rational is None:
expr = nfloat(expr, exponent=False)
return done(expr)
def sum_simplify(s, **kwargs):
"""Main function for Sum simplification"""
from sympy.concrete.summations import Sum
from sympy.core.function import expand
if not isinstance(s, Add):
s = s.xreplace(dict([(a, sum_simplify(a, **kwargs))
for a in s.atoms(Add) if a.has(Sum)]))
s = expand(s)
if not isinstance(s, Add):
return s
terms = s.args
s_t = [] # Sum Terms
o_t = [] # Other Terms
for term in terms:
sum_terms, other = sift(Mul.make_args(term),
lambda i: isinstance(i, Sum), binary=True)
if not sum_terms:
o_t.append(term)
continue
other = [Mul(*other)]
s_t.append(Mul(*(other + [s._eval_simplify(**kwargs) for s in sum_terms])))
result = Add(sum_combine(s_t), *o_t)
return result
def sum_combine(s_t):
"""Helper function for Sum simplification
Attempts to simplify a list of sums, by combining limits / sum function's
returns the simplified sum
"""
from sympy.concrete.summations import Sum
used = [False] * len(s_t)
for method in range(2):
for i, s_term1 in enumerate(s_t):
if not used[i]:
for j, s_term2 in enumerate(s_t):
if not used[j] and i != j:
temp = sum_add(s_term1, s_term2, method)
if isinstance(temp, Sum) or isinstance(temp, Mul):
s_t[i] = temp
s_term1 = s_t[i]
used[j] = True
result = S.Zero
for i, s_term in enumerate(s_t):
if not used[i]:
result = Add(result, s_term)
return result
def factor_sum(self, limits=None, radical=False, clear=False, fraction=False, sign=True):
"""Return Sum with constant factors extracted.
If ``limits`` is specified then ``self`` is the summand; the other
keywords are passed to ``factor_terms``.
Examples
========
>>> from sympy import Sum, Integral
>>> from sympy.abc import x, y
>>> from sympy.simplify.simplify import factor_sum
>>> s = Sum(x*y, (x, 1, 3))
>>> factor_sum(s)
y*Sum(x, (x, 1, 3))
>>> factor_sum(s.function, s.limits)
y*Sum(x, (x, 1, 3))
"""
# XXX deprecate in favor of direct call to factor_terms
from sympy.concrete.summations import Sum
kwargs = dict(radical=radical, clear=clear,
fraction=fraction, sign=sign)
expr = Sum(self, *limits) if limits else self
return factor_terms(expr, **kwargs)
def sum_add(self, other, method=0):
"""Helper function for Sum simplification"""
from sympy.concrete.summations import Sum
from sympy import Mul
#we know this is something in terms of a constant * a sum
#so we temporarily put the constants inside for simplification
#then simplify the result
def __refactor(val):
args = Mul.make_args(val)
sumv = next(x for x in args if isinstance(x, Sum))
constant = Mul(*[x for x in args if x != sumv])
return Sum(constant * sumv.function, *sumv.limits)
if isinstance(self, Mul):
rself = __refactor(self)
else:
rself = self
if isinstance(other, Mul):
rother = __refactor(other)
else:
rother = other
if type(rself) == type(rother):
if method == 0:
if rself.limits == rother.limits:
return factor_sum(Sum(rself.function + rother.function, *rself.limits))
elif method == 1:
if simplify(rself.function - rother.function) == 0:
if len(rself.limits) == len(rother.limits) == 1:
i = rself.limits[0][0]
x1 = rself.limits[0][1]
y1 = rself.limits[0][2]
j = rother.limits[0][0]
x2 = rother.limits[0][1]
y2 = rother.limits[0][2]
if i == j:
if x2 == y1 + 1:
return factor_sum(Sum(rself.function, (i, x1, y2)))
elif x1 == y2 + 1:
return factor_sum(Sum(rself.function, (i, x2, y1)))
return Add(self, other)
def product_simplify(s):
"""Main function for Product simplification"""
from sympy.concrete.products import Product
terms = Mul.make_args(s)
p_t = [] # Product Terms
o_t = [] # Other Terms
for term in terms:
if isinstance(term, Product):
p_t.append(term)
else:
o_t.append(term)
used = [False] * len(p_t)
for method in range(2):
for i, p_term1 in enumerate(p_t):
if not used[i]:
for j, p_term2 in enumerate(p_t):
if not used[j] and i != j:
if isinstance(product_mul(p_term1, p_term2, method), Product):
p_t[i] = product_mul(p_term1, p_term2, method)
used[j] = True
result = Mul(*o_t)
for i, p_term in enumerate(p_t):
if not used[i]:
result = Mul(result, p_term)
return result
def product_mul(self, other, method=0):
"""Helper function for Product simplification"""
from sympy.concrete.products import Product
if type(self) == type(other):
if method == 0:
if self.limits == other.limits:
return Product(self.function * other.function, *self.limits)
elif method == 1:
if simplify(self.function - other.function) == 0:
if len(self.limits) == len(other.limits) == 1:
i = self.limits[0][0]
x1 = self.limits[0][1]
y1 = self.limits[0][2]
j = other.limits[0][0]
x2 = other.limits[0][1]
y2 = other.limits[0][2]
if i == j:
if x2 == y1 + 1:
return Product(self.function, (i, x1, y2))
elif x1 == y2 + 1:
return Product(self.function, (i, x2, y1))
return Mul(self, other)
def _nthroot_solve(p, n, prec):
"""
helper function for ``nthroot``
It denests ``p**Rational(1, n)`` using its minimal polynomial
"""
from sympy.polys.numberfields import _minimal_polynomial_sq
from sympy.solvers import solve
while n % 2 == 0:
p = sqrtdenest(sqrt(p))
n = n // 2
if n == 1:
return p
pn = p**Rational(1, n)
x = Symbol('x')
f = _minimal_polynomial_sq(p, n, x)
if f is None:
return None
sols = solve(f, x)
for sol in sols:
if abs(sol - pn).n() < 1./10**prec:
sol = sqrtdenest(sol)
if _mexpand(sol**n) == p:
return sol
def logcombine(expr, force=False):
"""
Takes logarithms and combines them using the following rules:
- log(x) + log(y) == log(x*y) if both are positive
- a*log(x) == log(x**a) if x is positive and a is real
If ``force`` is True then the assumptions above will be assumed to hold if
there is no assumption already in place on a quantity. For example, if
``a`` is imaginary or the argument negative, force will not perform a
combination but if ``a`` is a symbol with no assumptions the change will
take place.
Examples
========
>>> from sympy import Symbol, symbols, log, logcombine, I
>>> from sympy.abc import a, x, y, z
>>> logcombine(a*log(x) + log(y) - log(z))
a*log(x) + log(y) - log(z)
>>> logcombine(a*log(x) + log(y) - log(z), force=True)
log(x**a*y/z)
>>> x,y,z = symbols('x,y,z', positive=True)
>>> a = Symbol('a', real=True)
>>> logcombine(a*log(x) + log(y) - log(z))
log(x**a*y/z)
The transformation is limited to factors and/or terms that
contain logs, so the result depends on the initial state of
expansion:
>>> eq = (2 + 3*I)*log(x)
>>> logcombine(eq, force=True) == eq
True
>>> logcombine(eq.expand(), force=True)
log(x**2) + I*log(x**3)
See Also
========
posify: replace all symbols with symbols having positive assumptions
sympy.core.function.expand_log: expand the logarithms of products
and powers; the opposite of logcombine
"""
def f(rv):
if not (rv.is_Add or rv.is_Mul):
return rv
def gooda(a):
# bool to tell whether the leading ``a`` in ``a*log(x)``
# could appear as log(x**a)
return (a is not S.NegativeOne and # -1 *could* go, but we disallow
(a.is_extended_real or force and a.is_extended_real is not False))
def goodlog(l):
# bool to tell whether log ``l``'s argument can combine with others
a = l.args[0]
return a.is_positive or force and a.is_nonpositive is not False
other = []
logs = []
log1 = defaultdict(list)
for a in Add.make_args(rv):
if isinstance(a, log) and goodlog(a):
log1[()].append(([], a))
elif not a.is_Mul:
other.append(a)
else:
ot = []
co = []
lo = []
for ai in a.args:
if ai.is_Rational and ai < 0:
ot.append(S.NegativeOne)
co.append(-ai)
elif isinstance(ai, log) and goodlog(ai):
lo.append(ai)
elif gooda(ai):
co.append(ai)
else:
ot.append(ai)
if len(lo) > 1:
logs.append((ot, co, lo))
elif lo:
log1[tuple(ot)].append((co, lo[0]))
else:
other.append(a)
# if there is only one log in other, put it with the
# good logs
if len(other) == 1 and isinstance(other[0], log):
log1[()].append(([], other.pop()))
# if there is only one log at each coefficient and none have
# an exponent to place inside the log then there is nothing to do
if not logs and all(len(log1[k]) == 1 and log1[k][0] == [] for k in log1):
return rv
# collapse multi-logs as far as possible in a canonical way
# TODO: see if x*log(a)+x*log(a)*log(b) -> x*log(a)*(1+log(b))?
# -- in this case, it's unambiguous, but if it were were a log(c) in
# each term then it's arbitrary whether they are grouped by log(a) or
# by log(c). So for now, just leave this alone; it's probably better to
# let the user decide
for o, e, l in logs:
l = list(ordered(l))
e = log(l.pop(0).args[0]**Mul(*e))
while l:
li = l.pop(0)
e = log(li.args[0]**e)
c, l = Mul(*o), e
if isinstance(l, log): # it should be, but check to be sure
log1[(c,)].append(([], l))
else:
other.append(c*l)
# logs that have the same coefficient can multiply
for k in list(log1.keys()):
log1[Mul(*k)] = log(logcombine(Mul(*[
l.args[0]**Mul(*c) for c, l in log1.pop(k)]),
force=force), evaluate=False)
# logs that have oppositely signed coefficients can divide
for k in ordered(list(log1.keys())):
if not k in log1: # already popped as -k
continue
if -k in log1:
# figure out which has the minus sign; the one with
# more op counts should be the one
num, den = k, -k
if num.count_ops() > den.count_ops():
num, den = den, num
other.append(
num*log(log1.pop(num).args[0]/log1.pop(den).args[0],
evaluate=False))
else:
other.append(k*log1.pop(k))
return Add(*other)
return bottom_up(expr, f)
def inversecombine(expr):
"""Simplify the composition of a function and its inverse.
No attention is paid to whether the inverse is a left inverse or a
right inverse; thus, the result will in general not be equivalent
to the original expression.
Examples
========
>>> from sympy.simplify.simplify import inversecombine
>>> from sympy import asin, sin, log, exp
>>> from sympy.abc import x
>>> inversecombine(asin(sin(x)))
x
>>> inversecombine(2*log(exp(3*x)))
6*x
"""
def f(rv):
if rv.is_Function and hasattr(rv, "inverse"):
if (len(rv.args) == 1 and len(rv.args[0].args) == 1 and
isinstance(rv.args[0], rv.inverse(argindex=1))):
rv = rv.args[0].args[0]
return rv
return bottom_up(expr, f)
def walk(e, *target):
"""iterate through the args that are the given types (target) and
return a list of the args that were traversed; arguments
that are not of the specified types are not traversed.
Examples
========
>>> from sympy.simplify.simplify import walk
>>> from sympy import Min, Max
>>> from sympy.abc import x, y, z
>>> list(walk(Min(x, Max(y, Min(1, z))), Min))
[Min(x, Max(y, Min(1, z)))]
>>> list(walk(Min(x, Max(y, Min(1, z))), Min, Max))
[Min(x, Max(y, Min(1, z))), Max(y, Min(1, z)), Min(1, z)]
See Also
========
bottom_up
"""
if isinstance(e, target):
yield e
for i in e.args:
for w in walk(i, *target):
yield w
def bottom_up(rv, F, atoms=False, nonbasic=False):
"""Apply ``F`` to all expressions in an expression tree from the
bottom up. If ``atoms`` is True, apply ``F`` even if there are no args;
if ``nonbasic`` is True, try to apply ``F`` to non-Basic objects.
"""
args = getattr(rv, 'args', None)
if args is not None:
if args:
args = tuple([bottom_up(a, F, atoms, nonbasic) for a in args])
if args != rv.args:
rv = rv.func(*args)
rv = F(rv)
elif atoms:
rv = F(rv)
else:
if nonbasic:
try:
rv = F(rv)
except TypeError:
pass
return rv
def kroneckersimp(expr):
"""
Simplify expressions with KroneckerDelta.
The only simplification currently attempted is to identify multiplicative cancellation:
>>> from sympy import KroneckerDelta, kroneckersimp
>>> from sympy.abc import i, j
>>> kroneckersimp(1 + KroneckerDelta(0, j) * KroneckerDelta(1, j))
1
"""
def args_cancel(args1, args2):
for i1 in range(2):
for i2 in range(2):
a1 = args1[i1]
a2 = args2[i2]
a3 = args1[(i1 + 1) % 2]
a4 = args2[(i2 + 1) % 2]
if Eq(a1, a2) is S.true and Eq(a3, a4) is S.false:
return True
return False
def cancel_kronecker_mul(m):
from sympy.utilities.iterables import subsets
args = m.args
deltas = [a for a in args if isinstance(a, KroneckerDelta)]
for delta1, delta2 in subsets(deltas, 2):
args1 = delta1.args
args2 = delta2.args
if args_cancel(args1, args2):
return 0*m
return m
if not expr.has(KroneckerDelta):
return expr
if expr.has(Piecewise):
expr = expr.rewrite(KroneckerDelta)
newexpr = expr
expr = None
while newexpr != expr:
expr = newexpr
newexpr = expr.replace(lambda e: isinstance(e, Mul), cancel_kronecker_mul)
return expr
def besselsimp(expr):
"""
Simplify bessel-type functions.
This routine tries to simplify bessel-type functions. Currently it only
works on the Bessel J and I functions, however. It works by looking at all
such functions in turn, and eliminating factors of "I" and "-1" (actually
their polar equivalents) in front of the argument. Then, functions of
half-integer order are rewritten using strigonometric functions and
functions of integer order (> 1) are rewritten using functions
of low order. Finally, if the expression was changed, compute
factorization of the result with factor().
>>> from sympy import besselj, besseli, besselsimp, polar_lift, I, S
>>> from sympy.abc import z, nu
>>> besselsimp(besselj(nu, z*polar_lift(-1)))
exp(I*pi*nu)*besselj(nu, z)
>>> besselsimp(besseli(nu, z*polar_lift(-I)))
exp(-I*pi*nu/2)*besselj(nu, z)
>>> besselsimp(besseli(S(-1)/2, z))
sqrt(2)*cosh(z)/(sqrt(pi)*sqrt(z))
>>> besselsimp(z*besseli(0, z) + z*(besseli(2, z))/2 + besseli(1, z))
3*z*besseli(0, z)/2
"""
# TODO
# - better algorithm?
# - simplify (cos(pi*b)*besselj(b,z) - besselj(-b,z))/sin(pi*b) ...
# - use contiguity relations?
def replacer(fro, to, factors):
factors = set(factors)
def repl(nu, z):
if factors.intersection(Mul.make_args(z)):
return to(nu, z)
return fro(nu, z)
return repl
def torewrite(fro, to):
def tofunc(nu, z):
return fro(nu, z).rewrite(to)
return tofunc
def tominus(fro):
def tofunc(nu, z):
return exp(I*pi*nu)*fro(nu, exp_polar(-I*pi)*z)
return tofunc
orig_expr = expr
ifactors = [I, exp_polar(I*pi/2), exp_polar(-I*pi/2)]
expr = expr.replace(
besselj, replacer(besselj,
torewrite(besselj, besseli), ifactors))
expr = expr.replace(
besseli, replacer(besseli,
torewrite(besseli, besselj), ifactors))
minusfactors = [-1, exp_polar(I*pi)]
expr = expr.replace(
besselj, replacer(besselj, tominus(besselj), minusfactors))
expr = expr.replace(
besseli, replacer(besseli, tominus(besseli), minusfactors))
z0 = Dummy('z')
def expander(fro):
def repl(nu, z):
if (nu % 1) == S.Half:
return simplify(trigsimp(unpolarify(
fro(nu, z0).rewrite(besselj).rewrite(jn).expand(
func=True)).subs(z0, z)))
elif nu.is_Integer and nu > 1:
return fro(nu, z).expand(func=True)
return fro(nu, z)
return repl
expr = expr.replace(besselj, expander(besselj))
expr = expr.replace(bessely, expander(bessely))
expr = expr.replace(besseli, expander(besseli))
expr = expr.replace(besselk, expander(besselk))
def _bessel_simp_recursion(expr):
def _use_recursion(bessel, expr):
while True:
bessels = expr.find(lambda x: isinstance(x, bessel))
try:
for ba in sorted(bessels, key=lambda x: re(x.args[0])):
a, x = ba.args
bap1 = bessel(a+1, x)
bap2 = bessel(a+2, x)
if expr.has(bap1) and expr.has(bap2):
expr = expr.subs(ba, 2*(a+1)/x*bap1 - bap2)
break
else:
return expr
except (ValueError, TypeError):
return expr
if expr.has(besselj):
expr = _use_recursion(besselj, expr)
if expr.has(bessely):
expr = _use_recursion(bessely, expr)
return expr
expr = _bessel_simp_recursion(expr)
if expr != orig_expr:
expr = expr.factor()
return expr
def nthroot(expr, n, max_len=4, prec=15):
"""
compute a real nth-root of a sum of surds
Parameters
==========
expr : sum of surds
n : integer
max_len : maximum number of surds passed as constants to ``nsimplify``
Algorithm
=========
First ``nsimplify`` is used to get a candidate root; if it is not a
root the minimal polynomial is computed; the answer is one of its
roots.
Examples
========
>>> from sympy.simplify.simplify import nthroot
>>> from sympy import Rational, sqrt
>>> nthroot(90 + 34*sqrt(7), 3)
sqrt(7) + 3
"""
expr = sympify(expr)
n = sympify(n)
p = expr**Rational(1, n)
if not n.is_integer:
return p
if not _is_sum_surds(expr):
return p
surds = []
coeff_muls = [x.as_coeff_Mul() for x in expr.args]
for x, y in coeff_muls:
if not x.is_rational:
return p
if y is S.One:
continue
if not (y.is_Pow and y.exp == S.Half and y.base.is_integer):
return p
surds.append(y)
surds.sort()
surds = surds[:max_len]
if expr < 0 and n % 2 == 1:
p = (-expr)**Rational(1, n)
a = nsimplify(p, constants=surds)
res = a if _mexpand(a**n) == _mexpand(-expr) else p
return -res
a = nsimplify(p, constants=surds)
if _mexpand(a) is not _mexpand(p) and _mexpand(a**n) == _mexpand(expr):
return _mexpand(a)
expr = _nthroot_solve(expr, n, prec)
if expr is None:
return p
return expr
def nsimplify(expr, constants=(), tolerance=None, full=False, rational=None,
rational_conversion='base10'):
"""
Find a simple representation for a number or, if there are free symbols or
if rational=True, then replace Floats with their Rational equivalents. If
no change is made and rational is not False then Floats will at least be
converted to Rationals.
For numerical expressions, a simple formula that numerically matches the
given numerical expression is sought (and the input should be possible
to evalf to a precision of at least 30 digits).
Optionally, a list of (rationally independent) constants to
include in the formula may be given.
A lower tolerance may be set to find less exact matches. If no tolerance
is given then the least precise value will set the tolerance (e.g. Floats
default to 15 digits of precision, so would be tolerance=10**-15).
With full=True, a more extensive search is performed
(this is useful to find simpler numbers when the tolerance
is set low).
When converting to rational, if rational_conversion='base10' (the default), then
convert floats to rationals using their base-10 (string) representation.
When rational_conversion='exact' it uses the exact, base-2 representation.
Examples
========
>>> from sympy import nsimplify, sqrt, GoldenRatio, exp, I, exp, pi
>>> nsimplify(4/(1+sqrt(5)), [GoldenRatio])
-2 + 2*GoldenRatio
>>> nsimplify((1/(exp(3*pi*I/5)+1)))
1/2 - I*sqrt(sqrt(5)/10 + 1/4)
>>> nsimplify(I**I, [pi])
exp(-pi/2)
>>> nsimplify(pi, tolerance=0.01)
22/7
>>> nsimplify(0.333333333333333, rational=True, rational_conversion='exact')
6004799503160655/18014398509481984
>>> nsimplify(0.333333333333333, rational=True)
1/3
See Also
========
sympy.core.function.nfloat
"""
try:
return sympify(as_int(expr))
except (TypeError, ValueError):
pass
expr = sympify(expr).xreplace({
Float('inf'): S.Infinity,
Float('-inf'): S.NegativeInfinity,
})
if expr is S.Infinity or expr is S.NegativeInfinity:
return expr
if rational or expr.free_symbols:
return _real_to_rational(expr, tolerance, rational_conversion)
# SymPy's default tolerance for Rationals is 15; other numbers may have
# lower tolerances set, so use them to pick the largest tolerance if None
# was given
if tolerance is None:
tolerance = 10**-min([15] +
[mpmath.libmp.libmpf.prec_to_dps(n._prec)
for n in expr.atoms(Float)])
# XXX should prec be set independent of tolerance or should it be computed
# from tolerance?
prec = 30
bprec = int(prec*3.33)
constants_dict = {}
for constant in constants:
constant = sympify(constant)
v = constant.evalf(prec)
if not v.is_Float:
raise ValueError("constants must be real-valued")
constants_dict[str(constant)] = v._to_mpmath(bprec)
exprval = expr.evalf(prec, chop=True)
re, im = exprval.as_real_imag()
# safety check to make sure that this evaluated to a number
if not (re.is_Number and im.is_Number):
return expr
def nsimplify_real(x):
orig = mpmath.mp.dps
xv = x._to_mpmath(bprec)
try:
# We'll be happy with low precision if a simple fraction
if not (tolerance or full):
mpmath.mp.dps = 15
rat = mpmath.pslq([xv, 1])
if rat is not None:
return Rational(-int(rat[1]), int(rat[0]))
mpmath.mp.dps = prec
newexpr = mpmath.identify(xv, constants=constants_dict,
tol=tolerance, full=full)
if not newexpr:
raise ValueError
if full:
newexpr = newexpr[0]
expr = sympify(newexpr)
if x and not expr: # don't let x become 0
raise ValueError
if expr.is_finite is False and not xv in [mpmath.inf, mpmath.ninf]:
raise ValueError
return expr
finally:
# even though there are returns above, this is executed
# before leaving
mpmath.mp.dps = orig
try:
if re:
re = nsimplify_real(re)
if im:
im = nsimplify_real(im)
except ValueError:
if rational is None:
return _real_to_rational(expr, rational_conversion=rational_conversion)
return expr
rv = re + im*S.ImaginaryUnit
# if there was a change or rational is explicitly not wanted
# return the value, else return the Rational representation
if rv != expr or rational is False:
return rv
return _real_to_rational(expr, rational_conversion=rational_conversion)
def _real_to_rational(expr, tolerance=None, rational_conversion='base10'):
"""
Replace all reals in expr with rationals.
Examples
========
>>> from sympy import Rational
>>> from sympy.simplify.simplify import _real_to_rational
>>> from sympy.abc import x
>>> _real_to_rational(.76 + .1*x**.5)
sqrt(x)/10 + 19/25
If rational_conversion='base10', this uses the base-10 string. If
rational_conversion='exact', the exact, base-2 representation is used.
>>> _real_to_rational(0.333333333333333, rational_conversion='exact')
6004799503160655/18014398509481984
>>> _real_to_rational(0.333333333333333)
1/3
"""
expr = _sympify(expr)
inf = Float('inf')
p = expr
reps = {}
reduce_num = None
if tolerance is not None and tolerance < 1:
reduce_num = ceiling(1/tolerance)
for fl in p.atoms(Float):
key = fl
if reduce_num is not None:
r = Rational(fl).limit_denominator(reduce_num)
elif (tolerance is not None and tolerance >= 1 and
fl.is_Integer is False):
r = Rational(tolerance*round(fl/tolerance)
).limit_denominator(int(tolerance))
else:
if rational_conversion == 'exact':
r = Rational(fl)
reps[key] = r
continue
elif rational_conversion != 'base10':
raise ValueError("rational_conversion must be 'base10' or 'exact'")
r = nsimplify(fl, rational=False)
# e.g. log(3).n() -> log(3) instead of a Rational
if fl and not r:
r = Rational(fl)
elif not r.is_Rational:
if fl == inf or fl == -inf:
r = S.ComplexInfinity
elif fl < 0:
fl = -fl
d = Pow(10, int((mpmath.log(fl)/mpmath.log(10))))
r = -Rational(str(fl/d))*d
elif fl > 0:
d = Pow(10, int((mpmath.log(fl)/mpmath.log(10))))
r = Rational(str(fl/d))*d
else:
r = Integer(0)
reps[key] = r
return p.subs(reps, simultaneous=True)
def clear_coefficients(expr, rhs=S.Zero):
"""Return `p, r` where `p` is the expression obtained when Rational
additive and multiplicative coefficients of `expr` have been stripped
away in a naive fashion (i.e. without simplification). The operations
needed to remove the coefficients will be applied to `rhs` and returned
as `r`.
Examples
========
>>> from sympy.simplify.simplify import clear_coefficients
>>> from sympy.abc import x, y
>>> from sympy import Dummy
>>> expr = 4*y*(6*x + 3)
>>> clear_coefficients(expr - 2)
(y*(2*x + 1), 1/6)
When solving 2 or more expressions like `expr = a`,
`expr = b`, etc..., it is advantageous to provide a Dummy symbol
for `rhs` and simply replace it with `a`, `b`, etc... in `r`.
>>> rhs = Dummy('rhs')
>>> clear_coefficients(expr, rhs)
(y*(2*x + 1), _rhs/12)
>>> _[1].subs(rhs, 2)
1/6
"""
was = None
free = expr.free_symbols
if expr.is_Rational:
return (S.Zero, rhs - expr)
while expr and was != expr:
was = expr
m, expr = (
expr.as_content_primitive()
if free else
factor_terms(expr).as_coeff_Mul(rational=True))
rhs /= m
c, expr = expr.as_coeff_Add(rational=True)
rhs -= c
expr = signsimp(expr, evaluate = False)
if _coeff_isneg(expr):
expr = -expr
rhs = -rhs
return expr, rhs
def nc_simplify(expr, deep=True):
'''
Simplify a non-commutative expression composed of multiplication
and raising to a power by grouping repeated subterms into one power.
Priority is given to simplifications that give the fewest number
of arguments in the end (for example, in a*b*a*b*c*a*b*c simplifying
to (a*b)**2*c*a*b*c gives 5 arguments while a*b*(a*b*c)**2 has 3).
If `expr` is a sum of such terms, the sum of the simplified terms
is returned.
Keyword argument `deep` controls whether or not subexpressions
nested deeper inside the main expression are simplified. See examples
below. Setting `deep` to `False` can save time on nested expressions
that don't need simplifying on all levels.
Examples
========
>>> from sympy import symbols
>>> from sympy.simplify.simplify import nc_simplify
>>> a, b, c = symbols("a b c", commutative=False)
>>> nc_simplify(a*b*a*b*c*a*b*c)
a*b*(a*b*c)**2
>>> expr = a**2*b*a**4*b*a**4
>>> nc_simplify(expr)
a**2*(b*a**4)**2
>>> nc_simplify(a*b*a*b*c**2*(a*b)**2*c**2)
((a*b)**2*c**2)**2
>>> nc_simplify(a*b*a*b + 2*a*c*a**2*c*a**2*c*a)
(a*b)**2 + 2*(a*c*a)**3
>>> nc_simplify(b**-1*a**-1*(a*b)**2)
a*b
>>> nc_simplify(a**-1*b**-1*c*a)
(b*a)**(-1)*c*a
>>> expr = (a*b*a*b)**2*a*c*a*c
>>> nc_simplify(expr)
(a*b)**4*(a*c)**2
>>> nc_simplify(expr, deep=False)
(a*b*a*b)**2*(a*c)**2
'''
from sympy.matrices.expressions import (MatrixExpr, MatAdd, MatMul,
MatPow, MatrixSymbol)
from sympy.core.exprtools import factor_nc
if isinstance(expr, MatrixExpr):
expr = expr.doit(inv_expand=False)
_Add, _Mul, _Pow, _Symbol = MatAdd, MatMul, MatPow, MatrixSymbol
else:
_Add, _Mul, _Pow, _Symbol = Add, Mul, Pow, Symbol
# =========== Auxiliary functions ========================
def _overlaps(args):
# Calculate a list of lists m such that m[i][j] contains the lengths
# of all possible overlaps between args[:i+1] and args[i+1+j:].
# An overlap is a suffix of the prefix that matches a prefix
# of the suffix.
# For example, let expr=c*a*b*a*b*a*b*a*b. Then m[3][0] contains
# the lengths of overlaps of c*a*b*a*b with a*b*a*b. The overlaps
# are a*b*a*b, a*b and the empty word so that m[3][0]=[4,2,0].
# All overlaps rather than only the longest one are recorded
# because this information helps calculate other overlap lengths.
m = [[([1, 0] if a == args[0] else [0]) for a in args[1:]]]
for i in range(1, len(args)):
overlaps = []
j = 0
for j in range(len(args) - i - 1):
overlap = []
for v in m[i-1][j+1]:
if j + i + 1 + v < len(args) and args[i] == args[j+i+1+v]:
overlap.append(v + 1)
overlap += [0]
overlaps.append(overlap)
m.append(overlaps)
return m
def _reduce_inverses(_args):
# replace consecutive negative powers by an inverse
# of a product of positive powers, e.g. a**-1*b**-1*c
# will simplify to (a*b)**-1*c;
# return that new args list and the number of negative
# powers in it (inv_tot)
inv_tot = 0 # total number of inverses
inverses = []
args = []
for arg in _args:
if isinstance(arg, _Pow) and arg.args[1] < 0:
inverses = [arg**-1] + inverses
inv_tot += 1
else:
if len(inverses) == 1:
args.append(inverses[0]**-1)
elif len(inverses) > 1:
args.append(_Pow(_Mul(*inverses), -1))
inv_tot -= len(inverses) - 1
inverses = []
args.append(arg)
if inverses:
args.append(_Pow(_Mul(*inverses), -1))
inv_tot -= len(inverses) - 1
return inv_tot, tuple(args)
def get_score(s):
# compute the number of arguments of s
# (including in nested expressions) overall
# but ignore exponents
if isinstance(s, _Pow):
return get_score(s.args[0])
elif isinstance(s, (_Add, _Mul)):
return sum([get_score(a) for a in s.args])
return 1
def compare(s, alt_s):
# compare two possible simplifications and return a
# "better" one
if s != alt_s and get_score(alt_s) < get_score(s):
return alt_s
return s
# ========================================================
if not isinstance(expr, (_Add, _Mul, _Pow)) or expr.is_commutative:
return expr
args = expr.args[:]
if isinstance(expr, _Pow):
if deep:
return _Pow(nc_simplify(args[0]), args[1]).doit()
else:
return expr
elif isinstance(expr, _Add):
return _Add(*[nc_simplify(a, deep=deep) for a in args]).doit()
else:
# get the non-commutative part
c_args, args = expr.args_cnc()
com_coeff = Mul(*c_args)
if com_coeff != 1:
return com_coeff*nc_simplify(expr/com_coeff, deep=deep)
inv_tot, args = _reduce_inverses(args)
# if most arguments are negative, work with the inverse
# of the expression, e.g. a**-1*b*a**-1*c**-1 will become
# (c*a*b**-1*a)**-1 at the end so can work with c*a*b**-1*a
invert = False
if inv_tot > len(args)/2:
invert = True
args = [a**-1 for a in args[::-1]]
if deep:
args = tuple(nc_simplify(a) for a in args)
m = _overlaps(args)
# simps will be {subterm: end} where `end` is the ending
# index of a sequence of repetitions of subterm;
# this is for not wasting time with subterms that are part
# of longer, already considered sequences
simps = {}
post = 1
pre = 1
# the simplification coefficient is the number of
# arguments by which contracting a given sequence
# would reduce the word; e.g. in a*b*a*b*c*a*b*c,
# contracting a*b*a*b to (a*b)**2 removes 3 arguments
# while a*b*c*a*b*c to (a*b*c)**2 removes 6. It's
# better to contract the latter so simplification
# with a maximum simplification coefficient will be chosen
max_simp_coeff = 0
simp = None # information about future simplification
for i in range(1, len(args)):
simp_coeff = 0
l = 0 # length of a subterm
p = 0 # the power of a subterm
if i < len(args) - 1:
rep = m[i][0]
start = i # starting index of the repeated sequence
end = i+1 # ending index of the repeated sequence
if i == len(args)-1 or rep == [0]:
# no subterm is repeated at this stage, at least as
# far as the arguments are concerned - there may be
# a repetition if powers are taken into account
if (isinstance(args[i], _Pow) and
not isinstance(args[i].args[0], _Symbol)):
subterm = args[i].args[0].args
l = len(subterm)
if args[i-l:i] == subterm:
# e.g. a*b in a*b*(a*b)**2 is not repeated
# in args (= [a, b, (a*b)**2]) but it
# can be matched here
p += 1
start -= l
if args[i+1:i+1+l] == subterm:
# e.g. a*b in (a*b)**2*a*b
p += 1
end += l
if p:
p += args[i].args[1]
else:
continue
else:
l = rep[0] # length of the longest repeated subterm at this point
start -= l - 1
subterm = args[start:end]
p = 2
end += l
if subterm in simps and simps[subterm] >= start:
# the subterm is part of a sequence that
# has already been considered
continue
# count how many times it's repeated
while end < len(args):
if l in m[end-1][0]:
p += 1
end += l
elif isinstance(args[end], _Pow) and args[end].args[0].args == subterm:
# for cases like a*b*a*b*(a*b)**2*a*b
p += args[end].args[1]
end += 1
else:
break
# see if another match can be made, e.g.
# for b*a**2 in b*a**2*b*a**3 or a*b in
# a**2*b*a*b
pre_exp = 0
pre_arg = 1
if start - l >= 0 and args[start-l+1:start] == subterm[1:]:
if isinstance(subterm[0], _Pow):
pre_arg = subterm[0].args[0]
exp = subterm[0].args[1]
else:
pre_arg = subterm[0]
exp = 1
if isinstance(args[start-l], _Pow) and args[start-l].args[0] == pre_arg:
pre_exp = args[start-l].args[1] - exp
start -= l
p += 1
elif args[start-l] == pre_arg:
pre_exp = 1 - exp
start -= l
p += 1
post_exp = 0
post_arg = 1
if end + l - 1 < len(args) and args[end:end+l-1] == subterm[:-1]:
if isinstance(subterm[-1], _Pow):
post_arg = subterm[-1].args[0]
exp = subterm[-1].args[1]
else:
post_arg = subterm[-1]
exp = 1
if isinstance(args[end+l-1], _Pow) and args[end+l-1].args[0] == post_arg:
post_exp = args[end+l-1].args[1] - exp
end += l
p += 1
elif args[end+l-1] == post_arg:
post_exp = 1 - exp
end += l
p += 1
# Consider a*b*a**2*b*a**2*b*a:
# b*a**2 is explicitly repeated, but note
# that in this case a*b*a is also repeated
# so there are two possible simplifications:
# a*(b*a**2)**3*a**-1 or (a*b*a)**3
# The latter is obviously simpler.
# But in a*b*a**2*b**2*a**2 the simplifications are
# a*(b*a**2)**2 and (a*b*a)**3*a in which case
# it's better to stick with the shorter subterm
if post_exp and exp % 2 == 0 and start > 0:
exp = exp/2
_pre_exp = 1
_post_exp = 1
if isinstance(args[start-1], _Pow) and args[start-1].args[0] == post_arg:
_post_exp = post_exp + exp
_pre_exp = args[start-1].args[1] - exp
elif args[start-1] == post_arg:
_post_exp = post_exp + exp
_pre_exp = 1 - exp
if _pre_exp == 0 or _post_exp == 0:
if not pre_exp:
start -= 1
post_exp = _post_exp
pre_exp = _pre_exp
pre_arg = post_arg
subterm = (post_arg**exp,) + subterm[:-1] + (post_arg**exp,)
simp_coeff += end-start
if post_exp:
simp_coeff -= 1
if pre_exp:
simp_coeff -= 1
simps[subterm] = end
if simp_coeff > max_simp_coeff:
max_simp_coeff = simp_coeff
simp = (start, _Mul(*subterm), p, end, l)
pre = pre_arg**pre_exp
post = post_arg**post_exp
if simp:
subterm = _Pow(nc_simplify(simp[1], deep=deep), simp[2])
pre = nc_simplify(_Mul(*args[:simp[0]])*pre, deep=deep)
post = post*nc_simplify(_Mul(*args[simp[3]:]), deep=deep)
simp = pre*subterm*post
if pre != 1 or post != 1:
# new simplifications may be possible but no need
# to recurse over arguments
simp = nc_simplify(simp, deep=False)
else:
simp = _Mul(*args)
if invert:
simp = _Pow(simp, -1)
# see if factor_nc(expr) is simplified better
if not isinstance(expr, MatrixExpr):
f_expr = factor_nc(expr)
if f_expr != expr:
alt_simp = nc_simplify(f_expr, deep=deep)
simp = compare(simp, alt_simp)
else:
simp = simp.doit(inv_expand=False)
return simp
|
fada39bb540345992528dcda3a3e3ce80fd36ffa05a576c449cbfe110520233a | from __future__ import print_function, division
from sympy.core import Function, S, Mul, Pow, Add
from sympy.core.compatibility import ordered, default_sort_key
from sympy.core.function import count_ops, expand_func
from sympy.functions.combinatorial.factorials import binomial
from sympy.functions import gamma, sqrt, sin
from sympy.polys import factor, cancel
from sympy.utilities.iterables import sift, uniq
def gammasimp(expr):
r"""
Simplify expressions with gamma functions.
This function takes as input an expression containing gamma
functions or functions that can be rewritten in terms of gamma
functions and tries to minimize the number of those functions and
reduce the size of their arguments.
The algorithm works by rewriting all gamma functions as expressions
involving rising factorials (Pochhammer symbols) and applies
recurrence relations and other transformations applicable to rising
factorials, to reduce their arguments, possibly letting the resulting
rising factorial to cancel. Rising factorials with the second argument
being an integer are expanded into polynomial forms and finally all
other rising factorial are rewritten in terms of gamma functions.
Then the following two steps are performed.
1. Reduce the number of gammas by applying the reflection theorem
gamma(x)*gamma(1-x) == pi/sin(pi*x).
2. Reduce the number of gammas by applying the multiplication theorem
gamma(x)*gamma(x+1/n)*...*gamma(x+(n-1)/n) == C*gamma(n*x).
It then reduces the number of prefactors by absorbing them into gammas
where possible and expands gammas with rational argument.
All transformation rules can be found (or was derived from) here:
1. http://functions.wolfram.com/GammaBetaErf/Pochhammer/17/01/02/
2. http://functions.wolfram.com/GammaBetaErf/Pochhammer/27/01/0005/
Examples
========
>>> from sympy.simplify import gammasimp
>>> from sympy import gamma, factorial, Symbol
>>> from sympy.abc import x
>>> n = Symbol('n', integer = True)
>>> gammasimp(gamma(x)/gamma(x - 3))
(x - 3)*(x - 2)*(x - 1)
>>> gammasimp(gamma(n + 3))
gamma(n + 3)
"""
expr = expr.rewrite(gamma)
return _gammasimp(expr, as_comb = False)
def _gammasimp(expr, as_comb):
"""
Helper function for gammasimp and combsimp.
Simplifies expressions written in terms of gamma function. If
as_comb is True, it tries to preserve integer arguments. See
docstring of gammasimp for more information. This was part of
combsimp() in combsimp.py.
"""
expr = expr.replace(gamma,
lambda n: _rf(1, (n - 1).expand()))
if as_comb:
expr = expr.replace(_rf,
lambda a, b: gamma(b + 1))
else:
expr = expr.replace(_rf,
lambda a, b: gamma(a + b)/gamma(a))
def rule(n, k):
coeff, rewrite = S.One, False
cn, _n = n.as_coeff_Add()
if _n and cn.is_Integer and cn:
coeff *= _rf(_n + 1, cn)/_rf(_n - k + 1, cn)
rewrite = True
n = _n
# this sort of binomial has already been removed by
# rising factorials but is left here in case the order
# of rule application is changed
if k.is_Add:
ck, _k = k.as_coeff_Add()
if _k and ck.is_Integer and ck:
coeff *= _rf(n - ck - _k + 1, ck)/_rf(_k + 1, ck)
rewrite = True
k = _k
if count_ops(k) > count_ops(n - k):
rewrite = True
k = n - k
if rewrite:
return coeff*binomial(n, k)
expr = expr.replace(binomial, rule)
def rule_gamma(expr, level=0):
""" Simplify products of gamma functions further. """
if expr.is_Atom:
return expr
def gamma_rat(x):
# helper to simplify ratios of gammas
was = x.count(gamma)
xx = x.replace(gamma, lambda n: _rf(1, (n - 1).expand()
).replace(_rf, lambda a, b: gamma(a + b)/gamma(a)))
if xx.count(gamma) < was:
x = xx
return x
def gamma_factor(x):
# return True if there is a gamma factor in shallow args
if isinstance(x, gamma):
return True
if x.is_Add or x.is_Mul:
return any(gamma_factor(xi) for xi in x.args)
if x.is_Pow and (x.exp.is_integer or x.base.is_positive):
return gamma_factor(x.base)
return False
# recursion step
if level == 0:
expr = expr.func(*[rule_gamma(x, level + 1) for x in expr.args])
level += 1
if not expr.is_Mul:
return expr
# non-commutative step
if level == 1:
args, nc = expr.args_cnc()
if not args:
return expr
if nc:
return rule_gamma(Mul._from_args(args), level + 1)*Mul._from_args(nc)
level += 1
# pure gamma handling, not factor absorption
if level == 2:
T, F = sift(expr.args, gamma_factor, binary=True)
gamma_ind = Mul(*F)
d = Mul(*T)
nd, dd = d.as_numer_denom()
for ipass in range(2):
args = list(ordered(Mul.make_args(nd)))
for i, ni in enumerate(args):
if ni.is_Add:
ni, dd = Add(*[
rule_gamma(gamma_rat(a/dd), level + 1) for a in ni.args]
).as_numer_denom()
args[i] = ni
if not dd.has(gamma):
break
nd = Mul(*args)
if ipass == 0 and not gamma_factor(nd):
break
nd, dd = dd, nd # now process in reversed order
expr = gamma_ind*nd/dd
if not (expr.is_Mul and (gamma_factor(dd) or gamma_factor(nd))):
return expr
level += 1
# iteration until constant
if level == 3:
while True:
was = expr
expr = rule_gamma(expr, 4)
if expr == was:
return expr
numer_gammas = []
denom_gammas = []
numer_others = []
denom_others = []
def explicate(p):
if p is S.One:
return None, []
b, e = p.as_base_exp()
if e.is_Integer:
if isinstance(b, gamma):
return True, [b.args[0]]*e
else:
return False, [b]*e
else:
return False, [p]
newargs = list(ordered(expr.args))
while newargs:
n, d = newargs.pop().as_numer_denom()
isg, l = explicate(n)
if isg:
numer_gammas.extend(l)
elif isg is False:
numer_others.extend(l)
isg, l = explicate(d)
if isg:
denom_gammas.extend(l)
elif isg is False:
denom_others.extend(l)
# =========== level 2 work: pure gamma manipulation =========
if not as_comb:
# Try to reduce the number of gamma factors by applying the
# reflection formula gamma(x)*gamma(1-x) = pi/sin(pi*x)
for gammas, numer, denom in [(
numer_gammas, numer_others, denom_others),
(denom_gammas, denom_others, numer_others)]:
new = []
while gammas:
g1 = gammas.pop()
if g1.is_integer:
new.append(g1)
continue
for i, g2 in enumerate(gammas):
n = g1 + g2 - 1
if not n.is_Integer:
continue
numer.append(S.Pi)
denom.append(sin(S.Pi*g1))
gammas.pop(i)
if n > 0:
for k in range(n):
numer.append(1 - g1 + k)
elif n < 0:
for k in range(-n):
denom.append(-g1 - k)
break
else:
new.append(g1)
# /!\ updating IN PLACE
gammas[:] = new
# Try to reduce the number of gammas by using the duplication
# theorem to cancel an upper and lower: gamma(2*s)/gamma(s) =
# 2**(2*s + 1)/(4*sqrt(pi))*gamma(s + 1/2). Although this could
# be done with higher argument ratios like gamma(3*x)/gamma(x),
# this would not reduce the number of gammas as in this case.
for ng, dg, no, do in [(numer_gammas, denom_gammas, numer_others,
denom_others),
(denom_gammas, numer_gammas, denom_others,
numer_others)]:
while True:
for x in ng:
for y in dg:
n = x - 2*y
if n.is_Integer:
break
else:
continue
break
else:
break
ng.remove(x)
dg.remove(y)
if n > 0:
for k in range(n):
no.append(2*y + k)
elif n < 0:
for k in range(-n):
do.append(2*y - 1 - k)
ng.append(y + S.Half)
no.append(2**(2*y - 1))
do.append(sqrt(S.Pi))
# Try to reduce the number of gamma factors by applying the
# multiplication theorem (used when n gammas with args differing
# by 1/n mod 1 are encountered).
#
# run of 2 with args differing by 1/2
#
# >>> gammasimp(gamma(x)*gamma(x+S.Half))
# 2*sqrt(2)*2**(-2*x - 1/2)*sqrt(pi)*gamma(2*x)
#
# run of 3 args differing by 1/3 (mod 1)
#
# >>> gammasimp(gamma(x)*gamma(x+S(1)/3)*gamma(x+S(2)/3))
# 6*3**(-3*x - 1/2)*pi*gamma(3*x)
# >>> gammasimp(gamma(x)*gamma(x+S(1)/3)*gamma(x+S(5)/3))
# 2*3**(-3*x - 1/2)*pi*(3*x + 2)*gamma(3*x)
#
def _run(coeffs):
# find runs in coeffs such that the difference in terms (mod 1)
# of t1, t2, ..., tn is 1/n
u = list(uniq(coeffs))
for i in range(len(u)):
dj = ([((u[j] - u[i]) % 1, j) for j in range(i + 1, len(u))])
for one, j in dj:
if one.p == 1 and one.q != 1:
n = one.q
got = [i]
get = list(range(1, n))
for d, j in dj:
m = n*d
if m.is_Integer and m in get:
get.remove(m)
got.append(j)
if not get:
break
else:
continue
for i, j in enumerate(got):
c = u[j]
coeffs.remove(c)
got[i] = c
return one.q, got[0], got[1:]
def _mult_thm(gammas, numer, denom):
# pull off and analyze the leading coefficient from each gamma arg
# looking for runs in those Rationals
# expr -> coeff + resid -> rats[resid] = coeff
rats = {}
for g in gammas:
c, resid = g.as_coeff_Add()
rats.setdefault(resid, []).append(c)
# look for runs in Rationals for each resid
keys = sorted(rats, key=default_sort_key)
for resid in keys:
coeffs = list(sorted(rats[resid]))
new = []
while True:
run = _run(coeffs)
if run is None:
break
# process the sequence that was found:
# 1) convert all the gamma functions to have the right
# argument (could be off by an integer)
# 2) append the factors corresponding to the theorem
# 3) append the new gamma function
n, ui, other = run
# (1)
for u in other:
con = resid + u - 1
for k in range(int(u - ui)):
numer.append(con - k)
con = n*(resid + ui) # for (2) and (3)
# (2)
numer.append((2*S.Pi)**(S(n - 1)/2)*
n**(S.Half - con))
# (3)
new.append(con)
# restore resid to coeffs
rats[resid] = [resid + c for c in coeffs] + new
# rebuild the gamma arguments
g = []
for resid in keys:
g += rats[resid]
# /!\ updating IN PLACE
gammas[:] = g
for l, numer, denom in [(numer_gammas, numer_others, denom_others),
(denom_gammas, denom_others, numer_others)]:
_mult_thm(l, numer, denom)
# =========== level >= 2 work: factor absorption =========
if level >= 2:
# Try to absorb factors into the gammas: x*gamma(x) -> gamma(x + 1)
# and gamma(x)/(x - 1) -> gamma(x - 1)
# This code (in particular repeated calls to find_fuzzy) can be very
# slow.
def find_fuzzy(l, x):
if not l:
return
S1, T1 = compute_ST(x)
for y in l:
S2, T2 = inv[y]
if T1 != T2 or (not S1.intersection(S2) and
(S1 != set() or S2 != set())):
continue
# XXX we want some simplification (e.g. cancel or
# simplify) but no matter what it's slow.
a = len(cancel(x/y).free_symbols)
b = len(x.free_symbols)
c = len(y.free_symbols)
# TODO is there a better heuristic?
if a == 0 and (b > 0 or c > 0):
return y
# We thus try to avoid expensive calls by building the following
# "invariants": For every factor or gamma function argument
# - the set of free symbols S
# - the set of functional components T
# We will only try to absorb if T1==T2 and (S1 intersect S2 != emptyset
# or S1 == S2 == emptyset)
inv = {}
def compute_ST(expr):
if expr in inv:
return inv[expr]
return (expr.free_symbols, expr.atoms(Function).union(
set(e.exp for e in expr.atoms(Pow))))
def update_ST(expr):
inv[expr] = compute_ST(expr)
for expr in numer_gammas + denom_gammas + numer_others + denom_others:
update_ST(expr)
for gammas, numer, denom in [(
numer_gammas, numer_others, denom_others),
(denom_gammas, denom_others, numer_others)]:
new = []
while gammas:
g = gammas.pop()
cont = True
while cont:
cont = False
y = find_fuzzy(numer, g)
if y is not None:
numer.remove(y)
if y != g:
numer.append(y/g)
update_ST(y/g)
g += 1
cont = True
y = find_fuzzy(denom, g - 1)
if y is not None:
denom.remove(y)
if y != g - 1:
numer.append((g - 1)/y)
update_ST((g - 1)/y)
g -= 1
cont = True
new.append(g)
# /!\ updating IN PLACE
gammas[:] = new
# =========== rebuild expr ==================================
return Mul(*[gamma(g) for g in numer_gammas]) \
/ Mul(*[gamma(g) for g in denom_gammas]) \
* Mul(*numer_others) / Mul(*denom_others)
# (for some reason we cannot use Basic.replace in this case)
was = factor(expr)
expr = rule_gamma(was)
if expr != was:
expr = factor(expr)
expr = expr.replace(gamma,
lambda n: expand_func(gamma(n)) if n.is_Rational else gamma(n))
return expr
class _rf(Function):
@classmethod
def eval(cls, a, b):
if b.is_Integer:
if not b:
return S.One
n, result = int(b), S.One
if n > 0:
for i in range(n):
result *= a + i
return result
elif n < 0:
for i in range(1, -n + 1):
result *= a - i
return 1/result
else:
if b.is_Add:
c, _b = b.as_coeff_Add()
if c.is_Integer:
if c > 0:
return _rf(a, _b)*_rf(a + _b, c)
elif c < 0:
return _rf(a, _b)/_rf(a + _b + c, -c)
if a.is_Add:
c, _a = a.as_coeff_Add()
if c.is_Integer:
if c > 0:
return _rf(_a, b)*_rf(_a + b, c)/_rf(_a, c)
elif c < 0:
return _rf(_a, b)*_rf(_a + c, -c)/_rf(_a + b + c, -c)
|
625d13b368b7124882bd0cb24848b8b999c697029a34ee042ebcc75c7ef2e6d3 | # References :
# http://www.euclideanspace.com/maths/algebra/realNormedAlgebra/quaternions/
# https://en.wikipedia.org/wiki/Quaternion
from __future__ import print_function
from sympy import S, Rational
from sympy import re, im, conjugate
from sympy import sqrt, sin, cos, acos, exp, ln
from sympy import trigsimp
from sympy import integrate
from sympy import Matrix
from sympy import sympify
from sympy.core.expr import Expr
class Quaternion(Expr):
"""Provides basic quaternion operations.
Quaternion objects can be instantiated as Quaternion(a, b, c, d)
as in (a + b*i + c*j + d*k).
Examples
========
>>> from sympy.algebras.quaternion import Quaternion
>>> q = Quaternion(1, 2, 3, 4)
>>> q
1 + 2*i + 3*j + 4*k
Quaternions over complex fields can be defined as :
>>> from sympy.algebras.quaternion import Quaternion
>>> from sympy import symbols, I
>>> x = symbols('x')
>>> q1 = Quaternion(x, x**3, x, x**2, real_field = False)
>>> q2 = Quaternion(3 + 4*I, 2 + 5*I, 0, 7 + 8*I, real_field = False)
>>> q1
x + x**3*i + x*j + x**2*k
>>> q2
(3 + 4*I) + (2 + 5*I)*i + 0*j + (7 + 8*I)*k
"""
_op_priority = 11.0
is_commutative = False
def __new__(cls, a=0, b=0, c=0, d=0, real_field=True):
a = sympify(a)
b = sympify(b)
c = sympify(c)
d = sympify(d)
if any(i.is_commutative is False for i in [a, b, c, d]):
raise ValueError("arguments have to be commutative")
else:
obj = Expr.__new__(cls, a, b, c, d)
obj._a = a
obj._b = b
obj._c = c
obj._d = d
obj._real_field = real_field
return obj
@property
def a(self):
return self._a
@property
def b(self):
return self._b
@property
def c(self):
return self._c
@property
def d(self):
return self._d
@property
def real_field(self):
return self._real_field
@classmethod
def from_axis_angle(cls, vector, angle):
"""Returns a rotation quaternion given the axis and the angle of rotation.
Parameters
==========
vector : tuple of three numbers
The vector representation of the given axis.
angle : number
The angle by which axis is rotated (in radians).
Returns
=======
Quaternion
The normalized rotation quaternion calculated from the given axis and the angle of rotation.
Examples
========
>>> from sympy.algebras.quaternion import Quaternion
>>> from sympy import pi, sqrt
>>> q = Quaternion.from_axis_angle((sqrt(3)/3, sqrt(3)/3, sqrt(3)/3), 2*pi/3)
>>> q
1/2 + 1/2*i + 1/2*j + 1/2*k
"""
(x, y, z) = vector
norm = sqrt(x**2 + y**2 + z**2)
(x, y, z) = (x / norm, y / norm, z / norm)
s = sin(angle * S.Half)
a = cos(angle * S.Half)
b = x * s
c = y * s
d = z * s
return cls(a, b, c, d).normalize()
@classmethod
def from_rotation_matrix(cls, M):
"""Returns the equivalent quaternion of a matrix. The quaternion will be normalized
only if the matrix is special orthogonal (orthogonal and det(M) = 1).
Parameters
==========
M : Matrix
Input matrix to be converted to equivalent quaternion. M must be special
orthogonal (orthogonal and det(M) = 1) for the quaternion to be normalized.
Returns
=======
Quaternion
The quaternion equivalent to given matrix.
Examples
========
>>> from sympy.algebras.quaternion import Quaternion
>>> from sympy import Matrix, symbols, cos, sin, trigsimp
>>> x = symbols('x')
>>> M = Matrix([[cos(x), -sin(x), 0], [sin(x), cos(x), 0], [0, 0, 1]])
>>> q = trigsimp(Quaternion.from_rotation_matrix(M))
>>> q
sqrt(2)*sqrt(cos(x) + 1)/2 + 0*i + 0*j + sqrt(2 - 2*cos(x))/2*k
"""
absQ = M.det()**Rational(1, 3)
a = sqrt(absQ + M[0, 0] + M[1, 1] + M[2, 2]) / 2
b = sqrt(absQ + M[0, 0] - M[1, 1] - M[2, 2]) / 2
c = sqrt(absQ - M[0, 0] + M[1, 1] - M[2, 2]) / 2
d = sqrt(absQ - M[0, 0] - M[1, 1] + M[2, 2]) / 2
try:
b = Quaternion.__copysign(b, M[2, 1] - M[1, 2])
c = Quaternion.__copysign(c, M[0, 2] - M[2, 0])
d = Quaternion.__copysign(d, M[1, 0] - M[0, 1])
except Exception:
pass
return Quaternion(a, b, c, d)
@staticmethod
def __copysign(x, y):
# Takes the sign from the second term and sets the sign of the first
# without altering the magnitude.
if y == 0:
return 0
return x if x*y > 0 else -x
def __add__(self, other):
return self.add(other)
def __radd__(self, other):
return self.add(other)
def __sub__(self, other):
return self.add(other*-1)
def __mul__(self, other):
return self._generic_mul(self, other)
def __rmul__(self, other):
return self._generic_mul(other, self)
def __pow__(self, p):
return self.pow(p)
def __neg__(self):
return Quaternion(-self._a, -self._b, -self._c, -self.d)
def __truediv__(self, other):
return self * sympify(other)**-1
__div__ = __truediv__
def __rtruediv__(self, other):
return sympify(other) * self**-1
__rdiv__ = __rtruediv__
def _eval_Integral(self, *args):
return self.integrate(*args)
def diff(self, *symbols, **kwargs):
kwargs.setdefault('evaluate', True)
return self.func(*[a.diff(*symbols, **kwargs) for a in self.args])
def add(self, other):
"""Adds quaternions.
Parameters
==========
other : Quaternion
The quaternion to add to current (self) quaternion.
Returns
=======
Quaternion
The resultant quaternion after adding self to other
Examples
========
>>> from sympy.algebras.quaternion import Quaternion
>>> from sympy import symbols
>>> q1 = Quaternion(1, 2, 3, 4)
>>> q2 = Quaternion(5, 6, 7, 8)
>>> q1.add(q2)
6 + 8*i + 10*j + 12*k
>>> q1 + 5
6 + 2*i + 3*j + 4*k
>>> x = symbols('x', real = True)
>>> q1.add(x)
(x + 1) + 2*i + 3*j + 4*k
Quaternions over complex fields :
>>> from sympy.algebras.quaternion import Quaternion
>>> from sympy import I
>>> q3 = Quaternion(3 + 4*I, 2 + 5*I, 0, 7 + 8*I, real_field = False)
>>> q3.add(2 + 3*I)
(5 + 7*I) + (2 + 5*I)*i + 0*j + (7 + 8*I)*k
"""
q1 = self
q2 = sympify(other)
# If q2 is a number or a sympy expression instead of a quaternion
if not isinstance(q2, Quaternion):
if q1.real_field and q2.is_complex:
return Quaternion(re(q2) + q1.a, im(q2) + q1.b, q1.c, q1.d)
elif q2.is_commutative:
return Quaternion(q1.a + q2, q1.b, q1.c, q1.d)
else:
raise ValueError("Only commutative expressions can be added with a Quaternion.")
return Quaternion(q1.a + q2.a, q1.b + q2.b, q1.c + q2.c, q1.d
+ q2.d)
def mul(self, other):
"""Multiplies quaternions.
Parameters
==========
other : Quaternion or symbol
The quaternion to multiply to current (self) quaternion.
Returns
=======
Quaternion
The resultant quaternion after multiplying self with other
Examples
========
>>> from sympy.algebras.quaternion import Quaternion
>>> from sympy import symbols
>>> q1 = Quaternion(1, 2, 3, 4)
>>> q2 = Quaternion(5, 6, 7, 8)
>>> q1.mul(q2)
(-60) + 12*i + 30*j + 24*k
>>> q1.mul(2)
2 + 4*i + 6*j + 8*k
>>> x = symbols('x', real = True)
>>> q1.mul(x)
x + 2*x*i + 3*x*j + 4*x*k
Quaternions over complex fields :
>>> from sympy.algebras.quaternion import Quaternion
>>> from sympy import I
>>> q3 = Quaternion(3 + 4*I, 2 + 5*I, 0, 7 + 8*I, real_field = False)
>>> q3.mul(2 + 3*I)
(2 + 3*I)*(3 + 4*I) + (2 + 3*I)*(2 + 5*I)*i + 0*j + (2 + 3*I)*(7 + 8*I)*k
"""
return self._generic_mul(self, other)
@staticmethod
def _generic_mul(q1, q2):
"""Generic multiplication.
Parameters
==========
q1 : Quaternion or symbol
q2 : Quaternion or symbol
It's important to note that if neither q1 nor q2 is a Quaternion,
this function simply returns q1 * q2.
Returns
=======
Quaternion
The resultant quaternion after multiplying q1 and q2
Examples
========
>>> from sympy.algebras.quaternion import Quaternion
>>> from sympy import Symbol
>>> q1 = Quaternion(1, 2, 3, 4)
>>> q2 = Quaternion(5, 6, 7, 8)
>>> Quaternion._generic_mul(q1, q2)
(-60) + 12*i + 30*j + 24*k
>>> Quaternion._generic_mul(q1, 2)
2 + 4*i + 6*j + 8*k
>>> x = Symbol('x', real = True)
>>> Quaternion._generic_mul(q1, x)
x + 2*x*i + 3*x*j + 4*x*k
Quaternions over complex fields :
>>> from sympy.algebras.quaternion import Quaternion
>>> from sympy import I
>>> q3 = Quaternion(3 + 4*I, 2 + 5*I, 0, 7 + 8*I, real_field = False)
>>> Quaternion._generic_mul(q3, 2 + 3*I)
(2 + 3*I)*(3 + 4*I) + (2 + 3*I)*(2 + 5*I)*i + 0*j + (2 + 3*I)*(7 + 8*I)*k
"""
q1 = sympify(q1)
q2 = sympify(q2)
# None is a Quaternion:
if not isinstance(q1, Quaternion) and not isinstance(q2, Quaternion):
return q1 * q2
# If q1 is a number or a sympy expression instead of a quaternion
if not isinstance(q1, Quaternion):
if q2.real_field and q1.is_complex:
return Quaternion(re(q1), im(q1), 0, 0) * q2
elif q1.is_commutative:
return Quaternion(q1 * q2.a, q1 * q2.b, q1 * q2.c, q1 * q2.d)
else:
raise ValueError("Only commutative expressions can be multiplied with a Quaternion.")
# If q2 is a number or a sympy expression instead of a quaternion
if not isinstance(q2, Quaternion):
if q1.real_field and q2.is_complex:
return q1 * Quaternion(re(q2), im(q2), 0, 0)
elif q2.is_commutative:
return Quaternion(q2 * q1.a, q2 * q1.b, q2 * q1.c, q2 * q1.d)
else:
raise ValueError("Only commutative expressions can be multiplied with a Quaternion.")
return Quaternion(-q1.b*q2.b - q1.c*q2.c - q1.d*q2.d + q1.a*q2.a,
q1.b*q2.a + q1.c*q2.d - q1.d*q2.c + q1.a*q2.b,
-q1.b*q2.d + q1.c*q2.a + q1.d*q2.b + q1.a*q2.c,
q1.b*q2.c - q1.c*q2.b + q1.d*q2.a + q1.a * q2.d)
def _eval_conjugate(self):
"""Returns the conjugate of the quaternion."""
q = self
return Quaternion(q.a, -q.b, -q.c, -q.d)
def norm(self):
"""Returns the norm of the quaternion."""
q = self
# trigsimp is used to simplify sin(x)^2 + cos(x)^2 (these terms
# arise when from_axis_angle is used).
return sqrt(trigsimp(q.a**2 + q.b**2 + q.c**2 + q.d**2))
def normalize(self):
"""Returns the normalized form of the quaternion."""
q = self
return q * (1/q.norm())
def inverse(self):
"""Returns the inverse of the quaternion."""
q = self
if not q.norm():
raise ValueError("Cannot compute inverse for a quaternion with zero norm")
return conjugate(q) * (1/q.norm()**2)
def pow(self, p):
"""Finds the pth power of the quaternion.
Parameters
==========
p : int
Power to be applied on quaternion.
Returns
=======
Quaternion
Returns the p-th power of the current quaternion.
Returns the inverse if p = -1.
Examples
========
>>> from sympy.algebras.quaternion import Quaternion
>>> q = Quaternion(1, 2, 3, 4)
>>> q.pow(4)
668 + (-224)*i + (-336)*j + (-448)*k
"""
p = sympify(p)
q = self
if p == -1:
return q.inverse()
res = 1
if not p.is_Integer:
return NotImplemented
if p < 0:
q, p = q.inverse(), -p
while p > 0:
if p % 2 == 1:
res = q * res
p = p//2
q = q * q
return res
def exp(self):
"""Returns the exponential of q (e^q).
Returns
=======
Quaternion
Exponential of q (e^q).
Examples
========
>>> from sympy.algebras.quaternion import Quaternion
>>> q = Quaternion(1, 2, 3, 4)
>>> q.exp()
E*cos(sqrt(29))
+ 2*sqrt(29)*E*sin(sqrt(29))/29*i
+ 3*sqrt(29)*E*sin(sqrt(29))/29*j
+ 4*sqrt(29)*E*sin(sqrt(29))/29*k
"""
# exp(q) = e^a(cos||v|| + v/||v||*sin||v||)
q = self
vector_norm = sqrt(q.b**2 + q.c**2 + q.d**2)
a = exp(q.a) * cos(vector_norm)
b = exp(q.a) * sin(vector_norm) * q.b / vector_norm
c = exp(q.a) * sin(vector_norm) * q.c / vector_norm
d = exp(q.a) * sin(vector_norm) * q.d / vector_norm
return Quaternion(a, b, c, d)
def _ln(self):
"""Returns the natural logarithm of the quaternion (_ln(q)).
Examples
========
>>> from sympy.algebras.quaternion import Quaternion
>>> q = Quaternion(1, 2, 3, 4)
>>> q._ln()
log(sqrt(30))
+ 2*sqrt(29)*acos(sqrt(30)/30)/29*i
+ 3*sqrt(29)*acos(sqrt(30)/30)/29*j
+ 4*sqrt(29)*acos(sqrt(30)/30)/29*k
"""
# _ln(q) = _ln||q|| + v/||v||*arccos(a/||q||)
q = self
vector_norm = sqrt(q.b**2 + q.c**2 + q.d**2)
q_norm = q.norm()
a = ln(q_norm)
b = q.b * acos(q.a / q_norm) / vector_norm
c = q.c * acos(q.a / q_norm) / vector_norm
d = q.d * acos(q.a / q_norm) / vector_norm
return Quaternion(a, b, c, d)
def pow_cos_sin(self, p):
"""Computes the pth power in the cos-sin form.
Parameters
==========
p : int
Power to be applied on quaternion.
Returns
=======
Quaternion
The p-th power in the cos-sin form.
Examples
========
>>> from sympy.algebras.quaternion import Quaternion
>>> q = Quaternion(1, 2, 3, 4)
>>> q.pow_cos_sin(4)
900*cos(4*acos(sqrt(30)/30))
+ 1800*sqrt(29)*sin(4*acos(sqrt(30)/30))/29*i
+ 2700*sqrt(29)*sin(4*acos(sqrt(30)/30))/29*j
+ 3600*sqrt(29)*sin(4*acos(sqrt(30)/30))/29*k
"""
# q = ||q||*(cos(a) + u*sin(a))
# q^p = ||q||^p * (cos(p*a) + u*sin(p*a))
q = self
(v, angle) = q.to_axis_angle()
q2 = Quaternion.from_axis_angle(v, p * angle)
return q2 * (q.norm()**p)
def integrate(self, *args):
# TODO: is this expression correct?
return Quaternion(integrate(self.a, *args), integrate(self.b, *args),
integrate(self.c, *args), integrate(self.d, *args))
@staticmethod
def rotate_point(pin, r):
"""Returns the coordinates of the point pin(a 3 tuple) after rotation.
Parameters
==========
pin : tuple
A 3-element tuple of coordinates of a point. This point will be
the axis of rotation.
r
Angle to be rotated.
Returns
=======
tuple
The coordinates of the quaternion after rotation.
Examples
========
>>> from sympy.algebras.quaternion import Quaternion
>>> from sympy import symbols, trigsimp, cos, sin
>>> x = symbols('x')
>>> q = Quaternion(cos(x/2), 0, 0, sin(x/2))
>>> trigsimp(Quaternion.rotate_point((1, 1, 1), q))
(sqrt(2)*cos(x + pi/4), sqrt(2)*sin(x + pi/4), 1)
>>> (axis, angle) = q.to_axis_angle()
>>> trigsimp(Quaternion.rotate_point((1, 1, 1), (axis, angle)))
(sqrt(2)*cos(x + pi/4), sqrt(2)*sin(x + pi/4), 1)
"""
if isinstance(r, tuple):
# if r is of the form (vector, angle)
q = Quaternion.from_axis_angle(r[0], r[1])
else:
# if r is a quaternion
q = r.normalize()
pout = q * Quaternion(0, pin[0], pin[1], pin[2]) * conjugate(q)
return (pout.b, pout.c, pout.d)
def to_axis_angle(self):
"""Returns the axis and angle of rotation of a quaternion
Returns
=======
tuple
Tuple of (axis, angle)
Examples
========
>>> from sympy.algebras.quaternion import Quaternion
>>> q = Quaternion(1, 1, 1, 1)
>>> (axis, angle) = q.to_axis_angle()
>>> axis
(sqrt(3)/3, sqrt(3)/3, sqrt(3)/3)
>>> angle
2*pi/3
"""
q = self
if q.a.is_negative:
q = q * -1
q = q.normalize()
angle = trigsimp(2 * acos(q.a))
# Since quaternion is normalised, q.a is less than 1.
s = sqrt(1 - q.a*q.a)
x = trigsimp(q.b / s)
y = trigsimp(q.c / s)
z = trigsimp(q.d / s)
v = (x, y, z)
t = (v, angle)
return t
def to_rotation_matrix(self, v=None):
"""Returns the equivalent rotation transformation matrix of the quaternion
which represents rotation about the origin if v is not passed.
Parameters
==========
v : tuple or None
Default value: None
Returns
=======
tuple
Returns the equivalent rotation transformation matrix of the quaternion
which represents rotation about the origin if v is not passed.
Examples
========
>>> from sympy.algebras.quaternion import Quaternion
>>> from sympy import symbols, trigsimp, cos, sin
>>> x = symbols('x')
>>> q = Quaternion(cos(x/2), 0, 0, sin(x/2))
>>> trigsimp(q.to_rotation_matrix())
Matrix([
[cos(x), -sin(x), 0],
[sin(x), cos(x), 0],
[ 0, 0, 1]])
Generates a 4x4 transformation matrix (used for rotation about a point
other than the origin) if the point(v) is passed as an argument.
Examples
========
>>> from sympy.algebras.quaternion import Quaternion
>>> from sympy import symbols, trigsimp, cos, sin
>>> x = symbols('x')
>>> q = Quaternion(cos(x/2), 0, 0, sin(x/2))
>>> trigsimp(q.to_rotation_matrix((1, 1, 1)))
Matrix([
[cos(x), -sin(x), 0, sin(x) - cos(x) + 1],
[sin(x), cos(x), 0, -sin(x) - cos(x) + 1],
[ 0, 0, 1, 0],
[ 0, 0, 0, 1]])
"""
q = self
s = q.norm()**-2
m00 = 1 - 2*s*(q.c**2 + q.d**2)
m01 = 2*s*(q.b*q.c - q.d*q.a)
m02 = 2*s*(q.b*q.d + q.c*q.a)
m10 = 2*s*(q.b*q.c + q.d*q.a)
m11 = 1 - 2*s*(q.b**2 + q.d**2)
m12 = 2*s*(q.c*q.d - q.b*q.a)
m20 = 2*s*(q.b*q.d - q.c*q.a)
m21 = 2*s*(q.c*q.d + q.b*q.a)
m22 = 1 - 2*s*(q.b**2 + q.c**2)
if not v:
return Matrix([[m00, m01, m02], [m10, m11, m12], [m20, m21, m22]])
else:
(x, y, z) = v
m03 = x - x*m00 - y*m01 - z*m02
m13 = y - x*m10 - y*m11 - z*m12
m23 = z - x*m20 - y*m21 - z*m22
m30 = m31 = m32 = 0
m33 = 1
return Matrix([[m00, m01, m02, m03], [m10, m11, m12, m13],
[m20, m21, m22, m23], [m30, m31, m32, m33]])
|
8ee0dff1285fc3c379f28a3e83ad1552855bafbc8ebd93cd541c150764ad63ac | """
This module contains SymPy functions mathcin corresponding to special math functions in the
C standard library (since C99, also available in C++11).
The functions defined in this module allows the user to express functions such as ``expm1``
as a SymPy function for symbolic manipulation.
"""
from sympy.core.function import ArgumentIndexError, Function
from sympy.core.numbers import Rational
from sympy.core.power import Pow
from sympy.core.singleton import S
from sympy.functions.elementary.exponential import exp, log
from sympy.functions.elementary.miscellaneous import sqrt
def _expm1(x):
return exp(x) - S.One
class expm1(Function):
"""
Represents the exponential function minus one.
The benefit of using ``expm1(x)`` over ``exp(x) - 1``
is that the latter is prone to cancellation under finite precision
arithmetic when x is close to zero.
Examples
========
>>> from sympy.abc import x
>>> from sympy.codegen.cfunctions import expm1
>>> '%.0e' % expm1(1e-99).evalf()
'1e-99'
>>> from math import exp
>>> exp(1e-99) - 1
0.0
>>> expm1(x).diff(x)
exp(x)
See Also
========
log1p
"""
nargs = 1
def fdiff(self, argindex=1):
"""
Returns the first derivative of this function.
"""
if argindex == 1:
return exp(*self.args)
else:
raise ArgumentIndexError(self, argindex)
def _eval_expand_func(self, **hints):
return _expm1(*self.args)
def _eval_rewrite_as_exp(self, arg, **kwargs):
return exp(arg) - S.One
_eval_rewrite_as_tractable = _eval_rewrite_as_exp
@classmethod
def eval(cls, arg):
exp_arg = exp.eval(arg)
if exp_arg is not None:
return exp_arg - S.One
def _eval_is_real(self):
return self.args[0].is_real
def _eval_is_finite(self):
return self.args[0].is_finite
def _log1p(x):
return log(x + S.One)
class log1p(Function):
"""
Represents the natural logarithm of a number plus one.
The benefit of using ``log1p(x)`` over ``log(x + 1)``
is that the latter is prone to cancellation under finite precision
arithmetic when x is close to zero.
Examples
========
>>> from sympy.abc import x
>>> from sympy.codegen.cfunctions import log1p
>>> from sympy.core.function import expand_log
>>> '%.0e' % expand_log(log1p(1e-99)).evalf()
'1e-99'
>>> from math import log
>>> log(1 + 1e-99)
0.0
>>> log1p(x).diff(x)
1/(x + 1)
See Also
========
expm1
"""
nargs = 1
def fdiff(self, argindex=1):
"""
Returns the first derivative of this function.
"""
if argindex == 1:
return S.One/(self.args[0] + S.One)
else:
raise ArgumentIndexError(self, argindex)
def _eval_expand_func(self, **hints):
return _log1p(*self.args)
def _eval_rewrite_as_log(self, arg, **kwargs):
return _log1p(arg)
_eval_rewrite_as_tractable = _eval_rewrite_as_log
@classmethod
def eval(cls, arg):
if arg.is_Rational:
return log(arg + S.One)
elif not arg.is_Float: # not safe to add 1 to Float
return log.eval(arg + S.One)
elif arg.is_number:
return log(Rational(arg) + S.One)
def _eval_is_real(self):
return (self.args[0] + S.One).is_nonnegative
def _eval_is_finite(self):
if (self.args[0] + S.One).is_zero:
return False
return self.args[0].is_finite
def _eval_is_positive(self):
return self.args[0].is_positive
def _eval_is_zero(self):
return self.args[0].is_zero
def _eval_is_nonnegative(self):
return self.args[0].is_nonnegative
_Two = S(2)
def _exp2(x):
return Pow(_Two, x)
class exp2(Function):
"""
Represents the exponential function with base two.
The benefit of using ``exp2(x)`` over ``2**x``
is that the latter is not as efficient under finite precision
arithmetic.
Examples
========
>>> from sympy.abc import x
>>> from sympy.codegen.cfunctions import exp2
>>> exp2(2).evalf() == 4
True
>>> exp2(x).diff(x)
log(2)*exp2(x)
See Also
========
log2
"""
nargs = 1
def fdiff(self, argindex=1):
"""
Returns the first derivative of this function.
"""
if argindex == 1:
return self*log(_Two)
else:
raise ArgumentIndexError(self, argindex)
def _eval_rewrite_as_Pow(self, arg, **kwargs):
return _exp2(arg)
_eval_rewrite_as_tractable = _eval_rewrite_as_Pow
def _eval_expand_func(self, **hints):
return _exp2(*self.args)
@classmethod
def eval(cls, arg):
if arg.is_number:
return _exp2(arg)
def _log2(x):
return log(x)/log(_Two)
class log2(Function):
"""
Represents the logarithm function with base two.
The benefit of using ``log2(x)`` over ``log(x)/log(2)``
is that the latter is not as efficient under finite precision
arithmetic.
Examples
========
>>> from sympy.abc import x
>>> from sympy.codegen.cfunctions import log2
>>> log2(4).evalf() == 2
True
>>> log2(x).diff(x)
1/(x*log(2))
See Also
========
exp2
log10
"""
nargs = 1
def fdiff(self, argindex=1):
"""
Returns the first derivative of this function.
"""
if argindex == 1:
return S.One/(log(_Two)*self.args[0])
else:
raise ArgumentIndexError(self, argindex)
@classmethod
def eval(cls, arg):
if arg.is_number:
result = log.eval(arg, base=_Two)
if result.is_Atom:
return result
elif arg.is_Pow and arg.base == _Two:
return arg.exp
def _eval_expand_func(self, **hints):
return _log2(*self.args)
def _eval_rewrite_as_log(self, arg, **kwargs):
return _log2(arg)
_eval_rewrite_as_tractable = _eval_rewrite_as_log
def _fma(x, y, z):
return x*y + z
class fma(Function):
"""
Represents "fused multiply add".
The benefit of using ``fma(x, y, z)`` over ``x*y + z``
is that, under finite precision arithmetic, the former is
supported by special instructions on some CPUs.
Examples
========
>>> from sympy.abc import x, y, z
>>> from sympy.codegen.cfunctions import fma
>>> fma(x, y, z).diff(x)
y
"""
nargs = 3
def fdiff(self, argindex=1):
"""
Returns the first derivative of this function.
"""
if argindex in (1, 2):
return self.args[2 - argindex]
elif argindex == 3:
return S.One
else:
raise ArgumentIndexError(self, argindex)
def _eval_expand_func(self, **hints):
return _fma(*self.args)
def _eval_rewrite_as_tractable(self, arg, **kwargs):
return _fma(arg)
_Ten = S(10)
def _log10(x):
return log(x)/log(_Ten)
class log10(Function):
"""
Represents the logarithm function with base ten.
Examples
========
>>> from sympy.abc import x
>>> from sympy.codegen.cfunctions import log10
>>> log10(100).evalf() == 2
True
>>> log10(x).diff(x)
1/(x*log(10))
See Also
========
log2
"""
nargs = 1
def fdiff(self, argindex=1):
"""
Returns the first derivative of this function.
"""
if argindex == 1:
return S.One/(log(_Ten)*self.args[0])
else:
raise ArgumentIndexError(self, argindex)
@classmethod
def eval(cls, arg):
if arg.is_number:
result = log.eval(arg, base=_Ten)
if result.is_Atom:
return result
elif arg.is_Pow and arg.base == _Ten:
return arg.exp
def _eval_expand_func(self, **hints):
return _log10(*self.args)
def _eval_rewrite_as_log(self, arg, **kwargs):
return _log10(arg)
_eval_rewrite_as_tractable = _eval_rewrite_as_log
def _Sqrt(x):
return Pow(x, S.Half)
class Sqrt(Function): # 'sqrt' already defined in sympy.functions.elementary.miscellaneous
"""
Represents the square root function.
The reason why one would use ``Sqrt(x)`` over ``sqrt(x)``
is that the latter is internally represented as ``Pow(x, S.Half)`` which
may not be what one wants when doing code-generation.
Examples
========
>>> from sympy.abc import x
>>> from sympy.codegen.cfunctions import Sqrt
>>> Sqrt(x)
Sqrt(x)
>>> Sqrt(x).diff(x)
1/(2*sqrt(x))
See Also
========
Cbrt
"""
nargs = 1
def fdiff(self, argindex=1):
"""
Returns the first derivative of this function.
"""
if argindex == 1:
return Pow(self.args[0], Rational(-1, 2))/_Two
else:
raise ArgumentIndexError(self, argindex)
def _eval_expand_func(self, **hints):
return _Sqrt(*self.args)
def _eval_rewrite_as_Pow(self, arg, **kwargs):
return _Sqrt(arg)
_eval_rewrite_as_tractable = _eval_rewrite_as_Pow
def _Cbrt(x):
return Pow(x, Rational(1, 3))
class Cbrt(Function): # 'cbrt' already defined in sympy.functions.elementary.miscellaneous
"""
Represents the cube root function.
The reason why one would use ``Cbrt(x)`` over ``cbrt(x)``
is that the latter is internally represented as ``Pow(x, Rational(1, 3))`` which
may not be what one wants when doing code-generation.
Examples
========
>>> from sympy.abc import x
>>> from sympy.codegen.cfunctions import Cbrt
>>> Cbrt(x)
Cbrt(x)
>>> Cbrt(x).diff(x)
1/(3*x**(2/3))
See Also
========
Sqrt
"""
nargs = 1
def fdiff(self, argindex=1):
"""
Returns the first derivative of this function.
"""
if argindex == 1:
return Pow(self.args[0], Rational(-_Two/3))/3
else:
raise ArgumentIndexError(self, argindex)
def _eval_expand_func(self, **hints):
return _Cbrt(*self.args)
def _eval_rewrite_as_Pow(self, arg, **kwargs):
return _Cbrt(arg)
_eval_rewrite_as_tractable = _eval_rewrite_as_Pow
def _hypot(x, y):
return sqrt(Pow(x, 2) + Pow(y, 2))
class hypot(Function):
"""
Represents the hypotenuse function.
The hypotenuse function is provided by e.g. the math library
in the C99 standard, hence one may want to represent the function
symbolically when doing code-generation.
Examples
========
>>> from sympy.abc import x, y
>>> from sympy.codegen.cfunctions import hypot
>>> hypot(3, 4).evalf() == 5
True
>>> hypot(x, y)
hypot(x, y)
>>> hypot(x, y).diff(x)
x/hypot(x, y)
"""
nargs = 2
def fdiff(self, argindex=1):
"""
Returns the first derivative of this function.
"""
if argindex in (1, 2):
return 2*self.args[argindex-1]/(_Two*self.func(*self.args))
else:
raise ArgumentIndexError(self, argindex)
def _eval_expand_func(self, **hints):
return _hypot(*self.args)
def _eval_rewrite_as_Pow(self, arg, **kwargs):
return _hypot(arg)
_eval_rewrite_as_tractable = _eval_rewrite_as_Pow
|
06f7191c576a833f263d8c9a5d3a529c8911aa3764bca69ce5f6d4be8a507c76 | r"""
This module contains :py:meth:`~sympy.solvers.ode.dsolve` and different helper
functions that it uses.
:py:meth:`~sympy.solvers.ode.dsolve` solves ordinary differential equations.
See the docstring on the various functions for their uses. Note that partial
differential equations support is in ``pde.py``. Note that hint functions
have docstrings describing their various methods, but they are intended for
internal use. Use ``dsolve(ode, func, hint=hint)`` to solve an ODE using a
specific hint. See also the docstring on
:py:meth:`~sympy.solvers.ode.dsolve`.
**Functions in this module**
These are the user functions in this module:
- :py:meth:`~sympy.solvers.ode.dsolve` - Solves ODEs.
- :py:meth:`~sympy.solvers.ode.classify_ode` - Classifies ODEs into
possible hints for :py:meth:`~sympy.solvers.ode.dsolve`.
- :py:meth:`~sympy.solvers.ode.checkodesol` - Checks if an equation is the
solution to an ODE.
- :py:meth:`~sympy.solvers.ode.homogeneous_order` - Returns the
homogeneous order of an expression.
- :py:meth:`~sympy.solvers.ode.infinitesimals` - Returns the infinitesimals
of the Lie group of point transformations of an ODE, such that it is
invariant.
- :py:meth:`~sympy.solvers.ode_checkinfsol` - Checks if the given infinitesimals
are the actual infinitesimals of a first order ODE.
These are the non-solver helper functions that are for internal use. The
user should use the various options to
:py:meth:`~sympy.solvers.ode.dsolve` to obtain the functionality provided
by these functions:
- :py:meth:`~sympy.solvers.ode.odesimp` - Does all forms of ODE
simplification.
- :py:meth:`~sympy.solvers.ode.ode_sol_simplicity` - A key function for
comparing solutions by simplicity.
- :py:meth:`~sympy.solvers.ode.constantsimp` - Simplifies arbitrary
constants.
- :py:meth:`~sympy.solvers.ode.constant_renumber` - Renumber arbitrary
constants.
- :py:meth:`~sympy.solvers.ode._handle_Integral` - Evaluate unevaluated
Integrals.
See also the docstrings of these functions.
**Currently implemented solver methods**
The following methods are implemented for solving ordinary differential
equations. See the docstrings of the various hint functions for more
information on each (run ``help(ode)``):
- 1st order separable differential equations.
- 1st order differential equations whose coefficients or `dx` and `dy` are
functions homogeneous of the same order.
- 1st order exact differential equations.
- 1st order linear differential equations.
- 1st order Bernoulli differential equations.
- Power series solutions for first order differential equations.
- Lie Group method of solving first order differential equations.
- 2nd order Liouville differential equations.
- Power series solutions for second order differential equations
at ordinary and regular singular points.
- `n`\th order differential equation that can be solved with algebraic
rearrangement and integration.
- `n`\th order linear homogeneous differential equation with constant
coefficients.
- `n`\th order linear inhomogeneous differential equation with constant
coefficients using the method of undetermined coefficients.
- `n`\th order linear inhomogeneous differential equation with constant
coefficients using the method of variation of parameters.
**Philosophy behind this module**
This module is designed to make it easy to add new ODE solving methods without
having to mess with the solving code for other methods. The idea is that
there is a :py:meth:`~sympy.solvers.ode.classify_ode` function, which takes in
an ODE and tells you what hints, if any, will solve the ODE. It does this
without attempting to solve the ODE, so it is fast. Each solving method is a
hint, and it has its own function, named ``ode_<hint>``. That function takes
in the ODE and any match expression gathered by
:py:meth:`~sympy.solvers.ode.classify_ode` and returns a solved result. If
this result has any integrals in it, the hint function will return an
unevaluated :py:class:`~sympy.integrals.Integral` class.
:py:meth:`~sympy.solvers.ode.dsolve`, which is the user wrapper function
around all of this, will then call :py:meth:`~sympy.solvers.ode.odesimp` on
the result, which, among other things, will attempt to solve the equation for
the dependent variable (the function we are solving for), simplify the
arbitrary constants in the expression, and evaluate any integrals, if the hint
allows it.
**How to add new solution methods**
If you have an ODE that you want :py:meth:`~sympy.solvers.ode.dsolve` to be
able to solve, try to avoid adding special case code here. Instead, try
finding a general method that will solve your ODE, as well as others. This
way, the :py:mod:`~sympy.solvers.ode` module will become more robust, and
unhindered by special case hacks. WolphramAlpha and Maple's
DETools[odeadvisor] function are two resources you can use to classify a
specific ODE. It is also better for a method to work with an `n`\th order ODE
instead of only with specific orders, if possible.
To add a new method, there are a few things that you need to do. First, you
need a hint name for your method. Try to name your hint so that it is
unambiguous with all other methods, including ones that may not be implemented
yet. If your method uses integrals, also include a ``hint_Integral`` hint.
If there is more than one way to solve ODEs with your method, include a hint
for each one, as well as a ``<hint>_best`` hint. Your ``ode_<hint>_best()``
function should choose the best using min with ``ode_sol_simplicity`` as the
key argument. See
:py:meth:`~sympy.solvers.ode.ode_1st_homogeneous_coeff_best`, for example.
The function that uses your method will be called ``ode_<hint>()``, so the
hint must only use characters that are allowed in a Python function name
(alphanumeric characters and the underscore '``_``' character). Include a
function for every hint, except for ``_Integral`` hints
(:py:meth:`~sympy.solvers.ode.dsolve` takes care of those automatically).
Hint names should be all lowercase, unless a word is commonly capitalized
(such as Integral or Bernoulli). If you have a hint that you do not want to
run with ``all_Integral`` that doesn't have an ``_Integral`` counterpart (such
as a best hint that would defeat the purpose of ``all_Integral``), you will
need to remove it manually in the :py:meth:`~sympy.solvers.ode.dsolve` code.
See also the :py:meth:`~sympy.solvers.ode.classify_ode` docstring for
guidelines on writing a hint name.
Determine *in general* how the solutions returned by your method compare with
other methods that can potentially solve the same ODEs. Then, put your hints
in the :py:data:`~sympy.solvers.ode.allhints` tuple in the order that they
should be called. The ordering of this tuple determines which hints are
default. Note that exceptions are ok, because it is easy for the user to
choose individual hints with :py:meth:`~sympy.solvers.ode.dsolve`. In
general, ``_Integral`` variants should go at the end of the list, and
``_best`` variants should go before the various hints they apply to. For
example, the ``undetermined_coefficients`` hint comes before the
``variation_of_parameters`` hint because, even though variation of parameters
is more general than undetermined coefficients, undetermined coefficients
generally returns cleaner results for the ODEs that it can solve than
variation of parameters does, and it does not require integration, so it is
much faster.
Next, you need to have a match expression or a function that matches the type
of the ODE, which you should put in :py:meth:`~sympy.solvers.ode.classify_ode`
(if the match function is more than just a few lines, like
:py:meth:`~sympy.solvers.ode._undetermined_coefficients_match`, it should go
outside of :py:meth:`~sympy.solvers.ode.classify_ode`). It should match the
ODE without solving for it as much as possible, so that
:py:meth:`~sympy.solvers.ode.classify_ode` remains fast and is not hindered by
bugs in solving code. Be sure to consider corner cases. For example, if your
solution method involves dividing by something, make sure you exclude the case
where that division will be 0.
In most cases, the matching of the ODE will also give you the various parts
that you need to solve it. You should put that in a dictionary (``.match()``
will do this for you), and add that as ``matching_hints['hint'] = matchdict``
in the relevant part of :py:meth:`~sympy.solvers.ode.classify_ode`.
:py:meth:`~sympy.solvers.ode.classify_ode` will then send this to
:py:meth:`~sympy.solvers.ode.dsolve`, which will send it to your function as
the ``match`` argument. Your function should be named ``ode_<hint>(eq, func,
order, match)`. If you need to send more information, put it in the ``match``
dictionary. For example, if you had to substitute in a dummy variable in
:py:meth:`~sympy.solvers.ode.classify_ode` to match the ODE, you will need to
pass it to your function using the `match` dict to access it. You can access
the independent variable using ``func.args[0]``, and the dependent variable
(the function you are trying to solve for) as ``func.func``. If, while trying
to solve the ODE, you find that you cannot, raise ``NotImplementedError``.
:py:meth:`~sympy.solvers.ode.dsolve` will catch this error with the ``all``
meta-hint, rather than causing the whole routine to fail.
Add a docstring to your function that describes the method employed. Like
with anything else in SymPy, you will need to add a doctest to the docstring,
in addition to real tests in ``test_ode.py``. Try to maintain consistency
with the other hint functions' docstrings. Add your method to the list at the
top of this docstring. Also, add your method to ``ode.rst`` in the
``docs/src`` directory, so that the Sphinx docs will pull its docstring into
the main SymPy documentation. Be sure to make the Sphinx documentation by
running ``make html`` from within the doc directory to verify that the
docstring formats correctly.
If your solution method involves integrating, use :py:meth:`Integral()
<sympy.integrals.integrals.Integral>` instead of
:py:meth:`~sympy.core.expr.Expr.integrate`. This allows the user to bypass
hard/slow integration by using the ``_Integral`` variant of your hint. In
most cases, calling :py:meth:`sympy.core.basic.Basic.doit` will integrate your
solution. If this is not the case, you will need to write special code in
:py:meth:`~sympy.solvers.ode._handle_Integral`. Arbitrary constants should be
symbols named ``C1``, ``C2``, and so on. All solution methods should return
an equality instance. If you need an arbitrary number of arbitrary constants,
you can use ``constants = numbered_symbols(prefix='C', cls=Symbol, start=1)``.
If it is possible to solve for the dependent function in a general way, do so.
Otherwise, do as best as you can, but do not call solve in your
``ode_<hint>()`` function. :py:meth:`~sympy.solvers.ode.odesimp` will attempt
to solve the solution for you, so you do not need to do that. Lastly, if your
ODE has a common simplification that can be applied to your solutions, you can
add a special case in :py:meth:`~sympy.solvers.ode.odesimp` for it. For
example, solutions returned from the ``1st_homogeneous_coeff`` hints often
have many :py:meth:`~sympy.functions.log` terms, so
:py:meth:`~sympy.solvers.ode.odesimp` calls
:py:meth:`~sympy.simplify.simplify.logcombine` on them (it also helps to write
the arbitrary constant as ``log(C1)`` instead of ``C1`` in this case). Also
consider common ways that you can rearrange your solution to have
:py:meth:`~sympy.solvers.ode.constantsimp` take better advantage of it. It is
better to put simplification in :py:meth:`~sympy.solvers.ode.odesimp` than in
your method, because it can then be turned off with the simplify flag in
:py:meth:`~sympy.solvers.ode.dsolve`. If you have any extraneous
simplification in your function, be sure to only run it using ``if
match.get('simplify', True):``, especially if it can be slow or if it can
reduce the domain of the solution.
Finally, as with every contribution to SymPy, your method will need to be
tested. Add a test for each method in ``test_ode.py``. Follow the
conventions there, i.e., test the solver using ``dsolve(eq, f(x),
hint=your_hint)``, and also test the solution using
:py:meth:`~sympy.solvers.ode.checkodesol` (you can put these in a separate
tests and skip/XFAIL if it runs too slow/doesn't work). Be sure to call your
hint specifically in :py:meth:`~sympy.solvers.ode.dsolve`, that way the test
won't be broken simply by the introduction of another matching hint. If your
method works for higher order (>1) ODEs, you will need to run ``sol =
constant_renumber(sol, 'C', 1, order)`` for each solution, where ``order`` is
the order of the ODE. This is because ``constant_renumber`` renumbers the
arbitrary constants by printing order, which is platform dependent. Try to
test every corner case of your solver, including a range of orders if it is a
`n`\th order solver, but if your solver is slow, such as if it involves hard
integration, try to keep the test run time down.
Feel free to refactor existing hints to avoid duplicating code or creating
inconsistencies. If you can show that your method exactly duplicates an
existing method, including in the simplicity and speed of obtaining the
solutions, then you can remove the old, less general method. The existing
code is tested extensively in ``test_ode.py``, so if anything is broken, one
of those tests will surely fail.
"""
from __future__ import print_function, division
from collections import defaultdict
from itertools import islice
from sympy.core import Add, S, Mul, Pow, oo, Rational
from sympy.core.compatibility import ordered, iterable, is_sequence, range, string_types
from sympy.core.containers import Tuple
from sympy.core.exprtools import factor_terms
from sympy.core.expr import AtomicExpr, Expr
from sympy.core.function import (Function, Derivative, AppliedUndef, diff,
expand, expand_mul, Subs, _mexpand)
from sympy.core.multidimensional import vectorize
from sympy.core.numbers import NaN, zoo, I, Number
from sympy.core.relational import Equality, Eq
from sympy.core.symbol import Symbol, Wild, Dummy, symbols
from sympy.core.sympify import sympify
from sympy.logic.boolalg import (BooleanAtom, And, Not, BooleanTrue,
BooleanFalse)
from sympy.functions import cos, exp, im, log, re, sin, tan, sqrt, \
atan2, conjugate, Piecewise, cbrt, besselj, bessely, airyai, airybi
from sympy.functions.combinatorial.factorials import factorial
from sympy.integrals.integrals import Integral, integrate
from sympy.matrices import wronskian, Matrix, eye, zeros
from sympy.polys import (Poly, RootOf, rootof, terms_gcd,
PolynomialError, lcm, roots)
from sympy.polys.polyroots import roots_quartic
from sympy.polys.polytools import cancel, degree, div
from sympy.series import Order
from sympy.series.series import series
from sympy.simplify import collect, logcombine, powsimp, separatevars, \
simplify, trigsimp, posify, cse, besselsimp
from sympy.simplify.powsimp import powdenest
from sympy.simplify.radsimp import collect_const, fraction
from sympy.solvers import checksol, solve
from sympy.solvers.pde import pdsolve
from sympy.utilities import numbered_symbols, default_sort_key, sift
from sympy.solvers.deutils import _preprocess, ode_order, _desolve
#: This is a list of hints in the order that they should be preferred by
#: :py:meth:`~sympy.solvers.ode.classify_ode`. In general, hints earlier in the
#: list should produce simpler solutions than those later in the list (for
#: ODEs that fit both). For now, the order of this list is based on empirical
#: observations by the developers of SymPy.
#:
#: The hint used by :py:meth:`~sympy.solvers.ode.dsolve` for a specific ODE
#: can be overridden (see the docstring).
#:
#: In general, ``_Integral`` hints are grouped at the end of the list, unless
#: there is a method that returns an unevaluable integral most of the time
#: (which go near the end of the list anyway). ``default``, ``all``,
#: ``best``, and ``all_Integral`` meta-hints should not be included in this
#: list, but ``_best`` and ``_Integral`` hints should be included.
allhints = (
"factorable",
"nth_algebraic",
"separable",
"1st_exact",
"1st_linear",
"Bernoulli",
"Riccati_special_minus2",
"1st_homogeneous_coeff_best",
"1st_homogeneous_coeff_subs_indep_div_dep",
"1st_homogeneous_coeff_subs_dep_div_indep",
"almost_linear",
"linear_coefficients",
"separable_reduced",
"1st_power_series",
"lie_group",
"nth_linear_constant_coeff_homogeneous",
"nth_linear_euler_eq_homogeneous",
"nth_linear_constant_coeff_undetermined_coefficients",
"nth_linear_euler_eq_nonhomogeneous_undetermined_coefficients",
"nth_linear_constant_coeff_variation_of_parameters",
"nth_linear_euler_eq_nonhomogeneous_variation_of_parameters",
"Liouville",
"2nd_linear_airy",
"2nd_linear_bessel",
"nth_order_reducible",
"2nd_power_series_ordinary",
"2nd_power_series_regular",
"nth_algebraic_Integral",
"separable_Integral",
"1st_exact_Integral",
"1st_linear_Integral",
"Bernoulli_Integral",
"1st_homogeneous_coeff_subs_indep_div_dep_Integral",
"1st_homogeneous_coeff_subs_dep_div_indep_Integral",
"almost_linear_Integral",
"linear_coefficients_Integral",
"separable_reduced_Integral",
"nth_linear_constant_coeff_variation_of_parameters_Integral",
"nth_linear_euler_eq_nonhomogeneous_variation_of_parameters_Integral",
"Liouville_Integral",
)
lie_heuristics = (
"abaco1_simple",
"abaco1_product",
"abaco2_similar",
"abaco2_unique_unknown",
"abaco2_unique_general",
"linear",
"function_sum",
"bivariate",
"chi"
)
def sub_func_doit(eq, func, new):
r"""
When replacing the func with something else, we usually want the
derivative evaluated, so this function helps in making that happen.
Examples
========
>>> from sympy import Derivative, symbols, Function
>>> from sympy.solvers.ode import sub_func_doit
>>> x, z = symbols('x, z')
>>> y = Function('y')
>>> sub_func_doit(3*Derivative(y(x), x) - 1, y(x), x)
2
>>> sub_func_doit(x*Derivative(y(x), x) - y(x)**2 + y(x), y(x),
... 1/(x*(z + 1/x)))
x*(-1/(x**2*(z + 1/x)) + 1/(x**3*(z + 1/x)**2)) + 1/(x*(z + 1/x))
...- 1/(x**2*(z + 1/x)**2)
"""
reps= {func: new}
for d in eq.atoms(Derivative):
if d.expr == func:
reps[d] = new.diff(*d.variable_count)
else:
reps[d] = d.xreplace({func: new}).doit(deep=False)
return eq.xreplace(reps)
def get_numbered_constants(eq, num=1, start=1, prefix='C'):
"""
Returns a list of constants that do not occur
in eq already.
"""
ncs = iter_numbered_constants(eq, start, prefix)
Cs = [next(ncs) for i in range(num)]
return (Cs[0] if num == 1 else tuple(Cs))
def iter_numbered_constants(eq, start=1, prefix='C'):
"""
Returns an iterator of constants that do not occur
in eq already.
"""
if isinstance(eq, Expr):
eq = [eq]
elif not iterable(eq):
raise ValueError("Expected Expr or iterable but got %s" % eq)
atom_set = set().union(*[i.free_symbols for i in eq])
func_set = set().union(*[i.atoms(Function) for i in eq])
if func_set:
atom_set |= {Symbol(str(f.func)) for f in func_set}
return numbered_symbols(start=start, prefix=prefix, exclude=atom_set)
def dsolve(eq, func=None, hint="default", simplify=True,
ics= None, xi=None, eta=None, x0=0, n=6, **kwargs):
r"""
Solves any (supported) kind of ordinary differential equation and
system of ordinary differential equations.
For single ordinary differential equation
=========================================
It is classified under this when number of equation in ``eq`` is one.
**Usage**
``dsolve(eq, f(x), hint)`` -> Solve ordinary differential equation
``eq`` for function ``f(x)``, using method ``hint``.
**Details**
``eq`` can be any supported ordinary differential equation (see the
:py:mod:`~sympy.solvers.ode` docstring for supported methods).
This can either be an :py:class:`~sympy.core.relational.Equality`,
or an expression, which is assumed to be equal to ``0``.
``f(x)`` is a function of one variable whose derivatives in that
variable make up the ordinary differential equation ``eq``. In
many cases it is not necessary to provide this; it will be
autodetected (and an error raised if it couldn't be detected).
``hint`` is the solving method that you want dsolve to use. Use
``classify_ode(eq, f(x))`` to get all of the possible hints for an
ODE. The default hint, ``default``, will use whatever hint is
returned first by :py:meth:`~sympy.solvers.ode.classify_ode`. See
Hints below for more options that you can use for hint.
``simplify`` enables simplification by
:py:meth:`~sympy.solvers.ode.odesimp`. See its docstring for more
information. Turn this off, for example, to disable solving of
solutions for ``func`` or simplification of arbitrary constants.
It will still integrate with this hint. Note that the solution may
contain more arbitrary constants than the order of the ODE with
this option enabled.
``xi`` and ``eta`` are the infinitesimal functions of an ordinary
differential equation. They are the infinitesimals of the Lie group
of point transformations for which the differential equation is
invariant. The user can specify values for the infinitesimals. If
nothing is specified, ``xi`` and ``eta`` are calculated using
:py:meth:`~sympy.solvers.ode.infinitesimals` with the help of various
heuristics.
``ics`` is the set of initial/boundary conditions for the differential equation.
It should be given in the form of ``{f(x0): x1, f(x).diff(x).subs(x, x2):
x3}`` and so on. For power series solutions, if no initial
conditions are specified ``f(0)`` is assumed to be ``C0`` and the power
series solution is calculated about 0.
``x0`` is the point about which the power series solution of a differential
equation is to be evaluated.
``n`` gives the exponent of the dependent variable up to which the power series
solution of a differential equation is to be evaluated.
**Hints**
Aside from the various solving methods, there are also some meta-hints
that you can pass to :py:meth:`~sympy.solvers.ode.dsolve`:
``default``:
This uses whatever hint is returned first by
:py:meth:`~sympy.solvers.ode.classify_ode`. This is the
default argument to :py:meth:`~sympy.solvers.ode.dsolve`.
``all``:
To make :py:meth:`~sympy.solvers.ode.dsolve` apply all
relevant classification hints, use ``dsolve(ODE, func,
hint="all")``. This will return a dictionary of
``hint:solution`` terms. If a hint causes dsolve to raise the
``NotImplementedError``, value of that hint's key will be the
exception object raised. The dictionary will also include
some special keys:
- ``order``: The order of the ODE. See also
:py:meth:`~sympy.solvers.deutils.ode_order` in
``deutils.py``.
- ``best``: The simplest hint; what would be returned by
``best`` below.
- ``best_hint``: The hint that would produce the solution
given by ``best``. If more than one hint produces the best
solution, the first one in the tuple returned by
:py:meth:`~sympy.solvers.ode.classify_ode` is chosen.
- ``default``: The solution that would be returned by default.
This is the one produced by the hint that appears first in
the tuple returned by
:py:meth:`~sympy.solvers.ode.classify_ode`.
``all_Integral``:
This is the same as ``all``, except if a hint also has a
corresponding ``_Integral`` hint, it only returns the
``_Integral`` hint. This is useful if ``all`` causes
:py:meth:`~sympy.solvers.ode.dsolve` to hang because of a
difficult or impossible integral. This meta-hint will also be
much faster than ``all``, because
:py:meth:`~sympy.core.expr.Expr.integrate` is an expensive
routine.
``best``:
To have :py:meth:`~sympy.solvers.ode.dsolve` try all methods
and return the simplest one. This takes into account whether
the solution is solvable in the function, whether it contains
any Integral classes (i.e. unevaluatable integrals), and
which one is the shortest in size.
See also the :py:meth:`~sympy.solvers.ode.classify_ode` docstring for
more info on hints, and the :py:mod:`~sympy.solvers.ode` docstring for
a list of all supported hints.
**Tips**
- You can declare the derivative of an unknown function this way:
>>> from sympy import Function, Derivative
>>> from sympy.abc import x # x is the independent variable
>>> f = Function("f")(x) # f is a function of x
>>> # f_ will be the derivative of f with respect to x
>>> f_ = Derivative(f, x)
- See ``test_ode.py`` for many tests, which serves also as a set of
examples for how to use :py:meth:`~sympy.solvers.ode.dsolve`.
- :py:meth:`~sympy.solvers.ode.dsolve` always returns an
:py:class:`~sympy.core.relational.Equality` class (except for the
case when the hint is ``all`` or ``all_Integral``). If possible, it
solves the solution explicitly for the function being solved for.
Otherwise, it returns an implicit solution.
- Arbitrary constants are symbols named ``C1``, ``C2``, and so on.
- Because all solutions should be mathematically equivalent, some
hints may return the exact same result for an ODE. Often, though,
two different hints will return the same solution formatted
differently. The two should be equivalent. Also note that sometimes
the values of the arbitrary constants in two different solutions may
not be the same, because one constant may have "absorbed" other
constants into it.
- Do ``help(ode.ode_<hintname>)`` to get help more information on a
specific hint, where ``<hintname>`` is the name of a hint without
``_Integral``.
For system of ordinary differential equations
=============================================
**Usage**
``dsolve(eq, func)`` -> Solve a system of ordinary differential
equations ``eq`` for ``func`` being list of functions including
`x(t)`, `y(t)`, `z(t)` where number of functions in the list depends
upon the number of equations provided in ``eq``.
**Details**
``eq`` can be any supported system of ordinary differential equations
This can either be an :py:class:`~sympy.core.relational.Equality`,
or an expression, which is assumed to be equal to ``0``.
``func`` holds ``x(t)`` and ``y(t)`` being functions of one variable which
together with some of their derivatives make up the system of ordinary
differential equation ``eq``. It is not necessary to provide this; it
will be autodetected (and an error raised if it couldn't be detected).
**Hints**
The hints are formed by parameters returned by classify_sysode, combining
them give hints name used later for forming method name.
Examples
========
>>> from sympy import Function, dsolve, Eq, Derivative, sin, cos, symbols
>>> from sympy.abc import x
>>> f = Function('f')
>>> dsolve(Derivative(f(x), x, x) + 9*f(x), f(x))
Eq(f(x), C1*sin(3*x) + C2*cos(3*x))
>>> eq = sin(x)*cos(f(x)) + cos(x)*sin(f(x))*f(x).diff(x)
>>> dsolve(eq, hint='1st_exact')
[Eq(f(x), -acos(C1/cos(x)) + 2*pi), Eq(f(x), acos(C1/cos(x)))]
>>> dsolve(eq, hint='almost_linear')
[Eq(f(x), -acos(C1/cos(x)) + 2*pi), Eq(f(x), acos(C1/cos(x)))]
>>> t = symbols('t')
>>> x, y = symbols('x, y', cls=Function)
>>> eq = (Eq(Derivative(x(t),t), 12*t*x(t) + 8*y(t)), Eq(Derivative(y(t),t), 21*x(t) + 7*t*y(t)))
>>> dsolve(eq)
[Eq(x(t), C1*x0(t) + C2*x0(t)*Integral(8*exp(Integral(7*t, t))*exp(Integral(12*t, t))/x0(t)**2, t)),
Eq(y(t), C1*y0(t) + C2*(y0(t)*Integral(8*exp(Integral(7*t, t))*exp(Integral(12*t, t))/x0(t)**2, t) +
exp(Integral(7*t, t))*exp(Integral(12*t, t))/x0(t)))]
>>> eq = (Eq(Derivative(x(t),t),x(t)*y(t)*sin(t)), Eq(Derivative(y(t),t),y(t)**2*sin(t)))
>>> dsolve(eq)
{Eq(x(t), -exp(C1)/(C2*exp(C1) - cos(t))), Eq(y(t), -1/(C1 - cos(t)))}
"""
if iterable(eq):
match = classify_sysode(eq, func)
eq = match['eq']
order = match['order']
func = match['func']
t = list(list(eq[0].atoms(Derivative))[0].atoms(Symbol))[0]
# keep highest order term coefficient positive
for i in range(len(eq)):
for func_ in func:
if isinstance(func_, list):
pass
else:
if eq[i].coeff(diff(func[i],t,ode_order(eq[i], func[i]))).is_negative:
eq[i] = -eq[i]
match['eq'] = eq
if len(set(order.values()))!=1:
raise ValueError("It solves only those systems of equations whose orders are equal")
match['order'] = list(order.values())[0]
def recur_len(l):
return sum(recur_len(item) if isinstance(item,list) else 1 for item in l)
if recur_len(func) != len(eq):
raise ValueError("dsolve() and classify_sysode() work with "
"number of functions being equal to number of equations")
if match['type_of_equation'] is None:
raise NotImplementedError
else:
if match['is_linear'] == True:
if match['no_of_equation'] > 3:
solvefunc = globals()['sysode_linear_neq_order%(order)s' % match]
else:
solvefunc = globals()['sysode_linear_%(no_of_equation)seq_order%(order)s' % match]
else:
solvefunc = globals()['sysode_nonlinear_%(no_of_equation)seq_order%(order)s' % match]
sols = solvefunc(match)
if ics:
constants = Tuple(*sols).free_symbols - Tuple(*eq).free_symbols
solved_constants = solve_ics(sols, func, constants, ics)
return [sol.subs(solved_constants) for sol in sols]
return sols
else:
given_hint = hint # hint given by the user
# See the docstring of _desolve for more details.
hints = _desolve(eq, func=func,
hint=hint, simplify=True, xi=xi, eta=eta, type='ode', ics=ics,
x0=x0, n=n, **kwargs)
eq = hints.pop('eq', eq)
all_ = hints.pop('all', False)
if all_:
retdict = {}
failed_hints = {}
gethints = classify_ode(eq, dict=True)
orderedhints = gethints['ordered_hints']
for hint in hints:
try:
rv = _helper_simplify(eq, hint, hints[hint], simplify)
except NotImplementedError as detail:
failed_hints[hint] = detail
else:
retdict[hint] = rv
func = hints[hint]['func']
retdict['best'] = min(list(retdict.values()), key=lambda x:
ode_sol_simplicity(x, func, trysolving=not simplify))
if given_hint == 'best':
return retdict['best']
for i in orderedhints:
if retdict['best'] == retdict.get(i, None):
retdict['best_hint'] = i
break
retdict['default'] = gethints['default']
retdict['order'] = gethints['order']
retdict.update(failed_hints)
return retdict
else:
# The key 'hint' stores the hint needed to be solved for.
hint = hints['hint']
return _helper_simplify(eq, hint, hints, simplify, ics=ics)
def _helper_simplify(eq, hint, match, simplify=True, ics=None, **kwargs):
r"""
Helper function of dsolve that calls the respective
:py:mod:`~sympy.solvers.ode` functions to solve for the ordinary
differential equations. This minimizes the computation in calling
:py:meth:`~sympy.solvers.deutils._desolve` multiple times.
"""
r = match
if hint.endswith('_Integral'):
solvefunc = globals()['ode_' + hint[:-len('_Integral')]]
else:
solvefunc = globals()['ode_' + hint]
func = r['func']
order = r['order']
match = r[hint]
free = eq.free_symbols
cons = lambda s: s.free_symbols.difference(free)
if simplify:
# odesimp() will attempt to integrate, if necessary, apply constantsimp(),
# attempt to solve for func, and apply any other hint specific
# simplifications
sols = solvefunc(eq, func, order, match)
if isinstance(sols, Expr):
rv = odesimp(eq, sols, func, hint)
else:
rv = [odesimp(eq, s, func, hint) for s in sols]
else:
# We still want to integrate (you can disable it separately with the hint)
match['simplify'] = False # Some hints can take advantage of this option
exprs = solvefunc(eq, func, order, match)
if isinstance(exprs, list):
rv = [_handle_Integral(expr, func, hint) for expr in exprs]
else:
rv = _handle_Integral(exprs, func, hint)
if isinstance(rv, list):
rv = _remove_redundant_solutions(eq, rv, order, func.args[0])
if len(rv) == 1:
rv = rv[0]
if ics and not 'power_series' in hint:
if isinstance(rv, Expr):
solved_constants = solve_ics([rv], [r['func']], cons(rv), ics)
rv = rv.subs(solved_constants)
else:
rv1 = []
for s in rv:
try:
solved_constants = solve_ics([s], [r['func']], cons(s), ics)
except ValueError:
continue
rv1.append(s.subs(solved_constants))
if len(rv1) == 1:
return rv1[0]
rv = rv1
return rv
def solve_ics(sols, funcs, constants, ics):
"""
Solve for the constants given initial conditions
``sols`` is a list of solutions.
``funcs`` is a list of functions.
``constants`` is a list of constants.
``ics`` is the set of initial/boundary conditions for the differential
equation. It should be given in the form of ``{f(x0): x1,
f(x).diff(x).subs(x, x2): x3}`` and so on.
Returns a dictionary mapping constants to values.
``solution.subs(constants)`` will replace the constants in ``solution``.
Example
=======
>>> # From dsolve(f(x).diff(x) - f(x), f(x))
>>> from sympy import symbols, Eq, exp, Function
>>> from sympy.solvers.ode import solve_ics
>>> f = Function('f')
>>> x, C1 = symbols('x C1')
>>> sols = [Eq(f(x), C1*exp(x))]
>>> funcs = [f(x)]
>>> constants = [C1]
>>> ics = {f(0): 2}
>>> solved_constants = solve_ics(sols, funcs, constants, ics)
>>> solved_constants
{C1: 2}
>>> sols[0].subs(solved_constants)
Eq(f(x), 2*exp(x))
"""
# Assume ics are of the form f(x0): value or Subs(diff(f(x), x, n), (x,
# x0)): value (currently checked by classify_ode). To solve, replace x
# with x0, f(x0) with value, then solve for constants. For f^(n)(x0),
# differentiate the solution n times, so that f^(n)(x) appears.
x = funcs[0].args[0]
diff_sols = []
subs_sols = []
diff_variables = set()
for funcarg, value in ics.items():
if isinstance(funcarg, AppliedUndef):
x0 = funcarg.args[0]
matching_func = [f for f in funcs if f.func == funcarg.func][0]
S = sols
elif isinstance(funcarg, (Subs, Derivative)):
if isinstance(funcarg, Subs):
# Make sure it stays a subs. Otherwise subs below will produce
# a different looking term.
funcarg = funcarg.doit()
if isinstance(funcarg, Subs):
deriv = funcarg.expr
x0 = funcarg.point[0]
variables = funcarg.expr.variables
matching_func = deriv
elif isinstance(funcarg, Derivative):
deriv = funcarg
x0 = funcarg.variables[0]
variables = (x,)*len(funcarg.variables)
matching_func = deriv.subs(x0, x)
if variables not in diff_variables:
for sol in sols:
if sol.has(deriv.expr.func):
diff_sols.append(Eq(sol.lhs.diff(*variables), sol.rhs.diff(*variables)))
diff_variables.add(variables)
S = diff_sols
else:
raise NotImplementedError("Unrecognized initial condition")
for sol in S:
if sol.has(matching_func):
sol2 = sol
sol2 = sol2.subs(x, x0)
sol2 = sol2.subs(funcarg, value)
# This check is necessary because of issue #15724
if not isinstance(sol2, BooleanAtom) or not subs_sols:
subs_sols = [s for s in subs_sols if not isinstance(s, BooleanAtom)]
subs_sols.append(sol2)
# TODO: Use solveset here
try:
solved_constants = solve(subs_sols, constants, dict=True)
except NotImplementedError:
solved_constants = []
# XXX: We can't differentiate between the solution not existing because of
# invalid initial conditions, and not existing because solve is not smart
# enough. If we could use solveset, this might be improvable, but for now,
# we use NotImplementedError in this case.
if not solved_constants:
raise ValueError("Couldn't solve for initial conditions")
if solved_constants == True:
raise ValueError("Initial conditions did not produce any solutions for constants. Perhaps they are degenerate.")
if len(solved_constants) > 1:
raise NotImplementedError("Initial conditions produced too many solutions for constants")
return solved_constants[0]
def classify_ode(eq, func=None, dict=False, ics=None, **kwargs):
r"""
Returns a tuple of possible :py:meth:`~sympy.solvers.ode.dsolve`
classifications for an ODE.
The tuple is ordered so that first item is the classification that
:py:meth:`~sympy.solvers.ode.dsolve` uses to solve the ODE by default. In
general, classifications at the near the beginning of the list will
produce better solutions faster than those near the end, thought there are
always exceptions. To make :py:meth:`~sympy.solvers.ode.dsolve` use a
different classification, use ``dsolve(ODE, func,
hint=<classification>)``. See also the
:py:meth:`~sympy.solvers.ode.dsolve` docstring for different meta-hints
you can use.
If ``dict`` is true, :py:meth:`~sympy.solvers.ode.classify_ode` will
return a dictionary of ``hint:match`` expression terms. This is intended
for internal use by :py:meth:`~sympy.solvers.ode.dsolve`. Note that
because dictionaries are ordered arbitrarily, this will most likely not be
in the same order as the tuple.
You can get help on different hints by executing
``help(ode.ode_hintname)``, where ``hintname`` is the name of the hint
without ``_Integral``.
See :py:data:`~sympy.solvers.ode.allhints` or the
:py:mod:`~sympy.solvers.ode` docstring for a list of all supported hints
that can be returned from :py:meth:`~sympy.solvers.ode.classify_ode`.
Notes
=====
These are remarks on hint names.
``_Integral``
If a classification has ``_Integral`` at the end, it will return the
expression with an unevaluated :py:class:`~sympy.integrals.Integral`
class in it. Note that a hint may do this anyway if
:py:meth:`~sympy.core.expr.Expr.integrate` cannot do the integral,
though just using an ``_Integral`` will do so much faster. Indeed, an
``_Integral`` hint will always be faster than its corresponding hint
without ``_Integral`` because
:py:meth:`~sympy.core.expr.Expr.integrate` is an expensive routine.
If :py:meth:`~sympy.solvers.ode.dsolve` hangs, it is probably because
:py:meth:`~sympy.core.expr.Expr.integrate` is hanging on a tough or
impossible integral. Try using an ``_Integral`` hint or
``all_Integral`` to get it return something.
Note that some hints do not have ``_Integral`` counterparts. This is
because :py:meth:`~sympy.solvers.ode.integrate` is not used in solving
the ODE for those method. For example, `n`\th order linear homogeneous
ODEs with constant coefficients do not require integration to solve,
so there is no ``nth_linear_homogeneous_constant_coeff_Integrate``
hint. You can easily evaluate any unevaluated
:py:class:`~sympy.integrals.Integral`\s in an expression by doing
``expr.doit()``.
Ordinals
Some hints contain an ordinal such as ``1st_linear``. This is to help
differentiate them from other hints, as well as from other methods
that may not be implemented yet. If a hint has ``nth`` in it, such as
the ``nth_linear`` hints, this means that the method used to applies
to ODEs of any order.
``indep`` and ``dep``
Some hints contain the words ``indep`` or ``dep``. These reference
the independent variable and the dependent function, respectively. For
example, if an ODE is in terms of `f(x)`, then ``indep`` will refer to
`x` and ``dep`` will refer to `f`.
``subs``
If a hints has the word ``subs`` in it, it means the the ODE is solved
by substituting the expression given after the word ``subs`` for a
single dummy variable. This is usually in terms of ``indep`` and
``dep`` as above. The substituted expression will be written only in
characters allowed for names of Python objects, meaning operators will
be spelled out. For example, ``indep``/``dep`` will be written as
``indep_div_dep``.
``coeff``
The word ``coeff`` in a hint refers to the coefficients of something
in the ODE, usually of the derivative terms. See the docstring for
the individual methods for more info (``help(ode)``). This is
contrast to ``coefficients``, as in ``undetermined_coefficients``,
which refers to the common name of a method.
``_best``
Methods that have more than one fundamental way to solve will have a
hint for each sub-method and a ``_best`` meta-classification. This
will evaluate all hints and return the best, using the same
considerations as the normal ``best`` meta-hint.
Examples
========
>>> from sympy import Function, classify_ode, Eq
>>> from sympy.abc import x
>>> f = Function('f')
>>> classify_ode(Eq(f(x).diff(x), 0), f(x))
('nth_algebraic', 'separable', '1st_linear', '1st_homogeneous_coeff_best',
'1st_homogeneous_coeff_subs_indep_div_dep',
'1st_homogeneous_coeff_subs_dep_div_indep',
'1st_power_series', 'lie_group',
'nth_linear_constant_coeff_homogeneous',
'nth_linear_euler_eq_homogeneous', 'nth_algebraic_Integral',
'separable_Integral', '1st_linear_Integral',
'1st_homogeneous_coeff_subs_indep_div_dep_Integral',
'1st_homogeneous_coeff_subs_dep_div_indep_Integral')
>>> classify_ode(f(x).diff(x, 2) + 3*f(x).diff(x) + 2*f(x) - 4)
('nth_linear_constant_coeff_undetermined_coefficients',
'nth_linear_constant_coeff_variation_of_parameters',
'nth_linear_constant_coeff_variation_of_parameters_Integral')
"""
ics = sympify(ics)
prep = kwargs.pop('prep', True)
if func and len(func.args) != 1:
raise ValueError("dsolve() and classify_ode() only "
"work with functions of one variable, not %s" % func)
# Some methods want the unprocessed equation
eq_orig = eq
if prep or func is None:
eq, func_ = _preprocess(eq, func)
if func is None:
func = func_
x = func.args[0]
f = func.func
y = Dummy('y')
xi = kwargs.get('xi')
eta = kwargs.get('eta')
terms = kwargs.get('n')
if isinstance(eq, Equality):
if eq.rhs != 0:
return classify_ode(eq.lhs - eq.rhs, func, dict=dict, ics=ics, xi=xi,
n=terms, eta=eta, prep=False)
eq = eq.lhs
order = ode_order(eq, f(x))
# hint:matchdict or hint:(tuple of matchdicts)
# Also will contain "default":<default hint> and "order":order items.
matching_hints = {"order": order}
df = f(x).diff(x)
a = Wild('a', exclude=[f(x)])
b = Wild('b', exclude=[f(x)])
c = Wild('c', exclude=[f(x)])
d = Wild('d', exclude=[df, f(x).diff(x, 2)])
e = Wild('e', exclude=[df])
k = Wild('k', exclude=[df])
n = Wild('n', exclude=[x, f(x), df])
c1 = Wild('c1', exclude=[x])
a2 = Wild('a2', exclude=[x, f(x), df])
b2 = Wild('b2', exclude=[x, f(x), df])
c2 = Wild('c2', exclude=[x, f(x), df])
d2 = Wild('d2', exclude=[x, f(x), df])
a3 = Wild('a3', exclude=[f(x), df, f(x).diff(x, 2)])
b3 = Wild('b3', exclude=[f(x), df, f(x).diff(x, 2)])
c3 = Wild('c3', exclude=[f(x), df, f(x).diff(x, 2)])
r3 = {'xi': xi, 'eta': eta} # Used for the lie_group hint
boundary = {} # Used to extract initial conditions
C1 = Symbol("C1")
# Preprocessing to get the initial conditions out
if ics is not None:
for funcarg in ics:
# Separating derivatives
if isinstance(funcarg, (Subs, Derivative)):
# f(x).diff(x).subs(x, 0) is a Subs, but f(x).diff(x).subs(x,
# y) is a Derivative
if isinstance(funcarg, Subs):
deriv = funcarg.expr
old = funcarg.variables[0]
new = funcarg.point[0]
elif isinstance(funcarg, Derivative):
deriv = funcarg
# No information on this. Just assume it was x
old = x
new = funcarg.variables[0]
if (isinstance(deriv, Derivative) and isinstance(deriv.args[0],
AppliedUndef) and deriv.args[0].func == f and
len(deriv.args[0].args) == 1 and old == x and not
new.has(x) and all(i == deriv.variables[0] for i in
deriv.variables) and not ics[funcarg].has(f)):
dorder = ode_order(deriv, x)
temp = 'f' + str(dorder)
boundary.update({temp: new, temp + 'val': ics[funcarg]})
else:
raise ValueError("Enter valid boundary conditions for Derivatives")
# Separating functions
elif isinstance(funcarg, AppliedUndef):
if (funcarg.func == f and len(funcarg.args) == 1 and
not funcarg.args[0].has(x) and not ics[funcarg].has(f)):
boundary.update({'f0': funcarg.args[0], 'f0val': ics[funcarg]})
else:
raise ValueError("Enter valid boundary conditions for Function")
else:
raise ValueError("Enter boundary conditions of the form ics={f(point}: value, f(x).diff(x, order).subs(x, point): value}")
# Factorable method
r = _ode_factorable_match(eq, func, kwargs.get('x0', 0))
if r:
matching_hints['factorable'] = r
# Any ODE that can be solved with a combination of algebra and
# integrals e.g.:
# d^3/dx^3(x y) = F(x)
r = _nth_algebraic_match(eq_orig, func)
if r['solutions']:
matching_hints['nth_algebraic'] = r
matching_hints['nth_algebraic_Integral'] = r
eq = expand(eq)
# Precondition to try remove f(x) from highest order derivative
reduced_eq = None
if eq.is_Add:
deriv_coef = eq.coeff(f(x).diff(x, order))
if deriv_coef not in (1, 0):
r = deriv_coef.match(a*f(x)**c1)
if r and r[c1]:
den = f(x)**r[c1]
reduced_eq = Add(*[arg/den for arg in eq.args])
if not reduced_eq:
reduced_eq = eq
if order == 1:
## Linear case: a(x)*y'+b(x)*y+c(x) == 0
if eq.is_Add:
ind, dep = reduced_eq.as_independent(f)
else:
u = Dummy('u')
ind, dep = (reduced_eq + u).as_independent(f)
ind, dep = [tmp.subs(u, 0) for tmp in [ind, dep]]
r = {a: dep.coeff(df),
b: dep.coeff(f(x)),
c: ind}
# double check f[a] since the preconditioning may have failed
if not r[a].has(f) and not r[b].has(f) and (
r[a]*df + r[b]*f(x) + r[c]).expand() - reduced_eq == 0:
r['a'] = a
r['b'] = b
r['c'] = c
matching_hints["1st_linear"] = r
matching_hints["1st_linear_Integral"] = r
## Bernoulli case: a(x)*y'+b(x)*y+c(x)*y**n == 0
r = collect(
reduced_eq, f(x), exact=True).match(a*df + b*f(x) + c*f(x)**n)
if r and r[c] != 0 and r[n] != 1: # See issue 4676
r['a'] = a
r['b'] = b
r['c'] = c
r['n'] = n
matching_hints["Bernoulli"] = r
matching_hints["Bernoulli_Integral"] = r
## Riccati special n == -2 case: a2*y'+b2*y**2+c2*y/x+d2/x**2 == 0
r = collect(reduced_eq,
f(x), exact=True).match(a2*df + b2*f(x)**2 + c2*f(x)/x + d2/x**2)
if r and r[b2] != 0 and (r[c2] != 0 or r[d2] != 0):
r['a2'] = a2
r['b2'] = b2
r['c2'] = c2
r['d2'] = d2
matching_hints["Riccati_special_minus2"] = r
# NON-REDUCED FORM OF EQUATION matches
r = collect(eq, df, exact=True).match(d + e * df)
if r:
r['d'] = d
r['e'] = e
r['y'] = y
r[d] = r[d].subs(f(x), y)
r[e] = r[e].subs(f(x), y)
# FIRST ORDER POWER SERIES WHICH NEEDS INITIAL CONDITIONS
# TODO: Hint first order series should match only if d/e is analytic.
# For now, only d/e and (d/e).diff(arg) is checked for existence at
# at a given point.
# This is currently done internally in ode_1st_power_series.
point = boundary.get('f0', 0)
value = boundary.get('f0val', C1)
check = cancel(r[d]/r[e])
check1 = check.subs({x: point, y: value})
if not check1.has(oo) and not check1.has(zoo) and \
not check1.has(NaN) and not check1.has(-oo):
check2 = (check1.diff(x)).subs({x: point, y: value})
if not check2.has(oo) and not check2.has(zoo) and \
not check2.has(NaN) and not check2.has(-oo):
rseries = r.copy()
rseries.update({'terms': terms, 'f0': point, 'f0val': value})
matching_hints["1st_power_series"] = rseries
r3.update(r)
## Exact Differential Equation: P(x, y) + Q(x, y)*y' = 0 where
# dP/dy == dQ/dx
try:
if r[d] != 0:
numerator = simplify(r[d].diff(y) - r[e].diff(x))
# The following few conditions try to convert a non-exact
# differential equation into an exact one.
# References : Differential equations with applications
# and historical notes - George E. Simmons
if numerator:
# If (dP/dy - dQ/dx) / Q = f(x)
# then exp(integral(f(x))*equation becomes exact
factor = simplify(numerator/r[e])
variables = factor.free_symbols
if len(variables) == 1 and x == variables.pop():
factor = exp(Integral(factor).doit())
r[d] *= factor
r[e] *= factor
matching_hints["1st_exact"] = r
matching_hints["1st_exact_Integral"] = r
else:
# If (dP/dy - dQ/dx) / -P = f(y)
# then exp(integral(f(y))*equation becomes exact
factor = simplify(-numerator/r[d])
variables = factor.free_symbols
if len(variables) == 1 and y == variables.pop():
factor = exp(Integral(factor).doit())
r[d] *= factor
r[e] *= factor
matching_hints["1st_exact"] = r
matching_hints["1st_exact_Integral"] = r
else:
matching_hints["1st_exact"] = r
matching_hints["1st_exact_Integral"] = r
except NotImplementedError:
# Differentiating the coefficients might fail because of things
# like f(2*x).diff(x). See issue 4624 and issue 4719.
pass
# Any first order ODE can be ideally solved by the Lie Group
# method
matching_hints["lie_group"] = r3
# This match is used for several cases below; we now collect on
# f(x) so the matching works.
r = collect(reduced_eq, df, exact=True).match(d + e*df)
if r:
# Using r[d] and r[e] without any modification for hints
# linear-coefficients and separable-reduced.
num, den = r[d], r[e] # ODE = d/e + df
r['d'] = d
r['e'] = e
r['y'] = y
r[d] = num.subs(f(x), y)
r[e] = den.subs(f(x), y)
## Separable Case: y' == P(y)*Q(x)
r[d] = separatevars(r[d])
r[e] = separatevars(r[e])
# m1[coeff]*m1[x]*m1[y] + m2[coeff]*m2[x]*m2[y]*y'
m1 = separatevars(r[d], dict=True, symbols=(x, y))
m2 = separatevars(r[e], dict=True, symbols=(x, y))
if m1 and m2:
r1 = {'m1': m1, 'm2': m2, 'y': y}
matching_hints["separable"] = r1
matching_hints["separable_Integral"] = r1
## First order equation with homogeneous coefficients:
# dy/dx == F(y/x) or dy/dx == F(x/y)
ordera = homogeneous_order(r[d], x, y)
if ordera is not None:
orderb = homogeneous_order(r[e], x, y)
if ordera == orderb:
# u1=y/x and u2=x/y
u1 = Dummy('u1')
u2 = Dummy('u2')
s = "1st_homogeneous_coeff_subs"
s1 = s + "_dep_div_indep"
s2 = s + "_indep_div_dep"
if simplify((r[d] + u1*r[e]).subs({x: 1, y: u1})) != 0:
matching_hints[s1] = r
matching_hints[s1 + "_Integral"] = r
if simplify((r[e] + u2*r[d]).subs({x: u2, y: 1})) != 0:
matching_hints[s2] = r
matching_hints[s2 + "_Integral"] = r
if s1 in matching_hints and s2 in matching_hints:
matching_hints["1st_homogeneous_coeff_best"] = r
## Linear coefficients of the form
# y'+ F((a*x + b*y + c)/(a'*x + b'y + c')) = 0
# that can be reduced to homogeneous form.
F = num/den
params = _linear_coeff_match(F, func)
if params:
xarg, yarg = params
u = Dummy('u')
t = Dummy('t')
# Dummy substitution for df and f(x).
dummy_eq = reduced_eq.subs(((df, t), (f(x), u)))
reps = ((x, x + xarg), (u, u + yarg), (t, df), (u, f(x)))
dummy_eq = simplify(dummy_eq.subs(reps))
# get the re-cast values for e and d
r2 = collect(expand(dummy_eq), [df, f(x)]).match(e*df + d)
if r2:
orderd = homogeneous_order(r2[d], x, f(x))
if orderd is not None:
ordere = homogeneous_order(r2[e], x, f(x))
if orderd == ordere:
# Match arguments are passed in such a way that it
# is coherent with the already existing homogeneous
# functions.
r2[d] = r2[d].subs(f(x), y)
r2[e] = r2[e].subs(f(x), y)
r2.update({'xarg': xarg, 'yarg': yarg,
'd': d, 'e': e, 'y': y})
matching_hints["linear_coefficients"] = r2
matching_hints["linear_coefficients_Integral"] = r2
## Equation of the form y' + (y/x)*H(x^n*y) = 0
# that can be reduced to separable form
factor = simplify(x/f(x)*num/den)
# Try representing factor in terms of x^n*y
# where n is lowest power of x in factor;
# first remove terms like sqrt(2)*3 from factor.atoms(Mul)
u = None
for mul in ordered(factor.atoms(Mul)):
if mul.has(x):
_, u = mul.as_independent(x, f(x))
break
if u and u.has(f(x)):
h = x**(degree(Poly(u.subs(f(x), y), gen=x)))*f(x)
p = Wild('p')
if (u/h == 1) or ((u/h).simplify().match(x**p)):
t = Dummy('t')
r2 = {'t': t}
xpart, ypart = u.as_independent(f(x))
test = factor.subs(((u, t), (1/u, 1/t)))
free = test.free_symbols
if len(free) == 1 and free.pop() == t:
r2.update({'power': xpart.as_base_exp()[1], 'u': test})
matching_hints["separable_reduced"] = r2
matching_hints["separable_reduced_Integral"] = r2
## Almost-linear equation of the form f(x)*g(y)*y' + k(x)*l(y) + m(x) = 0
r = collect(eq, [df, f(x)]).match(e*df + d)
if r:
r2 = r.copy()
r2[c] = S.Zero
if r2[d].is_Add:
# Separate the terms having f(x) to r[d] and
# remaining to r[c]
no_f, r2[d] = r2[d].as_independent(f(x))
r2[c] += no_f
factor = simplify(r2[d].diff(f(x))/r[e])
if factor and not factor.has(f(x)):
r2[d] = factor_terms(r2[d])
u = r2[d].as_independent(f(x), as_Add=False)[1]
r2.update({'a': e, 'b': d, 'c': c, 'u': u})
r2[d] /= u
r2[e] /= u.diff(f(x))
matching_hints["almost_linear"] = r2
matching_hints["almost_linear_Integral"] = r2
elif order == 2:
# Liouville ODE in the form
# f(x).diff(x, 2) + g(f(x))*(f(x).diff(x))**2 + h(x)*f(x).diff(x)
# See Goldstein and Braun, "Advanced Methods for the Solution of
# Differential Equations", pg. 98
s = d*f(x).diff(x, 2) + e*df**2 + k*df
r = reduced_eq.match(s)
if r and r[d] != 0:
y = Dummy('y')
g = simplify(r[e]/r[d]).subs(f(x), y)
h = simplify(r[k]/r[d]).subs(f(x), y)
if y in h.free_symbols or x in g.free_symbols:
pass
else:
r = {'g': g, 'h': h, 'y': y}
matching_hints["Liouville"] = r
matching_hints["Liouville_Integral"] = r
# Homogeneous second order differential equation of the form
# a3*f(x).diff(x, 2) + b3*f(x).diff(x) + c3
# It has a definite power series solution at point x0 if, b3/a3 and c3/a3
# are analytic at x0.
deq = a3*(f(x).diff(x, 2)) + b3*df + c3*f(x)
r = collect(reduced_eq,
[f(x).diff(x, 2), f(x).diff(x), f(x)]).match(deq)
ordinary = False
if r:
if not all([r[key].is_polynomial() for key in r]):
n, d = reduced_eq.as_numer_denom()
reduced_eq = expand(n)
r = collect(reduced_eq,
[f(x).diff(x, 2), f(x).diff(x), f(x)]).match(deq)
if r and r[a3] != 0:
p = cancel(r[b3]/r[a3]) # Used below
q = cancel(r[c3]/r[a3]) # Used below
point = kwargs.get('x0', 0)
check = p.subs(x, point)
if not check.has(oo, NaN, zoo, -oo):
check = q.subs(x, point)
if not check.has(oo, NaN, zoo, -oo):
ordinary = True
r.update({'a3': a3, 'b3': b3, 'c3': c3, 'x0': point, 'terms': terms})
matching_hints["2nd_power_series_ordinary"] = r
# Checking if the differential equation has a regular singular point
# at x0. It has a regular singular point at x0, if (b3/a3)*(x - x0)
# and (c3/a3)*((x - x0)**2) are analytic at x0.
if not ordinary:
p = cancel((x - point)*p)
check = p.subs(x, point)
if not check.has(oo, NaN, zoo, -oo):
q = cancel(((x - point)**2)*q)
check = q.subs(x, point)
if not check.has(oo, NaN, zoo, -oo):
coeff_dict = {'p': p, 'q': q, 'x0': point, 'terms': terms}
matching_hints["2nd_power_series_regular"] = coeff_dict
# If the ODE has regular singular point at x0 and is of the form
# Eq((x)**2*Derivative(y(x), x, x) + x*Derivative(y(x), x) +
# (a4**2*x**(2*p)-n**2)*y(x) thus Bessel's equation
rn = match_2nd_linear_bessel(r, f(x))
if rn:
matching_hints["2nd_linear_bessel"] = rn
# If the ODE is ordinary and is of the form of Airy's Equation
# Eq(x**2*Derivative(y(x),x,x)-(ax+b)*y(x))
if p.is_zero:
a4 = Wild('a4', exclude=[x,f(x),df])
b4 = Wild('b4', exclude=[x,f(x),df])
rn = q.match(a4+b4*x)
if rn and rn[b4] != 0:
rn = {'b':rn[a4],'m':rn[b4]}
matching_hints["2nd_linear_airy"] = rn
if order > 0:
# Any ODE that can be solved with a substitution and
# repeated integration e.g.:
# `d^2/dx^2(y) + x*d/dx(y) = constant
#f'(x) must be finite for this to work
r = _nth_order_reducible_match(reduced_eq, func)
if r:
matching_hints['nth_order_reducible'] = r
# nth order linear ODE
# a_n(x)y^(n) + ... + a_1(x)y' + a_0(x)y = F(x) = b
r = _nth_linear_match(reduced_eq, func, order)
# Constant coefficient case (a_i is constant for all i)
if r and not any(r[i].has(x) for i in r if i >= 0):
# Inhomogeneous case: F(x) is not identically 0
if r[-1]:
undetcoeff = _undetermined_coefficients_match(r[-1], x)
s = "nth_linear_constant_coeff_variation_of_parameters"
matching_hints[s] = r
matching_hints[s + "_Integral"] = r
if undetcoeff['test']:
r['trialset'] = undetcoeff['trialset']
matching_hints[
"nth_linear_constant_coeff_undetermined_coefficients"
] = r
# Homogeneous case: F(x) is identically 0
else:
matching_hints["nth_linear_constant_coeff_homogeneous"] = r
# nth order Euler equation a_n*x**n*y^(n) + ... + a_1*x*y' + a_0*y = F(x)
#In case of Homogeneous euler equation F(x) = 0
def _test_term(coeff, order):
r"""
Linear Euler ODEs have the form K*x**order*diff(y(x),x,order) = F(x),
where K is independent of x and y(x), order>= 0.
So we need to check that for each term, coeff == K*x**order from
some K. We have a few cases, since coeff may have several
different types.
"""
if order < 0:
raise ValueError("order should be greater than 0")
if coeff == 0:
return True
if order == 0:
if x in coeff.free_symbols:
return False
return True
if coeff.is_Mul:
if coeff.has(f(x)):
return False
return x**order in coeff.args
elif coeff.is_Pow:
return coeff.as_base_exp() == (x, order)
elif order == 1:
return x == coeff
return False
# Find coefficient for highest derivative, multiply coefficients to
# bring the equation into Euler form if possible
r_rescaled = None
if r is not None:
coeff = r[order]
factor = x**order / coeff
r_rescaled = {i: factor*r[i] for i in r}
if r_rescaled and not any(not _test_term(r_rescaled[i], i) for i in
r_rescaled if i != 'trialset' and i >= 0):
if not r_rescaled[-1]:
matching_hints["nth_linear_euler_eq_homogeneous"] = r_rescaled
else:
matching_hints["nth_linear_euler_eq_nonhomogeneous_variation_of_parameters"] = r_rescaled
matching_hints["nth_linear_euler_eq_nonhomogeneous_variation_of_parameters_Integral"] = r_rescaled
e, re = posify(r_rescaled[-1].subs(x, exp(x)))
undetcoeff = _undetermined_coefficients_match(e.subs(re), x)
if undetcoeff['test']:
r_rescaled['trialset'] = undetcoeff['trialset']
matching_hints["nth_linear_euler_eq_nonhomogeneous_undetermined_coefficients"] = r_rescaled
# Order keys based on allhints.
retlist = [i for i in allhints if i in matching_hints]
if dict:
# Dictionaries are ordered arbitrarily, so make note of which
# hint would come first for dsolve(). Use an ordered dict in Py 3.
matching_hints["default"] = retlist[0] if retlist else None
matching_hints["ordered_hints"] = tuple(retlist)
return matching_hints
else:
return tuple(retlist)
def match_2nd_linear_bessel(r, func):
from sympy.polys.polytools import factor
# eq = a3*f(x).diff(x, 2) + b3*f(x).diff(x) + c3*f(x)
f = func
x = func.args[0]
df = f.diff(x)
a = Wild('a', exclude=[f,df])
b = Wild('b', exclude=[x, f,df])
a4 = Wild('a4', exclude=[x,f,df])
b4 = Wild('b4', exclude=[x,f,df])
c4 = Wild('c4', exclude=[x,f,df])
d4 = Wild('d4', exclude=[x,f,df])
a3 = Wild('a3', exclude=[f, df, f.diff(x, 2)])
b3 = Wild('b3', exclude=[f, df, f.diff(x, 2)])
c3 = Wild('c3', exclude=[f, df, f.diff(x, 2)])
# leading coeff of f(x).diff(x, 2)
coeff = factor(r[a3]).match(a4*(x-b)**b4)
if coeff:
# if coeff[b4] = 0 means constant coefficient
if coeff[b4] == 0:
return None
point = coeff[b]
else:
return None
if point:
r[a3] = simplify(r[a3].subs(x, x+point))
r[b3] = simplify(r[b3].subs(x, x+point))
r[c3] = simplify(r[c3].subs(x, x+point))
# making a3 in the form of x**2
r[a3] = cancel(r[a3]/(coeff[a4]*(x)**(-2+coeff[b4])))
r[b3] = cancel(r[b3]/(coeff[a4]*(x)**(-2+coeff[b4])))
r[c3] = cancel(r[c3]/(coeff[a4]*(x)**(-2+coeff[b4])))
# checking if b3 is of form c*(x-b)
coeff1 = factor(r[b3]).match(a4*(x))
if coeff1 is None:
return None
# c3 maybe of very complex form so I am simply checking (a - b) form
# if yes later I will match with the standerd form of bessel in a and b
# a, b are wild variable defined above.
_coeff2 = r[c3].match(a - b)
if _coeff2 is None:
return None
# matching with standerd form for c3
coeff2 = factor(_coeff2[a]).match(c4**2*(x)**(2*a4))
if coeff2 is None:
return None
if _coeff2[b] == 0:
coeff2[d4] = 0
else:
coeff2[d4] = factor(_coeff2[b]).match(d4**2)[d4]
rn = {'n':coeff2[d4], 'a4':coeff2[c4], 'd4':coeff2[a4]}
rn['c4'] = coeff1[a4]
rn['b4'] = point
return rn
def classify_sysode(eq, funcs=None, **kwargs):
r"""
Returns a dictionary of parameter names and values that define the system
of ordinary differential equations in ``eq``.
The parameters are further used in
:py:meth:`~sympy.solvers.ode.dsolve` for solving that system.
The parameter names and values are:
'is_linear' (boolean), which tells whether the given system is linear.
Note that "linear" here refers to the operator: terms such as ``x*diff(x,t)`` are
nonlinear, whereas terms like ``sin(t)*diff(x,t)`` are still linear operators.
'func' (list) contains the :py:class:`~sympy.core.function.Function`s that
appear with a derivative in the ODE, i.e. those that we are trying to solve
the ODE for.
'order' (dict) with the maximum derivative for each element of the 'func'
parameter.
'func_coeff' (dict) with the coefficient for each triple ``(equation number,
function, order)```. The coefficients are those subexpressions that do not
appear in 'func', and hence can be considered constant for purposes of ODE
solving.
'eq' (list) with the equations from ``eq``, sympified and transformed into
expressions (we are solving for these expressions to be zero).
'no_of_equations' (int) is the number of equations (same as ``len(eq)``).
'type_of_equation' (string) is an internal classification of the type of
ODE.
References
==========
-http://eqworld.ipmnet.ru/en/solutions/sysode/sode-toc1.htm
-A. D. Polyanin and A. V. Manzhirov, Handbook of Mathematics for Engineers and Scientists
Examples
========
>>> from sympy import Function, Eq, symbols, diff
>>> from sympy.solvers.ode import classify_sysode
>>> from sympy.abc import t
>>> f, x, y = symbols('f, x, y', cls=Function)
>>> k, l, m, n = symbols('k, l, m, n', Integer=True)
>>> x1 = diff(x(t), t) ; y1 = diff(y(t), t)
>>> x2 = diff(x(t), t, t) ; y2 = diff(y(t), t, t)
>>> eq = (Eq(5*x1, 12*x(t) - 6*y(t)), Eq(2*y1, 11*x(t) + 3*y(t)))
>>> classify_sysode(eq)
{'eq': [-12*x(t) + 6*y(t) + 5*Derivative(x(t), t), -11*x(t) - 3*y(t) + 2*Derivative(y(t), t)],
'func': [x(t), y(t)], 'func_coeff': {(0, x(t), 0): -12, (0, x(t), 1): 5, (0, y(t), 0): 6,
(0, y(t), 1): 0, (1, x(t), 0): -11, (1, x(t), 1): 0, (1, y(t), 0): -3, (1, y(t), 1): 2},
'is_linear': True, 'no_of_equation': 2, 'order': {x(t): 1, y(t): 1}, 'type_of_equation': 'type1'}
>>> eq = (Eq(diff(x(t),t), 5*t*x(t) + t**2*y(t)), Eq(diff(y(t),t), -t**2*x(t) + 5*t*y(t)))
>>> classify_sysode(eq)
{'eq': [-t**2*y(t) - 5*t*x(t) + Derivative(x(t), t), t**2*x(t) - 5*t*y(t) + Derivative(y(t), t)],
'func': [x(t), y(t)], 'func_coeff': {(0, x(t), 0): -5*t, (0, x(t), 1): 1, (0, y(t), 0): -t**2,
(0, y(t), 1): 0, (1, x(t), 0): t**2, (1, x(t), 1): 0, (1, y(t), 0): -5*t, (1, y(t), 1): 1},
'is_linear': True, 'no_of_equation': 2, 'order': {x(t): 1, y(t): 1}, 'type_of_equation': 'type4'}
"""
# Sympify equations and convert iterables of equations into
# a list of equations
def _sympify(eq):
return list(map(sympify, eq if iterable(eq) else [eq]))
eq, funcs = (_sympify(w) for w in [eq, funcs])
for i, fi in enumerate(eq):
if isinstance(fi, Equality):
eq[i] = fi.lhs - fi.rhs
matching_hints = {"no_of_equation":i+1}
matching_hints['eq'] = eq
if i==0:
raise ValueError("classify_sysode() works for systems of ODEs. "
"For scalar ODEs, classify_ode should be used")
t = list(list(eq[0].atoms(Derivative))[0].atoms(Symbol))[0]
# find all the functions if not given
order = dict()
if funcs==[None]:
funcs = []
for eqs in eq:
derivs = eqs.atoms(Derivative)
func = set().union(*[d.atoms(AppliedUndef) for d in derivs])
for func_ in func:
funcs.append(func_)
funcs = list(set(funcs))
if len(funcs) != len(eq):
raise ValueError("Number of functions given is not equal to the number of equations %s" % funcs)
func_dict = dict()
for func in funcs:
if not order.get(func, False):
max_order = 0
for i, eqs_ in enumerate(eq):
order_ = ode_order(eqs_,func)
if max_order < order_:
max_order = order_
eq_no = i
if eq_no in func_dict:
list_func = []
list_func.append(func_dict[eq_no])
list_func.append(func)
func_dict[eq_no] = list_func
else:
func_dict[eq_no] = func
order[func] = max_order
funcs = [func_dict[i] for i in range(len(func_dict))]
matching_hints['func'] = funcs
for func in funcs:
if isinstance(func, list):
for func_elem in func:
if len(func_elem.args) != 1:
raise ValueError("dsolve() and classify_sysode() work with "
"functions of one variable only, not %s" % func)
else:
if func and len(func.args) != 1:
raise ValueError("dsolve() and classify_sysode() work with "
"functions of one variable only, not %s" % func)
# find the order of all equation in system of odes
matching_hints["order"] = order
# find coefficients of terms f(t), diff(f(t),t) and higher derivatives
# and similarly for other functions g(t), diff(g(t),t) in all equations.
# Here j denotes the equation number, funcs[l] denotes the function about
# which we are talking about and k denotes the order of function funcs[l]
# whose coefficient we are calculating.
def linearity_check(eqs, j, func, is_linear_):
for k in range(order[func] + 1):
func_coef[j, func, k] = collect(eqs.expand(), [diff(func, t, k)]).coeff(diff(func, t, k))
if is_linear_ == True:
if func_coef[j, func, k] == 0:
if k == 0:
coef = eqs.as_independent(func, as_Add=True)[1]
for xr in range(1, ode_order(eqs,func) + 1):
coef -= eqs.as_independent(diff(func, t, xr), as_Add=True)[1]
if coef != 0:
is_linear_ = False
else:
if eqs.as_independent(diff(func, t, k), as_Add=True)[1]:
is_linear_ = False
else:
for func_ in funcs:
if isinstance(func_, list):
for elem_func_ in func_:
dep = func_coef[j, func, k].as_independent(elem_func_, as_Add=True)[1]
if dep != 0:
is_linear_ = False
else:
dep = func_coef[j, func, k].as_independent(func_, as_Add=True)[1]
if dep != 0:
is_linear_ = False
return is_linear_
func_coef = {}
is_linear = True
for j, eqs in enumerate(eq):
for func in funcs:
if isinstance(func, list):
for func_elem in func:
is_linear = linearity_check(eqs, j, func_elem, is_linear)
else:
is_linear = linearity_check(eqs, j, func, is_linear)
matching_hints['func_coeff'] = func_coef
matching_hints['is_linear'] = is_linear
if len(set(order.values())) == 1:
order_eq = list(matching_hints['order'].values())[0]
if matching_hints['is_linear'] == True:
if matching_hints['no_of_equation'] == 2:
if order_eq == 1:
type_of_equation = check_linear_2eq_order1(eq, funcs, func_coef)
elif order_eq == 2:
type_of_equation = check_linear_2eq_order2(eq, funcs, func_coef)
else:
type_of_equation = None
elif matching_hints['no_of_equation'] == 3:
if order_eq == 1:
type_of_equation = check_linear_3eq_order1(eq, funcs, func_coef)
if type_of_equation is None:
type_of_equation = check_linear_neq_order1(eq, funcs, func_coef)
else:
type_of_equation = None
else:
if order_eq == 1:
type_of_equation = check_linear_neq_order1(eq, funcs, func_coef)
else:
type_of_equation = None
else:
if matching_hints['no_of_equation'] == 2:
if order_eq == 1:
type_of_equation = check_nonlinear_2eq_order1(eq, funcs, func_coef)
else:
type_of_equation = None
elif matching_hints['no_of_equation'] == 3:
if order_eq == 1:
type_of_equation = check_nonlinear_3eq_order1(eq, funcs, func_coef)
else:
type_of_equation = None
else:
type_of_equation = None
else:
type_of_equation = None
matching_hints['type_of_equation'] = type_of_equation
return matching_hints
def check_linear_2eq_order1(eq, func, func_coef):
x = func[0].func
y = func[1].func
fc = func_coef
t = list(list(eq[0].atoms(Derivative))[0].atoms(Symbol))[0]
r = dict()
# for equations Eq(a1*diff(x(t),t), b1*x(t) + c1*y(t) + d1)
# and Eq(a2*diff(y(t),t), b2*x(t) + c2*y(t) + d2)
r['a1'] = fc[0,x(t),1] ; r['a2'] = fc[1,y(t),1]
r['b1'] = -fc[0,x(t),0]/fc[0,x(t),1] ; r['b2'] = -fc[1,x(t),0]/fc[1,y(t),1]
r['c1'] = -fc[0,y(t),0]/fc[0,x(t),1] ; r['c2'] = -fc[1,y(t),0]/fc[1,y(t),1]
forcing = [S.Zero,S.Zero]
for i in range(2):
for j in Add.make_args(eq[i]):
if not j.has(x(t), y(t)):
forcing[i] += j
if not (forcing[0].has(t) or forcing[1].has(t)):
# We can handle homogeneous case and simple constant forcings
r['d1'] = forcing[0]
r['d2'] = forcing[1]
else:
# Issue #9244: nonhomogeneous linear systems are not supported
return None
# Conditions to check for type 6 whose equations are Eq(diff(x(t),t), f(t)*x(t) + g(t)*y(t)) and
# Eq(diff(y(t),t), a*[f(t) + a*h(t)]x(t) + a*[g(t) - h(t)]*y(t))
p = 0
q = 0
p1 = cancel(r['b2']/(cancel(r['b2']/r['c2']).as_numer_denom()[0]))
p2 = cancel(r['b1']/(cancel(r['b1']/r['c1']).as_numer_denom()[0]))
for n, i in enumerate([p1, p2]):
for j in Mul.make_args(collect_const(i)):
if not j.has(t):
q = j
if q and n==0:
if ((r['b2']/j - r['b1'])/(r['c1'] - r['c2']/j)) == j:
p = 1
elif q and n==1:
if ((r['b1']/j - r['b2'])/(r['c2'] - r['c1']/j)) == j:
p = 2
# End of condition for type 6
if r['d1']!=0 or r['d2']!=0:
if not r['d1'].has(t) and not r['d2'].has(t):
if all(not r[k].has(t) for k in 'a1 a2 b1 b2 c1 c2'.split()):
# Equations for type 2 are Eq(a1*diff(x(t),t),b1*x(t)+c1*y(t)+d1) and Eq(a2*diff(y(t),t),b2*x(t)+c2*y(t)+d2)
return "type2"
else:
return None
else:
if all(not r[k].has(t) for k in 'a1 a2 b1 b2 c1 c2'.split()):
# Equations for type 1 are Eq(a1*diff(x(t),t),b1*x(t)+c1*y(t)) and Eq(a2*diff(y(t),t),b2*x(t)+c2*y(t))
return "type1"
else:
r['b1'] = r['b1']/r['a1'] ; r['b2'] = r['b2']/r['a2']
r['c1'] = r['c1']/r['a1'] ; r['c2'] = r['c2']/r['a2']
if (r['b1'] == r['c2']) and (r['c1'] == r['b2']):
# Equation for type 3 are Eq(diff(x(t),t), f(t)*x(t) + g(t)*y(t)) and Eq(diff(y(t),t), g(t)*x(t) + f(t)*y(t))
return "type3"
elif (r['b1'] == r['c2']) and (r['c1'] == -r['b2']) or (r['b1'] == -r['c2']) and (r['c1'] == r['b2']):
# Equation for type 4 are Eq(diff(x(t),t), f(t)*x(t) + g(t)*y(t)) and Eq(diff(y(t),t), -g(t)*x(t) + f(t)*y(t))
return "type4"
elif (not cancel(r['b2']/r['c1']).has(t) and not cancel((r['c2']-r['b1'])/r['c1']).has(t)) \
or (not cancel(r['b1']/r['c2']).has(t) and not cancel((r['c1']-r['b2'])/r['c2']).has(t)):
# Equations for type 5 are Eq(diff(x(t),t), f(t)*x(t) + g(t)*y(t)) and Eq(diff(y(t),t), a*g(t)*x(t) + [f(t) + b*g(t)]*y(t)
return "type5"
elif p:
return "type6"
else:
# Equations for type 7 are Eq(diff(x(t),t), f(t)*x(t) + g(t)*y(t)) and Eq(diff(y(t),t), h(t)*x(t) + p(t)*y(t))
return "type7"
def check_linear_2eq_order2(eq, func, func_coef):
x = func[0].func
y = func[1].func
fc = func_coef
t = list(list(eq[0].atoms(Derivative))[0].atoms(Symbol))[0]
r = dict()
a = Wild('a', exclude=[1/t])
b = Wild('b', exclude=[1/t**2])
u = Wild('u', exclude=[t, t**2])
v = Wild('v', exclude=[t, t**2])
w = Wild('w', exclude=[t, t**2])
p = Wild('p', exclude=[t, t**2])
r['a1'] = fc[0,x(t),2] ; r['a2'] = fc[1,y(t),2]
r['b1'] = fc[0,x(t),1] ; r['b2'] = fc[1,x(t),1]
r['c1'] = fc[0,y(t),1] ; r['c2'] = fc[1,y(t),1]
r['d1'] = fc[0,x(t),0] ; r['d2'] = fc[1,x(t),0]
r['e1'] = fc[0,y(t),0] ; r['e2'] = fc[1,y(t),0]
const = [S.Zero, S.Zero]
for i in range(2):
for j in Add.make_args(eq[i]):
if not (j.has(x(t)) or j.has(y(t))):
const[i] += j
r['f1'] = const[0]
r['f2'] = const[1]
if r['f1']!=0 or r['f2']!=0:
if all(not r[k].has(t) for k in 'a1 a2 d1 d2 e1 e2 f1 f2'.split()) \
and r['b1']==r['c1']==r['b2']==r['c2']==0:
return "type2"
elif all(not r[k].has(t) for k in 'a1 a2 b1 b2 c1 c2 d1 d2 e1 e1'.split()):
p = [S.Zero, S.Zero] ; q = [S.Zero, S.Zero]
for n, e in enumerate([r['f1'], r['f2']]):
if e.has(t):
tpart = e.as_independent(t, Mul)[1]
for i in Mul.make_args(tpart):
if i.has(exp):
b, e = i.as_base_exp()
co = e.coeff(t)
if co and not co.has(t) and co.has(I):
p[n] = 1
else:
q[n] = 1
else:
q[n] = 1
else:
q[n] = 1
if p[0]==1 and p[1]==1 and q[0]==0 and q[1]==0:
return "type4"
else:
return None
else:
return None
else:
if r['b1']==r['b2']==r['c1']==r['c2']==0 and all(not r[k].has(t) \
for k in 'a1 a2 d1 d2 e1 e2'.split()):
return "type1"
elif r['b1']==r['e1']==r['c2']==r['d2']==0 and all(not r[k].has(t) \
for k in 'a1 a2 b2 c1 d1 e2'.split()) and r['c1'] == -r['b2'] and \
r['d1'] == r['e2']:
return "type3"
elif cancel(-r['b2']/r['d2'])==t and cancel(-r['c1']/r['e1'])==t and not \
(r['d2']/r['a2']).has(t) and not (r['e1']/r['a1']).has(t) and \
r['b1']==r['d1']==r['c2']==r['e2']==0:
return "type5"
elif ((r['a1']/r['d1']).expand()).match((p*(u*t**2+v*t+w)**2).expand()) and not \
(cancel(r['a1']*r['d2']/(r['a2']*r['d1']))).has(t) and not (r['d1']/r['e1']).has(t) and not \
(r['d2']/r['e2']).has(t) and r['b1'] == r['b2'] == r['c1'] == r['c2'] == 0:
return "type10"
elif not cancel(r['d1']/r['e1']).has(t) and not cancel(r['d2']/r['e2']).has(t) and not \
cancel(r['d1']*r['a2']/(r['d2']*r['a1'])).has(t) and r['b1']==r['b2']==r['c1']==r['c2']==0:
return "type6"
elif not cancel(r['b1']/r['c1']).has(t) and not cancel(r['b2']/r['c2']).has(t) and not \
cancel(r['b1']*r['a2']/(r['b2']*r['a1'])).has(t) and r['d1']==r['d2']==r['e1']==r['e2']==0:
return "type7"
elif cancel(-r['b2']/r['d2'])==t and cancel(-r['c1']/r['e1'])==t and not \
cancel(r['e1']*r['a2']/(r['d2']*r['a1'])).has(t) and r['e1'].has(t) \
and r['b1']==r['d1']==r['c2']==r['e2']==0:
return "type8"
elif (r['b1']/r['a1']).match(a/t) and (r['b2']/r['a2']).match(a/t) and not \
(r['b1']/r['c1']).has(t) and not (r['b2']/r['c2']).has(t) and \
(r['d1']/r['a1']).match(b/t**2) and (r['d2']/r['a2']).match(b/t**2) \
and not (r['d1']/r['e1']).has(t) and not (r['d2']/r['e2']).has(t):
return "type9"
elif -r['b1']/r['d1']==-r['c1']/r['e1']==-r['b2']/r['d2']==-r['c2']/r['e2']==t:
return "type11"
else:
return None
def check_linear_3eq_order1(eq, func, func_coef):
x = func[0].func
y = func[1].func
z = func[2].func
fc = func_coef
t = list(list(eq[0].atoms(Derivative))[0].atoms(Symbol))[0]
r = dict()
r['a1'] = fc[0,x(t),1]; r['a2'] = fc[1,y(t),1]; r['a3'] = fc[2,z(t),1]
r['b1'] = fc[0,x(t),0]; r['b2'] = fc[1,x(t),0]; r['b3'] = fc[2,x(t),0]
r['c1'] = fc[0,y(t),0]; r['c2'] = fc[1,y(t),0]; r['c3'] = fc[2,y(t),0]
r['d1'] = fc[0,z(t),0]; r['d2'] = fc[1,z(t),0]; r['d3'] = fc[2,z(t),0]
forcing = [S.Zero, S.Zero, S.Zero]
for i in range(3):
for j in Add.make_args(eq[i]):
if not j.has(x(t), y(t), z(t)):
forcing[i] += j
if forcing[0].has(t) or forcing[1].has(t) or forcing[2].has(t):
# We can handle homogeneous case and simple constant forcings.
# Issue #9244: nonhomogeneous linear systems are not supported
return None
if all(not r[k].has(t) for k in 'a1 a2 a3 b1 b2 b3 c1 c2 c3 d1 d2 d3'.split()):
if r['c1']==r['d1']==r['d2']==0:
return 'type1'
elif r['c1'] == -r['b2'] and r['d1'] == -r['b3'] and r['d2'] == -r['c3'] \
and r['b1'] == r['c2'] == r['d3'] == 0:
return 'type2'
elif r['b1'] == r['c2'] == r['d3'] == 0 and r['c1']/r['a1'] == -r['d1']/r['a1'] \
and r['d2']/r['a2'] == -r['b2']/r['a2'] and r['b3']/r['a3'] == -r['c3']/r['a3']:
return 'type3'
else:
return None
else:
for k1 in 'c1 d1 b2 d2 b3 c3'.split():
if r[k1] == 0:
continue
else:
if all(not cancel(r[k1]/r[k]).has(t) for k in 'd1 b2 d2 b3 c3'.split() if r[k]!=0) \
and all(not cancel(r[k1]/(r['b1'] - r[k])).has(t) for k in 'b1 c2 d3'.split() if r['b1']!=r[k]):
return 'type4'
else:
break
return None
def check_linear_neq_order1(eq, func, func_coef):
fc = func_coef
t = list(list(eq[0].atoms(Derivative))[0].atoms(Symbol))[0]
n = len(eq)
for i in range(n):
for j in range(n):
if (fc[i, func[j], 0]/fc[i, func[i], 1]).has(t):
return None
if len(eq) == 3:
return 'type6'
return 'type1'
def check_nonlinear_2eq_order1(eq, func, func_coef):
t = list(list(eq[0].atoms(Derivative))[0].atoms(Symbol))[0]
f = Wild('f')
g = Wild('g')
u, v = symbols('u, v', cls=Dummy)
def check_type(x, y):
r1 = eq[0].match(t*diff(x(t),t) - x(t) + f)
r2 = eq[1].match(t*diff(y(t),t) - y(t) + g)
if not (r1 and r2):
r1 = eq[0].match(diff(x(t),t) - x(t)/t + f/t)
r2 = eq[1].match(diff(y(t),t) - y(t)/t + g/t)
if not (r1 and r2):
r1 = (-eq[0]).match(t*diff(x(t),t) - x(t) + f)
r2 = (-eq[1]).match(t*diff(y(t),t) - y(t) + g)
if not (r1 and r2):
r1 = (-eq[0]).match(diff(x(t),t) - x(t)/t + f/t)
r2 = (-eq[1]).match(diff(y(t),t) - y(t)/t + g/t)
if r1 and r2 and not (r1[f].subs(diff(x(t),t),u).subs(diff(y(t),t),v).has(t) \
or r2[g].subs(diff(x(t),t),u).subs(diff(y(t),t),v).has(t)):
return 'type5'
else:
return None
for func_ in func:
if isinstance(func_, list):
x = func[0][0].func
y = func[0][1].func
eq_type = check_type(x, y)
if not eq_type:
eq_type = check_type(y, x)
return eq_type
x = func[0].func
y = func[1].func
fc = func_coef
n = Wild('n', exclude=[x(t),y(t)])
f1 = Wild('f1', exclude=[v,t])
f2 = Wild('f2', exclude=[v,t])
g1 = Wild('g1', exclude=[u,t])
g2 = Wild('g2', exclude=[u,t])
for i in range(2):
eqs = 0
for terms in Add.make_args(eq[i]):
eqs += terms/fc[i,func[i],1]
eq[i] = eqs
r = eq[0].match(diff(x(t),t) - x(t)**n*f)
if r:
g = (diff(y(t),t) - eq[1])/r[f]
if r and not (g.has(x(t)) or g.subs(y(t),v).has(t) or r[f].subs(x(t),u).subs(y(t),v).has(t)):
return 'type1'
r = eq[0].match(diff(x(t),t) - exp(n*x(t))*f)
if r:
g = (diff(y(t),t) - eq[1])/r[f]
if r and not (g.has(x(t)) or g.subs(y(t),v).has(t) or r[f].subs(x(t),u).subs(y(t),v).has(t)):
return 'type2'
g = Wild('g')
r1 = eq[0].match(diff(x(t),t) - f)
r2 = eq[1].match(diff(y(t),t) - g)
if r1 and r2 and not (r1[f].subs(x(t),u).subs(y(t),v).has(t) or \
r2[g].subs(x(t),u).subs(y(t),v).has(t)):
return 'type3'
r1 = eq[0].match(diff(x(t),t) - f)
r2 = eq[1].match(diff(y(t),t) - g)
num, den = (
(r1[f].subs(x(t),u).subs(y(t),v))/
(r2[g].subs(x(t),u).subs(y(t),v))).as_numer_denom()
R1 = num.match(f1*g1)
R2 = den.match(f2*g2)
# phi = (r1[f].subs(x(t),u).subs(y(t),v))/num
if R1 and R2:
return 'type4'
return None
def check_nonlinear_2eq_order2(eq, func, func_coef):
return None
def check_nonlinear_3eq_order1(eq, func, func_coef):
x = func[0].func
y = func[1].func
z = func[2].func
fc = func_coef
t = list(list(eq[0].atoms(Derivative))[0].atoms(Symbol))[0]
u, v, w = symbols('u, v, w', cls=Dummy)
a = Wild('a', exclude=[x(t), y(t), z(t), t])
b = Wild('b', exclude=[x(t), y(t), z(t), t])
c = Wild('c', exclude=[x(t), y(t), z(t), t])
f = Wild('f')
F1 = Wild('F1')
F2 = Wild('F2')
F3 = Wild('F3')
for i in range(3):
eqs = 0
for terms in Add.make_args(eq[i]):
eqs += terms/fc[i,func[i],1]
eq[i] = eqs
r1 = eq[0].match(diff(x(t),t) - a*y(t)*z(t))
r2 = eq[1].match(diff(y(t),t) - b*z(t)*x(t))
r3 = eq[2].match(diff(z(t),t) - c*x(t)*y(t))
if r1 and r2 and r3:
num1, den1 = r1[a].as_numer_denom()
num2, den2 = r2[b].as_numer_denom()
num3, den3 = r3[c].as_numer_denom()
if solve([num1*u-den1*(v-w), num2*v-den2*(w-u), num3*w-den3*(u-v)],[u, v]):
return 'type1'
r = eq[0].match(diff(x(t),t) - y(t)*z(t)*f)
if r:
r1 = collect_const(r[f]).match(a*f)
r2 = ((diff(y(t),t) - eq[1])/r1[f]).match(b*z(t)*x(t))
r3 = ((diff(z(t),t) - eq[2])/r1[f]).match(c*x(t)*y(t))
if r1 and r2 and r3:
num1, den1 = r1[a].as_numer_denom()
num2, den2 = r2[b].as_numer_denom()
num3, den3 = r3[c].as_numer_denom()
if solve([num1*u-den1*(v-w), num2*v-den2*(w-u), num3*w-den3*(u-v)],[u, v]):
return 'type2'
r = eq[0].match(diff(x(t),t) - (F2-F3))
if r:
r1 = collect_const(r[F2]).match(c*F2)
r1.update(collect_const(r[F3]).match(b*F3))
if r1:
if eq[1].has(r1[F2]) and not eq[1].has(r1[F3]):
r1[F2], r1[F3] = r1[F3], r1[F2]
r1[c], r1[b] = -r1[b], -r1[c]
r2 = eq[1].match(diff(y(t),t) - a*r1[F3] + r1[c]*F1)
if r2:
r3 = (eq[2] == diff(z(t),t) - r1[b]*r2[F1] + r2[a]*r1[F2])
if r1 and r2 and r3:
return 'type3'
r = eq[0].match(diff(x(t),t) - z(t)*F2 + y(t)*F3)
if r:
r1 = collect_const(r[F2]).match(c*F2)
r1.update(collect_const(r[F3]).match(b*F3))
if r1:
if eq[1].has(r1[F2]) and not eq[1].has(r1[F3]):
r1[F2], r1[F3] = r1[F3], r1[F2]
r1[c], r1[b] = -r1[b], -r1[c]
r2 = (diff(y(t),t) - eq[1]).match(a*x(t)*r1[F3] - r1[c]*z(t)*F1)
if r2:
r3 = (diff(z(t),t) - eq[2] == r1[b]*y(t)*r2[F1] - r2[a]*x(t)*r1[F2])
if r1 and r2 and r3:
return 'type4'
r = (diff(x(t),t) - eq[0]).match(x(t)*(F2 - F3))
if r:
r1 = collect_const(r[F2]).match(c*F2)
r1.update(collect_const(r[F3]).match(b*F3))
if r1:
if eq[1].has(r1[F2]) and not eq[1].has(r1[F3]):
r1[F2], r1[F3] = r1[F3], r1[F2]
r1[c], r1[b] = -r1[b], -r1[c]
r2 = (diff(y(t),t) - eq[1]).match(y(t)*(a*r1[F3] - r1[c]*F1))
if r2:
r3 = (diff(z(t),t) - eq[2] == z(t)*(r1[b]*r2[F1] - r2[a]*r1[F2]))
if r1 and r2 and r3:
return 'type5'
return None
def check_nonlinear_3eq_order2(eq, func, func_coef):
return None
def checksysodesol(eqs, sols, func=None):
r"""
Substitutes corresponding ``sols`` for each functions into each ``eqs`` and
checks that the result of substitutions for each equation is ``0``. The
equations and solutions passed can be any iterable.
This only works when each ``sols`` have one function only, like `x(t)` or `y(t)`.
For each function, ``sols`` can have a single solution or a list of solutions.
In most cases it will not be necessary to explicitly identify the function,
but if the function cannot be inferred from the original equation it
can be supplied through the ``func`` argument.
When a sequence of equations is passed, the same sequence is used to return
the result for each equation with each function substituted with corresponding
solutions.
It tries the following method to find zero equivalence for each equation:
Substitute the solutions for functions, like `x(t)` and `y(t)` into the
original equations containing those functions.
This function returns a tuple. The first item in the tuple is ``True`` if
the substitution results for each equation is ``0``, and ``False`` otherwise.
The second item in the tuple is what the substitution results in. Each element
of the ``list`` should always be ``0`` corresponding to each equation if the
first item is ``True``. Note that sometimes this function may return ``False``,
but with an expression that is identically equal to ``0``, instead of returning
``True``. This is because :py:meth:`~sympy.simplify.simplify.simplify` cannot
reduce the expression to ``0``. If an expression returned by each function
vanishes identically, then ``sols`` really is a solution to ``eqs``.
If this function seems to hang, it is probably because of a difficult simplification.
Examples
========
>>> from sympy import Eq, diff, symbols, sin, cos, exp, sqrt, S, Function
>>> from sympy.solvers.ode import checksysodesol
>>> C1, C2 = symbols('C1:3')
>>> t = symbols('t')
>>> x, y = symbols('x, y', cls=Function)
>>> eq = (Eq(diff(x(t),t), x(t) + y(t) + 17), Eq(diff(y(t),t), -2*x(t) + y(t) + 12))
>>> sol = [Eq(x(t), (C1*sin(sqrt(2)*t) + C2*cos(sqrt(2)*t))*exp(t) - S(5)/3),
... Eq(y(t), (sqrt(2)*C1*cos(sqrt(2)*t) - sqrt(2)*C2*sin(sqrt(2)*t))*exp(t) - S(46)/3)]
>>> checksysodesol(eq, sol)
(True, [0, 0])
>>> eq = (Eq(diff(x(t),t),x(t)*y(t)**4), Eq(diff(y(t),t),y(t)**3))
>>> sol = [Eq(x(t), C1*exp(-1/(4*(C2 + t)))), Eq(y(t), -sqrt(2)*sqrt(-1/(C2 + t))/2),
... Eq(x(t), C1*exp(-1/(4*(C2 + t)))), Eq(y(t), sqrt(2)*sqrt(-1/(C2 + t))/2)]
>>> checksysodesol(eq, sol)
(True, [0, 0])
"""
def _sympify(eq):
return list(map(sympify, eq if iterable(eq) else [eq]))
eqs = _sympify(eqs)
for i in range(len(eqs)):
if isinstance(eqs[i], Equality):
eqs[i] = eqs[i].lhs - eqs[i].rhs
if func is None:
funcs = []
for eq in eqs:
derivs = eq.atoms(Derivative)
func = set().union(*[d.atoms(AppliedUndef) for d in derivs])
for func_ in func:
funcs.append(func_)
funcs = list(set(funcs))
if not all(isinstance(func, AppliedUndef) and len(func.args) == 1 for func in funcs)\
and len({func.args for func in funcs})!=1:
raise ValueError("func must be a function of one variable, not %s" % func)
for sol in sols:
if len(sol.atoms(AppliedUndef)) != 1:
raise ValueError("solutions should have one function only")
if len(funcs) != len({sol.lhs for sol in sols}):
raise ValueError("number of solutions provided does not match the number of equations")
dictsol = dict()
for sol in sols:
func = list(sol.atoms(AppliedUndef))[0]
if sol.rhs == func:
sol = sol.reversed
solved = sol.lhs == func and not sol.rhs.has(func)
if not solved:
rhs = solve(sol, func)
if not rhs:
raise NotImplementedError
else:
rhs = sol.rhs
dictsol[func] = rhs
checkeq = []
for eq in eqs:
for func in funcs:
eq = sub_func_doit(eq, func, dictsol[func])
ss = simplify(eq)
if ss != 0:
eq = ss.expand(force=True)
else:
eq = 0
checkeq.append(eq)
if len(set(checkeq)) == 1 and list(set(checkeq))[0] == 0:
return (True, checkeq)
else:
return (False, checkeq)
@vectorize(0)
def odesimp(ode, eq, func, hint):
r"""
Simplifies solutions of ODEs, including trying to solve for ``func`` and
running :py:meth:`~sympy.solvers.ode.constantsimp`.
It may use knowledge of the type of solution that the hint returns to
apply additional simplifications.
It also attempts to integrate any :py:class:`~sympy.integrals.Integral`\s
in the expression, if the hint is not an ``_Integral`` hint.
This function should have no effect on expressions returned by
:py:meth:`~sympy.solvers.ode.dsolve`, as
:py:meth:`~sympy.solvers.ode.dsolve` already calls
:py:meth:`~sympy.solvers.ode.odesimp`, but the individual hint functions
do not call :py:meth:`~sympy.solvers.ode.odesimp` (because the
:py:meth:`~sympy.solvers.ode.dsolve` wrapper does). Therefore, this
function is designed for mainly internal use.
Examples
========
>>> from sympy import sin, symbols, dsolve, pprint, Function
>>> from sympy.solvers.ode import odesimp
>>> x , u2, C1= symbols('x,u2,C1')
>>> f = Function('f')
>>> eq = dsolve(x*f(x).diff(x) - f(x) - x*sin(f(x)/x), f(x),
... hint='1st_homogeneous_coeff_subs_indep_div_dep_Integral',
... simplify=False)
>>> pprint(eq, wrap_line=False)
x
----
f(x)
/
|
| / 1 \
| -|u2 + -------|
| | /1 \|
| | sin|--||
| \ \u2//
log(f(x)) = log(C1) + | ---------------- d(u2)
| 2
| u2
|
/
>>> pprint(odesimp(eq, f(x), 1, {C1},
... hint='1st_homogeneous_coeff_subs_indep_div_dep'
... )) #doctest: +SKIP
x
--------- = C1
/f(x)\
tan|----|
\2*x /
"""
x = func.args[0]
f = func.func
C1 = get_numbered_constants(eq, num=1)
constants = eq.free_symbols - ode.free_symbols
# First, integrate if the hint allows it.
eq = _handle_Integral(eq, func, hint)
if hint.startswith("nth_linear_euler_eq_nonhomogeneous"):
eq = simplify(eq)
if not isinstance(eq, Equality):
raise TypeError("eq should be an instance of Equality")
# Second, clean up the arbitrary constants.
# Right now, nth linear hints can put as many as 2*order constants in an
# expression. If that number grows with another hint, the third argument
# here should be raised accordingly, or constantsimp() rewritten to handle
# an arbitrary number of constants.
eq = constantsimp(eq, constants)
# Lastly, now that we have cleaned up the expression, try solving for func.
# When CRootOf is implemented in solve(), we will want to return a CRootOf
# every time instead of an Equality.
# Get the f(x) on the left if possible.
if eq.rhs == func and not eq.lhs.has(func):
eq = [Eq(eq.rhs, eq.lhs)]
# make sure we are working with lists of solutions in simplified form.
if eq.lhs == func and not eq.rhs.has(func):
# The solution is already solved
eq = [eq]
# special simplification of the rhs
if hint.startswith("nth_linear_constant_coeff"):
# Collect terms to make the solution look nice.
# This is also necessary for constantsimp to remove unnecessary
# terms from the particular solution from variation of parameters
#
# Collect is not behaving reliably here. The results for
# some linear constant-coefficient equations with repeated
# roots do not properly simplify all constants sometimes.
# 'collectterms' gives different orders sometimes, and results
# differ in collect based on that order. The
# sort-reverse trick fixes things, but may fail in the
# future. In addition, collect is splitting exponentials with
# rational powers for no reason. We have to do a match
# to fix this using Wilds.
global collectterms
try:
collectterms.sort(key=default_sort_key)
collectterms.reverse()
except Exception:
pass
assert len(eq) == 1 and eq[0].lhs == f(x)
sol = eq[0].rhs
sol = expand_mul(sol)
for i, reroot, imroot in collectterms:
sol = collect(sol, x**i*exp(reroot*x)*sin(abs(imroot)*x))
sol = collect(sol, x**i*exp(reroot*x)*cos(imroot*x))
for i, reroot, imroot in collectterms:
sol = collect(sol, x**i*exp(reroot*x))
del collectterms
# Collect is splitting exponentials with rational powers for
# no reason. We call powsimp to fix.
sol = powsimp(sol)
eq[0] = Eq(f(x), sol)
else:
# The solution is not solved, so try to solve it
try:
floats = any(i.is_Float for i in eq.atoms(Number))
eqsol = solve(eq, func, force=True, rational=False if floats else None)
if not eqsol:
raise NotImplementedError
except (NotImplementedError, PolynomialError):
eq = [eq]
else:
def _expand(expr):
numer, denom = expr.as_numer_denom()
if denom.is_Add:
return expr
else:
return powsimp(expr.expand(), combine='exp', deep=True)
# XXX: the rest of odesimp() expects each ``t`` to be in a
# specific normal form: rational expression with numerator
# expanded, but with combined exponential functions (at
# least in this setup all tests pass).
eq = [Eq(f(x), _expand(t)) for t in eqsol]
# special simplification of the lhs.
if hint.startswith("1st_homogeneous_coeff"):
for j, eqi in enumerate(eq):
newi = logcombine(eqi, force=True)
if isinstance(newi.lhs, log) and newi.rhs == 0:
newi = Eq(newi.lhs.args[0]/C1, C1)
eq[j] = newi
# We cleaned up the constants before solving to help the solve engine with
# a simpler expression, but the solved expression could have introduced
# things like -C1, so rerun constantsimp() one last time before returning.
for i, eqi in enumerate(eq):
eq[i] = constantsimp(eqi, constants)
eq[i] = constant_renumber(eq[i], ode.free_symbols)
# If there is only 1 solution, return it;
# otherwise return the list of solutions.
if len(eq) == 1:
eq = eq[0]
return eq
def checkodesol(ode, sol, func=None, order='auto', solve_for_func=True):
r"""
Substitutes ``sol`` into ``ode`` and checks that the result is ``0``.
This only works when ``func`` is one function, like `f(x)`. ``sol`` can
be a single solution or a list of solutions. Each solution may be an
:py:class:`~sympy.core.relational.Equality` that the solution satisfies,
e.g. ``Eq(f(x), C1), Eq(f(x) + C1, 0)``; or simply an
:py:class:`~sympy.core.expr.Expr`, e.g. ``f(x) - C1``. In most cases it
will not be necessary to explicitly identify the function, but if the
function cannot be inferred from the original equation it can be supplied
through the ``func`` argument.
If a sequence of solutions is passed, the same sort of container will be
used to return the result for each solution.
It tries the following methods, in order, until it finds zero equivalence:
1. Substitute the solution for `f` in the original equation. This only
works if ``ode`` is solved for `f`. It will attempt to solve it first
unless ``solve_for_func == False``.
2. Take `n` derivatives of the solution, where `n` is the order of
``ode``, and check to see if that is equal to the solution. This only
works on exact ODEs.
3. Take the 1st, 2nd, ..., `n`\th derivatives of the solution, each time
solving for the derivative of `f` of that order (this will always be
possible because `f` is a linear operator). Then back substitute each
derivative into ``ode`` in reverse order.
This function returns a tuple. The first item in the tuple is ``True`` if
the substitution results in ``0``, and ``False`` otherwise. The second
item in the tuple is what the substitution results in. It should always
be ``0`` if the first item is ``True``. Sometimes this function will
return ``False`` even when an expression is identically equal to ``0``.
This happens when :py:meth:`~sympy.simplify.simplify.simplify` does not
reduce the expression to ``0``. If an expression returned by this
function vanishes identically, then ``sol`` really is a solution to
the ``ode``.
If this function seems to hang, it is probably because of a hard
simplification.
To use this function to test, test the first item of the tuple.
Examples
========
>>> from sympy import Eq, Function, checkodesol, symbols
>>> x, C1 = symbols('x,C1')
>>> f = Function('f')
>>> checkodesol(f(x).diff(x), Eq(f(x), C1))
(True, 0)
>>> assert checkodesol(f(x).diff(x), C1)[0]
>>> assert not checkodesol(f(x).diff(x), x)[0]
>>> checkodesol(f(x).diff(x, 2), x**2)
(False, 2)
"""
if not isinstance(ode, Equality):
ode = Eq(ode, 0)
if func is None:
try:
_, func = _preprocess(ode.lhs)
except ValueError:
funcs = [s.atoms(AppliedUndef) for s in (
sol if is_sequence(sol, set) else [sol])]
funcs = set().union(*funcs)
if len(funcs) != 1:
raise ValueError(
'must pass func arg to checkodesol for this case.')
func = funcs.pop()
if not isinstance(func, AppliedUndef) or len(func.args) != 1:
raise ValueError(
"func must be a function of one variable, not %s" % func)
if is_sequence(sol, set):
return type(sol)([checkodesol(ode, i, order=order, solve_for_func=solve_for_func) for i in sol])
if not isinstance(sol, Equality):
sol = Eq(func, sol)
elif sol.rhs == func:
sol = sol.reversed
if order == 'auto':
order = ode_order(ode, func)
solved = sol.lhs == func and not sol.rhs.has(func)
if solve_for_func and not solved:
rhs = solve(sol, func)
if rhs:
eqs = [Eq(func, t) for t in rhs]
if len(rhs) == 1:
eqs = eqs[0]
return checkodesol(ode, eqs, order=order,
solve_for_func=False)
s = True
testnum = 0
x = func.args[0]
while s:
if testnum == 0:
# First pass, try substituting a solved solution directly into the
# ODE. This has the highest chance of succeeding.
ode_diff = ode.lhs - ode.rhs
if sol.lhs == func:
s = sub_func_doit(ode_diff, func, sol.rhs)
s = besselsimp(s)
else:
testnum += 1
continue
ss = simplify(s)
if ss:
# with the new numer_denom in power.py, if we do a simple
# expansion then testnum == 0 verifies all solutions.
s = ss.expand(force=True)
else:
s = 0
testnum += 1
elif testnum == 1:
# Second pass. If we cannot substitute f, try seeing if the nth
# derivative is equal, this will only work for odes that are exact,
# by definition.
s = simplify(
trigsimp(diff(sol.lhs, x, order) - diff(sol.rhs, x, order)) -
trigsimp(ode.lhs) + trigsimp(ode.rhs))
# s2 = simplify(
# diff(sol.lhs, x, order) - diff(sol.rhs, x, order) - \
# ode.lhs + ode.rhs)
testnum += 1
elif testnum == 2:
# Third pass. Try solving for df/dx and substituting that into the
# ODE. Thanks to Chris Smith for suggesting this method. Many of
# the comments below are his, too.
# The method:
# - Take each of 1..n derivatives of the solution.
# - Solve each nth derivative for d^(n)f/dx^(n)
# (the differential of that order)
# - Back substitute into the ODE in decreasing order
# (i.e., n, n-1, ...)
# - Check the result for zero equivalence
if sol.lhs == func and not sol.rhs.has(func):
diffsols = {0: sol.rhs}
elif sol.rhs == func and not sol.lhs.has(func):
diffsols = {0: sol.lhs}
else:
diffsols = {}
sol = sol.lhs - sol.rhs
for i in range(1, order + 1):
# Differentiation is a linear operator, so there should always
# be 1 solution. Nonetheless, we test just to make sure.
# We only need to solve once. After that, we automatically
# have the solution to the differential in the order we want.
if i == 1:
ds = sol.diff(x)
try:
sdf = solve(ds, func.diff(x, i))
if not sdf:
raise NotImplementedError
except NotImplementedError:
testnum += 1
break
else:
diffsols[i] = sdf[0]
else:
# This is what the solution says df/dx should be.
diffsols[i] = diffsols[i - 1].diff(x)
# Make sure the above didn't fail.
if testnum > 2:
continue
else:
# Substitute it into ODE to check for self consistency.
lhs, rhs = ode.lhs, ode.rhs
for i in range(order, -1, -1):
if i == 0 and 0 not in diffsols:
# We can only substitute f(x) if the solution was
# solved for f(x).
break
lhs = sub_func_doit(lhs, func.diff(x, i), diffsols[i])
rhs = sub_func_doit(rhs, func.diff(x, i), diffsols[i])
ode_or_bool = Eq(lhs, rhs)
ode_or_bool = simplify(ode_or_bool)
if isinstance(ode_or_bool, (bool, BooleanAtom)):
if ode_or_bool:
lhs = rhs = S.Zero
else:
lhs = ode_or_bool.lhs
rhs = ode_or_bool.rhs
# No sense in overworking simplify -- just prove that the
# numerator goes to zero
num = trigsimp((lhs - rhs).as_numer_denom()[0])
# since solutions are obtained using force=True we test
# using the same level of assumptions
## replace function with dummy so assumptions will work
_func = Dummy('func')
num = num.subs(func, _func)
## posify the expression
num, reps = posify(num)
s = simplify(num).xreplace(reps).xreplace({_func: func})
testnum += 1
else:
break
if not s:
return (True, s)
elif s is True: # The code above never was able to change s
raise NotImplementedError("Unable to test if " + str(sol) +
" is a solution to " + str(ode) + ".")
else:
return (False, s)
def ode_sol_simplicity(sol, func, trysolving=True):
r"""
Returns an extended integer representing how simple a solution to an ODE
is.
The following things are considered, in order from most simple to least:
- ``sol`` is solved for ``func``.
- ``sol`` is not solved for ``func``, but can be if passed to solve (e.g.,
a solution returned by ``dsolve(ode, func, simplify=False``).
- If ``sol`` is not solved for ``func``, then base the result on the
length of ``sol``, as computed by ``len(str(sol))``.
- If ``sol`` has any unevaluated :py:class:`~sympy.integrals.Integral`\s,
this will automatically be considered less simple than any of the above.
This function returns an integer such that if solution A is simpler than
solution B by above metric, then ``ode_sol_simplicity(sola, func) <
ode_sol_simplicity(solb, func)``.
Currently, the following are the numbers returned, but if the heuristic is
ever improved, this may change. Only the ordering is guaranteed.
+----------------------------------------------+-------------------+
| Simplicity | Return |
+==============================================+===================+
| ``sol`` solved for ``func`` | ``-2`` |
+----------------------------------------------+-------------------+
| ``sol`` not solved for ``func`` but can be | ``-1`` |
+----------------------------------------------+-------------------+
| ``sol`` is not solved nor solvable for | ``len(str(sol))`` |
| ``func`` | |
+----------------------------------------------+-------------------+
| ``sol`` contains an | ``oo`` |
| :py:class:`~sympy.integrals.Integral` | |
+----------------------------------------------+-------------------+
``oo`` here means the SymPy infinity, which should compare greater than
any integer.
If you already know :py:meth:`~sympy.solvers.solvers.solve` cannot solve
``sol``, you can use ``trysolving=False`` to skip that step, which is the
only potentially slow step. For example,
:py:meth:`~sympy.solvers.ode.dsolve` with the ``simplify=False`` flag
should do this.
If ``sol`` is a list of solutions, if the worst solution in the list
returns ``oo`` it returns that, otherwise it returns ``len(str(sol))``,
that is, the length of the string representation of the whole list.
Examples
========
This function is designed to be passed to ``min`` as the key argument,
such as ``min(listofsolutions, key=lambda i: ode_sol_simplicity(i,
f(x)))``.
>>> from sympy import symbols, Function, Eq, tan, cos, sqrt, Integral
>>> from sympy.solvers.ode import ode_sol_simplicity
>>> x, C1, C2 = symbols('x, C1, C2')
>>> f = Function('f')
>>> ode_sol_simplicity(Eq(f(x), C1*x**2), f(x))
-2
>>> ode_sol_simplicity(Eq(x**2 + f(x), C1), f(x))
-1
>>> ode_sol_simplicity(Eq(f(x), C1*Integral(2*x, x)), f(x))
oo
>>> eq1 = Eq(f(x)/tan(f(x)/(2*x)), C1)
>>> eq2 = Eq(f(x)/tan(f(x)/(2*x) + f(x)), C2)
>>> [ode_sol_simplicity(eq, f(x)) for eq in [eq1, eq2]]
[28, 35]
>>> min([eq1, eq2], key=lambda i: ode_sol_simplicity(i, f(x)))
Eq(f(x)/tan(f(x)/(2*x)), C1)
"""
# TODO: if two solutions are solved for f(x), we still want to be
# able to get the simpler of the two
# See the docstring for the coercion rules. We check easier (faster)
# things here first, to save time.
if iterable(sol):
# See if there are Integrals
for i in sol:
if ode_sol_simplicity(i, func, trysolving=trysolving) == oo:
return oo
return len(str(sol))
if sol.has(Integral):
return oo
# Next, try to solve for func. This code will change slightly when CRootOf
# is implemented in solve(). Probably a CRootOf solution should fall
# somewhere between a normal solution and an unsolvable expression.
# First, see if they are already solved
if sol.lhs == func and not sol.rhs.has(func) or \
sol.rhs == func and not sol.lhs.has(func):
return -2
# We are not so lucky, try solving manually
if trysolving:
try:
sols = solve(sol, func)
if not sols:
raise NotImplementedError
except NotImplementedError:
pass
else:
return -1
# Finally, a naive computation based on the length of the string version
# of the expression. This may favor combined fractions because they
# will not have duplicate denominators, and may slightly favor expressions
# with fewer additions and subtractions, as those are separated by spaces
# by the printer.
# Additional ideas for simplicity heuristics are welcome, like maybe
# checking if a equation has a larger domain, or if constantsimp has
# introduced arbitrary constants numbered higher than the order of a
# given ODE that sol is a solution of.
return len(str(sol))
def _get_constant_subexpressions(expr, Cs):
Cs = set(Cs)
Ces = []
def _recursive_walk(expr):
expr_syms = expr.free_symbols
if expr_syms and expr_syms.issubset(Cs):
Ces.append(expr)
else:
if expr.func == exp:
expr = expr.expand(mul=True)
if expr.func in (Add, Mul):
d = sift(expr.args, lambda i : i.free_symbols.issubset(Cs))
if len(d[True]) > 1:
x = expr.func(*d[True])
if not x.is_number:
Ces.append(x)
elif isinstance(expr, Integral):
if expr.free_symbols.issubset(Cs) and \
all(len(x) == 3 for x in expr.limits):
Ces.append(expr)
for i in expr.args:
_recursive_walk(i)
return
_recursive_walk(expr)
return Ces
def __remove_linear_redundancies(expr, Cs):
cnts = {i: expr.count(i) for i in Cs}
Cs = [i for i in Cs if cnts[i] > 0]
def _linear(expr):
if isinstance(expr, Add):
xs = [i for i in Cs if expr.count(i)==cnts[i] \
and 0 == expr.diff(i, 2)]
d = {}
for x in xs:
y = expr.diff(x)
if y not in d:
d[y]=[]
d[y].append(x)
for y in d:
if len(d[y]) > 1:
d[y].sort(key=str)
for x in d[y][1:]:
expr = expr.subs(x, 0)
return expr
def _recursive_walk(expr):
if len(expr.args) != 0:
expr = expr.func(*[_recursive_walk(i) for i in expr.args])
expr = _linear(expr)
return expr
if isinstance(expr, Equality):
lhs, rhs = [_recursive_walk(i) for i in expr.args]
f = lambda i: isinstance(i, Number) or i in Cs
if isinstance(lhs, Symbol) and lhs in Cs:
rhs, lhs = lhs, rhs
if lhs.func in (Add, Symbol) and rhs.func in (Add, Symbol):
dlhs = sift([lhs] if isinstance(lhs, AtomicExpr) else lhs.args, f)
drhs = sift([rhs] if isinstance(rhs, AtomicExpr) else rhs.args, f)
for i in [True, False]:
for hs in [dlhs, drhs]:
if i not in hs:
hs[i] = [0]
# this calculation can be simplified
lhs = Add(*dlhs[False]) - Add(*drhs[False])
rhs = Add(*drhs[True]) - Add(*dlhs[True])
elif lhs.func in (Mul, Symbol) and rhs.func in (Mul, Symbol):
dlhs = sift([lhs] if isinstance(lhs, AtomicExpr) else lhs.args, f)
if True in dlhs:
if False not in dlhs:
dlhs[False] = [1]
lhs = Mul(*dlhs[False])
rhs = rhs/Mul(*dlhs[True])
return Eq(lhs, rhs)
else:
return _recursive_walk(expr)
@vectorize(0)
def constantsimp(expr, constants):
r"""
Simplifies an expression with arbitrary constants in it.
This function is written specifically to work with
:py:meth:`~sympy.solvers.ode.dsolve`, and is not intended for general use.
Simplification is done by "absorbing" the arbitrary constants into other
arbitrary constants, numbers, and symbols that they are not independent
of.
The symbols must all have the same name with numbers after it, for
example, ``C1``, ``C2``, ``C3``. The ``symbolname`` here would be
'``C``', the ``startnumber`` would be 1, and the ``endnumber`` would be 3.
If the arbitrary constants are independent of the variable ``x``, then the
independent symbol would be ``x``. There is no need to specify the
dependent function, such as ``f(x)``, because it already has the
independent symbol, ``x``, in it.
Because terms are "absorbed" into arbitrary constants and because
constants are renumbered after simplifying, the arbitrary constants in
expr are not necessarily equal to the ones of the same name in the
returned result.
If two or more arbitrary constants are added, multiplied, or raised to the
power of each other, they are first absorbed together into a single
arbitrary constant. Then the new constant is combined into other terms if
necessary.
Absorption of constants is done with limited assistance:
1. terms of :py:class:`~sympy.core.add.Add`\s are collected to try join
constants so `e^x (C_1 \cos(x) + C_2 \cos(x))` will simplify to `e^x
C_1 \cos(x)`;
2. powers with exponents that are :py:class:`~sympy.core.add.Add`\s are
expanded so `e^{C_1 + x}` will be simplified to `C_1 e^x`.
Use :py:meth:`~sympy.solvers.ode.constant_renumber` to renumber constants
after simplification or else arbitrary numbers on constants may appear,
e.g. `C_1 + C_3 x`.
In rare cases, a single constant can be "simplified" into two constants.
Every differential equation solution should have as many arbitrary
constants as the order of the differential equation. The result here will
be technically correct, but it may, for example, have `C_1` and `C_2` in
an expression, when `C_1` is actually equal to `C_2`. Use your discretion
in such situations, and also take advantage of the ability to use hints in
:py:meth:`~sympy.solvers.ode.dsolve`.
Examples
========
>>> from sympy import symbols
>>> from sympy.solvers.ode import constantsimp
>>> C1, C2, C3, x, y = symbols('C1, C2, C3, x, y')
>>> constantsimp(2*C1*x, {C1, C2, C3})
C1*x
>>> constantsimp(C1 + 2 + x, {C1, C2, C3})
C1 + x
>>> constantsimp(C1*C2 + 2 + C2 + C3*x, {C1, C2, C3})
C1 + C3*x
"""
# This function works recursively. The idea is that, for Mul,
# Add, Pow, and Function, if the class has a constant in it, then
# we can simplify it, which we do by recursing down and
# simplifying up. Otherwise, we can skip that part of the
# expression.
Cs = constants
orig_expr = expr
constant_subexprs = _get_constant_subexpressions(expr, Cs)
for xe in constant_subexprs:
xes = list(xe.free_symbols)
if not xes:
continue
if all([expr.count(c) == xe.count(c) for c in xes]):
xes.sort(key=str)
expr = expr.subs(xe, xes[0])
# try to perform common sub-expression elimination of constant terms
try:
commons, rexpr = cse(expr)
commons.reverse()
rexpr = rexpr[0]
for s in commons:
cs = list(s[1].atoms(Symbol))
if len(cs) == 1 and cs[0] in Cs and \
cs[0] not in rexpr.atoms(Symbol) and \
not any(cs[0] in ex for ex in commons if ex != s):
rexpr = rexpr.subs(s[0], cs[0])
else:
rexpr = rexpr.subs(*s)
expr = rexpr
except Exception:
pass
expr = __remove_linear_redundancies(expr, Cs)
def _conditional_term_factoring(expr):
new_expr = terms_gcd(expr, clear=False, deep=True, expand=False)
# we do not want to factor exponentials, so handle this separately
if new_expr.is_Mul:
infac = False
asfac = False
for m in new_expr.args:
if isinstance(m, exp):
asfac = True
elif m.is_Add:
infac = any(isinstance(fi, exp) for t in m.args
for fi in Mul.make_args(t))
if asfac and infac:
new_expr = expr
break
return new_expr
expr = _conditional_term_factoring(expr)
# call recursively if more simplification is possible
if orig_expr != expr:
return constantsimp(expr, Cs)
return expr
def constant_renumber(expr, variables=None, newconstants=None):
r"""
Renumber arbitrary constants in ``expr`` to use the symbol names as given
in ``newconstants``. In the process, this reorders expression terms in a
standard way.
If ``newconstants`` is not provided then the new constant names will be
``C1``, ``C2`` etc. Otherwise ``newconstants`` should be an iterable
giving the new symbols to use for the constants in order.
The ``variables`` argument is a list of non-constant symbols. All other
free symbols found in ``expr`` are assumed to be constants and will be
renumbered. If ``variables`` is not given then any numbered symbol
beginning with ``C`` (e.g. ``C1``) is assumed to be a constant.
Symbols are renumbered based on ``.sort_key()``, so they should be
numbered roughly in the order that they appear in the final, printed
expression. Note that this ordering is based in part on hashes, so it can
produce different results on different machines.
The structure of this function is very similar to that of
:py:meth:`~sympy.solvers.ode.constantsimp`.
Examples
========
>>> from sympy import symbols, Eq, pprint
>>> from sympy.solvers.ode import constant_renumber
>>> x, C1, C2, C3 = symbols('x,C1:4')
>>> expr = C3 + C2*x + C1*x**2
>>> expr
C1*x**2 + C2*x + C3
>>> constant_renumber(expr)
C1 + C2*x + C3*x**2
The ``variables`` argument specifies which are constants so that the
other symbols will not be renumbered:
>>> constant_renumber(expr, [C1, x])
C1*x**2 + C2 + C3*x
The ``newconstants`` argument is used to specify what symbols to use when
replacing the constants:
>>> constant_renumber(expr, [x], newconstants=symbols('E1:4'))
E1 + E2*x + E3*x**2
"""
if type(expr) in (set, list, tuple):
renumbered = [constant_renumber(e, variables, newconstants) for e in expr]
return type(expr)(renumbered)
# Symbols in solution but not ODE are constants
if variables is not None:
variables = set(variables)
constantsymbols = list(expr.free_symbols - variables)
# Any Cn is a constant...
else:
variables = set()
isconstant = lambda s: s.startswith('C') and s[1:].isdigit()
constantsymbols = [sym for sym in expr.free_symbols if isconstant(sym.name)]
# Find new constants checking that they aren't already in the ODE
if newconstants is None:
iter_constants = numbered_symbols(start=1, prefix='C', exclude=variables)
else:
iter_constants = (sym for sym in newconstants if sym not in variables)
global newstartnumber
newstartnumber = 1
endnumber = len(constantsymbols)
constants_found = [None]*(endnumber + 2)
# make a mapping to send all constantsymbols to S.One and use
# that to make sure that term ordering is not dependent on
# the indexed value of C
C_1 = [(ci, S.One) for ci in constantsymbols]
sort_key=lambda arg: default_sort_key(arg.subs(C_1))
def _constant_renumber(expr):
r"""
We need to have an internal recursive function so that
newstartnumber maintains its values throughout recursive calls.
"""
# FIXME: Use nonlocal here when support for Py2 is dropped:
global newstartnumber
if isinstance(expr, Equality):
return Eq(
_constant_renumber(expr.lhs),
_constant_renumber(expr.rhs))
if type(expr) not in (Mul, Add, Pow) and not expr.is_Function and \
not expr.has(*constantsymbols):
# Base case, as above. Hope there aren't constants inside
# of some other class, because they won't be renumbered.
return expr
elif expr.is_Piecewise:
return expr
elif expr in constantsymbols:
if expr not in constants_found:
constants_found[newstartnumber] = expr
newstartnumber += 1
return expr
elif expr.is_Function or expr.is_Pow or isinstance(expr, Tuple):
return expr.func(
*[_constant_renumber(x) for x in expr.args])
else:
sortedargs = list(expr.args)
sortedargs.sort(key=sort_key)
return expr.func(*[_constant_renumber(x) for x in sortedargs])
expr = _constant_renumber(expr)
# Don't renumber symbols present in the ODE.
constants_found = [c for c in constants_found if c not in variables]
# Renumbering happens here
expr = expr.subs(zip(constants_found[1:], iter_constants), simultaneous=True)
return expr
def _handle_Integral(expr, func, hint):
r"""
Converts a solution with Integrals in it into an actual solution.
For most hints, this simply runs ``expr.doit()``.
"""
global y
x = func.args[0]
f = func.func
if hint == "1st_exact":
sol = (expr.doit()).subs(y, f(x))
del y
elif hint == "1st_exact_Integral":
sol = Eq(Subs(expr.lhs, y, f(x)), expr.rhs)
del y
elif hint == "nth_linear_constant_coeff_homogeneous":
sol = expr
elif not hint.endswith("_Integral"):
sol = expr.doit()
else:
sol = expr
return sol
def _ode_factorable_match(eq, func, x0):
from sympy.polys.polytools import factor
eqs = factor(eq)
eqs = fraction(eqs)[0] # p/q =0, So we need to solve only p=0
eqns = []
r = None
if isinstance(eqs, Pow):
# if f(x)**p=0 then f(x)=0 (p>0)
if (expr.exp).is_positive:
eq = expr.base
if isinstance(eq, Pow):
return None
else:
r = _ode_factorable_match(eq, func, x0)
if r is None:
r = {'eqns' : [eq], 'x0': x0}
return r
if isinstance(eqs, Mul):
fac = eqs.args
for i in fac:
if i.has(func):
eqns.append(i)
if len(eqns)>0:
r = {'eqns' : eqns, 'x0' : x0}
return r
# FIXME: replace the general solution in the docstring with
# dsolve(equation, hint='1st_exact_Integral'). You will need to be able
# to have assumptions on P and Q that dP/dy = dQ/dx.
def ode_1st_exact(eq, func, order, match):
r"""
Solves 1st order exact ordinary differential equations.
A 1st order differential equation is called exact if it is the total
differential of a function. That is, the differential equation
.. math:: P(x, y) \,\partial{}x + Q(x, y) \,\partial{}y = 0
is exact if there is some function `F(x, y)` such that `P(x, y) =
\partial{}F/\partial{}x` and `Q(x, y) = \partial{}F/\partial{}y`. It can
be shown that a necessary and sufficient condition for a first order ODE
to be exact is that `\partial{}P/\partial{}y = \partial{}Q/\partial{}x`.
Then, the solution will be as given below::
>>> from sympy import Function, Eq, Integral, symbols, pprint
>>> x, y, t, x0, y0, C1= symbols('x,y,t,x0,y0,C1')
>>> P, Q, F= map(Function, ['P', 'Q', 'F'])
>>> pprint(Eq(Eq(F(x, y), Integral(P(t, y), (t, x0, x)) +
... Integral(Q(x0, t), (t, y0, y))), C1))
x y
/ /
| |
F(x, y) = | P(t, y) dt + | Q(x0, t) dt = C1
| |
/ /
x0 y0
Where the first partials of `P` and `Q` exist and are continuous in a
simply connected region.
A note: SymPy currently has no way to represent inert substitution on an
expression, so the hint ``1st_exact_Integral`` will return an integral
with `dy`. This is supposed to represent the function that you are
solving for.
Examples
========
>>> from sympy import Function, dsolve, cos, sin
>>> from sympy.abc import x
>>> f = Function('f')
>>> dsolve(cos(f(x)) - (x*sin(f(x)) - f(x)**2)*f(x).diff(x),
... f(x), hint='1st_exact')
Eq(x*cos(f(x)) + f(x)**3/3, C1)
References
==========
- https://en.wikipedia.org/wiki/Exact_differential_equation
- M. Tenenbaum & H. Pollard, "Ordinary Differential Equations",
Dover 1963, pp. 73
# indirect doctest
"""
x = func.args[0]
r = match # d+e*diff(f(x),x)
e = r[r['e']]
d = r[r['d']]
global y # This is the only way to pass dummy y to _handle_Integral
y = r['y']
C1 = get_numbered_constants(eq, num=1)
# Refer Joel Moses, "Symbolic Integration - The Stormy Decade",
# Communications of the ACM, Volume 14, Number 8, August 1971, pp. 558
# which gives the method to solve an exact differential equation.
sol = Integral(d, x) + Integral((e - (Integral(d, x).diff(y))), y)
return Eq(sol, C1)
def ode_1st_homogeneous_coeff_best(eq, func, order, match):
r"""
Returns the best solution to an ODE from the two hints
``1st_homogeneous_coeff_subs_dep_div_indep`` and
``1st_homogeneous_coeff_subs_indep_div_dep``.
This is as determined by :py:meth:`~sympy.solvers.ode.ode_sol_simplicity`.
See the
:py:meth:`~sympy.solvers.ode.ode_1st_homogeneous_coeff_subs_indep_div_dep`
and
:py:meth:`~sympy.solvers.ode.ode_1st_homogeneous_coeff_subs_dep_div_indep`
docstrings for more information on these hints. Note that there is no
``ode_1st_homogeneous_coeff_best_Integral`` hint.
Examples
========
>>> from sympy import Function, dsolve, pprint
>>> from sympy.abc import x
>>> f = Function('f')
>>> pprint(dsolve(2*x*f(x) + (x**2 + f(x)**2)*f(x).diff(x), f(x),
... hint='1st_homogeneous_coeff_best', simplify=False))
/ 2 \
| 3*x |
log|----- + 1|
| 2 |
\f (x) /
log(f(x)) = log(C1) - --------------
3
References
==========
- https://en.wikipedia.org/wiki/Homogeneous_differential_equation
- M. Tenenbaum & H. Pollard, "Ordinary Differential Equations",
Dover 1963, pp. 59
# indirect doctest
"""
# There are two substitutions that solve the equation, u1=y/x and u2=x/y
# They produce different integrals, so try them both and see which
# one is easier.
sol1 = ode_1st_homogeneous_coeff_subs_indep_div_dep(eq,
func, order, match)
sol2 = ode_1st_homogeneous_coeff_subs_dep_div_indep(eq,
func, order, match)
simplify = match.get('simplify', True)
if simplify:
# why is odesimp called here? Should it be at the usual spot?
sol1 = odesimp(eq, sol1, func, "1st_homogeneous_coeff_subs_indep_div_dep")
sol2 = odesimp(eq, sol2, func, "1st_homogeneous_coeff_subs_dep_div_indep")
return min([sol1, sol2], key=lambda x: ode_sol_simplicity(x, func,
trysolving=not simplify))
def ode_1st_homogeneous_coeff_subs_dep_div_indep(eq, func, order, match):
r"""
Solves a 1st order differential equation with homogeneous coefficients
using the substitution `u_1 = \frac{\text{<dependent
variable>}}{\text{<independent variable>}}`.
This is a differential equation
.. math:: P(x, y) + Q(x, y) dy/dx = 0
such that `P` and `Q` are homogeneous and of the same order. A function
`F(x, y)` is homogeneous of order `n` if `F(x t, y t) = t^n F(x, y)`.
Equivalently, `F(x, y)` can be rewritten as `G(y/x)` or `H(x/y)`. See
also the docstring of :py:meth:`~sympy.solvers.ode.homogeneous_order`.
If the coefficients `P` and `Q` in the differential equation above are
homogeneous functions of the same order, then it can be shown that the
substitution `y = u_1 x` (i.e. `u_1 = y/x`) will turn the differential
equation into an equation separable in the variables `x` and `u`. If
`h(u_1)` is the function that results from making the substitution `u_1 =
f(x)/x` on `P(x, f(x))` and `g(u_2)` is the function that results from the
substitution on `Q(x, f(x))` in the differential equation `P(x, f(x)) +
Q(x, f(x)) f'(x) = 0`, then the general solution is::
>>> from sympy import Function, dsolve, pprint
>>> from sympy.abc import x
>>> f, g, h = map(Function, ['f', 'g', 'h'])
>>> genform = g(f(x)/x) + h(f(x)/x)*f(x).diff(x)
>>> pprint(genform)
/f(x)\ /f(x)\ d
g|----| + h|----|*--(f(x))
\ x / \ x / dx
>>> pprint(dsolve(genform, f(x),
... hint='1st_homogeneous_coeff_subs_dep_div_indep_Integral'))
f(x)
----
x
/
|
| -h(u1)
log(x) = C1 + | ---------------- d(u1)
| u1*h(u1) + g(u1)
|
/
Where `u_1 h(u_1) + g(u_1) \ne 0` and `x \ne 0`.
See also the docstrings of
:py:meth:`~sympy.solvers.ode.ode_1st_homogeneous_coeff_best` and
:py:meth:`~sympy.solvers.ode.ode_1st_homogeneous_coeff_subs_indep_div_dep`.
Examples
========
>>> from sympy import Function, dsolve
>>> from sympy.abc import x
>>> f = Function('f')
>>> pprint(dsolve(2*x*f(x) + (x**2 + f(x)**2)*f(x).diff(x), f(x),
... hint='1st_homogeneous_coeff_subs_dep_div_indep', simplify=False))
/ 3 \
|3*f(x) f (x)|
log|------ + -----|
| x 3 |
\ x /
log(x) = log(C1) - -------------------
3
References
==========
- https://en.wikipedia.org/wiki/Homogeneous_differential_equation
- M. Tenenbaum & H. Pollard, "Ordinary Differential Equations",
Dover 1963, pp. 59
# indirect doctest
"""
x = func.args[0]
f = func.func
u = Dummy('u')
u1 = Dummy('u1') # u1 == f(x)/x
r = match # d+e*diff(f(x),x)
C1 = get_numbered_constants(eq, num=1)
xarg = match.get('xarg', 0)
yarg = match.get('yarg', 0)
int = Integral(
(-r[r['e']]/(r[r['d']] + u1*r[r['e']])).subs({x: 1, r['y']: u1}),
(u1, None, f(x)/x))
sol = logcombine(Eq(log(x), int + log(C1)), force=True)
sol = sol.subs(f(x), u).subs(((u, u - yarg), (x, x - xarg), (u, f(x))))
return sol
def ode_1st_homogeneous_coeff_subs_indep_div_dep(eq, func, order, match):
r"""
Solves a 1st order differential equation with homogeneous coefficients
using the substitution `u_2 = \frac{\text{<independent
variable>}}{\text{<dependent variable>}}`.
This is a differential equation
.. math:: P(x, y) + Q(x, y) dy/dx = 0
such that `P` and `Q` are homogeneous and of the same order. A function
`F(x, y)` is homogeneous of order `n` if `F(x t, y t) = t^n F(x, y)`.
Equivalently, `F(x, y)` can be rewritten as `G(y/x)` or `H(x/y)`. See
also the docstring of :py:meth:`~sympy.solvers.ode.homogeneous_order`.
If the coefficients `P` and `Q` in the differential equation above are
homogeneous functions of the same order, then it can be shown that the
substitution `x = u_2 y` (i.e. `u_2 = x/y`) will turn the differential
equation into an equation separable in the variables `y` and `u_2`. If
`h(u_2)` is the function that results from making the substitution `u_2 =
x/f(x)` on `P(x, f(x))` and `g(u_2)` is the function that results from the
substitution on `Q(x, f(x))` in the differential equation `P(x, f(x)) +
Q(x, f(x)) f'(x) = 0`, then the general solution is:
>>> from sympy import Function, dsolve, pprint
>>> from sympy.abc import x
>>> f, g, h = map(Function, ['f', 'g', 'h'])
>>> genform = g(x/f(x)) + h(x/f(x))*f(x).diff(x)
>>> pprint(genform)
/ x \ / x \ d
g|----| + h|----|*--(f(x))
\f(x)/ \f(x)/ dx
>>> pprint(dsolve(genform, f(x),
... hint='1st_homogeneous_coeff_subs_indep_div_dep_Integral'))
x
----
f(x)
/
|
| -g(u2)
| ---------------- d(u2)
| u2*g(u2) + h(u2)
|
/
<BLANKLINE>
f(x) = C1*e
Where `u_2 g(u_2) + h(u_2) \ne 0` and `f(x) \ne 0`.
See also the docstrings of
:py:meth:`~sympy.solvers.ode.ode_1st_homogeneous_coeff_best` and
:py:meth:`~sympy.solvers.ode.ode_1st_homogeneous_coeff_subs_dep_div_indep`.
Examples
========
>>> from sympy import Function, pprint, dsolve
>>> from sympy.abc import x
>>> f = Function('f')
>>> pprint(dsolve(2*x*f(x) + (x**2 + f(x)**2)*f(x).diff(x), f(x),
... hint='1st_homogeneous_coeff_subs_indep_div_dep',
... simplify=False))
/ 2 \
| 3*x |
log|----- + 1|
| 2 |
\f (x) /
log(f(x)) = log(C1) - --------------
3
References
==========
- https://en.wikipedia.org/wiki/Homogeneous_differential_equation
- M. Tenenbaum & H. Pollard, "Ordinary Differential Equations",
Dover 1963, pp. 59
# indirect doctest
"""
x = func.args[0]
f = func.func
u = Dummy('u')
u2 = Dummy('u2') # u2 == x/f(x)
r = match # d+e*diff(f(x),x)
C1 = get_numbered_constants(eq, num=1)
xarg = match.get('xarg', 0) # If xarg present take xarg, else zero
yarg = match.get('yarg', 0) # If yarg present take yarg, else zero
int = Integral(
simplify(
(-r[r['d']]/(r[r['e']] + u2*r[r['d']])).subs({x: u2, r['y']: 1})),
(u2, None, x/f(x)))
sol = logcombine(Eq(log(f(x)), int + log(C1)), force=True)
sol = sol.subs(f(x), u).subs(((u, u - yarg), (x, x - xarg), (u, f(x))))
return sol
# XXX: Should this function maybe go somewhere else?
def homogeneous_order(eq, *symbols):
r"""
Returns the order `n` if `g` is homogeneous and ``None`` if it is not
homogeneous.
Determines if a function is homogeneous and if so of what order. A
function `f(x, y, \cdots)` is homogeneous of order `n` if `f(t x, t y,
\cdots) = t^n f(x, y, \cdots)`.
If the function is of two variables, `F(x, y)`, then `f` being homogeneous
of any order is equivalent to being able to rewrite `F(x, y)` as `G(x/y)`
or `H(y/x)`. This fact is used to solve 1st order ordinary differential
equations whose coefficients are homogeneous of the same order (see the
docstrings of
:py:meth:`~solvers.ode.ode_1st_homogeneous_coeff_subs_dep_div_indep` and
:py:meth:`~solvers.ode.ode_1st_homogeneous_coeff_subs_indep_div_dep`).
Symbols can be functions, but every argument of the function must be a
symbol, and the arguments of the function that appear in the expression
must match those given in the list of symbols. If a declared function
appears with different arguments than given in the list of symbols,
``None`` is returned.
Examples
========
>>> from sympy import Function, homogeneous_order, sqrt
>>> from sympy.abc import x, y
>>> f = Function('f')
>>> homogeneous_order(f(x), f(x)) is None
True
>>> homogeneous_order(f(x,y), f(y, x), x, y) is None
True
>>> homogeneous_order(f(x), f(x), x)
1
>>> homogeneous_order(x**2*f(x)/sqrt(x**2+f(x)**2), x, f(x))
2
>>> homogeneous_order(x**2+f(x), x, f(x)) is None
True
"""
if not symbols:
raise ValueError("homogeneous_order: no symbols were given.")
symset = set(symbols)
eq = sympify(eq)
# The following are not supported
if eq.has(Order, Derivative):
return None
# These are all constants
if (eq.is_Number or
eq.is_NumberSymbol or
eq.is_number
):
return S.Zero
# Replace all functions with dummy variables
dum = numbered_symbols(prefix='d', cls=Dummy)
newsyms = set()
for i in [j for j in symset if getattr(j, 'is_Function')]:
iargs = set(i.args)
if iargs.difference(symset):
return None
else:
dummyvar = next(dum)
eq = eq.subs(i, dummyvar)
symset.remove(i)
newsyms.add(dummyvar)
symset.update(newsyms)
if not eq.free_symbols & symset:
return None
# assuming order of a nested function can only be equal to zero
if isinstance(eq, Function):
return None if homogeneous_order(
eq.args[0], *tuple(symset)) != 0 else S.Zero
# make the replacement of x with x*t and see if t can be factored out
t = Dummy('t', positive=True) # It is sufficient that t > 0
eqs = separatevars(eq.subs([(i, t*i) for i in symset]), [t], dict=True)[t]
if eqs is S.One:
return S.Zero # there was no term with only t
i, d = eqs.as_independent(t, as_Add=False)
b, e = d.as_base_exp()
if b == t:
return e
def ode_1st_linear(eq, func, order, match):
r"""
Solves 1st order linear differential equations.
These are differential equations of the form
.. math:: dy/dx + P(x) y = Q(x)\text{.}
These kinds of differential equations can be solved in a general way. The
integrating factor `e^{\int P(x) \,dx}` will turn the equation into a
separable equation. The general solution is::
>>> from sympy import Function, dsolve, Eq, pprint, diff, sin
>>> from sympy.abc import x
>>> f, P, Q = map(Function, ['f', 'P', 'Q'])
>>> genform = Eq(f(x).diff(x) + P(x)*f(x), Q(x))
>>> pprint(genform)
d
P(x)*f(x) + --(f(x)) = Q(x)
dx
>>> pprint(dsolve(genform, f(x), hint='1st_linear_Integral'))
/ / \
| | |
| | / | /
| | | | |
| | | P(x) dx | - | P(x) dx
| | | | |
| | / | /
f(x) = |C1 + | Q(x)*e dx|*e
| | |
\ / /
Examples
========
>>> f = Function('f')
>>> pprint(dsolve(Eq(x*diff(f(x), x) - f(x), x**2*sin(x)),
... f(x), '1st_linear'))
f(x) = x*(C1 - cos(x))
References
==========
- https://en.wikipedia.org/wiki/Linear_differential_equation#First_order_equation
- M. Tenenbaum & H. Pollard, "Ordinary Differential Equations",
Dover 1963, pp. 92
# indirect doctest
"""
x = func.args[0]
f = func.func
r = match # a*diff(f(x),x) + b*f(x) + c
C1 = get_numbered_constants(eq, num=1)
t = exp(Integral(r[r['b']]/r[r['a']], x))
tt = Integral(t*(-r[r['c']]/r[r['a']]), x)
f = match.get('u', f(x)) # take almost-linear u if present, else f(x)
return Eq(f, (tt + C1)/t)
def ode_Bernoulli(eq, func, order, match):
r"""
Solves Bernoulli differential equations.
These are equations of the form
.. math:: dy/dx + P(x) y = Q(x) y^n\text{, }n \ne 1`\text{.}
The substitution `w = 1/y^{1-n}` will transform an equation of this form
into one that is linear (see the docstring of
:py:meth:`~sympy.solvers.ode.ode_1st_linear`). The general solution is::
>>> from sympy import Function, dsolve, Eq, pprint
>>> from sympy.abc import x, n
>>> f, P, Q = map(Function, ['f', 'P', 'Q'])
>>> genform = Eq(f(x).diff(x) + P(x)*f(x), Q(x)*f(x)**n)
>>> pprint(genform)
d n
P(x)*f(x) + --(f(x)) = Q(x)*f (x)
dx
>>> pprint(dsolve(genform, f(x), hint='Bernoulli_Integral'), num_columns=100)
1
-----
1 - n
// / \ \
|| | | |
|| | / | / |
|| | | | | |
|| | (1 - n)* | P(x) dx | -(1 - n)* | P(x) dx|
|| | | | | |
|| | / | / |
f(x) = ||C1 + (n - 1)* | -Q(x)*e dx|*e |
|| | | |
\\ / / /
Note that the equation is separable when `n = 1` (see the docstring of
:py:meth:`~sympy.solvers.ode.ode_separable`).
>>> pprint(dsolve(Eq(f(x).diff(x) + P(x)*f(x), Q(x)*f(x)), f(x),
... hint='separable_Integral'))
f(x)
/
| /
| 1 |
| - dy = C1 + | (-P(x) + Q(x)) dx
| y |
| /
/
Examples
========
>>> from sympy import Function, dsolve, Eq, pprint, log
>>> from sympy.abc import x
>>> f = Function('f')
>>> pprint(dsolve(Eq(x*f(x).diff(x) + f(x), log(x)*f(x)**2),
... f(x), hint='Bernoulli'))
1
f(x) = -------------------
/ log(x) 1\
x*|C1 + ------ + -|
\ x x/
References
==========
- https://en.wikipedia.org/wiki/Bernoulli_differential_equation
- M. Tenenbaum & H. Pollard, "Ordinary Differential Equations",
Dover 1963, pp. 95
# indirect doctest
"""
x = func.args[0]
f = func.func
r = match # a*diff(f(x),x) + b*f(x) + c*f(x)**n, n != 1
C1 = get_numbered_constants(eq, num=1)
t = exp((1 - r[r['n']])*Integral(r[r['b']]/r[r['a']], x))
tt = (r[r['n']] - 1)*Integral(t*r[r['c']]/r[r['a']], x)
return Eq(f(x), ((tt + C1)/t)**(1/(1 - r[r['n']])))
def ode_Riccati_special_minus2(eq, func, order, match):
r"""
The general Riccati equation has the form
.. math:: dy/dx = f(x) y^2 + g(x) y + h(x)\text{.}
While it does not have a general solution [1], the "special" form, `dy/dx
= a y^2 - b x^c`, does have solutions in many cases [2]. This routine
returns a solution for `a(dy/dx) = b y^2 + c y/x + d/x^2` that is obtained
by using a suitable change of variables to reduce it to the special form
and is valid when neither `a` nor `b` are zero and either `c` or `d` is
zero.
>>> from sympy.abc import x, y, a, b, c, d
>>> from sympy.solvers.ode import dsolve, checkodesol
>>> from sympy import pprint, Function
>>> f = Function('f')
>>> y = f(x)
>>> genform = a*y.diff(x) - (b*y**2 + c*y/x + d/x**2)
>>> sol = dsolve(genform, y)
>>> pprint(sol, wrap_line=False)
/ / __________________ \\
| __________________ | / 2 ||
| / 2 | \/ 4*b*d - (a + c) *log(x)||
-|a + c - \/ 4*b*d - (a + c) *tan|C1 + ----------------------------||
\ \ 2*a //
f(x) = ------------------------------------------------------------------------
2*b*x
>>> checkodesol(genform, sol, order=1)[0]
True
References
==========
1. http://www.maplesoft.com/support/help/Maple/view.aspx?path=odeadvisor/Riccati
2. http://eqworld.ipmnet.ru/en/solutions/ode/ode0106.pdf -
http://eqworld.ipmnet.ru/en/solutions/ode/ode0123.pdf
"""
x = func.args[0]
f = func.func
r = match # a2*diff(f(x),x) + b2*f(x) + c2*f(x)/x + d2/x**2
a2, b2, c2, d2 = [r[r[s]] for s in 'a2 b2 c2 d2'.split()]
C1 = get_numbered_constants(eq, num=1)
mu = sqrt(4*d2*b2 - (a2 - c2)**2)
return Eq(f(x), (a2 - c2 - mu*tan(mu/(2*a2)*log(x) + C1))/(2*b2*x))
def ode_Liouville(eq, func, order, match):
r"""
Solves 2nd order Liouville differential equations.
The general form of a Liouville ODE is
.. math:: \frac{d^2 y}{dx^2} + g(y) \left(\!
\frac{dy}{dx}\!\right)^2 + h(x)
\frac{dy}{dx}\text{.}
The general solution is:
>>> from sympy import Function, dsolve, Eq, pprint, diff
>>> from sympy.abc import x
>>> f, g, h = map(Function, ['f', 'g', 'h'])
>>> genform = Eq(diff(f(x),x,x) + g(f(x))*diff(f(x),x)**2 +
... h(x)*diff(f(x),x), 0)
>>> pprint(genform)
2 2
/d \ d d
g(f(x))*|--(f(x))| + h(x)*--(f(x)) + ---(f(x)) = 0
\dx / dx 2
dx
>>> pprint(dsolve(genform, f(x), hint='Liouville_Integral'))
f(x)
/ /
| |
| / | /
| | | |
| - | h(x) dx | | g(y) dy
| | | |
| / | /
C1 + C2* | e dx + | e dy = 0
| |
/ /
Examples
========
>>> from sympy import Function, dsolve, Eq, pprint
>>> from sympy.abc import x
>>> f = Function('f')
>>> pprint(dsolve(diff(f(x), x, x) + diff(f(x), x)**2/f(x) +
... diff(f(x), x)/x, f(x), hint='Liouville'))
________________ ________________
[f(x) = -\/ C1 + C2*log(x) , f(x) = \/ C1 + C2*log(x) ]
References
==========
- Goldstein and Braun, "Advanced Methods for the Solution of Differential
Equations", pp. 98
- http://www.maplesoft.com/support/help/Maple/view.aspx?path=odeadvisor/Liouville
# indirect doctest
"""
# Liouville ODE:
# f(x).diff(x, 2) + g(f(x))*(f(x).diff(x, 2))**2 + h(x)*f(x).diff(x)
# See Goldstein and Braun, "Advanced Methods for the Solution of
# Differential Equations", pg. 98, as well as
# http://www.maplesoft.com/support/help/view.aspx?path=odeadvisor/Liouville
x = func.args[0]
f = func.func
r = match # f(x).diff(x, 2) + g*f(x).diff(x)**2 + h*f(x).diff(x)
y = r['y']
C1, C2 = get_numbered_constants(eq, num=2)
int = Integral(exp(Integral(r['g'], y)), (y, None, f(x)))
sol = Eq(int + C1*Integral(exp(-Integral(r['h'], x)), x) + C2, 0)
return sol
def ode_2nd_power_series_ordinary(eq, func, order, match):
r"""
Gives a power series solution to a second order homogeneous differential
equation with polynomial coefficients at an ordinary point. A homogeneous
differential equation is of the form
.. math :: P(x)\frac{d^2y}{dx^2} + Q(x)\frac{dy}{dx} + R(x) = 0
For simplicity it is assumed that `P(x)`, `Q(x)` and `R(x)` are polynomials,
it is sufficient that `\frac{Q(x)}{P(x)}` and `\frac{R(x)}{P(x)}` exists at
`x_{0}`. A recurrence relation is obtained by substituting `y` as `\sum_{n=0}^\infty a_{n}x^{n}`,
in the differential equation, and equating the nth term. Using this relation
various terms can be generated.
Examples
========
>>> from sympy import dsolve, Function, pprint
>>> from sympy.abc import x, y
>>> f = Function("f")
>>> eq = f(x).diff(x, 2) + f(x)
>>> pprint(dsolve(eq, hint='2nd_power_series_ordinary'))
/ 4 2 \ / 2\
|x x | | x | / 6\
f(x) = C2*|-- - -- + 1| + C1*x*|1 - --| + O\x /
\24 2 / \ 6 /
References
==========
- http://tutorial.math.lamar.edu/Classes/DE/SeriesSolutions.aspx
- George E. Simmons, "Differential Equations with Applications and
Historical Notes", p.p 176 - 184
"""
x = func.args[0]
f = func.func
C0, C1 = get_numbered_constants(eq, num=2)
n = Dummy("n", integer=True)
s = Wild("s")
k = Wild("k", exclude=[x])
x0 = match.get('x0')
terms = match.get('terms', 5)
p = match[match['a3']]
q = match[match['b3']]
r = match[match['c3']]
seriesdict = {}
recurr = Function("r")
# Generating the recurrence relation which works this way:
# for the second order term the summation begins at n = 2. The coefficients
# p is multiplied with an*(n - 1)*(n - 2)*x**n-2 and a substitution is made such that
# the exponent of x becomes n.
# For example, if p is x, then the second degree recurrence term is
# an*(n - 1)*(n - 2)*x**n-1, substituting (n - 1) as n, it transforms to
# an+1*n*(n - 1)*x**n.
# A similar process is done with the first order and zeroth order term.
coefflist = [(recurr(n), r), (n*recurr(n), q), (n*(n - 1)*recurr(n), p)]
for index, coeff in enumerate(coefflist):
if coeff[1]:
f2 = powsimp(expand((coeff[1]*(x - x0)**(n - index)).subs(x, x + x0)))
if f2.is_Add:
addargs = f2.args
else:
addargs = [f2]
for arg in addargs:
powm = arg.match(s*x**k)
term = coeff[0]*powm[s]
if not powm[k].is_Symbol:
term = term.subs(n, n - powm[k].as_independent(n)[0])
startind = powm[k].subs(n, index)
# Seeing if the startterm can be reduced further.
# If it vanishes for n lesser than startind, it is
# equal to summation from n.
if startind:
for i in reversed(range(startind)):
if not term.subs(n, i):
seriesdict[term] = i
else:
seriesdict[term] = i + 1
break
else:
seriesdict[term] = S.Zero
# Stripping of terms so that the sum starts with the same number.
teq = S.Zero
suminit = seriesdict.values()
rkeys = seriesdict.keys()
req = Add(*rkeys)
if any(suminit):
maxval = max(suminit)
for term in seriesdict:
val = seriesdict[term]
if val != maxval:
for i in range(val, maxval):
teq += term.subs(n, val)
finaldict = {}
if teq:
fargs = teq.atoms(AppliedUndef)
if len(fargs) == 1:
finaldict[fargs.pop()] = 0
else:
maxf = max(fargs, key = lambda x: x.args[0])
sol = solve(teq, maxf)
if isinstance(sol, list):
sol = sol[0]
finaldict[maxf] = sol
# Finding the recurrence relation in terms of the largest term.
fargs = req.atoms(AppliedUndef)
maxf = max(fargs, key = lambda x: x.args[0])
minf = min(fargs, key = lambda x: x.args[0])
if minf.args[0].is_Symbol:
startiter = 0
else:
startiter = -minf.args[0].as_independent(n)[0]
lhs = maxf
rhs = solve(req, maxf)
if isinstance(rhs, list):
rhs = rhs[0]
# Checking how many values are already present
tcounter = len([t for t in finaldict.values() if t])
for _ in range(tcounter, terms - 3): # Assuming c0 and c1 to be arbitrary
check = rhs.subs(n, startiter)
nlhs = lhs.subs(n, startiter)
nrhs = check.subs(finaldict)
finaldict[nlhs] = nrhs
startiter += 1
# Post processing
series = C0 + C1*(x - x0)
for term in finaldict:
if finaldict[term]:
fact = term.args[0]
series += (finaldict[term].subs([(recurr(0), C0), (recurr(1), C1)])*(
x - x0)**fact)
series = collect(expand_mul(series), [C0, C1]) + Order(x**terms)
return Eq(f(x), series)
def ode_2nd_linear_airy(eq, func, order, match):
r"""
Gives solution of the Airy differential equation
.. math :: \frac{d^2y}{dx^2} + (a + b x) y(x) = 0
in terms of Airy special functions airyai and airybi.
Examples
========
>>> from sympy import dsolve, Function, pprint
>>> from sympy.abc import x
>>> f = Function("f")
>>> eq = f(x).diff(x, 2) - x*f(x)
>>> dsolve(eq)
Eq(f(x), C1*airyai(x) + C2*airybi(x))
"""
x = func.args[0]
f = func.func
C0, C1 = get_numbered_constants(eq, num=2)
b = match['b']
m = match['m']
if m.is_positive:
arg = - b/cbrt(m)**2 - cbrt(m)*x
elif m.is_negative:
arg = - b/cbrt(-m)**2 + cbrt(-m)*x
else:
arg = - b/cbrt(-m)**2 + cbrt(-m)*x
return Eq(f(x), C0*airyai(arg) + C1*airybi(arg))
def ode_2nd_power_series_regular(eq, func, order, match):
r"""
Gives a power series solution to a second order homogeneous differential
equation with polynomial coefficients at a regular point. A second order
homogeneous differential equation is of the form
.. math :: P(x)\frac{d^2y}{dx^2} + Q(x)\frac{dy}{dx} + R(x) = 0
A point is said to regular singular at `x0` if `x - x0\frac{Q(x)}{P(x)}`
and `(x - x0)^{2}\frac{R(x)}{P(x)}` are analytic at `x0`. For simplicity
`P(x)`, `Q(x)` and `R(x)` are assumed to be polynomials. The algorithm for
finding the power series solutions is:
1. Try expressing `(x - x0)P(x)` and `((x - x0)^{2})Q(x)` as power series
solutions about x0. Find `p0` and `q0` which are the constants of the
power series expansions.
2. Solve the indicial equation `f(m) = m(m - 1) + m*p0 + q0`, to obtain the
roots `m1` and `m2` of the indicial equation.
3. If `m1 - m2` is a non integer there exists two series solutions. If
`m1 = m2`, there exists only one solution. If `m1 - m2` is an integer,
then the existence of one solution is confirmed. The other solution may
or may not exist.
The power series solution is of the form `x^{m}\sum_{n=0}^\infty a_{n}x^{n}`. The
coefficients are determined by the following recurrence relation.
`a_{n} = -\frac{\sum_{k=0}^{n-1} q_{n-k} + (m + k)p_{n-k}}{f(m + n)}`. For the case
in which `m1 - m2` is an integer, it can be seen from the recurrence relation
that for the lower root `m`, when `n` equals the difference of both the
roots, the denominator becomes zero. So if the numerator is not equal to zero,
a second series solution exists.
Examples
========
>>> from sympy import dsolve, Function, pprint
>>> from sympy.abc import x, y
>>> f = Function("f")
>>> eq = x*(f(x).diff(x, 2)) + 2*(f(x).diff(x)) + x*f(x)
>>> pprint(dsolve(eq, hint='2nd_power_series_regular'))
/ 6 4 2 \
| x x x |
/ 4 2 \ C1*|- --- + -- - -- + 1|
| x x | \ 720 24 2 / / 6\
f(x) = C2*|--- - -- + 1| + ------------------------ + O\x /
\120 6 / x
References
==========
- George E. Simmons, "Differential Equations with Applications and
Historical Notes", p.p 176 - 184
"""
x = func.args[0]
f = func.func
C0, C1 = get_numbered_constants(eq, num=2)
m = Dummy("m") # for solving the indicial equation
x0 = match.get('x0')
terms = match.get('terms', 5)
p = match['p']
q = match['q']
# Generating the indicial equation
indicial = []
for term in [p, q]:
if not term.has(x):
indicial.append(term)
else:
term = series(term, n=1, x0=x0)
if isinstance(term, Order):
indicial.append(S.Zero)
else:
for arg in term.args:
if not arg.has(x):
indicial.append(arg)
break
p0, q0 = indicial
sollist = solve(m*(m - 1) + m*p0 + q0, m)
if sollist and isinstance(sollist, list) and all(
[sol.is_real for sol in sollist]):
serdict1 = {}
serdict2 = {}
if len(sollist) == 1:
# Only one series solution exists in this case.
m1 = m2 = sollist.pop()
if terms-m1-1 <= 0:
return Eq(f(x), Order(terms))
serdict1 = _frobenius(terms-m1-1, m1, p0, q0, p, q, x0, x, C0)
else:
m1 = sollist[0]
m2 = sollist[1]
if m1 < m2:
m1, m2 = m2, m1
# Irrespective of whether m1 - m2 is an integer or not, one
# Frobenius series solution exists.
serdict1 = _frobenius(terms-m1-1, m1, p0, q0, p, q, x0, x, C0)
if not (m1 - m2).is_integer:
# Second frobenius series solution exists.
serdict2 = _frobenius(terms-m2-1, m2, p0, q0, p, q, x0, x, C1)
else:
# Check if second frobenius series solution exists.
serdict2 = _frobenius(terms-m2-1, m2, p0, q0, p, q, x0, x, C1, check=m1)
if serdict1:
finalseries1 = C0
for key in serdict1:
power = int(key.name[1:])
finalseries1 += serdict1[key]*(x - x0)**power
finalseries1 = (x - x0)**m1*finalseries1
finalseries2 = S.Zero
if serdict2:
for key in serdict2:
power = int(key.name[1:])
finalseries2 += serdict2[key]*(x - x0)**power
finalseries2 += C1
finalseries2 = (x - x0)**m2*finalseries2
return Eq(f(x), collect(finalseries1 + finalseries2,
[C0, C1]) + Order(x**terms))
def ode_2nd_linear_bessel(eq, func, order, match):
r"""
Gives solution of the Bessel differential equation
.. math :: x^2 \frac{d^2y}{dx^2} + x \frac{dy}{dx} y(x) + (x^2-n^2) y(x)
if n is integer then the solution is of the form Eq(f(x), C0 besselj(n,x)
+ C1 bessely(n,x)) as both the solutions are linearly independent else if
n is a fraction then the solution is of the form Eq(f(x), C0 besselj(n,x)
+ C1 besselj(-n,x)) which can also transform into Eq(f(x), C0 besselj(n,x)
+ C1 bessely(n,x)).
Examples
========
>>> from sympy.abc import x, y, a
>>> from sympy import Symbol
>>> v = Symbol('v', positive=True)
>>> from sympy.solvers.ode import dsolve, checkodesol
>>> from sympy import pprint, Function
>>> f = Function('f')
>>> y = f(x)
>>> genform = x**2*y.diff(x, 2) + x*y.diff(x) + (x**2 - v**2)*y
>>> dsolve(genform)
Eq(f(x), C1*besselj(v, x) + C2*bessely(v, x))
References
==========
https://www.math24.net/bessel-differential-equation/
"""
x = func.args[0]
f = func.func
C0, C1 = get_numbered_constants(eq, num=2)
n = match['n']
a4 = match['a4']
c4 = match['c4']
d4 = match['d4']
b4 = match['b4']
n = sqrt(n**2 + Rational(1, 4)*(c4 - 1)**2)
return Eq(f(x), ((x**(Rational(1-c4,2)))*(C0*besselj(n/d4,a4*x**d4/d4)
+ C1*bessely(n/d4,a4*x**d4/d4))).subs(x, x-b4))
def _frobenius(n, m, p0, q0, p, q, x0, x, c, check=None):
r"""
Returns a dict with keys as coefficients and values as their values in terms of C0
"""
n = int(n)
# In cases where m1 - m2 is not an integer
m2 = check
d = Dummy("d")
numsyms = numbered_symbols("C", start=0)
numsyms = [next(numsyms) for i in range(n + 1)]
serlist = []
for ser in [p, q]:
# Order term not present
if ser.is_polynomial(x) and Poly(ser, x).degree() <= n:
if x0:
ser = ser.subs(x, x + x0)
dict_ = Poly(ser, x).as_dict()
# Order term present
else:
tseries = series(ser, x=x0, n=n+1)
# Removing order
dict_ = Poly(list(ordered(tseries.args))[: -1], x).as_dict()
# Fill in with zeros, if coefficients are zero.
for i in range(n + 1):
if (i,) not in dict_:
dict_[(i,)] = S.Zero
serlist.append(dict_)
pseries = serlist[0]
qseries = serlist[1]
indicial = d*(d - 1) + d*p0 + q0
frobdict = {}
for i in range(1, n + 1):
num = c*(m*pseries[(i,)] + qseries[(i,)])
for j in range(1, i):
sym = Symbol("C" + str(j))
num += frobdict[sym]*((m + j)*pseries[(i - j,)] + qseries[(i - j,)])
# Checking for cases when m1 - m2 is an integer. If num equals zero
# then a second Frobenius series solution cannot be found. If num is not zero
# then set constant as zero and proceed.
if m2 is not None and i == m2 - m:
if num:
return False
else:
frobdict[numsyms[i]] = S.Zero
else:
frobdict[numsyms[i]] = -num/(indicial.subs(d, m+i))
return frobdict
def _nth_order_reducible_match(eq, func):
r"""
Matches any differential equation that can be rewritten with a smaller
order. Only derivatives of ``func`` alone, wrt a single variable,
are considered, and only in them should ``func`` appear.
"""
# ODE only handles functions of 1 variable so this affirms that state
assert len(func.args) == 1
x = func.args[0]
vc = [d.variable_count[0] for d in eq.atoms(Derivative)
if d.expr == func and len(d.variable_count) == 1]
ords = [c for v, c in vc if v == x]
if len(ords) < 2:
return
smallest = min(ords)
# make sure func does not appear outside of derivatives
D = Dummy()
if eq.subs(func.diff(x, smallest), D).has(func):
return
return {'n': smallest}
def ode_nth_order_reducible(eq, func, order, match):
r"""
Solves ODEs that only involve derivatives of the dependent variable using
a substitution of the form `f^n(x) = g(x)`.
For example any second order ODE of the form `f''(x) = h(f'(x), x)` can be
transformed into a pair of 1st order ODEs `g'(x) = h(g(x), x)` and
`f'(x) = g(x)`. Usually the 1st order ODE for `g` is easier to solve. If
that gives an explicit solution for `g` then `f` is found simply by
integration.
Examples
========
>>> from sympy import Function, dsolve, Eq
>>> from sympy.abc import x
>>> f = Function('f')
>>> eq = Eq(x*f(x).diff(x)**2 + f(x).diff(x, 2), 0)
>>> dsolve(eq, f(x), hint='nth_order_reducible')
... # doctest: +NORMALIZE_WHITESPACE
Eq(f(x), C1 - sqrt(-1/C2)*log(-C2*sqrt(-1/C2) + x) + sqrt(-1/C2)*log(C2*sqrt(-1/C2) + x))
"""
x = func.args[0]
f = func.func
n = match['n']
# get a unique function name for g
names = [a.name for a in eq.atoms(AppliedUndef)]
while True:
name = Dummy().name
if name not in names:
g = Function(name)
break
w = f(x).diff(x, n)
geq = eq.subs(w, g(x))
gsol = dsolve(geq, g(x))
if not isinstance(gsol, list):
gsol = [gsol]
# Might be multiple solutions to the reduced ODE:
fsol = []
for gsoli in gsol:
fsoli = dsolve(gsoli.subs(g(x), w), f(x)) # or do integration n times
fsol.append(fsoli)
if len(fsol) == 1:
fsol = fsol[0]
return fsol
# This needs to produce an invertible function but the inverse depends
# which variable we are integrating with respect to. Since the class can
# be stored in cached results we need to ensure that we always get the
# same class back for each particular integration variable so we store these
# classes in a global dict:
_nth_algebraic_diffx_stored = {}
def _nth_algebraic_diffx(var):
cls = _nth_algebraic_diffx_stored.get(var, None)
if cls is None:
# A class that behaves like Derivative wrt var but is "invertible".
class diffx(Function):
def inverse(self):
# don't use integrate here because fx has been replaced by _t
# in the equation; integrals will not be correct while solve
# is at work.
return lambda expr: Integral(expr, var) + Dummy('C')
cls = _nth_algebraic_diffx_stored.setdefault(var, diffx)
return cls
def _nth_algebraic_match(eq, func):
r"""
Matches any differential equation that nth_algebraic can solve. Uses
`sympy.solve` but teaches it how to integrate derivatives.
This involves calling `sympy.solve` and does most of the work of finding a
solution (apart from evaluating the integrals).
"""
# The independent variable
var = func.args[0]
# Derivative that solve can handle:
diffx = _nth_algebraic_diffx(var)
# Replace derivatives wrt the independent variable with diffx
def replace(eq, var):
def expand_diffx(*args):
differand, diffs = args[0], args[1:]
toreplace = differand
for v, n in diffs:
for _ in range(n):
if v == var:
toreplace = diffx(toreplace)
else:
toreplace = Derivative(toreplace, v)
return toreplace
return eq.replace(Derivative, expand_diffx)
# Restore derivatives in solution afterwards
def unreplace(eq, var):
return eq.replace(diffx, lambda e: Derivative(e, var))
subs_eqn = replace(eq, var)
try:
# turn off simplification to protect Integrals that have
# _t instead of fx in them and would otherwise factor
# as t_*Integral(1, x)
solns = solve(subs_eqn, func, simplify=False)
except NotImplementedError:
solns = []
solns = [simplify(unreplace(soln, var)) for soln in solns]
solns = [Equality(func, soln) for soln in solns]
return {'var':var, 'solutions':solns}
def ode_nth_algebraic(eq, func, order, match):
r"""
Solves an `n`\th order ordinary differential equation using algebra and
integrals.
There is no general form for the kind of equation that this can solve. The
the equation is solved algebraically treating differentiation as an
invertible algebraic function.
Examples
========
>>> from sympy import Function, dsolve, Eq
>>> from sympy.abc import x
>>> f = Function('f')
>>> eq = Eq(f(x) * (f(x).diff(x)**2 - 1), 0)
>>> dsolve(eq, f(x), hint='nth_algebraic')
... # doctest: +NORMALIZE_WHITESPACE
[Eq(f(x), 0), Eq(f(x), C1 - x), Eq(f(x), C1 + x)]
Note that this solver can return algebraic solutions that do not have any
integration constants (f(x) = 0 in the above example).
# indirect doctest
"""
return match['solutions']
def _remove_redundant_solutions(eq, solns, order, var):
r"""
Remove redundant solutions from the set of solutions.
This function is needed because otherwise dsolve can return
redundant solutions. As an example consider:
eq = Eq((f(x).diff(x, 2))*f(x).diff(x), 0)
There are two ways to find solutions to eq. The first is to solve f(x).diff(x, 2) = 0
leading to solution f(x)=C1 + C2*x. The second is to solve the equation f(x).diff(x) = 0
leading to the solution f(x) = C1. In this particular case we then see
that the second solution is a special case of the first and we don't
want to return it.
This does not always happen. If we have
eq = Eq((f(x)**2-4)*(f(x).diff(x)-4), 0)
then we get the algebraic solution f(x) = [-2, 2] and the integral solution
f(x) = x + C1 and in this case the two solutions are not equivalent wrt
initial conditions so both should be returned.
"""
def is_special_case_of(soln1, soln2):
return _is_special_case_of(soln1, soln2, eq, order, var)
unique_solns = []
for soln1 in solns:
for soln2 in unique_solns[:]:
if is_special_case_of(soln1, soln2):
break
elif is_special_case_of(soln2, soln1):
unique_solns.remove(soln2)
else:
unique_solns.append(soln1)
return unique_solns
def _is_special_case_of(soln1, soln2, eq, order, var):
r"""
True if soln1 is found to be a special case of soln2 wrt some value of the
constants that appear in soln2. False otherwise.
"""
# The solutions returned by dsolve may be given explicitly or implicitly.
# We will equate the sol1=(soln1.rhs - soln1.lhs), sol2=(soln2.rhs - soln2.lhs)
# of the two solutions.
#
# Since this is supposed to hold for all x it also holds for derivatives.
# For an order n ode we should be able to differentiate
# each solution n times to get n+1 equations.
#
# We then try to solve those n+1 equations for the integrations constants
# in sol2. If we can find a solution that doesn't depend on x then it
# means that some value of the constants in sol1 is a special case of
# sol2 corresponding to a particular choice of the integration constants.
# In case the solution is in implicit form we subtract the sides
soln1 = soln1.rhs - soln1.lhs
soln2 = soln2.rhs - soln2.lhs
# Work for the series solution
if soln1.has(Order) and soln2.has(Order):
if soln1.getO() == soln2.getO():
soln1 = soln1.removeO()
soln2 = soln2.removeO()
else:
return False
elif soln1.has(Order) or soln2.has(Order):
return False
constants1 = soln1.free_symbols.difference(eq.free_symbols)
constants2 = soln2.free_symbols.difference(eq.free_symbols)
constants1_new = get_numbered_constants(soln1 - soln2, len(constants1))
if len(constants1) == 1:
constants1_new = {constants1_new}
for c_old, c_new in zip(constants1, constants1_new):
soln1 = soln1.subs(c_old, c_new)
# n equations for sol1 = sol2, sol1'=sol2', ...
lhs = soln1
rhs = soln2
eqns = [Eq(lhs, rhs)]
for n in range(1, order):
lhs = lhs.diff(var)
rhs = rhs.diff(var)
eq = Eq(lhs, rhs)
eqns.append(eq)
# BooleanTrue/False awkwardly show up for trivial equations
if any(isinstance(eq, BooleanFalse) for eq in eqns):
return False
eqns = [eq for eq in eqns if not isinstance(eq, BooleanTrue)]
try:
constant_solns = solve(eqns, constants2)
except NotImplementedError:
return False
# Sometimes returns a dict and sometimes a list of dicts
if isinstance(constant_solns, dict):
constant_solns = [constant_solns]
# after solving the issue 17418, maybe we don't need the following checksol code.
for constant_soln in constant_solns:
for eq in eqns:
eq=eq.rhs-eq.lhs
if checksol(eq, constant_soln) is not True:
return False
# If any solution gives all constants as expressions that don't depend on
# x then there exists constants for soln2 that give soln1
for constant_soln in constant_solns:
if not any(c.has(var) for c in constant_soln.values()):
return True
return False
def _nth_linear_match(eq, func, order):
r"""
Matches a differential equation to the linear form:
.. math:: a_n(x) y^{(n)} + \cdots + a_1(x)y' + a_0(x) y + B(x) = 0
Returns a dict of order:coeff terms, where order is the order of the
derivative on each term, and coeff is the coefficient of that derivative.
The key ``-1`` holds the function `B(x)`. Returns ``None`` if the ODE is
not linear. This function assumes that ``func`` has already been checked
to be good.
Examples
========
>>> from sympy import Function, cos, sin
>>> from sympy.abc import x
>>> from sympy.solvers.ode import _nth_linear_match
>>> f = Function('f')
>>> _nth_linear_match(f(x).diff(x, 3) + 2*f(x).diff(x) +
... x*f(x).diff(x, 2) + cos(x)*f(x).diff(x) + x - f(x) -
... sin(x), f(x), 3)
{-1: x - sin(x), 0: -1, 1: cos(x) + 2, 2: x, 3: 1}
>>> _nth_linear_match(f(x).diff(x, 3) + 2*f(x).diff(x) +
... x*f(x).diff(x, 2) + cos(x)*f(x).diff(x) + x - f(x) -
... sin(f(x)), f(x), 3) == None
True
"""
x = func.args[0]
one_x = {x}
terms = {i: S.Zero for i in range(-1, order + 1)}
for i in Add.make_args(eq):
if not i.has(func):
terms[-1] += i
else:
c, f = i.as_independent(func)
if (isinstance(f, Derivative)
and set(f.variables) == one_x
and f.args[0] == func):
terms[f.derivative_count] += c
elif f == func:
terms[len(f.args[1:])] += c
else:
return None
return terms
def ode_nth_linear_euler_eq_homogeneous(eq, func, order, match, returns='sol'):
r"""
Solves an `n`\th order linear homogeneous variable-coefficient
Cauchy-Euler equidimensional ordinary differential equation.
This is an equation with form `0 = a_0 f(x) + a_1 x f'(x) + a_2 x^2 f''(x)
\cdots`.
These equations can be solved in a general manner, by substituting
solutions of the form `f(x) = x^r`, and deriving a characteristic equation
for `r`. When there are repeated roots, we include extra terms of the
form `C_{r k} \ln^k(x) x^r`, where `C_{r k}` is an arbitrary integration
constant, `r` is a root of the characteristic equation, and `k` ranges
over the multiplicity of `r`. In the cases where the roots are complex,
solutions of the form `C_1 x^a \sin(b \log(x)) + C_2 x^a \cos(b \log(x))`
are returned, based on expansions with Euler's formula. The general
solution is the sum of the terms found. If SymPy cannot find exact roots
to the characteristic equation, a
:py:class:`~sympy.polys.rootoftools.CRootOf` instance will be returned
instead.
>>> from sympy import Function, dsolve, Eq
>>> from sympy.abc import x
>>> f = Function('f')
>>> dsolve(4*x**2*f(x).diff(x, 2) + f(x), f(x),
... hint='nth_linear_euler_eq_homogeneous')
... # doctest: +NORMALIZE_WHITESPACE
Eq(f(x), sqrt(x)*(C1 + C2*log(x)))
Note that because this method does not involve integration, there is no
``nth_linear_euler_eq_homogeneous_Integral`` hint.
The following is for internal use:
- ``returns = 'sol'`` returns the solution to the ODE.
- ``returns = 'list'`` returns a list of linearly independent solutions,
corresponding to the fundamental solution set, for use with non
homogeneous solution methods like variation of parameters and
undetermined coefficients. Note that, though the solutions should be
linearly independent, this function does not explicitly check that. You
can do ``assert simplify(wronskian(sollist)) != 0`` to check for linear
independence. Also, ``assert len(sollist) == order`` will need to pass.
- ``returns = 'both'``, return a dictionary ``{'sol': <solution to ODE>,
'list': <list of linearly independent solutions>}``.
Examples
========
>>> from sympy import Function, dsolve, pprint
>>> from sympy.abc import x
>>> f = Function('f')
>>> eq = f(x).diff(x, 2)*x**2 - 4*f(x).diff(x)*x + 6*f(x)
>>> pprint(dsolve(eq, f(x),
... hint='nth_linear_euler_eq_homogeneous'))
2
f(x) = x *(C1 + C2*x)
References
==========
- https://en.wikipedia.org/wiki/Cauchy%E2%80%93Euler_equation
- C. Bender & S. Orszag, "Advanced Mathematical Methods for Scientists and
Engineers", Springer 1999, pp. 12
# indirect doctest
"""
global collectterms
collectterms = []
x = func.args[0]
f = func.func
r = match
# First, set up characteristic equation.
chareq, symbol = S.Zero, Dummy('x')
for i in r.keys():
if not isinstance(i, string_types) and i >= 0:
chareq += (r[i]*diff(x**symbol, x, i)*x**-symbol).expand()
chareq = Poly(chareq, symbol)
chareqroots = [rootof(chareq, k) for k in range(chareq.degree())]
# A generator of constants
constants = list(get_numbered_constants(eq, num=chareq.degree()*2))
constants.reverse()
# Create a dict root: multiplicity or charroots
charroots = defaultdict(int)
for root in chareqroots:
charroots[root] += 1
gsol = S.Zero
# We need keep track of terms so we can run collect() at the end.
# This is necessary for constantsimp to work properly.
ln = log
for root, multiplicity in charroots.items():
for i in range(multiplicity):
if isinstance(root, RootOf):
gsol += (x**root) * constants.pop()
if multiplicity != 1:
raise ValueError("Value should be 1")
collectterms = [(0, root, 0)] + collectterms
elif root.is_real:
gsol += ln(x)**i*(x**root) * constants.pop()
collectterms = [(i, root, 0)] + collectterms
else:
reroot = re(root)
imroot = im(root)
gsol += ln(x)**i * (x**reroot) * (
constants.pop() * sin(abs(imroot)*ln(x))
+ constants.pop() * cos(imroot*ln(x)))
# Preserve ordering (multiplicity, real part, imaginary part)
# It will be assumed implicitly when constructing
# fundamental solution sets.
collectterms = [(i, reroot, imroot)] + collectterms
if returns == 'sol':
return Eq(f(x), gsol)
elif returns in ('list' 'both'):
# HOW TO TEST THIS CODE? (dsolve does not pass 'returns' through)
# Create a list of (hopefully) linearly independent solutions
gensols = []
# Keep track of when to use sin or cos for nonzero imroot
for i, reroot, imroot in collectterms:
if imroot == 0:
gensols.append(ln(x)**i*x**reroot)
else:
sin_form = ln(x)**i*x**reroot*sin(abs(imroot)*ln(x))
if sin_form in gensols:
cos_form = ln(x)**i*x**reroot*cos(imroot*ln(x))
gensols.append(cos_form)
else:
gensols.append(sin_form)
if returns == 'list':
return gensols
else:
return {'sol': Eq(f(x), gsol), 'list': gensols}
else:
raise ValueError('Unknown value for key "returns".')
def ode_nth_linear_euler_eq_nonhomogeneous_undetermined_coefficients(eq, func, order, match, returns='sol'):
r"""
Solves an `n`\th order linear non homogeneous Cauchy-Euler equidimensional
ordinary differential equation using undetermined coefficients.
This is an equation with form `g(x) = a_0 f(x) + a_1 x f'(x) + a_2 x^2 f''(x)
\cdots`.
These equations can be solved in a general manner, by substituting
solutions of the form `x = exp(t)`, and deriving a characteristic equation
of form `g(exp(t)) = b_0 f(t) + b_1 f'(t) + b_2 f''(t) \cdots` which can
be then solved by nth_linear_constant_coeff_undetermined_coefficients if
g(exp(t)) has finite number of linearly independent derivatives.
Functions that fit this requirement are finite sums functions of the form
`a x^i e^{b x} \sin(c x + d)` or `a x^i e^{b x} \cos(c x + d)`, where `i`
is a non-negative integer and `a`, `b`, `c`, and `d` are constants. For
example any polynomial in `x`, functions like `x^2 e^{2 x}`, `x \sin(x)`,
and `e^x \cos(x)` can all be used. Products of `\sin`'s and `\cos`'s have
a finite number of derivatives, because they can be expanded into `\sin(a
x)` and `\cos(b x)` terms. However, SymPy currently cannot do that
expansion, so you will need to manually rewrite the expression in terms of
the above to use this method. So, for example, you will need to manually
convert `\sin^2(x)` into `(1 + \cos(2 x))/2` to properly apply the method
of undetermined coefficients on it.
After replacement of x by exp(t), this method works by creating a trial function
from the expression and all of its linear independent derivatives and
substituting them into the original ODE. The coefficients for each term
will be a system of linear equations, which are be solved for and
substituted, giving the solution. If any of the trial functions are linearly
dependent on the solution to the homogeneous equation, they are multiplied
by sufficient `x` to make them linearly independent.
Examples
========
>>> from sympy import dsolve, Function, Derivative, log
>>> from sympy.abc import x
>>> f = Function('f')
>>> eq = x**2*Derivative(f(x), x, x) - 2*x*Derivative(f(x), x) + 2*f(x) - log(x)
>>> dsolve(eq, f(x),
... hint='nth_linear_euler_eq_nonhomogeneous_undetermined_coefficients').expand()
Eq(f(x), C1*x + C2*x**2 + log(x)/2 + 3/4)
"""
x = func.args[0]
f = func.func
r = match
chareq, eq, symbol = S.Zero, S.Zero, Dummy('x')
for i in r.keys():
if not isinstance(i, string_types) and i >= 0:
chareq += (r[i]*diff(x**symbol, x, i)*x**-symbol).expand()
for i in range(1,degree(Poly(chareq, symbol))+1):
eq += chareq.coeff(symbol**i)*diff(f(x), x, i)
if chareq.as_coeff_add(symbol)[0]:
eq += chareq.as_coeff_add(symbol)[0]*f(x)
e, re = posify(r[-1].subs(x, exp(x)))
eq += e.subs(re)
match = _nth_linear_match(eq, f(x), ode_order(eq, f(x)))
match['trialset'] = r['trialset']
return ode_nth_linear_constant_coeff_undetermined_coefficients(eq, func, order, match).subs(x, log(x)).subs(f(log(x)), f(x)).expand()
def ode_nth_linear_euler_eq_nonhomogeneous_variation_of_parameters(eq, func, order, match, returns='sol'):
r"""
Solves an `n`\th order linear non homogeneous Cauchy-Euler equidimensional
ordinary differential equation using variation of parameters.
This is an equation with form `g(x) = a_0 f(x) + a_1 x f'(x) + a_2 x^2 f''(x)
\cdots`.
This method works by assuming that the particular solution takes the form
.. math:: \sum_{x=1}^{n} c_i(x) y_i(x) {a_n} {x^n} \text{,}
where `y_i` is the `i`\th solution to the homogeneous equation. The
solution is then solved using Wronskian's and Cramer's Rule. The
particular solution is given by multiplying eq given below with `a_n x^{n}`
.. math:: \sum_{x=1}^n \left( \int \frac{W_i(x)}{W(x)} \,dx
\right) y_i(x) \text{,}
where `W(x)` is the Wronskian of the fundamental system (the system of `n`
linearly independent solutions to the homogeneous equation), and `W_i(x)`
is the Wronskian of the fundamental system with the `i`\th column replaced
with `[0, 0, \cdots, 0, \frac{x^{- n}}{a_n} g{\left(x \right)}]`.
This method is general enough to solve any `n`\th order inhomogeneous
linear differential equation, but sometimes SymPy cannot simplify the
Wronskian well enough to integrate it. If this method hangs, try using the
``nth_linear_constant_coeff_variation_of_parameters_Integral`` hint and
simplifying the integrals manually. Also, prefer using
``nth_linear_constant_coeff_undetermined_coefficients`` when it
applies, because it doesn't use integration, making it faster and more
reliable.
Warning, using simplify=False with
'nth_linear_constant_coeff_variation_of_parameters' in
:py:meth:`~sympy.solvers.ode.dsolve` may cause it to hang, because it will
not attempt to simplify the Wronskian before integrating. It is
recommended that you only use simplify=False with
'nth_linear_constant_coeff_variation_of_parameters_Integral' for this
method, especially if the solution to the homogeneous equation has
trigonometric functions in it.
Examples
========
>>> from sympy import Function, dsolve, Derivative
>>> from sympy.abc import x
>>> f = Function('f')
>>> eq = x**2*Derivative(f(x), x, x) - 2*x*Derivative(f(x), x) + 2*f(x) - x**4
>>> dsolve(eq, f(x),
... hint='nth_linear_euler_eq_nonhomogeneous_variation_of_parameters').expand()
Eq(f(x), C1*x + C2*x**2 + x**4/6)
"""
x = func.args[0]
f = func.func
r = match
gensol = ode_nth_linear_euler_eq_homogeneous(eq, func, order, match, returns='both')
match.update(gensol)
r[-1] = r[-1]/r[ode_order(eq, f(x))]
sol = _solve_variation_of_parameters(eq, func, order, match)
return Eq(f(x), r['sol'].rhs + (sol.rhs - r['sol'].rhs)*r[ode_order(eq, f(x))])
def ode_almost_linear(eq, func, order, match):
r"""
Solves an almost-linear differential equation.
The general form of an almost linear differential equation is
.. math:: f(x) g(y) y + k(x) l(y) + m(x) = 0
\text{where} l'(y) = g(y)\text{.}
This can be solved by substituting `l(y) = u(y)`. Making the given
substitution reduces it to a linear differential equation of the form `u'
+ P(x) u + Q(x) = 0`.
The general solution is
>>> from sympy import Function, dsolve, Eq, pprint
>>> from sympy.abc import x, y, n
>>> f, g, k, l = map(Function, ['f', 'g', 'k', 'l'])
>>> genform = Eq(f(x)*(l(y).diff(y)) + k(x)*l(y) + g(x), 0)
>>> pprint(genform)
d
f(x)*--(l(y)) + g(x) + k(x)*l(y) = 0
dy
>>> pprint(dsolve(genform, hint = 'almost_linear'))
/ // y*k(x) \\
| || ------ ||
| || f(x) || -y*k(x)
| ||-g(x)*e || --------
| ||-------------- for k(x) != 0|| f(x)
l(y) = |C1 + |< k(x) ||*e
| || ||
| || -y*g(x) ||
| || -------- otherwise ||
| || f(x) ||
\ \\ //
See Also
========
:meth:`sympy.solvers.ode.ode_1st_linear`
Examples
========
>>> from sympy import Function, Derivative, pprint
>>> from sympy.solvers.ode import dsolve, classify_ode
>>> from sympy.abc import x
>>> f = Function('f')
>>> d = f(x).diff(x)
>>> eq = x*d + x*f(x) + 1
>>> dsolve(eq, f(x), hint='almost_linear')
Eq(f(x), (C1 - Ei(x))*exp(-x))
>>> pprint(dsolve(eq, f(x), hint='almost_linear'))
-x
f(x) = (C1 - Ei(x))*e
References
==========
- Joel Moses, "Symbolic Integration - The Stormy Decade", Communications
of the ACM, Volume 14, Number 8, August 1971, pp. 558
"""
# Since ode_1st_linear has already been implemented, and the
# coefficients have been modified to the required form in
# classify_ode, just passing eq, func, order and match to
# ode_1st_linear will give the required output.
return ode_1st_linear(eq, func, order, match)
def _linear_coeff_match(expr, func):
r"""
Helper function to match hint ``linear_coefficients``.
Matches the expression to the form `(a_1 x + b_1 f(x) + c_1)/(a_2 x + b_2
f(x) + c_2)` where the following conditions hold:
1. `a_1`, `b_1`, `c_1`, `a_2`, `b_2`, `c_2` are Rationals;
2. `c_1` or `c_2` are not equal to zero;
3. `a_2 b_1 - a_1 b_2` is not equal to zero.
Return ``xarg``, ``yarg`` where
1. ``xarg`` = `(b_2 c_1 - b_1 c_2)/(a_2 b_1 - a_1 b_2)`
2. ``yarg`` = `(a_1 c_2 - a_2 c_1)/(a_2 b_1 - a_1 b_2)`
Examples
========
>>> from sympy import Function
>>> from sympy.abc import x
>>> from sympy.solvers.ode import _linear_coeff_match
>>> from sympy.functions.elementary.trigonometric import sin
>>> f = Function('f')
>>> _linear_coeff_match((
... (-25*f(x) - 8*x + 62)/(4*f(x) + 11*x - 11)), f(x))
(1/9, 22/9)
>>> _linear_coeff_match(
... sin((-5*f(x) - 8*x + 6)/(4*f(x) + x - 1)), f(x))
(19/27, 2/27)
>>> _linear_coeff_match(sin(f(x)/x), f(x))
"""
f = func.func
x = func.args[0]
def abc(eq):
r'''
Internal function of _linear_coeff_match
that returns Rationals a, b, c
if eq is a*x + b*f(x) + c, else None.
'''
eq = _mexpand(eq)
c = eq.as_independent(x, f(x), as_Add=True)[0]
if not c.is_Rational:
return
a = eq.coeff(x)
if not a.is_Rational:
return
b = eq.coeff(f(x))
if not b.is_Rational:
return
if eq == a*x + b*f(x) + c:
return a, b, c
def match(arg):
r'''
Internal function of _linear_coeff_match that returns Rationals a1,
b1, c1, a2, b2, c2 and a2*b1 - a1*b2 of the expression (a1*x + b1*f(x)
+ c1)/(a2*x + b2*f(x) + c2) if one of c1 or c2 and a2*b1 - a1*b2 is
non-zero, else None.
'''
n, d = arg.together().as_numer_denom()
m = abc(n)
if m is not None:
a1, b1, c1 = m
m = abc(d)
if m is not None:
a2, b2, c2 = m
d = a2*b1 - a1*b2
if (c1 or c2) and d:
return a1, b1, c1, a2, b2, c2, d
m = [fi.args[0] for fi in expr.atoms(Function) if fi.func != f and
len(fi.args) == 1 and not fi.args[0].is_Function] or {expr}
m1 = match(m.pop())
if m1 and all(match(mi) == m1 for mi in m):
a1, b1, c1, a2, b2, c2, denom = m1
return (b2*c1 - b1*c2)/denom, (a1*c2 - a2*c1)/denom
def ode_linear_coefficients(eq, func, order, match):
r"""
Solves a differential equation with linear coefficients.
The general form of a differential equation with linear coefficients is
.. math:: y' + F\left(\!\frac{a_1 x + b_1 y + c_1}{a_2 x + b_2 y +
c_2}\!\right) = 0\text{,}
where `a_1`, `b_1`, `c_1`, `a_2`, `b_2`, `c_2` are constants and `a_1 b_2
- a_2 b_1 \ne 0`.
This can be solved by substituting:
.. math:: x = x' + \frac{b_2 c_1 - b_1 c_2}{a_2 b_1 - a_1 b_2}
y = y' + \frac{a_1 c_2 - a_2 c_1}{a_2 b_1 - a_1
b_2}\text{.}
This substitution reduces the equation to a homogeneous differential
equation.
See Also
========
:meth:`sympy.solvers.ode.ode_1st_homogeneous_coeff_best`
:meth:`sympy.solvers.ode.ode_1st_homogeneous_coeff_subs_indep_div_dep`
:meth:`sympy.solvers.ode.ode_1st_homogeneous_coeff_subs_dep_div_indep`
Examples
========
>>> from sympy import Function, Derivative, pprint
>>> from sympy.solvers.ode import dsolve, classify_ode
>>> from sympy.abc import x
>>> f = Function('f')
>>> df = f(x).diff(x)
>>> eq = (x + f(x) + 1)*df + (f(x) - 6*x + 1)
>>> dsolve(eq, hint='linear_coefficients')
[Eq(f(x), -x - sqrt(C1 + 7*x**2) - 1), Eq(f(x), -x + sqrt(C1 + 7*x**2) - 1)]
>>> pprint(dsolve(eq, hint='linear_coefficients'))
___________ ___________
/ 2 / 2
[f(x) = -x - \/ C1 + 7*x - 1, f(x) = -x + \/ C1 + 7*x - 1]
References
==========
- Joel Moses, "Symbolic Integration - The Stormy Decade", Communications
of the ACM, Volume 14, Number 8, August 1971, pp. 558
"""
return ode_1st_homogeneous_coeff_best(eq, func, order, match)
def ode_separable_reduced(eq, func, order, match):
r"""
Solves a differential equation that can be reduced to the separable form.
The general form of this equation is
.. math:: y' + (y/x) H(x^n y) = 0\text{}.
This can be solved by substituting `u(y) = x^n y`. The equation then
reduces to the separable form `\frac{u'}{u (\mathrm{power} - H(u))} -
\frac{1}{x} = 0`.
The general solution is:
>>> from sympy import Function, dsolve, Eq, pprint
>>> from sympy.abc import x, n
>>> f, g = map(Function, ['f', 'g'])
>>> genform = f(x).diff(x) + (f(x)/x)*g(x**n*f(x))
>>> pprint(genform)
/ n \
d f(x)*g\x *f(x)/
--(f(x)) + ---------------
dx x
>>> pprint(dsolve(genform, hint='separable_reduced'))
n
x *f(x)
/
|
| 1
| ------------ dy = C1 + log(x)
| y*(n - g(y))
|
/
See Also
========
:meth:`sympy.solvers.ode.ode_separable`
Examples
========
>>> from sympy import Function, Derivative, pprint
>>> from sympy.solvers.ode import dsolve, classify_ode
>>> from sympy.abc import x
>>> f = Function('f')
>>> d = f(x).diff(x)
>>> eq = (x - x**2*f(x))*d - f(x)
>>> dsolve(eq, hint='separable_reduced')
[Eq(f(x), (1 - sqrt(C1*x**2 + 1))/x), Eq(f(x), (sqrt(C1*x**2 + 1) + 1)/x)]
>>> pprint(dsolve(eq, hint='separable_reduced'))
___________ ___________
/ 2 / 2
1 - \/ C1*x + 1 \/ C1*x + 1 + 1
[f(x) = ------------------, f(x) = ------------------]
x x
References
==========
- Joel Moses, "Symbolic Integration - The Stormy Decade", Communications
of the ACM, Volume 14, Number 8, August 1971, pp. 558
"""
# Arguments are passed in a way so that they are coherent with the
# ode_separable function
x = func.args[0]
f = func.func
y = Dummy('y')
u = match['u'].subs(match['t'], y)
ycoeff = 1/(y*(match['power'] - u))
m1 = {y: 1, x: -1/x, 'coeff': 1}
m2 = {y: ycoeff, x: 1, 'coeff': 1}
r = {'m1': m1, 'm2': m2, 'y': y, 'hint': x**match['power']*f(x)}
return ode_separable(eq, func, order, r)
def ode_1st_power_series(eq, func, order, match):
r"""
The power series solution is a method which gives the Taylor series expansion
to the solution of a differential equation.
For a first order differential equation `\frac{dy}{dx} = h(x, y)`, a power
series solution exists at a point `x = x_{0}` if `h(x, y)` is analytic at `x_{0}`.
The solution is given by
.. math:: y(x) = y(x_{0}) + \sum_{n = 1}^{\infty} \frac{F_{n}(x_{0},b)(x - x_{0})^n}{n!},
where `y(x_{0}) = b` is the value of y at the initial value of `x_{0}`.
To compute the values of the `F_{n}(x_{0},b)` the following algorithm is
followed, until the required number of terms are generated.
1. `F_1 = h(x_{0}, b)`
2. `F_{n+1} = \frac{\partial F_{n}}{\partial x} + \frac{\partial F_{n}}{\partial y}F_{1}`
Examples
========
>>> from sympy import Function, Derivative, pprint, exp
>>> from sympy.solvers.ode import dsolve
>>> from sympy.abc import x
>>> f = Function('f')
>>> eq = exp(x)*(f(x).diff(x)) - f(x)
>>> pprint(dsolve(eq, hint='1st_power_series'))
3 4 5
C1*x C1*x C1*x / 6\
f(x) = C1 + C1*x - ----- + ----- + ----- + O\x /
6 24 60
References
==========
- Travis W. Walker, Analytic power series technique for solving first-order
differential equations, p.p 17, 18
"""
x = func.args[0]
y = match['y']
f = func.func
h = -match[match['d']]/match[match['e']]
point = match.get('f0')
value = match.get('f0val')
terms = match.get('terms')
# First term
F = h
if not h:
return Eq(f(x), value)
# Initialization
series = value
if terms > 1:
hc = h.subs({x: point, y: value})
if hc.has(oo) or hc.has(NaN) or hc.has(zoo):
# Derivative does not exist, not analytic
return Eq(f(x), oo)
elif hc:
series += hc*(x - point)
for factcount in range(2, terms):
Fnew = F.diff(x) + F.diff(y)*h
Fnewc = Fnew.subs({x: point, y: value})
# Same logic as above
if Fnewc.has(oo) or Fnewc.has(NaN) or Fnewc.has(-oo) or Fnewc.has(zoo):
return Eq(f(x), oo)
series += Fnewc*((x - point)**factcount)/factorial(factcount)
F = Fnew
series += Order(x**terms)
return Eq(f(x), series)
def ode_nth_linear_constant_coeff_homogeneous(eq, func, order, match,
returns='sol'):
r"""
Solves an `n`\th order linear homogeneous differential equation with
constant coefficients.
This is an equation of the form
.. math:: a_n f^{(n)}(x) + a_{n-1} f^{(n-1)}(x) + \cdots + a_1 f'(x)
+ a_0 f(x) = 0\text{.}
These equations can be solved in a general manner, by taking the roots of
the characteristic equation `a_n m^n + a_{n-1} m^{n-1} + \cdots + a_1 m +
a_0 = 0`. The solution will then be the sum of `C_n x^i e^{r x}` terms,
for each where `C_n` is an arbitrary constant, `r` is a root of the
characteristic equation and `i` is one of each from 0 to the multiplicity
of the root - 1 (for example, a root 3 of multiplicity 2 would create the
terms `C_1 e^{3 x} + C_2 x e^{3 x}`). The exponential is usually expanded
for complex roots using Euler's equation `e^{I x} = \cos(x) + I \sin(x)`.
Complex roots always come in conjugate pairs in polynomials with real
coefficients, so the two roots will be represented (after simplifying the
constants) as `e^{a x} \left(C_1 \cos(b x) + C_2 \sin(b x)\right)`.
If SymPy cannot find exact roots to the characteristic equation, a
:py:class:`~sympy.polys.rootoftools.CRootOf` instance will be return
instead.
>>> from sympy import Function, dsolve, Eq
>>> from sympy.abc import x
>>> f = Function('f')
>>> dsolve(f(x).diff(x, 5) + 10*f(x).diff(x) - 2*f(x), f(x),
... hint='nth_linear_constant_coeff_homogeneous')
... # doctest: +NORMALIZE_WHITESPACE
Eq(f(x), C5*exp(x*CRootOf(_x**5 + 10*_x - 2, 0))
+ (C1*sin(x*im(CRootOf(_x**5 + 10*_x - 2, 1)))
+ C2*cos(x*im(CRootOf(_x**5 + 10*_x - 2, 1))))*exp(x*re(CRootOf(_x**5 + 10*_x - 2, 1)))
+ (C3*sin(x*im(CRootOf(_x**5 + 10*_x - 2, 3)))
+ C4*cos(x*im(CRootOf(_x**5 + 10*_x - 2, 3))))*exp(x*re(CRootOf(_x**5 + 10*_x - 2, 3))))
Note that because this method does not involve integration, there is no
``nth_linear_constant_coeff_homogeneous_Integral`` hint.
The following is for internal use:
- ``returns = 'sol'`` returns the solution to the ODE.
- ``returns = 'list'`` returns a list of linearly independent solutions,
for use with non homogeneous solution methods like variation of
parameters and undetermined coefficients. Note that, though the
solutions should be linearly independent, this function does not
explicitly check that. You can do ``assert simplify(wronskian(sollist))
!= 0`` to check for linear independence. Also, ``assert len(sollist) ==
order`` will need to pass.
- ``returns = 'both'``, return a dictionary ``{'sol': <solution to ODE>,
'list': <list of linearly independent solutions>}``.
Examples
========
>>> from sympy import Function, dsolve, pprint
>>> from sympy.abc import x
>>> f = Function('f')
>>> pprint(dsolve(f(x).diff(x, 4) + 2*f(x).diff(x, 3) -
... 2*f(x).diff(x, 2) - 6*f(x).diff(x) + 5*f(x), f(x),
... hint='nth_linear_constant_coeff_homogeneous'))
x -2*x
f(x) = (C1 + C2*x)*e + (C3*sin(x) + C4*cos(x))*e
References
==========
- https://en.wikipedia.org/wiki/Linear_differential_equation section:
Nonhomogeneous_equation_with_constant_coefficients
- M. Tenenbaum & H. Pollard, "Ordinary Differential Equations",
Dover 1963, pp. 211
# indirect doctest
"""
x = func.args[0]
f = func.func
r = match
# First, set up characteristic equation.
chareq, symbol = S.Zero, Dummy('x')
for i in r.keys():
if type(i) == str or i < 0:
pass
else:
chareq += r[i]*symbol**i
chareq = Poly(chareq, symbol)
# Can't just call roots because it doesn't return rootof for unsolveable
# polynomials.
chareqroots = roots(chareq, multiple=True)
if len(chareqroots) != order:
chareqroots = [rootof(chareq, k) for k in range(chareq.degree())]
chareq_is_complex = not all([i.is_real for i in chareq.all_coeffs()])
# A generator of constants
constants = list(get_numbered_constants(eq, num=chareq.degree()*2))
# Create a dict root: multiplicity or charroots
charroots = defaultdict(int)
for root in chareqroots:
charroots[root] += 1
# We need to keep track of terms so we can run collect() at the end.
# This is necessary for constantsimp to work properly.
global collectterms
collectterms = []
gensols = []
conjugate_roots = [] # used to prevent double-use of conjugate roots
# Loop over roots in theorder provided by roots/rootof...
for root in chareqroots:
# but don't repoeat multiple roots.
if root not in charroots:
continue
multiplicity = charroots.pop(root)
for i in range(multiplicity):
if chareq_is_complex:
gensols.append(x**i*exp(root*x))
collectterms = [(i, root, 0)] + collectterms
continue
reroot = re(root)
imroot = im(root)
if imroot.has(atan2) and reroot.has(atan2):
# Remove this condition when re and im stop returning
# circular atan2 usages.
gensols.append(x**i*exp(root*x))
collectterms = [(i, root, 0)] + collectterms
else:
if root in conjugate_roots:
collectterms = [(i, reroot, imroot)] + collectterms
continue
if imroot == 0:
gensols.append(x**i*exp(reroot*x))
collectterms = [(i, reroot, 0)] + collectterms
continue
conjugate_roots.append(conjugate(root))
gensols.append(x**i*exp(reroot*x) * sin(abs(imroot) * x))
gensols.append(x**i*exp(reroot*x) * cos( imroot * x))
# This ordering is important
collectterms = [(i, reroot, imroot)] + collectterms
if returns == 'list':
return gensols
elif returns in ('sol' 'both'):
gsol = Add(*[i*j for (i, j) in zip(constants, gensols)])
if returns == 'sol':
return Eq(f(x), gsol)
else:
return {'sol': Eq(f(x), gsol), 'list': gensols}
else:
raise ValueError('Unknown value for key "returns".')
def ode_nth_linear_constant_coeff_undetermined_coefficients(eq, func, order, match):
r"""
Solves an `n`\th order linear differential equation with constant
coefficients using the method of undetermined coefficients.
This method works on differential equations of the form
.. math:: a_n f^{(n)}(x) + a_{n-1} f^{(n-1)}(x) + \cdots + a_1 f'(x)
+ a_0 f(x) = P(x)\text{,}
where `P(x)` is a function that has a finite number of linearly
independent derivatives.
Functions that fit this requirement are finite sums functions of the form
`a x^i e^{b x} \sin(c x + d)` or `a x^i e^{b x} \cos(c x + d)`, where `i`
is a non-negative integer and `a`, `b`, `c`, and `d` are constants. For
example any polynomial in `x`, functions like `x^2 e^{2 x}`, `x \sin(x)`,
and `e^x \cos(x)` can all be used. Products of `\sin`'s and `\cos`'s have
a finite number of derivatives, because they can be expanded into `\sin(a
x)` and `\cos(b x)` terms. However, SymPy currently cannot do that
expansion, so you will need to manually rewrite the expression in terms of
the above to use this method. So, for example, you will need to manually
convert `\sin^2(x)` into `(1 + \cos(2 x))/2` to properly apply the method
of undetermined coefficients on it.
This method works by creating a trial function from the expression and all
of its linear independent derivatives and substituting them into the
original ODE. The coefficients for each term will be a system of linear
equations, which are be solved for and substituted, giving the solution.
If any of the trial functions are linearly dependent on the solution to
the homogeneous equation, they are multiplied by sufficient `x` to make
them linearly independent.
Examples
========
>>> from sympy import Function, dsolve, pprint, exp, cos
>>> from sympy.abc import x
>>> f = Function('f')
>>> pprint(dsolve(f(x).diff(x, 2) + 2*f(x).diff(x) + f(x) -
... 4*exp(-x)*x**2 + cos(2*x), f(x),
... hint='nth_linear_constant_coeff_undetermined_coefficients'))
/ 4\
| x | -x 4*sin(2*x) 3*cos(2*x)
f(x) = |C1 + C2*x + --|*e - ---------- + ----------
\ 3 / 25 25
References
==========
- https://en.wikipedia.org/wiki/Method_of_undetermined_coefficients
- M. Tenenbaum & H. Pollard, "Ordinary Differential Equations",
Dover 1963, pp. 221
# indirect doctest
"""
gensol = ode_nth_linear_constant_coeff_homogeneous(eq, func, order, match,
returns='both')
match.update(gensol)
return _solve_undetermined_coefficients(eq, func, order, match)
def _solve_undetermined_coefficients(eq, func, order, match):
r"""
Helper function for the method of undetermined coefficients.
See the
:py:meth:`~sympy.solvers.ode.ode_nth_linear_constant_coeff_undetermined_coefficients`
docstring for more information on this method.
The parameter ``match`` should be a dictionary that has the following
keys:
``list``
A list of solutions to the homogeneous equation, such as the list
returned by
``ode_nth_linear_constant_coeff_homogeneous(returns='list')``.
``sol``
The general solution, such as the solution returned by
``ode_nth_linear_constant_coeff_homogeneous(returns='sol')``.
``trialset``
The set of trial functions as returned by
``_undetermined_coefficients_match()['trialset']``.
"""
x = func.args[0]
f = func.func
r = match
coeffs = numbered_symbols('a', cls=Dummy)
coefflist = []
gensols = r['list']
gsol = r['sol']
trialset = r['trialset']
notneedset = set([])
global collectterms
if len(gensols) != order:
raise NotImplementedError("Cannot find " + str(order) +
" solutions to the homogeneous equation necessary to apply" +
" undetermined coefficients to " + str(eq) +
" (number of terms != order)")
usedsin = set([])
mult = 0 # The multiplicity of the root
getmult = True
for i, reroot, imroot in collectterms:
if getmult:
mult = i + 1
getmult = False
if i == 0:
getmult = True
if imroot:
# Alternate between sin and cos
if (i, reroot) in usedsin:
check = x**i*exp(reroot*x)*cos(imroot*x)
else:
check = x**i*exp(reroot*x)*sin(abs(imroot)*x)
usedsin.add((i, reroot))
else:
check = x**i*exp(reroot*x)
if check in trialset:
# If an element of the trial function is already part of the
# homogeneous solution, we need to multiply by sufficient x to
# make it linearly independent. We also don't need to bother
# checking for the coefficients on those elements, since we
# already know it will be 0.
while True:
if check*x**mult in trialset:
mult += 1
else:
break
trialset.add(check*x**mult)
notneedset.add(check)
newtrialset = trialset - notneedset
trialfunc = 0
for i in newtrialset:
c = next(coeffs)
coefflist.append(c)
trialfunc += c*i
eqs = sub_func_doit(eq, f(x), trialfunc)
coeffsdict = dict(list(zip(trialset, [0]*(len(trialset) + 1))))
eqs = _mexpand(eqs)
for i in Add.make_args(eqs):
s = separatevars(i, dict=True, symbols=[x])
coeffsdict[s[x]] += s['coeff']
coeffvals = solve(list(coeffsdict.values()), coefflist)
if not coeffvals:
raise NotImplementedError(
"Could not solve `%s` using the "
"method of undetermined coefficients "
"(unable to solve for coefficients)." % eq)
psol = trialfunc.subs(coeffvals)
return Eq(f(x), gsol.rhs + psol)
def _undetermined_coefficients_match(expr, x):
r"""
Returns a trial function match if undetermined coefficients can be applied
to ``expr``, and ``None`` otherwise.
A trial expression can be found for an expression for use with the method
of undetermined coefficients if the expression is an
additive/multiplicative combination of constants, polynomials in `x` (the
independent variable of expr), `\sin(a x + b)`, `\cos(a x + b)`, and
`e^{a x}` terms (in other words, it has a finite number of linearly
independent derivatives).
Note that you may still need to multiply each term returned here by
sufficient `x` to make it linearly independent with the solutions to the
homogeneous equation.
This is intended for internal use by ``undetermined_coefficients`` hints.
SymPy currently has no way to convert `\sin^n(x) \cos^m(y)` into a sum of
only `\sin(a x)` and `\cos(b x)` terms, so these are not implemented. So,
for example, you will need to manually convert `\sin^2(x)` into `[1 +
\cos(2 x)]/2` to properly apply the method of undetermined coefficients on
it.
Examples
========
>>> from sympy import log, exp
>>> from sympy.solvers.ode import _undetermined_coefficients_match
>>> from sympy.abc import x
>>> _undetermined_coefficients_match(9*x*exp(x) + exp(-x), x)
{'test': True, 'trialset': {x*exp(x), exp(-x), exp(x)}}
>>> _undetermined_coefficients_match(log(x), x)
{'test': False}
"""
a = Wild('a', exclude=[x])
b = Wild('b', exclude=[x])
expr = powsimp(expr, combine='exp') # exp(x)*exp(2*x + 1) => exp(3*x + 1)
retdict = {}
def _test_term(expr, x):
r"""
Test if ``expr`` fits the proper form for undetermined coefficients.
"""
if not expr.has(x):
return True
elif expr.is_Add:
return all(_test_term(i, x) for i in expr.args)
elif expr.is_Mul:
if expr.has(sin, cos):
foundtrig = False
# Make sure that there is only one trig function in the args.
# See the docstring.
for i in expr.args:
if i.has(sin, cos):
if foundtrig:
return False
else:
foundtrig = True
return all(_test_term(i, x) for i in expr.args)
elif expr.is_Function:
if expr.func in (sin, cos, exp):
if expr.args[0].match(a*x + b):
return True
else:
return False
else:
return False
elif expr.is_Pow and expr.base.is_Symbol and expr.exp.is_Integer and \
expr.exp >= 0:
return True
elif expr.is_Pow and expr.base.is_number:
if expr.exp.match(a*x + b):
return True
else:
return False
elif expr.is_Symbol or expr.is_number:
return True
else:
return False
def _get_trial_set(expr, x, exprs=set([])):
r"""
Returns a set of trial terms for undetermined coefficients.
The idea behind undetermined coefficients is that the terms expression
repeat themselves after a finite number of derivatives, except for the
coefficients (they are linearly dependent). So if we collect these,
we should have the terms of our trial function.
"""
def _remove_coefficient(expr, x):
r"""
Returns the expression without a coefficient.
Similar to expr.as_independent(x)[1], except it only works
multiplicatively.
"""
term = S.One
if expr.is_Mul:
for i in expr.args:
if i.has(x):
term *= i
elif expr.has(x):
term = expr
return term
expr = expand_mul(expr)
if expr.is_Add:
for term in expr.args:
if _remove_coefficient(term, x) in exprs:
pass
else:
exprs.add(_remove_coefficient(term, x))
exprs = exprs.union(_get_trial_set(term, x, exprs))
else:
term = _remove_coefficient(expr, x)
tmpset = exprs.union({term})
oldset = set([])
while tmpset != oldset:
# If you get stuck in this loop, then _test_term is probably
# broken
oldset = tmpset.copy()
expr = expr.diff(x)
term = _remove_coefficient(expr, x)
if term.is_Add:
tmpset = tmpset.union(_get_trial_set(term, x, tmpset))
else:
tmpset.add(term)
exprs = tmpset
return exprs
retdict['test'] = _test_term(expr, x)
if retdict['test']:
# Try to generate a list of trial solutions that will have the
# undetermined coefficients. Note that if any of these are not linearly
# independent with any of the solutions to the homogeneous equation,
# then they will need to be multiplied by sufficient x to make them so.
# This function DOES NOT do that (it doesn't even look at the
# homogeneous equation).
retdict['trialset'] = _get_trial_set(expr, x)
return retdict
def ode_nth_linear_constant_coeff_variation_of_parameters(eq, func, order, match):
r"""
Solves an `n`\th order linear differential equation with constant
coefficients using the method of variation of parameters.
This method works on any differential equations of the form
.. math:: f^{(n)}(x) + a_{n-1} f^{(n-1)}(x) + \cdots + a_1 f'(x) + a_0
f(x) = P(x)\text{.}
This method works by assuming that the particular solution takes the form
.. math:: \sum_{x=1}^{n} c_i(x) y_i(x)\text{,}
where `y_i` is the `i`\th solution to the homogeneous equation. The
solution is then solved using Wronskian's and Cramer's Rule. The
particular solution is given by
.. math:: \sum_{x=1}^n \left( \int \frac{W_i(x)}{W(x)} \,dx
\right) y_i(x) \text{,}
where `W(x)` is the Wronskian of the fundamental system (the system of `n`
linearly independent solutions to the homogeneous equation), and `W_i(x)`
is the Wronskian of the fundamental system with the `i`\th column replaced
with `[0, 0, \cdots, 0, P(x)]`.
This method is general enough to solve any `n`\th order inhomogeneous
linear differential equation with constant coefficients, but sometimes
SymPy cannot simplify the Wronskian well enough to integrate it. If this
method hangs, try using the
``nth_linear_constant_coeff_variation_of_parameters_Integral`` hint and
simplifying the integrals manually. Also, prefer using
``nth_linear_constant_coeff_undetermined_coefficients`` when it
applies, because it doesn't use integration, making it faster and more
reliable.
Warning, using simplify=False with
'nth_linear_constant_coeff_variation_of_parameters' in
:py:meth:`~sympy.solvers.ode.dsolve` may cause it to hang, because it will
not attempt to simplify the Wronskian before integrating. It is
recommended that you only use simplify=False with
'nth_linear_constant_coeff_variation_of_parameters_Integral' for this
method, especially if the solution to the homogeneous equation has
trigonometric functions in it.
Examples
========
>>> from sympy import Function, dsolve, pprint, exp, log
>>> from sympy.abc import x
>>> f = Function('f')
>>> pprint(dsolve(f(x).diff(x, 3) - 3*f(x).diff(x, 2) +
... 3*f(x).diff(x) - f(x) - exp(x)*log(x), f(x),
... hint='nth_linear_constant_coeff_variation_of_parameters'))
/ 3 \
| 2 x *(6*log(x) - 11)| x
f(x) = |C1 + C2*x + C3*x + ------------------|*e
\ 36 /
References
==========
- https://en.wikipedia.org/wiki/Variation_of_parameters
- http://planetmath.org/VariationOfParameters
- M. Tenenbaum & H. Pollard, "Ordinary Differential Equations",
Dover 1963, pp. 233
# indirect doctest
"""
gensol = ode_nth_linear_constant_coeff_homogeneous(eq, func, order, match,
returns='both')
match.update(gensol)
return _solve_variation_of_parameters(eq, func, order, match)
def _solve_variation_of_parameters(eq, func, order, match):
r"""
Helper function for the method of variation of parameters and nonhomogeneous euler eq.
See the
:py:meth:`~sympy.solvers.ode.ode_nth_linear_constant_coeff_variation_of_parameters`
docstring for more information on this method.
The parameter ``match`` should be a dictionary that has the following
keys:
``list``
A list of solutions to the homogeneous equation, such as the list
returned by
``ode_nth_linear_constant_coeff_homogeneous(returns='list')``.
``sol``
The general solution, such as the solution returned by
``ode_nth_linear_constant_coeff_homogeneous(returns='sol')``.
"""
x = func.args[0]
f = func.func
r = match
psol = 0
gensols = r['list']
gsol = r['sol']
wr = wronskian(gensols, x)
if r.get('simplify', True):
wr = simplify(wr) # We need much better simplification for
# some ODEs. See issue 4662, for example.
# To reduce commonly occurring sin(x)**2 + cos(x)**2 to 1
wr = trigsimp(wr, deep=True, recursive=True)
if not wr:
# The wronskian will be 0 iff the solutions are not linearly
# independent.
raise NotImplementedError("Cannot find " + str(order) +
" solutions to the homogeneous equation necessary to apply " +
"variation of parameters to " + str(eq) + " (Wronskian == 0)")
if len(gensols) != order:
raise NotImplementedError("Cannot find " + str(order) +
" solutions to the homogeneous equation necessary to apply " +
"variation of parameters to " +
str(eq) + " (number of terms != order)")
negoneterm = (-1)**(order)
for i in gensols:
psol += negoneterm*Integral(wronskian([sol for sol in gensols if sol != i], x)*r[-1]/wr, x)*i/r[order]
negoneterm *= -1
if r.get('simplify', True):
psol = simplify(psol)
psol = trigsimp(psol, deep=True)
return Eq(f(x), gsol.rhs + psol)
def ode_factorable(eq, func, order, match):
r"""
Solves equations having a solvable factor.
This function is used to solve the equation having factors. Factors may be of type algebraic or ode. It
will try to solve each factor independently. Factors will be solved by calling dsolve. We will return the
list of solutions.
Examples
========
>>> from sympy import Function, dsolve, Eq, pprint, Derivative
>>> from sympy.abc import x
>>> f = Function('f')
>>> eq = (f(x)**2-4)*(f(x).diff(x)+f(x))
>>> pprint(dsolve(eq, f(x)))
-x
[f(x) = 2, f(x) = -2, f(x) = C1*e ]
"""
eqns = match['eqns']
x0 = match['x0']
sols = []
for eq in eqns:
try:
sol = dsolve(eq, func, x0=x0)
except NotImplementedError:
continue
else:
if isinstance(sol, list):
sols.extend(sol)
else:
sols.append(sol)
if sols == []:
raise NotImplementedError("The given ODE " + str(eq) + " cannot be solved by"
+ " the factorable group method")
return sols
def ode_separable(eq, func, order, match):
r"""
Solves separable 1st order differential equations.
This is any differential equation that can be written as `P(y)
\tfrac{dy}{dx} = Q(x)`. The solution can then just be found by
rearranging terms and integrating: `\int P(y) \,dy = \int Q(x) \,dx`.
This hint uses :py:meth:`sympy.simplify.simplify.separatevars` as its back
end, so if a separable equation is not caught by this solver, it is most
likely the fault of that function.
:py:meth:`~sympy.simplify.simplify.separatevars` is
smart enough to do most expansion and factoring necessary to convert a
separable equation `F(x, y)` into the proper form `P(x)\cdot{}Q(y)`. The
general solution is::
>>> from sympy import Function, dsolve, Eq, pprint
>>> from sympy.abc import x
>>> a, b, c, d, f = map(Function, ['a', 'b', 'c', 'd', 'f'])
>>> genform = Eq(a(x)*b(f(x))*f(x).diff(x), c(x)*d(f(x)))
>>> pprint(genform)
d
a(x)*b(f(x))*--(f(x)) = c(x)*d(f(x))
dx
>>> pprint(dsolve(genform, f(x), hint='separable_Integral'))
f(x)
/ /
| |
| b(y) | c(x)
| ---- dy = C1 + | ---- dx
| d(y) | a(x)
| |
/ /
Examples
========
>>> from sympy import Function, dsolve, Eq
>>> from sympy.abc import x
>>> f = Function('f')
>>> pprint(dsolve(Eq(f(x)*f(x).diff(x) + x, 3*x*f(x)**2), f(x),
... hint='separable', simplify=False))
/ 2 \ 2
log\3*f (x) - 1/ x
---------------- = C1 + --
6 2
References
==========
- M. Tenenbaum & H. Pollard, "Ordinary Differential Equations",
Dover 1963, pp. 52
# indirect doctest
"""
x = func.args[0]
f = func.func
C1 = get_numbered_constants(eq, num=1)
r = match # {'m1':m1, 'm2':m2, 'y':y}
u = r.get('hint', f(x)) # get u from separable_reduced else get f(x)
return Eq(Integral(r['m2']['coeff']*r['m2'][r['y']]/r['m1'][r['y']],
(r['y'], None, u)), Integral(-r['m1']['coeff']*r['m1'][x]/
r['m2'][x], x) + C1)
def checkinfsol(eq, infinitesimals, func=None, order=None):
r"""
This function is used to check if the given infinitesimals are the
actual infinitesimals of the given first order differential equation.
This method is specific to the Lie Group Solver of ODEs.
As of now, it simply checks, by substituting the infinitesimals in the
partial differential equation.
.. math:: \frac{\partial \eta}{\partial x} + \left(\frac{\partial \eta}{\partial y}
- \frac{\partial \xi}{\partial x}\right)*h
- \frac{\partial \xi}{\partial y}*h^{2}
- \xi\frac{\partial h}{\partial x} - \eta\frac{\partial h}{\partial y} = 0
where `\eta`, and `\xi` are the infinitesimals and `h(x,y) = \frac{dy}{dx}`
The infinitesimals should be given in the form of a list of dicts
``[{xi(x, y): inf, eta(x, y): inf}]``, corresponding to the
output of the function infinitesimals. It returns a list
of values of the form ``[(True/False, sol)]`` where ``sol`` is the value
obtained after substituting the infinitesimals in the PDE. If it
is ``True``, then ``sol`` would be 0.
"""
if isinstance(eq, Equality):
eq = eq.lhs - eq.rhs
if not func:
eq, func = _preprocess(eq)
variables = func.args
if len(variables) != 1:
raise ValueError("ODE's have only one independent variable")
else:
x = variables[0]
if not order:
order = ode_order(eq, func)
if order != 1:
raise NotImplementedError("Lie groups solver has been implemented "
"only for first order differential equations")
else:
df = func.diff(x)
a = Wild('a', exclude = [df])
b = Wild('b', exclude = [df])
match = collect(expand(eq), df).match(a*df + b)
if match:
h = -simplify(match[b]/match[a])
else:
try:
sol = solve(eq, df)
except NotImplementedError:
raise NotImplementedError("Infinitesimals for the "
"first order ODE could not be found")
else:
h = sol[0] # Find infinitesimals for one solution
y = Dummy('y')
h = h.subs(func, y)
xi = Function('xi')(x, y)
eta = Function('eta')(x, y)
dxi = Function('xi')(x, func)
deta = Function('eta')(x, func)
pde = (eta.diff(x) + (eta.diff(y) - xi.diff(x))*h -
(xi.diff(y))*h**2 - xi*(h.diff(x)) - eta*(h.diff(y)))
soltup = []
for sol in infinitesimals:
tsol = {xi: S(sol[dxi]).subs(func, y),
eta: S(sol[deta]).subs(func, y)}
sol = simplify(pde.subs(tsol).doit())
if sol:
soltup.append((False, sol.subs(y, func)))
else:
soltup.append((True, 0))
return soltup
def _ode_lie_group_try_heuristic(eq, heuristic, func, match, inf):
xi = Function("xi")
eta = Function("eta")
f = func.func
x = func.args[0]
y = match['y']
h = match['h']
tempsol = []
if not inf:
try:
inf = infinitesimals(eq, hint=heuristic, func=func, order=1, match=match)
except ValueError:
return None
for infsim in inf:
xiinf = (infsim[xi(x, func)]).subs(func, y)
etainf = (infsim[eta(x, func)]).subs(func, y)
# This condition creates recursion while using pdsolve.
# Since the first step while solving a PDE of form
# a*(f(x, y).diff(x)) + b*(f(x, y).diff(y)) + c = 0
# is to solve the ODE dy/dx = b/a
if simplify(etainf/xiinf) == h:
continue
rpde = f(x, y).diff(x)*xiinf + f(x, y).diff(y)*etainf
r = pdsolve(rpde, func=f(x, y)).rhs
s = pdsolve(rpde - 1, func=f(x, y)).rhs
newcoord = [_lie_group_remove(coord) for coord in [r, s]]
r = Dummy("r")
s = Dummy("s")
C1 = Symbol("C1")
rcoord = newcoord[0]
scoord = newcoord[-1]
try:
sol = solve([r - rcoord, s - scoord], x, y, dict=True)
if sol == []:
continue
except NotImplementedError:
continue
else:
sol = sol[0]
xsub = sol[x]
ysub = sol[y]
num = simplify(scoord.diff(x) + scoord.diff(y)*h)
denom = simplify(rcoord.diff(x) + rcoord.diff(y)*h)
if num and denom:
diffeq = simplify((num/denom).subs([(x, xsub), (y, ysub)]))
sep = separatevars(diffeq, symbols=[r, s], dict=True)
if sep:
# Trying to separate, r and s coordinates
deq = integrate((1/sep[s]), s) + C1 - integrate(sep['coeff']*sep[r], r)
# Substituting and reverting back to original coordinates
deq = deq.subs([(r, rcoord), (s, scoord)])
try:
sdeq = solve(deq, y)
except NotImplementedError:
tempsol.append(deq)
else:
return [Eq(f(x), sol) for sol in sdeq]
elif denom: # (ds/dr) is zero which means s is constant
return [Eq(f(x), solve(scoord - C1, y)[0])]
elif num: # (dr/ds) is zero which means r is constant
return [Eq(f(x), solve(rcoord - C1, y)[0])]
# If nothing works, return solution as it is, without solving for y
if tempsol:
return [Eq(sol.subs(y, f(x)), 0) for sol in tempsol]
return None
def _ode_lie_group( s, func, order, match):
heuristics = lie_heuristics
inf = {}
f = func.func
x = func.args[0]
df = func.diff(x)
xi = Function("xi")
eta = Function("eta")
xis = match['xi']
etas = match['eta']
y = match.pop('y', None)
if y:
h = -simplify(match[match['d']]/match[match['e']])
y = y
else:
y = Dummy("y")
h = s.subs(func, y)
if xis is not None and etas is not None:
inf = [{xi(x, f(x)): S(xis), eta(x, f(x)): S(etas)}]
if checkinfsol(Eq(df, s), inf, func=f(x), order=1)[0][0]:
heuristics = ["user_defined"] + list(heuristics)
match = {'h': h, 'y': y}
# This is done so that if:
# a] any heuristic raises a ValueError
# another heuristic can be used.
sol = None
for heuristic in heuristics:
sol = _ode_lie_group_try_heuristic(Eq(df, s), heuristic, func, match, inf)
if sol:
return sol
return sol
def ode_lie_group(eq, func, order, match):
r"""
This hint implements the Lie group method of solving first order differential
equations. The aim is to convert the given differential equation from the
given coordinate given system into another coordinate system where it becomes
invariant under the one-parameter Lie group of translations. The converted ODE is
quadrature and can be solved easily. It makes use of the
:py:meth:`sympy.solvers.ode.infinitesimals` function which returns the
infinitesimals of the transformation.
The coordinates `r` and `s` can be found by solving the following Partial
Differential Equations.
.. math :: \xi\frac{\partial r}{\partial x} + \eta\frac{\partial r}{\partial y}
= 0
.. math :: \xi\frac{\partial s}{\partial x} + \eta\frac{\partial s}{\partial y}
= 1
The differential equation becomes separable in the new coordinate system
.. math :: \frac{ds}{dr} = \frac{\frac{\partial s}{\partial x} +
h(x, y)\frac{\partial s}{\partial y}}{
\frac{\partial r}{\partial x} + h(x, y)\frac{\partial r}{\partial y}}
After finding the solution by integration, it is then converted back to the original
coordinate system by substituting `r` and `s` in terms of `x` and `y` again.
Examples
========
>>> from sympy import Function, dsolve, Eq, exp, pprint
>>> from sympy.abc import x
>>> f = Function('f')
>>> pprint(dsolve(f(x).diff(x) + 2*x*f(x) - x*exp(-x**2), f(x),
... hint='lie_group'))
/ 2\ 2
| x | -x
f(x) = |C1 + --|*e
\ 2 /
References
==========
- Solving differential equations by Symmetry Groups,
John Starrett, pp. 1 - pp. 14
"""
f = func.func
x = func.args[0]
df = func.diff(x)
try:
eqsol = solve(eq, df)
except NotImplementedError:
eqsol = []
desols = []
for s in eqsol:
sol = _ode_lie_group(s, func, order, match=match)
if sol:
desols.extend(sol)
if desols == []:
raise NotImplementedError("The given ODE " + str(eq) + " cannot be solved by"
+ " the lie group method")
return desols
def _lie_group_remove(coords):
r"""
This function is strictly meant for internal use by the Lie group ODE solving
method. It replaces arbitrary functions returned by pdsolve with either 0 or 1 or the
args of the arbitrary function.
The algorithm used is:
1] If coords is an instance of an Undefined Function, then the args are returned
2] If the arbitrary function is present in an Add object, it is replaced by zero.
3] If the arbitrary function is present in an Mul object, it is replaced by one.
4] If coords has no Undefined Function, it is returned as it is.
Examples
========
>>> from sympy.solvers.ode import _lie_group_remove
>>> from sympy import Function
>>> from sympy.abc import x, y
>>> F = Function("F")
>>> eq = x**2*y
>>> _lie_group_remove(eq)
x**2*y
>>> eq = F(x**2*y)
>>> _lie_group_remove(eq)
x**2*y
>>> eq = y**2*x + F(x**3)
>>> _lie_group_remove(eq)
x*y**2
>>> eq = (F(x**3) + y)*x**4
>>> _lie_group_remove(eq)
x**4*y
"""
if isinstance(coords, AppliedUndef):
return coords.args[0]
elif coords.is_Add:
subfunc = coords.atoms(AppliedUndef)
if subfunc:
for func in subfunc:
coords = coords.subs(func, 0)
return coords
elif coords.is_Pow:
base, expr = coords.as_base_exp()
base = _lie_group_remove(base)
expr = _lie_group_remove(expr)
return base**expr
elif coords.is_Mul:
mulargs = []
coordargs = coords.args
for arg in coordargs:
if not isinstance(coords, AppliedUndef):
mulargs.append(_lie_group_remove(arg))
return Mul(*mulargs)
return coords
def infinitesimals(eq, func=None, order=None, hint='default', match=None):
r"""
The infinitesimal functions of an ordinary differential equation, `\xi(x,y)`
and `\eta(x,y)`, are the infinitesimals of the Lie group of point transformations
for which the differential equation is invariant. So, the ODE `y'=f(x,y)`
would admit a Lie group `x^*=X(x,y;\varepsilon)=x+\varepsilon\xi(x,y)`,
`y^*=Y(x,y;\varepsilon)=y+\varepsilon\eta(x,y)` such that `(y^*)'=f(x^*, y^*)`.
A change of coordinates, to `r(x,y)` and `s(x,y)`, can be performed so this Lie group
becomes the translation group, `r^*=r` and `s^*=s+\varepsilon`.
They are tangents to the coordinate curves of the new system.
Consider the transformation `(x, y) \to (X, Y)` such that the
differential equation remains invariant. `\xi` and `\eta` are the tangents to
the transformed coordinates `X` and `Y`, at `\varepsilon=0`.
.. math:: \left(\frac{\partial X(x,y;\varepsilon)}{\partial\varepsilon
}\right)|_{\varepsilon=0} = \xi,
\left(\frac{\partial Y(x,y;\varepsilon)}{\partial\varepsilon
}\right)|_{\varepsilon=0} = \eta,
The infinitesimals can be found by solving the following PDE:
>>> from sympy import Function, diff, Eq, pprint
>>> from sympy.abc import x, y
>>> xi, eta, h = map(Function, ['xi', 'eta', 'h'])
>>> h = h(x, y) # dy/dx = h
>>> eta = eta(x, y)
>>> xi = xi(x, y)
>>> genform = Eq(eta.diff(x) + (eta.diff(y) - xi.diff(x))*h
... - (xi.diff(y))*h**2 - xi*(h.diff(x)) - eta*(h.diff(y)), 0)
>>> pprint(genform)
/d d \ d 2 d
|--(eta(x, y)) - --(xi(x, y))|*h(x, y) - eta(x, y)*--(h(x, y)) - h (x, y)*--(x
\dy dx / dy dy
<BLANKLINE>
d d
i(x, y)) - xi(x, y)*--(h(x, y)) + --(eta(x, y)) = 0
dx dx
Solving the above mentioned PDE is not trivial, and can be solved only by
making intelligent assumptions for `\xi` and `\eta` (heuristics). Once an
infinitesimal is found, the attempt to find more heuristics stops. This is done to
optimise the speed of solving the differential equation. If a list of all the
infinitesimals is needed, ``hint`` should be flagged as ``all``, which gives
the complete list of infinitesimals. If the infinitesimals for a particular
heuristic needs to be found, it can be passed as a flag to ``hint``.
Examples
========
>>> from sympy import Function, diff
>>> from sympy.solvers.ode import infinitesimals
>>> from sympy.abc import x
>>> f = Function('f')
>>> eq = f(x).diff(x) - x**2*f(x)
>>> infinitesimals(eq)
[{eta(x, f(x)): exp(x**3/3), xi(x, f(x)): 0}]
References
==========
- Solving differential equations by Symmetry Groups,
John Starrett, pp. 1 - pp. 14
"""
if isinstance(eq, Equality):
eq = eq.lhs - eq.rhs
if not func:
eq, func = _preprocess(eq)
variables = func.args
if len(variables) != 1:
raise ValueError("ODE's have only one independent variable")
else:
x = variables[0]
if not order:
order = ode_order(eq, func)
if order != 1:
raise NotImplementedError("Infinitesimals for only "
"first order ODE's have been implemented")
else:
df = func.diff(x)
# Matching differential equation of the form a*df + b
a = Wild('a', exclude = [df])
b = Wild('b', exclude = [df])
if match: # Used by lie_group hint
h = match['h']
y = match['y']
else:
match = collect(expand(eq), df).match(a*df + b)
if match:
h = -simplify(match[b]/match[a])
else:
try:
sol = solve(eq, df)
except NotImplementedError:
raise NotImplementedError("Infinitesimals for the "
"first order ODE could not be found")
else:
h = sol[0] # Find infinitesimals for one solution
y = Dummy("y")
h = h.subs(func, y)
u = Dummy("u")
hx = h.diff(x)
hy = h.diff(y)
hinv = ((1/h).subs([(x, u), (y, x)])).subs(u, y) # Inverse ODE
match = {'h': h, 'func': func, 'hx': hx, 'hy': hy, 'y': y, 'hinv': hinv}
if hint == 'all':
xieta = []
for heuristic in lie_heuristics:
function = globals()['lie_heuristic_' + heuristic]
inflist = function(match, comp=True)
if inflist:
xieta.extend([inf for inf in inflist if inf not in xieta])
if xieta:
return xieta
else:
raise NotImplementedError("Infinitesimals could not be found for "
"the given ODE")
elif hint == 'default':
for heuristic in lie_heuristics:
function = globals()['lie_heuristic_' + heuristic]
xieta = function(match, comp=False)
if xieta:
return xieta
raise NotImplementedError("Infinitesimals could not be found for"
" the given ODE")
elif hint not in lie_heuristics:
raise ValueError("Heuristic not recognized: " + hint)
else:
function = globals()['lie_heuristic_' + hint]
xieta = function(match, comp=True)
if xieta:
return xieta
else:
raise ValueError("Infinitesimals could not be found using the"
" given heuristic")
def lie_heuristic_abaco1_simple(match, comp=False):
r"""
The first heuristic uses the following four sets of
assumptions on `\xi` and `\eta`
.. math:: \xi = 0, \eta = f(x)
.. math:: \xi = 0, \eta = f(y)
.. math:: \xi = f(x), \eta = 0
.. math:: \xi = f(y), \eta = 0
The success of this heuristic is determined by algebraic factorisation.
For the first assumption `\xi = 0` and `\eta` to be a function of `x`, the PDE
.. math:: \frac{\partial \eta}{\partial x} + (\frac{\partial \eta}{\partial y}
- \frac{\partial \xi}{\partial x})*h
- \frac{\partial \xi}{\partial y}*h^{2}
- \xi*\frac{\partial h}{\partial x} - \eta*\frac{\partial h}{\partial y} = 0
reduces to `f'(x) - f\frac{\partial h}{\partial y} = 0`
If `\frac{\partial h}{\partial y}` is a function of `x`, then this can usually
be integrated easily. A similar idea is applied to the other 3 assumptions as well.
References
==========
- E.S Cheb-Terrab, L.G.S Duarte and L.A,C.P da Mota, Computer Algebra
Solving of First Order ODEs Using Symmetry Methods, pp. 8
"""
xieta = []
y = match['y']
h = match['h']
func = match['func']
x = func.args[0]
hx = match['hx']
hy = match['hy']
xi = Function('xi')(x, func)
eta = Function('eta')(x, func)
hysym = hy.free_symbols
if y not in hysym:
try:
fx = exp(integrate(hy, x))
except NotImplementedError:
pass
else:
inf = {xi: S.Zero, eta: fx}
if not comp:
return [inf]
if comp and inf not in xieta:
xieta.append(inf)
factor = hy/h
facsym = factor.free_symbols
if x not in facsym:
try:
fy = exp(integrate(factor, y))
except NotImplementedError:
pass
else:
inf = {xi: S.Zero, eta: fy.subs(y, func)}
if not comp:
return [inf]
if comp and inf not in xieta:
xieta.append(inf)
factor = -hx/h
facsym = factor.free_symbols
if y not in facsym:
try:
fx = exp(integrate(factor, x))
except NotImplementedError:
pass
else:
inf = {xi: fx, eta: S.Zero}
if not comp:
return [inf]
if comp and inf not in xieta:
xieta.append(inf)
factor = -hx/(h**2)
facsym = factor.free_symbols
if x not in facsym:
try:
fy = exp(integrate(factor, y))
except NotImplementedError:
pass
else:
inf = {xi: fy.subs(y, func), eta: S.Zero}
if not comp:
return [inf]
if comp and inf not in xieta:
xieta.append(inf)
if xieta:
return xieta
def lie_heuristic_abaco1_product(match, comp=False):
r"""
The second heuristic uses the following two assumptions on `\xi` and `\eta`
.. math:: \eta = 0, \xi = f(x)*g(y)
.. math:: \eta = f(x)*g(y), \xi = 0
The first assumption of this heuristic holds good if
`\frac{1}{h^{2}}\frac{\partial^2}{\partial x \partial y}\log(h)` is
separable in `x` and `y`, then the separated factors containing `x`
is `f(x)`, and `g(y)` is obtained by
.. math:: e^{\int f\frac{\partial}{\partial x}\left(\frac{1}{f*h}\right)\,dy}
provided `f\frac{\partial}{\partial x}\left(\frac{1}{f*h}\right)` is a function
of `y` only.
The second assumption holds good if `\frac{dy}{dx} = h(x, y)` is rewritten as
`\frac{dy}{dx} = \frac{1}{h(y, x)}` and the same properties of the first assumption
satisfies. After obtaining `f(x)` and `g(y)`, the coordinates are again
interchanged, to get `\eta` as `f(x)*g(y)`
References
==========
- E.S. Cheb-Terrab, A.D. Roche, Symmetries and First Order
ODE Patterns, pp. 7 - pp. 8
"""
xieta = []
y = match['y']
h = match['h']
hinv = match['hinv']
func = match['func']
x = func.args[0]
xi = Function('xi')(x, func)
eta = Function('eta')(x, func)
inf = separatevars(((log(h).diff(y)).diff(x))/h**2, dict=True, symbols=[x, y])
if inf and inf['coeff']:
fx = inf[x]
gy = simplify(fx*((1/(fx*h)).diff(x)))
gysyms = gy.free_symbols
if x not in gysyms:
gy = exp(integrate(gy, y))
inf = {eta: S.Zero, xi: (fx*gy).subs(y, func)}
if not comp:
return [inf]
if comp and inf not in xieta:
xieta.append(inf)
u1 = Dummy("u1")
inf = separatevars(((log(hinv).diff(y)).diff(x))/hinv**2, dict=True, symbols=[x, y])
if inf and inf['coeff']:
fx = inf[x]
gy = simplify(fx*((1/(fx*hinv)).diff(x)))
gysyms = gy.free_symbols
if x not in gysyms:
gy = exp(integrate(gy, y))
etaval = fx*gy
etaval = (etaval.subs([(x, u1), (y, x)])).subs(u1, y)
inf = {eta: etaval.subs(y, func), xi: S.Zero}
if not comp:
return [inf]
if comp and inf not in xieta:
xieta.append(inf)
if xieta:
return xieta
def lie_heuristic_bivariate(match, comp=False):
r"""
The third heuristic assumes the infinitesimals `\xi` and `\eta`
to be bi-variate polynomials in `x` and `y`. The assumption made here
for the logic below is that `h` is a rational function in `x` and `y`
though that may not be necessary for the infinitesimals to be
bivariate polynomials. The coefficients of the infinitesimals
are found out by substituting them in the PDE and grouping similar terms
that are polynomials and since they form a linear system, solve and check
for non trivial solutions. The degree of the assumed bivariates
are increased till a certain maximum value.
References
==========
- Lie Groups and Differential Equations
pp. 327 - pp. 329
"""
h = match['h']
hx = match['hx']
hy = match['hy']
func = match['func']
x = func.args[0]
y = match['y']
xi = Function('xi')(x, func)
eta = Function('eta')(x, func)
if h.is_rational_function():
# The maximum degree that the infinitesimals can take is
# calculated by this technique.
etax, etay, etad, xix, xiy, xid = symbols("etax etay etad xix xiy xid")
ipde = etax + (etay - xix)*h - xiy*h**2 - xid*hx - etad*hy
num, denom = cancel(ipde).as_numer_denom()
deg = Poly(num, x, y).total_degree()
deta = Function('deta')(x, y)
dxi = Function('dxi')(x, y)
ipde = (deta.diff(x) + (deta.diff(y) - dxi.diff(x))*h - (dxi.diff(y))*h**2
- dxi*hx - deta*hy)
xieq = Symbol("xi0")
etaeq = Symbol("eta0")
for i in range(deg + 1):
if i:
xieq += Add(*[
Symbol("xi_" + str(power) + "_" + str(i - power))*x**power*y**(i - power)
for power in range(i + 1)])
etaeq += Add(*[
Symbol("eta_" + str(power) + "_" + str(i - power))*x**power*y**(i - power)
for power in range(i + 1)])
pden, denom = (ipde.subs({dxi: xieq, deta: etaeq}).doit()).as_numer_denom()
pden = expand(pden)
# If the individual terms are monomials, the coefficients
# are grouped
if pden.is_polynomial(x, y) and pden.is_Add:
polyy = Poly(pden, x, y).as_dict()
if polyy:
symset = xieq.free_symbols.union(etaeq.free_symbols) - {x, y}
soldict = solve(polyy.values(), *symset)
if isinstance(soldict, list):
soldict = soldict[0]
if any(soldict.values()):
xired = xieq.subs(soldict)
etared = etaeq.subs(soldict)
# Scaling is done by substituting one for the parameters
# This can be any number except zero.
dict_ = dict((sym, 1) for sym in symset)
inf = {eta: etared.subs(dict_).subs(y, func),
xi: xired.subs(dict_).subs(y, func)}
return [inf]
def lie_heuristic_chi(match, comp=False):
r"""
The aim of the fourth heuristic is to find the function `\chi(x, y)`
that satisfies the PDE `\frac{d\chi}{dx} + h\frac{d\chi}{dx}
- \frac{\partial h}{\partial y}\chi = 0`.
This assumes `\chi` to be a bivariate polynomial in `x` and `y`. By intuition,
`h` should be a rational function in `x` and `y`. The method used here is
to substitute a general binomial for `\chi` up to a certain maximum degree
is reached. The coefficients of the polynomials, are calculated by by collecting
terms of the same order in `x` and `y`.
After finding `\chi`, the next step is to use `\eta = \xi*h + \chi`, to
determine `\xi` and `\eta`. This can be done by dividing `\chi` by `h`
which would give `-\xi` as the quotient and `\eta` as the remainder.
References
==========
- E.S Cheb-Terrab, L.G.S Duarte and L.A,C.P da Mota, Computer Algebra
Solving of First Order ODEs Using Symmetry Methods, pp. 8
"""
h = match['h']
hy = match['hy']
func = match['func']
x = func.args[0]
y = match['y']
xi = Function('xi')(x, func)
eta = Function('eta')(x, func)
if h.is_rational_function():
schi, schix, schiy = symbols("schi, schix, schiy")
cpde = schix + h*schiy - hy*schi
num, denom = cancel(cpde).as_numer_denom()
deg = Poly(num, x, y).total_degree()
chi = Function('chi')(x, y)
chix = chi.diff(x)
chiy = chi.diff(y)
cpde = chix + h*chiy - hy*chi
chieq = Symbol("chi")
for i in range(1, deg + 1):
chieq += Add(*[
Symbol("chi_" + str(power) + "_" + str(i - power))*x**power*y**(i - power)
for power in range(i + 1)])
cnum, cden = cancel(cpde.subs({chi : chieq}).doit()).as_numer_denom()
cnum = expand(cnum)
if cnum.is_polynomial(x, y) and cnum.is_Add:
cpoly = Poly(cnum, x, y).as_dict()
if cpoly:
solsyms = chieq.free_symbols - {x, y}
soldict = solve(cpoly.values(), *solsyms)
if isinstance(soldict, list):
soldict = soldict[0]
if any(soldict.values()):
chieq = chieq.subs(soldict)
dict_ = dict((sym, 1) for sym in solsyms)
chieq = chieq.subs(dict_)
# After finding chi, the main aim is to find out
# eta, xi by the equation eta = xi*h + chi
# One method to set xi, would be rearranging it to
# (eta/h) - xi = (chi/h). This would mean dividing
# chi by h would give -xi as the quotient and eta
# as the remainder. Thanks to Sean Vig for suggesting
# this method.
xic, etac = div(chieq, h)
inf = {eta: etac.subs(y, func), xi: -xic.subs(y, func)}
return [inf]
def lie_heuristic_function_sum(match, comp=False):
r"""
This heuristic uses the following two assumptions on `\xi` and `\eta`
.. math:: \eta = 0, \xi = f(x) + g(y)
.. math:: \eta = f(x) + g(y), \xi = 0
The first assumption of this heuristic holds good if
.. math:: \frac{\partial}{\partial y}[(h\frac{\partial^{2}}{
\partial x^{2}}(h^{-1}))^{-1}]
is separable in `x` and `y`,
1. The separated factors containing `y` is `\frac{\partial g}{\partial y}`.
From this `g(y)` can be determined.
2. The separated factors containing `x` is `f''(x)`.
3. `h\frac{\partial^{2}}{\partial x^{2}}(h^{-1})` equals
`\frac{f''(x)}{f(x) + g(y)}`. From this `f(x)` can be determined.
The second assumption holds good if `\frac{dy}{dx} = h(x, y)` is rewritten as
`\frac{dy}{dx} = \frac{1}{h(y, x)}` and the same properties of the first
assumption satisfies. After obtaining `f(x)` and `g(y)`, the coordinates
are again interchanged, to get `\eta` as `f(x) + g(y)`.
For both assumptions, the constant factors are separated among `g(y)`
and `f''(x)`, such that `f''(x)` obtained from 3] is the same as that
obtained from 2]. If not possible, then this heuristic fails.
References
==========
- E.S. Cheb-Terrab, A.D. Roche, Symmetries and First Order
ODE Patterns, pp. 7 - pp. 8
"""
xieta = []
h = match['h']
func = match['func']
hinv = match['hinv']
x = func.args[0]
y = match['y']
xi = Function('xi')(x, func)
eta = Function('eta')(x, func)
for odefac in [h, hinv]:
factor = odefac*((1/odefac).diff(x, 2))
sep = separatevars((1/factor).diff(y), dict=True, symbols=[x, y])
if sep and sep['coeff'] and sep[x].has(x) and sep[y].has(y):
k = Dummy("k")
try:
gy = k*integrate(sep[y], y)
except NotImplementedError:
pass
else:
fdd = 1/(k*sep[x]*sep['coeff'])
fx = simplify(fdd/factor - gy)
check = simplify(fx.diff(x, 2) - fdd)
if fx:
if not check:
fx = fx.subs(k, 1)
gy = (gy/k)
else:
sol = solve(check, k)
if sol:
sol = sol[0]
fx = fx.subs(k, sol)
gy = (gy/k)*sol
else:
continue
if odefac == hinv: # Inverse ODE
fx = fx.subs(x, y)
gy = gy.subs(y, x)
etaval = factor_terms(fx + gy)
if etaval.is_Mul:
etaval = Mul(*[arg for arg in etaval.args if arg.has(x, y)])
if odefac == hinv: # Inverse ODE
inf = {eta: etaval.subs(y, func), xi : S.Zero}
else:
inf = {xi: etaval.subs(y, func), eta : S.Zero}
if not comp:
return [inf]
else:
xieta.append(inf)
if xieta:
return xieta
def lie_heuristic_abaco2_similar(match, comp=False):
r"""
This heuristic uses the following two assumptions on `\xi` and `\eta`
.. math:: \eta = g(x), \xi = f(x)
.. math:: \eta = f(y), \xi = g(y)
For the first assumption,
1. First `\frac{\frac{\partial h}{\partial y}}{\frac{\partial^{2} h}{
\partial yy}}` is calculated. Let us say this value is A
2. If this is constant, then `h` is matched to the form `A(x) + B(x)e^{
\frac{y}{C}}` then, `\frac{e^{\int \frac{A(x)}{C} \,dx}}{B(x)}` gives `f(x)`
and `A(x)*f(x)` gives `g(x)`
3. Otherwise `\frac{\frac{\partial A}{\partial X}}{\frac{\partial A}{
\partial Y}} = \gamma` is calculated. If
a] `\gamma` is a function of `x` alone
b] `\frac{\gamma\frac{\partial h}{\partial y} - \gamma'(x) - \frac{
\partial h}{\partial x}}{h + \gamma} = G` is a function of `x` alone.
then, `e^{\int G \,dx}` gives `f(x)` and `-\gamma*f(x)` gives `g(x)`
The second assumption holds good if `\frac{dy}{dx} = h(x, y)` is rewritten as
`\frac{dy}{dx} = \frac{1}{h(y, x)}` and the same properties of the first assumption
satisfies. After obtaining `f(x)` and `g(x)`, the coordinates are again
interchanged, to get `\xi` as `f(x^*)` and `\eta` as `g(y^*)`
References
==========
- E.S. Cheb-Terrab, A.D. Roche, Symmetries and First Order
ODE Patterns, pp. 10 - pp. 12
"""
h = match['h']
hx = match['hx']
hy = match['hy']
func = match['func']
hinv = match['hinv']
x = func.args[0]
y = match['y']
xi = Function('xi')(x, func)
eta = Function('eta')(x, func)
factor = cancel(h.diff(y)/h.diff(y, 2))
factorx = factor.diff(x)
factory = factor.diff(y)
if not factor.has(x) and not factor.has(y):
A = Wild('A', exclude=[y])
B = Wild('B', exclude=[y])
C = Wild('C', exclude=[x, y])
match = h.match(A + B*exp(y/C))
try:
tau = exp(-integrate(match[A]/match[C]), x)/match[B]
except NotImplementedError:
pass
else:
gx = match[A]*tau
return [{xi: tau, eta: gx}]
else:
gamma = cancel(factorx/factory)
if not gamma.has(y):
tauint = cancel((gamma*hy - gamma.diff(x) - hx)/(h + gamma))
if not tauint.has(y):
try:
tau = exp(integrate(tauint, x))
except NotImplementedError:
pass
else:
gx = -tau*gamma
return [{xi: tau, eta: gx}]
factor = cancel(hinv.diff(y)/hinv.diff(y, 2))
factorx = factor.diff(x)
factory = factor.diff(y)
if not factor.has(x) and not factor.has(y):
A = Wild('A', exclude=[y])
B = Wild('B', exclude=[y])
C = Wild('C', exclude=[x, y])
match = h.match(A + B*exp(y/C))
try:
tau = exp(-integrate(match[A]/match[C]), x)/match[B]
except NotImplementedError:
pass
else:
gx = match[A]*tau
return [{eta: tau.subs(x, func), xi: gx.subs(x, func)}]
else:
gamma = cancel(factorx/factory)
if not gamma.has(y):
tauint = cancel((gamma*hinv.diff(y) - gamma.diff(x) - hinv.diff(x))/(
hinv + gamma))
if not tauint.has(y):
try:
tau = exp(integrate(tauint, x))
except NotImplementedError:
pass
else:
gx = -tau*gamma
return [{eta: tau.subs(x, func), xi: gx.subs(x, func)}]
def lie_heuristic_abaco2_unique_unknown(match, comp=False):
r"""
This heuristic assumes the presence of unknown functions or known functions
with non-integer powers.
1. A list of all functions and non-integer powers containing x and y
2. Loop over each element `f` in the list, find `\frac{\frac{\partial f}{\partial x}}{
\frac{\partial f}{\partial x}} = R`
If it is separable in `x` and `y`, let `X` be the factors containing `x`. Then
a] Check if `\xi = X` and `\eta = -\frac{X}{R}` satisfy the PDE. If yes, then return
`\xi` and `\eta`
b] Check if `\xi = \frac{-R}{X}` and `\eta = -\frac{1}{X}` satisfy the PDE.
If yes, then return `\xi` and `\eta`
If not, then check if
a] :math:`\xi = -R,\eta = 1`
b] :math:`\xi = 1, \eta = -\frac{1}{R}`
are solutions.
References
==========
- E.S. Cheb-Terrab, A.D. Roche, Symmetries and First Order
ODE Patterns, pp. 10 - pp. 12
"""
h = match['h']
hx = match['hx']
hy = match['hy']
func = match['func']
x = func.args[0]
y = match['y']
xi = Function('xi')(x, func)
eta = Function('eta')(x, func)
funclist = []
for atom in h.atoms(Pow):
base, exp = atom.as_base_exp()
if base.has(x) and base.has(y):
if not exp.is_Integer:
funclist.append(atom)
for function in h.atoms(AppliedUndef):
syms = function.free_symbols
if x in syms and y in syms:
funclist.append(function)
for f in funclist:
frac = cancel(f.diff(y)/f.diff(x))
sep = separatevars(frac, dict=True, symbols=[x, y])
if sep and sep['coeff']:
xitry1 = sep[x]
etatry1 = -1/(sep[y]*sep['coeff'])
pde1 = etatry1.diff(y)*h - xitry1.diff(x)*h - xitry1*hx - etatry1*hy
if not simplify(pde1):
return [{xi: xitry1, eta: etatry1.subs(y, func)}]
xitry2 = 1/etatry1
etatry2 = 1/xitry1
pde2 = etatry2.diff(x) - (xitry2.diff(y))*h**2 - xitry2*hx - etatry2*hy
if not simplify(expand(pde2)):
return [{xi: xitry2.subs(y, func), eta: etatry2}]
else:
etatry = -1/frac
pde = etatry.diff(x) + etatry.diff(y)*h - hx - etatry*hy
if not simplify(pde):
return [{xi: S.One, eta: etatry.subs(y, func)}]
xitry = -frac
pde = -xitry.diff(x)*h -xitry.diff(y)*h**2 - xitry*hx -hy
if not simplify(expand(pde)):
return [{xi: xitry.subs(y, func), eta: S.One}]
def lie_heuristic_abaco2_unique_general(match, comp=False):
r"""
This heuristic finds if infinitesimals of the form `\eta = f(x)`, `\xi = g(y)`
without making any assumptions on `h`.
The complete sequence of steps is given in the paper mentioned below.
References
==========
- E.S. Cheb-Terrab, A.D. Roche, Symmetries and First Order
ODE Patterns, pp. 10 - pp. 12
"""
hx = match['hx']
hy = match['hy']
func = match['func']
x = func.args[0]
y = match['y']
xi = Function('xi')(x, func)
eta = Function('eta')(x, func)
A = hx.diff(y)
B = hy.diff(y) + hy**2
C = hx.diff(x) - hx**2
if not (A and B and C):
return
Ax = A.diff(x)
Ay = A.diff(y)
Axy = Ax.diff(y)
Axx = Ax.diff(x)
Ayy = Ay.diff(y)
D = simplify(2*Axy + hx*Ay - Ax*hy + (hx*hy + 2*A)*A)*A - 3*Ax*Ay
if not D:
E1 = simplify(3*Ax**2 + ((hx**2 + 2*C)*A - 2*Axx)*A)
if E1:
E2 = simplify((2*Ayy + (2*B - hy**2)*A)*A - 3*Ay**2)
if not E2:
E3 = simplify(
E1*((28*Ax + 4*hx*A)*A**3 - E1*(hy*A + Ay)) - E1.diff(x)*8*A**4)
if not E3:
etaval = cancel((4*A**3*(Ax - hx*A) + E1*(hy*A - Ay))/(S(2)*A*E1))
if x not in etaval:
try:
etaval = exp(integrate(etaval, y))
except NotImplementedError:
pass
else:
xival = -4*A**3*etaval/E1
if y not in xival:
return [{xi: xival, eta: etaval.subs(y, func)}]
else:
E1 = simplify((2*Ayy + (2*B - hy**2)*A)*A - 3*Ay**2)
if E1:
E2 = simplify(
4*A**3*D - D**2 + E1*((2*Axx - (hx**2 + 2*C)*A)*A - 3*Ax**2))
if not E2:
E3 = simplify(
-(A*D)*E1.diff(y) + ((E1.diff(x) - hy*D)*A + 3*Ay*D +
(A*hx - 3*Ax)*E1)*E1)
if not E3:
etaval = cancel(((A*hx - Ax)*E1 - (Ay + A*hy)*D)/(S(2)*A*D))
if x not in etaval:
try:
etaval = exp(integrate(etaval, y))
except NotImplementedError:
pass
else:
xival = -E1*etaval/D
if y not in xival:
return [{xi: xival, eta: etaval.subs(y, func)}]
def lie_heuristic_linear(match, comp=False):
r"""
This heuristic assumes
1. `\xi = ax + by + c` and
2. `\eta = fx + gy + h`
After substituting the following assumptions in the determining PDE, it
reduces to
.. math:: f + (g - a)h - bh^{2} - (ax + by + c)\frac{\partial h}{\partial x}
- (fx + gy + c)\frac{\partial h}{\partial y}
Solving the reduced PDE obtained, using the method of characteristics, becomes
impractical. The method followed is grouping similar terms and solving the system
of linear equations obtained. The difference between the bivariate heuristic is that
`h` need not be a rational function in this case.
References
==========
- E.S. Cheb-Terrab, A.D. Roche, Symmetries and First Order
ODE Patterns, pp. 10 - pp. 12
"""
h = match['h']
hx = match['hx']
hy = match['hy']
func = match['func']
x = func.args[0]
y = match['y']
xi = Function('xi')(x, func)
eta = Function('eta')(x, func)
coeffdict = {}
symbols = numbered_symbols("c", cls=Dummy)
symlist = [next(symbols) for _ in islice(symbols, 6)]
C0, C1, C2, C3, C4, C5 = symlist
pde = C3 + (C4 - C0)*h - (C0*x + C1*y + C2)*hx - (C3*x + C4*y + C5)*hy - C1*h**2
pde, denom = pde.as_numer_denom()
pde = powsimp(expand(pde))
if pde.is_Add:
terms = pde.args
for term in terms:
if term.is_Mul:
rem = Mul(*[m for m in term.args if not m.has(x, y)])
xypart = term/rem
if xypart not in coeffdict:
coeffdict[xypart] = rem
else:
coeffdict[xypart] += rem
else:
if term not in coeffdict:
coeffdict[term] = S.One
else:
coeffdict[term] += S.One
sollist = coeffdict.values()
soldict = solve(sollist, symlist)
if soldict:
if isinstance(soldict, list):
soldict = soldict[0]
subval = soldict.values()
if any(t for t in subval):
onedict = dict(zip(symlist, [1]*6))
xival = C0*x + C1*func + C2
etaval = C3*x + C4*func + C5
xival = xival.subs(soldict)
etaval = etaval.subs(soldict)
xival = xival.subs(onedict)
etaval = etaval.subs(onedict)
return [{xi: xival, eta: etaval}]
def sysode_linear_2eq_order1(match_):
x = match_['func'][0].func
y = match_['func'][1].func
func = match_['func']
fc = match_['func_coeff']
eq = match_['eq']
r = dict()
t = list(list(eq[0].atoms(Derivative))[0].atoms(Symbol))[0]
for i in range(2):
eqs = 0
for terms in Add.make_args(eq[i]):
eqs += terms/fc[i,func[i],1]
eq[i] = eqs
# for equations Eq(a1*diff(x(t),t), a*x(t) + b*y(t) + k1)
# and Eq(a2*diff(x(t),t), c*x(t) + d*y(t) + k2)
r['a'] = -fc[0,x(t),0]/fc[0,x(t),1]
r['c'] = -fc[1,x(t),0]/fc[1,y(t),1]
r['b'] = -fc[0,y(t),0]/fc[0,x(t),1]
r['d'] = -fc[1,y(t),0]/fc[1,y(t),1]
forcing = [S.Zero,S.Zero]
for i in range(2):
for j in Add.make_args(eq[i]):
if not j.has(x(t), y(t)):
forcing[i] += j
if not (forcing[0].has(t) or forcing[1].has(t)):
r['k1'] = forcing[0]
r['k2'] = forcing[1]
else:
raise NotImplementedError("Only homogeneous problems are supported" +
" (and constant inhomogeneity)")
if match_['type_of_equation'] == 'type1':
sol = _linear_2eq_order1_type1(x, y, t, r, eq)
if match_['type_of_equation'] == 'type2':
gsol = _linear_2eq_order1_type1(x, y, t, r, eq)
psol = _linear_2eq_order1_type2(x, y, t, r, eq)
sol = [Eq(x(t), gsol[0].rhs+psol[0]), Eq(y(t), gsol[1].rhs+psol[1])]
if match_['type_of_equation'] == 'type3':
sol = _linear_2eq_order1_type3(x, y, t, r, eq)
if match_['type_of_equation'] == 'type4':
sol = _linear_2eq_order1_type4(x, y, t, r, eq)
if match_['type_of_equation'] == 'type5':
sol = _linear_2eq_order1_type5(x, y, t, r, eq)
if match_['type_of_equation'] == 'type6':
sol = _linear_2eq_order1_type6(x, y, t, r, eq)
if match_['type_of_equation'] == 'type7':
sol = _linear_2eq_order1_type7(x, y, t, r, eq)
return sol
def _linear_2eq_order1_type1(x, y, t, r, eq):
r"""
It is classified under system of two linear homogeneous first-order constant-coefficient
ordinary differential equations.
The equations which come under this type are
.. math:: x' = ax + by,
.. math:: y' = cx + dy
The characteristics equation is written as
.. math:: \lambda^{2} + (a+d) \lambda + ad - bc = 0
and its discriminant is `D = (a-d)^{2} + 4bc`. There are several cases
1. Case when `ad - bc \neq 0`. The origin of coordinates, `x = y = 0`,
is the only stationary point; it is
- a node if `D = 0`
- a node if `D > 0` and `ad - bc > 0`
- a saddle if `D > 0` and `ad - bc < 0`
- a focus if `D < 0` and `a + d \neq 0`
- a centre if `D < 0` and `a + d \neq 0`.
1.1. If `D > 0`. The characteristic equation has two distinct real roots
`\lambda_1` and `\lambda_ 2` . The general solution of the system in question is expressed as
.. math:: x = C_1 b e^{\lambda_1 t} + C_2 b e^{\lambda_2 t}
.. math:: y = C_1 (\lambda_1 - a) e^{\lambda_1 t} + C_2 (\lambda_2 - a) e^{\lambda_2 t}
where `C_1` and `C_2` being arbitrary constants
1.2. If `D < 0`. The characteristics equation has two conjugate
roots, `\lambda_1 = \sigma + i \beta` and `\lambda_2 = \sigma - i \beta`.
The general solution of the system is given by
.. math:: x = b e^{\sigma t} (C_1 \sin(\beta t) + C_2 \cos(\beta t))
.. math:: y = e^{\sigma t} ([(\sigma - a) C_1 - \beta C_2] \sin(\beta t) + [\beta C_1 + (\sigma - a) C_2 \cos(\beta t)])
1.3. If `D = 0` and `a \neq d`. The characteristic equation has
two equal roots, `\lambda_1 = \lambda_2`. The general solution of the system is written as
.. math:: x = 2b (C_1 + \frac{C_2}{a-d} + C_2 t) e^{\frac{a+d}{2} t}
.. math:: y = [(d - a) C_1 + C_2 + (d - a) C_2 t] e^{\frac{a+d}{2} t}
1.4. If `D = 0` and `a = d \neq 0` and `b = 0`
.. math:: x = C_1 e^{a t} , y = (c C_1 t + C_2) e^{a t}
1.5. If `D = 0` and `a = d \neq 0` and `c = 0`
.. math:: x = (b C_1 t + C_2) e^{a t} , y = C_1 e^{a t}
2. Case when `ad - bc = 0` and `a^{2} + b^{2} > 0`. The whole straight
line `ax + by = 0` consists of singular points. The original system of differential
equations can be rewritten as
.. math:: x' = ax + by , y' = k (ax + by)
2.1 If `a + bk \neq 0`, solution will be
.. math:: x = b C_1 + C_2 e^{(a + bk) t} , y = -a C_1 + k C_2 e^{(a + bk) t}
2.2 If `a + bk = 0`, solution will be
.. math:: x = C_1 (bk t - 1) + b C_2 t , y = k^{2} b C_1 t + (b k^{2} t + 1) C_2
"""
C1, C2 = get_numbered_constants(eq, num=2)
a, b, c, d = r['a'], r['b'], r['c'], r['d']
real_coeff = all(v.is_real for v in (a, b, c, d))
D = (a - d)**2 + 4*b*c
l1 = (a + d + sqrt(D))/2
l2 = (a + d - sqrt(D))/2
equal_roots = Eq(D, 0).expand()
gsol1, gsol2 = [], []
# Solutions have exponential form if either D > 0 with real coefficients
# or D != 0 with complex coefficients. Eigenvalues are distinct.
# For each eigenvalue lam, pick an eigenvector, making sure we don't get (0, 0)
# The candidates are (b, lam-a) and (lam-d, c).
exponential_form = D > 0 if real_coeff else Not(equal_roots)
bad_ab_vector1 = And(Eq(b, 0), Eq(l1, a))
bad_ab_vector2 = And(Eq(b, 0), Eq(l2, a))
vector1 = Matrix((Piecewise((l1 - d, bad_ab_vector1), (b, True)),
Piecewise((c, bad_ab_vector1), (l1 - a, True))))
vector2 = Matrix((Piecewise((l2 - d, bad_ab_vector2), (b, True)),
Piecewise((c, bad_ab_vector2), (l2 - a, True))))
sol_vector = C1*exp(l1*t)*vector1 + C2*exp(l2*t)*vector2
gsol1.append((sol_vector[0], exponential_form))
gsol2.append((sol_vector[1], exponential_form))
# Solutions have trigonometric form for real coefficients with D < 0
# Both b and c are nonzero in this case, so (b, lam-a) is an eigenvector
# It splits into real/imag parts as (b, sigma-a) and (0, beta). Then
# multiply it by C1(cos(beta*t) + I*C2*sin(beta*t)) and separate real/imag
trigonometric_form = D < 0 if real_coeff else False
sigma = re(l1)
if im(l1).is_positive:
beta = im(l1)
else:
beta = im(l2)
vector1 = Matrix((b, sigma - a))
vector2 = Matrix((0, beta))
sol_vector = exp(sigma*t) * (C1*(cos(beta*t)*vector1 - sin(beta*t)*vector2) + \
C2*(sin(beta*t)*vector1 + cos(beta*t)*vector2))
gsol1.append((sol_vector[0], trigonometric_form))
gsol2.append((sol_vector[1], trigonometric_form))
# Final case is D == 0, a single eigenvalue. If the eigenspace is 2-dimensional
# then we have a scalar matrix, deal with this case first.
scalar_matrix = And(Eq(a, d), Eq(b, 0), Eq(c, 0))
vector1 = Matrix((S.One, S.Zero))
vector2 = Matrix((S.Zero, S.One))
sol_vector = exp(l1*t) * (C1*vector1 + C2*vector2)
gsol1.append((sol_vector[0], scalar_matrix))
gsol2.append((sol_vector[1], scalar_matrix))
# Have one eigenvector. Get a generalized eigenvector from (A-lam)*vector2 = vector1
vector1 = Matrix((Piecewise((l1 - d, bad_ab_vector1), (b, True)),
Piecewise((c, bad_ab_vector1), (l1 - a, True))))
vector2 = Matrix((Piecewise((S.One, bad_ab_vector1), (S.Zero, Eq(a, l1)),
(b/(a - l1), True)),
Piecewise((S.Zero, bad_ab_vector1), (S.One, Eq(a, l1)),
(S.Zero, True))))
sol_vector = exp(l1*t) * (C1*vector1 + C2*(vector2 + t*vector1))
gsol1.append((sol_vector[0], equal_roots))
gsol2.append((sol_vector[1], equal_roots))
return [Eq(x(t), Piecewise(*gsol1)), Eq(y(t), Piecewise(*gsol2))]
def _linear_2eq_order1_type2(x, y, t, r, eq):
r"""
The equations of this type are
.. math:: x' = ax + by + k1 , y' = cx + dy + k2
The general solution of this system is given by sum of its particular solution and the
general solution of the corresponding homogeneous system is obtained from type1.
1. When `ad - bc \neq 0`. The particular solution will be
`x = x_0` and `y = y_0` where `x_0` and `y_0` are determined by solving linear system of equations
.. math:: a x_0 + b y_0 + k1 = 0 , c x_0 + d y_0 + k2 = 0
2. When `ad - bc = 0` and `a^{2} + b^{2} > 0`. In this case, the system of equation becomes
.. math:: x' = ax + by + k_1 , y' = k (ax + by) + k_2
2.1 If `\sigma = a + bk \neq 0`, particular solution is given by
.. math:: x = b \sigma^{-1} (c_1 k - c_2) t - \sigma^{-2} (a c_1 + b c_2)
.. math:: y = kx + (c_2 - c_1 k) t
2.2 If `\sigma = a + bk = 0`, particular solution is given by
.. math:: x = \frac{1}{2} b (c_2 - c_1 k) t^{2} + c_1 t
.. math:: y = kx + (c_2 - c_1 k) t
"""
r['k1'] = -r['k1']; r['k2'] = -r['k2']
if (r['a']*r['d'] - r['b']*r['c']) != 0:
x0, y0 = symbols('x0, y0', cls=Dummy)
sol = solve((r['a']*x0+r['b']*y0+r['k1'], r['c']*x0+r['d']*y0+r['k2']), x0, y0)
psol = [sol[x0], sol[y0]]
elif (r['a']*r['d'] - r['b']*r['c']) == 0 and (r['a']**2+r['b']**2) > 0:
k = r['c']/r['a']
sigma = r['a'] + r['b']*k
if sigma != 0:
sol1 = r['b']*sigma**-1*(r['k1']*k-r['k2'])*t - sigma**-2*(r['a']*r['k1']+r['b']*r['k2'])
sol2 = k*sol1 + (r['k2']-r['k1']*k)*t
else:
# FIXME: a previous typo fix shows this is not covered by tests
sol1 = r['b']*(r['k2']-r['k1']*k)*t**2 + r['k1']*t
sol2 = k*sol1 + (r['k2']-r['k1']*k)*t
psol = [sol1, sol2]
return psol
def _linear_2eq_order1_type3(x, y, t, r, eq):
r"""
The equations of this type of ode are
.. math:: x' = f(t) x + g(t) y
.. math:: y' = g(t) x + f(t) y
The solution of such equations is given by
.. math:: x = e^{F} (C_1 e^{G} + C_2 e^{-G}) , y = e^{F} (C_1 e^{G} - C_2 e^{-G})
where `C_1` and `C_2` are arbitrary constants, and
.. math:: F = \int f(t) \,dt , G = \int g(t) \,dt
"""
C1, C2, C3, C4 = get_numbered_constants(eq, num=4)
F = Integral(r['a'], t)
G = Integral(r['b'], t)
sol1 = exp(F)*(C1*exp(G) + C2*exp(-G))
sol2 = exp(F)*(C1*exp(G) - C2*exp(-G))
return [Eq(x(t), sol1), Eq(y(t), sol2)]
def _linear_2eq_order1_type4(x, y, t, r, eq):
r"""
The equations of this type of ode are .
.. math:: x' = f(t) x + g(t) y
.. math:: y' = -g(t) x + f(t) y
The solution is given by
.. math:: x = F (C_1 \cos(G) + C_2 \sin(G)), y = F (-C_1 \sin(G) + C_2 \cos(G))
where `C_1` and `C_2` are arbitrary constants, and
.. math:: F = \int f(t) \,dt , G = \int g(t) \,dt
"""
C1, C2, C3, C4 = get_numbered_constants(eq, num=4)
if r['b'] == -r['c']:
F = exp(Integral(r['a'], t))
G = Integral(r['b'], t)
sol1 = F*(C1*cos(G) + C2*sin(G))
sol2 = F*(-C1*sin(G) + C2*cos(G))
elif r['d'] == -r['a']:
F = exp(Integral(r['c'], t))
G = Integral(r['d'], t)
sol1 = F*(-C1*sin(G) + C2*cos(G))
sol2 = F*(C1*cos(G) + C2*sin(G))
return [Eq(x(t), sol1), Eq(y(t), sol2)]
def _linear_2eq_order1_type5(x, y, t, r, eq):
r"""
The equations of this type of ode are .
.. math:: x' = f(t) x + g(t) y
.. math:: y' = a g(t) x + [f(t) + b g(t)] y
The transformation of
.. math:: x = e^{\int f(t) \,dt} u , y = e^{\int f(t) \,dt} v , T = \int g(t) \,dt
leads to a system of constant coefficient linear differential equations
.. math:: u'(T) = v , v'(T) = au + bv
"""
u, v = symbols('u, v', cls=Function)
T = Symbol('T')
if not cancel(r['c']/r['b']).has(t):
p = cancel(r['c']/r['b'])
q = cancel((r['d']-r['a'])/r['b'])
eq = (Eq(diff(u(T),T), v(T)), Eq(diff(v(T),T), p*u(T)+q*v(T)))
sol = dsolve(eq)
sol1 = exp(Integral(r['a'], t))*sol[0].rhs.subs(T, Integral(r['b'], t))
sol2 = exp(Integral(r['a'], t))*sol[1].rhs.subs(T, Integral(r['b'], t))
if not cancel(r['a']/r['d']).has(t):
p = cancel(r['a']/r['d'])
q = cancel((r['b']-r['c'])/r['d'])
sol = dsolve(Eq(diff(u(T),T), v(T)), Eq(diff(v(T),T), p*u(T)+q*v(T)))
sol1 = exp(Integral(r['c'], t))*sol[1].rhs.subs(T, Integral(r['d'], t))
sol2 = exp(Integral(r['c'], t))*sol[0].rhs.subs(T, Integral(r['d'], t))
return [Eq(x(t), sol1), Eq(y(t), sol2)]
def _linear_2eq_order1_type6(x, y, t, r, eq):
r"""
The equations of this type of ode are .
.. math:: x' = f(t) x + g(t) y
.. math:: y' = a [f(t) + a h(t)] x + a [g(t) - h(t)] y
This is solved by first multiplying the first equation by `-a` and adding
it to the second equation to obtain
.. math:: y' - a x' = -a h(t) (y - a x)
Setting `U = y - ax` and integrating the equation we arrive at
.. math:: y - ax = C_1 e^{-a \int h(t) \,dt}
and on substituting the value of y in first equation give rise to first order ODEs. After solving for
`x`, we can obtain `y` by substituting the value of `x` in second equation.
"""
C1, C2, C3, C4 = get_numbered_constants(eq, num=4)
p = 0
q = 0
p1 = cancel(r['c']/cancel(r['c']/r['d']).as_numer_denom()[0])
p2 = cancel(r['a']/cancel(r['a']/r['b']).as_numer_denom()[0])
for n, i in enumerate([p1, p2]):
for j in Mul.make_args(collect_const(i)):
if not j.has(t):
q = j
if q!=0 and n==0:
if ((r['c']/j - r['a'])/(r['b'] - r['d']/j)) == j:
p = 1
s = j
break
if q!=0 and n==1:
if ((r['a']/j - r['c'])/(r['d'] - r['b']/j)) == j:
p = 2
s = j
break
if p == 1:
equ = diff(x(t),t) - r['a']*x(t) - r['b']*(s*x(t) + C1*exp(-s*Integral(r['b'] - r['d']/s, t)))
hint1 = classify_ode(equ)[1]
sol1 = dsolve(equ, hint=hint1+'_Integral').rhs
sol2 = s*sol1 + C1*exp(-s*Integral(r['b'] - r['d']/s, t))
elif p ==2:
equ = diff(y(t),t) - r['c']*y(t) - r['d']*s*y(t) + C1*exp(-s*Integral(r['d'] - r['b']/s, t))
hint1 = classify_ode(equ)[1]
sol2 = dsolve(equ, hint=hint1+'_Integral').rhs
sol1 = s*sol2 + C1*exp(-s*Integral(r['d'] - r['b']/s, t))
return [Eq(x(t), sol1), Eq(y(t), sol2)]
def _linear_2eq_order1_type7(x, y, t, r, eq):
r"""
The equations of this type of ode are .
.. math:: x' = f(t) x + g(t) y
.. math:: y' = h(t) x + p(t) y
Differentiating the first equation and substituting the value of `y`
from second equation will give a second-order linear equation
.. math:: g x'' - (fg + gp + g') x' + (fgp - g^{2} h + f g' - f' g) x = 0
This above equation can be easily integrated if following conditions are satisfied.
1. `fgp - g^{2} h + f g' - f' g = 0`
2. `fgp - g^{2} h + f g' - f' g = ag, fg + gp + g' = bg`
If first condition is satisfied then it is solved by current dsolve solver and in second case it becomes
a constant coefficient differential equation which is also solved by current solver.
Otherwise if the above condition fails then,
a particular solution is assumed as `x = x_0(t)` and `y = y_0(t)`
Then the general solution is expressed as
.. math:: x = C_1 x_0(t) + C_2 x_0(t) \int \frac{g(t) F(t) P(t)}{x_0^{2}(t)} \,dt
.. math:: y = C_1 y_0(t) + C_2 [\frac{F(t) P(t)}{x_0(t)} + y_0(t) \int \frac{g(t) F(t) P(t)}{x_0^{2}(t)} \,dt]
where C1 and C2 are arbitrary constants and
.. math:: F(t) = e^{\int f(t) \,dt} , P(t) = e^{\int p(t) \,dt}
"""
C1, C2, C3, C4 = get_numbered_constants(eq, num=4)
e1 = r['a']*r['b']*r['c'] - r['b']**2*r['c'] + r['a']*diff(r['b'],t) - diff(r['a'],t)*r['b']
e2 = r['a']*r['c']*r['d'] - r['b']*r['c']**2 + diff(r['c'],t)*r['d'] - r['c']*diff(r['d'],t)
m1 = r['a']*r['b'] + r['b']*r['d'] + diff(r['b'],t)
m2 = r['a']*r['c'] + r['c']*r['d'] + diff(r['c'],t)
if e1 == 0:
sol1 = dsolve(r['b']*diff(x(t),t,t) - m1*diff(x(t),t)).rhs
sol2 = dsolve(diff(y(t),t) - r['c']*sol1 - r['d']*y(t)).rhs
elif e2 == 0:
sol2 = dsolve(r['c']*diff(y(t),t,t) - m2*diff(y(t),t)).rhs
sol1 = dsolve(diff(x(t),t) - r['a']*x(t) - r['b']*sol2).rhs
elif not (e1/r['b']).has(t) and not (m1/r['b']).has(t):
sol1 = dsolve(diff(x(t),t,t) - (m1/r['b'])*diff(x(t),t) - (e1/r['b'])*x(t)).rhs
sol2 = dsolve(diff(y(t),t) - r['c']*sol1 - r['d']*y(t)).rhs
elif not (e2/r['c']).has(t) and not (m2/r['c']).has(t):
sol2 = dsolve(diff(y(t),t,t) - (m2/r['c'])*diff(y(t),t) - (e2/r['c'])*y(t)).rhs
sol1 = dsolve(diff(x(t),t) - r['a']*x(t) - r['b']*sol2).rhs
else:
x0 = Function('x0')(t) # x0 and y0 being particular solutions
y0 = Function('y0')(t)
F = exp(Integral(r['a'],t))
P = exp(Integral(r['d'],t))
sol1 = C1*x0 + C2*x0*Integral(r['b']*F*P/x0**2, t)
sol2 = C1*y0 + C2*(F*P/x0 + y0*Integral(r['b']*F*P/x0**2, t))
return [Eq(x(t), sol1), Eq(y(t), sol2)]
def sysode_linear_2eq_order2(match_):
x = match_['func'][0].func
y = match_['func'][1].func
func = match_['func']
fc = match_['func_coeff']
eq = match_['eq']
r = dict()
t = list(list(eq[0].atoms(Derivative))[0].atoms(Symbol))[0]
for i in range(2):
eqs = []
for terms in Add.make_args(eq[i]):
eqs.append(terms/fc[i,func[i],2])
eq[i] = Add(*eqs)
# for equations Eq(diff(x(t),t,t), a1*diff(x(t),t)+b1*diff(y(t),t)+c1*x(t)+d1*y(t)+e1)
# and Eq(a2*diff(y(t),t,t), a2*diff(x(t),t)+b2*diff(y(t),t)+c2*x(t)+d2*y(t)+e2)
r['a1'] = -fc[0,x(t),1]/fc[0,x(t),2] ; r['a2'] = -fc[1,x(t),1]/fc[1,y(t),2]
r['b1'] = -fc[0,y(t),1]/fc[0,x(t),2] ; r['b2'] = -fc[1,y(t),1]/fc[1,y(t),2]
r['c1'] = -fc[0,x(t),0]/fc[0,x(t),2] ; r['c2'] = -fc[1,x(t),0]/fc[1,y(t),2]
r['d1'] = -fc[0,y(t),0]/fc[0,x(t),2] ; r['d2'] = -fc[1,y(t),0]/fc[1,y(t),2]
const = [S.Zero, S.Zero]
for i in range(2):
for j in Add.make_args(eq[i]):
if not (j.has(x(t)) or j.has(y(t))):
const[i] += j
r['e1'] = -const[0]
r['e2'] = -const[1]
if match_['type_of_equation'] == 'type1':
sol = _linear_2eq_order2_type1(x, y, t, r, eq)
elif match_['type_of_equation'] == 'type2':
gsol = _linear_2eq_order2_type1(x, y, t, r, eq)
psol = _linear_2eq_order2_type2(x, y, t, r, eq)
sol = [Eq(x(t), gsol[0].rhs+psol[0]), Eq(y(t), gsol[1].rhs+psol[1])]
elif match_['type_of_equation'] == 'type3':
sol = _linear_2eq_order2_type3(x, y, t, r, eq)
elif match_['type_of_equation'] == 'type4':
sol = _linear_2eq_order2_type4(x, y, t, r, eq)
elif match_['type_of_equation'] == 'type5':
sol = _linear_2eq_order2_type5(x, y, t, r, eq)
elif match_['type_of_equation'] == 'type6':
sol = _linear_2eq_order2_type6(x, y, t, r, eq)
elif match_['type_of_equation'] == 'type7':
sol = _linear_2eq_order2_type7(x, y, t, r, eq)
elif match_['type_of_equation'] == 'type8':
sol = _linear_2eq_order2_type8(x, y, t, r, eq)
elif match_['type_of_equation'] == 'type9':
sol = _linear_2eq_order2_type9(x, y, t, r, eq)
elif match_['type_of_equation'] == 'type10':
sol = _linear_2eq_order2_type10(x, y, t, r, eq)
elif match_['type_of_equation'] == 'type11':
sol = _linear_2eq_order2_type11(x, y, t, r, eq)
return sol
def _linear_2eq_order2_type1(x, y, t, r, eq):
r"""
System of two constant-coefficient second-order linear homogeneous differential equations
.. math:: x'' = ax + by
.. math:: y'' = cx + dy
The characteristic equation for above equations
.. math:: \lambda^4 - (a + d) \lambda^2 + ad - bc = 0
whose discriminant is `D = (a - d)^2 + 4bc \neq 0`
1. When `ad - bc \neq 0`
1.1. If `D \neq 0`. The characteristic equation has four distinct roots, `\lambda_1, \lambda_2, \lambda_3, \lambda_4`.
The general solution of the system is
.. math:: x = C_1 b e^{\lambda_1 t} + C_2 b e^{\lambda_2 t} + C_3 b e^{\lambda_3 t} + C_4 b e^{\lambda_4 t}
.. math:: y = C_1 (\lambda_1^{2} - a) e^{\lambda_1 t} + C_2 (\lambda_2^{2} - a) e^{\lambda_2 t} + C_3 (\lambda_3^{2} - a) e^{\lambda_3 t} + C_4 (\lambda_4^{2} - a) e^{\lambda_4 t}
where `C_1,..., C_4` are arbitrary constants.
1.2. If `D = 0` and `a \neq d`:
.. math:: x = 2 C_1 (bt + \frac{2bk}{a - d}) e^{\frac{kt}{2}} + 2 C_2 (bt + \frac{2bk}{a - d}) e^{\frac{-kt}{2}} + 2b C_3 t e^{\frac{kt}{2}} + 2b C_4 t e^{\frac{-kt}{2}}
.. math:: y = C_1 (d - a) t e^{\frac{kt}{2}} + C_2 (d - a) t e^{\frac{-kt}{2}} + C_3 [(d - a) t + 2k] e^{\frac{kt}{2}} + C_4 [(d - a) t - 2k] e^{\frac{-kt}{2}}
where `C_1,..., C_4` are arbitrary constants and `k = \sqrt{2 (a + d)}`
1.3. If `D = 0` and `a = d \neq 0` and `b = 0`:
.. math:: x = 2 \sqrt{a} C_1 e^{\sqrt{a} t} + 2 \sqrt{a} C_2 e^{-\sqrt{a} t}
.. math:: y = c C_1 t e^{\sqrt{a} t} - c C_2 t e^{-\sqrt{a} t} + C_3 e^{\sqrt{a} t} + C_4 e^{-\sqrt{a} t}
1.4. If `D = 0` and `a = d \neq 0` and `c = 0`:
.. math:: x = b C_1 t e^{\sqrt{a} t} - b C_2 t e^{-\sqrt{a} t} + C_3 e^{\sqrt{a} t} + C_4 e^{-\sqrt{a} t}
.. math:: y = 2 \sqrt{a} C_1 e^{\sqrt{a} t} + 2 \sqrt{a} C_2 e^{-\sqrt{a} t}
2. When `ad - bc = 0` and `a^2 + b^2 > 0`. Then the original system becomes
.. math:: x'' = ax + by
.. math:: y'' = k (ax + by)
2.1. If `a + bk \neq 0`:
.. math:: x = C_1 e^{t \sqrt{a + bk}} + C_2 e^{-t \sqrt{a + bk}} + C_3 bt + C_4 b
.. math:: y = C_1 k e^{t \sqrt{a + bk}} + C_2 k e^{-t \sqrt{a + bk}} - C_3 at - C_4 a
2.2. If `a + bk = 0`:
.. math:: x = C_1 b t^3 + C_2 b t^2 + C_3 t + C_4
.. math:: y = kx + 6 C_1 t + 2 C_2
"""
r['a'] = r['c1']
r['b'] = r['d1']
r['c'] = r['c2']
r['d'] = r['d2']
l = Symbol('l')
C1, C2, C3, C4 = get_numbered_constants(eq, num=4)
chara_eq = l**4 - (r['a']+r['d'])*l**2 + r['a']*r['d'] - r['b']*r['c']
l1 = rootof(chara_eq, 0)
l2 = rootof(chara_eq, 1)
l3 = rootof(chara_eq, 2)
l4 = rootof(chara_eq, 3)
D = (r['a'] - r['d'])**2 + 4*r['b']*r['c']
if (r['a']*r['d'] - r['b']*r['c']) != 0:
if D != 0:
gsol1 = C1*r['b']*exp(l1*t) + C2*r['b']*exp(l2*t) + C3*r['b']*exp(l3*t) \
+ C4*r['b']*exp(l4*t)
gsol2 = C1*(l1**2-r['a'])*exp(l1*t) + C2*(l2**2-r['a'])*exp(l2*t) + \
C3*(l3**2-r['a'])*exp(l3*t) + C4*(l4**2-r['a'])*exp(l4*t)
else:
if r['a'] != r['d']:
k = sqrt(2*(r['a']+r['d']))
mid = r['b']*t+2*r['b']*k/(r['a']-r['d'])
gsol1 = 2*C1*mid*exp(k*t/2) + 2*C2*mid*exp(-k*t/2) + \
2*r['b']*C3*t*exp(k*t/2) + 2*r['b']*C4*t*exp(-k*t/2)
gsol2 = C1*(r['d']-r['a'])*t*exp(k*t/2) + C2*(r['d']-r['a'])*t*exp(-k*t/2) + \
C3*((r['d']-r['a'])*t+2*k)*exp(k*t/2) + C4*((r['d']-r['a'])*t-2*k)*exp(-k*t/2)
elif r['a'] == r['d'] != 0 and r['b'] == 0:
sa = sqrt(r['a'])
gsol1 = 2*sa*C1*exp(sa*t) + 2*sa*C2*exp(-sa*t)
gsol2 = r['c']*C1*t*exp(sa*t)-r['c']*C2*t*exp(-sa*t)+C3*exp(sa*t)+C4*exp(-sa*t)
elif r['a'] == r['d'] != 0 and r['c'] == 0:
sa = sqrt(r['a'])
gsol1 = r['b']*C1*t*exp(sa*t)-r['b']*C2*t*exp(-sa*t)+C3*exp(sa*t)+C4*exp(-sa*t)
gsol2 = 2*sa*C1*exp(sa*t) + 2*sa*C2*exp(-sa*t)
elif (r['a']*r['d'] - r['b']*r['c']) == 0 and (r['a']**2 + r['b']**2) > 0:
k = r['c']/r['a']
if r['a'] + r['b']*k != 0:
mid = sqrt(r['a'] + r['b']*k)
gsol1 = C1*exp(mid*t) + C2*exp(-mid*t) + C3*r['b']*t + C4*r['b']
gsol2 = C1*k*exp(mid*t) + C2*k*exp(-mid*t) - C3*r['a']*t - C4*r['a']
else:
gsol1 = C1*r['b']*t**3 + C2*r['b']*t**2 + C3*t + C4
gsol2 = k*gsol1 + 6*C1*t + 2*C2
return [Eq(x(t), gsol1), Eq(y(t), gsol2)]
def _linear_2eq_order2_type2(x, y, t, r, eq):
r"""
The equations in this type are
.. math:: x'' = a_1 x + b_1 y + c_1
.. math:: y'' = a_2 x + b_2 y + c_2
The general solution of this system is given by the sum of its particular solution
and the general solution of the homogeneous system. The general solution is given
by the linear system of 2 equation of order 2 and type 1
1. If `a_1 b_2 - a_2 b_1 \neq 0`. A particular solution will be `x = x_0` and `y = y_0`
where the constants `x_0` and `y_0` are determined by solving the linear algebraic system
.. math:: a_1 x_0 + b_1 y_0 + c_1 = 0, a_2 x_0 + b_2 y_0 + c_2 = 0
2. If `a_1 b_2 - a_2 b_1 = 0` and `a_1^2 + b_1^2 > 0`. In this case, the system in question becomes
.. math:: x'' = ax + by + c_1, y'' = k (ax + by) + c_2
2.1. If `\sigma = a + bk \neq 0`, the particular solution will be
.. math:: x = \frac{1}{2} b \sigma^{-1} (c_1 k - c_2) t^2 - \sigma^{-2} (a c_1 + b c_2)
.. math:: y = kx + \frac{1}{2} (c_2 - c_1 k) t^2
2.2. If `\sigma = a + bk = 0`, the particular solution will be
.. math:: x = \frac{1}{24} b (c_2 - c_1 k) t^4 + \frac{1}{2} c_1 t^2
.. math:: y = kx + \frac{1}{2} (c_2 - c_1 k) t^2
"""
x0, y0 = symbols('x0, y0')
if r['c1']*r['d2'] - r['c2']*r['d1'] != 0:
sol = solve((r['c1']*x0+r['d1']*y0+r['e1'], r['c2']*x0+r['d2']*y0+r['e2']), x0, y0)
psol = [sol[x0], sol[y0]]
elif r['c1']*r['d2'] - r['c2']*r['d1'] == 0 and (r['c1']**2 + r['d1']**2) > 0:
k = r['c2']/r['c1']
sig = r['c1'] + r['d1']*k
if sig != 0:
psol1 = r['d1']*sig**-1*(r['e1']*k-r['e2'])*t**2/2 - \
sig**-2*(r['c1']*r['e1']+r['d1']*r['e2'])
psol2 = k*psol1 + (r['e2'] - r['e1']*k)*t**2/2
psol = [psol1, psol2]
else:
psol1 = r['d1']*(r['e2']-r['e1']*k)*t**4/24 + r['e1']*t**2/2
psol2 = k*psol1 + (r['e2']-r['e1']*k)*t**2/2
psol = [psol1, psol2]
return psol
def _linear_2eq_order2_type3(x, y, t, r, eq):
r"""
These type of equation is used for describing the horizontal motion of a pendulum
taking into account the Earth rotation.
The solution is given with `a^2 + 4b > 0`:
.. math:: x = C_1 \cos(\alpha t) + C_2 \sin(\alpha t) + C_3 \cos(\beta t) + C_4 \sin(\beta t)
.. math:: y = -C_1 \sin(\alpha t) + C_2 \cos(\alpha t) - C_3 \sin(\beta t) + C_4 \cos(\beta t)
where `C_1,...,C_4` and
.. math:: \alpha = \frac{1}{2} a + \frac{1}{2} \sqrt{a^2 + 4b}, \beta = \frac{1}{2} a - \frac{1}{2} \sqrt{a^2 + 4b}
"""
C1, C2, C3, C4 = get_numbered_constants(eq, num=4)
if r['b1']**2 - 4*r['c1'] > 0:
r['a'] = r['b1'] ; r['b'] = -r['c1']
alpha = r['a']/2 + sqrt(r['a']**2 + 4*r['b'])/2
beta = r['a']/2 - sqrt(r['a']**2 + 4*r['b'])/2
sol1 = C1*cos(alpha*t) + C2*sin(alpha*t) + C3*cos(beta*t) + C4*sin(beta*t)
sol2 = -C1*sin(alpha*t) + C2*cos(alpha*t) - C3*sin(beta*t) + C4*cos(beta*t)
return [Eq(x(t), sol1), Eq(y(t), sol2)]
def _linear_2eq_order2_type4(x, y, t, r, eq):
r"""
These equations are found in the theory of oscillations
.. math:: x'' + a_1 x' + b_1 y' + c_1 x + d_1 y = k_1 e^{i \omega t}
.. math:: y'' + a_2 x' + b_2 y' + c_2 x + d_2 y = k_2 e^{i \omega t}
The general solution of this linear nonhomogeneous system of constant-coefficient
differential equations is given by the sum of its particular solution and the
general solution of the corresponding homogeneous system (with `k_1 = k_2 = 0`)
1. A particular solution is obtained by the method of undetermined coefficients:
.. math:: x = A_* e^{i \omega t}, y = B_* e^{i \omega t}
On substituting these expressions into the original system of differential equations,
one arrive at a linear nonhomogeneous system of algebraic equations for the
coefficients `A` and `B`.
2. The general solution of the homogeneous system of differential equations is determined
by a linear combination of linearly independent particular solutions determined by
the method of undetermined coefficients in the form of exponentials:
.. math:: x = A e^{\lambda t}, y = B e^{\lambda t}
On substituting these expressions into the original system and collecting the
coefficients of the unknown `A` and `B`, one obtains
.. math:: (\lambda^{2} + a_1 \lambda + c_1) A + (b_1 \lambda + d_1) B = 0
.. math:: (a_2 \lambda + c_2) A + (\lambda^{2} + b_2 \lambda + d_2) B = 0
The determinant of this system must vanish for nontrivial solutions A, B to exist.
This requirement results in the following characteristic equation for `\lambda`
.. math:: (\lambda^2 + a_1 \lambda + c_1) (\lambda^2 + b_2 \lambda + d_2) - (b_1 \lambda + d_1) (a_2 \lambda + c_2) = 0
If all roots `k_1,...,k_4` of this equation are distinct, the general solution of the original
system of the differential equations has the form
.. math:: x = C_1 (b_1 \lambda_1 + d_1) e^{\lambda_1 t} - C_2 (b_1 \lambda_2 + d_1) e^{\lambda_2 t} - C_3 (b_1 \lambda_3 + d_1) e^{\lambda_3 t} - C_4 (b_1 \lambda_4 + d_1) e^{\lambda_4 t}
.. math:: y = C_1 (\lambda_1^{2} + a_1 \lambda_1 + c_1) e^{\lambda_1 t} + C_2 (\lambda_2^{2} + a_1 \lambda_2 + c_1) e^{\lambda_2 t} + C_3 (\lambda_3^{2} + a_1 \lambda_3 + c_1) e^{\lambda_3 t} + C_4 (\lambda_4^{2} + a_1 \lambda_4 + c_1) e^{\lambda_4 t}
"""
C1, C2, C3, C4 = get_numbered_constants(eq, num=4)
k = Symbol('k')
Ra, Ca, Rb, Cb = symbols('Ra, Ca, Rb, Cb')
a1 = r['a1'] ; a2 = r['a2']
b1 = r['b1'] ; b2 = r['b2']
c1 = r['c1'] ; c2 = r['c2']
d1 = r['d1'] ; d2 = r['d2']
k1 = r['e1'].expand().as_independent(t)[0]
k2 = r['e2'].expand().as_independent(t)[0]
ew1 = r['e1'].expand().as_independent(t)[1]
ew2 = powdenest(ew1).as_base_exp()[1]
ew3 = collect(ew2, t).coeff(t)
w = cancel(ew3/I)
# The particular solution is assumed to be (Ra+I*Ca)*exp(I*w*t) and
# (Rb+I*Cb)*exp(I*w*t) for x(t) and y(t) respectively
# peq1, peq2, peq3, peq4 unused
# peq1 = (-w**2+c1)*Ra - a1*w*Ca + d1*Rb - b1*w*Cb - k1
# peq2 = a1*w*Ra + (-w**2+c1)*Ca + b1*w*Rb + d1*Cb
# peq3 = c2*Ra - a2*w*Ca + (-w**2+d2)*Rb - b2*w*Cb - k2
# peq4 = a2*w*Ra + c2*Ca + b2*w*Rb + (-w**2+d2)*Cb
# FIXME: solve for what in what? Ra, Rb, etc I guess
# but then psol not used for anything?
# psol = solve([peq1, peq2, peq3, peq4])
chareq = (k**2+a1*k+c1)*(k**2+b2*k+d2) - (b1*k+d1)*(a2*k+c2)
[k1, k2, k3, k4] = roots_quartic(Poly(chareq))
sol1 = -C1*(b1*k1+d1)*exp(k1*t) - C2*(b1*k2+d1)*exp(k2*t) - \
C3*(b1*k3+d1)*exp(k3*t) - C4*(b1*k4+d1)*exp(k4*t) + (Ra+I*Ca)*exp(I*w*t)
a1_ = (a1-1)
sol2 = C1*(k1**2+a1_*k1+c1)*exp(k1*t) + C2*(k2**2+a1_*k2+c1)*exp(k2*t) + \
C3*(k3**2+a1_*k3+c1)*exp(k3*t) + C4*(k4**2+a1_*k4+c1)*exp(k4*t) + (Rb+I*Cb)*exp(I*w*t)
return [Eq(x(t), sol1), Eq(y(t), sol2)]
def _linear_2eq_order2_type5(x, y, t, r, eq):
r"""
The equation which come under this category are
.. math:: x'' = a (t y' - y)
.. math:: y'' = b (t x' - x)
The transformation
.. math:: u = t x' - x, b = t y' - y
leads to the first-order system
.. math:: u' = atv, v' = btu
The general solution of this system is given by
If `ab > 0`:
.. math:: u = C_1 a e^{\frac{1}{2} \sqrt{ab} t^2} + C_2 a e^{-\frac{1}{2} \sqrt{ab} t^2}
.. math:: v = C_1 \sqrt{ab} e^{\frac{1}{2} \sqrt{ab} t^2} - C_2 \sqrt{ab} e^{-\frac{1}{2} \sqrt{ab} t^2}
If `ab < 0`:
.. math:: u = C_1 a \cos(\frac{1}{2} \sqrt{\left|ab\right|} t^2) + C_2 a \sin(-\frac{1}{2} \sqrt{\left|ab\right|} t^2)
.. math:: v = C_1 \sqrt{\left|ab\right|} \sin(\frac{1}{2} \sqrt{\left|ab\right|} t^2) + C_2 \sqrt{\left|ab\right|} \cos(-\frac{1}{2} \sqrt{\left|ab\right|} t^2)
where `C_1` and `C_2` are arbitrary constants. On substituting the value of `u` and `v`
in above equations and integrating the resulting expressions, the general solution will become
.. math:: x = C_3 t + t \int \frac{u}{t^2} \,dt, y = C_4 t + t \int \frac{u}{t^2} \,dt
where `C_3` and `C_4` are arbitrary constants.
"""
C1, C2, C3, C4 = get_numbered_constants(eq, num=4)
r['a'] = -r['d1'] ; r['b'] = -r['c2']
mul = sqrt(abs(r['a']*r['b']))
if r['a']*r['b'] > 0:
u = C1*r['a']*exp(mul*t**2/2) + C2*r['a']*exp(-mul*t**2/2)
v = C1*mul*exp(mul*t**2/2) - C2*mul*exp(-mul*t**2/2)
else:
u = C1*r['a']*cos(mul*t**2/2) + C2*r['a']*sin(mul*t**2/2)
v = -C1*mul*sin(mul*t**2/2) + C2*mul*cos(mul*t**2/2)
sol1 = C3*t + t*Integral(u/t**2, t)
sol2 = C4*t + t*Integral(v/t**2, t)
return [Eq(x(t), sol1), Eq(y(t), sol2)]
def _linear_2eq_order2_type6(x, y, t, r, eq):
r"""
The equations are
.. math:: x'' = f(t) (a_1 x + b_1 y)
.. math:: y'' = f(t) (a_2 x + b_2 y)
If `k_1` and `k_2` are roots of the quadratic equation
.. math:: k^2 - (a_1 + b_2) k + a_1 b_2 - a_2 b_1 = 0
Then by multiplying appropriate constants and adding together original equations
we obtain two independent equations:
.. math:: z_1'' = k_1 f(t) z_1, z_1 = a_2 x + (k_1 - a_1) y
.. math:: z_2'' = k_2 f(t) z_2, z_2 = a_2 x + (k_2 - a_1) y
Solving the equations will give the values of `x` and `y` after obtaining the value
of `z_1` and `z_2` by solving the differential equation and substituting the result.
"""
k = Symbol('k')
z = Function('z')
num, den = cancel(
(r['c1']*x(t) + r['d1']*y(t))/
(r['c2']*x(t) + r['d2']*y(t))).as_numer_denom()
f = r['c1']/num.coeff(x(t))
a1 = num.coeff(x(t))
b1 = num.coeff(y(t))
a2 = den.coeff(x(t))
b2 = den.coeff(y(t))
chareq = k**2 - (a1 + b2)*k + a1*b2 - a2*b1
k1, k2 = [rootof(chareq, k) for k in range(Poly(chareq).degree())]
z1 = dsolve(diff(z(t),t,t) - k1*f*z(t)).rhs
z2 = dsolve(diff(z(t),t,t) - k2*f*z(t)).rhs
sol1 = (k1*z2 - k2*z1 + a1*(z1 - z2))/(a2*(k1-k2))
sol2 = (z1 - z2)/(k1 - k2)
return [Eq(x(t), sol1), Eq(y(t), sol2)]
def _linear_2eq_order2_type7(x, y, t, r, eq):
r"""
The equations are given as
.. math:: x'' = f(t) (a_1 x' + b_1 y')
.. math:: y'' = f(t) (a_2 x' + b_2 y')
If `k_1` and 'k_2` are roots of the quadratic equation
.. math:: k^2 - (a_1 + b_2) k + a_1 b_2 - a_2 b_1 = 0
Then the system can be reduced by adding together the two equations multiplied
by appropriate constants give following two independent equations:
.. math:: z_1'' = k_1 f(t) z_1', z_1 = a_2 x + (k_1 - a_1) y
.. math:: z_2'' = k_2 f(t) z_2', z_2 = a_2 x + (k_2 - a_1) y
Integrating these and returning to the original variables, one arrives at a linear
algebraic system for the unknowns `x` and `y`:
.. math:: a_2 x + (k_1 - a_1) y = C_1 \int e^{k_1 F(t)} \,dt + C_2
.. math:: a_2 x + (k_2 - a_1) y = C_3 \int e^{k_2 F(t)} \,dt + C_4
where `C_1,...,C_4` are arbitrary constants and `F(t) = \int f(t) \,dt`
"""
C1, C2, C3, C4 = get_numbered_constants(eq, num=4)
k = Symbol('k')
num, den = cancel(
(r['a1']*x(t) + r['b1']*y(t))/
(r['a2']*x(t) + r['b2']*y(t))).as_numer_denom()
f = r['a1']/num.coeff(x(t))
a1 = num.coeff(x(t))
b1 = num.coeff(y(t))
a2 = den.coeff(x(t))
b2 = den.coeff(y(t))
chareq = k**2 - (a1 + b2)*k + a1*b2 - a2*b1
[k1, k2] = [rootof(chareq, k) for k in range(Poly(chareq).degree())]
F = Integral(f, t)
z1 = C1*Integral(exp(k1*F), t) + C2
z2 = C3*Integral(exp(k2*F), t) + C4
sol1 = (k1*z2 - k2*z1 + a1*(z1 - z2))/(a2*(k1-k2))
sol2 = (z1 - z2)/(k1 - k2)
return [Eq(x(t), sol1), Eq(y(t), sol2)]
def _linear_2eq_order2_type8(x, y, t, r, eq):
r"""
The equation of this category are
.. math:: x'' = a f(t) (t y' - y)
.. math:: y'' = b f(t) (t x' - x)
The transformation
.. math:: u = t x' - x, v = t y' - y
leads to the system of first-order equations
.. math:: u' = a t f(t) v, v' = b t f(t) u
The general solution of this system has the form
If `ab > 0`:
.. math:: u = C_1 a e^{\sqrt{ab} \int t f(t) \,dt} + C_2 a e^{-\sqrt{ab} \int t f(t) \,dt}
.. math:: v = C_1 \sqrt{ab} e^{\sqrt{ab} \int t f(t) \,dt} - C_2 \sqrt{ab} e^{-\sqrt{ab} \int t f(t) \,dt}
If `ab < 0`:
.. math:: u = C_1 a \cos(\sqrt{\left|ab\right|} \int t f(t) \,dt) + C_2 a \sin(-\sqrt{\left|ab\right|} \int t f(t) \,dt)
.. math:: v = C_1 \sqrt{\left|ab\right|} \sin(\sqrt{\left|ab\right|} \int t f(t) \,dt) + C_2 \sqrt{\left|ab\right|} \cos(-\sqrt{\left|ab\right|} \int t f(t) \,dt)
where `C_1` and `C_2` are arbitrary constants. On substituting the value of `u` and `v`
in above equations and integrating the resulting expressions, the general solution will become
.. math:: x = C_3 t + t \int \frac{u}{t^2} \,dt, y = C_4 t + t \int \frac{u}{t^2} \,dt
where `C_3` and `C_4` are arbitrary constants.
"""
C1, C2, C3, C4 = get_numbered_constants(eq, num=4)
num, den = cancel(r['d1']/r['c2']).as_numer_denom()
f = -r['d1']/num
a = num
b = den
mul = sqrt(abs(a*b))
Igral = Integral(t*f, t)
if a*b > 0:
u = C1*a*exp(mul*Igral) + C2*a*exp(-mul*Igral)
v = C1*mul*exp(mul*Igral) - C2*mul*exp(-mul*Igral)
else:
u = C1*a*cos(mul*Igral) + C2*a*sin(mul*Igral)
v = -C1*mul*sin(mul*Igral) + C2*mul*cos(mul*Igral)
sol1 = C3*t + t*Integral(u/t**2, t)
sol2 = C4*t + t*Integral(v/t**2, t)
return [Eq(x(t), sol1), Eq(y(t), sol2)]
def _linear_2eq_order2_type9(x, y, t, r, eq):
r"""
.. math:: t^2 x'' + a_1 t x' + b_1 t y' + c_1 x + d_1 y = 0
.. math:: t^2 y'' + a_2 t x' + b_2 t y' + c_2 x + d_2 y = 0
These system of equations are euler type.
The substitution of `t = \sigma e^{\tau} (\sigma \neq 0)` leads to the system of constant
coefficient linear differential equations
.. math:: x'' + (a_1 - 1) x' + b_1 y' + c_1 x + d_1 y = 0
.. math:: y'' + a_2 x' + (b_2 - 1) y' + c_2 x + d_2 y = 0
The general solution of the homogeneous system of differential equations is determined
by a linear combination of linearly independent particular solutions determined by
the method of undetermined coefficients in the form of exponentials
.. math:: x = A e^{\lambda t}, y = B e^{\lambda t}
On substituting these expressions into the original system and collecting the
coefficients of the unknown `A` and `B`, one obtains
.. math:: (\lambda^{2} + (a_1 - 1) \lambda + c_1) A + (b_1 \lambda + d_1) B = 0
.. math:: (a_2 \lambda + c_2) A + (\lambda^{2} + (b_2 - 1) \lambda + d_2) B = 0
The determinant of this system must vanish for nontrivial solutions A, B to exist.
This requirement results in the following characteristic equation for `\lambda`
.. math:: (\lambda^2 + (a_1 - 1) \lambda + c_1) (\lambda^2 + (b_2 - 1) \lambda + d_2) - (b_1 \lambda + d_1) (a_2 \lambda + c_2) = 0
If all roots `k_1,...,k_4` of this equation are distinct, the general solution of the original
system of the differential equations has the form
.. math:: x = C_1 (b_1 \lambda_1 + d_1) e^{\lambda_1 t} - C_2 (b_1 \lambda_2 + d_1) e^{\lambda_2 t} - C_3 (b_1 \lambda_3 + d_1) e^{\lambda_3 t} - C_4 (b_1 \lambda_4 + d_1) e^{\lambda_4 t}
.. math:: y = C_1 (\lambda_1^{2} + (a_1 - 1) \lambda_1 + c_1) e^{\lambda_1 t} + C_2 (\lambda_2^{2} + (a_1 - 1) \lambda_2 + c_1) e^{\lambda_2 t} + C_3 (\lambda_3^{2} + (a_1 - 1) \lambda_3 + c_1) e^{\lambda_3 t} + C_4 (\lambda_4^{2} + (a_1 - 1) \lambda_4 + c_1) e^{\lambda_4 t}
"""
C1, C2, C3, C4 = get_numbered_constants(eq, num=4)
k = Symbol('k')
a1 = -r['a1']*t; a2 = -r['a2']*t
b1 = -r['b1']*t; b2 = -r['b2']*t
c1 = -r['c1']*t**2; c2 = -r['c2']*t**2
d1 = -r['d1']*t**2; d2 = -r['d2']*t**2
eq = (k**2+(a1-1)*k+c1)*(k**2+(b2-1)*k+d2)-(b1*k+d1)*(a2*k+c2)
[k1, k2, k3, k4] = roots_quartic(Poly(eq))
sol1 = -C1*(b1*k1+d1)*exp(k1*log(t)) - C2*(b1*k2+d1)*exp(k2*log(t)) - \
C3*(b1*k3+d1)*exp(k3*log(t)) - C4*(b1*k4+d1)*exp(k4*log(t))
a1_ = (a1-1)
sol2 = C1*(k1**2+a1_*k1+c1)*exp(k1*log(t)) + C2*(k2**2+a1_*k2+c1)*exp(k2*log(t)) \
+ C3*(k3**2+a1_*k3+c1)*exp(k3*log(t)) + C4*(k4**2+a1_*k4+c1)*exp(k4*log(t))
return [Eq(x(t), sol1), Eq(y(t), sol2)]
def _linear_2eq_order2_type10(x, y, t, r, eq):
r"""
The equation of this category are
.. math:: (\alpha t^2 + \beta t + \gamma)^{2} x'' = ax + by
.. math:: (\alpha t^2 + \beta t + \gamma)^{2} y'' = cx + dy
The transformation
.. math:: \tau = \int \frac{1}{\alpha t^2 + \beta t + \gamma} \,dt , u = \frac{x}{\sqrt{\left|\alpha t^2 + \beta t + \gamma\right|}} , v = \frac{y}{\sqrt{\left|\alpha t^2 + \beta t + \gamma\right|}}
leads to a constant coefficient linear system of equations
.. math:: u'' = (a - \alpha \gamma + \frac{1}{4} \beta^{2}) u + b v
.. math:: v'' = c u + (d - \alpha \gamma + \frac{1}{4} \beta^{2}) v
These system of equations obtained can be solved by type1 of System of two
constant-coefficient second-order linear homogeneous differential equations.
"""
u, v = symbols('u, v', cls=Function)
assert False
p = Wild('p', exclude=[t, t**2])
q = Wild('q', exclude=[t, t**2])
s = Wild('s', exclude=[t, t**2])
n = Wild('n', exclude=[t, t**2])
num, den = r['c1'].as_numer_denom()
dic = den.match((n*(p*t**2+q*t+s)**2).expand())
eqz = dic[p]*t**2 + dic[q]*t + dic[s]
a = num/dic[n]
b = cancel(r['d1']*eqz**2)
c = cancel(r['c2']*eqz**2)
d = cancel(r['d2']*eqz**2)
[msol1, msol2] = dsolve([Eq(diff(u(t), t, t), (a - dic[p]*dic[s] + dic[q]**2/4)*u(t) \
+ b*v(t)), Eq(diff(v(t),t,t), c*u(t) + (d - dic[p]*dic[s] + dic[q]**2/4)*v(t))])
sol1 = (msol1.rhs*sqrt(abs(eqz))).subs(t, Integral(1/eqz, t))
sol2 = (msol2.rhs*sqrt(abs(eqz))).subs(t, Integral(1/eqz, t))
return [Eq(x(t), sol1), Eq(y(t), sol2)]
def _linear_2eq_order2_type11(x, y, t, r, eq):
r"""
The equations which comes under this type are
.. math:: x'' = f(t) (t x' - x) + g(t) (t y' - y)
.. math:: y'' = h(t) (t x' - x) + p(t) (t y' - y)
The transformation
.. math:: u = t x' - x, v = t y' - y
leads to the linear system of first-order equations
.. math:: u' = t f(t) u + t g(t) v, v' = t h(t) u + t p(t) v
On substituting the value of `u` and `v` in transformed equation gives value of `x` and `y` as
.. math:: x = C_3 t + t \int \frac{u}{t^2} \,dt , y = C_4 t + t \int \frac{v}{t^2} \,dt.
where `C_3` and `C_4` are arbitrary constants.
"""
C1, C2, C3, C4 = get_numbered_constants(eq, num=4)
u, v = symbols('u, v', cls=Function)
f = -r['c1'] ; g = -r['d1']
h = -r['c2'] ; p = -r['d2']
[msol1, msol2] = dsolve([Eq(diff(u(t),t), t*f*u(t) + t*g*v(t)), Eq(diff(v(t),t), t*h*u(t) + t*p*v(t))])
sol1 = C3*t + t*Integral(msol1.rhs/t**2, t)
sol2 = C4*t + t*Integral(msol2.rhs/t**2, t)
return [Eq(x(t), sol1), Eq(y(t), sol2)]
def sysode_linear_3eq_order1(match_):
x = match_['func'][0].func
y = match_['func'][1].func
z = match_['func'][2].func
func = match_['func']
fc = match_['func_coeff']
eq = match_['eq']
r = dict()
t = list(list(eq[0].atoms(Derivative))[0].atoms(Symbol))[0]
for i in range(3):
eqs = 0
for terms in Add.make_args(eq[i]):
eqs += terms/fc[i,func[i],1]
eq[i] = eqs
# for equations:
# Eq(g1*diff(x(t),t), a1*x(t)+b1*y(t)+c1*z(t)+d1),
# Eq(g2*diff(y(t),t), a2*x(t)+b2*y(t)+c2*z(t)+d2), and
# Eq(g3*diff(z(t),t), a3*x(t)+b3*y(t)+c3*z(t)+d3)
r['a1'] = fc[0,x(t),0]/fc[0,x(t),1]; r['a2'] = fc[1,x(t),0]/fc[1,y(t),1];
r['a3'] = fc[2,x(t),0]/fc[2,z(t),1]
r['b1'] = fc[0,y(t),0]/fc[0,x(t),1]; r['b2'] = fc[1,y(t),0]/fc[1,y(t),1];
r['b3'] = fc[2,y(t),0]/fc[2,z(t),1]
r['c1'] = fc[0,z(t),0]/fc[0,x(t),1]; r['c2'] = fc[1,z(t),0]/fc[1,y(t),1];
r['c3'] = fc[2,z(t),0]/fc[2,z(t),1]
for i in range(3):
for j in Add.make_args(eq[i]):
if not j.has(x(t), y(t), z(t)):
raise NotImplementedError("Only homogeneous problems are supported, non-homogeneous are not supported currently.")
if match_['type_of_equation'] == 'type1':
sol = _linear_3eq_order1_type1(x, y, z, t, r, eq)
if match_['type_of_equation'] == 'type2':
sol = _linear_3eq_order1_type2(x, y, z, t, r, eq)
if match_['type_of_equation'] == 'type3':
sol = _linear_3eq_order1_type3(x, y, z, t, r, eq)
if match_['type_of_equation'] == 'type4':
sol = _linear_3eq_order1_type4(x, y, z, t, r, eq)
if match_['type_of_equation'] == 'type6':
sol = _linear_neq_order1_type1(match_)
return sol
def _linear_3eq_order1_type1(x, y, z, t, r, eq):
r"""
.. math:: x' = ax
.. math:: y' = bx + cy
.. math:: z' = dx + ky + pz
Solution of such equations are forward substitution. Solving first equations
gives the value of `x`, substituting it in second and third equation and
solving second equation gives `y` and similarly substituting `y` in third
equation give `z`.
.. math:: x = C_1 e^{at}
.. math:: y = \frac{b C_1}{a - c} e^{at} + C_2 e^{ct}
.. math:: z = \frac{C_1}{a - p} (d + \frac{bk}{a - c}) e^{at} + \frac{k C_2}{c - p} e^{ct} + C_3 e^{pt}
where `C_1, C_2` and `C_3` are arbitrary constants.
"""
C1, C2, C3, C4 = get_numbered_constants(eq, num=4)
a = -r['a1']; b = -r['a2']; c = -r['b2']
d = -r['a3']; k = -r['b3']; p = -r['c3']
sol1 = C1*exp(a*t)
sol2 = b*C1*exp(a*t)/(a-c) + C2*exp(c*t)
sol3 = C1*(d+b*k/(a-c))*exp(a*t)/(a-p) + k*C2*exp(c*t)/(c-p) + C3*exp(p*t)
return [Eq(x(t), sol1), Eq(y(t), sol2), Eq(z(t), sol3)]
def _linear_3eq_order1_type2(x, y, z, t, r, eq):
r"""
The equations of this type are
.. math:: x' = cy - bz
.. math:: y' = az - cx
.. math:: z' = bx - ay
1. First integral:
.. math:: ax + by + cz = A \qquad - (1)
.. math:: x^2 + y^2 + z^2 = B^2 \qquad - (2)
where `A` and `B` are arbitrary constants. It follows from these integrals
that the integral lines are circles formed by the intersection of the planes
`(1)` and sphere `(2)`
2. Solution:
.. math:: x = a C_0 + k C_1 \cos(kt) + (c C_2 - b C_3) \sin(kt)
.. math:: y = b C_0 + k C_2 \cos(kt) + (a C_2 - c C_3) \sin(kt)
.. math:: z = c C_0 + k C_3 \cos(kt) + (b C_2 - a C_3) \sin(kt)
where `k = \sqrt{a^2 + b^2 + c^2}` and the four constants of integration,
`C_1,...,C_4` are constrained by a single relation,
.. math:: a C_1 + b C_2 + c C_3 = 0
"""
C0, C1, C2, C3 = get_numbered_constants(eq, num=4, start=0)
a = -r['c2']; b = -r['a3']; c = -r['b1']
k = sqrt(a**2 + b**2 + c**2)
C3 = (-a*C1 - b*C2)/c
sol1 = a*C0 + k*C1*cos(k*t) + (c*C2-b*C3)*sin(k*t)
sol2 = b*C0 + k*C2*cos(k*t) + (a*C3-c*C1)*sin(k*t)
sol3 = c*C0 + k*C3*cos(k*t) + (b*C1-a*C2)*sin(k*t)
return [Eq(x(t), sol1), Eq(y(t), sol2), Eq(z(t), sol3)]
def _linear_3eq_order1_type3(x, y, z, t, r, eq):
r"""
Equations of this system of ODEs
.. math:: a x' = bc (y - z)
.. math:: b y' = ac (z - x)
.. math:: c z' = ab (x - y)
1. First integral:
.. math:: a^2 x + b^2 y + c^2 z = A
where A is an arbitrary constant. It follows that the integral lines are plane curves.
2. Solution:
.. math:: x = C_0 + k C_1 \cos(kt) + a^{-1} bc (C_2 - C_3) \sin(kt)
.. math:: y = C_0 + k C_2 \cos(kt) + a b^{-1} c (C_3 - C_1) \sin(kt)
.. math:: z = C_0 + k C_3 \cos(kt) + ab c^{-1} (C_1 - C_2) \sin(kt)
where `k = \sqrt{a^2 + b^2 + c^2}` and the four constants of integration,
`C_1,...,C_4` are constrained by a single relation
.. math:: a^2 C_1 + b^2 C_2 + c^2 C_3 = 0
"""
C0, C1, C2, C3 = get_numbered_constants(eq, num=4, start=0)
c = sqrt(r['b1']*r['c2'])
b = sqrt(r['b1']*r['a3'])
a = sqrt(r['c2']*r['a3'])
C3 = (-a**2*C1-b**2*C2)/c**2
k = sqrt(a**2 + b**2 + c**2)
sol1 = C0 + k*C1*cos(k*t) + a**-1*b*c*(C2-C3)*sin(k*t)
sol2 = C0 + k*C2*cos(k*t) + a*b**-1*c*(C3-C1)*sin(k*t)
sol3 = C0 + k*C3*cos(k*t) + a*b*c**-1*(C1-C2)*sin(k*t)
return [Eq(x(t), sol1), Eq(y(t), sol2), Eq(z(t), sol3)]
def _linear_3eq_order1_type4(x, y, z, t, r, eq):
r"""
Equations:
.. math:: x' = (a_1 f(t) + g(t)) x + a_2 f(t) y + a_3 f(t) z
.. math:: y' = b_1 f(t) x + (b_2 f(t) + g(t)) y + b_3 f(t) z
.. math:: z' = c_1 f(t) x + c_2 f(t) y + (c_3 f(t) + g(t)) z
The transformation
.. math:: x = e^{\int g(t) \,dt} u, y = e^{\int g(t) \,dt} v, z = e^{\int g(t) \,dt} w, \tau = \int f(t) \,dt
leads to the system of constant coefficient linear differential equations
.. math:: u' = a_1 u + a_2 v + a_3 w
.. math:: v' = b_1 u + b_2 v + b_3 w
.. math:: w' = c_1 u + c_2 v + c_3 w
These system of equations are solved by homogeneous linear system of constant
coefficients of `n` equations of first order. Then substituting the value of
`u, v` and `w` in transformed equation gives value of `x, y` and `z`.
"""
u, v, w = symbols('u, v, w', cls=Function)
a2, a3 = cancel(r['b1']/r['c1']).as_numer_denom()
f = cancel(r['b1']/a2)
b1 = cancel(r['a2']/f); b3 = cancel(r['c2']/f)
c1 = cancel(r['a3']/f); c2 = cancel(r['b3']/f)
a1, g = div(r['a1'],f)
b2 = div(r['b2'],f)[0]
c3 = div(r['c3'],f)[0]
trans_eq = (diff(u(t),t)-a1*u(t)-a2*v(t)-a3*w(t), diff(v(t),t)-b1*u(t)-\
b2*v(t)-b3*w(t), diff(w(t),t)-c1*u(t)-c2*v(t)-c3*w(t))
sol = dsolve(trans_eq)
sol1 = exp(Integral(g,t))*((sol[0].rhs).subs(t, Integral(f,t)))
sol2 = exp(Integral(g,t))*((sol[1].rhs).subs(t, Integral(f,t)))
sol3 = exp(Integral(g,t))*((sol[2].rhs).subs(t, Integral(f,t)))
return [Eq(x(t), sol1), Eq(y(t), sol2), Eq(z(t), sol3)]
def sysode_linear_neq_order1(match_):
sol = _linear_neq_order1_type1(match_)
return sol
def _linear_neq_order1_type1(match_):
r"""
System of n first-order constant-coefficient linear nonhomogeneous differential equation
.. math:: y'_k = a_{k1} y_1 + a_{k2} y_2 +...+ a_{kn} y_n; k = 1,2,...,n
or that can be written as `\vec{y'} = A . \vec{y}`
where `\vec{y}` is matrix of `y_k` for `k = 1,2,...n` and `A` is a `n \times n` matrix.
Since these equations are equivalent to a first order homogeneous linear
differential equation. So the general solution will contain `n` linearly
independent parts and solution will consist some type of exponential
functions. Assuming `y = \vec{v} e^{rt}` is a solution of the system where
`\vec{v}` is a vector of coefficients of `y_1,...,y_n`. Substituting `y` and
`y' = r v e^{r t}` into the equation `\vec{y'} = A . \vec{y}`, we get
.. math:: r \vec{v} e^{rt} = A \vec{v} e^{rt}
.. math:: r \vec{v} = A \vec{v}
where `r` comes out to be eigenvalue of `A` and vector `\vec{v}` is the eigenvector
of `A` corresponding to `r`. There are three possibilities of eigenvalues of `A`
- `n` distinct real eigenvalues
- complex conjugate eigenvalues
- eigenvalues with multiplicity `k`
1. When all eigenvalues `r_1,..,r_n` are distinct with `n` different eigenvectors
`v_1,...v_n` then the solution is given by
.. math:: \vec{y} = C_1 e^{r_1 t} \vec{v_1} + C_2 e^{r_2 t} \vec{v_2} +...+ C_n e^{r_n t} \vec{v_n}
where `C_1,C_2,...,C_n` are arbitrary constants.
2. When some eigenvalues are complex then in order to make the solution real,
we take a linear combination: if `r = a + bi` has an eigenvector
`\vec{v} = \vec{w_1} + i \vec{w_2}` then to obtain real-valued solutions to
the system, replace the complex-valued solutions `e^{rx} \vec{v}`
with real-valued solution `e^{ax} (\vec{w_1} \cos(bx) - \vec{w_2} \sin(bx))`
and for `r = a - bi` replace the solution `e^{-r x} \vec{v}` with
`e^{ax} (\vec{w_1} \sin(bx) + \vec{w_2} \cos(bx))`
3. If some eigenvalues are repeated. Then we get fewer than `n` linearly
independent eigenvectors, we miss some of the solutions and need to
construct the missing ones. We do this via generalized eigenvectors, vectors
which are not eigenvectors but are close enough that we can use to write
down the remaining solutions. For a eigenvalue `r` with eigenvector `\vec{w}`
we obtain `\vec{w_2},...,\vec{w_k}` using
.. math:: (A - r I) . \vec{w_2} = \vec{w}
.. math:: (A - r I) . \vec{w_3} = \vec{w_2}
.. math:: \vdots
.. math:: (A - r I) . \vec{w_k} = \vec{w_{k-1}}
Then the solutions to the system for the eigenspace are `e^{rt} [\vec{w}],
e^{rt} [t \vec{w} + \vec{w_2}], e^{rt} [\frac{t^2}{2} \vec{w} + t \vec{w_2} + \vec{w_3}],
...,e^{rt} [\frac{t^{k-1}}{(k-1)!} \vec{w} + \frac{t^{k-2}}{(k-2)!} \vec{w_2} +...+ t \vec{w_{k-1}}
+ \vec{w_k}]`
So, If `\vec{y_1},...,\vec{y_n}` are `n` solution of obtained from three
categories of `A`, then general solution to the system `\vec{y'} = A . \vec{y}`
.. math:: \vec{y} = C_1 \vec{y_1} + C_2 \vec{y_2} + \cdots + C_n \vec{y_n}
"""
eq = match_['eq']
func = match_['func']
fc = match_['func_coeff']
n = len(eq)
t = list(list(eq[0].atoms(Derivative))[0].atoms(Symbol))[0]
constants = numbered_symbols(prefix='C', cls=Symbol, start=1)
M = Matrix(n,n,lambda i,j:-fc[i,func[j],0])
evector = M.eigenvects(simplify=True)
def is_complex(mat, root):
return Matrix(n, 1, lambda i,j: re(mat[i])*cos(im(root)*t) - im(mat[i])*sin(im(root)*t))
def is_complex_conjugate(mat, root):
return Matrix(n, 1, lambda i,j: re(mat[i])*sin(abs(im(root))*t) + im(mat[i])*cos(im(root)*t)*abs(im(root))/im(root))
conjugate_root = []
e_vector = zeros(n,1)
for evects in evector:
if evects[0] not in conjugate_root:
# If number of column of an eigenvector is not equal to the multiplicity
# of its eigenvalue then the legt eigenvectors are calculated
if len(evects[2])!=evects[1]:
var_mat = Matrix(n, 1, lambda i,j: Symbol('x'+str(i)))
Mnew = (M - evects[0]*eye(evects[2][-1].rows))*var_mat
w = [0 for i in range(evects[1])]
w[0] = evects[2][-1]
for r in range(1, evects[1]):
w_ = Mnew - w[r-1]
sol_dict = solve(list(w_), var_mat[1:])
sol_dict[var_mat[0]] = var_mat[0]
for key, value in sol_dict.items():
sol_dict[key] = value.subs(var_mat[0],1)
w[r] = Matrix(n, 1, lambda i,j: sol_dict[var_mat[i]])
evects[2].append(w[r])
for i in range(evects[1]):
C = next(constants)
for j in range(i+1):
if evects[0].has(I):
evects[2][j] = simplify(evects[2][j])
e_vector += C*is_complex(evects[2][j], evects[0])*t**(i-j)*exp(re(evects[0])*t)/factorial(i-j)
C = next(constants)
e_vector += C*is_complex_conjugate(evects[2][j], evects[0])*t**(i-j)*exp(re(evects[0])*t)/factorial(i-j)
else:
e_vector += C*evects[2][j]*t**(i-j)*exp(evects[0]*t)/factorial(i-j)
if evects[0].has(I):
conjugate_root.append(conjugate(evects[0]))
sol = []
for i in range(len(eq)):
sol.append(Eq(func[i],e_vector[i]))
return sol
def sysode_nonlinear_2eq_order1(match_):
func = match_['func']
eq = match_['eq']
fc = match_['func_coeff']
t = list(list(eq[0].atoms(Derivative))[0].atoms(Symbol))[0]
if match_['type_of_equation'] == 'type5':
sol = _nonlinear_2eq_order1_type5(func, t, eq)
return sol
x = func[0].func
y = func[1].func
for i in range(2):
eqs = 0
for terms in Add.make_args(eq[i]):
eqs += terms/fc[i,func[i],1]
eq[i] = eqs
if match_['type_of_equation'] == 'type1':
sol = _nonlinear_2eq_order1_type1(x, y, t, eq)
elif match_['type_of_equation'] == 'type2':
sol = _nonlinear_2eq_order1_type2(x, y, t, eq)
elif match_['type_of_equation'] == 'type3':
sol = _nonlinear_2eq_order1_type3(x, y, t, eq)
elif match_['type_of_equation'] == 'type4':
sol = _nonlinear_2eq_order1_type4(x, y, t, eq)
return sol
def _nonlinear_2eq_order1_type1(x, y, t, eq):
r"""
Equations:
.. math:: x' = x^n F(x,y)
.. math:: y' = g(y) F(x,y)
Solution:
.. math:: x = \varphi(y), \int \frac{1}{g(y) F(\varphi(y),y)} \,dy = t + C_2
where
if `n \neq 1`
.. math:: \varphi = [C_1 + (1-n) \int \frac{1}{g(y)} \,dy]^{\frac{1}{1-n}}
if `n = 1`
.. math:: \varphi = C_1 e^{\int \frac{1}{g(y)} \,dy}
where `C_1` and `C_2` are arbitrary constants.
"""
C1, C2 = get_numbered_constants(eq, num=2)
n = Wild('n', exclude=[x(t),y(t)])
f = Wild('f')
u, v = symbols('u, v')
r = eq[0].match(diff(x(t),t) - x(t)**n*f)
g = ((diff(y(t),t) - eq[1])/r[f]).subs(y(t),v)
F = r[f].subs(x(t),u).subs(y(t),v)
n = r[n]
if n!=1:
phi = (C1 + (1-n)*Integral(1/g, v))**(1/(1-n))
else:
phi = C1*exp(Integral(1/g, v))
phi = phi.doit()
sol2 = solve(Integral(1/(g*F.subs(u,phi)), v).doit() - t - C2, v)
sol = []
for sols in sol2:
sol.append(Eq(x(t),phi.subs(v, sols)))
sol.append(Eq(y(t), sols))
return sol
def _nonlinear_2eq_order1_type2(x, y, t, eq):
r"""
Equations:
.. math:: x' = e^{\lambda x} F(x,y)
.. math:: y' = g(y) F(x,y)
Solution:
.. math:: x = \varphi(y), \int \frac{1}{g(y) F(\varphi(y),y)} \,dy = t + C_2
where
if `\lambda \neq 0`
.. math:: \varphi = -\frac{1}{\lambda} log(C_1 - \lambda \int \frac{1}{g(y)} \,dy)
if `\lambda = 0`
.. math:: \varphi = C_1 + \int \frac{1}{g(y)} \,dy
where `C_1` and `C_2` are arbitrary constants.
"""
C1, C2 = get_numbered_constants(eq, num=2)
n = Wild('n', exclude=[x(t),y(t)])
f = Wild('f')
u, v = symbols('u, v')
r = eq[0].match(diff(x(t),t) - exp(n*x(t))*f)
g = ((diff(y(t),t) - eq[1])/r[f]).subs(y(t),v)
F = r[f].subs(x(t),u).subs(y(t),v)
n = r[n]
if n:
phi = -1/n*log(C1 - n*Integral(1/g, v))
else:
phi = C1 + Integral(1/g, v)
phi = phi.doit()
sol2 = solve(Integral(1/(g*F.subs(u,phi)), v).doit() - t - C2, v)
sol = []
for sols in sol2:
sol.append(Eq(x(t),phi.subs(v, sols)))
sol.append(Eq(y(t), sols))
return sol
def _nonlinear_2eq_order1_type3(x, y, t, eq):
r"""
Autonomous system of general form
.. math:: x' = F(x,y)
.. math:: y' = G(x,y)
Assuming `y = y(x, C_1)` where `C_1` is an arbitrary constant is the general
solution of the first-order equation
.. math:: F(x,y) y'_x = G(x,y)
Then the general solution of the original system of equations has the form
.. math:: \int \frac{1}{F(x,y(x,C_1))} \,dx = t + C_1
"""
C1, C2, C3, C4 = get_numbered_constants(eq, num=4)
v = Function('v')
u = Symbol('u')
f = Wild('f')
g = Wild('g')
r1 = eq[0].match(diff(x(t),t) - f)
r2 = eq[1].match(diff(y(t),t) - g)
F = r1[f].subs(x(t), u).subs(y(t), v(u))
G = r2[g].subs(x(t), u).subs(y(t), v(u))
sol2r = dsolve(Eq(diff(v(u), u), G/F))
if isinstance(sol2r, Expr):
sol2r = [sol2r]
for sol2s in sol2r:
sol1 = solve(Integral(1/F.subs(v(u), sol2s.rhs), u).doit() - t - C2, u)
sol = []
for sols in sol1:
sol.append(Eq(x(t), sols))
sol.append(Eq(y(t), (sol2s.rhs).subs(u, sols)))
return sol
def _nonlinear_2eq_order1_type4(x, y, t, eq):
r"""
Equation:
.. math:: x' = f_1(x) g_1(y) \phi(x,y,t)
.. math:: y' = f_2(x) g_2(y) \phi(x,y,t)
First integral:
.. math:: \int \frac{f_2(x)}{f_1(x)} \,dx - \int \frac{g_1(y)}{g_2(y)} \,dy = C
where `C` is an arbitrary constant.
On solving the first integral for `x` (resp., `y` ) and on substituting the
resulting expression into either equation of the original solution, one
arrives at a first-order equation for determining `y` (resp., `x` ).
"""
C1, C2 = get_numbered_constants(eq, num=2)
u, v = symbols('u, v')
U, V = symbols('U, V', cls=Function)
f = Wild('f')
g = Wild('g')
f1 = Wild('f1', exclude=[v,t])
f2 = Wild('f2', exclude=[v,t])
g1 = Wild('g1', exclude=[u,t])
g2 = Wild('g2', exclude=[u,t])
r1 = eq[0].match(diff(x(t),t) - f)
r2 = eq[1].match(diff(y(t),t) - g)
num, den = (
(r1[f].subs(x(t),u).subs(y(t),v))/
(r2[g].subs(x(t),u).subs(y(t),v))).as_numer_denom()
R1 = num.match(f1*g1)
R2 = den.match(f2*g2)
phi = (r1[f].subs(x(t),u).subs(y(t),v))/num
F1 = R1[f1]; F2 = R2[f2]
G1 = R1[g1]; G2 = R2[g2]
sol1r = solve(Integral(F2/F1, u).doit() - Integral(G1/G2,v).doit() - C1, u)
sol2r = solve(Integral(F2/F1, u).doit() - Integral(G1/G2,v).doit() - C1, v)
sol = []
for sols in sol1r:
sol.append(Eq(y(t), dsolve(diff(V(t),t) - F2.subs(u,sols).subs(v,V(t))*G2.subs(v,V(t))*phi.subs(u,sols).subs(v,V(t))).rhs))
for sols in sol2r:
sol.append(Eq(x(t), dsolve(diff(U(t),t) - F1.subs(u,U(t))*G1.subs(v,sols).subs(u,U(t))*phi.subs(v,sols).subs(u,U(t))).rhs))
return set(sol)
def _nonlinear_2eq_order1_type5(func, t, eq):
r"""
Clairaut system of ODEs
.. math:: x = t x' + F(x',y')
.. math:: y = t y' + G(x',y')
The following are solutions of the system
`(i)` straight lines:
.. math:: x = C_1 t + F(C_1, C_2), y = C_2 t + G(C_1, C_2)
where `C_1` and `C_2` are arbitrary constants;
`(ii)` envelopes of the above lines;
`(iii)` continuously differentiable lines made up from segments of the lines
`(i)` and `(ii)`.
"""
C1, C2 = get_numbered_constants(eq, num=2)
f = Wild('f')
g = Wild('g')
def check_type(x, y):
r1 = eq[0].match(t*diff(x(t),t) - x(t) + f)
r2 = eq[1].match(t*diff(y(t),t) - y(t) + g)
if not (r1 and r2):
r1 = eq[0].match(diff(x(t),t) - x(t)/t + f/t)
r2 = eq[1].match(diff(y(t),t) - y(t)/t + g/t)
if not (r1 and r2):
r1 = (-eq[0]).match(t*diff(x(t),t) - x(t) + f)
r2 = (-eq[1]).match(t*diff(y(t),t) - y(t) + g)
if not (r1 and r2):
r1 = (-eq[0]).match(diff(x(t),t) - x(t)/t + f/t)
r2 = (-eq[1]).match(diff(y(t),t) - y(t)/t + g/t)
return [r1, r2]
for func_ in func:
if isinstance(func_, list):
x = func[0][0].func
y = func[0][1].func
[r1, r2] = check_type(x, y)
if not (r1 and r2):
[r1, r2] = check_type(y, x)
x, y = y, x
x1 = diff(x(t),t); y1 = diff(y(t),t)
return {Eq(x(t), C1*t + r1[f].subs(x1,C1).subs(y1,C2)), Eq(y(t), C2*t + r2[g].subs(x1,C1).subs(y1,C2))}
def sysode_nonlinear_3eq_order1(match_):
x = match_['func'][0].func
y = match_['func'][1].func
z = match_['func'][2].func
eq = match_['eq']
t = list(list(eq[0].atoms(Derivative))[0].atoms(Symbol))[0]
if match_['type_of_equation'] == 'type1':
sol = _nonlinear_3eq_order1_type1(x, y, z, t, eq)
if match_['type_of_equation'] == 'type2':
sol = _nonlinear_3eq_order1_type2(x, y, z, t, eq)
if match_['type_of_equation'] == 'type3':
sol = _nonlinear_3eq_order1_type3(x, y, z, t, eq)
if match_['type_of_equation'] == 'type4':
sol = _nonlinear_3eq_order1_type4(x, y, z, t, eq)
if match_['type_of_equation'] == 'type5':
sol = _nonlinear_3eq_order1_type5(x, y, z, t, eq)
return sol
def _nonlinear_3eq_order1_type1(x, y, z, t, eq):
r"""
Equations:
.. math:: a x' = (b - c) y z, \enspace b y' = (c - a) z x, \enspace c z' = (a - b) x y
First Integrals:
.. math:: a x^{2} + b y^{2} + c z^{2} = C_1
.. math:: a^{2} x^{2} + b^{2} y^{2} + c^{2} z^{2} = C_2
where `C_1` and `C_2` are arbitrary constants. On solving the integrals for `y` and
`z` and on substituting the resulting expressions into the first equation of the
system, we arrives at a separable first-order equation on `x`. Similarly doing that
for other two equations, we will arrive at first order equation on `y` and `z` too.
References
==========
-http://eqworld.ipmnet.ru/en/solutions/sysode/sode0401.pdf
"""
C1, C2 = get_numbered_constants(eq, num=2)
u, v, w = symbols('u, v, w')
p = Wild('p', exclude=[x(t), y(t), z(t), t])
q = Wild('q', exclude=[x(t), y(t), z(t), t])
s = Wild('s', exclude=[x(t), y(t), z(t), t])
r = (diff(x(t),t) - eq[0]).match(p*y(t)*z(t))
r.update((diff(y(t),t) - eq[1]).match(q*z(t)*x(t)))
r.update((diff(z(t),t) - eq[2]).match(s*x(t)*y(t)))
n1, d1 = r[p].as_numer_denom()
n2, d2 = r[q].as_numer_denom()
n3, d3 = r[s].as_numer_denom()
val = solve([n1*u-d1*v+d1*w, d2*u+n2*v-d2*w, d3*u-d3*v-n3*w],[u,v])
vals = [val[v], val[u]]
c = lcm(vals[0].as_numer_denom()[1], vals[1].as_numer_denom()[1])
b = vals[0].subs(w, c)
a = vals[1].subs(w, c)
y_x = sqrt(((c*C1-C2) - a*(c-a)*x(t)**2)/(b*(c-b)))
z_x = sqrt(((b*C1-C2) - a*(b-a)*x(t)**2)/(c*(b-c)))
z_y = sqrt(((a*C1-C2) - b*(a-b)*y(t)**2)/(c*(a-c)))
x_y = sqrt(((c*C1-C2) - b*(c-b)*y(t)**2)/(a*(c-a)))
x_z = sqrt(((b*C1-C2) - c*(b-c)*z(t)**2)/(a*(b-a)))
y_z = sqrt(((a*C1-C2) - c*(a-c)*z(t)**2)/(b*(a-b)))
sol1 = dsolve(a*diff(x(t),t) - (b-c)*y_x*z_x)
sol2 = dsolve(b*diff(y(t),t) - (c-a)*z_y*x_y)
sol3 = dsolve(c*diff(z(t),t) - (a-b)*x_z*y_z)
return [sol1, sol2, sol3]
def _nonlinear_3eq_order1_type2(x, y, z, t, eq):
r"""
Equations:
.. math:: a x' = (b - c) y z f(x, y, z, t)
.. math:: b y' = (c - a) z x f(x, y, z, t)
.. math:: c z' = (a - b) x y f(x, y, z, t)
First Integrals:
.. math:: a x^{2} + b y^{2} + c z^{2} = C_1
.. math:: a^{2} x^{2} + b^{2} y^{2} + c^{2} z^{2} = C_2
where `C_1` and `C_2` are arbitrary constants. On solving the integrals for `y` and
`z` and on substituting the resulting expressions into the first equation of the
system, we arrives at a first-order differential equations on `x`. Similarly doing
that for other two equations we will arrive at first order equation on `y` and `z`.
References
==========
-http://eqworld.ipmnet.ru/en/solutions/sysode/sode0402.pdf
"""
C1, C2 = get_numbered_constants(eq, num=2)
u, v, w = symbols('u, v, w')
p = Wild('p', exclude=[x(t), y(t), z(t), t])
q = Wild('q', exclude=[x(t), y(t), z(t), t])
s = Wild('s', exclude=[x(t), y(t), z(t), t])
f = Wild('f')
r1 = (diff(x(t),t) - eq[0]).match(y(t)*z(t)*f)
r = collect_const(r1[f]).match(p*f)
r.update(((diff(y(t),t) - eq[1])/r[f]).match(q*z(t)*x(t)))
r.update(((diff(z(t),t) - eq[2])/r[f]).match(s*x(t)*y(t)))
n1, d1 = r[p].as_numer_denom()
n2, d2 = r[q].as_numer_denom()
n3, d3 = r[s].as_numer_denom()
val = solve([n1*u-d1*v+d1*w, d2*u+n2*v-d2*w, -d3*u+d3*v+n3*w],[u,v])
vals = [val[v], val[u]]
c = lcm(vals[0].as_numer_denom()[1], vals[1].as_numer_denom()[1])
a = vals[0].subs(w, c)
b = vals[1].subs(w, c)
y_x = sqrt(((c*C1-C2) - a*(c-a)*x(t)**2)/(b*(c-b)))
z_x = sqrt(((b*C1-C2) - a*(b-a)*x(t)**2)/(c*(b-c)))
z_y = sqrt(((a*C1-C2) - b*(a-b)*y(t)**2)/(c*(a-c)))
x_y = sqrt(((c*C1-C2) - b*(c-b)*y(t)**2)/(a*(c-a)))
x_z = sqrt(((b*C1-C2) - c*(b-c)*z(t)**2)/(a*(b-a)))
y_z = sqrt(((a*C1-C2) - c*(a-c)*z(t)**2)/(b*(a-b)))
sol1 = dsolve(a*diff(x(t),t) - (b-c)*y_x*z_x*r[f])
sol2 = dsolve(b*diff(y(t),t) - (c-a)*z_y*x_y*r[f])
sol3 = dsolve(c*diff(z(t),t) - (a-b)*x_z*y_z*r[f])
return [sol1, sol2, sol3]
def _nonlinear_3eq_order1_type3(x, y, z, t, eq):
r"""
Equations:
.. math:: x' = c F_2 - b F_3, \enspace y' = a F_3 - c F_1, \enspace z' = b F_1 - a F_2
where `F_n = F_n(x, y, z, t)`.
1. First Integral:
.. math:: a x + b y + c z = C_1,
where C is an arbitrary constant.
2. If we assume function `F_n` to be independent of `t`,i.e, `F_n` = `F_n (x, y, z)`
Then, on eliminating `t` and `z` from the first two equation of the system, one
arrives at the first-order equation
.. math:: \frac{dy}{dx} = \frac{a F_3 (x, y, z) - c F_1 (x, y, z)}{c F_2 (x, y, z) -
b F_3 (x, y, z)}
where `z = \frac{1}{c} (C_1 - a x - b y)`
References
==========
-http://eqworld.ipmnet.ru/en/solutions/sysode/sode0404.pdf
"""
C1 = get_numbered_constants(eq, num=1)
u, v, w = symbols('u, v, w')
p = Wild('p', exclude=[x(t), y(t), z(t), t])
q = Wild('q', exclude=[x(t), y(t), z(t), t])
s = Wild('s', exclude=[x(t), y(t), z(t), t])
F1, F2, F3 = symbols('F1, F2, F3', cls=Wild)
r1 = (diff(x(t), t) - eq[0]).match(F2-F3)
r = collect_const(r1[F2]).match(s*F2)
r.update(collect_const(r1[F3]).match(q*F3))
if eq[1].has(r[F2]) and not eq[1].has(r[F3]):
r[F2], r[F3] = r[F3], r[F2]
r[s], r[q] = -r[q], -r[s]
r.update((diff(y(t), t) - eq[1]).match(p*r[F3] - r[s]*F1))
a = r[p]; b = r[q]; c = r[s]
F1 = r[F1].subs(x(t), u).subs(y(t),v).subs(z(t), w)
F2 = r[F2].subs(x(t), u).subs(y(t),v).subs(z(t), w)
F3 = r[F3].subs(x(t), u).subs(y(t),v).subs(z(t), w)
z_xy = (C1-a*u-b*v)/c
y_zx = (C1-a*u-c*w)/b
x_yz = (C1-b*v-c*w)/a
y_x = dsolve(diff(v(u),u) - ((a*F3-c*F1)/(c*F2-b*F3)).subs(w,z_xy).subs(v,v(u))).rhs
z_x = dsolve(diff(w(u),u) - ((b*F1-a*F2)/(c*F2-b*F3)).subs(v,y_zx).subs(w,w(u))).rhs
z_y = dsolve(diff(w(v),v) - ((b*F1-a*F2)/(a*F3-c*F1)).subs(u,x_yz).subs(w,w(v))).rhs
x_y = dsolve(diff(u(v),v) - ((c*F2-b*F3)/(a*F3-c*F1)).subs(w,z_xy).subs(u,u(v))).rhs
y_z = dsolve(diff(v(w),w) - ((a*F3-c*F1)/(b*F1-a*F2)).subs(u,x_yz).subs(v,v(w))).rhs
x_z = dsolve(diff(u(w),w) - ((c*F2-b*F3)/(b*F1-a*F2)).subs(v,y_zx).subs(u,u(w))).rhs
sol1 = dsolve(diff(u(t),t) - (c*F2 - b*F3).subs(v,y_x).subs(w,z_x).subs(u,u(t))).rhs
sol2 = dsolve(diff(v(t),t) - (a*F3 - c*F1).subs(u,x_y).subs(w,z_y).subs(v,v(t))).rhs
sol3 = dsolve(diff(w(t),t) - (b*F1 - a*F2).subs(u,x_z).subs(v,y_z).subs(w,w(t))).rhs
return [sol1, sol2, sol3]
def _nonlinear_3eq_order1_type4(x, y, z, t, eq):
r"""
Equations:
.. math:: x' = c z F_2 - b y F_3, \enspace y' = a x F_3 - c z F_1, \enspace z' = b y F_1 - a x F_2
where `F_n = F_n (x, y, z, t)`
1. First integral:
.. math:: a x^{2} + b y^{2} + c z^{2} = C_1
where `C` is an arbitrary constant.
2. Assuming the function `F_n` is independent of `t`: `F_n = F_n (x, y, z)`. Then on
eliminating `t` and `z` from the first two equations of the system, one arrives at
the first-order equation
.. math:: \frac{dy}{dx} = \frac{a x F_3 (x, y, z) - c z F_1 (x, y, z)}
{c z F_2 (x, y, z) - b y F_3 (x, y, z)}
where `z = \pm \sqrt{\frac{1}{c} (C_1 - a x^{2} - b y^{2})}`
References
==========
-http://eqworld.ipmnet.ru/en/solutions/sysode/sode0405.pdf
"""
C1 = get_numbered_constants(eq, num=1)
u, v, w = symbols('u, v, w')
p = Wild('p', exclude=[x(t), y(t), z(t), t])
q = Wild('q', exclude=[x(t), y(t), z(t), t])
s = Wild('s', exclude=[x(t), y(t), z(t), t])
F1, F2, F3 = symbols('F1, F2, F3', cls=Wild)
r1 = eq[0].match(diff(x(t),t) - z(t)*F2 + y(t)*F3)
r = collect_const(r1[F2]).match(s*F2)
r.update(collect_const(r1[F3]).match(q*F3))
if eq[1].has(r[F2]) and not eq[1].has(r[F3]):
r[F2], r[F3] = r[F3], r[F2]
r[s], r[q] = -r[q], -r[s]
r.update((diff(y(t),t) - eq[1]).match(p*x(t)*r[F3] - r[s]*z(t)*F1))
a = r[p]; b = r[q]; c = r[s]
F1 = r[F1].subs(x(t),u).subs(y(t),v).subs(z(t),w)
F2 = r[F2].subs(x(t),u).subs(y(t),v).subs(z(t),w)
F3 = r[F3].subs(x(t),u).subs(y(t),v).subs(z(t),w)
x_yz = sqrt((C1 - b*v**2 - c*w**2)/a)
y_zx = sqrt((C1 - c*w**2 - a*u**2)/b)
z_xy = sqrt((C1 - a*u**2 - b*v**2)/c)
y_x = dsolve(diff(v(u),u) - ((a*u*F3-c*w*F1)/(c*w*F2-b*v*F3)).subs(w,z_xy).subs(v,v(u))).rhs
z_x = dsolve(diff(w(u),u) - ((b*v*F1-a*u*F2)/(c*w*F2-b*v*F3)).subs(v,y_zx).subs(w,w(u))).rhs
z_y = dsolve(diff(w(v),v) - ((b*v*F1-a*u*F2)/(a*u*F3-c*w*F1)).subs(u,x_yz).subs(w,w(v))).rhs
x_y = dsolve(diff(u(v),v) - ((c*w*F2-b*v*F3)/(a*u*F3-c*w*F1)).subs(w,z_xy).subs(u,u(v))).rhs
y_z = dsolve(diff(v(w),w) - ((a*u*F3-c*w*F1)/(b*v*F1-a*u*F2)).subs(u,x_yz).subs(v,v(w))).rhs
x_z = dsolve(diff(u(w),w) - ((c*w*F2-b*v*F3)/(b*v*F1-a*u*F2)).subs(v,y_zx).subs(u,u(w))).rhs
sol1 = dsolve(diff(u(t),t) - (c*w*F2 - b*v*F3).subs(v,y_x).subs(w,z_x).subs(u,u(t))).rhs
sol2 = dsolve(diff(v(t),t) - (a*u*F3 - c*w*F1).subs(u,x_y).subs(w,z_y).subs(v,v(t))).rhs
sol3 = dsolve(diff(w(t),t) - (b*v*F1 - a*u*F2).subs(u,x_z).subs(v,y_z).subs(w,w(t))).rhs
return [sol1, sol2, sol3]
def _nonlinear_3eq_order1_type5(x, y, z, t, eq):
r"""
.. math:: x' = x (c F_2 - b F_3), \enspace y' = y (a F_3 - c F_1), \enspace z' = z (b F_1 - a F_2)
where `F_n = F_n (x, y, z, t)` and are arbitrary functions.
First Integral:
.. math:: \left|x\right|^{a} \left|y\right|^{b} \left|z\right|^{c} = C_1
where `C` is an arbitrary constant. If the function `F_n` is independent of `t`,
then, by eliminating `t` and `z` from the first two equations of the system, one
arrives at a first-order equation.
References
==========
-http://eqworld.ipmnet.ru/en/solutions/sysode/sode0406.pdf
"""
C1 = get_numbered_constants(eq, num=1)
u, v, w = symbols('u, v, w')
p = Wild('p', exclude=[x(t), y(t), z(t), t])
q = Wild('q', exclude=[x(t), y(t), z(t), t])
s = Wild('s', exclude=[x(t), y(t), z(t), t])
F1, F2, F3 = symbols('F1, F2, F3', cls=Wild)
r1 = eq[0].match(diff(x(t), t) - x(t)*(F2 - F3))
r = collect_const(r1[F2]).match(s*F2)
r.update(collect_const(r1[F3]).match(q*F3))
if eq[1].has(r[F2]) and not eq[1].has(r[F3]):
r[F2], r[F3] = r[F3], r[F2]
r[s], r[q] = -r[q], -r[s]
r.update((diff(y(t), t) - eq[1]).match(y(t)*(p*r[F3] - r[s]*F1)))
a = r[p]; b = r[q]; c = r[s]
F1 = r[F1].subs(x(t), u).subs(y(t), v).subs(z(t), w)
F2 = r[F2].subs(x(t), u).subs(y(t), v).subs(z(t), w)
F3 = r[F3].subs(x(t), u).subs(y(t), v).subs(z(t), w)
x_yz = (C1*v**-b*w**-c)**-a
y_zx = (C1*w**-c*u**-a)**-b
z_xy = (C1*u**-a*v**-b)**-c
y_x = dsolve(diff(v(u), u) - ((v*(a*F3 - c*F1))/(u*(c*F2 - b*F3))).subs(w, z_xy).subs(v, v(u))).rhs
z_x = dsolve(diff(w(u), u) - ((w*(b*F1 - a*F2))/(u*(c*F2 - b*F3))).subs(v, y_zx).subs(w, w(u))).rhs
z_y = dsolve(diff(w(v), v) - ((w*(b*F1 - a*F2))/(v*(a*F3 - c*F1))).subs(u, x_yz).subs(w, w(v))).rhs
x_y = dsolve(diff(u(v), v) - ((u*(c*F2 - b*F3))/(v*(a*F3 - c*F1))).subs(w, z_xy).subs(u, u(v))).rhs
y_z = dsolve(diff(v(w), w) - ((v*(a*F3 - c*F1))/(w*(b*F1 - a*F2))).subs(u, x_yz).subs(v, v(w))).rhs
x_z = dsolve(diff(u(w), w) - ((u*(c*F2 - b*F3))/(w*(b*F1 - a*F2))).subs(v, y_zx).subs(u, u(w))).rhs
sol1 = dsolve(diff(u(t), t) - (u*(c*F2 - b*F3)).subs(v, y_x).subs(w, z_x).subs(u, u(t))).rhs
sol2 = dsolve(diff(v(t), t) - (v*(a*F3 - c*F1)).subs(u, x_y).subs(w, z_y).subs(v, v(t))).rhs
sol3 = dsolve(diff(w(t), t) - (w*(b*F1 - a*F2)).subs(u, x_z).subs(v, y_z).subs(w, w(t))).rhs
return [sol1, sol2, sol3]
|
acc820a040b28398a5536a59359b22b78f71e4161d322ba96233fcbbbbb86ec9 | r"""
This module is intended for solving recurrences or, in other words,
difference equations. Currently supported are linear, inhomogeneous
equations with polynomial or rational coefficients.
The solutions are obtained among polynomials, rational functions,
hypergeometric terms, or combinations of hypergeometric term which
are pairwise dissimilar.
``rsolve_X`` functions were meant as a low level interface
for ``rsolve`` which would use Mathematica's syntax.
Given a recurrence relation:
.. math:: a_{k}(n) y(n+k) + a_{k-1}(n) y(n+k-1) +
... + a_{0}(n) y(n) = f(n)
where `k > 0` and `a_{i}(n)` are polynomials in `n`. To use
``rsolve_X`` we need to put all coefficients in to a list ``L`` of
`k+1` elements the following way:
``L = [a_{0}(n), ..., a_{k-1}(n), a_{k}(n)]``
where ``L[i]``, for `i=0, \ldots, k`, maps to
`a_{i}(n) y(n+i)` (`y(n+i)` is implicit).
For example if we would like to compute `m`-th Bernoulli polynomial
up to a constant (example was taken from rsolve_poly docstring),
then we would use `b(n+1) - b(n) = m n^{m-1}` recurrence, which
has solution `b(n) = B_m + C`.
Then ``L = [-1, 1]`` and `f(n) = m n^(m-1)` and finally for `m=4`:
>>> from sympy import Symbol, bernoulli, rsolve_poly
>>> n = Symbol('n', integer=True)
>>> rsolve_poly([-1, 1], 4*n**3, n)
C0 + n**4 - 2*n**3 + n**2
>>> bernoulli(4, n)
n**4 - 2*n**3 + n**2 - 1/30
For the sake of completeness, `f(n)` can be:
[1] a polynomial -> rsolve_poly
[2] a rational function -> rsolve_ratio
[3] a hypergeometric function -> rsolve_hyper
"""
from __future__ import print_function, division
from collections import defaultdict
from sympy.core.singleton import S
from sympy.core.numbers import Rational, I
from sympy.core.symbol import Symbol, Wild, Dummy
from sympy.core.relational import Equality
from sympy.core.add import Add
from sympy.core.mul import Mul
from sympy.core import sympify
from sympy.simplify import simplify, hypersimp, hypersimilar
from sympy.solvers import solve, solve_undetermined_coeffs
from sympy.polys import Poly, quo, gcd, lcm, roots, resultant
from sympy.functions import binomial, factorial, FallingFactorial, RisingFactorial
from sympy.matrices import Matrix, casoratian
from sympy.concrete import product
from sympy.core.compatibility import default_sort_key, range
from sympy.utilities.iterables import numbered_symbols
def rsolve_poly(coeffs, f, n, **hints):
r"""
Given linear recurrence operator `\operatorname{L}` of order
`k` with polynomial coefficients and inhomogeneous equation
`\operatorname{L} y = f`, where `f` is a polynomial, we seek for
all polynomial solutions over field `K` of characteristic zero.
The algorithm performs two basic steps:
(1) Compute degree `N` of the general polynomial solution.
(2) Find all polynomials of degree `N` or less
of `\operatorname{L} y = f`.
There are two methods for computing the polynomial solutions.
If the degree bound is relatively small, i.e. it's smaller than
or equal to the order of the recurrence, then naive method of
undetermined coefficients is being used. This gives system
of algebraic equations with `N+1` unknowns.
In the other case, the algorithm performs transformation of the
initial equation to an equivalent one, for which the system of
algebraic equations has only `r` indeterminates. This method is
quite sophisticated (in comparison with the naive one) and was
invented together by Abramov, Bronstein and Petkovsek.
It is possible to generalize the algorithm implemented here to
the case of linear q-difference and differential equations.
Lets say that we would like to compute `m`-th Bernoulli polynomial
up to a constant. For this we can use `b(n+1) - b(n) = m n^{m-1}`
recurrence, which has solution `b(n) = B_m + C`. For example:
>>> from sympy import Symbol, rsolve_poly
>>> n = Symbol('n', integer=True)
>>> rsolve_poly([-1, 1], 4*n**3, n)
C0 + n**4 - 2*n**3 + n**2
References
==========
.. [1] S. A. Abramov, M. Bronstein and M. Petkovsek, On polynomial
solutions of linear operator equations, in: T. Levelt, ed.,
Proc. ISSAC '95, ACM Press, New York, 1995, 290-296.
.. [2] M. Petkovsek, Hypergeometric solutions of linear recurrences
with polynomial coefficients, J. Symbolic Computation,
14 (1992), 243-264.
.. [3] M. Petkovsek, H. S. Wilf, D. Zeilberger, A = B, 1996.
"""
f = sympify(f)
if not f.is_polynomial(n):
return None
homogeneous = f.is_zero
r = len(coeffs) - 1
coeffs = [Poly(coeff, n) for coeff in coeffs]
polys = [Poly(0, n)]*(r + 1)
terms = [(S.Zero, S.NegativeInfinity)]*(r + 1)
for i in range(r + 1):
for j in range(i, r + 1):
polys[i] += coeffs[j]*binomial(j, i)
if not polys[i].is_zero:
(exp,), coeff = polys[i].LT()
terms[i] = (coeff, exp)
d = b = terms[0][1]
for i in range(1, r + 1):
if terms[i][1] > d:
d = terms[i][1]
if terms[i][1] - i > b:
b = terms[i][1] - i
d, b = int(d), int(b)
x = Dummy('x')
degree_poly = S.Zero
for i in range(r + 1):
if terms[i][1] - i == b:
degree_poly += terms[i][0]*FallingFactorial(x, i)
nni_roots = list(roots(degree_poly, x, filter='Z',
predicate=lambda r: r >= 0).keys())
if nni_roots:
N = [max(nni_roots)]
else:
N = []
if homogeneous:
N += [-b - 1]
else:
N += [f.as_poly(n).degree() - b, -b - 1]
N = int(max(N))
if N < 0:
if homogeneous:
if hints.get('symbols', False):
return (S.Zero, [])
else:
return S.Zero
else:
return None
if N <= r:
C = []
y = E = S.Zero
for i in range(N + 1):
C.append(Symbol('C' + str(i)))
y += C[i] * n**i
for i in range(r + 1):
E += coeffs[i].as_expr()*y.subs(n, n + i)
solutions = solve_undetermined_coeffs(E - f, C, n)
if solutions is not None:
C = [c for c in C if (c not in solutions)]
result = y.subs(solutions)
else:
return None # TBD
else:
A = r
U = N + A + b + 1
nni_roots = list(roots(polys[r], filter='Z',
predicate=lambda r: r >= 0).keys())
if nni_roots != []:
a = max(nni_roots) + 1
else:
a = S.Zero
def _zero_vector(k):
return [S.Zero] * k
def _one_vector(k):
return [S.One] * k
def _delta(p, k):
B = S.One
D = p.subs(n, a + k)
for i in range(1, k + 1):
B *= Rational(i - k - 1, i)
D += B * p.subs(n, a + k - i)
return D
alpha = {}
for i in range(-A, d + 1):
I = _one_vector(d + 1)
for k in range(1, d + 1):
I[k] = I[k - 1] * (x + i - k + 1)/k
alpha[i] = S.Zero
for j in range(A + 1):
for k in range(d + 1):
B = binomial(k, i + j)
D = _delta(polys[j].as_expr(), k)
alpha[i] += I[k]*B*D
V = Matrix(U, A, lambda i, j: int(i == j))
if homogeneous:
for i in range(A, U):
v = _zero_vector(A)
for k in range(1, A + b + 1):
if i - k < 0:
break
B = alpha[k - A].subs(x, i - k)
for j in range(A):
v[j] += B * V[i - k, j]
denom = alpha[-A].subs(x, i)
for j in range(A):
V[i, j] = -v[j] / denom
else:
G = _zero_vector(U)
for i in range(A, U):
v = _zero_vector(A)
g = S.Zero
for k in range(1, A + b + 1):
if i - k < 0:
break
B = alpha[k - A].subs(x, i - k)
for j in range(A):
v[j] += B * V[i - k, j]
g += B * G[i - k]
denom = alpha[-A].subs(x, i)
for j in range(A):
V[i, j] = -v[j] / denom
G[i] = (_delta(f, i - A) - g) / denom
P, Q = _one_vector(U), _zero_vector(A)
for i in range(1, U):
P[i] = (P[i - 1] * (n - a - i + 1)/i).expand()
for i in range(A):
Q[i] = Add(*[(v*p).expand() for v, p in zip(V[:, i], P)])
if not homogeneous:
h = Add(*[(g*p).expand() for g, p in zip(G, P)])
C = [Symbol('C' + str(i)) for i in range(A)]
g = lambda i: Add(*[c*_delta(q, i) for c, q in zip(C, Q)])
if homogeneous:
E = [g(i) for i in range(N + 1, U)]
else:
E = [g(i) + _delta(h, i) for i in range(N + 1, U)]
if E != []:
solutions = solve(E, *C)
if not solutions:
if homogeneous:
if hints.get('symbols', False):
return (S.Zero, [])
else:
return S.Zero
else:
return None
else:
solutions = {}
if homogeneous:
result = S.Zero
else:
result = h
for c, q in list(zip(C, Q)):
if c in solutions:
s = solutions[c]*q
C.remove(c)
else:
s = c*q
result += s.expand()
if hints.get('symbols', False):
return (result, C)
else:
return result
def rsolve_ratio(coeffs, f, n, **hints):
r"""
Given linear recurrence operator `\operatorname{L}` of order `k`
with polynomial coefficients and inhomogeneous equation
`\operatorname{L} y = f`, where `f` is a polynomial, we seek
for all rational solutions over field `K` of characteristic zero.
This procedure accepts only polynomials, however if you are
interested in solving recurrence with rational coefficients
then use ``rsolve`` which will pre-process the given equation
and run this procedure with polynomial arguments.
The algorithm performs two basic steps:
(1) Compute polynomial `v(n)` which can be used as universal
denominator of any rational solution of equation
`\operatorname{L} y = f`.
(2) Construct new linear difference equation by substitution
`y(n) = u(n)/v(n)` and solve it for `u(n)` finding all its
polynomial solutions. Return ``None`` if none were found.
Algorithm implemented here is a revised version of the original
Abramov's algorithm, developed in 1989. The new approach is much
simpler to implement and has better overall efficiency. This
method can be easily adapted to q-difference equations case.
Besides finding rational solutions alone, this functions is
an important part of Hyper algorithm were it is used to find
particular solution of inhomogeneous part of a recurrence.
Examples
========
>>> from sympy.abc import x
>>> from sympy.solvers.recurr import rsolve_ratio
>>> rsolve_ratio([-2*x**3 + x**2 + 2*x - 1, 2*x**3 + x**2 - 6*x,
... - 2*x**3 - 11*x**2 - 18*x - 9, 2*x**3 + 13*x**2 + 22*x + 8], 0, x)
C2*(2*x - 3)/(2*(x**2 - 1))
References
==========
.. [1] S. A. Abramov, Rational solutions of linear difference
and q-difference equations with polynomial coefficients,
in: T. Levelt, ed., Proc. ISSAC '95, ACM Press, New York,
1995, 285-289
See Also
========
rsolve_hyper
"""
f = sympify(f)
if not f.is_polynomial(n):
return None
coeffs = list(map(sympify, coeffs))
r = len(coeffs) - 1
A, B = coeffs[r], coeffs[0]
A = A.subs(n, n - r).expand()
h = Dummy('h')
res = resultant(A, B.subs(n, n + h), n)
if not res.is_polynomial(h):
p, q = res.as_numer_denom()
res = quo(p, q, h)
nni_roots = list(roots(res, h, filter='Z',
predicate=lambda r: r >= 0).keys())
if not nni_roots:
return rsolve_poly(coeffs, f, n, **hints)
else:
C, numers = S.One, [S.Zero]*(r + 1)
for i in range(int(max(nni_roots)), -1, -1):
d = gcd(A, B.subs(n, n + i), n)
A = quo(A, d, n)
B = quo(B, d.subs(n, n - i), n)
C *= Mul(*[d.subs(n, n - j) for j in range(i + 1)])
denoms = [C.subs(n, n + i) for i in range(r + 1)]
for i in range(r + 1):
g = gcd(coeffs[i], denoms[i], n)
numers[i] = quo(coeffs[i], g, n)
denoms[i] = quo(denoms[i], g, n)
for i in range(r + 1):
numers[i] *= Mul(*(denoms[:i] + denoms[i + 1:]))
result = rsolve_poly(numers, f * Mul(*denoms), n, **hints)
if result is not None:
if hints.get('symbols', False):
return (simplify(result[0] / C), result[1])
else:
return simplify(result / C)
else:
return None
def rsolve_hyper(coeffs, f, n, **hints):
r"""
Given linear recurrence operator `\operatorname{L}` of order `k`
with polynomial coefficients and inhomogeneous equation
`\operatorname{L} y = f` we seek for all hypergeometric solutions
over field `K` of characteristic zero.
The inhomogeneous part can be either hypergeometric or a sum
of a fixed number of pairwise dissimilar hypergeometric terms.
The algorithm performs three basic steps:
(1) Group together similar hypergeometric terms in the
inhomogeneous part of `\operatorname{L} y = f`, and find
particular solution using Abramov's algorithm.
(2) Compute generating set of `\operatorname{L}` and find basis
in it, so that all solutions are linearly independent.
(3) Form final solution with the number of arbitrary
constants equal to dimension of basis of `\operatorname{L}`.
Term `a(n)` is hypergeometric if it is annihilated by first order
linear difference equations with polynomial coefficients or, in
simpler words, if consecutive term ratio is a rational function.
The output of this procedure is a linear combination of fixed
number of hypergeometric terms. However the underlying method
can generate larger class of solutions - D'Alembertian terms.
Note also that this method not only computes the kernel of the
inhomogeneous equation, but also reduces in to a basis so that
solutions generated by this procedure are linearly independent
Examples
========
>>> from sympy.solvers import rsolve_hyper
>>> from sympy.abc import x
>>> rsolve_hyper([-1, -1, 1], 0, x)
C0*(1/2 - sqrt(5)/2)**x + C1*(1/2 + sqrt(5)/2)**x
>>> rsolve_hyper([-1, 1], 1 + x, x)
C0 + x*(x + 1)/2
References
==========
.. [1] M. Petkovsek, Hypergeometric solutions of linear recurrences
with polynomial coefficients, J. Symbolic Computation,
14 (1992), 243-264.
.. [2] M. Petkovsek, H. S. Wilf, D. Zeilberger, A = B, 1996.
"""
coeffs = list(map(sympify, coeffs))
f = sympify(f)
r, kernel, symbols = len(coeffs) - 1, [], set()
if not f.is_zero:
if f.is_Add:
similar = {}
for g in f.expand().args:
if not g.is_hypergeometric(n):
return None
for h in similar.keys():
if hypersimilar(g, h, n):
similar[h] += g
break
else:
similar[g] = S.Zero
inhomogeneous = []
for g, h in similar.items():
inhomogeneous.append(g + h)
elif f.is_hypergeometric(n):
inhomogeneous = [f]
else:
return None
for i, g in enumerate(inhomogeneous):
coeff, polys = S.One, coeffs[:]
denoms = [S.One]*(r + 1)
s = hypersimp(g, n)
for j in range(1, r + 1):
coeff *= s.subs(n, n + j - 1)
p, q = coeff.as_numer_denom()
polys[j] *= p
denoms[j] = q
for j in range(r + 1):
polys[j] *= Mul(*(denoms[:j] + denoms[j + 1:]))
R = rsolve_poly(polys, Mul(*denoms), n)
if not (R is None or R is S.Zero):
inhomogeneous[i] *= R
else:
return None
result = Add(*inhomogeneous)
else:
result = S.Zero
Z = Dummy('Z')
p, q = coeffs[0], coeffs[r].subs(n, n - r + 1)
p_factors = [z for z in roots(p, n).keys()]
q_factors = [z for z in roots(q, n).keys()]
factors = [(S.One, S.One)]
for p in p_factors:
for q in q_factors:
if p.is_integer and q.is_integer and p <= q:
continue
else:
factors += [(n - p, n - q)]
p = [(n - p, S.One) for p in p_factors]
q = [(S.One, n - q) for q in q_factors]
factors = p + factors + q
for A, B in factors:
polys, degrees = [], []
D = A*B.subs(n, n + r - 1)
for i in range(r + 1):
a = Mul(*[A.subs(n, n + j) for j in range(i)])
b = Mul(*[B.subs(n, n + j) for j in range(i, r)])
poly = quo(coeffs[i]*a*b, D, n)
polys.append(poly.as_poly(n))
if not poly.is_zero:
degrees.append(polys[i].degree())
if degrees:
d, poly = max(degrees), S.Zero
else:
return None
for i in range(r + 1):
coeff = polys[i].nth(d)
if coeff is not S.Zero:
poly += coeff * Z**i
for z in roots(poly, Z).keys():
if z.is_zero:
continue
(C, s) = rsolve_poly([polys[i]*z**i for i in range(r + 1)], 0, n, symbols=True)
if C is not None and C is not S.Zero:
symbols |= set(s)
ratio = z * A * C.subs(n, n + 1) / B / C
ratio = simplify(ratio)
# If there is a nonnegative root in the denominator of the ratio,
# this indicates that the term y(n_root) is zero, and one should
# start the product with the term y(n_root + 1).
n0 = 0
for n_root in roots(ratio.as_numer_denom()[1], n).keys():
if n_root.has(I):
return None
elif (n0 < (n_root + 1)) == True:
n0 = n_root + 1
K = product(ratio, (n, n0, n - 1))
if K.has(factorial, FallingFactorial, RisingFactorial):
K = simplify(K)
if casoratian(kernel + [K], n, zero=False) != 0:
kernel.append(K)
kernel.sort(key=default_sort_key)
sk = list(zip(numbered_symbols('C'), kernel))
if sk:
for C, ker in sk:
result += C * ker
else:
return None
if hints.get('symbols', False):
symbols |= {s for s, k in sk}
return (result, list(symbols))
else:
return result
def rsolve(f, y, init=None):
r"""
Solve univariate recurrence with rational coefficients.
Given `k`-th order linear recurrence `\operatorname{L} y = f`,
or equivalently:
.. math:: a_{k}(n) y(n+k) + a_{k-1}(n) y(n+k-1) +
\cdots + a_{0}(n) y(n) = f(n)
where `a_{i}(n)`, for `i=0, \ldots, k`, are polynomials or rational
functions in `n`, and `f` is a hypergeometric function or a sum
of a fixed number of pairwise dissimilar hypergeometric terms in
`n`, finds all solutions or returns ``None``, if none were found.
Initial conditions can be given as a dictionary in two forms:
(1) ``{ n_0 : v_0, n_1 : v_1, ..., n_m : v_m}``
(2) ``{y(n_0) : v_0, y(n_1) : v_1, ..., y(n_m) : v_m}``
or as a list ``L`` of values:
``L = [v_0, v_1, ..., v_m]``
where ``L[i] = v_i``, for `i=0, \ldots, m`, maps to `y(n_i)`.
Examples
========
Lets consider the following recurrence:
.. math:: (n - 1) y(n + 2) - (n^2 + 3 n - 2) y(n + 1) +
2 n (n + 1) y(n) = 0
>>> from sympy import Function, rsolve
>>> from sympy.abc import n
>>> y = Function('y')
>>> f = (n - 1)*y(n + 2) - (n**2 + 3*n - 2)*y(n + 1) + 2*n*(n + 1)*y(n)
>>> rsolve(f, y(n))
2**n*C0 + C1*factorial(n)
>>> rsolve(f, y(n), {y(0):0, y(1):3})
3*2**n - 3*factorial(n)
See Also
========
rsolve_poly, rsolve_ratio, rsolve_hyper
"""
if isinstance(f, Equality):
f = f.lhs - f.rhs
n = y.args[0]
k = Wild('k', exclude=(n,))
# Preprocess user input to allow things like
# y(n) + a*(y(n + 1) + y(n - 1))/2
f = f.expand().collect(y.func(Wild('m', integer=True)))
h_part = defaultdict(lambda: S.Zero)
i_part = S.Zero
for g in Add.make_args(f):
coeff = S.One
kspec = None
for h in Mul.make_args(g):
if h.is_Function:
if h.func == y.func:
result = h.args[0].match(n + k)
if result is not None:
kspec = int(result[k])
else:
raise ValueError(
"'%s(%s + k)' expected, got '%s'" % (y.func, n, h))
else:
raise ValueError(
"'%s' expected, got '%s'" % (y.func, h.func))
else:
coeff *= h
if kspec is not None:
h_part[kspec] += coeff
else:
i_part += coeff
for k, coeff in h_part.items():
h_part[k] = simplify(coeff)
common = S.One
for coeff in h_part.values():
if coeff.is_rational_function(n):
if not coeff.is_polynomial(n):
common = lcm(common, coeff.as_numer_denom()[1], n)
else:
raise ValueError(
"Polynomial or rational function expected, got '%s'" % coeff)
i_numer, i_denom = i_part.as_numer_denom()
if i_denom.is_polynomial(n):
common = lcm(common, i_denom, n)
if common is not S.One:
for k, coeff in h_part.items():
numer, denom = coeff.as_numer_denom()
h_part[k] = numer*quo(common, denom, n)
i_part = i_numer*quo(common, i_denom, n)
K_min = min(h_part.keys())
if K_min < 0:
K = abs(K_min)
H_part = defaultdict(lambda: S.Zero)
i_part = i_part.subs(n, n + K).expand()
common = common.subs(n, n + K).expand()
for k, coeff in h_part.items():
H_part[k + K] = coeff.subs(n, n + K).expand()
else:
H_part = h_part
K_max = max(H_part.keys())
coeffs = [H_part[i] for i in range(K_max + 1)]
result = rsolve_hyper(coeffs, -i_part, n, symbols=True)
if result is None:
return None
solution, symbols = result
if init == {} or init == []:
init = None
if symbols and init is not None:
if isinstance(init, list):
init = {i: init[i] for i in range(len(init))}
equations = []
for k, v in init.items():
try:
i = int(k)
except TypeError:
if k.is_Function and k.func == y.func:
i = int(k.args[0])
else:
raise ValueError("Integer or term expected, got '%s'" % k)
try:
eq = solution.limit(n, i) - v
except NotImplementedError:
eq = solution.subs(n, i) - v
equations.append(eq)
result = solve(equations, *symbols)
if not result:
return None
else:
solution = solution.subs(result)
return solution
|
c85f8fa330f81a99f093d3f504c451bf3aa6370bb0e840b332bc08c3d24936d7 | """
This module contains functions to:
- solve a single equation for a single variable, in any domain either real or complex.
- solve a single transcendental equation for a single variable in any domain either real or complex.
(currently supports solving in real domain only)
- solve a system of linear equations with N variables and M equations.
- solve a system of Non Linear Equations with N variables and M equations
"""
from __future__ import print_function, division
from sympy.core.sympify import sympify
from sympy.core import (S, Pow, Dummy, pi, Expr, Wild, Mul, Equality,
Add)
from sympy.core.containers import Tuple
from sympy.core.facts import InconsistentAssumptions
from sympy.core.numbers import I, Number, Rational, oo
from sympy.core.function import (Lambda, expand_complex, AppliedUndef,
expand_log, _mexpand)
from sympy.core.mod import Mod
from sympy.core.numbers import igcd
from sympy.core.relational import Eq, Ne
from sympy.core.symbol import Symbol
from sympy.core.sympify import _sympify
from sympy.simplify.simplify import simplify, fraction, trigsimp
from sympy.simplify import powdenest, logcombine
from sympy.functions import (log, Abs, tan, cot, sin, cos, sec, csc, exp,
acos, asin, acsc, asec, arg,
piecewise_fold, Piecewise)
from sympy.functions.elementary.trigonometric import (TrigonometricFunction,
HyperbolicFunction)
from sympy.functions.elementary.miscellaneous import real_root
from sympy.logic.boolalg import And
from sympy.sets import (FiniteSet, EmptySet, imageset, Interval, Intersection,
Union, ConditionSet, ImageSet, Complement, Contains)
from sympy.sets.sets import Set
from sympy.matrices import Matrix, MatrixBase
from sympy.ntheory import totient
from sympy.ntheory.factor_ import divisors
from sympy.ntheory.residue_ntheory import discrete_log, nthroot_mod
from sympy.polys import (roots, Poly, degree, together, PolynomialError,
RootOf, factor)
from sympy.polys.polyerrors import CoercionFailed
from sympy.polys.polytools import invert
from sympy.solvers.solvers import (checksol, denoms, unrad,
_simple_dens, recast_to_symbols)
from sympy.solvers.polysys import solve_poly_system
from sympy.solvers.inequalities import solve_univariate_inequality
from sympy.utilities import filldedent
from sympy.utilities.iterables import numbered_symbols, has_dups
from sympy.calculus.util import periodicity, continuous_domain
from sympy.core.compatibility import ordered, default_sort_key, is_sequence
from types import GeneratorType
from collections import defaultdict
def _masked(f, *atoms):
"""Return ``f``, with all objects given by ``atoms`` replaced with
Dummy symbols, ``d``, and the list of replacements, ``(d, e)``,
where ``e`` is an object of type given by ``atoms`` in which
any other instances of atoms have been recursively replaced with
Dummy symbols, too. The tuples are ordered so that if they are
applied in sequence, the origin ``f`` will be restored.
Examples
========
>>> from sympy import cos
>>> from sympy.abc import x
>>> from sympy.solvers.solveset import _masked
>>> f = cos(cos(x) + 1)
>>> f, reps = _masked(cos(1 + cos(x)), cos)
>>> f
_a1
>>> reps
[(_a1, cos(_a0 + 1)), (_a0, cos(x))]
>>> for d, e in reps:
... f = f.xreplace({d: e})
>>> f
cos(cos(x) + 1)
"""
sym = numbered_symbols('a', cls=Dummy, real=True)
mask = []
for a in ordered(f.atoms(*atoms)):
for i in mask:
a = a.replace(*i)
mask.append((a, next(sym)))
for i, (o, n) in enumerate(mask):
f = f.replace(o, n)
mask[i] = (n, o)
mask = list(reversed(mask))
return f, mask
def _invert(f_x, y, x, domain=S.Complexes):
r"""
Reduce the complex valued equation ``f(x) = y`` to a set of equations
``{g(x) = h_1(y), g(x) = h_2(y), ..., g(x) = h_n(y) }`` where ``g(x)`` is
a simpler function than ``f(x)``. The return value is a tuple ``(g(x),
set_h)``, where ``g(x)`` is a function of ``x`` and ``set_h`` is
the set of function ``{h_1(y), h_2(y), ..., h_n(y)}``.
Here, ``y`` is not necessarily a symbol.
The ``set_h`` contains the functions, along with the information
about the domain in which they are valid, through set
operations. For instance, if ``y = Abs(x) - n`` is inverted
in the real domain, then ``set_h`` is not simply
`{-n, n}` as the nature of `n` is unknown; rather, it is:
`Intersection([0, oo) {n}) U Intersection((-oo, 0], {-n})`
By default, the complex domain is used which means that inverting even
seemingly simple functions like ``exp(x)`` will give very different
results from those obtained in the real domain.
(In the case of ``exp(x)``, the inversion via ``log`` is multi-valued
in the complex domain, having infinitely many branches.)
If you are working with real values only (or you are not sure which
function to use) you should probably set the domain to
``S.Reals`` (or use `invert\_real` which does that automatically).
Examples
========
>>> from sympy.solvers.solveset import invert_complex, invert_real
>>> from sympy.abc import x, y
>>> from sympy import exp, log
When does exp(x) == y?
>>> invert_complex(exp(x), y, x)
(x, ImageSet(Lambda(_n, I*(2*_n*pi + arg(y)) + log(Abs(y))), Integers))
>>> invert_real(exp(x), y, x)
(x, Intersection({log(y)}, Reals))
When does exp(x) == 1?
>>> invert_complex(exp(x), 1, x)
(x, ImageSet(Lambda(_n, 2*_n*I*pi), Integers))
>>> invert_real(exp(x), 1, x)
(x, {0})
See Also
========
invert_real, invert_complex
"""
x = sympify(x)
if not x.is_Symbol:
raise ValueError("x must be a symbol")
f_x = sympify(f_x)
if x not in f_x.free_symbols:
raise ValueError("Inverse of constant function doesn't exist")
y = sympify(y)
if x in y.free_symbols:
raise ValueError("y should be independent of x ")
if domain.is_subset(S.Reals):
x1, s = _invert_real(f_x, FiniteSet(y), x)
else:
x1, s = _invert_complex(f_x, FiniteSet(y), x)
if not isinstance(s, FiniteSet) or x1 != x:
return x1, s
return x1, s.intersection(domain)
invert_complex = _invert
def invert_real(f_x, y, x, domain=S.Reals):
"""
Inverts a real-valued function. Same as _invert, but sets
the domain to ``S.Reals`` before inverting.
"""
return _invert(f_x, y, x, domain)
def _invert_real(f, g_ys, symbol):
"""Helper function for _invert."""
if f == symbol:
return (f, g_ys)
n = Dummy('n', real=True)
if hasattr(f, 'inverse') and not isinstance(f, (
TrigonometricFunction,
HyperbolicFunction,
)):
if len(f.args) > 1:
raise ValueError("Only functions with one argument are supported.")
return _invert_real(f.args[0],
imageset(Lambda(n, f.inverse()(n)), g_ys),
symbol)
if isinstance(f, Abs):
return _invert_abs(f.args[0], g_ys, symbol)
if f.is_Add:
# f = g + h
g, h = f.as_independent(symbol)
if g is not S.Zero:
return _invert_real(h, imageset(Lambda(n, n - g), g_ys), symbol)
if f.is_Mul:
# f = g*h
g, h = f.as_independent(symbol)
if g is not S.One:
return _invert_real(h, imageset(Lambda(n, n/g), g_ys), symbol)
if f.is_Pow:
base, expo = f.args
base_has_sym = base.has(symbol)
expo_has_sym = expo.has(symbol)
if not expo_has_sym:
res = imageset(Lambda(n, real_root(n, expo)), g_ys)
if expo.is_rational:
numer, denom = expo.as_numer_denom()
if denom % 2 == 0:
base_positive = solveset(base >= 0, symbol, S.Reals)
res = imageset(Lambda(n, real_root(n, expo)
), g_ys.intersect(
Interval.Ropen(S.Zero, S.Infinity)))
_inv, _set = _invert_real(base, res, symbol)
return (_inv, _set.intersect(base_positive))
elif numer % 2 == 0:
n = Dummy('n')
neg_res = imageset(Lambda(n, -n), res)
return _invert_real(base, res + neg_res, symbol)
else:
return _invert_real(base, res, symbol)
else:
if not base.is_positive:
raise ValueError("x**w where w is irrational is not "
"defined for negative x")
return _invert_real(base, res, symbol)
if not base_has_sym:
rhs = g_ys.args[0]
if base.is_positive:
return _invert_real(expo,
imageset(Lambda(n, log(n, base, evaluate=False)), g_ys), symbol)
elif base.is_negative:
from sympy.core.power import integer_log
s, b = integer_log(rhs, base)
if b:
return _invert_real(expo, FiniteSet(s), symbol)
else:
return _invert_real(expo, S.EmptySet, symbol)
elif base.is_zero:
one = Eq(rhs, 1)
if one == S.true:
# special case: 0**x - 1
return _invert_real(expo, FiniteSet(0), symbol)
elif one == S.false:
return _invert_real(expo, S.EmptySet, symbol)
if isinstance(f, TrigonometricFunction):
if isinstance(g_ys, FiniteSet):
def inv(trig):
if isinstance(f, (sin, csc)):
F = asin if isinstance(f, sin) else acsc
return (lambda a: n*pi + (-1)**n*F(a),)
if isinstance(f, (cos, sec)):
F = acos if isinstance(f, cos) else asec
return (
lambda a: 2*n*pi + F(a),
lambda a: 2*n*pi - F(a),)
if isinstance(f, (tan, cot)):
return (lambda a: n*pi + f.inverse()(a),)
n = Dummy('n', integer=True)
invs = S.EmptySet
for L in inv(f):
invs += Union(*[imageset(Lambda(n, L(g)), S.Integers) for g in g_ys])
return _invert_real(f.args[0], invs, symbol)
return (f, g_ys)
def _invert_complex(f, g_ys, symbol):
"""Helper function for _invert."""
if f == symbol:
return (f, g_ys)
n = Dummy('n')
if f.is_Add:
# f = g + h
g, h = f.as_independent(symbol)
if g is not S.Zero:
return _invert_complex(h, imageset(Lambda(n, n - g), g_ys), symbol)
if f.is_Mul:
# f = g*h
g, h = f.as_independent(symbol)
if g is not S.One:
if g in set([S.NegativeInfinity, S.ComplexInfinity, S.Infinity]):
return (h, S.EmptySet)
return _invert_complex(h, imageset(Lambda(n, n/g), g_ys), symbol)
if hasattr(f, 'inverse') and \
not isinstance(f, TrigonometricFunction) and \
not isinstance(f, HyperbolicFunction) and \
not isinstance(f, exp):
if len(f.args) > 1:
raise ValueError("Only functions with one argument are supported.")
return _invert_complex(f.args[0],
imageset(Lambda(n, f.inverse()(n)), g_ys), symbol)
if isinstance(f, exp):
if isinstance(g_ys, FiniteSet):
exp_invs = Union(*[imageset(Lambda(n, I*(2*n*pi + arg(g_y)) +
log(Abs(g_y))), S.Integers)
for g_y in g_ys if g_y != 0])
return _invert_complex(f.args[0], exp_invs, symbol)
return (f, g_ys)
def _invert_abs(f, g_ys, symbol):
"""Helper function for inverting absolute value functions.
Returns the complete result of inverting an absolute value
function along with the conditions which must also be satisfied.
If it is certain that all these conditions are met, a `FiniteSet`
of all possible solutions is returned. If any condition cannot be
satisfied, an `EmptySet` is returned. Otherwise, a `ConditionSet`
of the solutions, with all the required conditions specified, is
returned.
"""
if not g_ys.is_FiniteSet:
# this could be used for FiniteSet, but the
# results are more compact if they aren't, e.g.
# ConditionSet(x, Contains(n, Interval(0, oo)), {-n, n}) vs
# Union(Intersection(Interval(0, oo), {n}), Intersection(Interval(-oo, 0), {-n}))
# for the solution of abs(x) - n
pos = Intersection(g_ys, Interval(0, S.Infinity))
parg = _invert_real(f, pos, symbol)
narg = _invert_real(-f, pos, symbol)
if parg[0] != narg[0]:
raise NotImplementedError
return parg[0], Union(narg[1], parg[1])
# check conditions: all these must be true. If any are unknown
# then return them as conditions which must be satisfied
unknown = []
for a in g_ys.args:
ok = a.is_nonnegative if a.is_Number else a.is_positive
if ok is None:
unknown.append(a)
elif not ok:
return symbol, S.EmptySet
if unknown:
conditions = And(*[Contains(i, Interval(0, oo))
for i in unknown])
else:
conditions = True
n = Dummy('n', real=True)
# this is slightly different than above: instead of solving
# +/-f on positive values, here we solve for f on +/- g_ys
g_x, values = _invert_real(f, Union(
imageset(Lambda(n, n), g_ys),
imageset(Lambda(n, -n), g_ys)), symbol)
return g_x, ConditionSet(g_x, conditions, values)
def domain_check(f, symbol, p):
"""Returns False if point p is infinite or any subexpression of f
is infinite or becomes so after replacing symbol with p. If none of
these conditions is met then True will be returned.
Examples
========
>>> from sympy import Mul, oo
>>> from sympy.abc import x
>>> from sympy.solvers.solveset import domain_check
>>> g = 1/(1 + (1/(x + 1))**2)
>>> domain_check(g, x, -1)
False
>>> domain_check(x**2, x, 0)
True
>>> domain_check(1/x, x, oo)
False
* The function relies on the assumption that the original form
of the equation has not been changed by automatic simplification.
>>> domain_check(x/x, x, 0) # x/x is automatically simplified to 1
True
* To deal with automatic evaluations use evaluate=False:
>>> domain_check(Mul(x, 1/x, evaluate=False), x, 0)
False
"""
f, p = sympify(f), sympify(p)
if p.is_infinite:
return False
return _domain_check(f, symbol, p)
def _domain_check(f, symbol, p):
# helper for domain check
if f.is_Atom and f.is_finite:
return True
elif f.subs(symbol, p).is_infinite:
return False
else:
return all([_domain_check(g, symbol, p)
for g in f.args])
def _is_finite_with_finite_vars(f, domain=S.Complexes):
"""
Return True if the given expression is finite. For symbols that
don't assign a value for `complex` and/or `real`, the domain will
be used to assign a value; symbols that don't assign a value
for `finite` will be made finite. All other assumptions are
left unmodified.
"""
def assumptions(s):
A = s.assumptions0
A.setdefault('finite', A.get('finite', True))
if domain.is_subset(S.Reals):
# if this gets set it will make complex=True, too
A.setdefault('real', True)
else:
# don't change 'real' because being complex implies
# nothing about being real
A.setdefault('complex', True)
return A
reps = {s: Dummy(**assumptions(s)) for s in f.free_symbols}
return f.xreplace(reps).is_finite
def _is_function_class_equation(func_class, f, symbol):
""" Tests whether the equation is an equation of the given function class.
The given equation belongs to the given function class if it is
comprised of functions of the function class which are multiplied by
or added to expressions independent of the symbol. In addition, the
arguments of all such functions must be linear in the symbol as well.
Examples
========
>>> from sympy.solvers.solveset import _is_function_class_equation
>>> from sympy import tan, sin, tanh, sinh, exp
>>> from sympy.abc import x
>>> from sympy.functions.elementary.trigonometric import (TrigonometricFunction,
... HyperbolicFunction)
>>> _is_function_class_equation(TrigonometricFunction, exp(x) + tan(x), x)
False
>>> _is_function_class_equation(TrigonometricFunction, tan(x) + sin(x), x)
True
>>> _is_function_class_equation(TrigonometricFunction, tan(x**2), x)
False
>>> _is_function_class_equation(TrigonometricFunction, tan(x + 2), x)
True
>>> _is_function_class_equation(HyperbolicFunction, tanh(x) + sinh(x), x)
True
"""
if f.is_Mul or f.is_Add:
return all(_is_function_class_equation(func_class, arg, symbol)
for arg in f.args)
if f.is_Pow:
if not f.exp.has(symbol):
return _is_function_class_equation(func_class, f.base, symbol)
else:
return False
if not f.has(symbol):
return True
if isinstance(f, func_class):
try:
g = Poly(f.args[0], symbol)
return g.degree() <= 1
except PolynomialError:
return False
else:
return False
def _solve_as_rational(f, symbol, domain):
""" solve rational functions"""
f = together(f, deep=True)
g, h = fraction(f)
if not h.has(symbol):
try:
return _solve_as_poly(g, symbol, domain)
except NotImplementedError:
# The polynomial formed from g could end up having
# coefficients in a ring over which finding roots
# isn't implemented yet, e.g. ZZ[a] for some symbol a
return ConditionSet(symbol, Eq(f, 0), domain)
except CoercionFailed:
# contained oo, zoo or nan
return S.EmptySet
else:
valid_solns = _solveset(g, symbol, domain)
invalid_solns = _solveset(h, symbol, domain)
return valid_solns - invalid_solns
def _solve_trig(f, symbol, domain):
"""Function to call other helpers to solve trigonometric equations """
sol1 = sol = None
try:
sol1 = _solve_trig1(f, symbol, domain)
except BaseException:
pass
if sol1 is None or isinstance(sol1, ConditionSet):
try:
sol = _solve_trig2(f, symbol, domain)
except BaseException:
sol = sol1
if isinstance(sol1, ConditionSet) and isinstance(sol, ConditionSet):
if sol1.count_ops() < sol.count_ops():
sol = sol1
else:
sol = sol1
if sol is None:
raise NotImplementedError(filldedent('''
Solution to this kind of trigonometric equations
is yet to be implemented'''))
return sol
def _solve_trig1(f, symbol, domain):
"""Primary Helper to solve trigonometric equations """
f = trigsimp(f)
f_original = f
f = f.rewrite(exp)
f = together(f)
g, h = fraction(f)
y = Dummy('y')
g, h = g.expand(), h.expand()
g, h = g.subs(exp(I*symbol), y), h.subs(exp(I*symbol), y)
if g.has(symbol) or h.has(symbol):
return ConditionSet(symbol, Eq(f, 0), S.Reals)
solns = solveset_complex(g, y) - solveset_complex(h, y)
if isinstance(solns, ConditionSet):
raise NotImplementedError
if isinstance(solns, FiniteSet):
if any(isinstance(s, RootOf) for s in solns):
raise NotImplementedError
result = Union(*[invert_complex(exp(I*symbol), s, symbol)[1]
for s in solns])
return Intersection(result, domain)
elif solns is S.EmptySet:
return S.EmptySet
else:
return ConditionSet(symbol, Eq(f_original, 0), S.Reals)
def _solve_trig2(f, symbol, domain):
"""Secondary helper to solve trigonometric equations,
called when first helper fails """
from sympy import ilcm, expand_trig, degree
f = trigsimp(f)
f_original = f
trig_functions = f.atoms(sin, cos, tan, sec, cot, csc)
trig_arguments = [e.args[0] for e in trig_functions]
denominators = []
numerators = []
for ar in trig_arguments:
try:
poly_ar = Poly(ar, symbol)
except ValueError:
raise ValueError("give up, we can't solve if this is not a polynomial in x")
if poly_ar.degree() > 1: # degree >1 still bad
raise ValueError("degree of variable inside polynomial should not exceed one")
if poly_ar.degree() == 0: # degree 0, don't care
continue
c = poly_ar.all_coeffs()[0] # got the coefficient of 'symbol'
numerators.append(Rational(c).p)
denominators.append(Rational(c).q)
x = Dummy('x')
# ilcm() and igcd() require more than one argument
if len(numerators) > 1:
mu = Rational(2)*ilcm(*denominators)/igcd(*numerators)
else:
assert len(numerators) == 1
mu = Rational(2)*denominators[0]/numerators[0]
f = f.subs(symbol, mu*x)
f = f.rewrite(tan)
f = expand_trig(f)
f = together(f)
g, h = fraction(f)
y = Dummy('y')
g, h = g.expand(), h.expand()
g, h = g.subs(tan(x), y), h.subs(tan(x), y)
if g.has(x) or h.has(x):
return ConditionSet(symbol, Eq(f_original, 0), domain)
solns = solveset(g, y, S.Reals) - solveset(h, y, S.Reals)
if isinstance(solns, FiniteSet):
result = Union(*[invert_real(tan(symbol/mu), s, symbol)[1]
for s in solns])
dsol = invert_real(tan(symbol/mu), oo, symbol)[1]
if degree(h) > degree(g): # If degree(denom)>degree(num) then there
result = Union(result, dsol) # would be another sol at Lim(denom-->oo)
return Intersection(result, domain)
elif solns is S.EmptySet:
return S.EmptySet
else:
return ConditionSet(symbol, Eq(f_original, 0), S.Reals)
def _solve_as_poly(f, symbol, domain=S.Complexes):
"""
Solve the equation using polynomial techniques if it already is a
polynomial equation or, with a change of variables, can be made so.
"""
result = None
if f.is_polynomial(symbol):
solns = roots(f, symbol, cubics=True, quartics=True,
quintics=True, domain='EX')
num_roots = sum(solns.values())
if degree(f, symbol) <= num_roots:
result = FiniteSet(*solns.keys())
else:
poly = Poly(f, symbol)
solns = poly.all_roots()
if poly.degree() <= len(solns):
result = FiniteSet(*solns)
else:
result = ConditionSet(symbol, Eq(f, 0), domain)
else:
poly = Poly(f)
if poly is None:
result = ConditionSet(symbol, Eq(f, 0), domain)
gens = [g for g in poly.gens if g.has(symbol)]
if len(gens) == 1:
poly = Poly(poly, gens[0])
gen = poly.gen
deg = poly.degree()
poly = Poly(poly.as_expr(), poly.gen, composite=True)
poly_solns = FiniteSet(*roots(poly, cubics=True, quartics=True,
quintics=True).keys())
if len(poly_solns) < deg:
result = ConditionSet(symbol, Eq(f, 0), domain)
if gen != symbol:
y = Dummy('y')
inverter = invert_real if domain.is_subset(S.Reals) else invert_complex
lhs, rhs_s = inverter(gen, y, symbol)
if lhs == symbol:
result = Union(*[rhs_s.subs(y, s) for s in poly_solns])
else:
result = ConditionSet(symbol, Eq(f, 0), domain)
else:
result = ConditionSet(symbol, Eq(f, 0), domain)
if result is not None:
if isinstance(result, FiniteSet):
# this is to simplify solutions like -sqrt(-I) to sqrt(2)/2
# - sqrt(2)*I/2. We are not expanding for solution with symbols
# or undefined functions because that makes the solution more complicated.
# For example, expand_complex(a) returns re(a) + I*im(a)
if all([s.atoms(Symbol, AppliedUndef) == set() and not isinstance(s, RootOf)
for s in result]):
s = Dummy('s')
result = imageset(Lambda(s, expand_complex(s)), result)
if isinstance(result, FiniteSet):
result = result.intersection(domain)
return result
else:
return ConditionSet(symbol, Eq(f, 0), domain)
def _has_rational_power(expr, symbol):
"""
Returns (bool, den) where bool is True if the term has a
non-integer rational power and den is the denominator of the
expression's exponent.
Examples
========
>>> from sympy.solvers.solveset import _has_rational_power
>>> from sympy import sqrt
>>> from sympy.abc import x
>>> _has_rational_power(sqrt(x), x)
(True, 2)
>>> _has_rational_power(x**2, x)
(False, 1)
"""
a, p, q = Wild('a'), Wild('p'), Wild('q')
pattern_match = expr.match(a*p**q) or {}
if pattern_match.get(a, S.Zero).is_zero:
return (False, S.One)
elif p not in pattern_match.keys():
return (False, S.One)
elif isinstance(pattern_match[q], Rational) \
and pattern_match[p].has(symbol):
if not pattern_match[q].q == S.One:
return (True, pattern_match[q].q)
if not isinstance(pattern_match[a], Pow) \
or isinstance(pattern_match[a], Mul):
return (False, S.One)
else:
return _has_rational_power(pattern_match[a], symbol)
def _solve_radical(f, symbol, solveset_solver):
""" Helper function to solve equations with radicals """
eq, cov = unrad(f)
if not cov:
result = solveset_solver(eq, symbol) - \
Union(*[solveset_solver(g, symbol) for g in denoms(f, symbol)])
else:
y, yeq = cov
if not solveset_solver(y - I, y):
yreal = Dummy('yreal', real=True)
yeq = yeq.xreplace({y: yreal})
eq = eq.xreplace({y: yreal})
y = yreal
g_y_s = solveset_solver(yeq, symbol)
f_y_sols = solveset_solver(eq, y)
result = Union(*[imageset(Lambda(y, g_y), f_y_sols)
for g_y in g_y_s])
if isinstance(result, Complement) or isinstance(result,ConditionSet):
solution_set = result
else:
f_set = [] # solutions for FiniteSet
c_set = [] # solutions for ConditionSet
for s in result:
if checksol(f, symbol, s):
f_set.append(s)
else:
c_set.append(s)
solution_set = FiniteSet(*f_set) + ConditionSet(symbol, Eq(f, 0), FiniteSet(*c_set))
return solution_set
def _solve_abs(f, symbol, domain):
""" Helper function to solve equation involving absolute value function """
if not domain.is_subset(S.Reals):
raise ValueError(filldedent('''
Absolute values cannot be inverted in the
complex domain.'''))
p, q, r = Wild('p'), Wild('q'), Wild('r')
pattern_match = f.match(p*Abs(q) + r) or {}
f_p, f_q, f_r = [pattern_match.get(i, S.Zero) for i in (p, q, r)]
if not (f_p.is_zero or f_q.is_zero):
domain = continuous_domain(f_q, symbol, domain)
q_pos_cond = solve_univariate_inequality(f_q >= 0, symbol,
relational=False, domain=domain, continuous=True)
q_neg_cond = q_pos_cond.complement(domain)
sols_q_pos = solveset_real(f_p*f_q + f_r,
symbol).intersect(q_pos_cond)
sols_q_neg = solveset_real(f_p*(-f_q) + f_r,
symbol).intersect(q_neg_cond)
return Union(sols_q_pos, sols_q_neg)
else:
return ConditionSet(symbol, Eq(f, 0), domain)
def solve_decomposition(f, symbol, domain):
"""
Function to solve equations via the principle of "Decomposition
and Rewriting".
Examples
========
>>> from sympy import exp, sin, Symbol, pprint, S
>>> from sympy.solvers.solveset import solve_decomposition as sd
>>> x = Symbol('x')
>>> f1 = exp(2*x) - 3*exp(x) + 2
>>> sd(f1, x, S.Reals)
{0, log(2)}
>>> f2 = sin(x)**2 + 2*sin(x) + 1
>>> pprint(sd(f2, x, S.Reals), use_unicode=False)
3*pi
{2*n*pi + ---- | n in Integers}
2
>>> f3 = sin(x + 2)
>>> pprint(sd(f3, x, S.Reals), use_unicode=False)
{2*n*pi - 2 | n in Integers} U {2*n*pi - 2 + pi | n in Integers}
"""
from sympy.solvers.decompogen import decompogen
from sympy.calculus.util import function_range
# decompose the given function
g_s = decompogen(f, symbol)
# `y_s` represents the set of values for which the function `g` is to be
# solved.
# `solutions` represent the solutions of the equations `g = y_s` or
# `g = 0` depending on the type of `y_s`.
# As we are interested in solving the equation: f = 0
y_s = FiniteSet(0)
for g in g_s:
frange = function_range(g, symbol, domain)
y_s = Intersection(frange, y_s)
result = S.EmptySet
if isinstance(y_s, FiniteSet):
for y in y_s:
solutions = solveset(Eq(g, y), symbol, domain)
if not isinstance(solutions, ConditionSet):
result += solutions
else:
if isinstance(y_s, ImageSet):
iter_iset = (y_s,)
elif isinstance(y_s, Union):
iter_iset = y_s.args
elif isinstance(y_s, EmptySet):
# y_s is not in the range of g in g_s, so no solution exists
#in the given domain
return y_s
for iset in iter_iset:
new_solutions = solveset(Eq(iset.lamda.expr, g), symbol, domain)
dummy_var = tuple(iset.lamda.expr.free_symbols)[0]
base_set = iset.base_set
if isinstance(new_solutions, FiniteSet):
new_exprs = new_solutions
elif isinstance(new_solutions, Intersection):
if isinstance(new_solutions.args[1], FiniteSet):
new_exprs = new_solutions.args[1]
for new_expr in new_exprs:
result += ImageSet(Lambda(dummy_var, new_expr), base_set)
if result is S.EmptySet:
return ConditionSet(symbol, Eq(f, 0), domain)
y_s = result
return y_s
def _solveset(f, symbol, domain, _check=False):
"""Helper for solveset to return a result from an expression
that has already been sympify'ed and is known to contain the
given symbol."""
# _check controls whether the answer is checked or not
from sympy.simplify.simplify import signsimp
orig_f = f
if f.is_Mul:
coeff, f = f.as_independent(symbol, as_Add=False)
if coeff in set([S.ComplexInfinity, S.NegativeInfinity, S.Infinity]):
f = together(orig_f)
elif f.is_Add:
a, h = f.as_independent(symbol)
m, h = h.as_independent(symbol, as_Add=False)
if m not in set([S.ComplexInfinity, S.Zero, S.Infinity,
S.NegativeInfinity]):
f = a/m + h # XXX condition `m != 0` should be added to soln
# assign the solvers to use
solver = lambda f, x, domain=domain: _solveset(f, x, domain)
inverter = lambda f, rhs, symbol: _invert(f, rhs, symbol, domain)
result = EmptySet()
if f.expand().is_zero:
return domain
elif not f.has(symbol):
return EmptySet()
elif f.is_Mul and all(_is_finite_with_finite_vars(m, domain)
for m in f.args):
# if f(x) and g(x) are both finite we can say that the solution of
# f(x)*g(x) == 0 is same as Union(f(x) == 0, g(x) == 0) is not true in
# general. g(x) can grow to infinitely large for the values where
# f(x) == 0. To be sure that we are not silently allowing any
# wrong solutions we are using this technique only if both f and g are
# finite for a finite input.
result = Union(*[solver(m, symbol) for m in f.args])
elif _is_function_class_equation(TrigonometricFunction, f, symbol) or \
_is_function_class_equation(HyperbolicFunction, f, symbol):
result = _solve_trig(f, symbol, domain)
elif isinstance(f, arg):
a = f.args[0]
result = solveset_real(a > 0, symbol)
elif f.is_Piecewise:
result = EmptySet()
expr_set_pairs = f.as_expr_set_pairs(domain)
for (expr, in_set) in expr_set_pairs:
if in_set.is_Relational:
in_set = in_set.as_set()
solns = solver(expr, symbol, in_set)
result += solns
elif isinstance(f, Eq):
result = solver(Add(f.lhs, - f.rhs, evaluate=False), symbol, domain)
elif f.is_Relational:
if not domain.is_subset(S.Reals):
raise NotImplementedError(filldedent('''
Inequalities in the complex domain are
not supported. Try the real domain by
setting domain=S.Reals'''))
try:
result = solve_univariate_inequality(
f, symbol, domain=domain, relational=False)
except NotImplementedError:
result = ConditionSet(symbol, f, domain)
return result
elif _is_modular(f, symbol):
result = _solve_modular(f, symbol, domain)
else:
lhs, rhs_s = inverter(f, 0, symbol)
if lhs == symbol:
# do some very minimal simplification since
# repeated inversion may have left the result
# in a state that other solvers (e.g. poly)
# would have simplified; this is done here
# rather than in the inverter since here it
# is only done once whereas there it would
# be repeated for each step of the inversion
if isinstance(rhs_s, FiniteSet):
rhs_s = FiniteSet(*[Mul(*
signsimp(i).as_content_primitive())
for i in rhs_s])
result = rhs_s
elif isinstance(rhs_s, FiniteSet):
for equation in [lhs - rhs for rhs in rhs_s]:
if equation == f:
if any(_has_rational_power(g, symbol)[0]
for g in equation.args) or _has_rational_power(
equation, symbol)[0]:
result += _solve_radical(equation,
symbol,
solver)
elif equation.has(Abs):
result += _solve_abs(f, symbol, domain)
else:
result_rational = _solve_as_rational(equation, symbol, domain)
if isinstance(result_rational, ConditionSet):
# may be a transcendental type equation
result += _transolve(equation, symbol, domain)
else:
result += result_rational
else:
result += solver(equation, symbol)
elif rhs_s is not S.EmptySet:
result = ConditionSet(symbol, Eq(f, 0), domain)
if isinstance(result, ConditionSet):
num, den = f.as_numer_denom()
if den.has(symbol):
_result = _solveset(num, symbol, domain)
if not isinstance(_result, ConditionSet):
singularities = _solveset(den, symbol, domain)
result = _result - singularities
if _check:
if isinstance(result, ConditionSet):
# it wasn't solved or has enumerated all conditions
# -- leave it alone
return result
# whittle away all but the symbol-containing core
# to use this for testing
fx = orig_f.as_independent(symbol, as_Add=True)[1]
fx = fx.as_independent(symbol, as_Add=False)[1]
if isinstance(result, FiniteSet):
# check the result for invalid solutions
result = FiniteSet(*[s for s in result
if isinstance(s, RootOf)
or domain_check(fx, symbol, s)])
return result
def _is_modular(f, symbol):
"""
Helper function to check below mentioned types of modular equations.
``A - Mod(B, C) = 0``
A -> This can or cannot be a function of symbol.
B -> This is surely a function of symbol.
C -> It is an integer.
Parameters
==========
f : Expr
The equation to be checked.
symbol : Symbol
The concerned variable for which the equation is to be checked.
Examples
========
>>> from sympy import symbols, exp, Mod
>>> from sympy.solvers.solveset import _is_modular as check
>>> x, y = symbols('x y')
>>> check(Mod(x, 3) - 1, x)
True
>>> check(Mod(x, 3) - 1, y)
False
>>> check(Mod(x, 3)**2 - 5, x)
False
>>> check(Mod(x, 3)**2 - y, x)
False
>>> check(exp(Mod(x, 3)) - 1, x)
False
>>> check(Mod(3, y) - 1, y)
False
"""
if not f.has(Mod):
return False
# extract modterms from f.
modterms = list(f.atoms(Mod))
return (len(modterms) == 1 and # only one Mod should be present
modterms[0].args[0].has(symbol) and # B-> function of symbol
modterms[0].args[1].is_integer and # C-> to be an integer.
any(isinstance(term, Mod)
for term in list(_term_factors(f))) # free from other funcs
)
def _invert_modular(modterm, rhs, n, symbol):
"""
Helper function to invert modular equation.
``Mod(a, m) - rhs = 0``
Generally it is inverted as (a, ImageSet(Lambda(n, m*n + rhs), S.Integers)).
More simplified form will be returned if possible.
If it is not invertible then (modterm, rhs) is returned.
The following cases arise while inverting equation ``Mod(a, m) - rhs = 0``:
1. If a is symbol then m*n + rhs is the required solution.
2. If a is an instance of ``Add`` then we try to find two symbol independent
parts of a and the symbol independent part gets tranferred to the other
side and again the ``_invert_modular`` is called on the symbol
dependent part.
3. If a is an instance of ``Mul`` then same as we done in ``Add`` we separate
out the symbol dependent and symbol independent parts and transfer the
symbol independent part to the rhs with the help of invert and again the
``_invert_modular`` is called on the symbol dependent part.
4. If a is an instance of ``Pow`` then two cases arise as following:
- If a is of type (symbol_indep)**(symbol_dep) then the remainder is
evaluated with the help of discrete_log function and then the least
period is being found out with the help of totient function.
period*n + remainder is the required solution in this case.
For reference: (https://en.wikipedia.org/wiki/Euler's_theorem)
- If a is of type (symbol_dep)**(symbol_indep) then we try to find all
primitive solutions list with the help of nthroot_mod function.
m*n + rem is the general solution where rem belongs to solutions list
from nthroot_mod function.
Parameters
==========
modterm, rhs : Expr
The modular equation to be inverted, ``modterm - rhs = 0``
symbol : Symbol
The variable in the equation to be inverted.
n : Dummy
Dummy variable for output g_n.
Returns
=======
A tuple (f_x, g_n) is being returned where f_x is modular independent function
of symbol and g_n being set of values f_x can have.
Examples
========
>>> from sympy import symbols, exp, Mod, Dummy, S
>>> from sympy.solvers.solveset import _invert_modular as invert_modular
>>> x, y = symbols('x y')
>>> n = Dummy('n')
>>> invert_modular(Mod(exp(x), 7), S(5), n, x)
(Mod(exp(x), 7), 5)
>>> invert_modular(Mod(x, 7), S(5), n, x)
(x, ImageSet(Lambda(_n, 7*_n + 5), Integers))
>>> invert_modular(Mod(3*x + 8, 7), S(5), n, x)
(x, ImageSet(Lambda(_n, 7*_n + 6), Integers))
>>> invert_modular(Mod(x**4, 7), S(5), n, x)
(x, EmptySet())
>>> invert_modular(Mod(2**(x**2 + x + 1), 7), S(2), n, x)
(x**2 + x + 1, ImageSet(Lambda(_n, 3*_n + 1), Naturals0))
"""
a, m = modterm.args
if rhs.is_real is False or any(term.is_real is False
for term in list(_term_factors(a))):
# Check for complex arguments
return modterm, rhs
if abs(rhs) >= abs(m):
# if rhs has value greater than value of m.
return symbol, EmptySet()
if a is symbol:
return symbol, ImageSet(Lambda(n, m*n + rhs), S.Integers)
if a.is_Add:
# g + h = a
g, h = a.as_independent(symbol)
if g is not S.Zero:
x_indep_term = rhs - Mod(g, m)
return _invert_modular(Mod(h, m), Mod(x_indep_term, m), n, symbol)
if a.is_Mul:
# g*h = a
g, h = a.as_independent(symbol)
if g is not S.One:
x_indep_term = rhs*invert(g, m)
return _invert_modular(Mod(h, m), Mod(x_indep_term, m), n, symbol)
if a.is_Pow:
# base**expo = a
base, expo = a.args
if expo.has(symbol) and not base.has(symbol):
# remainder -> solution independent of n of equation.
# m, rhs are made coprime by dividing igcd(m, rhs)
try:
remainder = discrete_log(m / igcd(m, rhs), rhs, a.base)
except ValueError: # log does not exist
return modterm, rhs
# period -> coefficient of n in the solution and also referred as
# the least period of expo in which it is repeats itself.
# (a**(totient(m)) - 1) divides m. Here is link of theorem:
# (https://en.wikipedia.org/wiki/Euler's_theorem)
period = totient(m)
for p in divisors(period):
# there might a lesser period exist than totient(m).
if pow(a.base, p, m / igcd(m, a.base)) == 1:
period = p
break
# recursion is not applied here since _invert_modular is currently
# not smart enough to handle infinite rhs as here expo has infinite
# rhs = ImageSet(Lambda(n, period*n + remainder), S.Naturals0).
return expo, ImageSet(Lambda(n, period*n + remainder), S.Naturals0)
elif base.has(symbol) and not expo.has(symbol):
try:
remainder_list = nthroot_mod(rhs, expo, m, all_roots=True)
if remainder_list is None:
return symbol, EmptySet()
except (ValueError, NotImplementedError):
return modterm, rhs
g_n = EmptySet()
for rem in remainder_list:
g_n += ImageSet(Lambda(n, m*n + rem), S.Integers)
return base, g_n
return modterm, rhs
def _solve_modular(f, symbol, domain):
r"""
Helper function for solving modular equations of type ``A - Mod(B, C) = 0``,
where A can or cannot be a function of symbol, B is surely a function of
symbol and C is an integer.
Currently ``_solve_modular`` is only able to solve cases
where A is not a function of symbol.
Parameters
==========
f : Expr
The modular equation to be solved, ``f = 0``
symbol : Symbol
The variable in the equation to be solved.
domain : Set
A set over which the equation is solved. It has to be a subset of
Integers.
Returns
=======
A set of integer solutions satisfying the given modular equation.
A ``ConditionSet`` if the equation is unsolvable.
Examples
========
>>> from sympy.solvers.solveset import _solve_modular as solve_modulo
>>> from sympy import S, Symbol, sin, Intersection, Range, Interval
>>> from sympy.core.mod import Mod
>>> x = Symbol('x')
>>> solve_modulo(Mod(5*x - 8, 7) - 3, x, S.Integers)
ImageSet(Lambda(_n, 7*_n + 5), Integers)
>>> solve_modulo(Mod(5*x - 8, 7) - 3, x, S.Reals) # domain should be subset of integers.
ConditionSet(x, Eq(Mod(5*x + 6, 7) - 3, 0), Reals)
>>> solve_modulo(-7 + Mod(x, 5), x, S.Integers)
EmptySet()
>>> solve_modulo(Mod(12**x, 21) - 18, x, S.Integers)
ImageSet(Lambda(_n, 6*_n + 2), Naturals0)
>>> solve_modulo(Mod(sin(x), 7) - 3, x, S.Integers) # not solvable
ConditionSet(x, Eq(Mod(sin(x), 7) - 3, 0), Integers)
>>> solve_modulo(3 - Mod(x, 5), x, Intersection(S.Integers, Interval(0, 100)))
Intersection(ImageSet(Lambda(_n, 5*_n + 3), Integers), Range(0, 101, 1))
"""
# extract modterm and g_y from f
unsolved_result = ConditionSet(symbol, Eq(f, 0), domain)
modterm = list(f.atoms(Mod))[0]
rhs = -S.One*(f.subs(modterm, S.Zero))
if f.as_coefficients_dict()[modterm].is_negative:
# checks if coefficient of modterm is negative in main equation.
rhs *= -S.One
if not domain.is_subset(S.Integers):
return unsolved_result
if rhs.has(symbol):
# TODO Case: A-> function of symbol, can be extended here
# in future.
return unsolved_result
n = Dummy('n', integer=True)
f_x, g_n = _invert_modular(modterm, rhs, n, symbol)
if f_x is modterm and g_n is rhs:
return unsolved_result
if f_x is symbol:
if domain is not S.Integers:
return domain.intersect(g_n)
return g_n
if isinstance(g_n, ImageSet):
lamda_expr = g_n.lamda.expr
lamda_vars = g_n.lamda.variables
base_set = g_n.base_set
sol_set = _solveset(f_x - lamda_expr, symbol, S.Integers)
if isinstance(sol_set, FiniteSet):
tmp_sol = EmptySet()
for sol in sol_set:
tmp_sol += ImageSet(Lambda(lamda_vars, sol), base_set)
sol_set = tmp_sol
else:
sol_set = ImageSet(Lambda(lamda_vars, sol_set), base_set)
return domain.intersect(sol_set)
return unsolved_result
def _term_factors(f):
"""
Iterator to get the factors of all terms present
in the given equation.
Parameters
==========
f : Expr
Equation that needs to be addressed
Returns
=======
Factors of all terms present in the equation.
Examples
========
>>> from sympy import symbols
>>> from sympy.solvers.solveset import _term_factors
>>> x = symbols('x')
>>> list(_term_factors(-2 - x**2 + x*(x + 1)))
[-2, -1, x**2, x, x + 1]
"""
for add_arg in Add.make_args(f):
for mul_arg in Mul.make_args(add_arg):
yield mul_arg
def _solve_exponential(lhs, rhs, symbol, domain):
r"""
Helper function for solving (supported) exponential equations.
Exponential equations are the sum of (currently) at most
two terms with one or both of them having a power with a
symbol-dependent exponent.
For example
.. math:: 5^{2x + 3} - 5^{3x - 1}
.. math:: 4^{5 - 9x} - e^{2 - x}
Parameters
==========
lhs, rhs : Expr
The exponential equation to be solved, `lhs = rhs`
symbol : Symbol
The variable in which the equation is solved
domain : Set
A set over which the equation is solved.
Returns
=======
A set of solutions satisfying the given equation.
A ``ConditionSet`` if the equation is unsolvable or
if the assumptions are not properly defined, in that case
a different style of ``ConditionSet`` is returned having the
solution(s) of the equation with the desired assumptions.
Examples
========
>>> from sympy.solvers.solveset import _solve_exponential as solve_expo
>>> from sympy import symbols, S
>>> x = symbols('x', real=True)
>>> a, b = symbols('a b')
>>> solve_expo(2**x + 3**x - 5**x, 0, x, S.Reals) # not solvable
ConditionSet(x, Eq(2**x + 3**x - 5**x, 0), Reals)
>>> solve_expo(a**x - b**x, 0, x, S.Reals) # solvable but incorrect assumptions
ConditionSet(x, (a > 0) & (b > 0), {0})
>>> solve_expo(3**(2*x) - 2**(x + 3), 0, x, S.Reals)
{-3*log(2)/(-2*log(3) + log(2))}
>>> solve_expo(2**x - 4**x, 0, x, S.Reals)
{0}
* Proof of correctness of the method
The logarithm function is the inverse of the exponential function.
The defining relation between exponentiation and logarithm is:
.. math:: {\log_b x} = y \enspace if \enspace b^y = x
Therefore if we are given an equation with exponent terms, we can
convert every term to its corresponding logarithmic form. This is
achieved by taking logarithms and expanding the equation using
logarithmic identities so that it can easily be handled by ``solveset``.
For example:
.. math:: 3^{2x} = 2^{x + 3}
Taking log both sides will reduce the equation to
.. math:: (2x)\log(3) = (x + 3)\log(2)
This form can be easily handed by ``solveset``.
"""
unsolved_result = ConditionSet(symbol, Eq(lhs - rhs, 0), domain)
newlhs = powdenest(lhs)
if lhs != newlhs:
# it may also be advantageous to factor the new expr
return _solveset(factor(newlhs - rhs), symbol, domain) # try again with _solveset
if not (isinstance(lhs, Add) and len(lhs.args) == 2):
# solving for the sum of more than two powers is possible
# but not yet implemented
return unsolved_result
if rhs != 0:
return unsolved_result
a, b = list(ordered(lhs.args))
a_term = a.as_independent(symbol)[1]
b_term = b.as_independent(symbol)[1]
a_base, a_exp = a_term.base, a_term.exp
b_base, b_exp = b_term.base, b_term.exp
from sympy.functions.elementary.complexes import im
if domain.is_subset(S.Reals):
conditions = And(
a_base > 0,
b_base > 0,
Eq(im(a_exp), 0),
Eq(im(b_exp), 0))
else:
conditions = And(
Ne(a_base, 0),
Ne(b_base, 0))
L, R = map(lambda i: expand_log(log(i), force=True), (a, -b))
solutions = _solveset(L - R, symbol, domain)
return ConditionSet(symbol, conditions, solutions)
def _is_exponential(f, symbol):
r"""
Return ``True`` if one or more terms contain ``symbol`` only in
exponents, else ``False``.
Parameters
==========
f : Expr
The equation to be checked
symbol : Symbol
The variable in which the equation is checked
Examples
========
>>> from sympy import symbols, cos, exp
>>> from sympy.solvers.solveset import _is_exponential as check
>>> x, y = symbols('x y')
>>> check(y, y)
False
>>> check(x**y - 1, y)
True
>>> check(x**y*2**y - 1, y)
True
>>> check(exp(x + 3) + 3**x, x)
True
>>> check(cos(2**x), x)
False
* Philosophy behind the helper
The function extracts each term of the equation and checks if it is
of exponential form w.r.t ``symbol``.
"""
rv = False
for expr_arg in _term_factors(f):
if symbol not in expr_arg.free_symbols:
continue
if (isinstance(expr_arg, Pow) and
symbol not in expr_arg.base.free_symbols or
isinstance(expr_arg, exp)):
rv = True # symbol in exponent
else:
return False # dependent on symbol in non-exponential way
return rv
def _solve_logarithm(lhs, rhs, symbol, domain):
r"""
Helper to solve logarithmic equations which are reducible
to a single instance of `\log`.
Logarithmic equations are (currently) the equations that contains
`\log` terms which can be reduced to a single `\log` term or
a constant using various logarithmic identities.
For example:
.. math:: \log(x) + \log(x - 4)
can be reduced to:
.. math:: \log(x(x - 4))
Parameters
==========
lhs, rhs : Expr
The logarithmic equation to be solved, `lhs = rhs`
symbol : Symbol
The variable in which the equation is solved
domain : Set
A set over which the equation is solved.
Returns
=======
A set of solutions satisfying the given equation.
A ``ConditionSet`` if the equation is unsolvable.
Examples
========
>>> from sympy import symbols, log, S
>>> from sympy.solvers.solveset import _solve_logarithm as solve_log
>>> x = symbols('x')
>>> f = log(x - 3) + log(x + 3)
>>> solve_log(f, 0, x, S.Reals)
{-sqrt(10), sqrt(10)}
* Proof of correctness
A logarithm is another way to write exponent and is defined by
.. math:: {\log_b x} = y \enspace if \enspace b^y = x
When one side of the equation contains a single logarithm, the
equation can be solved by rewriting the equation as an equivalent
exponential equation as defined above. But if one side contains
more than one logarithm, we need to use the properties of logarithm
to condense it into a single logarithm.
Take for example
.. math:: \log(2x) - 15 = 0
contains single logarithm, therefore we can directly rewrite it to
exponential form as
.. math:: x = \frac{e^{15}}{2}
But if the equation has more than one logarithm as
.. math:: \log(x - 3) + \log(x + 3) = 0
we use logarithmic identities to convert it into a reduced form
Using,
.. math:: \log(a) + \log(b) = \log(ab)
the equation becomes,
.. math:: \log((x - 3)(x + 3))
This equation contains one logarithm and can be solved by rewriting
to exponents.
"""
new_lhs = logcombine(lhs, force=True)
new_f = new_lhs - rhs
return _solveset(new_f, symbol, domain)
def _is_logarithmic(f, symbol):
r"""
Return ``True`` if the equation is in the form
`a\log(f(x)) + b\log(g(x)) + ... + c` else ``False``.
Parameters
==========
f : Expr
The equation to be checked
symbol : Symbol
The variable in which the equation is checked
Returns
=======
``True`` if the equation is logarithmic otherwise ``False``.
Examples
========
>>> from sympy import symbols, tan, log
>>> from sympy.solvers.solveset import _is_logarithmic as check
>>> x, y = symbols('x y')
>>> check(log(x + 2) - log(x + 3), x)
True
>>> check(tan(log(2*x)), x)
False
>>> check(x*log(x), x)
False
>>> check(x + log(x), x)
False
>>> check(y + log(x), x)
True
* Philosophy behind the helper
The function extracts each term and checks whether it is
logarithmic w.r.t ``symbol``.
"""
rv = False
for term in Add.make_args(f):
saw_log = False
for term_arg in Mul.make_args(term):
if symbol not in term_arg.free_symbols:
continue
if isinstance(term_arg, log):
if saw_log:
return False # more than one log in term
saw_log = True
else:
return False # dependent on symbol in non-log way
if saw_log:
rv = True
return rv
def _transolve(f, symbol, domain):
r"""
Function to solve transcendental equations. It is a helper to
``solveset`` and should be used internally. ``_transolve``
currently supports the following class of equations:
- Exponential equations
- Logarithmic equations
Parameters
==========
f : Any transcendental equation that needs to be solved.
This needs to be an expression, which is assumed
to be equal to ``0``.
symbol : The variable for which the equation is solved.
This needs to be of class ``Symbol``.
domain : A set over which the equation is solved.
This needs to be of class ``Set``.
Returns
=======
Set
A set of values for ``symbol`` for which ``f`` is equal to
zero. An ``EmptySet`` is returned if ``f`` does not have solutions
in respective domain. A ``ConditionSet`` is returned as unsolved
object if algorithms to evaluate complete solution are not
yet implemented.
How to use ``_transolve``
=========================
``_transolve`` should not be used as an independent function, because
it assumes that the equation (``f``) and the ``symbol`` comes from
``solveset`` and might have undergone a few modification(s).
To use ``_transolve`` as an independent function the equation (``f``)
and the ``symbol`` should be passed as they would have been by
``solveset``.
Examples
========
>>> from sympy.solvers.solveset import _transolve as transolve
>>> from sympy.solvers.solvers import _tsolve as tsolve
>>> from sympy import symbols, S, pprint
>>> x = symbols('x', real=True) # assumption added
>>> transolve(5**(x - 3) - 3**(2*x + 1), x, S.Reals)
{-(log(3) + 3*log(5))/(-log(5) + 2*log(3))}
How ``_transolve`` works
========================
``_transolve`` uses two types of helper functions to solve equations
of a particular class:
Identifying helpers: To determine whether a given equation
belongs to a certain class of equation or not. Returns either
``True`` or ``False``.
Solving helpers: Once an equation is identified, a corresponding
helper either solves the equation or returns a form of the equation
that ``solveset`` might better be able to handle.
* Philosophy behind the module
The purpose of ``_transolve`` is to take equations which are not
already polynomial in their generator(s) and to either recast them
as such through a valid transformation or to solve them outright.
A pair of helper functions for each class of supported
transcendental functions are employed for this purpose. One
identifies the transcendental form of an equation and the other
either solves it or recasts it into a tractable form that can be
solved by ``solveset``.
For example, an equation in the form `ab^{f(x)} - cd^{g(x)} = 0`
can be transformed to
`\log(a) + f(x)\log(b) - \log(c) - g(x)\log(d) = 0`
(under certain assumptions) and this can be solved with ``solveset``
if `f(x)` and `g(x)` are in polynomial form.
How ``_transolve`` is better than ``_tsolve``
=============================================
1) Better output
``_transolve`` provides expressions in a more simplified form.
Consider a simple exponential equation
>>> f = 3**(2*x) - 2**(x + 3)
>>> pprint(transolve(f, x, S.Reals), use_unicode=False)
-3*log(2)
{------------------}
-2*log(3) + log(2)
>>> pprint(tsolve(f, x), use_unicode=False)
/ 3 \
| --------|
| log(2/9)|
[-log\2 /]
2) Extensible
The API of ``_transolve`` is designed such that it is easily
extensible, i.e. the code that solves a given class of
equations is encapsulated in a helper and not mixed in with
the code of ``_transolve`` itself.
3) Modular
``_transolve`` is designed to be modular i.e, for every class of
equation a separate helper for identification and solving is
implemented. This makes it easy to change or modify any of the
method implemented directly in the helpers without interfering
with the actual structure of the API.
4) Faster Computation
Solving equation via ``_transolve`` is much faster as compared to
``_tsolve``. In ``solve``, attempts are made computing every possibility
to get the solutions. This series of attempts makes solving a bit
slow. In ``_transolve``, computation begins only after a particular
type of equation is identified.
How to add new class of equations
=================================
Adding a new class of equation solver is a three-step procedure:
- Identify the type of the equations
Determine the type of the class of equations to which they belong:
it could be of ``Add``, ``Pow``, etc. types. Separate internal functions
are used for each type. Write identification and solving helpers
and use them from within the routine for the given type of equation
(after adding it, if necessary). Something like:
.. code-block:: python
def add_type(lhs, rhs, x):
....
if _is_exponential(lhs, x):
new_eq = _solve_exponential(lhs, rhs, x)
....
rhs, lhs = eq.as_independent(x)
if lhs.is_Add:
result = add_type(lhs, rhs, x)
- Define the identification helper.
- Define the solving helper.
Apart from this, a few other things needs to be taken care while
adding an equation solver:
- Naming conventions:
Name of the identification helper should be as
``_is_class`` where class will be the name or abbreviation
of the class of equation. The solving helper will be named as
``_solve_class``.
For example: for exponential equations it becomes
``_is_exponential`` and ``_solve_expo``.
- The identifying helpers should take two input parameters,
the equation to be checked and the variable for which a solution
is being sought, while solving helpers would require an additional
domain parameter.
- Be sure to consider corner cases.
- Add tests for each helper.
- Add a docstring to your helper that describes the method
implemented.
The documentation of the helpers should identify:
- the purpose of the helper,
- the method used to identify and solve the equation,
- a proof of correctness
- the return values of the helpers
"""
def add_type(lhs, rhs, symbol, domain):
"""
Helper for ``_transolve`` to handle equations of
``Add`` type, i.e. equations taking the form as
``a*f(x) + b*g(x) + .... = c``.
For example: 4**x + 8**x = 0
"""
result = ConditionSet(symbol, Eq(lhs - rhs, 0), domain)
# check if it is exponential type equation
if _is_exponential(lhs, symbol):
result = _solve_exponential(lhs, rhs, symbol, domain)
# check if it is logarithmic type equation
elif _is_logarithmic(lhs, symbol):
result = _solve_logarithm(lhs, rhs, symbol, domain)
return result
result = ConditionSet(symbol, Eq(f, 0), domain)
# invert_complex handles the call to the desired inverter based
# on the domain specified.
lhs, rhs_s = invert_complex(f, 0, symbol, domain)
if isinstance(rhs_s, FiniteSet):
assert (len(rhs_s.args)) == 1
rhs = rhs_s.args[0]
if lhs.is_Add:
result = add_type(lhs, rhs, symbol, domain)
else:
result = rhs_s
return result
def solveset(f, symbol=None, domain=S.Complexes):
r"""Solves a given inequality or equation with set as output
Parameters
==========
f : Expr or a relational.
The target equation or inequality
symbol : Symbol
The variable for which the equation is solved
domain : Set
The domain over which the equation is solved
Returns
=======
Set
A set of values for `symbol` for which `f` is True or is equal to
zero. An `EmptySet` is returned if `f` is False or nonzero.
A `ConditionSet` is returned as unsolved object if algorithms
to evaluate complete solution are not yet implemented.
`solveset` claims to be complete in the solution set that it returns.
Raises
======
NotImplementedError
The algorithms to solve inequalities in complex domain are
not yet implemented.
ValueError
The input is not valid.
RuntimeError
It is a bug, please report to the github issue tracker.
Notes
=====
Python interprets 0 and 1 as False and True, respectively, but
in this function they refer to solutions of an expression. So 0 and 1
return the Domain and EmptySet, respectively, while True and False
return the opposite (as they are assumed to be solutions of relational
expressions).
See Also
========
solveset_real: solver for real domain
solveset_complex: solver for complex domain
Examples
========
>>> from sympy import exp, sin, Symbol, pprint, S
>>> from sympy.solvers.solveset import solveset, solveset_real
* The default domain is complex. Not specifying a domain will lead
to the solving of the equation in the complex domain (and this
is not affected by the assumptions on the symbol):
>>> x = Symbol('x')
>>> pprint(solveset(exp(x) - 1, x), use_unicode=False)
{2*n*I*pi | n in Integers}
>>> x = Symbol('x', real=True)
>>> pprint(solveset(exp(x) - 1, x), use_unicode=False)
{2*n*I*pi | n in Integers}
* If you want to use `solveset` to solve the equation in the
real domain, provide a real domain. (Using ``solveset_real``
does this automatically.)
>>> R = S.Reals
>>> x = Symbol('x')
>>> solveset(exp(x) - 1, x, R)
{0}
>>> solveset_real(exp(x) - 1, x)
{0}
The solution is mostly unaffected by assumptions on the symbol,
but there may be some slight difference:
>>> pprint(solveset(sin(x)/x,x), use_unicode=False)
({2*n*pi | n in Integers} \ {0}) U ({2*n*pi + pi | n in Integers} \ {0})
>>> p = Symbol('p', positive=True)
>>> pprint(solveset(sin(p)/p, p), use_unicode=False)
{2*n*pi | n in Integers} U {2*n*pi + pi | n in Integers}
* Inequalities can be solved over the real domain only. Use of a complex
domain leads to a NotImplementedError.
>>> solveset(exp(x) > 1, x, R)
Interval.open(0, oo)
"""
f = sympify(f)
symbol = sympify(symbol)
if f is S.true:
return domain
if f is S.false:
return S.EmptySet
if not isinstance(f, (Expr, Number)):
raise ValueError("%s is not a valid SymPy expression" % f)
if not isinstance(symbol, Expr) and symbol is not None:
raise ValueError("%s is not a valid SymPy symbol" % symbol)
if not isinstance(domain, Set):
raise ValueError("%s is not a valid domain" %(domain))
free_symbols = f.free_symbols
if symbol is None and not free_symbols:
b = Eq(f, 0)
if b is S.true:
return domain
elif b is S.false:
return S.EmptySet
else:
raise NotImplementedError(filldedent('''
relationship between value and 0 is unknown: %s''' % b))
if symbol is None:
if len(free_symbols) == 1:
symbol = free_symbols.pop()
elif free_symbols:
raise ValueError(filldedent('''
The independent variable must be specified for a
multivariate equation.'''))
elif not isinstance(symbol, Symbol):
f, s, swap = recast_to_symbols([f], [symbol])
# the xreplace will be needed if a ConditionSet is returned
return solveset(f[0], s[0], domain).xreplace(swap)
if domain.is_subset(S.Reals):
if not symbol.is_real:
assumptions = symbol.assumptions0
assumptions['real'] = True
try:
r = Dummy('r', **assumptions)
return solveset(f.xreplace({symbol: r}), r, domain
).xreplace({r: symbol})
except InconsistentAssumptions:
pass
# Abs has its own handling method which avoids the
# rewriting property that the first piece of abs(x)
# is for x >= 0 and the 2nd piece for x < 0 -- solutions
# can look better if the 2nd condition is x <= 0. Since
# the solution is a set, duplication of results is not
# an issue, e.g. {y, -y} when y is 0 will be {0}
f, mask = _masked(f, Abs)
f = f.rewrite(Piecewise) # everything that's not an Abs
for d, e in mask:
# everything *in* an Abs
e = e.func(e.args[0].rewrite(Piecewise))
f = f.xreplace({d: e})
f = piecewise_fold(f)
return _solveset(f, symbol, domain, _check=True)
def solveset_real(f, symbol):
return solveset(f, symbol, S.Reals)
def solveset_complex(f, symbol):
return solveset(f, symbol, S.Complexes)
def solvify(f, symbol, domain):
"""Solves an equation using solveset and returns the solution in accordance
with the `solve` output API.
Returns
=======
We classify the output based on the type of solution returned by `solveset`.
Solution | Output
----------------------------------------
FiniteSet | list
ImageSet, | list (if `f` is periodic)
Union |
EmptySet | empty list
Others | None
Raises
======
NotImplementedError
A ConditionSet is the input.
Examples
========
>>> from sympy.solvers.solveset import solvify, solveset
>>> from sympy.abc import x
>>> from sympy import S, tan, sin, exp
>>> solvify(x**2 - 9, x, S.Reals)
[-3, 3]
>>> solvify(sin(x) - 1, x, S.Reals)
[pi/2]
>>> solvify(tan(x), x, S.Reals)
[0]
>>> solvify(exp(x) - 1, x, S.Complexes)
>>> solvify(exp(x) - 1, x, S.Reals)
[0]
"""
solution_set = solveset(f, symbol, domain)
result = None
if solution_set is S.EmptySet:
result = []
elif isinstance(solution_set, ConditionSet):
raise NotImplementedError('solveset is unable to solve this equation.')
elif isinstance(solution_set, FiniteSet):
result = list(solution_set)
else:
period = periodicity(f, symbol)
if period is not None:
solutions = S.EmptySet
iter_solutions = ()
if isinstance(solution_set, ImageSet):
iter_solutions = (solution_set,)
elif isinstance(solution_set, Union):
if all(isinstance(i, ImageSet) for i in solution_set.args):
iter_solutions = solution_set.args
for solution in iter_solutions:
solutions += solution.intersect(Interval(0, period, False, True))
if isinstance(solutions, FiniteSet):
result = list(solutions)
else:
solution = solution_set.intersect(domain)
if isinstance(solution, FiniteSet):
result += solution
return result
###############################################################################
################################ LINSOLVE #####################################
###############################################################################
def linear_coeffs(eq, *syms, **_kw):
"""Return a list whose elements are the coefficients of the
corresponding symbols in the sum of terms in ``eq``.
The additive constant is returned as the last element of the
list.
Examples
========
>>> from sympy.solvers.solveset import linear_coeffs
>>> from sympy.abc import x, y, z
>>> linear_coeffs(3*x + 2*y - 1, x, y)
[3, 2, -1]
It is not necessary to expand the expression:
>>> linear_coeffs(x + y*(z*(x*3 + 2) + 3), x)
[3*y*z + 1, y*(2*z + 3)]
But if there are nonlinear or cross terms -- even if they would
cancel after simplification -- an error is raised so the situation
does not pass silently past the caller's attention:
>>> eq = 1/x*(x - 1) + 1/x
>>> linear_coeffs(eq.expand(), x)
[0, 1]
>>> linear_coeffs(eq, x)
Traceback (most recent call last):
...
ValueError: nonlinear term encountered: 1/x
>>> linear_coeffs(x*(y + 1) - x*y, x, y)
Traceback (most recent call last):
...
ValueError: nonlinear term encountered: x*(y + 1)
"""
d = defaultdict(list)
c, terms = _sympify(eq).as_coeff_add(*syms)
d[0].extend(Add.make_args(c))
for t in terms:
m, f = t.as_coeff_mul(*syms)
if len(f) != 1:
break
f = f[0]
if f in syms:
d[f].append(m)
elif f.is_Add:
d1 = linear_coeffs(f, *syms, **{'dict': True})
d[0].append(m*d1.pop(0))
for xf, vf in d1.items():
d[xf].append(m*vf)
else:
break
else:
for k, v in d.items():
d[k] = Add(*v)
if not _kw:
return [d.get(s, S.Zero) for s in syms] + [d[0]]
return d # default is still list but this won't matter
raise ValueError('nonlinear term encountered: %s' % t)
def linear_eq_to_matrix(equations, *symbols):
r"""
Converts a given System of Equations into Matrix form.
Here `equations` must be a linear system of equations in
`symbols`. Element M[i, j] corresponds to the coefficient
of the jth symbol in the ith equation.
The Matrix form corresponds to the augmented matrix form.
For example:
.. math:: 4x + 2y + 3z = 1
.. math:: 3x + y + z = -6
.. math:: 2x + 4y + 9z = 2
This system would return `A` & `b` as given below:
::
[ 4 2 3 ] [ 1 ]
A = [ 3 1 1 ] b = [-6 ]
[ 2 4 9 ] [ 2 ]
The only simplification performed is to convert
`Eq(a, b) -> a - b`.
Raises
======
ValueError
The equations contain a nonlinear term.
The symbols are not given or are not unique.
Examples
========
>>> from sympy import linear_eq_to_matrix, symbols
>>> c, x, y, z = symbols('c, x, y, z')
The coefficients (numerical or symbolic) of the symbols will
be returned as matrices:
>>> eqns = [c*x + z - 1 - c, y + z, x - y]
>>> A, b = linear_eq_to_matrix(eqns, [x, y, z])
>>> A
Matrix([
[c, 0, 1],
[0, 1, 1],
[1, -1, 0]])
>>> b
Matrix([
[c + 1],
[ 0],
[ 0]])
This routine does not simplify expressions and will raise an error
if nonlinearity is encountered:
>>> eqns = [
... (x**2 - 3*x)/(x - 3) - 3,
... y**2 - 3*y - y*(y - 4) + x - 4]
>>> linear_eq_to_matrix(eqns, [x, y])
Traceback (most recent call last):
...
ValueError:
The term (x**2 - 3*x)/(x - 3) is nonlinear in {x, y}
Simplifying these equations will discard the removable singularity
in the first, reveal the linear structure of the second:
>>> [e.simplify() for e in eqns]
[x - 3, x + y - 4]
Any such simplification needed to eliminate nonlinear terms must
be done before calling this routine.
"""
if not symbols:
raise ValueError(filldedent('''
Symbols must be given, for which coefficients
are to be found.
'''))
if hasattr(symbols[0], '__iter__'):
symbols = symbols[0]
for i in symbols:
if not isinstance(i, Symbol):
raise ValueError(filldedent('''
Expecting a Symbol but got %s
''' % i))
if has_dups(symbols):
raise ValueError('Symbols must be unique')
equations = sympify(equations)
if isinstance(equations, MatrixBase):
equations = list(equations)
elif isinstance(equations, Expr):
equations = [equations]
elif not is_sequence(equations):
raise ValueError(filldedent('''
Equation(s) must be given as a sequence, Expr,
Eq or Matrix.
'''))
A, b = [], []
for i, f in enumerate(equations):
if isinstance(f, Equality):
f = f.rewrite(Add, evaluate=False)
coeff_list = linear_coeffs(f, *symbols)
b.append(-coeff_list.pop())
A.append(coeff_list)
A, b = map(Matrix, (A, b))
return A, b
def linsolve(system, *symbols):
r"""
Solve system of N linear equations with M variables; both
underdetermined and overdetermined systems are supported.
The possible number of solutions is zero, one or infinite.
Zero solutions throws a ValueError, whereas infinite
solutions are represented parametrically in terms of the given
symbols. For unique solution a FiniteSet of ordered tuples
is returned.
All Standard input formats are supported:
For the given set of Equations, the respective input types
are given below:
.. math:: 3x + 2y - z = 1
.. math:: 2x - 2y + 4z = -2
.. math:: 2x - y + 2z = 0
* Augmented Matrix Form, `system` given below:
::
[3 2 -1 1]
system = [2 -2 4 -2]
[2 -1 2 0]
* List Of Equations Form
`system = [3x + 2y - z - 1, 2x - 2y + 4z + 2, 2x - y + 2z]`
* Input A & b Matrix Form (from Ax = b) are given as below:
::
[3 2 -1 ] [ 1 ]
A = [2 -2 4 ] b = [ -2 ]
[2 -1 2 ] [ 0 ]
`system = (A, b)`
Symbols can always be passed but are actually only needed
when 1) a system of equations is being passed and 2) the
system is passed as an underdetermined matrix and one wants
to control the name of the free variables in the result.
An error is raised if no symbols are used for case 1, but if
no symbols are provided for case 2, internally generated symbols
will be provided. When providing symbols for case 2, there should
be at least as many symbols are there are columns in matrix A.
The algorithm used here is Gauss-Jordan elimination, which
results, after elimination, in a row echelon form matrix.
Returns
=======
A FiniteSet containing an ordered tuple of values for the
unknowns for which the `system` has a solution. (Wrapping
the tuple in FiniteSet is used to maintain a consistent
output format throughout solveset.)
Returns EmptySet(), if the linear system is inconsistent.
Raises
======
ValueError
The input is not valid.
The symbols are not given.
Examples
========
>>> from sympy import Matrix, S, linsolve, symbols
>>> x, y, z = symbols("x, y, z")
>>> A = Matrix([[1, 2, 3], [4, 5, 6], [7, 8, 10]])
>>> b = Matrix([3, 6, 9])
>>> A
Matrix([
[1, 2, 3],
[4, 5, 6],
[7, 8, 10]])
>>> b
Matrix([
[3],
[6],
[9]])
>>> linsolve((A, b), [x, y, z])
{(-1, 2, 0)}
* Parametric Solution: In case the system is underdetermined, the
function will return a parametric solution in terms of the given
symbols. Those that are free will be returned unchanged. e.g. in
the system below, `z` is returned as the solution for variable z;
it can take on any value.
>>> A = Matrix([[1, 2, 3], [4, 5, 6], [7, 8, 9]])
>>> b = Matrix([3, 6, 9])
>>> linsolve((A, b), x, y, z)
{(z - 1, 2 - 2*z, z)}
If no symbols are given, internally generated symbols will be used.
The `tau0` in the 3rd position indicates (as before) that the 3rd
variable -- whatever it's named -- can take on any value:
>>> linsolve((A, b))
{(tau0 - 1, 2 - 2*tau0, tau0)}
* List of Equations as input
>>> Eqns = [3*x + 2*y - z - 1, 2*x - 2*y + 4*z + 2, - x + y/2 - z]
>>> linsolve(Eqns, x, y, z)
{(1, -2, -2)}
* Augmented Matrix as input
>>> aug = Matrix([[2, 1, 3, 1], [2, 6, 8, 3], [6, 8, 18, 5]])
>>> aug
Matrix([
[2, 1, 3, 1],
[2, 6, 8, 3],
[6, 8, 18, 5]])
>>> linsolve(aug, x, y, z)
{(3/10, 2/5, 0)}
* Solve for symbolic coefficients
>>> a, b, c, d, e, f = symbols('a, b, c, d, e, f')
>>> eqns = [a*x + b*y - c, d*x + e*y - f]
>>> linsolve(eqns, x, y)
{((-b*f + c*e)/(a*e - b*d), (a*f - c*d)/(a*e - b*d))}
* A degenerate system returns solution as set of given
symbols.
>>> system = Matrix(([0, 0, 0], [0, 0, 0], [0, 0, 0]))
>>> linsolve(system, x, y)
{(x, y)}
* For an empty system linsolve returns empty set
>>> linsolve([], x)
EmptySet()
* An error is raised if, after expansion, any nonlinearity
is detected:
>>> linsolve([x*(1/x - 1), (y - 1)**2 - y**2 + 1], x, y)
{(1, 1)}
>>> linsolve([x**2 - 1], x)
Traceback (most recent call last):
...
ValueError:
The term x**2 is nonlinear in {x}
"""
if not system:
return S.EmptySet
# If second argument is an iterable
if symbols and hasattr(symbols[0], '__iter__'):
symbols = symbols[0]
sym_gen = isinstance(symbols, GeneratorType)
swap = {}
b = None # if we don't get b the input was bad
syms_needed_msg = None
# unpack system
if hasattr(system, '__iter__'):
# 1). (A, b)
if len(system) == 2 and isinstance(system[0], Matrix):
A, b = system
# 2). (eq1, eq2, ...)
if not isinstance(system[0], Matrix):
if sym_gen or not symbols:
raise ValueError(filldedent('''
When passing a system of equations, the explicit
symbols for which a solution is being sought must
be given as a sequence, too.
'''))
system = [
_mexpand(i.lhs - i.rhs if isinstance(i, Eq) else i,
recursive=True) for i in system]
system, symbols, swap = recast_to_symbols(system, symbols)
A, b = linear_eq_to_matrix(system, symbols)
syms_needed_msg = 'free symbols in the equations provided'
elif isinstance(system, Matrix) and not (
symbols and not isinstance(symbols, GeneratorType) and
isinstance(symbols[0], Matrix)):
# 3). A augmented with b
A, b = system[:, :-1], system[:, -1:]
if b is None:
raise ValueError("Invalid arguments")
syms_needed_msg = syms_needed_msg or 'columns of A'
if sym_gen:
symbols = [next(symbols) for i in range(A.cols)]
if any(set(symbols) & (A.free_symbols | b.free_symbols)):
raise ValueError(filldedent('''
At least one of the symbols provided
already appears in the system to be solved.
One way to avoid this is to use Dummy symbols in
the generator, e.g. numbered_symbols('%s', cls=Dummy)
''' % symbols[0].name.rstrip('1234567890')))
try:
solution, params, free_syms = A.gauss_jordan_solve(b, freevar=True)
except ValueError:
# No solution
return S.EmptySet
# Replace free parameters with free symbols
if params:
if not symbols:
symbols = [_ for _ in params]
# re-use the parameters but put them in order
# params [x, y, z]
# free_symbols [2, 0, 4]
# idx [1, 0, 2]
idx = list(zip(*sorted(zip(free_syms, range(len(free_syms))))))[1]
# simultaneous replacements {y: x, x: y, z: z}
replace_dict = dict(zip(symbols, [symbols[i] for i in idx]))
elif len(symbols) >= A.cols:
replace_dict = {v: symbols[free_syms[k]] for k, v in enumerate(params)}
else:
raise IndexError(filldedent('''
the number of symbols passed should have a length
equal to the number of %s.
''' % syms_needed_msg))
solution = [sol.xreplace(replace_dict) for sol in solution]
solution = [simplify(sol).xreplace(swap) for sol in solution]
return FiniteSet(tuple(solution))
##############################################################################
# ------------------------------nonlinsolve ---------------------------------#
##############################################################################
def _return_conditionset(eqs, symbols):
# return conditionset
condition_set = ConditionSet(
Tuple(*symbols),
FiniteSet(*eqs),
S.Complexes)
return condition_set
def substitution(system, symbols, result=[{}], known_symbols=[],
exclude=[], all_symbols=None):
r"""
Solves the `system` using substitution method. It is used in
`nonlinsolve`. This will be called from `nonlinsolve` when any
equation(s) is non polynomial equation.
Parameters
==========
system : list of equations
The target system of equations
symbols : list of symbols to be solved.
The variable(s) for which the system is solved
known_symbols : list of solved symbols
Values are known for these variable(s)
result : An empty list or list of dict
If No symbol values is known then empty list otherwise
symbol as keys and corresponding value in dict.
exclude : Set of expression.
Mostly denominator expression(s) of the equations of the system.
Final solution should not satisfy these expressions.
all_symbols : known_symbols + symbols(unsolved).
Returns
=======
A FiniteSet of ordered tuple of values of `all_symbols` for which the
`system` has solution. Order of values in the tuple is same as symbols
present in the parameter `all_symbols`. If parameter `all_symbols` is None
then same as symbols present in the parameter `symbols`.
Please note that general FiniteSet is unordered, the solution returned
here is not simply a FiniteSet of solutions, rather it is a FiniteSet of
ordered tuple, i.e. the first & only argument to FiniteSet is a tuple of
solutions, which is ordered, & hence the returned solution is ordered.
Also note that solution could also have been returned as an ordered tuple,
FiniteSet is just a wrapper `{}` around the tuple. It has no other
significance except for the fact it is just used to maintain a consistent
output format throughout the solveset.
Raises
======
ValueError
The input is not valid.
The symbols are not given.
AttributeError
The input symbols are not `Symbol` type.
Examples
========
>>> from sympy.core.symbol import symbols
>>> x, y = symbols('x, y', real=True)
>>> from sympy.solvers.solveset import substitution
>>> substitution([x + y], [x], [{y: 1}], [y], set([]), [x, y])
{(-1, 1)}
* when you want soln should not satisfy eq `x + 1 = 0`
>>> substitution([x + y], [x], [{y: 1}], [y], set([x + 1]), [y, x])
EmptySet()
>>> substitution([x + y], [x], [{y: 1}], [y], set([x - 1]), [y, x])
{(1, -1)}
>>> substitution([x + y - 1, y - x**2 + 5], [x, y])
{(-3, 4), (2, -1)}
* Returns both real and complex solution
>>> x, y, z = symbols('x, y, z')
>>> from sympy import exp, sin
>>> substitution([exp(x) - sin(y), y**2 - 4], [x, y])
{(ImageSet(Lambda(_n, I*(2*_n*pi + pi) + log(sin(2))), Integers), -2),
(ImageSet(Lambda(_n, 2*_n*I*pi + log(sin(2))), Integers), 2)}
>>> eqs = [z**2 + exp(2*x) - sin(y), -3 + exp(-y)]
>>> substitution(eqs, [y, z])
{(-log(3), -sqrt(-exp(2*x) - sin(log(3)))),
(-log(3), sqrt(-exp(2*x) - sin(log(3)))),
(ImageSet(Lambda(_n, 2*_n*I*pi - log(3)), Integers),
ImageSet(Lambda(_n, -sqrt(-exp(2*x) + sin(2*_n*I*pi - log(3)))), Integers)),
(ImageSet(Lambda(_n, 2*_n*I*pi - log(3)), Integers),
ImageSet(Lambda(_n, sqrt(-exp(2*x) + sin(2*_n*I*pi - log(3)))), Integers))}
"""
from sympy import Complement
from sympy.core.compatibility import is_sequence
if not system:
return S.EmptySet
if not symbols:
msg = ('Symbols must be given, for which solution of the '
'system is to be found.')
raise ValueError(filldedent(msg))
if not is_sequence(symbols):
msg = ('symbols should be given as a sequence, e.g. a list.'
'Not type %s: %s')
raise TypeError(filldedent(msg % (type(symbols), symbols)))
sym = getattr(symbols[0], 'is_Symbol', False)
if not sym:
msg = ('Iterable of symbols must be given as '
'second argument, not type %s: %s')
raise ValueError(filldedent(msg % (type(symbols[0]), symbols[0])))
# By default `all_symbols` will be same as `symbols`
if all_symbols is None:
all_symbols = symbols
old_result = result
# storing complements and intersection for particular symbol
complements = {}
intersections = {}
# when total_solveset_call equals total_conditionset
# it means that solveset failed to solve all eqs.
total_conditionset = -1
total_solveset_call = -1
def _unsolved_syms(eq, sort=False):
"""Returns the unsolved symbol present
in the equation `eq`.
"""
free = eq.free_symbols
unsolved = (free - set(known_symbols)) & set(all_symbols)
if sort:
unsolved = list(unsolved)
unsolved.sort(key=default_sort_key)
return unsolved
# end of _unsolved_syms()
# sort such that equation with the fewest potential symbols is first.
# means eq with less number of variable first in the list.
eqs_in_better_order = list(
ordered(system, lambda _: len(_unsolved_syms(_))))
def add_intersection_complement(result, sym_set, **flags):
# If solveset have returned some intersection/complement
# for any symbol. It will be added in final solution.
final_result = []
for res in result:
res_copy = res
for key_res, value_res in res.items():
# Intersection/complement is in Interval or Set.
intersection_true = flags.get('Intersection', True)
complements_true = flags.get('Complement', True)
for key_sym, value_sym in sym_set.items():
if key_sym == key_res:
if intersection_true:
# testcase is not added for this line(intersection)
new_value = \
Intersection(FiniteSet(value_res), value_sym)
if new_value is not S.EmptySet:
res_copy[key_res] = new_value
if complements_true:
new_value = \
Complement(FiniteSet(value_res), value_sym)
if new_value is not S.EmptySet:
res_copy[key_res] = new_value
final_result.append(res_copy)
return final_result
# end of def add_intersection_complement()
def _extract_main_soln(sol, soln_imageset):
"""separate the Complements, Intersections, ImageSet lambda expr
and it's base_set.
"""
# if there is union, then need to check
# Complement, Intersection, Imageset.
# Order should not be changed.
if isinstance(sol, Complement):
# extract solution and complement
complements[sym] = sol.args[1]
sol = sol.args[0]
# complement will be added at the end
# using `add_intersection_complement` method
if isinstance(sol, Intersection):
# Interval/Set will be at 0th index always
if sol.args[0] != Interval(-oo, oo):
# sometimes solveset returns soln
# with intersection `S.Reals`, to confirm that
# soln is in `domain=S.Reals` or not. We don't consider
# that intersection.
intersections[sym] = sol.args[0]
sol = sol.args[1]
# after intersection and complement Imageset should
# be checked.
if isinstance(sol, ImageSet):
soln_imagest = sol
expr2 = sol.lamda.expr
sol = FiniteSet(expr2)
soln_imageset[expr2] = soln_imagest
# if there is union of Imageset or other in soln.
# no testcase is written for this if block
if isinstance(sol, Union):
sol_args = sol.args
sol = S.EmptySet
# We need in sequence so append finteset elements
# and then imageset or other.
for sol_arg2 in sol_args:
if isinstance(sol_arg2, FiniteSet):
sol += sol_arg2
else:
# ImageSet, Intersection, complement then
# append them directly
sol += FiniteSet(sol_arg2)
if not isinstance(sol, FiniteSet):
sol = FiniteSet(sol)
return sol, soln_imageset
# end of def _extract_main_soln()
# helper function for _append_new_soln
def _check_exclude(rnew, imgset_yes):
rnew_ = rnew
if imgset_yes:
# replace all dummy variables (Imageset lambda variables)
# with zero before `checksol`. Considering fundamental soln
# for `checksol`.
rnew_copy = rnew.copy()
dummy_n = imgset_yes[0]
for key_res, value_res in rnew_copy.items():
rnew_copy[key_res] = value_res.subs(dummy_n, 0)
rnew_ = rnew_copy
# satisfy_exclude == true if it satisfies the expr of `exclude` list.
try:
# something like : `Mod(-log(3), 2*I*pi)` can't be
# simplified right now, so `checksol` returns `TypeError`.
# when this issue is fixed this try block should be
# removed. Mod(-log(3), 2*I*pi) == -log(3)
satisfy_exclude = any(
checksol(d, rnew_) for d in exclude)
except TypeError:
satisfy_exclude = None
return satisfy_exclude
# end of def _check_exclude()
# helper function for _append_new_soln
def _restore_imgset(rnew, original_imageset, newresult):
restore_sym = set(rnew.keys()) & \
set(original_imageset.keys())
for key_sym in restore_sym:
img = original_imageset[key_sym]
rnew[key_sym] = img
if rnew not in newresult:
newresult.append(rnew)
# end of def _restore_imgset()
def _append_eq(eq, result, res, delete_soln, n=None):
u = Dummy('u')
if n:
eq = eq.subs(n, 0)
satisfy = checksol(u, u, eq, minimal=True)
if satisfy is False:
delete_soln = True
res = {}
else:
result.append(res)
return result, res, delete_soln
def _append_new_soln(rnew, sym, sol, imgset_yes, soln_imageset,
original_imageset, newresult, eq=None):
"""If `rnew` (A dict <symbol: soln>) contains valid soln
append it to `newresult` list.
`imgset_yes` is (base, dummy_var) if there was imageset in previously
calculated result(otherwise empty tuple). `original_imageset` is dict
of imageset expr and imageset from this result.
`soln_imageset` dict of imageset expr and imageset of new soln.
"""
satisfy_exclude = _check_exclude(rnew, imgset_yes)
delete_soln = False
# soln should not satisfy expr present in `exclude` list.
if not satisfy_exclude:
local_n = None
# if it is imageset
if imgset_yes:
local_n = imgset_yes[0]
base = imgset_yes[1]
if sym and sol:
# when `sym` and `sol` is `None` means no new
# soln. In that case we will append rnew directly after
# substituting original imagesets in rnew values if present
# (second last line of this function using _restore_imgset)
dummy_list = list(sol.atoms(Dummy))
# use one dummy `n` which is in
# previous imageset
local_n_list = [
local_n for i in range(
0, len(dummy_list))]
dummy_zip = zip(dummy_list, local_n_list)
lam = Lambda(local_n, sol.subs(dummy_zip))
rnew[sym] = ImageSet(lam, base)
if eq is not None:
newresult, rnew, delete_soln = _append_eq(
eq, newresult, rnew, delete_soln, local_n)
elif eq is not None:
newresult, rnew, delete_soln = _append_eq(
eq, newresult, rnew, delete_soln)
elif soln_imageset:
rnew[sym] = soln_imageset[sol]
# restore original imageset
_restore_imgset(rnew, original_imageset, newresult)
else:
newresult.append(rnew)
elif satisfy_exclude:
delete_soln = True
rnew = {}
_restore_imgset(rnew, original_imageset, newresult)
return newresult, delete_soln
# end of def _append_new_soln()
def _new_order_result(result, eq):
# separate first, second priority. `res` that makes `eq` value equals
# to zero, should be used first then other result(second priority).
# If it is not done then we may miss some soln.
first_priority = []
second_priority = []
for res in result:
if not any(isinstance(val, ImageSet) for val in res.values()):
if eq.subs(res) == 0:
first_priority.append(res)
else:
second_priority.append(res)
if first_priority or second_priority:
return first_priority + second_priority
return result
def _solve_using_known_values(result, solver):
"""Solves the system using already known solution
(result contains the dict <symbol: value>).
solver is `solveset_complex` or `solveset_real`.
"""
# stores imageset <expr: imageset(Lambda(n, expr), base)>.
soln_imageset = {}
total_solvest_call = 0
total_conditionst = 0
# sort such that equation with the fewest potential symbols is first.
# means eq with less variable first
for index, eq in enumerate(eqs_in_better_order):
newresult = []
original_imageset = {}
# if imageset expr is used to solve other symbol
imgset_yes = False
result = _new_order_result(result, eq)
for res in result:
got_symbol = set() # symbols solved in one iteration
if soln_imageset:
# find the imageset and use its expr.
for key_res, value_res in res.items():
if isinstance(value_res, ImageSet):
res[key_res] = value_res.lamda.expr
original_imageset[key_res] = value_res
dummy_n = value_res.lamda.expr.atoms(Dummy).pop()
base = value_res.base_set
imgset_yes = (dummy_n, base)
# update eq with everything that is known so far
eq2 = eq.subs(res).expand()
unsolved_syms = _unsolved_syms(eq2, sort=True)
if not unsolved_syms:
if res:
newresult, delete_res = _append_new_soln(
res, None, None, imgset_yes, soln_imageset,
original_imageset, newresult, eq2)
if delete_res:
# `delete_res` is true, means substituting `res` in
# eq2 doesn't return `zero` or deleting the `res`
# (a soln) since it staisfies expr of `exclude`
# list.
result.remove(res)
continue # skip as it's independent of desired symbols
depen = eq2.as_independent(unsolved_syms)[0]
if depen.has(Abs) and solver == solveset_complex:
# Absolute values cannot be inverted in the
# complex domain
continue
soln_imageset = {}
for sym in unsolved_syms:
not_solvable = False
try:
soln = solver(eq2, sym)
total_solvest_call += 1
soln_new = S.EmptySet
if isinstance(soln, Complement):
# separate solution and complement
complements[sym] = soln.args[1]
soln = soln.args[0]
# complement will be added at the end
if isinstance(soln, Intersection):
# Interval will be at 0th index always
if soln.args[0] != Interval(-oo, oo):
# sometimes solveset returns soln
# with intersection S.Reals, to confirm that
# soln is in domain=S.Reals
intersections[sym] = soln.args[0]
soln_new += soln.args[1]
soln = soln_new if soln_new else soln
if index > 0 and solver == solveset_real:
# one symbol's real soln , another symbol may have
# corresponding complex soln.
if not isinstance(soln, (ImageSet, ConditionSet)):
soln += solveset_complex(eq2, sym)
except NotImplementedError:
# If sovleset is not able to solve equation `eq2`. Next
# time we may get soln using next equation `eq2`
continue
if isinstance(soln, ConditionSet):
soln = S.EmptySet
# don't do `continue` we may get soln
# in terms of other symbol(s)
not_solvable = True
total_conditionst += 1
if soln is not S.EmptySet:
soln, soln_imageset = _extract_main_soln(
soln, soln_imageset)
for sol in soln:
# sol is not a `Union` since we checked it
# before this loop
sol, soln_imageset = _extract_main_soln(
sol, soln_imageset)
sol = set(sol).pop()
free = sol.free_symbols
if got_symbol and any([
ss in free for ss in got_symbol
]):
# sol depends on previously solved symbols
# then continue
continue
rnew = res.copy()
# put each solution in res and append the new result
# in the new result list (solution for symbol `s`)
# along with old results.
for k, v in res.items():
if isinstance(v, Expr):
# if any unsolved symbol is present
# Then subs known value
rnew[k] = v.subs(sym, sol)
# and add this new solution
if soln_imageset:
# replace all lambda variables with 0.
imgst = soln_imageset[sol]
rnew[sym] = imgst.lamda(
*[0 for i in range(0, len(
imgst.lamda.variables))])
else:
rnew[sym] = sol
newresult, delete_res = _append_new_soln(
rnew, sym, sol, imgset_yes, soln_imageset,
original_imageset, newresult)
if delete_res:
# deleting the `res` (a soln) since it staisfies
# eq of `exclude` list
result.remove(res)
# solution got for sym
if not not_solvable:
got_symbol.add(sym)
# next time use this new soln
if newresult:
result = newresult
return result, total_solvest_call, total_conditionst
# end def _solve_using_know_values()
new_result_real, solve_call1, cnd_call1 = _solve_using_known_values(
old_result, solveset_real)
new_result_complex, solve_call2, cnd_call2 = _solve_using_known_values(
old_result, solveset_complex)
# when `total_solveset_call` is equals to `total_conditionset`
# means solvest fails to solve all the eq.
# return conditionset in this case
total_conditionset += (cnd_call1 + cnd_call2)
total_solveset_call += (solve_call1 + solve_call2)
if total_conditionset == total_solveset_call and total_solveset_call != -1:
return _return_conditionset(eqs_in_better_order, all_symbols)
# overall result
result = new_result_real + new_result_complex
result_all_variables = []
result_infinite = []
for res in result:
if not res:
# means {None : None}
continue
# If length < len(all_symbols) means infinite soln.
# Some or all the soln is dependent on 1 symbol.
# eg. {x: y+2} then final soln {x: y+2, y: y}
if len(res) < len(all_symbols):
solved_symbols = res.keys()
unsolved = list(filter(
lambda x: x not in solved_symbols, all_symbols))
for unsolved_sym in unsolved:
res[unsolved_sym] = unsolved_sym
result_infinite.append(res)
if res not in result_all_variables:
result_all_variables.append(res)
if result_infinite:
# we have general soln
# eg : [{x: -1, y : 1}, {x : -y , y: y}] then
# return [{x : -y, y : y}]
result_all_variables = result_infinite
if intersections and complements:
# no testcase is added for this block
result_all_variables = add_intersection_complement(
result_all_variables, intersections,
Intersection=True, Complement=True)
elif intersections:
result_all_variables = add_intersection_complement(
result_all_variables, intersections, Intersection=True)
elif complements:
result_all_variables = add_intersection_complement(
result_all_variables, complements, Complement=True)
# convert to ordered tuple
result = S.EmptySet
for r in result_all_variables:
temp = [r[symb] for symb in all_symbols]
result += FiniteSet(tuple(temp))
return result
# end of def substitution()
def _solveset_work(system, symbols):
soln = solveset(system[0], symbols[0])
if isinstance(soln, FiniteSet):
_soln = FiniteSet(*[tuple((s,)) for s in soln])
return _soln
else:
return FiniteSet(tuple(FiniteSet(soln)))
def _handle_positive_dimensional(polys, symbols, denominators):
from sympy.polys.polytools import groebner
# substitution method where new system is groebner basis of the system
_symbols = list(symbols)
_symbols.sort(key=default_sort_key)
basis = groebner(polys, _symbols, polys=True)
new_system = []
for poly_eq in basis:
new_system.append(poly_eq.as_expr())
result = [{}]
result = substitution(
new_system, symbols, result, [],
denominators)
return result
# end of def _handle_positive_dimensional()
def _handle_zero_dimensional(polys, symbols, system):
# solve 0 dimensional poly system using `solve_poly_system`
result = solve_poly_system(polys, *symbols)
# May be some extra soln is added because
# we used `unrad` in `_separate_poly_nonpoly`, so
# need to check and remove if it is not a soln.
result_update = S.EmptySet
for res in result:
dict_sym_value = dict(list(zip(symbols, res)))
if all(checksol(eq, dict_sym_value) for eq in system):
result_update += FiniteSet(res)
return result_update
# end of def _handle_zero_dimensional()
def _separate_poly_nonpoly(system, symbols):
polys = []
polys_expr = []
nonpolys = []
denominators = set()
poly = None
for eq in system:
# Store denom expression if it contains symbol
denominators.update(_simple_dens(eq, symbols))
# try to remove sqrt and rational power
without_radicals = unrad(simplify(eq))
if without_radicals:
eq_unrad, cov = without_radicals
if not cov:
eq = eq_unrad
if isinstance(eq, Expr):
eq = eq.as_numer_denom()[0]
poly = eq.as_poly(*symbols, extension=True)
elif simplify(eq).is_number:
continue
if poly is not None:
polys.append(poly)
polys_expr.append(poly.as_expr())
else:
nonpolys.append(eq)
return polys, polys_expr, nonpolys, denominators
# end of def _separate_poly_nonpoly()
def nonlinsolve(system, *symbols):
r"""
Solve system of N non linear equations with M variables, which means both
under and overdetermined systems are supported. Positive dimensional
system is also supported (A system with infinitely many solutions is said
to be positive-dimensional). In Positive dimensional system solution will
be dependent on at least one symbol. Returns both real solution
and complex solution(If system have). The possible number of solutions
is zero, one or infinite.
Parameters
==========
system : list of equations
The target system of equations
symbols : list of Symbols
symbols should be given as a sequence eg. list
Returns
=======
A FiniteSet of ordered tuple of values of `symbols` for which the `system`
has solution. Order of values in the tuple is same as symbols present in
the parameter `symbols`.
Please note that general FiniteSet is unordered, the solution returned
here is not simply a FiniteSet of solutions, rather it is a FiniteSet of
ordered tuple, i.e. the first & only argument to FiniteSet is a tuple of
solutions, which is ordered, & hence the returned solution is ordered.
Also note that solution could also have been returned as an ordered tuple,
FiniteSet is just a wrapper `{}` around the tuple. It has no other
significance except for the fact it is just used to maintain a consistent
output format throughout the solveset.
For the given set of Equations, the respective input types
are given below:
.. math:: x*y - 1 = 0
.. math:: 4*x**2 + y**2 - 5 = 0
`system = [x*y - 1, 4*x**2 + y**2 - 5]`
`symbols = [x, y]`
Raises
======
ValueError
The input is not valid.
The symbols are not given.
AttributeError
The input symbols are not `Symbol` type.
Examples
========
>>> from sympy.core.symbol import symbols
>>> from sympy.solvers.solveset import nonlinsolve
>>> x, y, z = symbols('x, y, z', real=True)
>>> nonlinsolve([x*y - 1, 4*x**2 + y**2 - 5], [x, y])
{(-1, -1), (-1/2, -2), (1/2, 2), (1, 1)}
1. Positive dimensional system and complements:
>>> from sympy import pprint
>>> from sympy.polys.polytools import is_zero_dimensional
>>> a, b, c, d = symbols('a, b, c, d', extended_real=True)
>>> eq1 = a + b + c + d
>>> eq2 = a*b + b*c + c*d + d*a
>>> eq3 = a*b*c + b*c*d + c*d*a + d*a*b
>>> eq4 = a*b*c*d - 1
>>> system = [eq1, eq2, eq3, eq4]
>>> is_zero_dimensional(system)
False
>>> pprint(nonlinsolve(system, [a, b, c, d]), use_unicode=False)
-1 1 1 -1
{(---, -d, -, {d} \ {0}), (-, -d, ---, {d} \ {0})}
d d d d
>>> nonlinsolve([(x+y)**2 - 4, x + y - 2], [x, y])
{(2 - y, y)}
2. If some of the equations are non-polynomial then `nonlinsolve`
will call the `substitution` function and return real and complex solutions,
if present.
>>> from sympy import exp, sin
>>> nonlinsolve([exp(x) - sin(y), y**2 - 4], [x, y])
{(ImageSet(Lambda(_n, I*(2*_n*pi + pi) + log(sin(2))), Integers), -2),
(ImageSet(Lambda(_n, 2*_n*I*pi + log(sin(2))), Integers), 2)}
3. If system is non-linear polynomial and zero-dimensional then it
returns both solution (real and complex solutions, if present) using
`solve_poly_system`:
>>> from sympy import sqrt
>>> nonlinsolve([x**2 - 2*y**2 -2, x*y - 2], [x, y])
{(-2, -1), (2, 1), (-sqrt(2)*I, sqrt(2)*I), (sqrt(2)*I, -sqrt(2)*I)}
4. `nonlinsolve` can solve some linear (zero or positive dimensional)
system (because it uses the `groebner` function to get the
groebner basis and then uses the `substitution` function basis as the
new `system`). But it is not recommended to solve linear system using
`nonlinsolve`, because `linsolve` is better for general linear systems.
>>> nonlinsolve([x + 2*y -z - 3, x - y - 4*z + 9 , y + z - 4], [x, y, z])
{(3*z - 5, 4 - z, z)}
5. System having polynomial equations and only real solution is
solved using `solve_poly_system`:
>>> e1 = sqrt(x**2 + y**2) - 10
>>> e2 = sqrt(y**2 + (-x + 10)**2) - 3
>>> nonlinsolve((e1, e2), (x, y))
{(191/20, -3*sqrt(391)/20), (191/20, 3*sqrt(391)/20)}
>>> nonlinsolve([x**2 + 2/y - 2, x + y - 3], [x, y])
{(1, 2), (1 - sqrt(5), 2 + sqrt(5)), (1 + sqrt(5), 2 - sqrt(5))}
>>> nonlinsolve([x**2 + 2/y - 2, x + y - 3], [y, x])
{(2, 1), (2 - sqrt(5), 1 + sqrt(5)), (2 + sqrt(5), 1 - sqrt(5))}
6. It is better to use symbols instead of Trigonometric Function or
Function (e.g. replace `sin(x)` with symbol, replace `f(x)` with symbol
and so on. Get soln from `nonlinsolve` and then using `solveset` get
the value of `x`)
How nonlinsolve is better than old solver `_solve_system` :
===========================================================
1. A positive dimensional system solver : nonlinsolve can return
solution for positive dimensional system. It finds the
Groebner Basis of the positive dimensional system(calling it as
basis) then we can start solving equation(having least number of
variable first in the basis) using solveset and substituting that
solved solutions into other equation(of basis) to get solution in
terms of minimum variables. Here the important thing is how we
are substituting the known values and in which equations.
2. Real and Complex both solutions : nonlinsolve returns both real
and complex solution. If all the equations in the system are polynomial
then using `solve_poly_system` both real and complex solution is returned.
If all the equations in the system are not polynomial equation then goes to
`substitution` method with this polynomial and non polynomial equation(s),
to solve for unsolved variables. Here to solve for particular variable
solveset_real and solveset_complex is used. For both real and complex
solution function `_solve_using_know_values` is used inside `substitution`
function.(`substitution` function will be called when there is any non
polynomial equation(s) is present). When solution is valid then add its
general solution in the final result.
3. Complement and Intersection will be added if any : nonlinsolve maintains
dict for complements and Intersections. If solveset find complements or/and
Intersection with any Interval or set during the execution of
`substitution` function ,then complement or/and Intersection for that
variable is added before returning final solution.
"""
from sympy.polys.polytools import is_zero_dimensional
if not system:
return S.EmptySet
if not symbols:
msg = ('Symbols must be given, for which solution of the '
'system is to be found.')
raise ValueError(filldedent(msg))
if hasattr(symbols[0], '__iter__'):
symbols = symbols[0]
if not is_sequence(symbols) or not symbols:
msg = ('Symbols must be given, for which solution of the '
'system is to be found.')
raise IndexError(filldedent(msg))
system, symbols, swap = recast_to_symbols(system, symbols)
if swap:
soln = nonlinsolve(system, symbols)
return FiniteSet(*[tuple(i.xreplace(swap) for i in s) for s in soln])
if len(system) == 1 and len(symbols) == 1:
return _solveset_work(system, symbols)
# main code of def nonlinsolve() starts from here
polys, polys_expr, nonpolys, denominators = _separate_poly_nonpoly(
system, symbols)
if len(symbols) == len(polys):
# If all the equations in the system are poly
if is_zero_dimensional(polys, symbols):
# finite number of soln (Zero dimensional system)
try:
return _handle_zero_dimensional(polys, symbols, system)
except NotImplementedError:
# Right now it doesn't fail for any polynomial system of
# equation. If `solve_poly_system` fails then `substitution`
# method will handle it.
result = substitution(
polys_expr, symbols, exclude=denominators)
return result
# positive dimensional system
res = _handle_positive_dimensional(polys, symbols, denominators)
if isinstance(res, EmptySet) and any(not p.domain.is_Exact for p in polys):
raise NotImplementedError("Equation not in exact domain. Try converting to rational")
else:
return res
else:
# If all the equations are not polynomial.
# Use `substitution` method for the system
result = substitution(
polys_expr + nonpolys, symbols, exclude=denominators)
return result
|
29d5da463acf5cf9b2db3d3e46763df7e465a9e9373f0c841fc800a9152306ce | """Tools for solving inequalities and systems of inequalities. """
from __future__ import print_function, division
from sympy.core import Symbol, Dummy, sympify
from sympy.core.compatibility import iterable
from sympy.core.exprtools import factor_terms
from sympy.core.relational import Relational, Eq, Ge, Lt
from sympy.sets import Interval
from sympy.sets.sets import FiniteSet, Union, EmptySet, Intersection
from sympy.core.singleton import S
from sympy.core.function import expand_mul
from sympy.functions import Abs
from sympy.logic import And
from sympy.polys import Poly, PolynomialError, parallel_poly_from_expr
from sympy.polys.polyutils import _nsort
from sympy.utilities.iterables import sift
from sympy.utilities.misc import filldedent
def solve_poly_inequality(poly, rel):
"""Solve a polynomial inequality with rational coefficients.
Examples
========
>>> from sympy import Poly
>>> from sympy.abc import x
>>> from sympy.solvers.inequalities import solve_poly_inequality
>>> solve_poly_inequality(Poly(x, x, domain='ZZ'), '==')
[{0}]
>>> solve_poly_inequality(Poly(x**2 - 1, x, domain='ZZ'), '!=')
[Interval.open(-oo, -1), Interval.open(-1, 1), Interval.open(1, oo)]
>>> solve_poly_inequality(Poly(x**2 - 1, x, domain='ZZ'), '==')
[{-1}, {1}]
See Also
========
solve_poly_inequalities
"""
if not isinstance(poly, Poly):
raise ValueError(
'For efficiency reasons, `poly` should be a Poly instance')
if poly.is_number:
t = Relational(poly.as_expr(), 0, rel)
if t is S.true:
return [S.Reals]
elif t is S.false:
return [S.EmptySet]
else:
raise NotImplementedError(
"could not determine truth value of %s" % t)
reals, intervals = poly.real_roots(multiple=False), []
if rel == '==':
for root, _ in reals:
interval = Interval(root, root)
intervals.append(interval)
elif rel == '!=':
left = S.NegativeInfinity
for right, _ in reals + [(S.Infinity, 1)]:
interval = Interval(left, right, True, True)
intervals.append(interval)
left = right
else:
if poly.LC() > 0:
sign = +1
else:
sign = -1
eq_sign, equal = None, False
if rel == '>':
eq_sign = +1
elif rel == '<':
eq_sign = -1
elif rel == '>=':
eq_sign, equal = +1, True
elif rel == '<=':
eq_sign, equal = -1, True
else:
raise ValueError("'%s' is not a valid relation" % rel)
right, right_open = S.Infinity, True
for left, multiplicity in reversed(reals):
if multiplicity % 2:
if sign == eq_sign:
intervals.insert(
0, Interval(left, right, not equal, right_open))
sign, right, right_open = -sign, left, not equal
else:
if sign == eq_sign and not equal:
intervals.insert(
0, Interval(left, right, True, right_open))
right, right_open = left, True
elif sign != eq_sign and equal:
intervals.insert(0, Interval(left, left))
if sign == eq_sign:
intervals.insert(
0, Interval(S.NegativeInfinity, right, True, right_open))
return intervals
def solve_poly_inequalities(polys):
"""Solve polynomial inequalities with rational coefficients.
Examples
========
>>> from sympy.solvers.inequalities import solve_poly_inequalities
>>> from sympy.polys import Poly
>>> from sympy.abc import x
>>> solve_poly_inequalities(((
... Poly(x**2 - 3), ">"), (
... Poly(-x**2 + 1), ">")))
Union(Interval.open(-oo, -sqrt(3)), Interval.open(-1, 1), Interval.open(sqrt(3), oo))
"""
from sympy import Union
return Union(*[s for p in polys for s in solve_poly_inequality(*p)])
def solve_rational_inequalities(eqs):
"""Solve a system of rational inequalities with rational coefficients.
Examples
========
>>> from sympy.abc import x
>>> from sympy import Poly
>>> from sympy.solvers.inequalities import solve_rational_inequalities
>>> solve_rational_inequalities([[
... ((Poly(-x + 1), Poly(1, x)), '>='),
... ((Poly(-x + 1), Poly(1, x)), '<=')]])
{1}
>>> solve_rational_inequalities([[
... ((Poly(x), Poly(1, x)), '!='),
... ((Poly(-x + 1), Poly(1, x)), '>=')]])
Union(Interval.open(-oo, 0), Interval.Lopen(0, 1))
See Also
========
solve_poly_inequality
"""
result = S.EmptySet
for _eqs in eqs:
if not _eqs:
continue
global_intervals = [Interval(S.NegativeInfinity, S.Infinity)]
for (numer, denom), rel in _eqs:
numer_intervals = solve_poly_inequality(numer*denom, rel)
denom_intervals = solve_poly_inequality(denom, '==')
intervals = []
for numer_interval in numer_intervals:
for global_interval in global_intervals:
interval = numer_interval.intersect(global_interval)
if interval is not S.EmptySet:
intervals.append(interval)
global_intervals = intervals
intervals = []
for global_interval in global_intervals:
for denom_interval in denom_intervals:
global_interval -= denom_interval
if global_interval is not S.EmptySet:
intervals.append(global_interval)
global_intervals = intervals
if not global_intervals:
break
for interval in global_intervals:
result = result.union(interval)
return result
def reduce_rational_inequalities(exprs, gen, relational=True):
"""Reduce a system of rational inequalities with rational coefficients.
Examples
========
>>> from sympy import Poly, Symbol
>>> from sympy.solvers.inequalities import reduce_rational_inequalities
>>> x = Symbol('x', real=True)
>>> reduce_rational_inequalities([[x**2 <= 0]], x)
Eq(x, 0)
>>> reduce_rational_inequalities([[x + 2 > 0]], x)
-2 < x
>>> reduce_rational_inequalities([[(x + 2, ">")]], x)
-2 < x
>>> reduce_rational_inequalities([[x + 2]], x)
Eq(x, -2)
This function find the non-infinite solution set so if the unknown symbol
is declared as extended real rather than real then the result may include
finiteness conditions:
>>> y = Symbol('y', extended_real=True)
>>> reduce_rational_inequalities([[y + 2 > 0]], y)
(-2 < y) & (y < oo)
"""
exact = True
eqs = []
solution = S.Reals if exprs else S.EmptySet
for _exprs in exprs:
_eqs = []
for expr in _exprs:
if isinstance(expr, tuple):
expr, rel = expr
else:
if expr.is_Relational:
expr, rel = expr.lhs - expr.rhs, expr.rel_op
else:
expr, rel = expr, '=='
if expr is S.true:
numer, denom, rel = S.Zero, S.One, '=='
elif expr is S.false:
numer, denom, rel = S.One, S.One, '=='
else:
numer, denom = expr.together().as_numer_denom()
try:
(numer, denom), opt = parallel_poly_from_expr(
(numer, denom), gen)
except PolynomialError:
raise PolynomialError(filldedent('''
only polynomials and rational functions are
supported in this context.
'''))
if not opt.domain.is_Exact:
numer, denom, exact = numer.to_exact(), denom.to_exact(), False
domain = opt.domain.get_exact()
if not (domain.is_ZZ or domain.is_QQ):
expr = numer/denom
expr = Relational(expr, 0, rel)
solution &= solve_univariate_inequality(expr, gen, relational=False)
else:
_eqs.append(((numer, denom), rel))
if _eqs:
eqs.append(_eqs)
if eqs:
solution &= solve_rational_inequalities(eqs)
exclude = solve_rational_inequalities([[((d, d.one), '==')
for i in eqs for ((n, d), _) in i if d.has(gen)]])
solution -= exclude
if not exact and solution:
solution = solution.evalf()
if relational:
solution = solution.as_relational(gen)
return solution
def reduce_abs_inequality(expr, rel, gen):
"""Reduce an inequality with nested absolute values.
Examples
========
>>> from sympy import Abs, Symbol
>>> from sympy.solvers.inequalities import reduce_abs_inequality
>>> x = Symbol('x', real=True)
>>> reduce_abs_inequality(Abs(x - 5) - 3, '<', x)
(2 < x) & (x < 8)
>>> reduce_abs_inequality(Abs(x + 2)*3 - 13, '<', x)
(-19/3 < x) & (x < 7/3)
See Also
========
reduce_abs_inequalities
"""
if gen.is_extended_real is False:
raise TypeError(filldedent('''
can't solve inequalities with absolute values containing
non-real variables.
'''))
def _bottom_up_scan(expr):
exprs = []
if expr.is_Add or expr.is_Mul:
op = expr.func
for arg in expr.args:
_exprs = _bottom_up_scan(arg)
if not exprs:
exprs = _exprs
else:
args = []
for expr, conds in exprs:
for _expr, _conds in _exprs:
args.append((op(expr, _expr), conds + _conds))
exprs = args
elif expr.is_Pow:
n = expr.exp
if not n.is_Integer:
raise ValueError("Only Integer Powers are allowed on Abs.")
_exprs = _bottom_up_scan(expr.base)
for expr, conds in _exprs:
exprs.append((expr**n, conds))
elif isinstance(expr, Abs):
_exprs = _bottom_up_scan(expr.args[0])
for expr, conds in _exprs:
exprs.append(( expr, conds + [Ge(expr, 0)]))
exprs.append((-expr, conds + [Lt(expr, 0)]))
else:
exprs = [(expr, [])]
return exprs
exprs = _bottom_up_scan(expr)
mapping = {'<': '>', '<=': '>='}
inequalities = []
for expr, conds in exprs:
if rel not in mapping.keys():
expr = Relational( expr, 0, rel)
else:
expr = Relational(-expr, 0, mapping[rel])
inequalities.append([expr] + conds)
return reduce_rational_inequalities(inequalities, gen)
def reduce_abs_inequalities(exprs, gen):
"""Reduce a system of inequalities with nested absolute values.
Examples
========
>>> from sympy import Abs, Symbol
>>> from sympy.abc import x
>>> from sympy.solvers.inequalities import reduce_abs_inequalities
>>> x = Symbol('x', extended_real=True)
>>> reduce_abs_inequalities([(Abs(3*x - 5) - 7, '<'),
... (Abs(x + 25) - 13, '>')], x)
(-2/3 < x) & (x < 4) & (((-oo < x) & (x < -38)) | ((-12 < x) & (x < oo)))
>>> reduce_abs_inequalities([(Abs(x - 4) + Abs(3*x - 5) - 7, '<')], x)
(1/2 < x) & (x < 4)
See Also
========
reduce_abs_inequality
"""
return And(*[ reduce_abs_inequality(expr, rel, gen)
for expr, rel in exprs ])
def solve_univariate_inequality(expr, gen, relational=True, domain=S.Reals, continuous=False):
"""Solves a real univariate inequality.
Parameters
==========
expr : Relational
The target inequality
gen : Symbol
The variable for which the inequality is solved
relational : bool
A Relational type output is expected or not
domain : Set
The domain over which the equation is solved
continuous: bool
True if expr is known to be continuous over the given domain
(and so continuous_domain() doesn't need to be called on it)
Raises
======
NotImplementedError
The solution of the inequality cannot be determined due to limitation
in `solvify`.
Notes
=====
Currently, we cannot solve all the inequalities due to limitations in
`solvify`. Also, the solution returned for trigonometric inequalities
are restricted in its periodic interval.
See Also
========
solvify: solver returning solveset solutions with solve's output API
Examples
========
>>> from sympy.solvers.inequalities import solve_univariate_inequality
>>> from sympy import Symbol, sin, Interval, S
>>> x = Symbol('x')
>>> solve_univariate_inequality(x**2 >= 4, x)
((2 <= x) & (x < oo)) | ((x <= -2) & (-oo < x))
>>> solve_univariate_inequality(x**2 >= 4, x, relational=False)
Union(Interval(-oo, -2), Interval(2, oo))
>>> domain = Interval(0, S.Infinity)
>>> solve_univariate_inequality(x**2 >= 4, x, False, domain)
Interval(2, oo)
>>> solve_univariate_inequality(sin(x) > 0, x, relational=False)
Interval.open(0, pi)
"""
from sympy import im
from sympy.calculus.util import (continuous_domain, periodicity,
function_range)
from sympy.solvers.solvers import denoms
from sympy.solvers.solveset import solvify, solveset
# This keeps the function independent of the assumptions about `gen`.
# `solveset` makes sure this function is called only when the domain is
# real.
_gen = gen
_domain = domain
if gen.is_extended_real is False:
rv = S.EmptySet
return rv if not relational else rv.as_relational(_gen)
elif gen.is_extended_real is None:
gen = Dummy('gen', extended_real=True)
try:
expr = expr.xreplace({_gen: gen})
except TypeError:
raise TypeError(filldedent('''
When gen is real, the relational has a complex part
which leads to an invalid comparison like I < 0.
'''))
rv = None
if expr is S.true:
rv = domain
elif expr is S.false:
rv = S.EmptySet
else:
e = expr.lhs - expr.rhs
period = periodicity(e, gen)
if period == S.Zero:
e = expand_mul(e)
const = expr.func(e, 0)
if const is S.true:
rv = domain
elif const is S.false:
rv = S.EmptySet
elif period is not None:
frange = function_range(e, gen, domain)
rel = expr.rel_op
if rel == '<' or rel == '<=':
if expr.func(frange.sup, 0):
rv = domain
elif not expr.func(frange.inf, 0):
rv = S.EmptySet
elif rel == '>' or rel == '>=':
if expr.func(frange.inf, 0):
rv = domain
elif not expr.func(frange.sup, 0):
rv = S.EmptySet
inf, sup = domain.inf, domain.sup
if sup - inf is S.Infinity:
domain = Interval(0, period, False, True)
if rv is None:
n, d = e.as_numer_denom()
try:
if gen not in n.free_symbols and len(e.free_symbols) > 1:
raise ValueError
# this might raise ValueError on its own
# or it might give None...
solns = solvify(e, gen, domain)
if solns is None:
# in which case we raise ValueError
raise ValueError
except (ValueError, NotImplementedError):
# replace gen with generic x since it's
# univariate anyway
raise NotImplementedError(filldedent('''
The inequality, %s, cannot be solved using
solve_univariate_inequality.
''' % expr.subs(gen, Symbol('x'))))
expanded_e = expand_mul(e)
def valid(x):
# this is used to see if gen=x satisfies the
# relational by substituting it into the
# expanded form and testing against 0, e.g.
# if expr = x*(x + 1) < 2 then e = x*(x + 1) - 2
# and expanded_e = x**2 + x - 2; the test is
# whether a given value of x satisfies
# x**2 + x - 2 < 0
#
# expanded_e, expr and gen used from enclosing scope
v = expanded_e.subs(gen, expand_mul(x))
try:
r = expr.func(v, 0)
except TypeError:
r = S.false
if r in (S.true, S.false):
return r
if v.is_extended_real is False:
return S.false
else:
v = v.n(2)
if v.is_comparable:
return expr.func(v, 0)
# not comparable or couldn't be evaluated
raise NotImplementedError(
'relationship did not evaluate: %s' % r)
singularities = []
for d in denoms(expr, gen):
singularities.extend(solvify(d, gen, domain))
if not continuous:
domain = continuous_domain(expanded_e, gen, domain)
include_x = '=' in expr.rel_op and expr.rel_op != '!='
try:
discontinuities = set(domain.boundary -
FiniteSet(domain.inf, domain.sup))
# remove points that are not between inf and sup of domain
critical_points = FiniteSet(*(solns + singularities + list(
discontinuities))).intersection(
Interval(domain.inf, domain.sup,
domain.inf not in domain, domain.sup not in domain))
if all(r.is_number for r in critical_points):
reals = _nsort(critical_points, separated=True)[0]
else:
sifted = sift(critical_points, lambda x: x.is_extended_real)
if sifted[None]:
# there were some roots that weren't known
# to be real
raise NotImplementedError
try:
reals = sifted[True]
if len(reals) > 1:
reals = list(sorted(reals))
except TypeError:
raise NotImplementedError
except NotImplementedError:
raise NotImplementedError('sorting of these roots is not supported')
# If expr contains imaginary coefficients, only take real
# values of x for which the imaginary part is 0
make_real = S.Reals
if im(expanded_e) != S.Zero:
check = True
im_sol = FiniteSet()
try:
a = solveset(im(expanded_e), gen, domain)
if not isinstance(a, Interval):
for z in a:
if z not in singularities and valid(z) and z.is_extended_real:
im_sol += FiniteSet(z)
else:
start, end = a.inf, a.sup
for z in _nsort(critical_points + FiniteSet(end)):
valid_start = valid(start)
if start != end:
valid_z = valid(z)
pt = _pt(start, z)
if pt not in singularities and pt.is_extended_real and valid(pt):
if valid_start and valid_z:
im_sol += Interval(start, z)
elif valid_start:
im_sol += Interval.Ropen(start, z)
elif valid_z:
im_sol += Interval.Lopen(start, z)
else:
im_sol += Interval.open(start, z)
start = z
for s in singularities:
im_sol -= FiniteSet(s)
except (TypeError):
im_sol = S.Reals
check = False
if isinstance(im_sol, EmptySet):
raise ValueError(filldedent('''
%s contains imaginary parts which cannot be
made 0 for any value of %s satisfying the
inequality, leading to relations like I < 0.
''' % (expr.subs(gen, _gen), _gen)))
make_real = make_real.intersect(im_sol)
sol_sets = [S.EmptySet]
start = domain.inf
if valid(start) and start.is_finite:
sol_sets.append(FiniteSet(start))
for x in reals:
end = x
if valid(_pt(start, end)):
sol_sets.append(Interval(start, end, True, True))
if x in singularities:
singularities.remove(x)
else:
if x in discontinuities:
discontinuities.remove(x)
_valid = valid(x)
else: # it's a solution
_valid = include_x
if _valid:
sol_sets.append(FiniteSet(x))
start = end
end = domain.sup
if valid(end) and end.is_finite:
sol_sets.append(FiniteSet(end))
if valid(_pt(start, end)):
sol_sets.append(Interval.open(start, end))
if im(expanded_e) != S.Zero and check:
rv = (make_real).intersect(_domain)
else:
rv = Intersection(
(Union(*sol_sets)), make_real, _domain).subs(gen, _gen)
return rv if not relational else rv.as_relational(_gen)
def _pt(start, end):
"""Return a point between start and end"""
if not start.is_infinite and not end.is_infinite:
pt = (start + end)/2
elif start.is_infinite and end.is_infinite:
pt = S.Zero
else:
if (start.is_infinite and start.is_extended_positive is None or
end.is_infinite and end.is_extended_positive is None):
raise ValueError('cannot proceed with unsigned infinite values')
if (end.is_infinite and end.is_extended_negative or
start.is_infinite and start.is_extended_positive):
start, end = end, start
# if possible, use a multiple of self which has
# better behavior when checking assumptions than
# an expression obtained by adding or subtracting 1
if end.is_infinite:
if start.is_extended_positive:
pt = start*2
elif start.is_extended_negative:
pt = start*S.Half
else:
pt = start + 1
elif start.is_infinite:
if end.is_extended_positive:
pt = end*S.Half
elif end.is_extended_negative:
pt = end*2
else:
pt = end - 1
return pt
def _solve_inequality(ie, s, linear=False):
"""Return the inequality with s isolated on the left, if possible.
If the relationship is non-linear, a solution involving And or Or
may be returned. False or True are returned if the relationship
is never True or always True, respectively.
If `linear` is True (default is False) an `s`-dependent expression
will be isolated on the left, if possible
but it will not be solved for `s` unless the expression is linear
in `s`. Furthermore, only "safe" operations which don't change the
sense of the relationship are applied: no division by an unsigned
value is attempted unless the relationship involves Eq or Ne and
no division by a value not known to be nonzero is ever attempted.
Examples
========
>>> from sympy import Eq, Symbol
>>> from sympy.solvers.inequalities import _solve_inequality as f
>>> from sympy.abc import x, y
For linear expressions, the symbol can be isolated:
>>> f(x - 2 < 0, x)
x < 2
>>> f(-x - 6 < x, x)
x > -3
Sometimes nonlinear relationships will be False
>>> f(x**2 + 4 < 0, x)
False
Or they may involve more than one region of values:
>>> f(x**2 - 4 < 0, x)
(-2 < x) & (x < 2)
To restrict the solution to a relational, set linear=True
and only the x-dependent portion will be isolated on the left:
>>> f(x**2 - 4 < 0, x, linear=True)
x**2 < 4
Division of only nonzero quantities is allowed, so x cannot
be isolated by dividing by y:
>>> y.is_nonzero is None # it is unknown whether it is 0 or not
True
>>> f(x*y < 1, x)
x*y < 1
And while an equality (or inequality) still holds after dividing by a
non-zero quantity
>>> nz = Symbol('nz', nonzero=True)
>>> f(Eq(x*nz, 1), x)
Eq(x, 1/nz)
the sign must be known for other inequalities involving > or <:
>>> f(x*nz <= 1, x)
nz*x <= 1
>>> p = Symbol('p', positive=True)
>>> f(x*p <= 1, x)
x <= 1/p
When there are denominators in the original expression that
are removed by expansion, conditions for them will be returned
as part of the result:
>>> f(x < x*(2/x - 1), x)
(x < 1) & Ne(x, 0)
"""
from sympy.solvers.solvers import denoms
if s not in ie.free_symbols:
return ie
if ie.rhs == s:
ie = ie.reversed
if ie.lhs == s and s not in ie.rhs.free_symbols:
return ie
def classify(ie, s, i):
# return True or False if ie evaluates when substituting s with
# i else None (if unevaluated) or NaN (when there is an error
# in evaluating)
try:
v = ie.subs(s, i)
if v is S.NaN:
return v
elif v not in (True, False):
return
return v
except TypeError:
return S.NaN
rv = None
oo = S.Infinity
expr = ie.lhs - ie.rhs
try:
p = Poly(expr, s)
if p.degree() == 0:
rv = ie.func(p.as_expr(), 0)
elif not linear and p.degree() > 1:
# handle in except clause
raise NotImplementedError
except (PolynomialError, NotImplementedError):
if not linear:
try:
rv = reduce_rational_inequalities([[ie]], s)
except PolynomialError:
rv = solve_univariate_inequality(ie, s)
# remove restrictions wrt +/-oo that may have been
# applied when using sets to simplify the relationship
okoo = classify(ie, s, oo)
if okoo is S.true and classify(rv, s, oo) is S.false:
rv = rv.subs(s < oo, True)
oknoo = classify(ie, s, -oo)
if (oknoo is S.true and
classify(rv, s, -oo) is S.false):
rv = rv.subs(-oo < s, True)
rv = rv.subs(s > -oo, True)
if rv is S.true:
rv = (s <= oo) if okoo is S.true else (s < oo)
if oknoo is not S.true:
rv = And(-oo < s, rv)
else:
p = Poly(expr)
conds = []
if rv is None:
e = p.as_expr() # this is in expanded form
# Do a safe inversion of e, moving non-s terms
# to the rhs and dividing by a nonzero factor if
# the relational is Eq/Ne; for other relationals
# the sign must also be positive or negative
rhs = 0
b, ax = e.as_independent(s, as_Add=True)
e -= b
rhs -= b
ef = factor_terms(e)
a, e = ef.as_independent(s, as_Add=False)
if (a.is_zero != False or # don't divide by potential 0
a.is_negative ==
a.is_positive is None and # if sign is not known then
ie.rel_op not in ('!=', '==')): # reject if not Eq/Ne
e = ef
a = S.One
rhs /= a
if a.is_positive:
rv = ie.func(e, rhs)
else:
rv = ie.reversed.func(e, rhs)
# return conditions under which the value is
# valid, too.
beginning_denoms = denoms(ie.lhs) | denoms(ie.rhs)
current_denoms = denoms(rv)
for d in beginning_denoms - current_denoms:
c = _solve_inequality(Eq(d, 0), s, linear=linear)
if isinstance(c, Eq) and c.lhs == s:
if classify(rv, s, c.rhs) is S.true:
# rv is permitting this value but it shouldn't
conds.append(~c)
for i in (-oo, oo):
if (classify(rv, s, i) is S.true and
classify(ie, s, i) is not S.true):
conds.append(s < i if i is oo else i < s)
conds.append(rv)
return And(*conds)
def _reduce_inequalities(inequalities, symbols):
# helper for reduce_inequalities
poly_part, abs_part = {}, {}
other = []
for inequality in inequalities:
expr, rel = inequality.lhs, inequality.rel_op # rhs is 0
# check for gens using atoms which is more strict than free_symbols to
# guard against EX domain which won't be handled by
# reduce_rational_inequalities
gens = expr.atoms(Symbol)
if len(gens) == 1:
gen = gens.pop()
else:
common = expr.free_symbols & symbols
if len(common) == 1:
gen = common.pop()
other.append(_solve_inequality(Relational(expr, 0, rel), gen))
continue
else:
raise NotImplementedError(filldedent('''
inequality has more than one symbol of interest.
'''))
if expr.is_polynomial(gen):
poly_part.setdefault(gen, []).append((expr, rel))
else:
components = expr.find(lambda u:
u.has(gen) and (
u.is_Function or u.is_Pow and not u.exp.is_Integer))
if components and all(isinstance(i, Abs) for i in components):
abs_part.setdefault(gen, []).append((expr, rel))
else:
other.append(_solve_inequality(Relational(expr, 0, rel), gen))
poly_reduced = []
abs_reduced = []
for gen, exprs in poly_part.items():
poly_reduced.append(reduce_rational_inequalities([exprs], gen))
for gen, exprs in abs_part.items():
abs_reduced.append(reduce_abs_inequalities(exprs, gen))
return And(*(poly_reduced + abs_reduced + other))
def reduce_inequalities(inequalities, symbols=[]):
"""Reduce a system of inequalities with rational coefficients.
Examples
========
>>> from sympy import sympify as S, Symbol
>>> from sympy.abc import x, y
>>> from sympy.solvers.inequalities import reduce_inequalities
>>> reduce_inequalities(0 <= x + 3, [])
(-3 <= x) & (x < oo)
>>> reduce_inequalities(0 <= x + y*2 - 1, [x])
(x < oo) & (x >= 1 - 2*y)
"""
if not iterable(inequalities):
inequalities = [inequalities]
inequalities = [sympify(i) for i in inequalities]
gens = set().union(*[i.free_symbols for i in inequalities])
if not iterable(symbols):
symbols = [symbols]
symbols = (set(symbols) or gens) & gens
if any(i.is_extended_real is False for i in symbols):
raise TypeError(filldedent('''
inequalities cannot contain symbols that are not real.
'''))
# make vanilla symbol real
recast = {i: Dummy(i.name, extended_real=True)
for i in gens if i.is_extended_real is None}
inequalities = [i.xreplace(recast) for i in inequalities]
symbols = {i.xreplace(recast) for i in symbols}
# prefilter
keep = []
for i in inequalities:
if isinstance(i, Relational):
i = i.func(i.lhs.as_expr() - i.rhs.as_expr(), 0)
elif i not in (True, False):
i = Eq(i, 0)
if i == True:
continue
elif i == False:
return S.false
if i.lhs.is_number:
raise NotImplementedError(
"could not determine truth value of %s" % i)
keep.append(i)
inequalities = keep
del keep
# solve system
rv = _reduce_inequalities(inequalities, symbols)
# restore original symbols and return
return rv.xreplace({v: k for k, v in recast.items()})
|
88a62674d27131b7c16903f732a57b54e845ef4ed9ab109f9edab289dc856d69 | from __future__ import print_function, division
from sympy.core.add import Add
from sympy.core.compatibility import as_int, is_sequence, range
from sympy.core.exprtools import factor_terms
from sympy.core.function import _mexpand
from sympy.core.mul import Mul
from sympy.core.numbers import Rational
from sympy.core.numbers import igcdex, ilcm, igcd
from sympy.core.power import integer_nthroot, isqrt
from sympy.core.relational import Eq
from sympy.core.singleton import S
from sympy.core.symbol import Symbol, symbols
from sympy.functions.elementary.complexes import sign
from sympy.functions.elementary.integers import floor
from sympy.functions.elementary.miscellaneous import sqrt
from sympy.matrices.dense import MutableDenseMatrix as Matrix
from sympy.ntheory.factor_ import (
divisors, factorint, multiplicity, perfect_power)
from sympy.ntheory.generate import nextprime
from sympy.ntheory.primetest import is_square, isprime
from sympy.ntheory.residue_ntheory import sqrt_mod
from sympy.polys.polyerrors import GeneratorsNeeded
from sympy.polys.polytools import Poly, factor_list
from sympy.simplify.simplify import signsimp
from sympy.solvers.solvers import check_assumptions
from sympy.solvers.solveset import solveset_real
from sympy.utilities import default_sort_key, numbered_symbols
from sympy.utilities.misc import filldedent
# these are imported with 'from sympy.solvers.diophantine import *
__all__ = ['diophantine', 'classify_diop']
# these types are known (but not necessarily handled)
diop_known = {
"binary_quadratic",
"cubic_thue",
"general_pythagorean",
"general_sum_of_even_powers",
"general_sum_of_squares",
"homogeneous_general_quadratic",
"homogeneous_ternary_quadratic",
"homogeneous_ternary_quadratic_normal",
"inhomogeneous_general_quadratic",
"inhomogeneous_ternary_quadratic",
"linear",
"univariate"}
def _is_int(i):
try:
as_int(i)
return True
except ValueError:
pass
def _sorted_tuple(*i):
return tuple(sorted(i))
def _remove_gcd(*x):
try:
g = igcd(*x)
except ValueError:
fx = list(filter(None, x))
if len(fx) < 2:
return x
g = igcd(*[i.as_content_primitive()[0] for i in fx])
except TypeError:
raise TypeError('_remove_gcd(a,b,c) or _remove_gcd(*container)')
if g == 1:
return x
return tuple([i//g for i in x])
def _rational_pq(a, b):
# return `(numer, denom)` for a/b; sign in numer and gcd removed
return _remove_gcd(sign(b)*a, abs(b))
def _nint_or_floor(p, q):
# return nearest int to p/q; in case of tie return floor(p/q)
w, r = divmod(p, q)
if abs(r) <= abs(q)//2:
return w
return w + 1
def _odd(i):
return i % 2 != 0
def _even(i):
return i % 2 == 0
def diophantine(eq, param=symbols("t", integer=True), syms=None,
permute=False):
"""
Simplify the solution procedure of diophantine equation ``eq`` by
converting it into a product of terms which should equal zero.
For example, when solving, `x^2 - y^2 = 0` this is treated as
`(x + y)(x - y) = 0` and `x + y = 0` and `x - y = 0` are solved
independently and combined. Each term is solved by calling
``diop_solve()``. (Although it is possible to call ``diop_solve()``
directly, one must be careful to pass an equation in the correct
form and to interpret the output correctly; ``diophantine()`` is
the public-facing function to use in general.)
Output of ``diophantine()`` is a set of tuples. The elements of the
tuple are the solutions for each variable in the equation and
are arranged according to the alphabetic ordering of the variables.
e.g. For an equation with two variables, `a` and `b`, the first
element of the tuple is the solution for `a` and the second for `b`.
Usage
=====
``diophantine(eq, t, syms)``: Solve the diophantine
equation ``eq``.
``t`` is the optional parameter to be used by ``diop_solve()``.
``syms`` is an optional list of symbols which determines the
order of the elements in the returned tuple.
By default, only the base solution is returned. If ``permute`` is set to
True then permutations of the base solution and/or permutations of the
signs of the values will be returned when applicable.
>>> from sympy.solvers.diophantine import diophantine
>>> from sympy.abc import a, b
>>> eq = a**4 + b**4 - (2**4 + 3**4)
>>> diophantine(eq)
{(2, 3)}
>>> diophantine(eq, permute=True)
{(-3, -2), (-3, 2), (-2, -3), (-2, 3), (2, -3), (2, 3), (3, -2), (3, 2)}
Details
=======
``eq`` should be an expression which is assumed to be zero.
``t`` is the parameter to be used in the solution.
Examples
========
>>> from sympy.abc import x, y, z
>>> diophantine(x**2 - y**2)
{(t_0, -t_0), (t_0, t_0)}
>>> diophantine(x*(2*x + 3*y - z))
{(0, n1, n2), (t_0, t_1, 2*t_0 + 3*t_1)}
>>> diophantine(x**2 + 3*x*y + 4*x)
{(0, n1), (3*t_0 - 4, -t_0)}
See Also
========
diop_solve()
sympy.utilities.iterables.permute_signs
sympy.utilities.iterables.signed_permutations
"""
from sympy.utilities.iterables import (
subsets, permute_signs, signed_permutations)
if isinstance(eq, Eq):
eq = eq.lhs - eq.rhs
try:
var = list(eq.expand(force=True).free_symbols)
var.sort(key=default_sort_key)
if syms:
if not is_sequence(syms):
raise TypeError(
'syms should be given as a sequence, e.g. a list')
syms = [i for i in syms if i in var]
if syms != var:
dict_sym_index = dict(zip(syms, range(len(syms))))
return {tuple([t[dict_sym_index[i]] for i in var])
for t in diophantine(eq, param)}
n, d = eq.as_numer_denom()
if n.is_number:
return set()
if not d.is_number:
dsol = diophantine(d)
good = diophantine(n) - dsol
return {s for s in good if _mexpand(d.subs(zip(var, s)))}
else:
eq = n
eq = factor_terms(eq)
assert not eq.is_number
eq = eq.as_independent(*var, as_Add=False)[1]
p = Poly(eq)
assert not any(g.is_number for g in p.gens)
eq = p.as_expr()
assert eq.is_polynomial()
except (GeneratorsNeeded, AssertionError, AttributeError):
raise TypeError(filldedent('''
Equation should be a polynomial with Rational coefficients.'''))
# permute only sign
do_permute_signs = False
# permute sign and values
do_permute_signs_var = False
# permute few signs
permute_few_signs = False
try:
# if we know that factoring should not be attempted, skip
# the factoring step
v, c, t = classify_diop(eq)
# check for permute sign
if permute:
len_var = len(v)
permute_signs_for = [
'general_sum_of_squares',
'general_sum_of_even_powers']
permute_signs_check = [
'homogeneous_ternary_quadratic',
'homogeneous_ternary_quadratic_normal',
'binary_quadratic']
if t in permute_signs_for:
do_permute_signs_var = True
elif t in permute_signs_check:
# if all the variables in eq have even powers
# then do_permute_sign = True
if len_var == 3:
var_mul = list(subsets(v, 2))
# here var_mul is like [(x, y), (x, z), (y, z)]
xy_coeff = True
x_coeff = True
var1_mul_var2 = map(lambda a: a[0]*a[1], var_mul)
# if coeff(y*z), coeff(y*x), coeff(x*z) is not 0 then
# `xy_coeff` => True and do_permute_sign => False.
# Means no permuted solution.
for v1_mul_v2 in var1_mul_var2:
try:
coeff = c[v1_mul_v2]
except KeyError:
coeff = 0
xy_coeff = bool(xy_coeff) and bool(coeff)
var_mul = list(subsets(v, 1))
# here var_mul is like [(x,), (y, )]
for v1 in var_mul:
try:
coeff = c[v1[0]]
except KeyError:
coeff = 0
x_coeff = bool(x_coeff) and bool(coeff)
if not any([xy_coeff, x_coeff]):
# means only x**2, y**2, z**2, const is present
do_permute_signs = True
elif not x_coeff:
permute_few_signs = True
elif len_var == 2:
var_mul = list(subsets(v, 2))
# here var_mul is like [(x, y)]
xy_coeff = True
x_coeff = True
var1_mul_var2 = map(lambda x: x[0]*x[1], var_mul)
for v1_mul_v2 in var1_mul_var2:
try:
coeff = c[v1_mul_v2]
except KeyError:
coeff = 0
xy_coeff = bool(xy_coeff) and bool(coeff)
var_mul = list(subsets(v, 1))
# here var_mul is like [(x,), (y, )]
for v1 in var_mul:
try:
coeff = c[v1[0]]
except KeyError:
coeff = 0
x_coeff = bool(x_coeff) and bool(coeff)
if not any([xy_coeff, x_coeff]):
# means only x**2, y**2 and const is present
# so we can get more soln by permuting this soln.
do_permute_signs = True
elif not x_coeff:
# when coeff(x), coeff(y) is not present then signs of
# x, y can be permuted such that their sign are same
# as sign of x*y.
# e.g 1. (x_val,y_val)=> (x_val,y_val), (-x_val,-y_val)
# 2. (-x_vall, y_val)=> (-x_val,y_val), (x_val,-y_val)
permute_few_signs = True
if t == 'general_sum_of_squares':
# trying to factor such expressions will sometimes hang
terms = [(eq, 1)]
else:
raise TypeError
except (TypeError, NotImplementedError):
terms = factor_list(eq)[1]
sols = set([])
for term in terms:
base, _ = term
var_t, _, eq_type = classify_diop(base, _dict=False)
_, base = signsimp(base, evaluate=False).as_coeff_Mul()
solution = diop_solve(base, param)
if eq_type in [
"linear",
"homogeneous_ternary_quadratic",
"homogeneous_ternary_quadratic_normal",
"general_pythagorean"]:
sols.add(merge_solution(var, var_t, solution))
elif eq_type in [
"binary_quadratic",
"general_sum_of_squares",
"general_sum_of_even_powers",
"univariate"]:
for sol in solution:
sols.add(merge_solution(var, var_t, sol))
else:
raise NotImplementedError('unhandled type: %s' % eq_type)
# remove null merge results
if () in sols:
sols.remove(())
null = tuple([0]*len(var))
# if there is no solution, return trivial solution
if not sols and eq.subs(zip(var, null)).is_zero:
sols.add(null)
final_soln = set([])
for sol in sols:
if all(_is_int(s) for s in sol):
if do_permute_signs:
permuted_sign = set(permute_signs(sol))
final_soln.update(permuted_sign)
elif permute_few_signs:
lst = list(permute_signs(sol))
lst = list(filter(lambda x: x[0]*x[1] == sol[1]*sol[0], lst))
permuted_sign = set(lst)
final_soln.update(permuted_sign)
elif do_permute_signs_var:
permuted_sign_var = set(signed_permutations(sol))
final_soln.update(permuted_sign_var)
else:
final_soln.add(sol)
else:
final_soln.add(sol)
return final_soln
def merge_solution(var, var_t, solution):
"""
This is used to construct the full solution from the solutions of sub
equations.
For example when solving the equation `(x - y)(x^2 + y^2 - z^2) = 0`,
solutions for each of the equations `x - y = 0` and `x^2 + y^2 - z^2` are
found independently. Solutions for `x - y = 0` are `(x, y) = (t, t)`. But
we should introduce a value for z when we output the solution for the
original equation. This function converts `(t, t)` into `(t, t, n_{1})`
where `n_{1}` is an integer parameter.
"""
sol = []
if None in solution:
return ()
solution = iter(solution)
params = numbered_symbols("n", integer=True, start=1)
for v in var:
if v in var_t:
sol.append(next(solution))
else:
sol.append(next(params))
for val, symb in zip(sol, var):
if check_assumptions(val, **symb.assumptions0) is False:
return tuple()
return tuple(sol)
def diop_solve(eq, param=symbols("t", integer=True)):
"""
Solves the diophantine equation ``eq``.
Unlike ``diophantine()``, factoring of ``eq`` is not attempted. Uses
``classify_diop()`` to determine the type of the equation and calls
the appropriate solver function.
Use of ``diophantine()`` is recommended over other helper functions.
``diop_solve()`` can return either a set or a tuple depending on the
nature of the equation.
Usage
=====
``diop_solve(eq, t)``: Solve diophantine equation, ``eq`` using ``t``
as a parameter if needed.
Details
=======
``eq`` should be an expression which is assumed to be zero.
``t`` is a parameter to be used in the solution.
Examples
========
>>> from sympy.solvers.diophantine import diop_solve
>>> from sympy.abc import x, y, z, w
>>> diop_solve(2*x + 3*y - 5)
(3*t_0 - 5, 5 - 2*t_0)
>>> diop_solve(4*x + 3*y - 4*z + 5)
(t_0, 8*t_0 + 4*t_1 + 5, 7*t_0 + 3*t_1 + 5)
>>> diop_solve(x + 3*y - 4*z + w - 6)
(t_0, t_0 + t_1, 6*t_0 + 5*t_1 + 4*t_2 - 6, 5*t_0 + 4*t_1 + 3*t_2 - 6)
>>> diop_solve(x**2 + y**2 - 5)
{(-2, -1), (-2, 1), (-1, -2), (-1, 2), (1, -2), (1, 2), (2, -1), (2, 1)}
See Also
========
diophantine()
"""
var, coeff, eq_type = classify_diop(eq, _dict=False)
if eq_type == "linear":
return _diop_linear(var, coeff, param)
elif eq_type == "binary_quadratic":
return _diop_quadratic(var, coeff, param)
elif eq_type == "homogeneous_ternary_quadratic":
x_0, y_0, z_0 = _diop_ternary_quadratic(var, coeff)
return _parametrize_ternary_quadratic(
(x_0, y_0, z_0), var, coeff)
elif eq_type == "homogeneous_ternary_quadratic_normal":
x_0, y_0, z_0 = _diop_ternary_quadratic_normal(var, coeff)
return _parametrize_ternary_quadratic(
(x_0, y_0, z_0), var, coeff)
elif eq_type == "general_pythagorean":
return _diop_general_pythagorean(var, coeff, param)
elif eq_type == "univariate":
return set([(int(i),) for i in solveset_real(
eq, var[0]).intersect(S.Integers)])
elif eq_type == "general_sum_of_squares":
return _diop_general_sum_of_squares(var, -int(coeff[1]), limit=S.Infinity)
elif eq_type == "general_sum_of_even_powers":
for k in coeff.keys():
if k.is_Pow and coeff[k]:
p = k.exp
return _diop_general_sum_of_even_powers(var, p, -int(coeff[1]), limit=S.Infinity)
if eq_type is not None and eq_type not in diop_known:
raise ValueError(filldedent('''
Alhough this type of equation was identified, it is not yet
handled. It should, however, be listed in `diop_known` at the
top of this file. Developers should see comments at the end of
`classify_diop`.
''')) # pragma: no cover
else:
raise NotImplementedError(
'No solver has been written for %s.' % eq_type)
def classify_diop(eq, _dict=True):
# docstring supplied externally
try:
var = list(eq.free_symbols)
assert var
except (AttributeError, AssertionError):
raise ValueError('equation should have 1 or more free symbols')
var.sort(key=default_sort_key)
eq = eq.expand(force=True)
coeff = eq.as_coefficients_dict()
if not all(_is_int(c) for c in coeff.values()):
raise TypeError("Coefficients should be Integers")
diop_type = None
total_degree = Poly(eq).total_degree()
homogeneous = 1 not in coeff
if total_degree == 1:
diop_type = "linear"
elif len(var) == 1:
diop_type = "univariate"
elif total_degree == 2 and len(var) == 2:
diop_type = "binary_quadratic"
elif total_degree == 2 and len(var) == 3 and homogeneous:
if set(coeff) & set(var):
diop_type = "inhomogeneous_ternary_quadratic"
else:
nonzero = [k for k in coeff if coeff[k]]
if len(nonzero) == 3 and all(i**2 in nonzero for i in var):
diop_type = "homogeneous_ternary_quadratic_normal"
else:
diop_type = "homogeneous_ternary_quadratic"
elif total_degree == 2 and len(var) >= 3:
if set(coeff) & set(var):
diop_type = "inhomogeneous_general_quadratic"
else:
# there may be Pow keys like x**2 or Mul keys like x*y
if any(k.is_Mul for k in coeff): # cross terms
if not homogeneous:
diop_type = "inhomogeneous_general_quadratic"
else:
diop_type = "homogeneous_general_quadratic"
else: # all squares: x**2 + y**2 + ... + constant
if all(coeff[k] == 1 for k in coeff if k != 1):
diop_type = "general_sum_of_squares"
elif all(is_square(abs(coeff[k])) for k in coeff):
if abs(sum(sign(coeff[k]) for k in coeff)) == \
len(var) - 2:
# all but one has the same sign
# e.g. 4*x**2 + y**2 - 4*z**2
diop_type = "general_pythagorean"
elif total_degree == 3 and len(var) == 2:
diop_type = "cubic_thue"
elif (total_degree > 3 and total_degree % 2 == 0 and
all(k.is_Pow and k.exp == total_degree for k in coeff if k != 1)):
if all(coeff[k] == 1 for k in coeff if k != 1):
diop_type = 'general_sum_of_even_powers'
if diop_type is not None:
return var, dict(coeff) if _dict else coeff, diop_type
# new diop type instructions
# --------------------------
# if this error raises and the equation *can* be classified,
# * it should be identified in the if-block above
# * the type should be added to the diop_known
# if a solver can be written for it,
# * a dedicated handler should be written (e.g. diop_linear)
# * it should be passed to that handler in diop_solve
raise NotImplementedError(filldedent('''
This equation is not yet recognized or else has not been
simplified sufficiently to put it in a form recognized by
diop_classify().'''))
classify_diop.func_doc = '''
Helper routine used by diop_solve() to find information about ``eq``.
Returns a tuple containing the type of the diophantine equation
along with the variables (free symbols) and their coefficients.
Variables are returned as a list and coefficients are returned
as a dict with the key being the respective term and the constant
term is keyed to 1. The type is one of the following:
* %s
Usage
=====
``classify_diop(eq)``: Return variables, coefficients and type of the
``eq``.
Details
=======
``eq`` should be an expression which is assumed to be zero.
``_dict`` is for internal use: when True (default) a dict is returned,
otherwise a defaultdict which supplies 0 for missing keys is returned.
Examples
========
>>> from sympy.solvers.diophantine import classify_diop
>>> from sympy.abc import x, y, z, w, t
>>> classify_diop(4*x + 6*y - 4)
([x, y], {1: -4, x: 4, y: 6}, 'linear')
>>> classify_diop(x + 3*y -4*z + 5)
([x, y, z], {1: 5, x: 1, y: 3, z: -4}, 'linear')
>>> classify_diop(x**2 + y**2 - x*y + x + 5)
([x, y], {1: 5, x: 1, x**2: 1, y**2: 1, x*y: -1}, 'binary_quadratic')
''' % ('\n * '.join(sorted(diop_known)))
def diop_linear(eq, param=symbols("t", integer=True)):
"""
Solves linear diophantine equations.
A linear diophantine equation is an equation of the form `a_{1}x_{1} +
a_{2}x_{2} + .. + a_{n}x_{n} = 0` where `a_{1}, a_{2}, ..a_{n}` are
integer constants and `x_{1}, x_{2}, ..x_{n}` are integer variables.
Usage
=====
``diop_linear(eq)``: Returns a tuple containing solutions to the
diophantine equation ``eq``. Values in the tuple is arranged in the same
order as the sorted variables.
Details
=======
``eq`` is a linear diophantine equation which is assumed to be zero.
``param`` is the parameter to be used in the solution.
Examples
========
>>> from sympy.solvers.diophantine import diop_linear
>>> from sympy.abc import x, y, z, t
>>> diop_linear(2*x - 3*y - 5) # solves equation 2*x - 3*y - 5 == 0
(3*t_0 - 5, 2*t_0 - 5)
Here x = -3*t_0 - 5 and y = -2*t_0 - 5
>>> diop_linear(2*x - 3*y - 4*z -3)
(t_0, 2*t_0 + 4*t_1 + 3, -t_0 - 3*t_1 - 3)
See Also
========
diop_quadratic(), diop_ternary_quadratic(), diop_general_pythagorean(),
diop_general_sum_of_squares()
"""
var, coeff, diop_type = classify_diop(eq, _dict=False)
if diop_type == "linear":
return _diop_linear(var, coeff, param)
def _diop_linear(var, coeff, param):
"""
Solves diophantine equations of the form:
a_0*x_0 + a_1*x_1 + ... + a_n*x_n == c
Note that no solution exists if gcd(a_0, ..., a_n) doesn't divide c.
"""
if 1 in coeff:
# negate coeff[] because input is of the form: ax + by + c == 0
# but is used as: ax + by == -c
c = -coeff[1]
else:
c = 0
# Some solutions will have multiple free variables in their solutions.
if param is None:
params = [symbols('t')]*len(var)
else:
temp = str(param) + "_%i"
params = [symbols(temp % i, integer=True) for i in range(len(var))]
if len(var) == 1:
q, r = divmod(c, coeff[var[0]])
if not r:
return (q,)
else:
return (None,)
'''
base_solution_linear() can solve diophantine equations of the form:
a*x + b*y == c
We break down multivariate linear diophantine equations into a
series of bivariate linear diophantine equations which can then
be solved individually by base_solution_linear().
Consider the following:
a_0*x_0 + a_1*x_1 + a_2*x_2 == c
which can be re-written as:
a_0*x_0 + g_0*y_0 == c
where
g_0 == gcd(a_1, a_2)
and
y == (a_1*x_1)/g_0 + (a_2*x_2)/g_0
This leaves us with two binary linear diophantine equations.
For the first equation:
a == a_0
b == g_0
c == c
For the second:
a == a_1/g_0
b == a_2/g_0
c == the solution we find for y_0 in the first equation.
The arrays A and B are the arrays of integers used for
'a' and 'b' in each of the n-1 bivariate equations we solve.
'''
A = [coeff[v] for v in var]
B = []
if len(var) > 2:
B.append(igcd(A[-2], A[-1]))
A[-2] = A[-2] // B[0]
A[-1] = A[-1] // B[0]
for i in range(len(A) - 3, 0, -1):
gcd = igcd(B[0], A[i])
B[0] = B[0] // gcd
A[i] = A[i] // gcd
B.insert(0, gcd)
B.append(A[-1])
'''
Consider the trivariate linear equation:
4*x_0 + 6*x_1 + 3*x_2 == 2
This can be re-written as:
4*x_0 + 3*y_0 == 2
where
y_0 == 2*x_1 + x_2
(Note that gcd(3, 6) == 3)
The complete integral solution to this equation is:
x_0 == 2 + 3*t_0
y_0 == -2 - 4*t_0
where 't_0' is any integer.
Now that we have a solution for 'x_0', find 'x_1' and 'x_2':
2*x_1 + x_2 == -2 - 4*t_0
We can then solve for '-2' and '-4' independently,
and combine the results:
2*x_1a + x_2a == -2
x_1a == 0 + t_0
x_2a == -2 - 2*t_0
2*x_1b + x_2b == -4*t_0
x_1b == 0*t_0 + t_1
x_2b == -4*t_0 - 2*t_1
==>
x_1 == t_0 + t_1
x_2 == -2 - 6*t_0 - 2*t_1
where 't_0' and 't_1' are any integers.
Note that:
4*(2 + 3*t_0) + 6*(t_0 + t_1) + 3*(-2 - 6*t_0 - 2*t_1) == 2
for any integral values of 't_0', 't_1'; as required.
This method is generalised for many variables, below.
'''
solutions = []
for i in range(len(B)):
tot_x, tot_y = [], []
for j, arg in enumerate(Add.make_args(c)):
if arg.is_Integer:
# example: 5 -> k = 5
k, p = arg, S.One
pnew = params[0]
else: # arg is a Mul or Symbol
# example: 3*t_1 -> k = 3
# example: t_0 -> k = 1
k, p = arg.as_coeff_Mul()
pnew = params[params.index(p) + 1]
sol = sol_x, sol_y = base_solution_linear(k, A[i], B[i], pnew)
if p is S.One:
if None in sol:
return tuple([None]*len(var))
else:
# convert a + b*pnew -> a*p + b*pnew
if isinstance(sol_x, Add):
sol_x = sol_x.args[0]*p + sol_x.args[1]
if isinstance(sol_y, Add):
sol_y = sol_y.args[0]*p + sol_y.args[1]
tot_x.append(sol_x)
tot_y.append(sol_y)
solutions.append(Add(*tot_x))
c = Add(*tot_y)
solutions.append(c)
if param is None:
# just keep the additive constant (i.e. replace t with 0)
solutions = [i.as_coeff_Add()[0] for i in solutions]
return tuple(solutions)
def base_solution_linear(c, a, b, t=None):
"""
Return the base solution for the linear equation, `ax + by = c`.
Used by ``diop_linear()`` to find the base solution of a linear
Diophantine equation. If ``t`` is given then the parametrized solution is
returned.
Usage
=====
``base_solution_linear(c, a, b, t)``: ``a``, ``b``, ``c`` are coefficients
in `ax + by = c` and ``t`` is the parameter to be used in the solution.
Examples
========
>>> from sympy.solvers.diophantine import base_solution_linear
>>> from sympy.abc import t
>>> base_solution_linear(5, 2, 3) # equation 2*x + 3*y = 5
(-5, 5)
>>> base_solution_linear(0, 5, 7) # equation 5*x + 7*y = 0
(0, 0)
>>> base_solution_linear(5, 2, 3, t) # equation 2*x + 3*y = 5
(3*t - 5, 5 - 2*t)
>>> base_solution_linear(0, 5, 7, t) # equation 5*x + 7*y = 0
(7*t, -5*t)
"""
a, b, c = _remove_gcd(a, b, c)
if c == 0:
if t is not None:
if b < 0:
t = -t
return (b*t , -a*t)
else:
return (0, 0)
else:
x0, y0, d = igcdex(abs(a), abs(b))
x0 *= sign(a)
y0 *= sign(b)
if divisible(c, d):
if t is not None:
if b < 0:
t = -t
return (c*x0 + b*t, c*y0 - a*t)
else:
return (c*x0, c*y0)
else:
return (None, None)
def divisible(a, b):
"""
Returns `True` if ``a`` is divisible by ``b`` and `False` otherwise.
"""
return not a % b
def diop_quadratic(eq, param=symbols("t", integer=True)):
"""
Solves quadratic diophantine equations.
i.e. equations of the form `Ax^2 + Bxy + Cy^2 + Dx + Ey + F = 0`. Returns a
set containing the tuples `(x, y)` which contains the solutions. If there
are no solutions then `(None, None)` is returned.
Usage
=====
``diop_quadratic(eq, param)``: ``eq`` is a quadratic binary diophantine
equation. ``param`` is used to indicate the parameter to be used in the
solution.
Details
=======
``eq`` should be an expression which is assumed to be zero.
``param`` is a parameter to be used in the solution.
Examples
========
>>> from sympy.abc import x, y, t
>>> from sympy.solvers.diophantine import diop_quadratic
>>> diop_quadratic(x**2 + y**2 + 2*x + 2*y + 2, t)
{(-1, -1)}
References
==========
.. [1] Methods to solve Ax^2 + Bxy + Cy^2 + Dx + Ey + F = 0, [online],
Available: http://www.alpertron.com.ar/METHODS.HTM
.. [2] Solving the equation ax^2+ bxy + cy^2 + dx + ey + f= 0, [online],
Available: http://www.jpr2718.org/ax2p.pdf
See Also
========
diop_linear(), diop_ternary_quadratic(), diop_general_sum_of_squares(),
diop_general_pythagorean()
"""
var, coeff, diop_type = classify_diop(eq, _dict=False)
if diop_type == "binary_quadratic":
return _diop_quadratic(var, coeff, param)
def _diop_quadratic(var, coeff, t):
x, y = var
A = coeff[x**2]
B = coeff[x*y]
C = coeff[y**2]
D = coeff[x]
E = coeff[y]
F = coeff[1]
A, B, C, D, E, F = [as_int(i) for i in _remove_gcd(A, B, C, D, E, F)]
# (1) Simple-Hyperbolic case: A = C = 0, B != 0
# In this case equation can be converted to (Bx + E)(By + D) = DE - BF
# We consider two cases; DE - BF = 0 and DE - BF != 0
# More details, http://www.alpertron.com.ar/METHODS.HTM#SHyperb
sol = set([])
discr = B**2 - 4*A*C
if A == 0 and C == 0 and B != 0:
if D*E - B*F == 0:
q, r = divmod(E, B)
if not r:
sol.add((-q, t))
q, r = divmod(D, B)
if not r:
sol.add((t, -q))
else:
div = divisors(D*E - B*F)
div = div + [-term for term in div]
for d in div:
x0, r = divmod(d - E, B)
if not r:
q, r = divmod(D*E - B*F, d)
if not r:
y0, r = divmod(q - D, B)
if not r:
sol.add((x0, y0))
# (2) Parabolic case: B**2 - 4*A*C = 0
# There are two subcases to be considered in this case.
# sqrt(c)D - sqrt(a)E = 0 and sqrt(c)D - sqrt(a)E != 0
# More Details, http://www.alpertron.com.ar/METHODS.HTM#Parabol
elif discr == 0:
if A == 0:
s = _diop_quadratic([y, x], coeff, t)
for soln in s:
sol.add((soln[1], soln[0]))
else:
g = sign(A)*igcd(A, C)
a = A // g
c = C // g
e = sign(B/A)
sqa = isqrt(a)
sqc = isqrt(c)
_c = e*sqc*D - sqa*E
if not _c:
z = symbols("z", real=True)
eq = sqa*g*z**2 + D*z + sqa*F
roots = solveset_real(eq, z).intersect(S.Integers)
for root in roots:
ans = diop_solve(sqa*x + e*sqc*y - root)
sol.add((ans[0], ans[1]))
elif _is_int(c):
solve_x = lambda u: -e*sqc*g*_c*t**2 - (E + 2*e*sqc*g*u)*t\
- (e*sqc*g*u**2 + E*u + e*sqc*F) // _c
solve_y = lambda u: sqa*g*_c*t**2 + (D + 2*sqa*g*u)*t \
+ (sqa*g*u**2 + D*u + sqa*F) // _c
for z0 in range(0, abs(_c)):
# Check if the coefficients of y and x obtained are integers or not
if (divisible(sqa*g*z0**2 + D*z0 + sqa*F, _c) and
divisible(e*sqc**g*z0**2 + E*z0 + e*sqc*F, _c)):
sol.add((solve_x(z0), solve_y(z0)))
# (3) Method used when B**2 - 4*A*C is a square, is described in p. 6 of the below paper
# by John P. Robertson.
# http://www.jpr2718.org/ax2p.pdf
elif is_square(discr):
if A != 0:
r = sqrt(discr)
u, v = symbols("u, v", integer=True)
eq = _mexpand(
4*A*r*u*v + 4*A*D*(B*v + r*u + r*v - B*u) +
2*A*4*A*E*(u - v) + 4*A*r*4*A*F)
solution = diop_solve(eq, t)
for s0, t0 in solution:
num = B*t0 + r*s0 + r*t0 - B*s0
x_0 = S(num)/(4*A*r)
y_0 = S(s0 - t0)/(2*r)
if isinstance(s0, Symbol) or isinstance(t0, Symbol):
if check_param(x_0, y_0, 4*A*r, t) != (None, None):
ans = check_param(x_0, y_0, 4*A*r, t)
sol.add((ans[0], ans[1]))
elif x_0.is_Integer and y_0.is_Integer:
if is_solution_quad(var, coeff, x_0, y_0):
sol.add((x_0, y_0))
else:
s = _diop_quadratic(var[::-1], coeff, t) # Interchange x and y
while s: # |
sol.add(s.pop()[::-1]) # and solution <--------+
# (4) B**2 - 4*A*C > 0 and B**2 - 4*A*C not a square or B**2 - 4*A*C < 0
else:
P, Q = _transformation_to_DN(var, coeff)
D, N = _find_DN(var, coeff)
solns_pell = diop_DN(D, N)
if D < 0:
for x0, y0 in solns_pell:
for x in [-x0, x0]:
for y in [-y0, y0]:
s = P*Matrix([x, y]) + Q
try:
sol.add(tuple([as_int(_) for _ in s]))
except ValueError:
pass
else:
# In this case equation can be transformed into a Pell equation
solns_pell = set(solns_pell)
for X, Y in list(solns_pell):
solns_pell.add((-X, -Y))
a = diop_DN(D, 1)
T = a[0][0]
U = a[0][1]
if all(_is_int(_) for _ in P[:4] + Q[:2]):
for r, s in solns_pell:
_a = (r + s*sqrt(D))*(T + U*sqrt(D))**t
_b = (r - s*sqrt(D))*(T - U*sqrt(D))**t
x_n = _mexpand(S(_a + _b)/2)
y_n = _mexpand(S(_a - _b)/(2*sqrt(D)))
s = P*Matrix([x_n, y_n]) + Q
sol.add(tuple(s))
else:
L = ilcm(*[_.q for _ in P[:4] + Q[:2]])
k = 1
T_k = T
U_k = U
while (T_k - 1) % L != 0 or U_k % L != 0:
T_k, U_k = T_k*T + D*U_k*U, T_k*U + U_k*T
k += 1
for X, Y in solns_pell:
for i in range(k):
if all(_is_int(_) for _ in P*Matrix([X, Y]) + Q):
_a = (X + sqrt(D)*Y)*(T_k + sqrt(D)*U_k)**t
_b = (X - sqrt(D)*Y)*(T_k - sqrt(D)*U_k)**t
Xt = S(_a + _b)/2
Yt = S(_a - _b)/(2*sqrt(D))
s = P*Matrix([Xt, Yt]) + Q
sol.add(tuple(s))
X, Y = X*T + D*U*Y, X*U + Y*T
return sol
def is_solution_quad(var, coeff, u, v):
"""
Check whether `(u, v)` is solution to the quadratic binary diophantine
equation with the variable list ``var`` and coefficient dictionary
``coeff``.
Not intended for use by normal users.
"""
reps = dict(zip(var, (u, v)))
eq = Add(*[j*i.xreplace(reps) for i, j in coeff.items()])
return _mexpand(eq) == 0
def diop_DN(D, N, t=symbols("t", integer=True)):
"""
Solves the equation `x^2 - Dy^2 = N`.
Mainly concerned with the case `D > 0, D` is not a perfect square,
which is the same as the generalized Pell equation. The LMM
algorithm [1]_ is used to solve this equation.
Returns one solution tuple, (`x, y)` for each class of the solutions.
Other solutions of the class can be constructed according to the
values of ``D`` and ``N``.
Usage
=====
``diop_DN(D, N, t)``: D and N are integers as in `x^2 - Dy^2 = N` and
``t`` is the parameter to be used in the solutions.
Details
=======
``D`` and ``N`` correspond to D and N in the equation.
``t`` is the parameter to be used in the solutions.
Examples
========
>>> from sympy.solvers.diophantine import diop_DN
>>> diop_DN(13, -4) # Solves equation x**2 - 13*y**2 = -4
[(3, 1), (393, 109), (36, 10)]
The output can be interpreted as follows: There are three fundamental
solutions to the equation `x^2 - 13y^2 = -4` given by (3, 1), (393, 109)
and (36, 10). Each tuple is in the form (x, y), i.e. solution (3, 1) means
that `x = 3` and `y = 1`.
>>> diop_DN(986, 1) # Solves equation x**2 - 986*y**2 = 1
[(49299, 1570)]
See Also
========
find_DN(), diop_bf_DN()
References
==========
.. [1] Solving the generalized Pell equation x**2 - D*y**2 = N, John P.
Robertson, July 31, 2004, Pages 16 - 17. [online], Available:
http://www.jpr2718.org/pell.pdf
"""
if D < 0:
if N == 0:
return [(0, 0)]
elif N < 0:
return []
elif N > 0:
sol = []
for d in divisors(square_factor(N)):
sols = cornacchia(1, -D, N // d**2)
if sols:
for x, y in sols:
sol.append((d*x, d*y))
if D == -1:
sol.append((d*y, d*x))
return sol
elif D == 0:
if N < 0:
return []
if N == 0:
return [(0, t)]
sN, _exact = integer_nthroot(N, 2)
if _exact:
return [(sN, t)]
else:
return []
else: # D > 0
sD, _exact = integer_nthroot(D, 2)
if _exact:
if N == 0:
return [(sD*t, t)]
else:
sol = []
for y in range(floor(sign(N)*(N - 1)/(2*sD)) + 1):
try:
sq, _exact = integer_nthroot(D*y**2 + N, 2)
except ValueError:
_exact = False
if _exact:
sol.append((sq, y))
return sol
elif 1 < N**2 < D:
# It is much faster to call `_special_diop_DN`.
return _special_diop_DN(D, N)
else:
if N == 0:
return [(0, 0)]
elif abs(N) == 1:
pqa = PQa(0, 1, D)
j = 0
G = []
B = []
for i in pqa:
a = i[2]
G.append(i[5])
B.append(i[4])
if j != 0 and a == 2*sD:
break
j = j + 1
if _odd(j):
if N == -1:
x = G[j - 1]
y = B[j - 1]
else:
count = j
while count < 2*j - 1:
i = next(pqa)
G.append(i[5])
B.append(i[4])
count += 1
x = G[count]
y = B[count]
else:
if N == 1:
x = G[j - 1]
y = B[j - 1]
else:
return []
return [(x, y)]
else:
fs = []
sol = []
div = divisors(N)
for d in div:
if divisible(N, d**2):
fs.append(d)
for f in fs:
m = N // f**2
zs = sqrt_mod(D, abs(m), all_roots=True)
zs = [i for i in zs if i <= abs(m) // 2 ]
if abs(m) != 2:
zs = zs + [-i for i in zs if i] # omit dupl 0
for z in zs:
pqa = PQa(z, abs(m), D)
j = 0
G = []
B = []
for i in pqa:
G.append(i[5])
B.append(i[4])
if j != 0 and abs(i[1]) == 1:
r = G[j-1]
s = B[j-1]
if r**2 - D*s**2 == m:
sol.append((f*r, f*s))
elif diop_DN(D, -1) != []:
a = diop_DN(D, -1)
sol.append((f*(r*a[0][0] + a[0][1]*s*D), f*(r*a[0][1] + s*a[0][0])))
break
j = j + 1
if j == length(z, abs(m), D):
break
return sol
def _special_diop_DN(D, N):
"""
Solves the equation `x^2 - Dy^2 = N` for the special case where
`1 < N**2 < D` and `D` is not a perfect square.
It is better to call `diop_DN` rather than this function, as
the former checks the condition `1 < N**2 < D`, and calls the latter only
if appropriate.
Usage
=====
WARNING: Internal method. Do not call directly!
``_special_diop_DN(D, N)``: D and N are integers as in `x^2 - Dy^2 = N`.
Details
=======
``D`` and ``N`` correspond to D and N in the equation.
Examples
========
>>> from sympy.solvers.diophantine import _special_diop_DN
>>> _special_diop_DN(13, -3) # Solves equation x**2 - 13*y**2 = -3
[(7, 2), (137, 38)]
The output can be interpreted as follows: There are two fundamental
solutions to the equation `x^2 - 13y^2 = -3` given by (7, 2) and
(137, 38). Each tuple is in the form (x, y), i.e. solution (7, 2) means
that `x = 7` and `y = 2`.
>>> _special_diop_DN(2445, -20) # Solves equation x**2 - 2445*y**2 = -20
[(445, 9), (17625560, 356454), (698095554475, 14118073569)]
See Also
========
diop_DN()
References
==========
.. [1] Section 4.4.4 of the following book:
Quadratic Diophantine Equations, T. Andreescu and D. Andrica,
Springer, 2015.
"""
# The following assertion was removed for efficiency, with the understanding
# that this method is not called directly. The parent method, `diop_DN`
# is responsible for performing the appropriate checks.
#
# assert (1 < N**2 < D) and (not integer_nthroot(D, 2)[1])
sqrt_D = sqrt(D)
F = [(N, 1)]
f = 2
while True:
f2 = f**2
if f2 > abs(N):
break
n, r = divmod(N, f2)
if r == 0:
F.append((n, f))
f += 1
P = 0
Q = 1
G0, G1 = 0, 1
B0, B1 = 1, 0
solutions = []
i = 0
while True:
a = floor((P + sqrt_D) / Q)
P = a*Q - P
Q = (D - P**2) // Q
G2 = a*G1 + G0
B2 = a*B1 + B0
for n, f in F:
if G2**2 - D*B2**2 == n:
solutions.append((f*G2, f*B2))
i += 1
if Q == 1 and i % 2 == 0:
break
G0, G1 = G1, G2
B0, B1 = B1, B2
return solutions
def cornacchia(a, b, m):
r"""
Solves `ax^2 + by^2 = m` where `\gcd(a, b) = 1 = gcd(a, m)` and `a, b > 0`.
Uses the algorithm due to Cornacchia. The method only finds primitive
solutions, i.e. ones with `\gcd(x, y) = 1`. So this method can't be used to
find the solutions of `x^2 + y^2 = 20` since the only solution to former is
`(x, y) = (4, 2)` and it is not primitive. When `a = b`, only the
solutions with `x \leq y` are found. For more details, see the References.
Examples
========
>>> from sympy.solvers.diophantine import cornacchia
>>> cornacchia(2, 3, 35) # equation 2x**2 + 3y**2 = 35
{(2, 3), (4, 1)}
>>> cornacchia(1, 1, 25) # equation x**2 + y**2 = 25
{(4, 3)}
References
===========
.. [1] A. Nitaj, "L'algorithme de Cornacchia"
.. [2] Solving the diophantine equation ax**2 + by**2 = m by Cornacchia's
method, [online], Available:
http://www.numbertheory.org/php/cornacchia.html
See Also
========
sympy.utilities.iterables.signed_permutations
"""
sols = set()
a1 = igcdex(a, m)[0]
v = sqrt_mod(-b*a1, m, all_roots=True)
if not v:
return None
for t in v:
if t < m // 2:
continue
u, r = t, m
while True:
u, r = r, u % r
if a*r**2 < m:
break
m1 = m - a*r**2
if m1 % b == 0:
m1 = m1 // b
s, _exact = integer_nthroot(m1, 2)
if _exact:
if a == b and r < s:
r, s = s, r
sols.add((int(r), int(s)))
return sols
def PQa(P_0, Q_0, D):
r"""
Returns useful information needed to solve the Pell equation.
There are six sequences of integers defined related to the continued
fraction representation of `\\frac{P + \sqrt{D}}{Q}`, namely {`P_{i}`},
{`Q_{i}`}, {`a_{i}`},{`A_{i}`}, {`B_{i}`}, {`G_{i}`}. ``PQa()`` Returns
these values as a 6-tuple in the same order as mentioned above. Refer [1]_
for more detailed information.
Usage
=====
``PQa(P_0, Q_0, D)``: ``P_0``, ``Q_0`` and ``D`` are integers corresponding
to `P_{0}`, `Q_{0}` and `D` in the continued fraction
`\\frac{P_{0} + \sqrt{D}}{Q_{0}}`.
Also it's assumed that `P_{0}^2 == D mod(|Q_{0}|)` and `D` is square free.
Examples
========
>>> from sympy.solvers.diophantine import PQa
>>> pqa = PQa(13, 4, 5) # (13 + sqrt(5))/4
>>> next(pqa) # (P_0, Q_0, a_0, A_0, B_0, G_0)
(13, 4, 3, 3, 1, -1)
>>> next(pqa) # (P_1, Q_1, a_1, A_1, B_1, G_1)
(-1, 1, 1, 4, 1, 3)
References
==========
.. [1] Solving the generalized Pell equation x^2 - Dy^2 = N, John P.
Robertson, July 31, 2004, Pages 4 - 8. http://www.jpr2718.org/pell.pdf
"""
A_i_2 = B_i_1 = 0
A_i_1 = B_i_2 = 1
G_i_2 = -P_0
G_i_1 = Q_0
P_i = P_0
Q_i = Q_0
while True:
a_i = floor((P_i + sqrt(D))/Q_i)
A_i = a_i*A_i_1 + A_i_2
B_i = a_i*B_i_1 + B_i_2
G_i = a_i*G_i_1 + G_i_2
yield P_i, Q_i, a_i, A_i, B_i, G_i
A_i_1, A_i_2 = A_i, A_i_1
B_i_1, B_i_2 = B_i, B_i_1
G_i_1, G_i_2 = G_i, G_i_1
P_i = a_i*Q_i - P_i
Q_i = (D - P_i**2)/Q_i
def diop_bf_DN(D, N, t=symbols("t", integer=True)):
r"""
Uses brute force to solve the equation, `x^2 - Dy^2 = N`.
Mainly concerned with the generalized Pell equation which is the case when
`D > 0, D` is not a perfect square. For more information on the case refer
[1]_. Let `(t, u)` be the minimal positive solution of the equation
`x^2 - Dy^2 = 1`. Then this method requires
`\sqrt{\\frac{\mid N \mid (t \pm 1)}{2D}}` to be small.
Usage
=====
``diop_bf_DN(D, N, t)``: ``D`` and ``N`` are coefficients in
`x^2 - Dy^2 = N` and ``t`` is the parameter to be used in the solutions.
Details
=======
``D`` and ``N`` correspond to D and N in the equation.
``t`` is the parameter to be used in the solutions.
Examples
========
>>> from sympy.solvers.diophantine import diop_bf_DN
>>> diop_bf_DN(13, -4)
[(3, 1), (-3, 1), (36, 10)]
>>> diop_bf_DN(986, 1)
[(49299, 1570)]
See Also
========
diop_DN()
References
==========
.. [1] Solving the generalized Pell equation x**2 - D*y**2 = N, John P.
Robertson, July 31, 2004, Page 15. http://www.jpr2718.org/pell.pdf
"""
D = as_int(D)
N = as_int(N)
sol = []
a = diop_DN(D, 1)
u = a[0][0]
if abs(N) == 1:
return diop_DN(D, N)
elif N > 1:
L1 = 0
L2 = integer_nthroot(int(N*(u - 1)/(2*D)), 2)[0] + 1
elif N < -1:
L1, _exact = integer_nthroot(-int(N/D), 2)
if not _exact:
L1 += 1
L2 = integer_nthroot(-int(N*(u + 1)/(2*D)), 2)[0] + 1
else: # N = 0
if D < 0:
return [(0, 0)]
elif D == 0:
return [(0, t)]
else:
sD, _exact = integer_nthroot(D, 2)
if _exact:
return [(sD*t, t), (-sD*t, t)]
else:
return [(0, 0)]
for y in range(L1, L2):
try:
x, _exact = integer_nthroot(N + D*y**2, 2)
except ValueError:
_exact = False
if _exact:
sol.append((x, y))
if not equivalent(x, y, -x, y, D, N):
sol.append((-x, y))
return sol
def equivalent(u, v, r, s, D, N):
"""
Returns True if two solutions `(u, v)` and `(r, s)` of `x^2 - Dy^2 = N`
belongs to the same equivalence class and False otherwise.
Two solutions `(u, v)` and `(r, s)` to the above equation fall to the same
equivalence class iff both `(ur - Dvs)` and `(us - vr)` are divisible by
`N`. See reference [1]_. No test is performed to test whether `(u, v)` and
`(r, s)` are actually solutions to the equation. User should take care of
this.
Usage
=====
``equivalent(u, v, r, s, D, N)``: `(u, v)` and `(r, s)` are two solutions
of the equation `x^2 - Dy^2 = N` and all parameters involved are integers.
Examples
========
>>> from sympy.solvers.diophantine import equivalent
>>> equivalent(18, 5, -18, -5, 13, -1)
True
>>> equivalent(3, 1, -18, 393, 109, -4)
False
References
==========
.. [1] Solving the generalized Pell equation x**2 - D*y**2 = N, John P.
Robertson, July 31, 2004, Page 12. http://www.jpr2718.org/pell.pdf
"""
return divisible(u*r - D*v*s, N) and divisible(u*s - v*r, N)
def length(P, Q, D):
r"""
Returns the (length of aperiodic part + length of periodic part) of
continued fraction representation of `\\frac{P + \sqrt{D}}{Q}`.
It is important to remember that this does NOT return the length of the
periodic part but the sum of the lengths of the two parts as mentioned
above.
Usage
=====
``length(P, Q, D)``: ``P``, ``Q`` and ``D`` are integers corresponding to
the continued fraction `\\frac{P + \sqrt{D}}{Q}`.
Details
=======
``P``, ``D`` and ``Q`` corresponds to P, D and Q in the continued fraction,
`\\frac{P + \sqrt{D}}{Q}`.
Examples
========
>>> from sympy.solvers.diophantine import length
>>> length(-2 , 4, 5) # (-2 + sqrt(5))/4
3
>>> length(-5, 4, 17) # (-5 + sqrt(17))/4
4
See Also
========
sympy.ntheory.continued_fraction.continued_fraction_periodic
"""
from sympy.ntheory.continued_fraction import continued_fraction_periodic
v = continued_fraction_periodic(P, Q, D)
if type(v[-1]) is list:
rpt = len(v[-1])
nonrpt = len(v) - 1
else:
rpt = 0
nonrpt = len(v)
return rpt + nonrpt
def transformation_to_DN(eq):
"""
This function transforms general quadratic,
`ax^2 + bxy + cy^2 + dx + ey + f = 0`
to more easy to deal with `X^2 - DY^2 = N` form.
This is used to solve the general quadratic equation by transforming it to
the latter form. Refer [1]_ for more detailed information on the
transformation. This function returns a tuple (A, B) where A is a 2 X 2
matrix and B is a 2 X 1 matrix such that,
Transpose([x y]) = A * Transpose([X Y]) + B
Usage
=====
``transformation_to_DN(eq)``: where ``eq`` is the quadratic to be
transformed.
Examples
========
>>> from sympy.abc import x, y
>>> from sympy.solvers.diophantine import transformation_to_DN
>>> from sympy.solvers.diophantine import classify_diop
>>> A, B = transformation_to_DN(x**2 - 3*x*y - y**2 - 2*y + 1)
>>> A
Matrix([
[1/26, 3/26],
[ 0, 1/13]])
>>> B
Matrix([
[-6/13],
[-4/13]])
A, B returned are such that Transpose((x y)) = A * Transpose((X Y)) + B.
Substituting these values for `x` and `y` and a bit of simplifying work
will give an equation of the form `x^2 - Dy^2 = N`.
>>> from sympy.abc import X, Y
>>> from sympy import Matrix, simplify
>>> u = (A*Matrix([X, Y]) + B)[0] # Transformation for x
>>> u
X/26 + 3*Y/26 - 6/13
>>> v = (A*Matrix([X, Y]) + B)[1] # Transformation for y
>>> v
Y/13 - 4/13
Next we will substitute these formulas for `x` and `y` and do
``simplify()``.
>>> eq = simplify((x**2 - 3*x*y - y**2 - 2*y + 1).subs(zip((x, y), (u, v))))
>>> eq
X**2/676 - Y**2/52 + 17/13
By multiplying the denominator appropriately, we can get a Pell equation
in the standard form.
>>> eq * 676
X**2 - 13*Y**2 + 884
If only the final equation is needed, ``find_DN()`` can be used.
See Also
========
find_DN()
References
==========
.. [1] Solving the equation ax^2 + bxy + cy^2 + dx + ey + f = 0,
John P.Robertson, May 8, 2003, Page 7 - 11.
http://www.jpr2718.org/ax2p.pdf
"""
var, coeff, diop_type = classify_diop(eq, _dict=False)
if diop_type == "binary_quadratic":
return _transformation_to_DN(var, coeff)
def _transformation_to_DN(var, coeff):
x, y = var
a = coeff[x**2]
b = coeff[x*y]
c = coeff[y**2]
d = coeff[x]
e = coeff[y]
f = coeff[1]
a, b, c, d, e, f = [as_int(i) for i in _remove_gcd(a, b, c, d, e, f)]
X, Y = symbols("X, Y", integer=True)
if b:
B, C = _rational_pq(2*a, b)
A, T = _rational_pq(a, B**2)
# eq_1 = A*B*X**2 + B*(c*T - A*C**2)*Y**2 + d*T*X + (B*e*T - d*T*C)*Y + f*T*B
coeff = {X**2: A*B, X*Y: 0, Y**2: B*(c*T - A*C**2), X: d*T, Y: B*e*T - d*T*C, 1: f*T*B}
A_0, B_0 = _transformation_to_DN([X, Y], coeff)
return Matrix(2, 2, [S.One/B, -S(C)/B, 0, 1])*A_0, Matrix(2, 2, [S.One/B, -S(C)/B, 0, 1])*B_0
else:
if d:
B, C = _rational_pq(2*a, d)
A, T = _rational_pq(a, B**2)
# eq_2 = A*X**2 + c*T*Y**2 + e*T*Y + f*T - A*C**2
coeff = {X**2: A, X*Y: 0, Y**2: c*T, X: 0, Y: e*T, 1: f*T - A*C**2}
A_0, B_0 = _transformation_to_DN([X, Y], coeff)
return Matrix(2, 2, [S.One/B, 0, 0, 1])*A_0, Matrix(2, 2, [S.One/B, 0, 0, 1])*B_0 + Matrix([-S(C)/B, 0])
else:
if e:
B, C = _rational_pq(2*c, e)
A, T = _rational_pq(c, B**2)
# eq_3 = a*T*X**2 + A*Y**2 + f*T - A*C**2
coeff = {X**2: a*T, X*Y: 0, Y**2: A, X: 0, Y: 0, 1: f*T - A*C**2}
A_0, B_0 = _transformation_to_DN([X, Y], coeff)
return Matrix(2, 2, [1, 0, 0, S.One/B])*A_0, Matrix(2, 2, [1, 0, 0, S.One/B])*B_0 + Matrix([0, -S(C)/B])
else:
# TODO: pre-simplification: Not necessary but may simplify
# the equation.
return Matrix(2, 2, [S.One/a, 0, 0, 1]), Matrix([0, 0])
def find_DN(eq):
"""
This function returns a tuple, `(D, N)` of the simplified form,
`x^2 - Dy^2 = N`, corresponding to the general quadratic,
`ax^2 + bxy + cy^2 + dx + ey + f = 0`.
Solving the general quadratic is then equivalent to solving the equation
`X^2 - DY^2 = N` and transforming the solutions by using the transformation
matrices returned by ``transformation_to_DN()``.
Usage
=====
``find_DN(eq)``: where ``eq`` is the quadratic to be transformed.
Examples
========
>>> from sympy.abc import x, y
>>> from sympy.solvers.diophantine import find_DN
>>> find_DN(x**2 - 3*x*y - y**2 - 2*y + 1)
(13, -884)
Interpretation of the output is that we get `X^2 -13Y^2 = -884` after
transforming `x^2 - 3xy - y^2 - 2y + 1` using the transformation returned
by ``transformation_to_DN()``.
See Also
========
transformation_to_DN()
References
==========
.. [1] Solving the equation ax^2 + bxy + cy^2 + dx + ey + f = 0,
John P.Robertson, May 8, 2003, Page 7 - 11.
http://www.jpr2718.org/ax2p.pdf
"""
var, coeff, diop_type = classify_diop(eq, _dict=False)
if diop_type == "binary_quadratic":
return _find_DN(var, coeff)
def _find_DN(var, coeff):
x, y = var
X, Y = symbols("X, Y", integer=True)
A, B = _transformation_to_DN(var, coeff)
u = (A*Matrix([X, Y]) + B)[0]
v = (A*Matrix([X, Y]) + B)[1]
eq = x**2*coeff[x**2] + x*y*coeff[x*y] + y**2*coeff[y**2] + x*coeff[x] + y*coeff[y] + coeff[1]
simplified = _mexpand(eq.subs(zip((x, y), (u, v))))
coeff = simplified.as_coefficients_dict()
return -coeff[Y**2]/coeff[X**2], -coeff[1]/coeff[X**2]
def check_param(x, y, a, t):
"""
If there is a number modulo ``a`` such that ``x`` and ``y`` are both
integers, then return a parametric representation for ``x`` and ``y``
else return (None, None).
Here ``x`` and ``y`` are functions of ``t``.
"""
from sympy.simplify.simplify import clear_coefficients
if x.is_number and not x.is_Integer:
return (None, None)
if y.is_number and not y.is_Integer:
return (None, None)
m, n = symbols("m, n", integer=True)
c, p = (m*x + n*y).as_content_primitive()
if a % c.q:
return (None, None)
# clear_coefficients(mx + b, R)[1] -> (R - b)/m
eq = clear_coefficients(x, m)[1] - clear_coefficients(y, n)[1]
junk, eq = eq.as_content_primitive()
return diop_solve(eq, t)
def diop_ternary_quadratic(eq):
"""
Solves the general quadratic ternary form,
`ax^2 + by^2 + cz^2 + fxy + gyz + hxz = 0`.
Returns a tuple `(x, y, z)` which is a base solution for the above
equation. If there are no solutions, `(None, None, None)` is returned.
Usage
=====
``diop_ternary_quadratic(eq)``: Return a tuple containing a basic solution
to ``eq``.
Details
=======
``eq`` should be an homogeneous expression of degree two in three variables
and it is assumed to be zero.
Examples
========
>>> from sympy.abc import x, y, z
>>> from sympy.solvers.diophantine import diop_ternary_quadratic
>>> diop_ternary_quadratic(x**2 + 3*y**2 - z**2)
(1, 0, 1)
>>> diop_ternary_quadratic(4*x**2 + 5*y**2 - z**2)
(1, 0, 2)
>>> diop_ternary_quadratic(45*x**2 - 7*y**2 - 8*x*y - z**2)
(28, 45, 105)
>>> diop_ternary_quadratic(x**2 - 49*y**2 - z**2 + 13*z*y -8*x*y)
(9, 1, 5)
"""
var, coeff, diop_type = classify_diop(eq, _dict=False)
if diop_type in (
"homogeneous_ternary_quadratic",
"homogeneous_ternary_quadratic_normal"):
return _diop_ternary_quadratic(var, coeff)
def _diop_ternary_quadratic(_var, coeff):
x, y, z = _var
var = [x, y, z]
# Equations of the form B*x*y + C*z*x + E*y*z = 0 and At least two of the
# coefficients A, B, C are non-zero.
# There are infinitely many solutions for the equation.
# Ex: (0, 0, t), (0, t, 0), (t, 0, 0)
# Equation can be re-written as y*(B*x + E*z) = -C*x*z and we can find rather
# unobvious solutions. Set y = -C and B*x + E*z = x*z. The latter can be solved by
# using methods for binary quadratic diophantine equations. Let's select the
# solution which minimizes |x| + |z|
if not any(coeff[i**2] for i in var):
if coeff[x*z]:
sols = diophantine(coeff[x*y]*x + coeff[y*z]*z - x*z)
s = sols.pop()
min_sum = abs(s[0]) + abs(s[1])
for r in sols:
m = abs(r[0]) + abs(r[1])
if m < min_sum:
s = r
min_sum = m
x_0, y_0, z_0 = _remove_gcd(s[0], -coeff[x*z], s[1])
else:
var[0], var[1] = _var[1], _var[0]
y_0, x_0, z_0 = _diop_ternary_quadratic(var, coeff)
return x_0, y_0, z_0
if coeff[x**2] == 0:
# If the coefficient of x is zero change the variables
if coeff[y**2] == 0:
var[0], var[2] = _var[2], _var[0]
z_0, y_0, x_0 = _diop_ternary_quadratic(var, coeff)
else:
var[0], var[1] = _var[1], _var[0]
y_0, x_0, z_0 = _diop_ternary_quadratic(var, coeff)
else:
if coeff[x*y] or coeff[x*z]:
# Apply the transformation x --> X - (B*y + C*z)/(2*A)
A = coeff[x**2]
B = coeff[x*y]
C = coeff[x*z]
D = coeff[y**2]
E = coeff[y*z]
F = coeff[z**2]
_coeff = dict()
_coeff[x**2] = 4*A**2
_coeff[y**2] = 4*A*D - B**2
_coeff[z**2] = 4*A*F - C**2
_coeff[y*z] = 4*A*E - 2*B*C
_coeff[x*y] = 0
_coeff[x*z] = 0
x_0, y_0, z_0 = _diop_ternary_quadratic(var, _coeff)
if x_0 is None:
return (None, None, None)
p, q = _rational_pq(B*y_0 + C*z_0, 2*A)
x_0, y_0, z_0 = x_0*q - p, y_0*q, z_0*q
elif coeff[z*y] != 0:
if coeff[y**2] == 0:
if coeff[z**2] == 0:
# Equations of the form A*x**2 + E*yz = 0.
A = coeff[x**2]
E = coeff[y*z]
b, a = _rational_pq(-E, A)
x_0, y_0, z_0 = b, a, b
else:
# Ax**2 + E*y*z + F*z**2 = 0
var[0], var[2] = _var[2], _var[0]
z_0, y_0, x_0 = _diop_ternary_quadratic(var, coeff)
else:
# A*x**2 + D*y**2 + E*y*z + F*z**2 = 0, C may be zero
var[0], var[1] = _var[1], _var[0]
y_0, x_0, z_0 = _diop_ternary_quadratic(var, coeff)
else:
# Ax**2 + D*y**2 + F*z**2 = 0, C may be zero
x_0, y_0, z_0 = _diop_ternary_quadratic_normal(var, coeff)
return _remove_gcd(x_0, y_0, z_0)
def transformation_to_normal(eq):
"""
Returns the transformation Matrix that converts a general ternary
quadratic equation `eq` (`ax^2 + by^2 + cz^2 + dxy + eyz + fxz`)
to a form without cross terms: `ax^2 + by^2 + cz^2 = 0`. This is
not used in solving ternary quadratics; it is only implemented for
the sake of completeness.
"""
var, coeff, diop_type = classify_diop(eq, _dict=False)
if diop_type in (
"homogeneous_ternary_quadratic",
"homogeneous_ternary_quadratic_normal"):
return _transformation_to_normal(var, coeff)
def _transformation_to_normal(var, coeff):
_var = list(var) # copy
x, y, z = var
if not any(coeff[i**2] for i in var):
# https://math.stackexchange.com/questions/448051/transform-quadratic-ternary-form-to-normal-form/448065#448065
a = coeff[x*y]
b = coeff[y*z]
c = coeff[x*z]
swap = False
if not a: # b can't be 0 or else there aren't 3 vars
swap = True
a, b = b, a
T = Matrix(((1, 1, -b/a), (1, -1, -c/a), (0, 0, 1)))
if swap:
T.row_swap(0, 1)
T.col_swap(0, 1)
return T
if coeff[x**2] == 0:
# If the coefficient of x is zero change the variables
if coeff[y**2] == 0:
_var[0], _var[2] = var[2], var[0]
T = _transformation_to_normal(_var, coeff)
T.row_swap(0, 2)
T.col_swap(0, 2)
return T
else:
_var[0], _var[1] = var[1], var[0]
T = _transformation_to_normal(_var, coeff)
T.row_swap(0, 1)
T.col_swap(0, 1)
return T
# Apply the transformation x --> X - (B*Y + C*Z)/(2*A)
if coeff[x*y] != 0 or coeff[x*z] != 0:
A = coeff[x**2]
B = coeff[x*y]
C = coeff[x*z]
D = coeff[y**2]
E = coeff[y*z]
F = coeff[z**2]
_coeff = dict()
_coeff[x**2] = 4*A**2
_coeff[y**2] = 4*A*D - B**2
_coeff[z**2] = 4*A*F - C**2
_coeff[y*z] = 4*A*E - 2*B*C
_coeff[x*y] = 0
_coeff[x*z] = 0
T_0 = _transformation_to_normal(_var, _coeff)
return Matrix(3, 3, [1, S(-B)/(2*A), S(-C)/(2*A), 0, 1, 0, 0, 0, 1])*T_0
elif coeff[y*z] != 0:
if coeff[y**2] == 0:
if coeff[z**2] == 0:
# Equations of the form A*x**2 + E*yz = 0.
# Apply transformation y -> Y + Z ans z -> Y - Z
return Matrix(3, 3, [1, 0, 0, 0, 1, 1, 0, 1, -1])
else:
# Ax**2 + E*y*z + F*z**2 = 0
_var[0], _var[2] = var[2], var[0]
T = _transformation_to_normal(_var, coeff)
T.row_swap(0, 2)
T.col_swap(0, 2)
return T
else:
# A*x**2 + D*y**2 + E*y*z + F*z**2 = 0, F may be zero
_var[0], _var[1] = var[1], var[0]
T = _transformation_to_normal(_var, coeff)
T.row_swap(0, 1)
T.col_swap(0, 1)
return T
else:
return Matrix.eye(3)
def parametrize_ternary_quadratic(eq):
"""
Returns the parametrized general solution for the ternary quadratic
equation ``eq`` which has the form
`ax^2 + by^2 + cz^2 + fxy + gyz + hxz = 0`.
Examples
========
>>> from sympy import Tuple, ordered
>>> from sympy.abc import x, y, z
>>> from sympy.solvers.diophantine import parametrize_ternary_quadratic
The parametrized solution may be returned with three parameters:
>>> parametrize_ternary_quadratic(2*x**2 + y**2 - 2*z**2)
(p**2 - 2*q**2, -2*p**2 + 4*p*q - 4*p*r - 4*q**2, p**2 - 4*p*q + 2*q**2 - 4*q*r)
There might also be only two parameters:
>>> parametrize_ternary_quadratic(4*x**2 + 2*y**2 - 3*z**2)
(2*p**2 - 3*q**2, -4*p**2 + 12*p*q - 6*q**2, 4*p**2 - 8*p*q + 6*q**2)
Notes
=====
Consider ``p`` and ``q`` in the previous 2-parameter
solution and observe that more than one solution can be represented
by a given pair of parameters. If `p` and ``q`` are not coprime, this is
trivially true since the common factor will also be a common factor of the
solution values. But it may also be true even when ``p`` and
``q`` are coprime:
>>> sol = Tuple(*_)
>>> p, q = ordered(sol.free_symbols)
>>> sol.subs([(p, 3), (q, 2)])
(6, 12, 12)
>>> sol.subs([(q, 1), (p, 1)])
(-1, 2, 2)
>>> sol.subs([(q, 0), (p, 1)])
(2, -4, 4)
>>> sol.subs([(q, 1), (p, 0)])
(-3, -6, 6)
Except for sign and a common factor, these are equivalent to
the solution of (1, 2, 2).
References
==========
.. [1] The algorithmic resolution of Diophantine equations, Nigel P. Smart,
London Mathematical Society Student Texts 41, Cambridge University
Press, Cambridge, 1998.
"""
var, coeff, diop_type = classify_diop(eq, _dict=False)
if diop_type in (
"homogeneous_ternary_quadratic",
"homogeneous_ternary_quadratic_normal"):
x_0, y_0, z_0 = _diop_ternary_quadratic(var, coeff)
return _parametrize_ternary_quadratic(
(x_0, y_0, z_0), var, coeff)
def _parametrize_ternary_quadratic(solution, _var, coeff):
# called for a*x**2 + b*y**2 + c*z**2 + d*x*y + e*y*z + f*x*z = 0
assert 1 not in coeff
x_0, y_0, z_0 = solution
v = list(_var) # copy
if x_0 is None:
return (None, None, None)
if solution.count(0) >= 2:
# if there are 2 zeros the equation reduces
# to k*X**2 == 0 where X is x, y, or z so X must
# be zero, too. So there is only the trivial
# solution.
return (None, None, None)
if x_0 == 0:
v[0], v[1] = v[1], v[0]
y_p, x_p, z_p = _parametrize_ternary_quadratic(
(y_0, x_0, z_0), v, coeff)
return x_p, y_p, z_p
x, y, z = v
r, p, q = symbols("r, p, q", integer=True)
eq = sum(k*v for k, v in coeff.items())
eq_1 = _mexpand(eq.subs(zip(
(x, y, z), (r*x_0, r*y_0 + p, r*z_0 + q))))
A, B = eq_1.as_independent(r, as_Add=True)
x = A*x_0
y = (A*y_0 - _mexpand(B/r*p))
z = (A*z_0 - _mexpand(B/r*q))
return _remove_gcd(x, y, z)
def diop_ternary_quadratic_normal(eq):
"""
Solves the quadratic ternary diophantine equation,
`ax^2 + by^2 + cz^2 = 0`.
Here the coefficients `a`, `b`, and `c` should be non zero. Otherwise the
equation will be a quadratic binary or univariate equation. If solvable,
returns a tuple `(x, y, z)` that satisfies the given equation. If the
equation does not have integer solutions, `(None, None, None)` is returned.
Usage
=====
``diop_ternary_quadratic_normal(eq)``: where ``eq`` is an equation of the form
`ax^2 + by^2 + cz^2 = 0`.
Examples
========
>>> from sympy.abc import x, y, z
>>> from sympy.solvers.diophantine import diop_ternary_quadratic_normal
>>> diop_ternary_quadratic_normal(x**2 + 3*y**2 - z**2)
(1, 0, 1)
>>> diop_ternary_quadratic_normal(4*x**2 + 5*y**2 - z**2)
(1, 0, 2)
>>> diop_ternary_quadratic_normal(34*x**2 - 3*y**2 - 301*z**2)
(4, 9, 1)
"""
var, coeff, diop_type = classify_diop(eq, _dict=False)
if diop_type == "homogeneous_ternary_quadratic_normal":
return _diop_ternary_quadratic_normal(var, coeff)
def _diop_ternary_quadratic_normal(var, coeff):
x, y, z = var
a = coeff[x**2]
b = coeff[y**2]
c = coeff[z**2]
try:
assert len([k for k in coeff if coeff[k]]) == 3
assert all(coeff[i**2] for i in var)
except AssertionError:
raise ValueError(filldedent('''
coeff dict is not consistent with assumption of this routine:
coefficients should be those of an expression in the form
a*x**2 + b*y**2 + c*z**2 where a*b*c != 0.'''))
(sqf_of_a, sqf_of_b, sqf_of_c), (a_1, b_1, c_1), (a_2, b_2, c_2) = \
sqf_normal(a, b, c, steps=True)
A = -a_2*c_2
B = -b_2*c_2
# If following two conditions are satisfied then there are no solutions
if A < 0 and B < 0:
return (None, None, None)
if (
sqrt_mod(-b_2*c_2, a_2) is None or
sqrt_mod(-c_2*a_2, b_2) is None or
sqrt_mod(-a_2*b_2, c_2) is None):
return (None, None, None)
z_0, x_0, y_0 = descent(A, B)
z_0, q = _rational_pq(z_0, abs(c_2))
x_0 *= q
y_0 *= q
x_0, y_0, z_0 = _remove_gcd(x_0, y_0, z_0)
# Holzer reduction
if sign(a) == sign(b):
x_0, y_0, z_0 = holzer(x_0, y_0, z_0, abs(a_2), abs(b_2), abs(c_2))
elif sign(a) == sign(c):
x_0, z_0, y_0 = holzer(x_0, z_0, y_0, abs(a_2), abs(c_2), abs(b_2))
else:
y_0, z_0, x_0 = holzer(y_0, z_0, x_0, abs(b_2), abs(c_2), abs(a_2))
x_0 = reconstruct(b_1, c_1, x_0)
y_0 = reconstruct(a_1, c_1, y_0)
z_0 = reconstruct(a_1, b_1, z_0)
sq_lcm = ilcm(sqf_of_a, sqf_of_b, sqf_of_c)
x_0 = abs(x_0*sq_lcm//sqf_of_a)
y_0 = abs(y_0*sq_lcm//sqf_of_b)
z_0 = abs(z_0*sq_lcm//sqf_of_c)
return _remove_gcd(x_0, y_0, z_0)
def sqf_normal(a, b, c, steps=False):
"""
Return `a', b', c'`, the coefficients of the square-free normal
form of `ax^2 + by^2 + cz^2 = 0`, where `a', b', c'` are pairwise
prime. If `steps` is True then also return three tuples:
`sq`, `sqf`, and `(a', b', c')` where `sq` contains the square
factors of `a`, `b` and `c` after removing the `gcd(a, b, c)`;
`sqf` contains the values of `a`, `b` and `c` after removing
both the `gcd(a, b, c)` and the square factors.
The solutions for `ax^2 + by^2 + cz^2 = 0` can be
recovered from the solutions of `a'x^2 + b'y^2 + c'z^2 = 0`.
Examples
========
>>> from sympy.solvers.diophantine import sqf_normal
>>> sqf_normal(2 * 3**2 * 5, 2 * 5 * 11, 2 * 7**2 * 11)
(11, 1, 5)
>>> sqf_normal(2 * 3**2 * 5, 2 * 5 * 11, 2 * 7**2 * 11, True)
((3, 1, 7), (5, 55, 11), (11, 1, 5))
References
==========
.. [1] Legendre's Theorem, Legrange's Descent,
http://public.csusm.edu/aitken_html/notes/legendre.pdf
See Also
========
reconstruct()
"""
ABC = _remove_gcd(a, b, c)
sq = tuple(square_factor(i) for i in ABC)
sqf = A, B, C = tuple([i//j**2 for i,j in zip(ABC, sq)])
pc = igcd(A, B)
A /= pc
B /= pc
pa = igcd(B, C)
B /= pa
C /= pa
pb = igcd(A, C)
A /= pb
B /= pb
A *= pa
B *= pb
C *= pc
if steps:
return (sq, sqf, (A, B, C))
else:
return A, B, C
def square_factor(a):
r"""
Returns an integer `c` s.t. `a = c^2k, \ c,k \in Z`. Here `k` is square
free. `a` can be given as an integer or a dictionary of factors.
Examples
========
>>> from sympy.solvers.diophantine import square_factor
>>> square_factor(24)
2
>>> square_factor(-36*3)
6
>>> square_factor(1)
1
>>> square_factor({3: 2, 2: 1, -1: 1}) # -18
3
See Also
========
sympy.ntheory.factor_.core
"""
f = a if isinstance(a, dict) else factorint(a)
return Mul(*[p**(e//2) for p, e in f.items()])
def reconstruct(A, B, z):
"""
Reconstruct the `z` value of an equivalent solution of `ax^2 + by^2 + cz^2`
from the `z` value of a solution of the square-free normal form of the
equation, `a'*x^2 + b'*y^2 + c'*z^2`, where `a'`, `b'` and `c'` are square
free and `gcd(a', b', c') == 1`.
"""
f = factorint(igcd(A, B))
for p, e in f.items():
if e != 1:
raise ValueError('a and b should be square-free')
z *= p
return z
def ldescent(A, B):
"""
Return a non-trivial solution to `w^2 = Ax^2 + By^2` using
Lagrange's method; return None if there is no such solution.
.
Here, `A \\neq 0` and `B \\neq 0` and `A` and `B` are square free. Output a
tuple `(w_0, x_0, y_0)` which is a solution to the above equation.
Examples
========
>>> from sympy.solvers.diophantine import ldescent
>>> ldescent(1, 1) # w^2 = x^2 + y^2
(1, 1, 0)
>>> ldescent(4, -7) # w^2 = 4x^2 - 7y^2
(2, -1, 0)
This means that `x = -1, y = 0` and `w = 2` is a solution to the equation
`w^2 = 4x^2 - 7y^2`
>>> ldescent(5, -1) # w^2 = 5x^2 - y^2
(2, 1, -1)
References
==========
.. [1] The algorithmic resolution of Diophantine equations, Nigel P. Smart,
London Mathematical Society Student Texts 41, Cambridge University
Press, Cambridge, 1998.
.. [2] Efficient Solution of Rational Conices, J. E. Cremona and D. Rusin,
[online], Available:
http://eprints.nottingham.ac.uk/60/1/kvxefz87.pdf
"""
if abs(A) > abs(B):
w, y, x = ldescent(B, A)
return w, x, y
if A == 1:
return (1, 1, 0)
if B == 1:
return (1, 0, 1)
if B == -1: # and A == -1
return
r = sqrt_mod(A, B)
Q = (r**2 - A) // B
if Q == 0:
B_0 = 1
d = 0
else:
div = divisors(Q)
B_0 = None
for i in div:
sQ, _exact = integer_nthroot(abs(Q) // i, 2)
if _exact:
B_0, d = sign(Q)*i, sQ
break
if B_0 is not None:
W, X, Y = ldescent(A, B_0)
return _remove_gcd((-A*X + r*W), (r*X - W), Y*(B_0*d))
def descent(A, B):
"""
Returns a non-trivial solution, (x, y, z), to `x^2 = Ay^2 + Bz^2`
using Lagrange's descent method with lattice-reduction. `A` and `B`
are assumed to be valid for such a solution to exist.
This is faster than the normal Lagrange's descent algorithm because
the Gaussian reduction is used.
Examples
========
>>> from sympy.solvers.diophantine import descent
>>> descent(3, 1) # x**2 = 3*y**2 + z**2
(1, 0, 1)
`(x, y, z) = (1, 0, 1)` is a solution to the above equation.
>>> descent(41, -113)
(-16, -3, 1)
References
==========
.. [1] Efficient Solution of Rational Conices, J. E. Cremona and D. Rusin,
Mathematics of Computation, Volume 00, Number 0.
"""
if abs(A) > abs(B):
x, y, z = descent(B, A)
return x, z, y
if B == 1:
return (1, 0, 1)
if A == 1:
return (1, 1, 0)
if B == -A:
return (0, 1, 1)
if B == A:
x, z, y = descent(-1, A)
return (A*y, z, x)
w = sqrt_mod(A, B)
x_0, z_0 = gaussian_reduce(w, A, B)
t = (x_0**2 - A*z_0**2) // B
t_2 = square_factor(t)
t_1 = t // t_2**2
x_1, z_1, y_1 = descent(A, t_1)
return _remove_gcd(x_0*x_1 + A*z_0*z_1, z_0*x_1 + x_0*z_1, t_1*t_2*y_1)
def gaussian_reduce(w, a, b):
r"""
Returns a reduced solution `(x, z)` to the congruence
`X^2 - aZ^2 \equiv 0 \ (mod \ b)` so that `x^2 + |a|z^2` is minimal.
Details
=======
Here ``w`` is a solution of the congruence `x^2 \equiv a \ (mod \ b)`
References
==========
.. [1] Gaussian lattice Reduction [online]. Available:
http://home.ie.cuhk.edu.hk/~wkshum/wordpress/?p=404
.. [2] Efficient Solution of Rational Conices, J. E. Cremona and D. Rusin,
Mathematics of Computation, Volume 00, Number 0.
"""
u = (0, 1)
v = (1, 0)
if dot(u, v, w, a, b) < 0:
v = (-v[0], -v[1])
if norm(u, w, a, b) < norm(v, w, a, b):
u, v = v, u
while norm(u, w, a, b) > norm(v, w, a, b):
k = dot(u, v, w, a, b) // dot(v, v, w, a, b)
u, v = v, (u[0]- k*v[0], u[1]- k*v[1])
u, v = v, u
if dot(u, v, w, a, b) < dot(v, v, w, a, b)/2 or norm((u[0]-v[0], u[1]-v[1]), w, a, b) > norm(v, w, a, b):
c = v
else:
c = (u[0] - v[0], u[1] - v[1])
return c[0]*w + b*c[1], c[0]
def dot(u, v, w, a, b):
r"""
Returns a special dot product of the vectors `u = (u_{1}, u_{2})` and
`v = (v_{1}, v_{2})` which is defined in order to reduce solution of
the congruence equation `X^2 - aZ^2 \equiv 0 \ (mod \ b)`.
"""
u_1, u_2 = u
v_1, v_2 = v
return (w*u_1 + b*u_2)*(w*v_1 + b*v_2) + abs(a)*u_1*v_1
def norm(u, w, a, b):
r"""
Returns the norm of the vector `u = (u_{1}, u_{2})` under the dot product
defined by `u \cdot v = (wu_{1} + bu_{2})(w*v_{1} + bv_{2}) + |a|*u_{1}*v_{1}`
where `u = (u_{1}, u_{2})` and `v = (v_{1}, v_{2})`.
"""
u_1, u_2 = u
return sqrt(dot((u_1, u_2), (u_1, u_2), w, a, b))
def holzer(x, y, z, a, b, c):
r"""
Simplify the solution `(x, y, z)` of the equation
`ax^2 + by^2 = cz^2` with `a, b, c > 0` and `z^2 \geq \mid ab \mid` to
a new reduced solution `(x', y', z')` such that `z'^2 \leq \mid ab \mid`.
The algorithm is an interpretation of Mordell's reduction as described
on page 8 of Cremona and Rusin's paper [1]_ and the work of Mordell in
reference [2]_.
References
==========
.. [1] Efficient Solution of Rational Conices, J. E. Cremona and D. Rusin,
Mathematics of Computation, Volume 00, Number 0.
.. [2] Diophantine Equations, L. J. Mordell, page 48.
"""
if _odd(c):
k = 2*c
else:
k = c//2
small = a*b*c
step = 0
while True:
t1, t2, t3 = a*x**2, b*y**2, c*z**2
# check that it's a solution
if t1 + t2 != t3:
if step == 0:
raise ValueError('bad starting solution')
break
x_0, y_0, z_0 = x, y, z
if max(t1, t2, t3) <= small:
# Holzer condition
break
uv = u, v = base_solution_linear(k, y_0, -x_0)
if None in uv:
break
p, q = -(a*u*x_0 + b*v*y_0), c*z_0
r = Rational(p, q)
if _even(c):
w = _nint_or_floor(p, q)
assert abs(w - r) <= S.Half
else:
w = p//q # floor
if _odd(a*u + b*v + c*w):
w += 1
assert abs(w - r) <= S.One
A = (a*u**2 + b*v**2 + c*w**2)
B = (a*u*x_0 + b*v*y_0 + c*w*z_0)
x = Rational(x_0*A - 2*u*B, k)
y = Rational(y_0*A - 2*v*B, k)
z = Rational(z_0*A - 2*w*B, k)
assert all(i.is_Integer for i in (x, y, z))
step += 1
return tuple([int(i) for i in (x_0, y_0, z_0)])
def diop_general_pythagorean(eq, param=symbols("m", integer=True)):
"""
Solves the general pythagorean equation,
`a_{1}^2x_{1}^2 + a_{2}^2x_{2}^2 + . . . + a_{n}^2x_{n}^2 - a_{n + 1}^2x_{n + 1}^2 = 0`.
Returns a tuple which contains a parametrized solution to the equation,
sorted in the same order as the input variables.
Usage
=====
``diop_general_pythagorean(eq, param)``: where ``eq`` is a general
pythagorean equation which is assumed to be zero and ``param`` is the base
parameter used to construct other parameters by subscripting.
Examples
========
>>> from sympy.solvers.diophantine import diop_general_pythagorean
>>> from sympy.abc import a, b, c, d, e
>>> diop_general_pythagorean(a**2 + b**2 + c**2 - d**2)
(m1**2 + m2**2 - m3**2, 2*m1*m3, 2*m2*m3, m1**2 + m2**2 + m3**2)
>>> diop_general_pythagorean(9*a**2 - 4*b**2 + 16*c**2 + 25*d**2 + e**2)
(10*m1**2 + 10*m2**2 + 10*m3**2 - 10*m4**2, 15*m1**2 + 15*m2**2 + 15*m3**2 + 15*m4**2, 15*m1*m4, 12*m2*m4, 60*m3*m4)
"""
var, coeff, diop_type = classify_diop(eq, _dict=False)
if diop_type == "general_pythagorean":
return _diop_general_pythagorean(var, coeff, param)
def _diop_general_pythagorean(var, coeff, t):
if sign(coeff[var[0]**2]) + sign(coeff[var[1]**2]) + sign(coeff[var[2]**2]) < 0:
for key in coeff.keys():
coeff[key] = -coeff[key]
n = len(var)
index = 0
for i, v in enumerate(var):
if sign(coeff[v**2]) == -1:
index = i
m = symbols('%s1:%i' % (t, n), integer=True)
ith = sum(m_i**2 for m_i in m)
L = [ith - 2*m[n - 2]**2]
L.extend([2*m[i]*m[n-2] for i in range(n - 2)])
sol = L[:index] + [ith] + L[index:]
lcm = 1
for i, v in enumerate(var):
if i == index or (index > 0 and i == 0) or (index == 0 and i == 1):
lcm = ilcm(lcm, sqrt(abs(coeff[v**2])))
else:
s = sqrt(coeff[v**2])
lcm = ilcm(lcm, s if _odd(s) else s//2)
for i, v in enumerate(var):
sol[i] = (lcm*sol[i]) / sqrt(abs(coeff[v**2]))
return tuple(sol)
def diop_general_sum_of_squares(eq, limit=1):
r"""
Solves the equation `x_{1}^2 + x_{2}^2 + . . . + x_{n}^2 - k = 0`.
Returns at most ``limit`` number of solutions.
Usage
=====
``general_sum_of_squares(eq, limit)`` : Here ``eq`` is an expression which
is assumed to be zero. Also, ``eq`` should be in the form,
`x_{1}^2 + x_{2}^2 + . . . + x_{n}^2 - k = 0`.
Details
=======
When `n = 3` if `k = 4^a(8m + 7)` for some `a, m \in Z` then there will be
no solutions. Refer [1]_ for more details.
Examples
========
>>> from sympy.solvers.diophantine import diop_general_sum_of_squares
>>> from sympy.abc import a, b, c, d, e, f
>>> diop_general_sum_of_squares(a**2 + b**2 + c**2 + d**2 + e**2 - 2345)
{(15, 22, 22, 24, 24)}
Reference
=========
.. [1] Representing an integer as a sum of three squares, [online],
Available:
http://www.proofwiki.org/wiki/Integer_as_Sum_of_Three_Squares
"""
var, coeff, diop_type = classify_diop(eq, _dict=False)
if diop_type == "general_sum_of_squares":
return _diop_general_sum_of_squares(var, -coeff[1], limit)
def _diop_general_sum_of_squares(var, k, limit=1):
# solves Eq(sum(i**2 for i in var), k)
n = len(var)
if n < 3:
raise ValueError('n must be greater than 2')
s = set()
if k < 0 or limit < 1:
return s
sign = [-1 if x.is_nonpositive else 1 for x in var]
negs = sign.count(-1) != 0
took = 0
for t in sum_of_squares(k, n, zeros=True):
if negs:
s.add(tuple([sign[i]*j for i, j in enumerate(t)]))
else:
s.add(t)
took += 1
if took == limit:
break
return s
def diop_general_sum_of_even_powers(eq, limit=1):
"""
Solves the equation `x_{1}^e + x_{2}^e + . . . + x_{n}^e - k = 0`
where `e` is an even, integer power.
Returns at most ``limit`` number of solutions.
Usage
=====
``general_sum_of_even_powers(eq, limit)`` : Here ``eq`` is an expression which
is assumed to be zero. Also, ``eq`` should be in the form,
`x_{1}^e + x_{2}^e + . . . + x_{n}^e - k = 0`.
Examples
========
>>> from sympy.solvers.diophantine import diop_general_sum_of_even_powers
>>> from sympy.abc import a, b
>>> diop_general_sum_of_even_powers(a**4 + b**4 - (2**4 + 3**4))
{(2, 3)}
See Also
========
power_representation()
"""
var, coeff, diop_type = classify_diop(eq, _dict=False)
if diop_type == "general_sum_of_even_powers":
for k in coeff.keys():
if k.is_Pow and coeff[k]:
p = k.exp
return _diop_general_sum_of_even_powers(var, p, -coeff[1], limit)
def _diop_general_sum_of_even_powers(var, p, n, limit=1):
# solves Eq(sum(i**2 for i in var), n)
k = len(var)
s = set()
if n < 0 or limit < 1:
return s
sign = [-1 if x.is_nonpositive else 1 for x in var]
negs = sign.count(-1) != 0
took = 0
for t in power_representation(n, p, k):
if negs:
s.add(tuple([sign[i]*j for i, j in enumerate(t)]))
else:
s.add(t)
took += 1
if took == limit:
break
return s
## Functions below this comment can be more suitably grouped under
## an Additive number theory module rather than the Diophantine
## equation module.
def partition(n, k=None, zeros=False):
"""
Returns a generator that can be used to generate partitions of an integer
`n`.
A partition of `n` is a set of positive integers which add up to `n`. For
example, partitions of 3 are 3, 1 + 2, 1 + 1 + 1. A partition is returned
as a tuple. If ``k`` equals None, then all possible partitions are returned
irrespective of their size, otherwise only the partitions of size ``k`` are
returned. If the ``zero`` parameter is set to True then a suitable
number of zeros are added at the end of every partition of size less than
``k``.
``zero`` parameter is considered only if ``k`` is not None. When the
partitions are over, the last `next()` call throws the ``StopIteration``
exception, so this function should always be used inside a try - except
block.
Details
=======
``partition(n, k)``: Here ``n`` is a positive integer and ``k`` is the size
of the partition which is also positive integer.
Examples
========
>>> from sympy.solvers.diophantine import partition
>>> f = partition(5)
>>> next(f)
(1, 1, 1, 1, 1)
>>> next(f)
(1, 1, 1, 2)
>>> g = partition(5, 3)
>>> next(g)
(1, 1, 3)
>>> next(g)
(1, 2, 2)
>>> g = partition(5, 3, zeros=True)
>>> next(g)
(0, 0, 5)
"""
from sympy.utilities.iterables import ordered_partitions
if not zeros or k is None:
for i in ordered_partitions(n, k):
yield tuple(i)
else:
for m in range(1, k + 1):
for i in ordered_partitions(n, m):
i = tuple(i)
yield (0,)*(k - len(i)) + i
def prime_as_sum_of_two_squares(p):
"""
Represent a prime `p` as a unique sum of two squares; this can
only be done if the prime is congruent to 1 mod 4.
Examples
========
>>> from sympy.solvers.diophantine import prime_as_sum_of_two_squares
>>> prime_as_sum_of_two_squares(7) # can't be done
>>> prime_as_sum_of_two_squares(5)
(1, 2)
Reference
=========
.. [1] Representing a number as a sum of four squares, [online],
Available: http://schorn.ch/lagrange.html
See Also
========
sum_of_squares()
"""
if not p % 4 == 1:
return
if p % 8 == 5:
b = 2
else:
b = 3
while pow(b, (p - 1) // 2, p) == 1:
b = nextprime(b)
b = pow(b, (p - 1) // 4, p)
a = p
while b**2 > p:
a, b = b, a % b
return (int(a % b), int(b)) # convert from long
def sum_of_three_squares(n):
r"""
Returns a 3-tuple `(a, b, c)` such that `a^2 + b^2 + c^2 = n` and
`a, b, c \geq 0`.
Returns None if `n = 4^a(8m + 7)` for some `a, m \in Z`. See
[1]_ for more details.
Usage
=====
``sum_of_three_squares(n)``: Here ``n`` is a non-negative integer.
Examples
========
>>> from sympy.solvers.diophantine import sum_of_three_squares
>>> sum_of_three_squares(44542)
(18, 37, 207)
References
==========
.. [1] Representing a number as a sum of three squares, [online],
Available: http://schorn.ch/lagrange.html
See Also
========
sum_of_squares()
"""
special = {1:(1, 0, 0), 2:(1, 1, 0), 3:(1, 1, 1), 10: (1, 3, 0), 34: (3, 3, 4), 58:(3, 7, 0),
85:(6, 7, 0), 130:(3, 11, 0), 214:(3, 6, 13), 226:(8, 9, 9), 370:(8, 9, 15),
526:(6, 7, 21), 706:(15, 15, 16), 730:(1, 27, 0), 1414:(6, 17, 33), 1906:(13, 21, 36),
2986: (21, 32, 39), 9634: (56, 57, 57)}
v = 0
if n == 0:
return (0, 0, 0)
v = multiplicity(4, n)
n //= 4**v
if n % 8 == 7:
return
if n in special.keys():
x, y, z = special[n]
return _sorted_tuple(2**v*x, 2**v*y, 2**v*z)
s, _exact = integer_nthroot(n, 2)
if _exact:
return (2**v*s, 0, 0)
x = None
if n % 8 == 3:
s = s if _odd(s) else s - 1
for x in range(s, -1, -2):
N = (n - x**2) // 2
if isprime(N):
y, z = prime_as_sum_of_two_squares(N)
return _sorted_tuple(2**v*x, 2**v*(y + z), 2**v*abs(y - z))
return
if n % 8 == 2 or n % 8 == 6:
s = s if _odd(s) else s - 1
else:
s = s - 1 if _odd(s) else s
for x in range(s, -1, -2):
N = n - x**2
if isprime(N):
y, z = prime_as_sum_of_two_squares(N)
return _sorted_tuple(2**v*x, 2**v*y, 2**v*z)
def sum_of_four_squares(n):
r"""
Returns a 4-tuple `(a, b, c, d)` such that `a^2 + b^2 + c^2 + d^2 = n`.
Here `a, b, c, d \geq 0`.
Usage
=====
``sum_of_four_squares(n)``: Here ``n`` is a non-negative integer.
Examples
========
>>> from sympy.solvers.diophantine import sum_of_four_squares
>>> sum_of_four_squares(3456)
(8, 8, 32, 48)
>>> sum_of_four_squares(1294585930293)
(0, 1234, 2161, 1137796)
References
==========
.. [1] Representing a number as a sum of four squares, [online],
Available: http://schorn.ch/lagrange.html
See Also
========
sum_of_squares()
"""
if n == 0:
return (0, 0, 0, 0)
v = multiplicity(4, n)
n //= 4**v
if n % 8 == 7:
d = 2
n = n - 4
elif n % 8 == 6 or n % 8 == 2:
d = 1
n = n - 1
else:
d = 0
x, y, z = sum_of_three_squares(n)
return _sorted_tuple(2**v*d, 2**v*x, 2**v*y, 2**v*z)
def power_representation(n, p, k, zeros=False):
"""
Returns a generator for finding k-tuples of integers,
`(n_{1}, n_{2}, . . . n_{k})`, such that
`n = n_{1}^p + n_{2}^p + . . . n_{k}^p`.
Usage
=====
``power_representation(n, p, k, zeros)``: Represent non-negative number
``n`` as a sum of ``k`` ``p``th powers. If ``zeros`` is true, then the
solutions is allowed to contain zeros.
Examples
========
>>> from sympy.solvers.diophantine import power_representation
Represent 1729 as a sum of two cubes:
>>> f = power_representation(1729, 3, 2)
>>> next(f)
(9, 10)
>>> next(f)
(1, 12)
If the flag `zeros` is True, the solution may contain tuples with
zeros; any such solutions will be generated after the solutions
without zeros:
>>> list(power_representation(125, 2, 3, zeros=True))
[(5, 6, 8), (3, 4, 10), (0, 5, 10), (0, 2, 11)]
For even `p` the `permute_sign` function can be used to get all
signed values:
>>> from sympy.utilities.iterables import permute_signs
>>> list(permute_signs((1, 12)))
[(1, 12), (-1, 12), (1, -12), (-1, -12)]
All possible signed permutations can also be obtained:
>>> from sympy.utilities.iterables import signed_permutations
>>> list(signed_permutations((1, 12)))
[(1, 12), (-1, 12), (1, -12), (-1, -12), (12, 1), (-12, 1), (12, -1), (-12, -1)]
"""
n, p, k = [as_int(i) for i in (n, p, k)]
if n < 0:
if p % 2:
for t in power_representation(-n, p, k, zeros):
yield tuple(-i for i in t)
return
if p < 1 or k < 1:
raise ValueError(filldedent('''
Expecting positive integers for `(p, k)`, but got `(%s, %s)`'''
% (p, k)))
if n == 0:
if zeros:
yield (0,)*k
return
if k == 1:
if p == 1:
yield (n,)
else:
be = perfect_power(n)
if be:
b, e = be
d, r = divmod(e, p)
if not r:
yield (b**d,)
return
if p == 1:
for t in partition(n, k, zeros=zeros):
yield t
return
if p == 2:
feasible = _can_do_sum_of_squares(n, k)
if not feasible:
return
if not zeros and n > 33 and k >= 5 and k <= n and n - k in (
13, 10, 7, 5, 4, 2, 1):
'''Todd G. Will, "When Is n^2 a Sum of k Squares?", [online].
Available: https://www.maa.org/sites/default/files/Will-MMz-201037918.pdf'''
return
if feasible is not True: # it's prime and k == 2
yield prime_as_sum_of_two_squares(n)
return
if k == 2 and p > 2:
be = perfect_power(n)
if be and be[1] % p == 0:
return # Fermat: a**n + b**n = c**n has no solution for n > 2
if n >= k:
a = integer_nthroot(n - (k - 1), p)[0]
for t in pow_rep_recursive(a, k, n, [], p):
yield tuple(reversed(t))
if zeros:
a = integer_nthroot(n, p)[0]
for i in range(1, k):
for t in pow_rep_recursive(a, i, n, [], p):
yield tuple(reversed(t + (0,) * (k - i)))
sum_of_powers = power_representation
def pow_rep_recursive(n_i, k, n_remaining, terms, p):
if k == 0 and n_remaining == 0:
yield tuple(terms)
else:
if n_i >= 1 and k > 0:
for t in pow_rep_recursive(n_i - 1, k, n_remaining, terms, p):
yield t
residual = n_remaining - pow(n_i, p)
if residual >= 0:
for t in pow_rep_recursive(n_i, k - 1, residual, terms + [n_i], p):
yield t
def sum_of_squares(n, k, zeros=False):
"""Return a generator that yields the k-tuples of nonnegative
values, the squares of which sum to n. If zeros is False (default)
then the solution will not contain zeros. The nonnegative
elements of a tuple are sorted.
* If k == 1 and n is square, (n,) is returned.
* If k == 2 then n can only be written as a sum of squares if
every prime in the factorization of n that has the form
4*k + 3 has an even multiplicity. If n is prime then
it can only be written as a sum of two squares if it is
in the form 4*k + 1.
* if k == 3 then n can be written as a sum of squares if it does
not have the form 4**m*(8*k + 7).
* all integers can be written as the sum of 4 squares.
* if k > 4 then n can be partitioned and each partition can
be written as a sum of 4 squares; if n is not evenly divisible
by 4 then n can be written as a sum of squares only if the
an additional partition can be written as sum of squares.
For example, if k = 6 then n is partitioned into two parts,
the first being written as a sum of 4 squares and the second
being written as a sum of 2 squares -- which can only be
done if the condition above for k = 2 can be met, so this will
automatically reject certain partitions of n.
Examples
========
>>> from sympy.solvers.diophantine import sum_of_squares
>>> list(sum_of_squares(25, 2))
[(3, 4)]
>>> list(sum_of_squares(25, 2, True))
[(3, 4), (0, 5)]
>>> list(sum_of_squares(25, 4))
[(1, 2, 2, 4)]
See Also
========
sympy.utilities.iterables.signed_permutations
"""
for t in power_representation(n, 2, k, zeros):
yield t
def _can_do_sum_of_squares(n, k):
"""Return True if n can be written as the sum of k squares,
False if it can't, or 1 if k == 2 and n is prime (in which
case it *can* be written as a sum of two squares). A False
is returned only if it can't be written as k-squares, even
if 0s are allowed.
"""
if k < 1:
return False
if n < 0:
return False
if n == 0:
return True
if k == 1:
return is_square(n)
if k == 2:
if n in (1, 2):
return True
if isprime(n):
if n % 4 == 1:
return 1 # signal that it was prime
return False
else:
f = factorint(n)
for p, m in f.items():
# we can proceed iff no prime factor in the form 4*k + 3
# has an odd multiplicity
if (p % 4 == 3) and m % 2:
return False
return True
if k == 3:
if (n//4**multiplicity(4, n)) % 8 == 7:
return False
# every number can be written as a sum of 4 squares; for k > 4 partitions
# can be 0
return True
|
ebbb2594155ad896ad6fa8c23e07d3d1772cf58714b9ea67db5ed278395aae87 | """
This module contain solvers for all kinds of equations:
- algebraic or transcendental, use solve()
- recurrence, use rsolve()
- differential, use dsolve()
- nonlinear (numerically), use nsolve()
(you will need a good starting point)
"""
from __future__ import print_function, division
from sympy import divisors
from sympy.core.compatibility import (iterable, is_sequence, ordered,
default_sort_key, range)
from sympy.core.sympify import sympify
from sympy.core import (S, Add, Symbol, Equality, Dummy, Expr, Mul,
Pow, Unequality)
from sympy.core.exprtools import factor_terms
from sympy.core.function import (expand_mul, expand_log,
Derivative, AppliedUndef, UndefinedFunction, nfloat,
Function, expand_power_exp, _mexpand, expand)
from sympy.integrals.integrals import Integral
from sympy.core.numbers import ilcm, Float, Rational
from sympy.core.relational import Relational
from sympy.core.logic import fuzzy_not, fuzzy_and
from sympy.core.power import integer_log
from sympy.logic.boolalg import And, Or, BooleanAtom
from sympy.core.basic import preorder_traversal
from sympy.functions import (log, exp, LambertW, cos, sin, tan, acos, asin, atan,
Abs, re, im, arg, sqrt, atan2)
from sympy.functions.elementary.trigonometric import (TrigonometricFunction,
HyperbolicFunction)
from sympy.simplify import (simplify, collect, powsimp, posify,
powdenest, nsimplify, denom, logcombine, sqrtdenest, fraction,
separatevars)
from sympy.simplify.sqrtdenest import sqrt_depth
from sympy.simplify.fu import TR1
from sympy.matrices import Matrix, zeros
from sympy.polys import roots, cancel, factor, Poly, degree
from sympy.polys.polyerrors import GeneratorsNeeded, PolynomialError
from sympy.functions.elementary.piecewise import piecewise_fold, Piecewise
from sympy.utilities.lambdify import lambdify
from sympy.utilities.misc import filldedent
from sympy.utilities.iterables import uniq, generate_bell, flatten
from sympy.utilities.decorator import conserve_mpmath_dps
from mpmath import findroot
from sympy.solvers.polysys import solve_poly_system
from sympy.solvers.inequalities import reduce_inequalities
from types import GeneratorType
from collections import defaultdict
import warnings
def recast_to_symbols(eqs, symbols):
"""Return (e, s, d) where e and s are versions of eqs and
symbols in which any non-Symbol objects in symbols have
been replaced with generic Dummy symbols and d is a dictionary
that can be used to restore the original expressions.
Examples
========
>>> from sympy.solvers.solvers import recast_to_symbols
>>> from sympy import symbols, Function
>>> x, y = symbols('x y')
>>> fx = Function('f')(x)
>>> eqs, syms = [fx + 1, x, y], [fx, y]
>>> e, s, d = recast_to_symbols(eqs, syms); (e, s, d)
([_X0 + 1, x, y], [_X0, y], {_X0: f(x)})
The original equations and symbols can be restored using d:
>>> assert [i.xreplace(d) for i in eqs] == eqs
>>> assert [d.get(i, i) for i in s] == syms
"""
if not iterable(eqs) and iterable(symbols):
raise ValueError('Both eqs and symbols must be iterable')
new_symbols = list(symbols)
swap_sym = {}
for i, s in enumerate(symbols):
if not isinstance(s, Symbol) and s not in swap_sym:
swap_sym[s] = Dummy('X%d' % i)
new_symbols[i] = swap_sym[s]
new_f = []
for i in eqs:
isubs = getattr(i, 'subs', None)
if isubs is not None:
new_f.append(isubs(swap_sym))
else:
new_f.append(i)
swap_sym = {v: k for k, v in swap_sym.items()}
return new_f, new_symbols, swap_sym
def _ispow(e):
"""Return True if e is a Pow or is exp."""
return isinstance(e, Expr) and (e.is_Pow or isinstance(e, exp))
def _simple_dens(f, symbols):
# when checking if a denominator is zero, we can just check the
# base of powers with nonzero exponents since if the base is zero
# the power will be zero, too. To keep it simple and fast, we
# limit simplification to exponents that are Numbers
dens = set()
for d in denoms(f, symbols):
if d.is_Pow and d.exp.is_Number:
if d.exp.is_zero:
continue # foo**0 is never 0
d = d.base
dens.add(d)
return dens
def denoms(eq, *symbols):
"""Return (recursively) set of all denominators that appear in eq
that contain any symbol in ``symbols``; if ``symbols`` are not
provided then all denominators will be returned.
Examples
========
>>> from sympy.solvers.solvers import denoms
>>> from sympy.abc import x, y, z
>>> from sympy import sqrt
>>> denoms(x/y)
{y}
>>> denoms(x/(y*z))
{y, z}
>>> denoms(3/x + y/z)
{x, z}
>>> denoms(x/2 + y/z)
{2, z}
If `symbols` are provided then only denominators containing
those symbols will be returned
>>> denoms(1/x + 1/y + 1/z, y, z)
{y, z}
"""
pot = preorder_traversal(eq)
dens = set()
for p in pot:
den = denom(p)
if den is S.One:
continue
for d in Mul.make_args(den):
dens.add(d)
if not symbols:
return dens
elif len(symbols) == 1:
if iterable(symbols[0]):
symbols = symbols[0]
rv = []
for d in dens:
free = d.free_symbols
if any(s in free for s in symbols):
rv.append(d)
return set(rv)
def checksol(f, symbol, sol=None, **flags):
"""Checks whether sol is a solution of equation f == 0.
Input can be either a single symbol and corresponding value
or a dictionary of symbols and values. When given as a dictionary
and flag ``simplify=True``, the values in the dictionary will be
simplified. ``f`` can be a single equation or an iterable of equations.
A solution must satisfy all equations in ``f`` to be considered valid;
if a solution does not satisfy any equation, False is returned; if one or
more checks are inconclusive (and none are False) then None
is returned.
Examples
========
>>> from sympy import symbols
>>> from sympy.solvers import checksol
>>> x, y = symbols('x,y')
>>> checksol(x**4 - 1, x, 1)
True
>>> checksol(x**4 - 1, x, 0)
False
>>> checksol(x**2 + y**2 - 5**2, {x: 3, y: 4})
True
To check if an expression is zero using checksol, pass it
as ``f`` and send an empty dictionary for ``symbol``:
>>> checksol(x**2 + x - x*(x + 1), {})
True
None is returned if checksol() could not conclude.
flags:
'numerical=True (default)'
do a fast numerical check if ``f`` has only one symbol.
'minimal=True (default is False)'
a very fast, minimal testing.
'warn=True (default is False)'
show a warning if checksol() could not conclude.
'simplify=True (default)'
simplify solution before substituting into function and
simplify the function before trying specific simplifications
'force=True (default is False)'
make positive all symbols without assumptions regarding sign.
"""
from sympy.physics.units import Unit
minimal = flags.get('minimal', False)
if sol is not None:
sol = {symbol: sol}
elif isinstance(symbol, dict):
sol = symbol
else:
msg = 'Expecting (sym, val) or ({sym: val}, None) but got (%s, %s)'
raise ValueError(msg % (symbol, sol))
if iterable(f):
if not f:
raise ValueError('no functions to check')
rv = True
for fi in f:
check = checksol(fi, sol, **flags)
if check:
continue
if check is False:
return False
rv = None # don't return, wait to see if there's a False
return rv
if isinstance(f, Poly):
f = f.as_expr()
elif isinstance(f, (Equality, Unequality)):
if f.rhs in (S.true, S.false):
f = f.reversed
B, E = f.args
if B in (S.true, S.false):
f = f.subs(sol)
if f not in (S.true, S.false):
return
else:
f = f.rewrite(Add, evaluate=False)
if isinstance(f, BooleanAtom):
return bool(f)
elif not f.is_Relational and not f:
return True
if sol and not f.free_symbols & set(sol.keys()):
# if f(y) == 0, x=3 does not set f(y) to zero...nor does it not
return None
illegal = set([S.NaN,
S.ComplexInfinity,
S.Infinity,
S.NegativeInfinity])
if any(sympify(v).atoms() & illegal for k, v in sol.items()):
return False
was = f
attempt = -1
numerical = flags.get('numerical', True)
while 1:
attempt += 1
if attempt == 0:
val = f.subs(sol)
if isinstance(val, Mul):
val = val.as_independent(Unit)[0]
if val.atoms() & illegal:
return False
elif attempt == 1:
if not val.is_number:
if not val.is_constant(*list(sol.keys()), simplify=not minimal):
return False
# there are free symbols -- simple expansion might work
_, val = val.as_content_primitive()
val = _mexpand(val.as_numer_denom()[0], recursive=True)
elif attempt == 2:
if minimal:
return
if flags.get('simplify', True):
for k in sol:
sol[k] = simplify(sol[k])
# start over without the failed expanded form, possibly
# with a simplified solution
val = simplify(f.subs(sol))
if flags.get('force', True):
val, reps = posify(val)
# expansion may work now, so try again and check
exval = _mexpand(val, recursive=True)
if exval.is_number:
# we can decide now
val = exval
else:
# if there are no radicals and no functions then this can't be
# zero anymore -- can it?
pot = preorder_traversal(expand_mul(val))
seen = set()
saw_pow_func = False
for p in pot:
if p in seen:
continue
seen.add(p)
if p.is_Pow and not p.exp.is_Integer:
saw_pow_func = True
elif p.is_Function:
saw_pow_func = True
elif isinstance(p, UndefinedFunction):
saw_pow_func = True
if saw_pow_func:
break
if saw_pow_func is False:
return False
if flags.get('force', True):
# don't do a zero check with the positive assumptions in place
val = val.subs(reps)
nz = fuzzy_not(val.is_zero)
if nz is not None:
# issue 5673: nz may be True even when False
# so these are just hacks to keep a false positive
# from being returned
# HACK 1: LambertW (issue 5673)
if val.is_number and val.has(LambertW):
# don't eval this to verify solution since if we got here,
# numerical must be False
return None
# add other HACKs here if necessary, otherwise we assume
# the nz value is correct
return not nz
break
if val == was:
continue
elif val.is_Rational:
return val == 0
if numerical and val.is_number:
if val in (S.true, S.false):
return bool(val)
return bool(abs(val.n(18).n(12, chop=True)) < 1e-9)
was = val
if flags.get('warn', False):
warnings.warn("\n\tWarning: could not verify solution %s." % sol)
# returns None if it can't conclude
# TODO: improve solution testing
def failing_assumptions(expr, **assumptions):
"""Return a dictionary containing assumptions with values not
matching those of the passed assumptions.
Examples
========
>>> from sympy import failing_assumptions, Symbol
>>> x = Symbol('x', real=True, positive=True)
>>> y = Symbol('y')
>>> failing_assumptions(6*x + y, real=True, positive=True)
{'positive': None, 'real': None}
>>> failing_assumptions(x**2 - 1, positive=True)
{'positive': None}
If all assumptions satisfy the `expr` an empty dictionary is returned.
>>> failing_assumptions(x**2, positive=True)
{}
"""
expr = sympify(expr)
failed = {}
for key in list(assumptions.keys()):
test = getattr(expr, 'is_%s' % key, None)
if test is not assumptions[key]:
failed[key] = test
return failed # {} or {assumption: value != desired}
def check_assumptions(expr, against=None, **assumptions):
"""Checks whether expression `expr` satisfies all assumptions.
`assumptions` is a dict of assumptions: {'assumption': True|False, ...}.
Examples
========
>>> from sympy import Symbol, pi, I, exp, check_assumptions
>>> check_assumptions(-5, integer=True)
True
>>> check_assumptions(pi, real=True, integer=False)
True
>>> check_assumptions(pi, real=True, negative=True)
False
>>> check_assumptions(exp(I*pi/7), real=False)
True
>>> x = Symbol('x', real=True, positive=True)
>>> check_assumptions(2*x + 1, real=True, positive=True)
True
>>> check_assumptions(-2*x - 5, real=True, positive=True)
False
To check assumptions of ``expr`` against another variable or expression,
pass the expression or variable as ``against``.
>>> check_assumptions(2*x + 1, x)
True
`None` is returned if check_assumptions() could not conclude.
>>> check_assumptions(2*x - 1, real=True, positive=True)
>>> z = Symbol('z')
>>> check_assumptions(z, real=True)
See Also
========
failing_assumptions
"""
expr = sympify(expr)
if against:
if not isinstance(against, Symbol):
raise TypeError('against should be of type Symbol')
if assumptions:
raise AssertionError('No assumptions should be specified')
assumptions = against.assumptions0
def _test(key):
v = getattr(expr, 'is_' + key, None)
if v is not None:
return assumptions[key] is v
return fuzzy_and(_test(key) for key in assumptions)
def solve(f, *symbols, **flags):
r"""
Algebraically solves equations and systems of equations.
Currently supported are:
- polynomial,
- transcendental
- piecewise combinations of the above
- systems of linear and polynomial equations
- systems containing relational expressions.
Input is formed as:
* f
- a single Expr or Poly that must be zero,
- an Equality
- a Relational expression
- a Boolean
- iterable of one or more of the above
* symbols (object(s) to solve for) specified as
- none given (other non-numeric objects will be used)
- single symbol
- denested list of symbols
e.g. solve(f, x, y)
- ordered iterable of symbols
e.g. solve(f, [x, y])
* flags
'dict'=True (default is False)
return list (perhaps empty) of solution mappings
'set'=True (default is False)
return list of symbols and set of tuple(s) of solution(s)
'exclude=[] (default)'
don't try to solve for any of the free symbols in exclude;
if expressions are given, the free symbols in them will
be extracted automatically.
'check=True (default)'
If False, don't do any testing of solutions. This can be
useful if one wants to include solutions that make any
denominator zero.
'numerical=True (default)'
do a fast numerical check if ``f`` has only one symbol.
'minimal=True (default is False)'
a very fast, minimal testing.
'warn=True (default is False)'
show a warning if checksol() could not conclude.
'simplify=True (default)'
simplify all but polynomials of order 3 or greater before
returning them and (if check is not False) use the
general simplify function on the solutions and the
expression obtained when they are substituted into the
function which should be zero
'force=True (default is False)'
make positive all symbols without assumptions regarding sign.
'rational=True (default)'
recast Floats as Rational; if this option is not used, the
system containing floats may fail to solve because of issues
with polys. If rational=None, Floats will be recast as
rationals but the answer will be recast as Floats. If the
flag is False then nothing will be done to the Floats.
'manual=True (default is False)'
do not use the polys/matrix method to solve a system of
equations, solve them one at a time as you might "manually"
'implicit=True (default is False)'
allows solve to return a solution for a pattern in terms of
other functions that contain that pattern; this is only
needed if the pattern is inside of some invertible function
like cos, exp, ....
'particular=True (default is False)'
instructs solve to try to find a particular solution to a linear
system with as many zeros as possible; this is very expensive
'quick=True (default is False)'
when using particular=True, use a fast heuristic instead to find a
solution with many zeros (instead of using the very slow method
guaranteed to find the largest number of zeros possible)
'cubics=True (default)'
return explicit solutions when cubic expressions are encountered
'quartics=True (default)'
return explicit solutions when quartic expressions are encountered
'quintics=True (default)'
return explicit solutions (if possible) when quintic expressions
are encountered
Examples
========
The output varies according to the input and can be seen by example::
>>> from sympy import solve, Poly, Eq, Function, exp
>>> from sympy.abc import x, y, z, a, b
>>> f = Function('f')
* boolean or univariate Relational
>>> solve(x < 3)
(-oo < x) & (x < 3)
* to always get a list of solution mappings, use flag dict=True
>>> solve(x - 3, dict=True)
[{x: 3}]
>>> sol = solve([x - 3, y - 1], dict=True)
>>> sol
[{x: 3, y: 1}]
>>> sol[0][x]
3
>>> sol[0][y]
1
* to get a list of symbols and set of solution(s) use flag set=True
>>> solve([x**2 - 3, y - 1], set=True)
([x, y], {(-sqrt(3), 1), (sqrt(3), 1)})
* single expression and single symbol that is in the expression
>>> solve(x - y, x)
[y]
>>> solve(x - 3, x)
[3]
>>> solve(Eq(x, 3), x)
[3]
>>> solve(Poly(x - 3), x)
[3]
>>> solve(x**2 - y**2, x, set=True)
([x], {(-y,), (y,)})
>>> solve(x**4 - 1, x, set=True)
([x], {(-1,), (1,), (-I,), (I,)})
* single expression with no symbol that is in the expression
>>> solve(3, x)
[]
>>> solve(x - 3, y)
[]
* single expression with no symbol given
In this case, all free symbols will be selected as potential
symbols to solve for. If the equation is univariate then a list
of solutions is returned; otherwise -- as is the case when symbols are
given as an iterable of length > 1 -- a list of mappings will be returned.
>>> solve(x - 3)
[3]
>>> solve(x**2 - y**2)
[{x: -y}, {x: y}]
>>> solve(z**2*x**2 - z**2*y**2)
[{x: -y}, {x: y}, {z: 0}]
>>> solve(z**2*x - z**2*y**2)
[{x: y**2}, {z: 0}]
* when an object other than a Symbol is given as a symbol, it is
isolated algebraically and an implicit solution may be obtained.
This is mostly provided as a convenience to save one from replacing
the object with a Symbol and solving for that Symbol. It will only
work if the specified object can be replaced with a Symbol using the
subs method.
>>> solve(f(x) - x, f(x))
[x]
>>> solve(f(x).diff(x) - f(x) - x, f(x).diff(x))
[x + f(x)]
>>> solve(f(x).diff(x) - f(x) - x, f(x))
[-x + Derivative(f(x), x)]
>>> solve(x + exp(x)**2, exp(x), set=True)
([exp(x)], {(-sqrt(-x),), (sqrt(-x),)})
>>> from sympy import Indexed, IndexedBase, Tuple, sqrt
>>> A = IndexedBase('A')
>>> eqs = Tuple(A[1] + A[2] - 3, A[1] - A[2] + 1)
>>> solve(eqs, eqs.atoms(Indexed))
{A[1]: 1, A[2]: 2}
* To solve for a *symbol* implicitly, use 'implicit=True':
>>> solve(x + exp(x), x)
[-LambertW(1)]
>>> solve(x + exp(x), x, implicit=True)
[-exp(x)]
* It is possible to solve for anything that can be targeted with
subs:
>>> solve(x + 2 + sqrt(3), x + 2)
[-sqrt(3)]
>>> solve((x + 2 + sqrt(3), x + 4 + y), y, x + 2)
{y: -2 + sqrt(3), x + 2: -sqrt(3)}
* Nothing heroic is done in this implicit solving so you may end up
with a symbol still in the solution:
>>> eqs = (x*y + 3*y + sqrt(3), x + 4 + y)
>>> solve(eqs, y, x + 2)
{y: -sqrt(3)/(x + 3), x + 2: (-2*x - 6 + sqrt(3))/(x + 3)}
>>> solve(eqs, y*x, x)
{x: -y - 4, x*y: -3*y - sqrt(3)}
* if you attempt to solve for a number remember that the number
you have obtained does not necessarily mean that the value is
equivalent to the expression obtained:
>>> solve(sqrt(2) - 1, 1)
[sqrt(2)]
>>> solve(x - y + 1, 1) # /!\ -1 is targeted, too
[x/(y - 1)]
>>> [_.subs(z, -1) for _ in solve((x - y + 1).subs(-1, z), 1)]
[-x + y]
* To solve for a function within a derivative, use dsolve.
* single expression and more than 1 symbol
* when there is a linear solution
>>> solve(x - y**2, x, y)
[(y**2, y)]
>>> solve(x**2 - y, x, y)
[(x, x**2)]
>>> solve(x**2 - y, x, y, dict=True)
[{y: x**2}]
* when undetermined coefficients are identified
* that are linear
>>> solve((a + b)*x - b + 2, a, b)
{a: -2, b: 2}
* that are nonlinear
>>> solve((a + b)*x - b**2 + 2, a, b, set=True)
([a, b], {(-sqrt(2), sqrt(2)), (sqrt(2), -sqrt(2))})
* if there is no linear solution then the first successful
attempt for a nonlinear solution will be returned
>>> solve(x**2 - y**2, x, y, dict=True)
[{x: -y}, {x: y}]
>>> solve(x**2 - y**2/exp(x), x, y, dict=True)
[{x: 2*LambertW(-y/2)}, {x: 2*LambertW(y/2)}]
>>> solve(x**2 - y**2/exp(x), y, x)
[(-x*sqrt(exp(x)), x), (x*sqrt(exp(x)), x)]
* iterable of one or more of the above
* involving relationals or bools
>>> solve([x < 3, x - 2])
Eq(x, 2)
>>> solve([x > 3, x - 2])
False
* when the system is linear
* with a solution
>>> solve([x - 3], x)
{x: 3}
>>> solve((x + 5*y - 2, -3*x + 6*y - 15), x, y)
{x: -3, y: 1}
>>> solve((x + 5*y - 2, -3*x + 6*y - 15), x, y, z)
{x: -3, y: 1}
>>> solve((x + 5*y - 2, -3*x + 6*y - z), z, x, y)
{x: 2 - 5*y, z: 21*y - 6}
* without a solution
>>> solve([x + 3, x - 3])
[]
* when the system is not linear
>>> solve([x**2 + y -2, y**2 - 4], x, y, set=True)
([x, y], {(-2, -2), (0, 2), (2, -2)})
* if no symbols are given, all free symbols will be selected and a list
of mappings returned
>>> solve([x - 2, x**2 + y])
[{x: 2, y: -4}]
>>> solve([x - 2, x**2 + f(x)], {f(x), x})
[{x: 2, f(x): -4}]
* if any equation doesn't depend on the symbol(s) given it will be
eliminated from the equation set and an answer may be given
implicitly in terms of variables that were not of interest
>>> solve([x - y, y - 3], x)
{x: y}
Notes
=====
solve() with check=True (default) will run through the symbol tags to
elimate unwanted solutions. If no assumptions are included all possible
solutions will be returned.
>>> from sympy import Symbol, solve
>>> x = Symbol("x")
>>> solve(x**2 - 1)
[-1, 1]
By using the positive tag only one solution will be returned:
>>> pos = Symbol("pos", positive=True)
>>> solve(pos**2 - 1)
[1]
Assumptions aren't checked when `solve()` input involves
relationals or bools.
When the solutions are checked, those that make any denominator zero
are automatically excluded. If you do not want to exclude such solutions
then use the check=False option:
>>> from sympy import sin, limit
>>> solve(sin(x)/x) # 0 is excluded
[pi]
If check=False then a solution to the numerator being zero is found: x = 0.
In this case, this is a spurious solution since sin(x)/x has the well known
limit (without dicontinuity) of 1 at x = 0:
>>> solve(sin(x)/x, check=False)
[0, pi]
In the following case, however, the limit exists and is equal to the
value of x = 0 that is excluded when check=True:
>>> eq = x**2*(1/x - z**2/x)
>>> solve(eq, x)
[]
>>> solve(eq, x, check=False)
[0]
>>> limit(eq, x, 0, '-')
0
>>> limit(eq, x, 0, '+')
0
Disabling high-order, explicit solutions
----------------------------------------
When solving polynomial expressions, one might not want explicit solutions
(which can be quite long). If the expression is univariate, CRootOf
instances will be returned instead:
>>> solve(x**3 - x + 1)
[-1/((-1/2 - sqrt(3)*I/2)*(3*sqrt(69)/2 + 27/2)**(1/3)) - (-1/2 -
sqrt(3)*I/2)*(3*sqrt(69)/2 + 27/2)**(1/3)/3, -(-1/2 +
sqrt(3)*I/2)*(3*sqrt(69)/2 + 27/2)**(1/3)/3 - 1/((-1/2 +
sqrt(3)*I/2)*(3*sqrt(69)/2 + 27/2)**(1/3)), -(3*sqrt(69)/2 +
27/2)**(1/3)/3 - 1/(3*sqrt(69)/2 + 27/2)**(1/3)]
>>> solve(x**3 - x + 1, cubics=False)
[CRootOf(x**3 - x + 1, 0),
CRootOf(x**3 - x + 1, 1),
CRootOf(x**3 - x + 1, 2)]
If the expression is multivariate, no solution might be returned:
>>> solve(x**3 - x + a, x, cubics=False)
[]
Sometimes solutions will be obtained even when a flag is False because the
expression could be factored. In the following example, the equation can
be factored as the product of a linear and a quadratic factor so explicit
solutions (which did not require solving a cubic expression) are obtained:
>>> eq = x**3 + 3*x**2 + x - 1
>>> solve(eq, cubics=False)
[-1, -1 + sqrt(2), -sqrt(2) - 1]
Solving equations involving radicals
------------------------------------
Because of SymPy's use of the principle root (issue #8789), some solutions
to radical equations will be missed unless check=False:
>>> from sympy import root
>>> eq = root(x**3 - 3*x**2, 3) + 1 - x
>>> solve(eq)
[]
>>> solve(eq, check=False)
[1/3]
In the above example there is only a single solution to the
equation. Other expressions will yield spurious roots which
must be checked manually; roots which give a negative argument
to odd-powered radicals will also need special checking:
>>> from sympy import real_root, S
>>> eq = root(x, 3) - root(x, 5) + S(1)/7
>>> solve(eq) # this gives 2 solutions but misses a 3rd
[CRootOf(7*_p**5 - 7*_p**3 + 1, 1)**15,
CRootOf(7*_p**5 - 7*_p**3 + 1, 2)**15]
>>> sol = solve(eq, check=False)
>>> [abs(eq.subs(x,i).n(2)) for i in sol]
[0.48, 0.e-110, 0.e-110, 0.052, 0.052]
The first solution is negative so real_root must be used to see
that it satisfies the expression:
>>> abs(real_root(eq.subs(x, sol[0])).n(2))
0.e-110
If the roots of the equation are not real then more care will be
necessary to find the roots, especially for higher order equations.
Consider the following expression:
>>> expr = root(x, 3) - root(x, 5)
We will construct a known value for this expression at x = 3 by selecting
the 1-th root for each radical:
>>> expr1 = root(x, 3, 1) - root(x, 5, 1)
>>> v = expr1.subs(x, -3)
The solve function is unable to find any exact roots to this equation:
>>> eq = Eq(expr, v); eq1 = Eq(expr1, v)
>>> solve(eq, check=False), solve(eq1, check=False)
([], [])
The function unrad, however, can be used to get a form of the equation for
which numerical roots can be found:
>>> from sympy.solvers.solvers import unrad
>>> from sympy import nroots
>>> e, (p, cov) = unrad(eq)
>>> pvals = nroots(e)
>>> inversion = solve(cov, x)[0]
>>> xvals = [inversion.subs(p, i) for i in pvals]
Although eq or eq1 could have been used to find xvals, the solution can
only be verified with expr1:
>>> z = expr - v
>>> [xi.n(chop=1e-9) for xi in xvals if abs(z.subs(x, xi).n()) < 1e-9]
[]
>>> z1 = expr1 - v
>>> [xi.n(chop=1e-9) for xi in xvals if abs(z1.subs(x, xi).n()) < 1e-9]
[-3.0]
See Also
========
- rsolve() for solving recurrence relationships
- dsolve() for solving differential equations
"""
# keeping track of how f was passed since if it is a list
# a dictionary of results will be returned.
###########################################################################
def _sympified_list(w):
return list(map(sympify, w if iterable(w) else [w]))
bare_f = not iterable(f)
ordered_symbols = (symbols and
symbols[0] and
(isinstance(symbols[0], Symbol) or
is_sequence(symbols[0],
include=GeneratorType)
)
)
f, symbols = (_sympified_list(w) for w in [f, symbols])
if isinstance(f, list):
f = [s for s in f if s is not S.true and s is not True]
implicit = flags.get('implicit', False)
# preprocess symbol(s)
###########################################################################
if not symbols:
# get symbols from equations
symbols = set().union(*[fi.free_symbols for fi in f])
if len(symbols) < len(f):
for fi in f:
pot = preorder_traversal(fi)
for p in pot:
if isinstance(p, AppliedUndef):
flags['dict'] = True # better show symbols
symbols.add(p)
pot.skip() # don't go any deeper
symbols = list(symbols)
ordered_symbols = False
elif len(symbols) == 1 and iterable(symbols[0]):
symbols = symbols[0]
# remove symbols the user is not interested in
exclude = flags.pop('exclude', set())
if exclude:
if isinstance(exclude, Expr):
exclude = [exclude]
exclude = set().union(*[e.free_symbols for e in sympify(exclude)])
symbols = [s for s in symbols if s not in exclude]
# preprocess equation(s)
###########################################################################
for i, fi in enumerate(f):
if isinstance(fi, (Equality, Unequality)):
if 'ImmutableDenseMatrix' in [type(a).__name__ for a in fi.args]:
fi = fi.lhs - fi.rhs
else:
args = fi.args
if args[1] in (S.true, S.false):
args = args[1], args[0]
L, R = args
if L in (S.false, S.true):
if isinstance(fi, Unequality):
L = ~L
if R.is_Relational:
fi = ~R if L is S.false else R
elif R.is_Symbol:
return L
elif R.is_Boolean and (~R).is_Symbol:
return ~L
else:
raise NotImplementedError(filldedent('''
Unanticipated argument of Eq when other arg
is True or False.
'''))
else:
fi = fi.rewrite(Add, evaluate=False)
f[i] = fi
if fi.is_Relational:
return reduce_inequalities(f, symbols=symbols)
if isinstance(fi, Poly):
f[i] = fi.as_expr()
# rewrite hyperbolics in terms of exp
f[i] = f[i].replace(lambda w: isinstance(w, HyperbolicFunction),
lambda w: w.rewrite(exp))
# if we have a Matrix, we need to iterate over its elements again
if f[i].is_Matrix:
bare_f = False
f.extend(list(f[i]))
f[i] = S.Zero
# if we can split it into real and imaginary parts then do so
freei = f[i].free_symbols
if freei and all(s.is_extended_real or s.is_imaginary for s in freei):
fr, fi = f[i].as_real_imag()
# accept as long as new re, im, arg or atan2 are not introduced
had = f[i].atoms(re, im, arg, atan2)
if fr and fi and fr != fi and not any(
i.atoms(re, im, arg, atan2) - had for i in (fr, fi)):
if bare_f:
bare_f = False
f[i: i + 1] = [fr, fi]
# real/imag handling -----------------------------
if any(isinstance(fi, (bool, BooleanAtom)) for fi in f):
if flags.get('set', False):
return [], set()
return []
for i, fi in enumerate(f):
# Abs
fi = fi.replace(Abs, lambda arg:
separatevars(Abs(arg)) if arg.has(*symbols) else Abs(arg))
fi = fi.replace(Abs, lambda arg:
Abs(arg).rewrite(Piecewise) if arg.has(*symbols) else Abs(arg))
for e in fi.find(Abs):
if e.has(*symbols):
raise NotImplementedError('solving %s when the argument '
'is not real or imaginary.' % e)
# arg
_arg = [a for a in fi.atoms(arg) if a.has(*symbols)]
fi = fi.xreplace(dict(list(zip(_arg,
[atan(im(a.args[0])/re(a.args[0])) for a in _arg]))))
# save changes
f[i] = fi
# see if re(s) or im(s) appear
irf = []
for s in symbols:
if s.is_extended_real or s.is_imaginary:
continue # neither re(x) nor im(x) will appear
# if re(s) or im(s) appear, the auxiliary equation must be present
if any(fi.has(re(s), im(s)) for fi in f):
irf.append((s, re(s) + S.ImaginaryUnit*im(s)))
if irf:
for s, rhs in irf:
for i, fi in enumerate(f):
f[i] = fi.xreplace({s: rhs})
f.append(s - rhs)
symbols.extend([re(s), im(s)])
if bare_f:
bare_f = False
flags['dict'] = True
# end of real/imag handling -----------------------------
symbols = list(uniq(symbols))
if not ordered_symbols:
# we do this to make the results returned canonical in case f
# contains a system of nonlinear equations; all other cases should
# be unambiguous
symbols = sorted(symbols, key=default_sort_key)
# we can solve for non-symbol entities by replacing them with Dummy symbols
f, symbols, swap_sym = recast_to_symbols(f, symbols)
# this is needed in the next two events
symset = set(symbols)
# get rid of equations that have no symbols of interest; we don't
# try to solve them because the user didn't ask and they might be
# hard to solve; this means that solutions may be given in terms
# of the eliminated equations e.g. solve((x-y, y-3), x) -> {x: y}
newf = []
for fi in f:
# let the solver handle equations that..
# - have no symbols but are expressions
# - have symbols of interest
# - have no symbols of interest but are constant
# but when an expression is not constant and has no symbols of
# interest, it can't change what we obtain for a solution from
# the remaining equations so we don't include it; and if it's
# zero it can be removed and if it's not zero, there is no
# solution for the equation set as a whole
#
# The reason for doing this filtering is to allow an answer
# to be obtained to queries like solve((x - y, y), x); without
# this mod the return value is []
ok = False
if fi.has(*symset):
ok = True
else:
if fi.is_number:
if fi.is_Number:
if fi.is_zero:
continue
return []
ok = True
else:
if fi.is_constant():
ok = True
if ok:
newf.append(fi)
if not newf:
return []
f = newf
del newf
# mask off any Object that we aren't going to invert: Derivative,
# Integral, etc... so that solving for anything that they contain will
# give an implicit solution
seen = set()
non_inverts = set()
for fi in f:
pot = preorder_traversal(fi)
for p in pot:
if not isinstance(p, Expr) or isinstance(p, Piecewise):
pass
elif (isinstance(p, bool) or
not p.args or
p in symset or
p.is_Add or p.is_Mul or
p.is_Pow and not implicit or
p.is_Function and not implicit) and p.func not in (re, im):
continue
elif not p in seen:
seen.add(p)
if p.free_symbols & symset:
non_inverts.add(p)
else:
continue
pot.skip()
del seen
non_inverts = dict(list(zip(non_inverts, [Dummy() for _ in non_inverts])))
f = [fi.subs(non_inverts) for fi in f]
# Both xreplace and subs are needed below: xreplace to force substitution
# inside Derivative, subs to handle non-straightforward substitutions
non_inverts = [(v, k.xreplace(swap_sym).subs(swap_sym)) for k, v in non_inverts.items()]
# rationalize Floats
floats = False
if flags.get('rational', True) is not False:
for i, fi in enumerate(f):
if fi.has(Float):
floats = True
f[i] = nsimplify(fi, rational=True)
# capture any denominators before rewriting since
# they may disappear after the rewrite, e.g. issue 14779
flags['_denominators'] = _simple_dens(f[0], symbols)
# Any embedded piecewise functions need to be brought out to the
# top level so that the appropriate strategy gets selected.
# However, this is necessary only if one of the piecewise
# functions depends on one of the symbols we are solving for.
def _has_piecewise(e):
if e.is_Piecewise:
return e.has(*symbols)
return any([_has_piecewise(a) for a in e.args])
for i, fi in enumerate(f):
if _has_piecewise(fi):
f[i] = piecewise_fold(fi)
#
# try to get a solution
###########################################################################
if bare_f:
solution = _solve(f[0], *symbols, **flags)
else:
solution = _solve_system(f, symbols, **flags)
#
# postprocessing
###########################################################################
# Restore masked-off objects
if non_inverts:
def _do_dict(solution):
return {k: v.subs(non_inverts) for k, v in
solution.items()}
for i in range(1):
if isinstance(solution, dict):
solution = _do_dict(solution)
break
elif solution and isinstance(solution, list):
if isinstance(solution[0], dict):
solution = [_do_dict(s) for s in solution]
break
elif isinstance(solution[0], tuple):
solution = [tuple([v.subs(non_inverts) for v in s]) for s
in solution]
break
else:
solution = [v.subs(non_inverts) for v in solution]
break
elif not solution:
break
else:
raise NotImplementedError(filldedent('''
no handling of %s was implemented''' % solution))
# Restore original "symbols" if a dictionary is returned.
# This is not necessary for
# - the single univariate equation case
# since the symbol will have been removed from the solution;
# - the nonlinear poly_system since that only supports zero-dimensional
# systems and those results come back as a list
#
# ** unless there were Derivatives with the symbols, but those were handled
# above.
if swap_sym:
symbols = [swap_sym.get(k, k) for k in symbols]
if isinstance(solution, dict):
solution = {swap_sym.get(k, k): v.subs(swap_sym)
for k, v in solution.items()}
elif solution and isinstance(solution, list) and isinstance(solution[0], dict):
for i, sol in enumerate(solution):
solution[i] = {swap_sym.get(k, k): v.subs(swap_sym)
for k, v in sol.items()}
# undo the dictionary solutions returned when the system was only partially
# solved with poly-system if all symbols are present
if (
not flags.get('dict', False) and
solution and
ordered_symbols and
not isinstance(solution, dict) and
all(isinstance(sol, dict) for sol in solution)
):
solution = [tuple([r.get(s, s).subs(r) for s in symbols])
for r in solution]
# Get assumptions about symbols, to filter solutions.
# Note that if assumptions about a solution can't be verified, it is still
# returned.
check = flags.get('check', True)
# restore floats
if floats and solution and flags.get('rational', None) is None:
solution = nfloat(solution, exponent=False)
if check and solution: # assumption checking
warn = flags.get('warn', False)
got_None = [] # solutions for which one or more symbols gave None
no_False = [] # solutions for which no symbols gave False
if isinstance(solution, tuple):
# this has already been checked and is in as_set form
return solution
elif isinstance(solution, list):
if isinstance(solution[0], tuple):
for sol in solution:
for symb, val in zip(symbols, sol):
test = check_assumptions(val, **symb.assumptions0)
if test is False:
break
if test is None:
got_None.append(sol)
else:
no_False.append(sol)
elif isinstance(solution[0], dict):
for sol in solution:
a_None = False
for symb, val in sol.items():
test = check_assumptions(val, **symb.assumptions0)
if test:
continue
if test is False:
break
a_None = True
else:
no_False.append(sol)
if a_None:
got_None.append(sol)
else: # list of expressions
for sol in solution:
test = check_assumptions(sol, **symbols[0].assumptions0)
if test is False:
continue
no_False.append(sol)
if test is None:
got_None.append(sol)
elif isinstance(solution, dict):
a_None = False
for symb, val in solution.items():
test = check_assumptions(val, **symb.assumptions0)
if test:
continue
if test is False:
no_False = None
break
a_None = True
else:
no_False = solution
if a_None:
got_None.append(solution)
elif isinstance(solution, (Relational, And, Or)):
if len(symbols) != 1:
raise ValueError("Length should be 1")
if warn and symbols[0].assumptions0:
warnings.warn(filldedent("""
\tWarning: assumptions about variable '%s' are
not handled currently.""" % symbols[0]))
# TODO: check also variable assumptions for inequalities
else:
raise TypeError('Unrecognized solution') # improve the checker
solution = no_False
if warn and got_None:
warnings.warn(filldedent("""
\tWarning: assumptions concerning following solution(s)
can't be checked:""" + '\n\t' +
', '.join(str(s) for s in got_None)))
#
# done
###########################################################################
as_dict = flags.get('dict', False)
as_set = flags.get('set', False)
if not as_set and isinstance(solution, list):
# Make sure that a list of solutions is ordered in a canonical way.
solution.sort(key=default_sort_key)
if not as_dict and not as_set:
return solution or []
# return a list of mappings or []
if not solution:
solution = []
else:
if isinstance(solution, dict):
solution = [solution]
elif iterable(solution[0]):
solution = [dict(list(zip(symbols, s))) for s in solution]
elif isinstance(solution[0], dict):
pass
else:
if len(symbols) != 1:
raise ValueError("Length should be 1")
solution = [{symbols[0]: s} for s in solution]
if as_dict:
return solution
assert as_set
if not solution:
return [], set()
k = list(ordered(solution[0].keys()))
return k, {tuple([s[ki] for ki in k]) for s in solution}
def _solve(f, *symbols, **flags):
"""Return a checked solution for f in terms of one or more of the
symbols. A list should be returned except for the case when a linear
undetermined-coefficients equation is encountered (in which case
a dictionary is returned).
If no method is implemented to solve the equation, a NotImplementedError
will be raised. In the case that conversion of an expression to a Poly
gives None a ValueError will be raised."""
not_impl_msg = "No algorithms are implemented to solve equation %s"
if len(symbols) != 1:
soln = None
free = f.free_symbols
ex = free - set(symbols)
if len(ex) != 1:
ind, dep = f.as_independent(*symbols)
ex = ind.free_symbols & dep.free_symbols
if len(ex) == 1:
ex = ex.pop()
try:
# soln may come back as dict, list of dicts or tuples, or
# tuple of symbol list and set of solution tuples
soln = solve_undetermined_coeffs(f, symbols, ex, **flags)
except NotImplementedError:
pass
if soln:
if flags.get('simplify', True):
if isinstance(soln, dict):
for k in soln:
soln[k] = simplify(soln[k])
elif isinstance(soln, list):
if isinstance(soln[0], dict):
for d in soln:
for k in d:
d[k] = simplify(d[k])
elif isinstance(soln[0], tuple):
soln = [tuple(simplify(i) for i in j) for j in soln]
else:
raise TypeError('unrecognized args in list')
elif isinstance(soln, tuple):
sym, sols = soln
soln = sym, {tuple(simplify(i) for i in j) for j in sols}
else:
raise TypeError('unrecognized solution type')
return soln
# find first successful solution
failed = []
got_s = set([])
result = []
for s in symbols:
xi, v = solve_linear(f, symbols=[s])
if xi == s:
# no need to check but we should simplify if desired
if flags.get('simplify', True):
v = simplify(v)
vfree = v.free_symbols
if got_s and any([ss in vfree for ss in got_s]):
# sol depends on previously solved symbols: discard it
continue
got_s.add(xi)
result.append({xi: v})
elif xi: # there might be a non-linear solution if xi is not 0
failed.append(s)
if not failed:
return result
for s in failed:
try:
soln = _solve(f, s, **flags)
for sol in soln:
if got_s and any([ss in sol.free_symbols for ss in got_s]):
# sol depends on previously solved symbols: discard it
continue
got_s.add(s)
result.append({s: sol})
except NotImplementedError:
continue
if got_s:
return result
else:
raise NotImplementedError(not_impl_msg % f)
symbol = symbols[0]
# /!\ capture this flag then set it to False so that no checking in
# recursive calls will be done; only the final answer is checked
flags['check'] = checkdens = check = flags.pop('check', True)
# build up solutions if f is a Mul
if f.is_Mul:
result = set()
for m in f.args:
if m in set([S.NegativeInfinity, S.ComplexInfinity, S.Infinity]):
result = set()
break
soln = _solve(m, symbol, **flags)
result.update(set(soln))
result = list(result)
if check:
# all solutions have been checked but now we must
# check that the solutions do not set denominators
# in any factor to zero
dens = flags.get('_denominators', _simple_dens(f, symbols))
result = [s for s in result if
all(not checksol(den, {symbol: s}, **flags) for den in
dens)]
# set flags for quick exit at end; solutions for each
# factor were already checked and simplified
check = False
flags['simplify'] = False
elif f.is_Piecewise:
result = set()
for i, (expr, cond) in enumerate(f.args):
if expr.is_zero:
raise NotImplementedError(
'solve cannot represent interval solutions')
candidates = _solve(expr, symbol, **flags)
# the explicit condition for this expr is the current cond
# and none of the previous conditions
args = [~c for _, c in f.args[:i]] + [cond]
cond = And(*args)
for candidate in candidates:
if candidate in result:
# an unconditional value was already there
continue
try:
v = cond.subs(symbol, candidate)
_eval_simplify = getattr(v, '_eval_simplify', None)
if _eval_simplify is not None:
# unconditionally take the simpification of v
v = _eval_simplify(ratio=2, measure=lambda x: 1)
except TypeError:
# incompatible type with condition(s)
continue
if v == False:
continue
if v == True:
result.add(candidate)
else:
result.add(Piecewise(
(candidate, v),
(S.NaN, True)))
# set flags for quick exit at end; solutions for each
# piece were already checked and simplified
check = False
flags['simplify'] = False
else:
# first see if it really depends on symbol and whether there
# is only a linear solution
f_num, sol = solve_linear(f, symbols=symbols)
if f_num.is_zero or sol is S.NaN:
return []
elif f_num.is_Symbol:
# no need to check but simplify if desired
if flags.get('simplify', True):
sol = simplify(sol)
return [sol]
result = False # no solution was obtained
msg = '' # there is no failure message
# Poly is generally robust enough to convert anything to
# a polynomial and tell us the different generators that it
# contains, so we will inspect the generators identified by
# polys to figure out what to do.
# try to identify a single generator that will allow us to solve this
# as a polynomial, followed (perhaps) by a change of variables if the
# generator is not a symbol
try:
poly = Poly(f_num)
if poly is None:
raise ValueError('could not convert %s to Poly' % f_num)
except GeneratorsNeeded:
simplified_f = simplify(f_num)
if simplified_f != f_num:
return _solve(simplified_f, symbol, **flags)
raise ValueError('expression appears to be a constant')
gens = [g for g in poly.gens if g.has(symbol)]
def _as_base_q(x):
"""Return (b**e, q) for x = b**(p*e/q) where p/q is the leading
Rational of the exponent of x, e.g. exp(-2*x/3) -> (exp(x), 3)
"""
b, e = x.as_base_exp()
if e.is_Rational:
return b, e.q
if not e.is_Mul:
return x, 1
c, ee = e.as_coeff_Mul()
if c.is_Rational and c is not S.One: # c could be a Float
return b**ee, c.q
return x, 1
if len(gens) > 1:
# If there is more than one generator, it could be that the
# generators have the same base but different powers, e.g.
# >>> Poly(exp(x) + 1/exp(x))
# Poly(exp(-x) + exp(x), exp(-x), exp(x), domain='ZZ')
#
# If unrad was not disabled then there should be no rational
# exponents appearing as in
# >>> Poly(sqrt(x) + sqrt(sqrt(x)))
# Poly(sqrt(x) + x**(1/4), sqrt(x), x**(1/4), domain='ZZ')
bases, qs = list(zip(*[_as_base_q(g) for g in gens]))
bases = set(bases)
if len(bases) > 1 or not all(q == 1 for q in qs):
funcs = set(b for b in bases if b.is_Function)
trig = set([_ for _ in funcs if
isinstance(_, TrigonometricFunction)])
other = funcs - trig
if not other and len(funcs.intersection(trig)) > 1:
newf = TR1(f_num).rewrite(tan)
if newf != f_num:
# don't check the rewritten form --check
# solutions in the un-rewritten form below
flags['check'] = False
result = _solve(newf, symbol, **flags)
flags['check'] = check
# just a simple case - see if replacement of single function
# clears all symbol-dependent functions, e.g.
# log(x) - log(log(x) - 1) - 3 can be solved even though it has
# two generators.
if result is False and funcs:
funcs = list(ordered(funcs)) # put shallowest function first
f1 = funcs[0]
t = Dummy('t')
# perform the substitution
ftry = f_num.subs(f1, t)
# if no Functions left, we can proceed with usual solve
if not ftry.has(symbol):
cv_sols = _solve(ftry, t, **flags)
cv_inv = _solve(t - f1, symbol, **flags)[0]
sols = list()
for sol in cv_sols:
sols.append(cv_inv.subs(t, sol))
result = list(ordered(sols))
if result is False:
msg = 'multiple generators %s' % gens
else:
# e.g. case where gens are exp(x), exp(-x)
u = bases.pop()
t = Dummy('t')
inv = _solve(u - t, symbol, **flags)
if isinstance(u, (Pow, exp)):
# this will be resolved by factor in _tsolve but we might
# as well try a simple expansion here to get things in
# order so something like the following will work now without
# having to factor:
#
# >>> eq = (exp(I*(-x-2))+exp(I*(x+2)))
# >>> eq.subs(exp(x),y) # fails
# exp(I*(-x - 2)) + exp(I*(x + 2))
# >>> eq.expand().subs(exp(x),y) # works
# y**I*exp(2*I) + y**(-I)*exp(-2*I)
def _expand(p):
b, e = p.as_base_exp()
e = expand_mul(e)
return expand_power_exp(b**e)
ftry = f_num.replace(
lambda w: w.is_Pow or isinstance(w, exp),
_expand).subs(u, t)
if not ftry.has(symbol):
soln = _solve(ftry, t, **flags)
sols = list()
for sol in soln:
for i in inv:
sols.append(i.subs(t, sol))
result = list(ordered(sols))
elif len(gens) == 1:
# There is only one generator that we are interested in, but
# there may have been more than one generator identified by
# polys (e.g. for symbols other than the one we are interested
# in) so recast the poly in terms of our generator of interest.
# Also use composite=True with f_num since Poly won't update
# poly as documented in issue 8810.
poly = Poly(f_num, gens[0], composite=True)
# if we aren't on the tsolve-pass, use roots
if not flags.pop('tsolve', False):
soln = None
deg = poly.degree()
flags['tsolve'] = True
solvers = {k: flags.get(k, True) for k in
('cubics', 'quartics', 'quintics')}
soln = roots(poly, **solvers)
if sum(soln.values()) < deg:
# e.g. roots(32*x**5 + 400*x**4 + 2032*x**3 +
# 5000*x**2 + 6250*x + 3189) -> {}
# so all_roots is used and RootOf instances are
# returned *unless* the system is multivariate
# or high-order EX domain.
try:
soln = poly.all_roots()
except NotImplementedError:
if not flags.get('incomplete', True):
raise NotImplementedError(
filldedent('''
Neither high-order multivariate polynomials
nor sorting of EX-domain polynomials is supported.
If you want to see any results, pass keyword incomplete=True to
solve; to see numerical values of roots
for univariate expressions, use nroots.
'''))
else:
pass
else:
soln = list(soln.keys())
if soln is not None:
u = poly.gen
if u != symbol:
try:
t = Dummy('t')
iv = _solve(u - t, symbol, **flags)
soln = list(ordered({i.subs(t, s) for i in iv for s in soln}))
except NotImplementedError:
# perhaps _tsolve can handle f_num
soln = None
else:
check = False # only dens need to be checked
if soln is not None:
if len(soln) > 2:
# if the flag wasn't set then unset it since high-order
# results are quite long. Perhaps one could base this
# decision on a certain critical length of the
# roots. In addition, wester test M2 has an expression
# whose roots can be shown to be real with the
# unsimplified form of the solution whereas only one of
# the simplified forms appears to be real.
flags['simplify'] = flags.get('simplify', False)
result = soln
# fallback if above fails
# -----------------------
if result is False:
# try unrad
if flags.pop('_unrad', True):
try:
u = unrad(f_num, symbol)
except (ValueError, NotImplementedError):
u = False
if u:
eq, cov = u
if cov:
isym, ieq = cov
inv = _solve(ieq, symbol, **flags)[0]
rv = {inv.subs(isym, xi) for xi in _solve(eq, isym, **flags)}
else:
try:
rv = set(_solve(eq, symbol, **flags))
except NotImplementedError:
rv = None
if rv is not None:
result = list(ordered(rv))
# if the flag wasn't set then unset it since unrad results
# can be quite long or of very high order
flags['simplify'] = flags.get('simplify', False)
else:
pass # for coverage
# try _tsolve
if result is False:
flags.pop('tsolve', None) # allow tsolve to be used on next pass
try:
soln = _tsolve(f_num, symbol, **flags)
if soln is not None:
result = soln
except PolynomialError:
pass
# ----------- end of fallback ----------------------------
if result is False:
raise NotImplementedError('\n'.join([msg, not_impl_msg % f]))
if flags.get('simplify', True):
result = list(map(simplify, result))
# we just simplified the solution so we now set the flag to
# False so the simplification doesn't happen again in checksol()
flags['simplify'] = False
if checkdens:
# reject any result that makes any denom. affirmatively 0;
# if in doubt, keep it
dens = _simple_dens(f, symbols)
result = [s for s in result if
all(not checksol(d, {symbol: s}, **flags)
for d in dens)]
if check:
# keep only results if the check is not False
result = [r for r in result if
checksol(f_num, {symbol: r}, **flags) is not False]
return result
def _solve_system(exprs, symbols, **flags):
if not exprs:
return []
polys = []
dens = set()
failed = []
result = False
linear = False
manual = flags.get('manual', False)
checkdens = check = flags.get('check', True)
for j, g in enumerate(exprs):
dens.update(_simple_dens(g, symbols))
i, d = _invert(g, *symbols)
g = d - i
g = g.as_numer_denom()[0]
if manual:
failed.append(g)
continue
poly = g.as_poly(*symbols, extension=True)
if poly is not None:
polys.append(poly)
else:
failed.append(g)
if not polys:
solved_syms = []
else:
if all(p.is_linear for p in polys):
n, m = len(polys), len(symbols)
matrix = zeros(n, m + 1)
for i, poly in enumerate(polys):
for monom, coeff in poly.terms():
try:
j = monom.index(1)
matrix[i, j] = coeff
except ValueError:
matrix[i, m] = -coeff
# returns a dictionary ({symbols: values}) or None
if flags.pop('particular', False):
result = minsolve_linear_system(matrix, *symbols, **flags)
else:
result = solve_linear_system(matrix, *symbols, **flags)
if failed:
if result:
solved_syms = list(result.keys())
else:
solved_syms = []
else:
linear = True
else:
if len(symbols) > len(polys):
from sympy.utilities.iterables import subsets
free = set().union(*[p.free_symbols for p in polys])
free = list(ordered(free.intersection(symbols)))
got_s = set()
result = []
for syms in subsets(free, len(polys)):
try:
# returns [] or list of tuples of solutions for syms
res = solve_poly_system(polys, *syms)
if res:
for r in res:
skip = False
for r1 in r:
if got_s and any([ss in r1.free_symbols
for ss in got_s]):
# sol depends on previously
# solved symbols: discard it
skip = True
if not skip:
got_s.update(syms)
result.extend([dict(list(zip(syms, r)))])
except NotImplementedError:
pass
if got_s:
solved_syms = list(got_s)
else:
raise NotImplementedError('no valid subset found')
else:
try:
result = solve_poly_system(polys, *symbols)
if result:
solved_syms = symbols
# we don't know here if the symbols provided
# were given or not, so let solve resolve that.
# A list of dictionaries is going to always be
# returned from here.
result = [dict(list(zip(solved_syms, r))) for r in result]
except NotImplementedError:
failed.extend([g.as_expr() for g in polys])
solved_syms = []
result = None
if result:
if isinstance(result, dict):
result = [result]
else:
result = [{}]
if failed:
# For each failed equation, see if we can solve for one of the
# remaining symbols from that equation. If so, we update the
# solution set and continue with the next failed equation,
# repeating until we are done or we get an equation that can't
# be solved.
def _ok_syms(e, sort=False):
rv = (e.free_symbols - solved_syms) & legal
if sort:
rv = list(rv)
rv.sort(key=default_sort_key)
return rv
solved_syms = set(solved_syms) # set of symbols we have solved for
legal = set(symbols) # what we are interested in
# sort so equation with the fewest potential symbols is first
u = Dummy() # used in solution checking
for eq in ordered(failed, lambda _: len(_ok_syms(_))):
newresult = []
bad_results = []
got_s = set()
hit = False
for r in result:
# update eq with everything that is known so far
eq2 = eq.subs(r)
# if check is True then we see if it satisfies this
# equation, otherwise we just accept it
if check and r:
b = checksol(u, u, eq2, minimal=True)
if b is not None:
# this solution is sufficient to know whether
# it is valid or not so we either accept or
# reject it, then continue
if b:
newresult.append(r)
else:
bad_results.append(r)
continue
# search for a symbol amongst those available that
# can be solved for
ok_syms = _ok_syms(eq2, sort=True)
if not ok_syms:
if r:
newresult.append(r)
break # skip as it's independent of desired symbols
for s in ok_syms:
try:
soln = _solve(eq2, s, **flags)
except NotImplementedError:
continue
# put each solution in r and append the now-expanded
# result in the new result list; use copy since the
# solution for s in being added in-place
for sol in soln:
if got_s and any([ss in sol.free_symbols for ss in got_s]):
# sol depends on previously solved symbols: discard it
continue
rnew = r.copy()
for k, v in r.items():
rnew[k] = v.subs(s, sol)
# and add this new solution
rnew[s] = sol
newresult.append(rnew)
hit = True
got_s.add(s)
if not hit:
raise NotImplementedError('could not solve %s' % eq2)
else:
result = newresult
for b in bad_results:
if b in result:
result.remove(b)
default_simplify = bool(failed) # rely on system-solvers to simplify
if flags.get('simplify', default_simplify):
for r in result:
for k in r:
r[k] = simplify(r[k])
flags['simplify'] = False # don't need to do so in checksol now
if checkdens:
result = [r for r in result
if not any(checksol(d, r, **flags) for d in dens)]
if check and not linear:
result = [r for r in result
if not any(checksol(e, r, **flags) is False for e in exprs)]
result = [r for r in result if r]
if linear and result:
result = result[0]
return result
def solve_linear(lhs, rhs=0, symbols=[], exclude=[]):
r""" Return a tuple derived from f = lhs - rhs that is one of
the following:
(0, 1) meaning that ``f`` is independent of the symbols in
``symbols`` that aren't in ``exclude``, e.g::
>>> from sympy.solvers.solvers import solve_linear
>>> from sympy.abc import x, y, z
>>> from sympy import cos, sin
>>> eq = y*cos(x)**2 + y*sin(x)**2 - y # = y*(1 - 1) = 0
>>> solve_linear(eq)
(0, 1)
>>> eq = cos(x)**2 + sin(x)**2 # = 1
>>> solve_linear(eq)
(0, 1)
>>> solve_linear(x, exclude=[x])
(0, 1)
(0, 0) meaning that there is no solution to the equation
amongst the symbols given.
(If the first element of the tuple is not zero then
the function is guaranteed to be dependent on a symbol
in ``symbols``.)
(symbol, solution) where symbol appears linearly in the
numerator of ``f``, is in ``symbols`` (if given) and is
not in ``exclude`` (if given). No simplification is done
to ``f`` other than a ``mul=True`` expansion, so the
solution will correspond strictly to a unique solution.
``(n, d)`` where ``n`` and ``d`` are the numerator and
denominator of ``f`` when the numerator was not linear
in any symbol of interest; ``n`` will never be a symbol
unless a solution for that symbol was found (in which case
the second element is the solution, not the denominator).
Examples
========
>>> from sympy.core.power import Pow
>>> from sympy.polys.polytools import cancel
The variable ``x`` appears as a linear variable in each of the
following:
>>> solve_linear(x + y**2)
(x, -y**2)
>>> solve_linear(1/x - y**2)
(x, y**(-2))
When not linear in x or y then the numerator and denominator are returned.
>>> solve_linear(x**2/y**2 - 3)
(x**2 - 3*y**2, y**2)
If the numerator of the expression is a symbol then (0, 0) is
returned if the solution for that symbol would have set any
denominator to 0:
>>> eq = 1/(1/x - 2)
>>> eq.as_numer_denom()
(x, 1 - 2*x)
>>> solve_linear(eq)
(0, 0)
But automatic rewriting may cause a symbol in the denominator to
appear in the numerator so a solution will be returned:
>>> (1/x)**-1
x
>>> solve_linear((1/x)**-1)
(x, 0)
Use an unevaluated expression to avoid this:
>>> solve_linear(Pow(1/x, -1, evaluate=False))
(0, 0)
If ``x`` is allowed to cancel in the following expression, then it
appears to be linear in ``x``, but this sort of cancellation is not
done by ``solve_linear`` so the solution will always satisfy the
original expression without causing a division by zero error.
>>> eq = x**2*(1/x - z**2/x)
>>> solve_linear(cancel(eq))
(x, 0)
>>> solve_linear(eq)
(x**2*(1 - z**2), x)
A list of symbols for which a solution is desired may be given:
>>> solve_linear(x + y + z, symbols=[y])
(y, -x - z)
A list of symbols to ignore may also be given:
>>> solve_linear(x + y + z, exclude=[x])
(y, -x - z)
(A solution for ``y`` is obtained because it is the first variable
from the canonically sorted list of symbols that had a linear
solution.)
"""
if isinstance(lhs, Equality):
if rhs:
raise ValueError(filldedent('''
If lhs is an Equality, rhs must be 0 but was %s''' % rhs))
rhs = lhs.rhs
lhs = lhs.lhs
dens = None
eq = lhs - rhs
n, d = eq.as_numer_denom()
if not n:
return S.Zero, S.One
free = n.free_symbols
if not symbols:
symbols = free
else:
bad = [s for s in symbols if not s.is_Symbol]
if bad:
if len(bad) == 1:
bad = bad[0]
if len(symbols) == 1:
eg = 'solve(%s, %s)' % (eq, symbols[0])
else:
eg = 'solve(%s, *%s)' % (eq, list(symbols))
raise ValueError(filldedent('''
solve_linear only handles symbols, not %s. To isolate
non-symbols use solve, e.g. >>> %s <<<.
''' % (bad, eg)))
symbols = free.intersection(symbols)
symbols = symbols.difference(exclude)
if not symbols:
return S.Zero, S.One
# derivatives are easy to do but tricky to analyze to see if they
# are going to disallow a linear solution, so for simplicity we
# just evaluate the ones that have the symbols of interest
derivs = defaultdict(list)
for der in n.atoms(Derivative):
csym = der.free_symbols & symbols
for c in csym:
derivs[c].append(der)
all_zero = True
for xi in sorted(symbols, key=default_sort_key): # canonical order
# if there are derivatives in this var, calculate them now
if isinstance(derivs[xi], list):
derivs[xi] = {der: der.doit() for der in derivs[xi]}
newn = n.subs(derivs[xi])
dnewn_dxi = newn.diff(xi)
# dnewn_dxi can be nonzero if it survives differentation by any
# of its free symbols
free = dnewn_dxi.free_symbols
if dnewn_dxi and (not free or any(dnewn_dxi.diff(s) for s in free)):
all_zero = False
if dnewn_dxi is S.NaN:
break
if xi not in dnewn_dxi.free_symbols:
vi = -1/dnewn_dxi*(newn.subs(xi, 0))
if dens is None:
dens = _simple_dens(eq, symbols)
if not any(checksol(di, {xi: vi}, minimal=True) is True
for di in dens):
# simplify any trivial integral
irep = [(i, i.doit()) for i in vi.atoms(Integral) if
i.function.is_number]
# do a slight bit of simplification
vi = expand_mul(vi.subs(irep))
return xi, vi
if all_zero:
return S.Zero, S.One
if n.is_Symbol: # no solution for this symbol was found
return S.Zero, S.Zero
return n, d
def minsolve_linear_system(system, *symbols, **flags):
r"""
Find a particular solution to a linear system.
In particular, try to find a solution with the minimal possible number
of non-zero variables using a naive algorithm with exponential complexity.
If ``quick=True``, a heuristic is used.
"""
quick = flags.get('quick', False)
# Check if there are any non-zero solutions at all
s0 = solve_linear_system(system, *symbols, **flags)
if not s0 or all(v == 0 for v in s0.values()):
return s0
if quick:
# We just solve the system and try to heuristically find a nice
# solution.
s = solve_linear_system(system, *symbols)
def update(determined, solution):
delete = []
for k, v in solution.items():
solution[k] = v.subs(determined)
if not solution[k].free_symbols:
delete.append(k)
determined[k] = solution[k]
for k in delete:
del solution[k]
determined = {}
update(determined, s)
while s:
# NOTE sort by default_sort_key to get deterministic result
k = max((k for k in s.values()),
key=lambda x: (len(x.free_symbols), default_sort_key(x)))
x = max(k.free_symbols, key=default_sort_key)
if len(k.free_symbols) != 1:
determined[x] = S.Zero
else:
val = solve(k)[0]
if val == 0 and all(v.subs(x, val) == 0 for v in s.values()):
determined[x] = S.One
else:
determined[x] = val
update(determined, s)
return determined
else:
# We try to select n variables which we want to be non-zero.
# All others will be assumed zero. We try to solve the modified system.
# If there is a non-trivial solution, just set the free variables to
# one. If we do this for increasing n, trying all combinations of
# variables, we will find an optimal solution.
# We speed up slightly by starting at one less than the number of
# variables the quick method manages.
from itertools import combinations
from sympy.utilities.misc import debug
N = len(symbols)
bestsol = minsolve_linear_system(system, *symbols, quick=True)
n0 = len([x for x in bestsol.values() if x != 0])
for n in range(n0 - 1, 1, -1):
debug('minsolve: %s' % n)
thissol = None
for nonzeros in combinations(list(range(N)), n):
subm = Matrix([system.col(i).T for i in nonzeros] + [system.col(-1).T]).T
s = solve_linear_system(subm, *[symbols[i] for i in nonzeros])
if s and not all(v == 0 for v in s.values()):
subs = [(symbols[v], S.One) for v in nonzeros]
for k, v in s.items():
s[k] = v.subs(subs)
for sym in symbols:
if sym not in s:
if symbols.index(sym) in nonzeros:
s[sym] = S.One
else:
s[sym] = S.Zero
thissol = s
break
if thissol is None:
break
bestsol = thissol
return bestsol
def solve_linear_system(system, *symbols, **flags):
r"""
Solve system of N linear equations with M variables, which means
both under- and overdetermined systems are supported. The possible
number of solutions is zero, one or infinite. Respectively, this
procedure will return None or a dictionary with solutions. In the
case of underdetermined systems, all arbitrary parameters are skipped.
This may cause a situation in which an empty dictionary is returned.
In that case, all symbols can be assigned arbitrary values.
Input to this functions is a Nx(M+1) matrix, which means it has
to be in augmented form. If you prefer to enter N equations and M
unknowns then use `solve(Neqs, *Msymbols)` instead. Note: a local
copy of the matrix is made by this routine so the matrix that is
passed will not be modified.
The algorithm used here is fraction-free Gaussian elimination,
which results, after elimination, in an upper-triangular matrix.
Then solutions are found using back-substitution. This approach
is more efficient and compact than the Gauss-Jordan method.
>>> from sympy import Matrix, solve_linear_system
>>> from sympy.abc import x, y
Solve the following system::
x + 4 y == 2
-2 x + y == 14
>>> system = Matrix(( (1, 4, 2), (-2, 1, 14)))
>>> solve_linear_system(system, x, y)
{x: -6, y: 2}
A degenerate system returns an empty dictionary.
>>> system = Matrix(( (0,0,0), (0,0,0) ))
>>> solve_linear_system(system, x, y)
{}
"""
do_simplify = flags.get('simplify', True)
if system.rows == system.cols - 1 == len(symbols):
try:
# well behaved n-equations and n-unknowns
inv = inv_quick(system[:, :-1])
rv = dict(zip(symbols, inv*system[:, -1]))
if do_simplify:
for k, v in rv.items():
rv[k] = simplify(v)
if not all(i.is_zero for i in rv.values()):
# non-trivial solution
return rv
except ValueError:
pass
matrix = system[:, :]
syms = list(symbols)
i, m = 0, matrix.cols - 1 # don't count augmentation
while i < matrix.rows:
if i == m:
# an overdetermined system
if any(matrix[i:, m]):
return None # no solutions
else:
# remove trailing rows
matrix = matrix[:i, :]
break
if not matrix[i, i]:
# there is no pivot in current column
# so try to find one in other columns
for k in range(i + 1, m):
if matrix[i, k]:
break
else:
if matrix[i, m]:
# We need to know if this is always zero or not. We
# assume that if there are free symbols that it is not
# identically zero (or that there is more than one way
# to make this zero). Otherwise, if there are none, this
# is a constant and we assume that it does not simplify
# to zero XXX are there better (fast) ways to test this?
# The .equals(0) method could be used but that can be
# slow; numerical testing is prone to errors of scaling.
if not matrix[i, m].free_symbols:
return None # no solution
# A row of zeros with a non-zero rhs can only be accepted
# if there is another equivalent row. Any such rows will
# be deleted.
nrows = matrix.rows
rowi = matrix.row(i)
ip = None
j = i + 1
while j < matrix.rows:
# do we need to see if the rhs of j
# is a constant multiple of i's rhs?
rowj = matrix.row(j)
if rowj == rowi:
matrix.row_del(j)
elif rowj[:-1] == rowi[:-1]:
if ip is None:
_, ip = rowi[-1].as_content_primitive()
_, jp = rowj[-1].as_content_primitive()
if not (simplify(jp - ip) or simplify(jp + ip)):
matrix.row_del(j)
j += 1
if nrows == matrix.rows:
# no solution
return None
# zero row or was a linear combination of
# other rows or was a row with a symbolic
# expression that matched other rows, e.g. [0, 0, x - y]
# so now we can safely skip it
matrix.row_del(i)
if not matrix:
# every choice of variable values is a solution
# so we return an empty dict instead of None
return dict()
continue
# we want to change the order of columns so
# the order of variables must also change
syms[i], syms[k] = syms[k], syms[i]
matrix.col_swap(i, k)
pivot_inv = S.One/matrix[i, i]
# divide all elements in the current row by the pivot
matrix.row_op(i, lambda x, _: x * pivot_inv)
for k in range(i + 1, matrix.rows):
if matrix[k, i]:
coeff = matrix[k, i]
# subtract from the current row the row containing
# pivot and multiplied by extracted coefficient
matrix.row_op(k, lambda x, j: simplify(x - matrix[i, j]*coeff))
i += 1
# if there weren't any problems, augmented matrix is now
# in row-echelon form so we can check how many solutions
# there are and extract them using back substitution
if len(syms) == matrix.rows:
# this system is Cramer equivalent so there is
# exactly one solution to this system of equations
k, solutions = i - 1, {}
while k >= 0:
content = matrix[k, m]
# run back-substitution for variables
for j in range(k + 1, m):
content -= matrix[k, j]*solutions[syms[j]]
if do_simplify:
solutions[syms[k]] = simplify(content)
else:
solutions[syms[k]] = content
k -= 1
return solutions
elif len(syms) > matrix.rows:
# this system will have infinite number of solutions
# dependent on exactly len(syms) - i parameters
k, solutions = i - 1, {}
while k >= 0:
content = matrix[k, m]
# run back-substitution for variables
for j in range(k + 1, i):
content -= matrix[k, j]*solutions[syms[j]]
# run back-substitution for parameters
for j in range(i, m):
content -= matrix[k, j]*syms[j]
if do_simplify:
solutions[syms[k]] = simplify(content)
else:
solutions[syms[k]] = content
k -= 1
return solutions
else:
return [] # no solutions
def solve_undetermined_coeffs(equ, coeffs, sym, **flags):
"""Solve equation of a type p(x; a_1, ..., a_k) == q(x) where both
p, q are univariate polynomials and f depends on k parameters.
The result of this functions is a dictionary with symbolic
values of those parameters with respect to coefficients in q.
This functions accepts both Equations class instances and ordinary
SymPy expressions. Specification of parameters and variable is
obligatory for efficiency and simplicity reason.
>>> from sympy import Eq
>>> from sympy.abc import a, b, c, x
>>> from sympy.solvers import solve_undetermined_coeffs
>>> solve_undetermined_coeffs(Eq(2*a*x + a+b, x), [a, b], x)
{a: 1/2, b: -1/2}
>>> solve_undetermined_coeffs(Eq(a*c*x + a+b, x), [a, b], x)
{a: 1/c, b: -1/c}
"""
if isinstance(equ, Equality):
# got equation, so move all the
# terms to the left hand side
equ = equ.lhs - equ.rhs
equ = cancel(equ).as_numer_denom()[0]
system = list(collect(equ.expand(), sym, evaluate=False).values())
if not any(equ.has(sym) for equ in system):
# consecutive powers in the input expressions have
# been successfully collected, so solve remaining
# system using Gaussian elimination algorithm
return solve(system, *coeffs, **flags)
else:
return None # no solutions
def solve_linear_system_LU(matrix, syms):
"""
Solves the augmented matrix system using LUsolve and returns a dictionary
in which solutions are keyed to the symbols of syms *as ordered*.
The matrix must be invertible.
Examples
========
>>> from sympy import Matrix
>>> from sympy.abc import x, y, z
>>> from sympy.solvers.solvers import solve_linear_system_LU
>>> solve_linear_system_LU(Matrix([
... [1, 2, 0, 1],
... [3, 2, 2, 1],
... [2, 0, 0, 1]]), [x, y, z])
{x: 1/2, y: 1/4, z: -1/2}
See Also
========
sympy.matrices.LUsolve
"""
if matrix.rows != matrix.cols - 1:
raise ValueError("Rows should be equal to columns - 1")
A = matrix[:matrix.rows, :matrix.rows]
b = matrix[:, matrix.cols - 1:]
soln = A.LUsolve(b)
solutions = {}
for i in range(soln.rows):
solutions[syms[i]] = soln[i, 0]
return solutions
def det_perm(M):
"""Return the det(``M``) by using permutations to select factors.
For size larger than 8 the number of permutations becomes prohibitively
large, or if there are no symbols in the matrix, it is better to use the
standard determinant routines, e.g. `M.det()`.
See Also
========
det_minor
det_quick
"""
args = []
s = True
n = M.rows
list_ = getattr(M, '_mat', None)
if list_ is None:
list_ = flatten(M.tolist())
for perm in generate_bell(n):
fac = []
idx = 0
for j in perm:
fac.append(list_[idx + j])
idx += n
term = Mul(*fac) # disaster with unevaluated Mul -- takes forever for n=7
args.append(term if s else -term)
s = not s
return Add(*args)
def det_minor(M):
"""Return the ``det(M)`` computed from minors without
introducing new nesting in products.
See Also
========
det_perm
det_quick
"""
n = M.rows
if n == 2:
return M[0, 0]*M[1, 1] - M[1, 0]*M[0, 1]
else:
return sum([(1, -1)[i % 2]*Add(*[M[0, i]*d for d in
Add.make_args(det_minor(M.minor_submatrix(0, i)))])
if M[0, i] else S.Zero for i in range(n)])
def det_quick(M, method=None):
"""Return ``det(M)`` assuming that either
there are lots of zeros or the size of the matrix
is small. If this assumption is not met, then the normal
Matrix.det function will be used with method = ``method``.
See Also
========
det_minor
det_perm
"""
if any(i.has(Symbol) for i in M):
if M.rows < 8 and all(i.has(Symbol) for i in M):
return det_perm(M)
return det_minor(M)
else:
return M.det(method=method) if method else M.det()
def inv_quick(M):
"""Return the inverse of ``M``, assuming that either
there are lots of zeros or the size of the matrix
is small.
"""
from sympy.matrices import zeros
if not all(i.is_Number for i in M):
if not any(i.is_Number for i in M):
det = lambda _: det_perm(_)
else:
det = lambda _: det_minor(_)
else:
return M.inv()
n = M.rows
d = det(M)
if d == S.Zero:
raise ValueError("Matrix det == 0; not invertible.")
ret = zeros(n)
s1 = -1
for i in range(n):
s = s1 = -s1
for j in range(n):
di = det(M.minor_submatrix(i, j))
ret[j, i] = s*di/d
s = -s
return ret
# these are functions that have multiple inverse values per period
multi_inverses = {
sin: lambda x: (asin(x), S.Pi - asin(x)),
cos: lambda x: (acos(x), 2*S.Pi - acos(x)),
}
def _tsolve(eq, sym, **flags):
"""
Helper for _solve that solves a transcendental equation with respect
to the given symbol. Various equations containing powers and logarithms,
can be solved.
There is currently no guarantee that all solutions will be returned or
that a real solution will be favored over a complex one.
Either a list of potential solutions will be returned or None will be
returned (in the case that no method was known to get a solution
for the equation). All other errors (like the inability to cast an
expression as a Poly) are unhandled.
Examples
========
>>> from sympy import log
>>> from sympy.solvers.solvers import _tsolve as tsolve
>>> from sympy.abc import x
>>> tsolve(3**(2*x + 5) - 4, x)
[-5/2 + log(2)/log(3), (-5*log(3)/2 + log(2) + I*pi)/log(3)]
>>> tsolve(log(x) + 2*x, x)
[LambertW(2)/2]
"""
if 'tsolve_saw' not in flags:
flags['tsolve_saw'] = []
if eq in flags['tsolve_saw']:
return None
else:
flags['tsolve_saw'].append(eq)
rhs, lhs = _invert(eq, sym)
if lhs == sym:
return [rhs]
try:
if lhs.is_Add:
# it's time to try factoring; powdenest is used
# to try get powers in standard form for better factoring
f = factor(powdenest(lhs - rhs))
if f.is_Mul:
return _solve(f, sym, **flags)
if rhs:
f = logcombine(lhs, force=flags.get('force', True))
if f.count(log) != lhs.count(log):
if isinstance(f, log):
return _solve(f.args[0] - exp(rhs), sym, **flags)
return _tsolve(f - rhs, sym, **flags)
elif lhs.is_Pow:
if lhs.exp.is_Integer:
if lhs - rhs != eq:
return _solve(lhs - rhs, sym, **flags)
if sym not in lhs.exp.free_symbols:
return _solve(lhs.base - rhs**(1/lhs.exp), sym, **flags)
# _tsolve calls this with Dummy before passing the actual number in.
if any(t.is_Dummy for t in rhs.free_symbols):
raise NotImplementedError # _tsolve will call here again...
# a ** g(x) == 0
if not rhs:
# f(x)**g(x) only has solutions where f(x) == 0 and g(x) != 0 at
# the same place
sol_base = _solve(lhs.base, sym, **flags)
return [s for s in sol_base if lhs.exp.subs(sym, s) != 0]
# a ** g(x) == b
if not lhs.base.has(sym):
if lhs.base == 0:
return _solve(lhs.exp, sym, **flags) if rhs != 0 else []
# Gets most solutions...
if lhs.base == rhs.as_base_exp()[0]:
# handles case when bases are equal
sol = _solve(lhs.exp - rhs.as_base_exp()[1], sym, **flags)
else:
# handles cases when bases are not equal and exp
# may or may not be equal
sol = _solve(exp(log(lhs.base)*lhs.exp)-exp(log(rhs)), sym, **flags)
# Check for duplicate solutions
def equal(expr1, expr2):
_ = Dummy()
eq = checksol(expr1 - _, _, expr2)
if eq is None:
if nsimplify(expr1) != nsimplify(expr2):
return False
# they might be coincidentally the same
# so check more rigorously
eq = expr1.equals(expr2)
return eq
# Guess a rational exponent
e_rat = nsimplify(log(abs(rhs))/log(abs(lhs.base)))
e_rat = simplify(posify(e_rat)[0])
n, d = fraction(e_rat)
if expand(lhs.base**n - rhs**d) == 0:
sol = [s for s in sol if not equal(lhs.exp.subs(sym, s), e_rat)]
sol.extend(_solve(lhs.exp - e_rat, sym, **flags))
return list(ordered(set(sol)))
# f(x) ** g(x) == c
else:
sol = []
logform = lhs.exp*log(lhs.base) - log(rhs)
if logform != lhs - rhs:
try:
sol.extend(_solve(logform, sym, **flags))
except NotImplementedError:
pass
# Collect possible solutions and check with substitution later.
check = []
if rhs == 1:
# f(x) ** g(x) = 1 -- g(x)=0 or f(x)=+-1
check.extend(_solve(lhs.exp, sym, **flags))
check.extend(_solve(lhs.base - 1, sym, **flags))
check.extend(_solve(lhs.base + 1, sym, **flags))
elif rhs.is_Rational:
for d in (i for i in divisors(abs(rhs.p)) if i != 1):
e, t = integer_log(rhs.p, d)
if not t:
continue # rhs.p != d**b
for s in divisors(abs(rhs.q)):
if s**e== rhs.q:
r = Rational(d, s)
check.extend(_solve(lhs.base - r, sym, **flags))
check.extend(_solve(lhs.base + r, sym, **flags))
check.extend(_solve(lhs.exp - e, sym, **flags))
elif rhs.is_irrational:
b_l, e_l = lhs.base.as_base_exp()
n, d = (e_l*lhs.exp).as_numer_denom()
b, e = sqrtdenest(rhs).as_base_exp()
check = [sqrtdenest(i) for i in (_solve(lhs.base - b, sym, **flags))]
check.extend([sqrtdenest(i) for i in (_solve(lhs.exp - e, sym, **flags))])
if e_l*d != 1:
check.extend(_solve(b_l**n - rhs**(e_l*d), sym, **flags))
for s in check:
ok = checksol(eq, sym, s)
if ok is None:
ok = eq.subs(sym, s).equals(0)
if ok:
sol.append(s)
return list(ordered(set(sol)))
elif lhs.is_Function and len(lhs.args) == 1:
if lhs.func in multi_inverses:
# sin(x) = 1/3 -> x - asin(1/3) & x - (pi - asin(1/3))
soln = []
for i in multi_inverses[lhs.func](rhs):
soln.extend(_solve(lhs.args[0] - i, sym, **flags))
return list(ordered(soln))
elif lhs.func == LambertW:
return _solve(lhs.args[0] - rhs*exp(rhs), sym, **flags)
rewrite = lhs.rewrite(exp)
if rewrite != lhs:
return _solve(rewrite - rhs, sym, **flags)
except NotImplementedError:
pass
# maybe it is a lambert pattern
if flags.pop('bivariate', True):
# lambert forms may need some help being recognized, e.g. changing
# 2**(3*x) + x**3*log(2)**3 + 3*x**2*log(2)**2 + 3*x*log(2) + 1
# to 2**(3*x) + (x*log(2) + 1)**3
g = _filtered_gens(eq.as_poly(), sym)
up_or_log = set()
for gi in g:
if isinstance(gi, exp) or isinstance(gi, log):
up_or_log.add(gi)
elif gi.is_Pow:
gisimp = powdenest(expand_power_exp(gi))
if gisimp.is_Pow and sym in gisimp.exp.free_symbols:
up_or_log.add(gi)
eq_down = expand_log(expand_power_exp(eq)).subs(
dict(list(zip(up_or_log, [0]*len(up_or_log)))))
eq = expand_power_exp(factor(eq_down, deep=True) + (eq - eq_down))
rhs, lhs = _invert(eq, sym)
if lhs.has(sym):
try:
poly = lhs.as_poly()
g = _filtered_gens(poly, sym)
_eq = lhs - rhs
sols = _solve_lambert(_eq, sym, g)
# use a simplified form if it satisfies eq
# and has fewer operations
for n, s in enumerate(sols):
ns = nsimplify(s)
if ns != s and ns.count_ops() <= s.count_ops():
ok = checksol(_eq, sym, ns)
if ok is None:
ok = _eq.subs(sym, ns).equals(0)
if ok:
sols[n] = ns
return sols
except NotImplementedError:
# maybe it's a convoluted function
if len(g) == 2:
try:
gpu = bivariate_type(lhs - rhs, *g)
if gpu is None:
raise NotImplementedError
g, p, u = gpu
flags['bivariate'] = False
inversion = _tsolve(g - u, sym, **flags)
if inversion:
sol = _solve(p, u, **flags)
return list(ordered(set([i.subs(u, s)
for i in inversion for s in sol])))
except NotImplementedError:
pass
else:
pass
if flags.pop('force', True):
flags['force'] = False
pos, reps = posify(lhs - rhs)
for u, s in reps.items():
if s == sym:
break
else:
u = sym
if pos.has(u):
try:
soln = _solve(pos, u, **flags)
return list(ordered([s.subs(reps) for s in soln]))
except NotImplementedError:
pass
else:
pass # here for coverage
return # here for coverage
# TODO: option for calculating J numerically
@conserve_mpmath_dps
def nsolve(*args, **kwargs):
r"""
Solve a nonlinear equation system numerically::
nsolve(f, [args,] x0, modules=['mpmath'], **kwargs)
f is a vector function of symbolic expressions representing the system.
args are the variables. If there is only one variable, this argument can
be omitted.
x0 is a starting vector close to a solution.
Use the modules keyword to specify which modules should be used to
evaluate the function and the Jacobian matrix. Make sure to use a module
that supports matrices. For more information on the syntax, please see the
docstring of lambdify.
If the keyword arguments contain 'dict'=True (default is False) nsolve
will return a list (perhaps empty) of solution mappings. This might be
especially useful if you want to use nsolve as a fallback to solve since
using the dict argument for both methods produces return values of
consistent type structure. Please note: to keep this consistency with
solve, the solution will be returned in a list even though nsolve
(currently at least) only finds one solution at a time.
Overdetermined systems are supported.
>>> from sympy import Symbol, nsolve
>>> import sympy
>>> import mpmath
>>> mpmath.mp.dps = 15
>>> x1 = Symbol('x1')
>>> x2 = Symbol('x2')
>>> f1 = 3 * x1**2 - 2 * x2**2 - 1
>>> f2 = x1**2 - 2 * x1 + x2**2 + 2 * x2 - 8
>>> print(nsolve((f1, f2), (x1, x2), (-1, 1)))
Matrix([[-1.19287309935246], [1.27844411169911]])
For one-dimensional functions the syntax is simplified:
>>> from sympy import sin, nsolve
>>> from sympy.abc import x
>>> nsolve(sin(x), x, 2)
3.14159265358979
>>> nsolve(sin(x), 2)
3.14159265358979
To solve with higher precision than the default, use the prec argument.
>>> from sympy import cos
>>> nsolve(cos(x) - x, 1)
0.739085133215161
>>> nsolve(cos(x) - x, 1, prec=50)
0.73908513321516064165531208767387340401341175890076
>>> cos(_)
0.73908513321516064165531208767387340401341175890076
To solve for complex roots of real functions, a nonreal initial point
must be specified:
>>> from sympy import I
>>> nsolve(x**2 + 2, I)
1.4142135623731*I
mpmath.findroot is used and you can find there more extensive
documentation, especially concerning keyword parameters and
available solvers. Note, however, that functions which are very
steep near the root the verification of the solution may fail. In
this case you should use the flag `verify=False` and
independently verify the solution.
>>> from sympy import cos, cosh
>>> from sympy.abc import i
>>> f = cos(x)*cosh(x) - 1
>>> nsolve(f, 3.14*100)
Traceback (most recent call last):
...
ValueError: Could not find root within given tolerance. (1.39267e+230 > 2.1684e-19)
>>> ans = nsolve(f, 3.14*100, verify=False); ans
312.588469032184
>>> f.subs(x, ans).n(2)
2.1e+121
>>> (f/f.diff(x)).subs(x, ans).n(2)
7.4e-15
One might safely skip the verification if bounds of the root are known
and a bisection method is used:
>>> bounds = lambda i: (3.14*i, 3.14*(i + 1))
>>> nsolve(f, bounds(100), solver='bisect', verify=False)
315.730061685774
Alternatively, a function may be better behaved when the
denominator is ignored. Since this is not always the case, however,
the decision of what function to use is left to the discretion of
the user.
>>> eq = x**2/(1 - x)/(1 - 2*x)**2 - 100
>>> nsolve(eq, 0.46)
Traceback (most recent call last):
...
ValueError: Could not find root within given tolerance. (10000 > 2.1684e-19)
Try another starting point or tweak arguments.
>>> nsolve(eq.as_numer_denom()[0], 0.46)
0.46792545969349058
"""
# there are several other SymPy functions that use method= so
# guard against that here
if 'method' in kwargs:
raise ValueError(filldedent('''
Keyword "method" should not be used in this context. When using
some mpmath solvers directly, the keyword "method" is
used, but when using nsolve (and findroot) the keyword to use is
"solver".'''))
if 'prec' in kwargs:
prec = kwargs.pop('prec')
import mpmath
mpmath.mp.dps = prec
else:
prec = None
# keyword argument to return result as a dictionary
as_dict = kwargs.pop('dict', False)
# interpret arguments
if len(args) == 3:
f = args[0]
fargs = args[1]
x0 = args[2]
if iterable(fargs) and iterable(x0):
if len(x0) != len(fargs):
raise TypeError('nsolve expected exactly %i guess vectors, got %i'
% (len(fargs), len(x0)))
elif len(args) == 2:
f = args[0]
fargs = None
x0 = args[1]
if iterable(f):
raise TypeError('nsolve expected 3 arguments, got 2')
elif len(args) < 2:
raise TypeError('nsolve expected at least 2 arguments, got %i'
% len(args))
else:
raise TypeError('nsolve expected at most 3 arguments, got %i'
% len(args))
modules = kwargs.get('modules', ['mpmath'])
if iterable(f):
f = list(f)
for i, fi in enumerate(f):
if isinstance(fi, Equality):
f[i] = fi.lhs - fi.rhs
f = Matrix(f).T
if iterable(x0):
x0 = list(x0)
if not isinstance(f, Matrix):
# assume it's a sympy expression
if isinstance(f, Equality):
f = f.lhs - f.rhs
syms = f.free_symbols
if fargs is None:
fargs = syms.copy().pop()
if not (len(syms) == 1 and (fargs in syms or fargs[0] in syms)):
raise ValueError(filldedent('''
expected a one-dimensional and numerical function'''))
# the function is much better behaved if there is no denominator
# but sending the numerator is left to the user since sometimes
# the function is better behaved when the denominator is present
# e.g., issue 11768
f = lambdify(fargs, f, modules)
x = sympify(findroot(f, x0, **kwargs))
if as_dict:
return [{fargs: x}]
return x
if len(fargs) > f.cols:
raise NotImplementedError(filldedent('''
need at least as many equations as variables'''))
verbose = kwargs.get('verbose', False)
if verbose:
print('f(x):')
print(f)
# derive Jacobian
J = f.jacobian(fargs)
if verbose:
print('J(x):')
print(J)
# create functions
f = lambdify(fargs, f.T, modules)
J = lambdify(fargs, J, modules)
# solve the system numerically
x = findroot(f, x0, J=J, **kwargs)
if as_dict:
return [dict(zip(fargs, [sympify(xi) for xi in x]))]
return Matrix(x)
def _invert(eq, *symbols, **kwargs):
"""Return tuple (i, d) where ``i`` is independent of ``symbols`` and ``d``
contains symbols. ``i`` and ``d`` are obtained after recursively using
algebraic inversion until an uninvertible ``d`` remains. If there are no
free symbols then ``d`` will be zero. Some (but not necessarily all)
solutions to the expression ``i - d`` will be related to the solutions of
the original expression.
Examples
========
>>> from sympy.solvers.solvers import _invert as invert
>>> from sympy import sqrt, cos
>>> from sympy.abc import x, y
>>> invert(x - 3)
(3, x)
>>> invert(3)
(3, 0)
>>> invert(2*cos(x) - 1)
(1/2, cos(x))
>>> invert(sqrt(x) - 3)
(3, sqrt(x))
>>> invert(sqrt(x) + y, x)
(-y, sqrt(x))
>>> invert(sqrt(x) + y, y)
(-sqrt(x), y)
>>> invert(sqrt(x) + y, x, y)
(0, sqrt(x) + y)
If there is more than one symbol in a power's base and the exponent
is not an Integer, then the principal root will be used for the
inversion:
>>> invert(sqrt(x + y) - 2)
(4, x + y)
>>> invert(sqrt(x + y) - 2)
(4, x + y)
If the exponent is an integer, setting ``integer_power`` to True
will force the principal root to be selected:
>>> invert(x**2 - 4, integer_power=True)
(2, x)
"""
eq = sympify(eq)
if eq.args:
# make sure we are working with flat eq
eq = eq.func(*eq.args)
free = eq.free_symbols
if not symbols:
symbols = free
if not free & set(symbols):
return eq, S.Zero
dointpow = bool(kwargs.get('integer_power', False))
lhs = eq
rhs = S.Zero
while True:
was = lhs
while True:
indep, dep = lhs.as_independent(*symbols)
# dep + indep == rhs
if lhs.is_Add:
# this indicates we have done it all
if indep.is_zero:
break
lhs = dep
rhs -= indep
# dep * indep == rhs
else:
# this indicates we have done it all
if indep is S.One:
break
lhs = dep
rhs /= indep
# collect like-terms in symbols
if lhs.is_Add:
terms = {}
for a in lhs.args:
i, d = a.as_independent(*symbols)
terms.setdefault(d, []).append(i)
if any(len(v) > 1 for v in terms.values()):
args = []
for d, i in terms.items():
if len(i) > 1:
args.append(Add(*i)*d)
else:
args.append(i[0]*d)
lhs = Add(*args)
# if it's a two-term Add with rhs = 0 and two powers we can get the
# dependent terms together, e.g. 3*f(x) + 2*g(x) -> f(x)/g(x) = -2/3
if lhs.is_Add and not rhs and len(lhs.args) == 2 and \
not lhs.is_polynomial(*symbols):
a, b = ordered(lhs.args)
ai, ad = a.as_independent(*symbols)
bi, bd = b.as_independent(*symbols)
if any(_ispow(i) for i in (ad, bd)):
a_base, a_exp = ad.as_base_exp()
b_base, b_exp = bd.as_base_exp()
if a_base == b_base:
# a = -b
lhs = powsimp(powdenest(ad/bd))
rhs = -bi/ai
else:
rat = ad/bd
_lhs = powsimp(ad/bd)
if _lhs != rat:
lhs = _lhs
rhs = -bi/ai
elif ai == -bi:
if isinstance(ad, Function) and ad.func == bd.func:
if len(ad.args) == len(bd.args) == 1:
lhs = ad.args[0] - bd.args[0]
elif len(ad.args) == len(bd.args):
# should be able to solve
# f(x, y) - f(2 - x, 0) == 0 -> x == 1
raise NotImplementedError(
'equal function with more than 1 argument')
else:
raise ValueError(
'function with different numbers of args')
elif lhs.is_Mul and any(_ispow(a) for a in lhs.args):
lhs = powsimp(powdenest(lhs))
if lhs.is_Function:
if hasattr(lhs, 'inverse') and len(lhs.args) == 1:
# -1
# f(x) = g -> x = f (g)
#
# /!\ inverse should not be defined if there are multiple values
# for the function -- these are handled in _tsolve
#
rhs = lhs.inverse()(rhs)
lhs = lhs.args[0]
elif isinstance(lhs, atan2):
y, x = lhs.args
lhs = 2*atan(y/(sqrt(x**2 + y**2) + x))
elif lhs.func == rhs.func:
if len(lhs.args) == len(rhs.args) == 1:
lhs = lhs.args[0]
rhs = rhs.args[0]
elif len(lhs.args) == len(rhs.args):
# should be able to solve
# f(x, y) == f(2, 3) -> x == 2
# f(x, x + y) == f(2, 3) -> x == 2
raise NotImplementedError(
'equal function with more than 1 argument')
else:
raise ValueError(
'function with different numbers of args')
if rhs and lhs.is_Pow and lhs.exp.is_Integer and lhs.exp < 0:
lhs = 1/lhs
rhs = 1/rhs
# base**a = b -> base = b**(1/a) if
# a is an Integer and dointpow=True (this gives real branch of root)
# a is not an Integer and the equation is multivariate and the
# base has more than 1 symbol in it
# The rationale for this is that right now the multi-system solvers
# doesn't try to resolve generators to see, for example, if the whole
# system is written in terms of sqrt(x + y) so it will just fail, so we
# do that step here.
if lhs.is_Pow and (
lhs.exp.is_Integer and dointpow or not lhs.exp.is_Integer and
len(symbols) > 1 and len(lhs.base.free_symbols & set(symbols)) > 1):
rhs = rhs**(1/lhs.exp)
lhs = lhs.base
if lhs == was:
break
return rhs, lhs
def unrad(eq, *syms, **flags):
""" Remove radicals with symbolic arguments and return (eq, cov),
None or raise an error:
None is returned if there are no radicals to remove.
NotImplementedError is raised if there are radicals and they cannot be
removed or if the relationship between the original symbols and the
change of variable needed to rewrite the system as a polynomial cannot
be solved.
Otherwise the tuple, ``(eq, cov)``, is returned where::
``eq``, ``cov``
``eq`` is an equation without radicals (in the symbol(s) of
interest) whose solutions are a superset of the solutions to the
original expression. ``eq`` might be re-written in terms of a new
variable; the relationship to the original variables is given by
``cov`` which is a list containing ``v`` and ``v**p - b`` where
``p`` is the power needed to clear the radical and ``b`` is the
radical now expressed as a polynomial in the symbols of interest.
For example, for sqrt(2 - x) the tuple would be
``(c, c**2 - 2 + x)``. The solutions of ``eq`` will contain
solutions to the original equation (if there are any).
``syms``
an iterable of symbols which, if provided, will limit the focus of
radical removal: only radicals with one or more of the symbols of
interest will be cleared. All free symbols are used if ``syms`` is not
set.
``flags`` are used internally for communication during recursive calls.
Two options are also recognized::
``take``, when defined, is interpreted as a single-argument function
that returns True if a given Pow should be handled.
Radicals can be removed from an expression if::
* all bases of the radicals are the same; a change of variables is
done in this case.
* if all radicals appear in one term of the expression
* there are only 4 terms with sqrt() factors or there are less than
four terms having sqrt() factors
* there are only two terms with radicals
Examples
========
>>> from sympy.solvers.solvers import unrad
>>> from sympy.abc import x
>>> from sympy import sqrt, Rational, root, real_roots, solve
>>> unrad(sqrt(x)*x**Rational(1, 3) + 2)
(x**5 - 64, [])
>>> unrad(sqrt(x) + root(x + 1, 3))
(x**3 - x**2 - 2*x - 1, [])
>>> eq = sqrt(x) + root(x, 3) - 2
>>> unrad(eq)
(_p**3 + _p**2 - 2, [_p, _p**6 - x])
"""
uflags = dict(check=False, simplify=False)
def _cov(p, e):
if cov:
# XXX - uncovered
oldp, olde = cov
if Poly(e, p).degree(p) in (1, 2):
cov[:] = [p, olde.subs(oldp, _solve(e, p, **uflags)[0])]
else:
raise NotImplementedError
else:
cov[:] = [p, e]
def _canonical(eq, cov):
if cov:
# change symbol to vanilla so no solutions are eliminated
p, e = cov
rep = {p: Dummy(p.name)}
eq = eq.xreplace(rep)
cov = [p.xreplace(rep), e.xreplace(rep)]
# remove constants and powers of factors since these don't change
# the location of the root; XXX should factor or factor_terms be used?
eq = factor_terms(_mexpand(eq.as_numer_denom()[0], recursive=True), clear=True)
if eq.is_Mul:
args = []
for f in eq.args:
if f.is_number:
continue
if f.is_Pow and _take(f, True):
args.append(f.base)
else:
args.append(f)
eq = Mul(*args) # leave as Mul for more efficient solving
# make the sign canonical
free = eq.free_symbols
if len(free) == 1:
if eq.coeff(free.pop()**degree(eq)).could_extract_minus_sign():
eq = -eq
elif eq.could_extract_minus_sign():
eq = -eq
return eq, cov
def _Q(pow):
# return leading Rational of denominator of Pow's exponent
c = pow.as_base_exp()[1].as_coeff_Mul()[0]
if not c.is_Rational:
return S.One
return c.q
# define the _take method that will determine whether a term is of interest
def _take(d, take_int_pow):
# return True if coefficient of any factor's exponent's den is not 1
for pow in Mul.make_args(d):
if not (pow.is_Symbol or pow.is_Pow):
continue
b, e = pow.as_base_exp()
if not b.has(*syms):
continue
if not take_int_pow and _Q(pow) == 1:
continue
free = pow.free_symbols
if free.intersection(syms):
return True
return False
_take = flags.setdefault('_take', _take)
cov, nwas, rpt = [flags.setdefault(k, v) for k, v in
sorted(dict(cov=[], n=None, rpt=0).items())]
# preconditioning
eq = powdenest(factor_terms(eq, radical=True, clear=True))
eq, d = eq.as_numer_denom()
eq = _mexpand(eq, recursive=True)
if eq.is_number:
return
syms = set(syms) or eq.free_symbols
poly = eq.as_poly()
gens = [g for g in poly.gens if _take(g, True)]
if not gens:
return
# check for trivial case
# - already a polynomial in integer powers
if all(_Q(g) == 1 for g in gens):
return
# - an exponent has a symbol of interest (don't handle)
if any(g.as_base_exp()[1].has(*syms) for g in gens):
return
def _rads_bases_lcm(poly):
# if all the bases are the same or all the radicals are in one
# term, `lcm` will be the lcm of the denominators of the
# exponents of the radicals
lcm = 1
rads = set()
bases = set()
for g in poly.gens:
if not _take(g, False):
continue
q = _Q(g)
if q != 1:
rads.add(g)
lcm = ilcm(lcm, q)
bases.add(g.base)
return rads, bases, lcm
rads, bases, lcm = _rads_bases_lcm(poly)
if not rads:
return
covsym = Dummy('p', nonnegative=True)
# only keep in syms symbols that actually appear in radicals;
# and update gens
newsyms = set()
for r in rads:
newsyms.update(syms & r.free_symbols)
if newsyms != syms:
syms = newsyms
gens = [g for g in gens if g.free_symbols & syms]
# get terms together that have common generators
drad = dict(list(zip(rads, list(range(len(rads))))))
rterms = {(): []}
args = Add.make_args(poly.as_expr())
for t in args:
if _take(t, False):
common = set(t.as_poly().gens).intersection(rads)
key = tuple(sorted([drad[i] for i in common]))
else:
key = ()
rterms.setdefault(key, []).append(t)
others = Add(*rterms.pop(()))
rterms = [Add(*rterms[k]) for k in rterms.keys()]
# the output will depend on the order terms are processed, so
# make it canonical quickly
rterms = list(reversed(list(ordered(rterms))))
ok = False # we don't have a solution yet
depth = sqrt_depth(eq)
if len(rterms) == 1 and not (rterms[0].is_Add and lcm > 2):
eq = rterms[0]**lcm - ((-others)**lcm)
ok = True
else:
if len(rterms) == 1 and rterms[0].is_Add:
rterms = list(rterms[0].args)
if len(bases) == 1:
b = bases.pop()
if len(syms) > 1:
free = b.free_symbols
x = {g for g in gens if g.is_Symbol} & free
if not x:
x = free
x = ordered(x)
else:
x = syms
x = list(x)[0]
try:
inv = _solve(covsym**lcm - b, x, **uflags)
if not inv:
raise NotImplementedError
eq = poly.as_expr().subs(b, covsym**lcm).subs(x, inv[0])
_cov(covsym, covsym**lcm - b)
return _canonical(eq, cov)
except NotImplementedError:
pass
else:
# no longer consider integer powers as generators
gens = [g for g in gens if _Q(g) != 1]
if len(rterms) == 2:
if not others:
eq = rterms[0]**lcm - (-rterms[1])**lcm
ok = True
elif not log(lcm, 2).is_Integer:
# the lcm-is-power-of-two case is handled below
r0, r1 = rterms
if flags.get('_reverse', False):
r1, r0 = r0, r1
i0 = _rads0, _bases0, lcm0 = _rads_bases_lcm(r0.as_poly())
i1 = _rads1, _bases1, lcm1 = _rads_bases_lcm(r1.as_poly())
for reverse in range(2):
if reverse:
i0, i1 = i1, i0
r0, r1 = r1, r0
_rads1, _, lcm1 = i1
_rads1 = Mul(*_rads1)
t1 = _rads1**lcm1
c = covsym**lcm1 - t1
for x in syms:
try:
sol = _solve(c, x, **uflags)
if not sol:
raise NotImplementedError
neweq = r0.subs(x, sol[0]) + covsym*r1/_rads1 + \
others
tmp = unrad(neweq, covsym)
if tmp:
eq, newcov = tmp
if newcov:
newp, newc = newcov
_cov(newp, c.subs(covsym,
_solve(newc, covsym, **uflags)[0]))
else:
_cov(covsym, c)
else:
eq = neweq
_cov(covsym, c)
ok = True
break
except NotImplementedError:
if reverse:
raise NotImplementedError(
'no successful change of variable found')
else:
pass
if ok:
break
elif len(rterms) == 3:
# two cube roots and another with order less than 5
# (so an analytical solution can be found) or a base
# that matches one of the cube root bases
info = [_rads_bases_lcm(i.as_poly()) for i in rterms]
RAD = 0
BASES = 1
LCM = 2
if info[0][LCM] != 3:
info.append(info.pop(0))
rterms.append(rterms.pop(0))
elif info[1][LCM] != 3:
info.append(info.pop(1))
rterms.append(rterms.pop(1))
if info[0][LCM] == info[1][LCM] == 3:
if info[1][BASES] != info[2][BASES]:
info[0], info[1] = info[1], info[0]
rterms[0], rterms[1] = rterms[1], rterms[0]
if info[1][BASES] == info[2][BASES]:
eq = rterms[0]**3 + (rterms[1] + rterms[2] + others)**3
ok = True
elif info[2][LCM] < 5:
# a*root(A, 3) + b*root(B, 3) + others = c
a, b, c, d, A, B = [Dummy(i) for i in 'abcdAB']
# zz represents the unraded expression into which the
# specifics for this case are substituted
zz = (c - d)*(A**3*a**9 + 3*A**2*B*a**6*b**3 -
3*A**2*a**6*c**3 + 9*A**2*a**6*c**2*d - 9*A**2*a**6*c*d**2 +
3*A**2*a**6*d**3 + 3*A*B**2*a**3*b**6 + 21*A*B*a**3*b**3*c**3 -
63*A*B*a**3*b**3*c**2*d + 63*A*B*a**3*b**3*c*d**2 -
21*A*B*a**3*b**3*d**3 + 3*A*a**3*c**6 - 18*A*a**3*c**5*d +
45*A*a**3*c**4*d**2 - 60*A*a**3*c**3*d**3 + 45*A*a**3*c**2*d**4 -
18*A*a**3*c*d**5 + 3*A*a**3*d**6 + B**3*b**9 - 3*B**2*b**6*c**3 +
9*B**2*b**6*c**2*d - 9*B**2*b**6*c*d**2 + 3*B**2*b**6*d**3 +
3*B*b**3*c**6 - 18*B*b**3*c**5*d + 45*B*b**3*c**4*d**2 -
60*B*b**3*c**3*d**3 + 45*B*b**3*c**2*d**4 - 18*B*b**3*c*d**5 +
3*B*b**3*d**6 - c**9 + 9*c**8*d - 36*c**7*d**2 + 84*c**6*d**3 -
126*c**5*d**4 + 126*c**4*d**5 - 84*c**3*d**6 + 36*c**2*d**7 -
9*c*d**8 + d**9)
def _t(i):
b = Mul(*info[i][RAD])
return cancel(rterms[i]/b), Mul(*info[i][BASES])
aa, AA = _t(0)
bb, BB = _t(1)
cc = -rterms[2]
dd = others
eq = zz.xreplace(dict(zip(
(a, A, b, B, c, d),
(aa, AA, bb, BB, cc, dd))))
ok = True
# handle power-of-2 cases
if not ok:
if log(lcm, 2).is_Integer and (not others and
len(rterms) == 4 or len(rterms) < 4):
def _norm2(a, b):
return a**2 + b**2 + 2*a*b
if len(rterms) == 4:
# (r0+r1)**2 - (r2+r3)**2
r0, r1, r2, r3 = rterms
eq = _norm2(r0, r1) - _norm2(r2, r3)
ok = True
elif len(rterms) == 3:
# (r1+r2)**2 - (r0+others)**2
r0, r1, r2 = rterms
eq = _norm2(r1, r2) - _norm2(r0, others)
ok = True
elif len(rterms) == 2:
# r0**2 - (r1+others)**2
r0, r1 = rterms
eq = r0**2 - _norm2(r1, others)
ok = True
new_depth = sqrt_depth(eq) if ok else depth
rpt += 1 # XXX how many repeats with others unchanging is enough?
if not ok or (
nwas is not None and len(rterms) == nwas and
new_depth is not None and new_depth == depth and
rpt > 3):
raise NotImplementedError('Cannot remove all radicals')
flags.update(dict(cov=cov, n=len(rterms), rpt=rpt))
neq = unrad(eq, *syms, **flags)
if neq:
eq, cov = neq
eq, cov = _canonical(eq, cov)
return eq, cov
from sympy.solvers.bivariate import (
bivariate_type, _solve_lambert, _filtered_gens)
|
3a35683f02f30dd52cb7b1f0f0dfc9287c198315c85c96c0e33ab7bf133cb0cc | # -*- coding: utf-8 -*-
from sympy.core.compatibility import range
from .cartan_type import CartanType
from mpmath import fac
from sympy.core.backend import Matrix, eye, Rational, Basic, igcd
class WeylGroup(Basic):
"""
For each semisimple Lie group, we have a Weyl group. It is a subgroup of
the isometry group of the root system. Specifically, it’s the subgroup
that is generated by reflections through the hyperplanes orthogonal to
the roots. Therefore, Weyl groups are reflection groups, and so a Weyl
group is a finite Coxeter group.
"""
def __new__(cls, cartantype):
obj = Basic.__new__(cls, cartantype)
obj.cartan_type = CartanType(cartantype)
return obj
def generators(self):
"""
This method creates the generating reflections of the Weyl group for
a given Lie algebra. For a Lie algebra of rank n, there are n
different generating reflections. This function returns them as
a list.
Examples
========
>>> from sympy.liealgebras.weyl_group import WeylGroup
>>> c = WeylGroup("F4")
>>> c.generators()
['r1', 'r2', 'r3', 'r4']
"""
n = self.cartan_type.rank()
generators = []
for i in range(1, n+1):
reflection = "r"+str(i)
generators.append(reflection)
return generators
def group_order(self):
"""
This method returns the order of the Weyl group.
For types A, B, C, D, and E the order depends on
the rank of the Lie algebra. For types F and G,
the order is fixed.
Examples
========
>>> from sympy.liealgebras.weyl_group import WeylGroup
>>> c = WeylGroup("D4")
>>> c.group_order()
192.0
"""
n = self.cartan_type.rank()
if self.cartan_type.series == "A":
return fac(n+1)
if self.cartan_type.series == "B" or self.cartan_type.series == "C":
return fac(n)*(2**n)
if self.cartan_type.series == "D":
return fac(n)*(2**(n-1))
if self.cartan_type.series == "E":
if n == 6:
return 51840
if n == 7:
return 2903040
if n == 8:
return 696729600
if self.cartan_type.series == "F":
return 1152
if self.cartan_type.series == "G":
return 12
def group_name(self):
"""
This method returns some general information about the Weyl group for
a given Lie algebra. It returns the name of the group and the elements
it acts on, if relevant.
"""
n = self.cartan_type.rank()
if self.cartan_type.series == "A":
return "S"+str(n+1) + ": the symmetric group acting on " + str(n+1) + " elements."
if self.cartan_type.series == "B" or self.cartan_type.series == "C":
return "The hyperoctahedral group acting on " + str(2*n) + " elements."
if self.cartan_type.series == "D":
return "The symmetry group of the " + str(n) + "-dimensional demihypercube."
if self.cartan_type.series == "E":
if n == 6:
return "The symmetry group of the 6-polytope."
if n == 7:
return "The symmetry group of the 7-polytope."
if n == 8:
return "The symmetry group of the 8-polytope."
if self.cartan_type.series == "F":
return "The symmetry group of the 24-cell, or icositetrachoron."
if self.cartan_type.series == "G":
return "D6, the dihedral group of order 12, and symmetry group of the hexagon."
def element_order(self, weylelt):
"""
This method returns the order of a given Weyl group element, which should
be specified by the user in the form of products of the generating
reflections, i.e. of the form r1*r2 etc.
For types A-F, this method current works by taking the matrix form of
the specified element, and then finding what power of the matrix is the
identity. It then returns this power.
Examples
========
>>> from sympy.liealgebras.weyl_group import WeylGroup
>>> b = WeylGroup("B4")
>>> b.element_order('r1*r4*r2')
4
"""
n = self.cartan_type.rank()
if self.cartan_type.series == "A":
a = self.matrix_form(weylelt)
order = 1
while a != eye(n+1):
a *= self.matrix_form(weylelt)
order += 1
return order
if self.cartan_type.series == "D":
a = self.matrix_form(weylelt)
order = 1
while a != eye(n):
a *= self.matrix_form(weylelt)
order += 1
return order
if self.cartan_type.series == "E":
a = self.matrix_form(weylelt)
order = 1
while a != eye(8):
a *= self.matrix_form(weylelt)
order += 1
return order
if self.cartan_type.series == "G":
elts = list(weylelt)
reflections = elts[1::3]
m = self.delete_doubles(reflections)
while self.delete_doubles(m) != m:
m = self.delete_doubles(m)
reflections = m
if len(reflections) % 2 == 1:
return 2
elif len(reflections) == 0:
return 1
else:
if len(reflections) == 1:
return 2
else:
m = len(reflections) // 2
lcm = (6 * m)/ igcd(m, 6)
order = lcm / m
return order
if self.cartan_type.series == 'F':
a = self.matrix_form(weylelt)
order = 1
while a != eye(4):
a *= self.matrix_form(weylelt)
order += 1
return order
if self.cartan_type.series == "B" or self.cartan_type.series == "C":
a = self.matrix_form(weylelt)
order = 1
while a != eye(n):
a *= self.matrix_form(weylelt)
order += 1
return order
def delete_doubles(self, reflections):
"""
This is a helper method for determining the order of an element in the
Weyl group of G2. It takes a Weyl element and if repeated simple reflections
in it, it deletes them.
"""
counter = 0
copy = list(reflections)
for elt in copy:
if counter < len(copy)-1:
if copy[counter + 1] == elt:
del copy[counter]
del copy[counter]
counter += 1
return copy
def matrix_form(self, weylelt):
"""
This method takes input from the user in the form of products of the
generating reflections, and returns the matrix corresponding to the
element of the Weyl group. Since each element of the Weyl group is
a reflection of some type, there is a corresponding matrix representation.
This method uses the standard representation for all the generating
reflections.
Examples
========
>>> from sympy.liealgebras.weyl_group import WeylGroup
>>> f = WeylGroup("F4")
>>> f.matrix_form('r2*r3')
Matrix([
[1, 0, 0, 0],
[0, 1, 0, 0],
[0, 0, 0, -1],
[0, 0, 1, 0]])
"""
elts = list(weylelt)
reflections = elts[1::3]
n = self.cartan_type.rank()
if self.cartan_type.series == 'A':
matrixform = eye(n+1)
for elt in reflections:
a = int(elt)
mat = eye(n+1)
mat[a-1, a-1] = 0
mat[a-1, a] = 1
mat[a, a-1] = 1
mat[a, a] = 0
matrixform *= mat
return matrixform
if self.cartan_type.series == 'D':
matrixform = eye(n)
for elt in reflections:
a = int(elt)
mat = eye(n)
if a < n:
mat[a-1, a-1] = 0
mat[a-1, a] = 1
mat[a, a-1] = 1
mat[a, a] = 0
matrixform *= mat
else:
mat[n-2, n-1] = -1
mat[n-2, n-2] = 0
mat[n-1, n-2] = -1
mat[n-1, n-1] = 0
matrixform *= mat
return matrixform
if self.cartan_type.series == 'G':
matrixform = eye(3)
for elt in reflections:
a = int(elt)
if a == 1:
gen1 = Matrix([[1, 0, 0], [0, 0, 1], [0, 1, 0]])
matrixform *= gen1
else:
gen2 = Matrix([[Rational(2, 3), Rational(2, 3), Rational(-1, 3)],
[Rational(2, 3), Rational(-1, 3), Rational(2, 3)],
[Rational(-1, 3), Rational(2, 3), Rational(2, 3)]])
matrixform *= gen2
return matrixform
if self.cartan_type.series == 'F':
matrixform = eye(4)
for elt in reflections:
a = int(elt)
if a == 1:
mat = Matrix([[1, 0, 0, 0], [0, 0, 1, 0], [0, 1, 0, 0], [0, 0, 0, 1]])
matrixform *= mat
elif a == 2:
mat = Matrix([[1, 0, 0, 0], [0, 1, 0, 0], [0, 0, 0, 1], [0, 0, 1, 0]])
matrixform *= mat
elif a == 3:
mat = Matrix([[1, 0, 0, 0], [0, 1, 0, 0], [0, 0, 1, 0], [0, 0, 0, -1]])
matrixform *= mat
else:
mat = Matrix([[Rational(1, 2), Rational(1, 2), Rational(1, 2), Rational(1, 2)],
[Rational(1, 2), Rational(1, 2), Rational(-1, 2), Rational(-1, 2)],
[Rational(1, 2), Rational(-1, 2), Rational(1, 2), Rational(-1, 2)],
[Rational(1, 2), Rational(-1, 2), Rational(-1, 2), Rational(1, 2)]])
matrixform *= mat
return matrixform
if self.cartan_type.series == 'E':
matrixform = eye(8)
for elt in reflections:
a = int(elt)
if a == 1:
mat = Matrix([[Rational(3, 4), Rational(1, 4), Rational(1, 4), Rational(1, 4),
Rational(1, 4), Rational(1, 4), Rational(1, 4), Rational(-1, 4)],
[Rational(1, 4), Rational(3, 4), Rational(-1, 4), Rational(-1, 4),
Rational(-1, 4), Rational(-1, 4), Rational(1, 4), Rational(-1, 4)],
[Rational(1, 4), Rational(-1, 4), Rational(3, 4), Rational(-1, 4),
Rational(-1, 4), Rational(-1, 4), Rational(-1, 4), Rational(1, 4)],
[Rational(1, 4), Rational(-1, 4), Rational(-1, 4), Rational(3, 4),
Rational(-1, 4), Rational(-1, 4), Rational(-1, 4), Rational(1, 4)],
[Rational(1, 4), Rational(-1, 4), Rational(-1, 4), Rational(-1, 4),
Rational(3, 4), Rational(-1, 4), Rational(-1, 4), Rational(1, 4)],
[Rational(1, 4), Rational(-1, 4), Rational(-1, 4), Rational(-1, 4),
Rational(-1, 4), Rational(3, 4), Rational(-1, 4), Rational(1, 4)],
[Rational(1, 4), Rational(-1, 4), Rational(-1, 4), Rational(-1, 4),
Rational(-1, 4), Rational(-1, 4), Rational(-3, 4), Rational(1, 4)],
[Rational(1, 4), Rational(-1, 4), Rational(-1, 4), Rational(-1, 4),
Rational(-1, 4), Rational(-1, 4), Rational(-1, 4), Rational(3, 4)]])
matrixform *= mat
elif a == 2:
mat = eye(8)
mat[0, 0] = 0
mat[0, 1] = -1
mat[1, 0] = -1
mat[1, 1] = 0
matrixform *= mat
else:
mat = eye(8)
mat[a-3, a-3] = 0
mat[a-3, a-2] = 1
mat[a-2, a-3] = 1
mat[a-2, a-2] = 0
matrixform *= mat
return matrixform
if self.cartan_type.series == 'B' or self.cartan_type.series == 'C':
matrixform = eye(n)
for elt in reflections:
a = int(elt)
mat = eye(n)
if a == 1:
mat[0, 0] = -1
matrixform *= mat
else:
mat[a - 2, a - 2] = 0
mat[a-2, a-1] = 1
mat[a - 1, a - 2] = 1
mat[a -1, a - 1] = 0
matrixform *= mat
return matrixform
def coxeter_diagram(self):
"""
This method returns the Coxeter diagram corresponding to a Weyl group.
The Coxeter diagram can be obtained from a Lie algebra's Dynkin diagram
by deleting all arrows; the Coxeter diagram is the undirected graph.
The vertices of the Coxeter diagram represent the generating reflections
of the Weyl group, , s_i. An edge is drawn between s_i and s_j if the order
m(i, j) of s_i*s_j is greater than two. If there is one edge, the order
m(i, j) is 3. If there are two edges, the order m(i, j) is 4, and if there
are three edges, the order m(i, j) is 6.
Examples
========
>>> from sympy.liealgebras.weyl_group import WeylGroup
>>> c = WeylGroup("B3")
>>> print(c.coxeter_diagram())
0---0===0
1 2 3
"""
n = self.cartan_type.rank()
if self.cartan_type.series == "A" or self.cartan_type.series == "D" or self.cartan_type.series == "E":
return self.cartan_type.dynkin_diagram()
if self.cartan_type.series == "B" or self.cartan_type.series == "C":
diag = "---".join("0" for i in range(1, n)) + "===0\n"
diag += " ".join(str(i) for i in range(1, n+1))
return diag
if self.cartan_type.series == "F":
diag = "0---0===0---0\n"
diag += " ".join(str(i) for i in range(1, 5))
return diag
if self.cartan_type.series == "G":
diag = "0≡≡≡0\n1 2"
return diag
|
59958d6fe1b93f66a519d0195e7df28ceb11f0c37fc4dd1d51bc0066b08adcd5 | """
Finite difference weights
=========================
This module implements an algorithm for efficient generation of finite
difference weights for ordinary differentials of functions for
derivatives from 0 (interpolation) up to arbitrary order.
The core algorithm is provided in the finite difference weight generating
function (``finite_diff_weights``), and two convenience functions are provided
for:
- estimating a derivative (or interpolate) directly from a series of points
is also provided (``apply_finite_diff``).
- differentiating by using finite difference approximations
(``differentiate_finite``).
"""
from sympy import Derivative, S
from sympy.core.compatibility import iterable, range
from sympy.core.decorators import deprecated
def finite_diff_weights(order, x_list, x0=S.One):
"""
Calculates the finite difference weights for an arbitrarily spaced
one-dimensional grid (``x_list``) for derivatives at ``x0`` of order
0, 1, ..., up to ``order`` using a recursive formula. Order of accuracy
is at least ``len(x_list) - order``, if ``x_list`` is defined correctly.
Parameters
==========
order: int
Up to what derivative order weights should be calculated.
0 corresponds to interpolation.
x_list: sequence
Sequence of (unique) values for the independent variable.
It is useful (but not necessary) to order ``x_list`` from
nearest to furthest from ``x0``; see examples below.
x0: Number or Symbol
Root or value of the independent variable for which the finite
difference weights should be generated. Default is ``S.One``.
Returns
=======
list
A list of sublists, each corresponding to coefficients for
increasing derivative order, and each containing lists of
coefficients for increasing subsets of x_list.
Examples
========
>>> from sympy import S
>>> from sympy.calculus import finite_diff_weights
>>> res = finite_diff_weights(1, [-S(1)/2, S(1)/2, S(3)/2, S(5)/2], 0)
>>> res
[[[1, 0, 0, 0],
[1/2, 1/2, 0, 0],
[3/8, 3/4, -1/8, 0],
[5/16, 15/16, -5/16, 1/16]],
[[0, 0, 0, 0],
[-1, 1, 0, 0],
[-1, 1, 0, 0],
[-23/24, 7/8, 1/8, -1/24]]]
>>> res[0][-1] # FD weights for 0th derivative, using full x_list
[5/16, 15/16, -5/16, 1/16]
>>> res[1][-1] # FD weights for 1st derivative
[-23/24, 7/8, 1/8, -1/24]
>>> res[1][-2] # FD weights for 1st derivative, using x_list[:-1]
[-1, 1, 0, 0]
>>> res[1][-1][0] # FD weight for 1st deriv. for x_list[0]
-23/24
>>> res[1][-1][1] # FD weight for 1st deriv. for x_list[1], etc.
7/8
Each sublist contains the most accurate formula at the end.
Note, that in the above example ``res[1][1]`` is the same as ``res[1][2]``.
Since res[1][2] has an order of accuracy of
``len(x_list[:3]) - order = 3 - 1 = 2``, the same is true for ``res[1][1]``!
>>> from sympy import S
>>> from sympy.calculus import finite_diff_weights
>>> res = finite_diff_weights(1, [S(0), S(1), -S(1), S(2), -S(2)], 0)[1]
>>> res
[[0, 0, 0, 0, 0],
[-1, 1, 0, 0, 0],
[0, 1/2, -1/2, 0, 0],
[-1/2, 1, -1/3, -1/6, 0],
[0, 2/3, -2/3, -1/12, 1/12]]
>>> res[0] # no approximation possible, using x_list[0] only
[0, 0, 0, 0, 0]
>>> res[1] # classic forward step approximation
[-1, 1, 0, 0, 0]
>>> res[2] # classic centered approximation
[0, 1/2, -1/2, 0, 0]
>>> res[3:] # higher order approximations
[[-1/2, 1, -1/3, -1/6, 0], [0, 2/3, -2/3, -1/12, 1/12]]
Let us compare this to a differently defined ``x_list``. Pay attention to
``foo[i][k]`` corresponding to the gridpoint defined by ``x_list[k]``.
>>> from sympy import S
>>> from sympy.calculus import finite_diff_weights
>>> foo = finite_diff_weights(1, [-S(2), -S(1), S(0), S(1), S(2)], 0)[1]
>>> foo
[[0, 0, 0, 0, 0],
[-1, 1, 0, 0, 0],
[1/2, -2, 3/2, 0, 0],
[1/6, -1, 1/2, 1/3, 0],
[1/12, -2/3, 0, 2/3, -1/12]]
>>> foo[1] # not the same and of lower accuracy as res[1]!
[-1, 1, 0, 0, 0]
>>> foo[2] # classic double backward step approximation
[1/2, -2, 3/2, 0, 0]
>>> foo[4] # the same as res[4]
[1/12, -2/3, 0, 2/3, -1/12]
Note that, unless you plan on using approximations based on subsets of
``x_list``, the order of gridpoints does not matter.
The capability to generate weights at arbitrary points can be
used e.g. to minimize Runge's phenomenon by using Chebyshev nodes:
>>> from sympy import cos, symbols, pi, simplify
>>> from sympy.calculus import finite_diff_weights
>>> N, (h, x) = 4, symbols('h x')
>>> x_list = [x+h*cos(i*pi/(N)) for i in range(N,-1,-1)] # chebyshev nodes
>>> print(x_list)
[-h + x, -sqrt(2)*h/2 + x, x, sqrt(2)*h/2 + x, h + x]
>>> mycoeffs = finite_diff_weights(1, x_list, 0)[1][4]
>>> [simplify(c) for c in mycoeffs] #doctest: +NORMALIZE_WHITESPACE
[(h**3/2 + h**2*x - 3*h*x**2 - 4*x**3)/h**4,
(-sqrt(2)*h**3 - 4*h**2*x + 3*sqrt(2)*h*x**2 + 8*x**3)/h**4,
6*x/h**2 - 8*x**3/h**4,
(sqrt(2)*h**3 - 4*h**2*x - 3*sqrt(2)*h*x**2 + 8*x**3)/h**4,
(-h**3/2 + h**2*x + 3*h*x**2 - 4*x**3)/h**4]
Notes
=====
If weights for a finite difference approximation of 3rd order
derivative is wanted, weights for 0th, 1st and 2nd order are
calculated "for free", so are formulae using subsets of ``x_list``.
This is something one can take advantage of to save computational cost.
Be aware that one should define ``x_list`` from nearest to furthest from
``x0``. If not, subsets of ``x_list`` will yield poorer approximations,
which might not grand an order of accuracy of ``len(x_list) - order``.
See also
========
sympy.calculus.finite_diff.apply_finite_diff
References
==========
.. [1] Generation of Finite Difference Formulas on Arbitrarily Spaced
Grids, Bengt Fornberg; Mathematics of computation; 51; 184;
(1988); 699-706; doi:10.1090/S0025-5718-1988-0935077-0
"""
# The notation below closely corresponds to the one used in the paper.
order = S(order)
if not order.is_number:
raise ValueError("Cannot handle symbolic order.")
if order < 0:
raise ValueError("Negative derivative order illegal.")
if int(order) != order:
raise ValueError("Non-integer order illegal")
M = order
N = len(x_list) - 1
delta = [[[0 for nu in range(N+1)] for n in range(N+1)] for
m in range(M+1)]
delta[0][0][0] = S.One
c1 = S.One
for n in range(1, N+1):
c2 = S.One
for nu in range(0, n):
c3 = x_list[n]-x_list[nu]
c2 = c2 * c3
if n <= M:
delta[n][n-1][nu] = 0
for m in range(0, min(n, M)+1):
delta[m][n][nu] = (x_list[n]-x0)*delta[m][n-1][nu] -\
m*delta[m-1][n-1][nu]
delta[m][n][nu] /= c3
for m in range(0, min(n, M)+1):
delta[m][n][n] = c1/c2*(m*delta[m-1][n-1][n-1] -
(x_list[n-1]-x0)*delta[m][n-1][n-1])
c1 = c2
return delta
def apply_finite_diff(order, x_list, y_list, x0=S.Zero):
"""
Calculates the finite difference approximation of
the derivative of requested order at ``x0`` from points
provided in ``x_list`` and ``y_list``.
Parameters
==========
order: int
order of derivative to approximate. 0 corresponds to interpolation.
x_list: sequence
Sequence of (unique) values for the independent variable.
y_list: sequence
The function value at corresponding values for the independent
variable in x_list.
x0: Number or Symbol
At what value of the independent variable the derivative should be
evaluated. Defaults to 0.
Returns
=======
sympy.core.add.Add or sympy.core.numbers.Number
The finite difference expression approximating the requested
derivative order at ``x0``.
Examples
========
>>> from sympy.calculus import apply_finite_diff
>>> cube = lambda arg: (1.0*arg)**3
>>> xlist = range(-3,3+1)
>>> apply_finite_diff(2, xlist, map(cube, xlist), 2) - 12 # doctest: +SKIP
-3.55271367880050e-15
we see that the example above only contain rounding errors.
apply_finite_diff can also be used on more abstract objects:
>>> from sympy import IndexedBase, Idx
>>> from sympy.calculus import apply_finite_diff
>>> x, y = map(IndexedBase, 'xy')
>>> i = Idx('i')
>>> x_list, y_list = zip(*[(x[i+j], y[i+j]) for j in range(-1,2)])
>>> apply_finite_diff(1, x_list, y_list, x[i])
((x[i + 1] - x[i])/(-x[i - 1] + x[i]) - 1)*y[i]/(x[i + 1] - x[i]) - \
(x[i + 1] - x[i])*y[i - 1]/((x[i + 1] - x[i - 1])*(-x[i - 1] + x[i])) + \
(-x[i - 1] + x[i])*y[i + 1]/((x[i + 1] - x[i - 1])*(x[i + 1] - x[i]))
Notes
=====
Order = 0 corresponds to interpolation.
Only supply so many points you think makes sense
to around x0 when extracting the derivative (the function
need to be well behaved within that region). Also beware
of Runge's phenomenon.
See also
========
sympy.calculus.finite_diff.finite_diff_weights
References
==========
Fortran 90 implementation with Python interface for numerics: finitediff_
.. _finitediff: https://github.com/bjodah/finitediff
"""
# In the original paper the following holds for the notation:
# M = order
# N = len(x_list) - 1
N = len(x_list) - 1
if len(x_list) != len(y_list):
raise ValueError("x_list and y_list not equal in length.")
delta = finite_diff_weights(order, x_list, x0)
derivative = 0
for nu in range(0, len(x_list)):
derivative += delta[order][N][nu]*y_list[nu]
return derivative
def _as_finite_diff(derivative, points=1, x0=None, wrt=None):
"""
Returns an approximation of a derivative of a function in
the form of a finite difference formula. The expression is a
weighted sum of the function at a number of discrete values of
(one of) the independent variable(s).
Parameters
==========
derivative: a Derivative instance
points: sequence or coefficient, optional
If sequence: discrete values (length >= order+1) of the
independent variable used for generating the finite
difference weights.
If it is a coefficient, it will be used as the step-size
for generating an equidistant sequence of length order+1
centered around ``x0``. default: 1 (step-size 1)
x0: number or Symbol, optional
the value of the independent variable (``wrt``) at which the
derivative is to be approximated. Default: same as ``wrt``.
wrt: Symbol, optional
"with respect to" the variable for which the (partial)
derivative is to be approximated for. If not provided it
is required that the Derivative is ordinary. Default: ``None``.
Examples
========
>>> from sympy import symbols, Function, exp, sqrt, Symbol, as_finite_diff
>>> from sympy.utilities.exceptions import SymPyDeprecationWarning
>>> import warnings
>>> warnings.simplefilter("ignore", SymPyDeprecationWarning)
>>> x, h = symbols('x h')
>>> f = Function('f')
>>> as_finite_diff(f(x).diff(x))
-f(x - 1/2) + f(x + 1/2)
The default step size and number of points are 1 and ``order + 1``
respectively. We can change the step size by passing a symbol
as a parameter:
>>> as_finite_diff(f(x).diff(x), h)
-f(-h/2 + x)/h + f(h/2 + x)/h
We can also specify the discretized values to be used in a sequence:
>>> as_finite_diff(f(x).diff(x), [x, x+h, x+2*h])
-3*f(x)/(2*h) + 2*f(h + x)/h - f(2*h + x)/(2*h)
The algorithm is not restricted to use equidistant spacing, nor
do we need to make the approximation around ``x0``, but we can get
an expression estimating the derivative at an offset:
>>> e, sq2 = exp(1), sqrt(2)
>>> xl = [x-h, x+h, x+e*h]
>>> as_finite_diff(f(x).diff(x, 1), xl, x+h*sq2)
2*h*((h + sqrt(2)*h)/(2*h) - (-sqrt(2)*h + h)/(2*h))*f(E*h + x)/\
((-h + E*h)*(h + E*h)) + (-(-sqrt(2)*h + h)/(2*h) - \
(-sqrt(2)*h + E*h)/(2*h))*f(-h + x)/(h + E*h) + \
(-(h + sqrt(2)*h)/(2*h) + (-sqrt(2)*h + E*h)/(2*h))*f(h + x)/(-h + E*h)
Partial derivatives are also supported:
>>> y = Symbol('y')
>>> d2fdxdy=f(x,y).diff(x,y)
>>> as_finite_diff(d2fdxdy, wrt=x)
-Derivative(f(x - 1/2, y), y) + Derivative(f(x + 1/2, y), y)
See also
========
sympy.calculus.finite_diff.apply_finite_diff
sympy.calculus.finite_diff.finite_diff_weights
"""
if derivative.is_Derivative:
pass
elif derivative.is_Atom:
return derivative
else:
return derivative.fromiter(
[_as_finite_diff(ar, points, x0, wrt) for ar
in derivative.args], **derivative.assumptions0)
if wrt is None:
old = None
for v in derivative.variables:
if old is v:
continue
derivative = _as_finite_diff(derivative, points, x0, v)
old = v
return derivative
order = derivative.variables.count(wrt)
if x0 is None:
x0 = wrt
if not iterable(points):
if getattr(points, 'is_Function', False) and wrt in points.args:
points = points.subs(wrt, x0)
# points is simply the step-size, let's make it a
# equidistant sequence centered around x0
if order % 2 == 0:
# even order => odd number of points, grid point included
points = [x0 + points*i for i
in range(-order//2, order//2 + 1)]
else:
# odd order => even number of points, half-way wrt grid point
points = [x0 + points*S(i)/2 for i
in range(-order, order + 1, 2)]
others = [wrt, 0]
for v in set(derivative.variables):
if v == wrt:
continue
others += [v, derivative.variables.count(v)]
if len(points) < order+1:
raise ValueError("Too few points for order %d" % order)
return apply_finite_diff(order, points, [
Derivative(derivative.expr.subs({wrt: x}), *others) for
x in points], x0)
as_finite_diff = deprecated(
useinstead="Derivative.as_finite_difference",
deprecated_since_version="1.1", issue=11410)(_as_finite_diff)
as_finite_diff.__doc__ = """
Deprecated function. Use Diff.as_finite_difference instead.
"""
def differentiate_finite(expr, *symbols,
# points=1, x0=None, wrt=None, evaluate=True, #Py2:
**kwargs):
r""" Differentiate expr and replace Derivatives with finite differences.
Parameters
==========
expr : expression
\*symbols : differentiate with respect to symbols
points: sequence or coefficient, optional
see ``Derivative.as_finite_difference``
x0: number or Symbol, optional
see ``Derivative.as_finite_difference``
wrt: Symbol, optional
see ``Derivative.as_finite_difference``
evaluate : bool
kwarg passed on to ``diff``, whether or not to
evaluate the Derivative intermediately (default: ``False``).
Examples
========
>>> from sympy import cos, sin, Function, differentiate_finite
>>> from sympy.abc import x, y, h
>>> f, g = Function('f'), Function('g')
>>> differentiate_finite(f(x)*g(x), x, points=[x-h, x+h])
-f(-h + x)*g(-h + x)/(2*h) + f(h + x)*g(h + x)/(2*h)
Note that the above form preserves the product rule in discrete form.
If we want we can pass ``evaluate=True`` to get another form (which is
usually not what we want):
>>> differentiate_finite(f(x)*g(x), x, points=[x-h, x+h], evaluate=True).simplify()
-((f(-h + x) - f(h + x))*g(x) + (g(-h + x) - g(h + x))*f(x))/(2*h)
``differentiate_finite`` works on any expression:
>>> differentiate_finite(f(x) + sin(x), x, 2)
-2*f(x) + f(x - 1) + f(x + 1) - 2*sin(x) + sin(x - 1) + sin(x + 1)
>>> differentiate_finite(f(x) + sin(x), x, 2, evaluate=True)
-2*f(x) + f(x - 1) + f(x + 1) - sin(x)
>>> differentiate_finite(f(x, y), x, y)
f(x - 1/2, y - 1/2) - f(x - 1/2, y + 1/2) - f(x + 1/2, y - 1/2) + f(x + 1/2, y + 1/2)
"""
# Key-word only arguments only available in Python 3
points = kwargs.pop('points', 1)
x0 = kwargs.pop('x0', None)
wrt = kwargs.pop('wrt', None)
evaluate = kwargs.pop('evaluate', False)
if kwargs:
raise ValueError("Unknown kwargs: %s" % kwargs)
Dexpr = expr.diff(*symbols, evaluate=evaluate)
return Dexpr.replace(
lambda arg: arg.is_Derivative,
lambda arg: arg.as_finite_difference(points=points, x0=x0, wrt=wrt))
|
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