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thermodynamics of nanoscale small systems
How to measure the temperature of a nanotube?
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No temperature at all
The answer is: no temperature at all.
Do not even think about measuring it.
This is a weird world
When going to the scale of few (say less than 100,000) atoms, which is possible for today's technology, one cannot even define the temperature.
This is a weird world. Some continuum concepts, like temperature, do not even exist.
How to hold a small system at a fixed temperature?
One way to think about temperature and a small system is to allow the small system to exchange energy with a much larger system (i.e. a reservoir of energy). The temperature of the reservoir is well defined. The reservoir is so large that, as the small system draws energy from the reservoir, the temperature of the reservoir remains unchanged.
Thus, the small system fluctuates from one quantum state to another quantum state. The probability for the small system to be in any one of its quantum state, of course, follows the Boltzmann distribution.
This picture is what we mean by saying "a system is held at a fixed temperature". In this sense, we can hold an arbitrarily small system at a fixed temperature.
I have collected my notes on temperature and the Boltzmann distribution, along with several other topics, in Statistical Mechanics. In these notes, I have deliberately treated the subject as an experimental science: all quantities must be measurable, including the number of quantum states of an isolated system. I'm particularly happy with the section on temperature. Several students have kindly mentioned to me that they appreciate this attitude.
isolated N-atom system
Give you a system of N atoms. If the system is isolated, i.e., not attached to any reservoir. How do you define the temperature of the N-atom system?
Operational definitions of temperature rely on thermal contact
At a basic level, defining temperature of any system requires thermal contact, namely, exchanging energy between systems. Here is the definition of the absolute temperature T
1/T = change in the logarithm of the number of quantum states divided by the change in the energy of the system, everything else being fixed.
All relative temperature scales are also defined via thermal contact. So far as I know, there is no operational definition of temperature other than those based on thermal contact.
Informal definition of temperature
Henry, Zhigang's explanation of temperature is spot on. However, if you want another "intuitive" notion regarding temperature of, say a nanotube (which you quoted), then you may think of temperature as the measure of the velocity or kinetic energy of the atoms. In fact, this notion is used to compute the temperature of a molecular dynamics ensemble. While at the level of each atom, all you can calculate is its kinetic energy, when you have an ensemble, statistical mechanics provides a route to compute the so-called temperature.
Pradeep, for a nanosystem
for a nanosystem, the total number of atoms, N, is limited.
When N is small, say N=100 which is possible for today's technology, the classical statistical mechanics adopted in molecular dynamics, which calculates the temperature based on the information of each atom, velocity, d6es not make sense.
Sure, for very small number
Sure, for very small number of atoms, stat mech may not be the solution but I am speaking of physical intuition. While the concept of "hotness" etc. are somewhat useless at that scale, relating temperature to the degree of motion of an atom provides an intuitive understanding of what temperature means at that scale
cannot be used quantitatively
Yes, you are right. Therefore, the temperature computed based on the sum of atomic kinetic energy, as in many classic molecular dynamics calculations, cannot be used quantitatively, but only qualitatively for physical intuition.
Mr Tan, But it
Mr Tan,
But it should make sense, as the molecules/atoms vibrate or move around, they do so because they have velocity. And when we talk about molecular dynamics wont we say KE = (1/2)mv2 where KE = (3/2)NkT (for a 3D system, K - Boltzmann's constant?)
Then we do have energy and thus 'temperature'.
statistical meaning
But the statistical meaning of the temperature is missing, which is the theme of this series of talk.
Re: statistical meaning of temperature
In teaching a course last spring, I updated my notes on temperature. The central aim of the notes is to reconcile the empircal notion of temperature and its statistical meaning. Hope that the notes help.
I read your lecture notes
Dear Zhigang,
I read your lecture notes on "Statistical Mechanics" posted in http://imechanica.org/node/288. They are very interesting and useful to me. I can understand the effort in reconciling the empirical notions and their statistical meaning.
However I feel that your notes are not complete, or self-sufficient in other word, in giving statistical meaning. The "quantum state" is the fundamental concept in your notes on isolated system, temperature, probability, entropy, free energy, and etc. Yet the "quantum state" itself is undefined.
quantum states and the fundamental postulate
The fundamental postulate is also intriguing. It says that a system isolated for a long time is equally probable to be in any of its quantum states. That our world is described by quantum states may be regarded as a law itself.
When saying that a system needs "a long time" to be in any of its quantum state, there are some questions:
1) How long?
2) If "time" is involved, it seems that a system needs time to evolve from one state to another state i.e., from one quantum state to another requires a mechanism?
3) During the time that is not that long, what is temperature?
Thermodynamics of irreversible processes
These are excellent questions, but generally useful answers do not exist. They belong to nonequilibrium phenomena.
For one class of nonequilibrium phenomena, the system is not in equilibrium as a whole, but the system can be divided into small elements, each element being in a state of equilibrium. One can follow the thermodynamics of irreversible processes to anaylze how the system as a whole approaches a state of equilibrium.
A classical example is conduction of heat in a solid. While the entire body is not in a state of equilibrium, each small element of the body is in its own state of equilibrium. It is not meaningful to talk about the temperature of the entire body, but one can talk about the temperature of each element of the body, and apply the equilibrium thermodynamics to every element. One then describes the conduction of heat by using a kinetic law (i.e., Fourier's law).
As another example, in my course on advanced elasticity, I describe nonequilibrium phenomena in gels.
An independent value (if exists), measuring it or not
I do not agree with Zhigang. If there is a temperature for a nanoscale small system, then, measuring it or not, temperature should be an independent state variable.
Quantify a notion through its experiemntal consequence
We may have entered the muddy water of philosophy of science, of which I'm not qualified to comment, but I agree with Zhenyu, if a notion has no measurable consequence, you may not be bothered to define it. If a notion does have experimental consequence, it might be possible to define a quantity through experimental consequence.
The notion of hotness can be quantified through the experimental consequence of thermal contact.
- In the case of two macroscopic systems, we can talk about the temperature of either system.
- In the case of a small system in contact with a heat reservoir, however, we do have a well defined way to characterize the system: the Boltzmann distribution.
Boltzmann distribution
In the derivation of the Boltzmann distribution for a small system, the system and the reservoir are in thermal contact, exchanging energy. All other modes of interactions between the system and the reservoir are blocked: no exchange of molecules, of volume, or anything else.
This block requirement works fine for macroscopic system.
However, for a nanoscale system the energy changes are associated with volume change which cannot be ignored as in macroscopic systems.
Therefore, the Boltzmann distribution needs to be modified to characterize nanoscale systems.
definition of temperature
Zhigang's definition of temperature should be changed to:
1/T = change in the logarithm of the number of quantum states divided by the change in the average energy of the system, everything else being fixed.
T is called the fundamental temperature.
The Kelvin temperature (absolute temperature) is
Boltzmann constant * fundamental temperature
The textbook definition of temperature
Dear Henry: I wish this were my definition. This is the definition in textbooks. For example, in Kittel and Kroemer, and in Landau and Lifshiz. A while back I wrote a fanatic short review of K-K. It was that book that made me "see" the subject.
I'm not entirely sure why you insert "average" in the above definition.
I'm imagining a system that can exchange energy with the rest of the world, while all other modes of interaction are blocked. Thus, the system is not an isolated system. However, when the energy of the system is held at a constant value U, the system becomes an isolated system, and has a certain number of quantum states Ω. As the energy changes, the number of quantum states changes as a function of the energy, Ω(U). This function characterizes a family of isolated systems.
For example, an electron and a proton form a hydrogen atom. The two-particle system can absorb energy by receiving photons. Thus, the system may be viewed as a family of isolated systems. According to quantum mechanics, the function Ω(U) takes the following values:
Ω(-13.6 eV) = 2, Ω(-3.39 eV) =8, Ω(-1.51 eV) = 18,...
For a large system, the discreetness in energy is small compared to the total energy, so that U may be treated as a continuous variable, and Ω(U) may be treated as a continuous function. In this case, an analysis of thermal contact leads to the definition of temperature:
The unit of temperature was discussed elsewhere in this thread.
Thank you, Henry, for initiating this thread of discussion. As you pointed out, the subject is really hard. I'm not sure if I have got everything correct. Please do point out if you find that I'm doing things wrong.
The word "average" should be removed
The word "average" in my last post should be removed. I was wrong.
A puzzle on entropy, temperature, ...
Here is a puzzle.
Give you two isolated systems A1 and A2. For system A1, the number of quantum states is N1; and for system A2, the number of quantum states is N2.
To simplify the quantum mechanics calculations, we assume A1 is a cubical box with side length a and containing only 1 electron; and so for A2, a cubical box with side length a and containing only 1 electron.
Now bring A1 and A2 together by putting the two boxes side by side. The system A=A1+A2 occupies space (a * a * 2a). Solving the Shrodinger equation for two electrons confined in the box A (not easy!), this gives the number of quantum states as N.
Obviously, N does not equal to N1+N2.
The fundamental assumption in statistical mechanics that
is violated!
Therefore, entropy ( = logN ) is not a well defined concept!
Then all other things, such as temperature, ...?
On the validity of S = S1 + S2
Dear Henry:
You probably mean to write
N=N1 x N2.
So when S = log N, you will have
You put your finger on an important point. In an introductory discussion of thermal physics, we analyze system in weak interaction, so that N=N1 x N2 is true. As I discussed in my notes on temperature, physically it means that all the interfacial states are negligible.
In your example, you have two electrons, so that the "interfacial state" is all you get, not negligible. In such case, we have no reason to assume N=N1 x N2.
But this is not the end of the game. Any time you get an interfacial phenomenon, you will violate N=N1 x N2. You will introduce excess quantities.
I'm not sure how to deal with your 2 electrons, though.
Thank you, Zhigang, Yes, I
Thank you, Zhigang,
Yes, I meant to write
Extensive vs. non-extensive entropy
I'll keep it short (lest I am off-the-mark). The additivity of entropy S = S1 + S2 assumes extensivity, whereas for systems that interact/exhibit long-range interactions (gravitational field is an example), the notion of entropy has been generalized to describe such non-extensive systems. Such entropic measures (Renyi, Tsallis and others are well-known) lead to non-extensivity, and the presence of an additional term (S = S1 + S2 + S1*S2*(1-q)). Tsallis statistics as it has come to be known is purported to be a generalization of Gibbs-Boltzmann statistics. Tsallis's entropic measure is non-extensive when q is not equal to 1 (q = 1 reduces to Shannon's measure). Tsallis entropy has received (for and against) much attention in the physics literature and also in areas outside it (networks, turbulence, finance, etc.) and it is used to describe many a complex systems (edge of chaos) that exhibit power-law distributions. An article that appeared in Science summarizes the gist of it all; Tsallis's original article appeared in 1988. So, instead of the Shannon entropy measure, use of Tsallis's non-extensive entropic measure in Jaynes's maximum-entropy formalism has been pursued.
nanoscale thermodynamics
Many thanks to Sukumar for bringing Tsallis's non-extensive statistics into our attention.
As the size of systems becomes smaller to nanoscale, effects of fluctuations and contributions from surface play more important roles.
I searched the literature, there are currently three approaches for nanoscale thermodyamics:
(1) generalizing the Boltzmann-Gibbs statistics as to take account of the non-extensive feature of such systems, e.g., Tsallis statistics (http://en.wikipedia.org/wiki/Tsallis_entropy);
(2) a modification of the Boltzmann-Gibbs statistics by adding subdivision energy;
(3) non-equilibrium thermodynamics including work fluctuations.
Thermodynamics is a funny subject
Arnold Sommerfeld, the theoretical physicist and teacher, once said, maybe even more than once, that:
"Thermodynamics is a funny subject.
The first time you go through the subject you don't understand it at all.
The second time you go through it, you think you do understand it, except for one or two small points.
The third time you go through it, you know you don't understand it, but by that time you are so used to the subject that it doesn't bother you any more."
I think I am in the stage of second time.
one has to learn at least three times
Sommerfeld's words remind me of Zhigang's comment (http://imechanica.org/node/207):
"...... As many people say, thermodynamics is a subject that one has to learn at least three times."
Thermodynamics and nanotechnology
Thermodynamics, largely driven into being by the steam engine, should be pushed into a further mature stage, driven by the nanotechnology that controls matter on the atomic scale.
here, ensemble of classical mechanical system does not work
Ensemble of classical mechanical system does not work for a nanosystem. One has to use the ensemble concept in quantum statistical mechanics.
Again, the importance is the length scale
Again, the importance is the length scale. Below what length scale, the temperature is meaningless? This may also depend on the material.
All their results are problematic
Searching the literature, I found many papers (at least one hundred) devoted to studing the temperature-dependent behaviors of nanotubes, nanowires, etc, using the classical molecular dynamics.
However, all their results are problematic.
Nanotubes present no challenge to statistical thermodynamics
As discussed above, you can hold arbitrarily small system at a fixed temperature by letting the small system exchange energy with a heat reservoir. In doing experiment with a nanotube, perhaps a holder will allow the nanotube to exchange energy with the environment.
I'm not familiar with how calculations are carried out, but at least conceptually and in experiments, nanotubes and such present no fundamental challenge to statistical thermodynamics.
a serious challenge to statistical thermodynamics
Let two nanotubes, one with temperature T and the other with the same temperature T, have thermal contact by putting them together. After reaching thermal equilibrium, the final temperature of the system is not T.
Therefore nanotubes, and other nanoscale system, present a serious challenge to statistical thermodynamics.
No need to define T for isolated systems
Reading through this line of discussions, I will have to agree with Zhigang (and some others), in the sense that there is even no need to be bothered by how the temperature should be defined for truly isolated systems, be they classical/macroscopic or quantum (such as those containing only very few numbers of elemental entities). Such systems, treated typically using microcanonical ensembles, are fully described by physical quantities such as the total (and conserved) energy, the volume, etc., with no specification of the temperature.
T claims its physical identity when a system is exchanging energy with its outside world, but by then the system is no longer isolated.
---Just some stochastic thoughts while fighting a cold and fever...:)
There is a need to define temperature for carbon nanotubes
Several structure changes due to increased temperature in Carbon Nanotubes (CNTs) were reported in Dr. Markus J. Buehler's paper (http://imechanica.org/node/917)
(1) thermal energy becomes sufficient to induce significant bending in the CNTs, even without application of external forces.
(2) temperature increase could induce unfolding of the racket-like structure of CNTs.
(3) the ripple shell buckling of single wall carbon nanotubes under compressive loading strongly dependents on the temperature.
What about Thermodynamic Laws in Nano Scale?
I heard some things about Nano-Scale Thermodynamics Law?
What's the state of Thermodynamic laws in nano-scale?
to what extent the thermodynamic concepts can be extended
Thermodynamics at nanoscale is a indespensible issue, in the face of the rapid miniaturization of many technical devices such as computer chips, the trend to utilize quantum mechanical systems, and the biological cell response in an nano-environments.
Currently, I think it is not clear to what extent the thermodynamic concepts can be extended to the nanoscale and which limits should be taken into account.
Violation of the 2nd law in nano-scale
Although this interesting discussion that I have tried to follow is not in my particular field, the current point has reminded me a paper published by the American Physical Society in 2002.
This is the paper just in case you have not seen:
Wang et al., "Experimental Demonstration of Violations of the Second Law of Thermodynamics for Small Systems and Short Time Scales", Physical Review Letters 89, 050601 (2002).
Here is another one:
Carberry et al. "Fluctuations and Irreversibility: An Experimental Demonstration of a Second-Law-Like Theorem Using a Colloidal Particle Held in an Optical Trap", Physical Review Letters 92, 140601 (2004).
Best regards,
Alper Erturk
time reversible nano-system (Loschmidt's paradox)
Dear Alper, thanks for pointing out the interesting paper of Wang et al.. I copied the first paragraph of their paper and pasted it here. I also provided a useful link for "Loschmidt's paradox".
Inventors and engineers endeavor to scale down machines and engines to nanometer sizes for a wide range of technological purposes. However, there is a fundamental limitation to miniaturization as small engines are not simple rescaled versions of their larger counterparts. If the work performed during the duty cycle of any machine is comparable to thermal energy per degree of freedom, then one can expect that the machine will operate in ''reverse'' over short time scales. That is, heat energy from the surroundings will be converted into useful work allowing the engine to run backwards. For larger engines, we would describe this as a violation of the second law of thermodynamics, as entropy is consumed rather than generated.This has received little attention in the nanotechnology literature, as there was no quantitative description of the probability of entropy consumption in such small engines. The only thermodynamic statement available was the second law itself, stating that, for large systems and over long times, the entropy production rate is necessarily positive. Even the foundations of statistical mechanics were unsettled as thermodynamicists questioned how the second law of thermodynamics could be reconciled with reversible microscopic equations of motion. Loschmidt's paradox (http://en.wikipedia.org/wiki/Reversibility_paradox) states that in a time reversible system, for every phase-space trajectory there exists a time-reversed antitrajectory. As the entropy production of a trajectory and its conjugate antitrajectory are of identical magnitude but opposite sign, then, so the argument goes, one cannot prove that entropy production is positive.
bridging microscopic & macroscopic domains of thermodynamics
Dear Alper, thanks for pointing out the interesting paper of Carberry et al.. I copied the abstract of their paper and pasted it here.
The puzzle of how time-reversible microscopic equations of mechanics lead to the time-irreversible macroscopic equations of thermodynamics has been a paradox since the days of Boltzmann. Boltzmann simply sidestepped this enigma by stating ''as soon as one looks at bodies of such small dimension that they contain only very few molecules, the validity of this theorem [the second law of thermodynamics and its description of irreversibility] must cease.'' Today we can state that the transient fluctuation theorem (TFT) of Evans and Searles is a generalized, second-law-like theorem that bridges the microscopic and macroscopic domains and links the time-reversible and irreversible descriptions.
Temperature of nanotubes and Prof. Suo's notes...
Some comments, in no particular order...
Prof. Zhigang Suo points out that temperature and energy have the same dimensions. This is an insightful statement, but requires certain qualifications to be made.
1. The equivalence between the two concepts is obtained after assuming many prior assumptions. It might be interesting to trace the route through which the equivalence is obtained.
First, a primarily kinetic description of the system is assumed. The system is taken to primarily consist of moving point-masses; let's call them particles. The motion of the particle is taken to remain restricted to a certain finite region of space. The total number of particles in the region may be taken to stay unchanged over any length of time. The collisions with the bounding surface usually are taken to be "perfectly" elastic.
The reason the particle is taken as a point-mass is that by doing so, the internal structure of the particle can be treated as of no consequence to the statements made within the framework of the theory. The same assumption also does away with any theoretical complications arising due to the spatial extents of the mass, e.g., complications due to moments, directions in collisions, etc.
Note that we talk about the mass and energy *of* the system. In other words, we do make meaningful statements about the system in and by itself, i.e., even if there is nothing outside of it. Thus, something outside of the system is not necessary to impart meaning to a given system itself or to any of its properties. In particular, no external reservoir is necessary to define temperature of the system.
The system here is identified as the sum total of the masses and their motions within a particular spatial region, together with the boundaries of the region and the special properties of the boundary such as the perfectly elastic collisions they give rise to.
Provided conditions such as above are met, even the entire universe can be taken, in an abstract sense, to be an isolated system. In any case, it's worth noting that every isolated system is actually an abstraction.
2. If the kinetic theory of matter (e.g. the atomic hypothesis of Dalton) is applied to a thermodynamically macroscopic system, then, completeness requires that every macroscopic property have some description in the kinetic-theoretic terms as well.
The kinetic-theoretical concept equivalent to temperature in thermodynamics turns out to be the *kinetic* energy of particles (e.g. atoms).
Note, only the kinetic energy is involved here, potential energy in any of its forms is not. The reason is that the kinetic theoretical abstraction primarily omits any form of interaction between the constituent particles making up the system.
Now, the above manner is not how actual atoms or subatomic particles behave. The small broken pieces of matter such as atoms (and, electron, protons, neutrons, even quarks...) do interact with the other small pieces. But this fact is against the spirit of the kinetic theory.
The interaction between particles is the fundamental reason why real gases deviate from the ideal gas law. It also is one fundamental reason why the temperature<->energy equivalence has only a limited, i.e. qualified, validity.
3. Note, temperature is primarily a property of the system--not of its constituents.
However, as a result of the fact that there can be no interactions among constituents, the simple additivity rule can be assumed. Hence, it is possible to linearly subdivide a given system into a number of constituent *systems.*
The constituent systems may conveniently be built so as to isolate a single particle, e.g. an atom.
It is then that one may ascribe a temperature to a single constituent, e.g., an atom.
4. Note, by the premises of kinetic theory, it really does not matter whether the system description carries one particle or N particles.
Even a subsystem may carry any number of particles. If the decomposition is not in integral terms, it's even permissible to think of a subsystem as carrying a fractional number of particles.
The kinetic abstraction itself is silent on these issues and its structure is equally applicable to all such possibilities.
5. Let's apply the above principles to a concrete case. Consider a moving car. It is possible to think of an abstract system consisting of this car and nothing else in the world.
If this abstract system is taken to exchange no matter or energy with anything else, then it can be taken as an isolated system. (Note, isolated systems are necessarily abstractions.)
Inasmuchas the car may be represented as a point-mass in an abstract system, it is also permissible to ascribe a "temperature" to that system.
Note, the actual hotness of the car (say due to its running engine), or the possibility of measuring it using a thermometer, has been summarily ignored right in the act of modeling it as a point-mass. Hence, its real temperature (say 27 degrees Celsius) does not at all enter into the discussion. The temperature of the system we mean here is the one which the car possesses by virtue of its motion--i.e. out of its kinetic energy.
Finally note, the issue is not really speaking microscopic vs macroscopic, or QM vs classical, etc. The issue is: Can you meaningfully speak of something in the terms of the kinetic theory or not, that's all.
6. If a principle that correlates the kinetic energy of a nanotube (say due to vibrations of the ionic cores and waves in the lattice gas) with something external can be discovered, then, even an experimental measurement of the temperature of the nanotube will be possible.
So, the question "Can you measure the temperature of a nanotube?" is not one ruled out by basic physical principles. It is to be answered by through developments in the experimental science.
7. To conclude:
- The description of temperature in terms of energy is not at all quite on the same footing as its description as a sensory quality.
- The temperature<->energy equivalence is not an unqualified one. Indeed, this equivalence denotes a high-level abstraction.
- Temperature is a property of the system, primarily, not of the point-masses. But the premise of composition allows us to ascribe temperature to individual entities--by assuming smaller systems encompassing the individual entities.
- Accordingly, even a single atom, electron, quark, etc. can be taken to possess a temperature. The procedure is meaningful in the above context.
- Yet, since such a description involves high-level abstractions, a certain amount of restrain must be exercised while using the term "temperature," especially when scientists make statements to lay people.
For example, the statement that a temperature of a billion K was reached in a laboratory can be careless if there is no explanatory context provided. In today's technology, such a temperature is reached only for a single constituent particle. But lay people take it to mean as if a whole assembly palpable at the gross scale was heated to that temperature. To not take the care to spell out the explanatory context is to mislead the public.
- It is alright to think of the temperature of nanoparticles even if the particles are made of only a few hundred atoms.
Temperature and energy are not equivalent
Dear Ajit: Thank you very much for your comments on my notes on temperature. I wish to reiterate a few points.
In the notes, I adopted the following definition of temperature T:
1/T = change in the logarithm of the number of quantum states divided by the change in the energy of the system, everything else being fixed.
- This temperature has the same dimension as energy.
- To preserve the notion of hotness, any monotonically increasing function of T can equally well be called the temperature.
- In particular, the SI unit asks you to rescale the above T with a linear factor, such that the triple point of a pure water is by definition 273.16K (exact). The conversion factor k (known as the Boltzmann constant), can be determined experimentally by this definition. See a website of NIST for detail of the defintion of Kelvin as a unit of temperature.
- Thus, k is a factor to convert two units of hotness, just like 2.54 is the factor to convert inch to centimeter. (If I were Boltzmann, I'd be amused to be reduced, without my knowledge, to a conversion factor!)
- Just because the two quantities have the same unit does not mean they are equivalent. I don't think that we should say that temperature and energy are equivalent. The above definition of T has made their nonequivalence quite clear.
- As outlined in my notes on temperature, the above definition does lead to experimental procedure to measure temperature, as well as measure the number of quantum states.
About equivalence...
Dear Zhigang,
It's nice that you reproduced the pertinent part of your notes for convenience of the reader's reference.
Frankly, though, I cannot understand why you wouldn't say the two are equivalent once the appropriate context was being specified. (Not necessarily the one I mentioned, but let's assume that a proper context has been given....)
IMHO, any time the physical dimensions of two quantities are identical, and the two concepts also refer to the same or similar phenomena, then the cognitive policy of theoretical integration requires that one also try and see the way in which the two concepts may be related, even equivalent.
In saying "equivalent," one still keeps the two concepts separate. The concepts still do not become "interchangeable" or "identical." Yet, there are contexts where the theoretically similar concepts are much more than being merely "analogous."
The parallels between the kinetic theory and thermodynamics (or particles and fields, speaking more broadly) is one such a context where, IMHO, it's perfectly OK to say "equivalent". On the other hand, the out-of-plane displacements of a soap membrane and the potential of an electrostatic field could never become "equivalent"--they must remain "analogous."
The basic test, I would suppose, is that in drawing theoretical parallels between two theories describing the same sphere of physical phenomena, if the two concepts go on to produce exactly the same physical effects, then, within the scope of the comparison, the two concepts should be regarded as equivalent--on the grounds that their "valence" (or capacity to produce effects) was equal.
But I suspect by now all this hair-splitting must have become positively boring, so let me stop!
It's just that your observation about the identity of the dimensions was really fine and got me thinking... It's a very fundamental point you made in your notes, and it's worth investing some thinking about... It's something like Planck's constant (having units of the physical "action") or the physical meaning of the constancy of speed of light (which Feynman asks in his Lectures to ignore through scaling, somewhat similar to the way you note Boltzmann's constant as a constant of scaling).
Before closing, let me add a word: I am new to iMechanica, being here for only about a month or so. But, it has been my pleasure to be a member here. Sometimes one does write at length. (In my case, most of the times!) Then, there are those other times when one feels like taking a shot in the dark, to be not very precise! I can understand that... In any case, the informality of a blog site preciesly is its strength! I am happy to have this chance to write more informally than in a paper, but more formally (and for a wider audience) than in a personal level talk...
So, my special thanks go to you and also to others (say the moderators) for taking this initiative...
Energy and temperature are not equivalent, really.
To see that energy and temperature are not equivalent, take a look at the following statement:
"When two systems are in thermal contact, energy goes from the system with high temperature to the system with low temperature."
If you swap the positions of the two words, energy and temperature, the statement becomes amusingly wrong.
Stick to equivalence; your example is of interchangeability...
I too initially found the example amusing but for a somewhat different reason--out of the fact that despite having clearly spelt out interchangeability as different from equivalence in my *immediately* above post, you still ask the reader of your site to consider an example of interchangeability as if it were an example of equivalence.
So, initially, I was amused.
But soon later on, I took a more serious view of it. This is the second time within a week or so that a superfluous post has been added after my entry, mandating nothing but reiterations. That too from people one would ordinarily take to be responsible, understanding and mature. I ignored the occurrence the first time, but now I must speak out.
It is this necessity to reiterate which leads me to suspect if people here consider having the last post as a prestige issue of sorts or what!
If so, I wouldn't mind being as speedy in leaving this forum as I was in joining it.
So what if it's Harvard, Stanford, or Cambridge or any other university out there! Truth, in my mind, is above all those institutions, let alone a very small community that is iMechanica. When truth becomes so easily dispensable as the click of a button and an addition of an entry just to have it as a last entry (on the lines of having the last laugh of sorts), I would have nothing to do with that kind of a forum--even if the sponsoring institution made a rather large song and dance about "VERITAS" in the logo. I could do better not to post at such a site. After all, I do have a personal Web site of my own, and Yahoo!, msnbc.com and other newsmakers *have* been following my case mindlessly for years too! So, if the whole matter is to keep praising publicly some people and to indirectly drive some others to a position that, to a casual reader, would show a lack of temperament on those others' part, then I know this is routine in Internet, but I would have none of it.
Once again, note, mindlessly adding entries not recognizing the contents of the previous posts is happenning for the second time in just one week for posts made by me. Once again, ask yourself if you are *not* giving an example of interchangeability in the name of equivalence.
Do let me know, publicly, if I should discontinue to be a member here.
That said, in the meanwhile, coming back once more, and from my side, for the last time, to the same physics as I explained right above:
If you really are consistent in holding the meanings of the terms, there indeed is no contradiction in the statement you offered at all. So, there is no reason for amusement. Consider this rephrasing of your statement (on the lines of equivalence, but not interchangeably, which simplycannot be done as I already said):
"When two systems are in thermal contact, the temperature of the system which has the higher level of kinetic energy goes down whereas the temperature for the system which has a lower level of kinetic energy goes up."
Tell me, what is wrong with this? And was is so hard to think up this example? Especially after having gone through my well explanatory post?
Let me know, on other points, publicly.
re: Stick to equivalence; your example is of interchangeability
Dear Ajit:
I have benefited from this thread of discussion. If anything that I posted has ever offended you, please accept my sincere apology. It is wholly unintentional. This message is not intended as the last word on anything. I simply feel that I should respond to your requests.
In online discussions, our intentions, unaided by facial expressions but quickened by a push of a button, may not be clear to each other. Such is the limitation of this mode of communication. One may recall the same situation in early days of emails. By now most of us have accepted that emails are less formal than snail mails.
We may think of iMechanica as an infinite hallway, where we can "meet" colleagues and discuss anything. People can express their thoughts freely, superfluous or profound or anything in between, just as in a conversation in a real hallway.
I have enjoyed your posts, including those in this thread. If you judge that the benefit of such a communication to you outweighs posts that you judge to be superfluous, then I would sincerely urge you to stay.
Now let us return to the topic of our discussion: temperature and energy. I think I see where you come from. Correct me if I have misinterpreted what you are trying to say.
For a classical gas, the temperature is proportional to average kinetic energy of particles. Indeed, for a classical gas, the temperature and the average kinetic energy are equivalent and interchangeable.
I have added the word average. I think that you would agree the word average is significant here. It makes the temperature an intensive quantity. The total kinetic energy is an extensive quantity. Thus, in thermal contact, the sum of the energies in the two systems is constant, but the sum of the temperatures of the two systems need not be constant. In equilibrium, the energies of the two systems need not be equal, but the temperatures of the two systems are equal. Even in this special case of classical gas, the temperature is not equivalent or interchangeable with total energy.
The statement you made between quotation marks will be correct if you replace the word "system" by the phrase "classical gas", and replace the the phrase "level of kinetic energy" by "average kinetic energy".
A generally applicable definition of temperature is (I apologize to repeat this again):
1/T = change in the logarithm of the number of quantum states divided by the change in the energy of the system, everything else being fixed.
This definition makes it clear that temperature involves two distinct quantities: the energy of a system, and the number of quantum states of the system. Both quantities depend on the size and the kind of the system (a piece of cheese or a glass of wine). Yet when two systems reach thermal equilibrium, the temperatures of the two systems are equal. Thus, temperature has this property that energy does not have.
Winding up my discussion in this thread for the time being...
Dear Zhigang,
Thank you for your reply.
Your apology was not necessary for a matter like this, and an apology wouldn't have been sufficient by itself either! But forget it! The way I look at it, when there is that sincerity to your words, *that* is enough by itself.
For the time being, I have decided to stay with the forum. Yet, I simply cannot be light-hearted about it; not yet. One man doesn't make a forum.
There is my experience of Americans, who often are mere power lusters but packaged in smooth or civilized appearances. Then, there are those arrogant and suppressive Harvard graduates and the companies they run that one does come across. I can cite Mr. Manu Parpia, the man, and Geometric Software, and 3D PLM Software, India, the companies he runs as a CEO. Something similar can be said for Stanford graduates too. I can directly cite Sandip Johri, V/P of Hewlette-Packard, a batch-mate of mine at COEP, and a personal friend *once upon a time*. Other examples where my dignity or my job applications or similar matters have suffered injustice or ill-treatment at the hands of Americans can be cited rather easily too. For example, at the hands of the IIT Bombay alumni in the San Francisco Bay Area (such as Mr. Jaggi Ayyangar), IITians who now are American citizens, people whose power-lust sometimes exceeds that of the American-borns themselves. (One route of harassment used by all such Americans--born in the USA or otherwise--has been by en-masse buying the staff and advertisement space in media, esp. Times of India, Pune edition. The reader may ask Dileep Padagonkar, the then editor, for more details. I am sure he knows me.)
If the reader thinks I have gone too far, he is requested to know more about my competence and skills by visiting my Web site: http://www.JadhavResearch.info, and then note that over the last 6.5 years, I have earned any money at all for precisely 5 months and a few days--not even for a half year (full six months). 6 years is a long time. People finish PhDs and buy houses in that time. Further, I have summarily been denied all my chances in CAE, despite all that hue and cry you undoubtedly hear about India's talent et cetera. (If in doubt, ask the Governor of the State of Virginia in the USA.) And this condition of mine is despite (or may be, because of) Harvard graduates. If this is not suppression, what else do you think would be?
All such factors do play a role in deciding how I should proceed with respect to anything being run by Americans or in America, the more prestigious, the more cautious I must be. (And no, all this writing about America and Americans is *not* a blanket moral certificate of better behavior by other nations or people.)
The above is not an explanation; it is as brief but direct an indication as I can at all give. (This was about third revision to make it further brief, and I cannot make the matter more condensed without losing the personal flavor about it--and then, whose decision and life is it anyways that I am talking about, here?)
Coming to the physics proper. Let me just note some thoughts without explaining them. Apparently, these points will need separate articles.
-- Any extensive property can be turned into an intensive one; simply divide by mass.
-- Your "definition" of temperature has the following roots. Start with the definition of entroy dS = deltaQ/T and Boltzmann's equation: dS = -k ln (w). (delta Q, for inexact differential.) Substitute, rearrange, and scale to remove Boltzmann's constant, k. Then, bring in the interpretation of w as in accordance with a particles approach, here and by your post, quantum states. Note, if the resulting equation is to be taken as giving us a *definition* of temperature then one already is very much within the kinetic-theoretical abstraction.
-- I note that you wish to differentiate classical gas and collection of quanta. I think this insistence is understandable but not really necessary. However, it will take a few more papers just to get going. I will publish them after my PhD thesis is done. Decades of QM developments have got it wrong, and I don't at all blame you personally (or anyone else) for honestly believing so. If anything, I appreciate your concern and the clarity of your expression.
-- I will also explain later more on equivalence in a separate post.
-- I plan not to post for a while. I plan to take my PhD thesis to a better stage of completion and then come back. May be, one week later or so.
Before closing, one more point, a clarification. This point is no reflection on Zhigang or admin or any other member at all but just a noting. Since some part of this post of mine indeed is dramatic, I want to note that if in future there arise some issues (say legal issues) for the iMechanica management out of this post, I will be only happy to leave the forum--but I will not on my own retract it. (My attitude is, and would be: "It moves!")
demonstration and satisfaction
Dear Ajit:
I understand your sensitivity. It will be a bit out of context (he is speaking of mathematics), but please take these words of T. Jefferson regarding the American approach on getting things done:
" ... We have no theories there, no uncertainties remain on the mind; all is demonstration and satisfaction."
Demonstrate your work and satisy our minds, you will be appreciated regardless of anything else.
Please keep writing here!
quotation by Thomas Jefferson
Dear Cetin:
The quotation by Thomas Jefferson was not on "American approach on getting things done", but on his views of mathematics (he was enthusiastic about mathematics).
A complete quotation should be:
"…… Having to conduct my grandson through his course of mathematics, I have resumed that study with great avidity. It was ever my favorite one. We have no theories there, no uncertainties remain on the mind; all is demonstration and satisfaction."
through developments in the experimental science
Agree with Ajit's point that:
The question "Can you measure the temperature of a nanotube?" is not one ruled out by basic physical principles. It is to be answered by through developments in the experimental science.
Please also read my recent post on the world's smallest thermometer (http://imechanica.org/node/1064#comment-1836)
However, Feng' concern is that (
the fluctuation becomes increasing bigger as the size decreases, so the deviation from the mean value increases.
Also, Cetin concluded (http://imechanica.org/node/1064#comment-1809) that
that phonons are hard to observe experimentally.
the concept of phonon is challenged
Thanks to Zhigang and others. I may need to change a little bit of my points (thermal physics is alway a hard topic):
The definition of temperature based on the number of quantum states, as in Zhigang's note and his comments here, is always true and fundamental.
The problem comes from here. To be applicable, the temperature of a solid is basically approximated based on the number of phonon modes.
The phonon based definition of solid temperature forms also the basis of the classical molecular dynamics.
Here the question is: for a small nano-system, the concept of phonon is challenged.
is the concept of photon challenged as well?
so, does this mean that you are also claiming that the concept of photons in finite-molecular/atomic systems is challenged?
Experimentally speaking, this is easier to answer since phonons are hard to observe.
how phonons are detected experimentally
Dear Cetin:
Thanks for pointing out the experimental observations.
I do not know how phonons are detected experimentally, and I am interested in knowing that. Could you show some basics, or point out any entry-level references? Thanks.
Imaging Phonons
A book entitled Imaging Phonons by J. P. Wolfe should provide an excellent introduction.
propagation and scattering of high-frequency phonons
Dear Cetin,
Thank you for the information.
I am learning the UIUC Physics Professor James P. Wolfe's phonon-imaging technique, and will be benefited a lot from his book.
Laser excitation of a crystal produces a local source of thermal energy, composed of quantized lattice vibrations (phonons). Phonon imaging can be used to examine the propagation and scattering of high-frequency phonons in crystals.
It is interesting to think about this: Human being knew about temperature and thermodynamics long before they discovered quantum mechanics. But now they have to define temperature based on the quantum states.
temperature for one single atom (my previous point was wrong)
I agree with this, that even for one single atom there is a temperature associated with it. My previous point, that there is no temperature defined for a nano-scale system, was wrong.
I did a quantum mechanics calculation for a single atom confined in a cubical box, by solving the Schrodinger wave equation of the atom.
I got the expression for the number of quantum states n as a function of the U, where U is the thermal average energy of the atom in the box.
Then I proceed to calculate the Kelvin temperature T, according to
T =1/ kB / [ d(log n) / dU ]
where kB is the Boltzmann constant.
I found the relation that
U = 3/2 * kB * T
More on thermodynamics of nanostructures?
I found all you discussions are very stimulating and interesting, so I would like share with you some of my thoughts, and possibly stir the water even more...
Thare have been similar dissussions on wether thermodynamics (equilibrium theory) can be applied to small systems of finite size (such as nanostructures), because they are in principle "metastable" (relative to bulk). For example, one intriguing question whether a finite system (a few atoms) ever melts? If it does, what's the melting temperature?
Temperature, as well as any other thermodynamic state variable, an statistical mean (ensemble average) of certain thermodynamic measure. In dependent of system size, such average (or measure) can always be performed (as suggested Zhigang and others). One concern is fluctuation becomes increasing bigger as the size decreases, so the deviation from the mean value increases, which sometimes makes the analysis "questionable"? For example, temperature fluctuations make the melting point ill defined.
Technically, in fact, some other thermodynamic quantities are even harder to define for the small systems than temperature. As discuss here, one may always calculate temperature by the Boltzman distribution of quantum states or avearging over kinetic energy of atoms (in MD simulation), but the volume of a finite system is in fact somewhat "arbitrary", without a definite position of boundary.
So, extending the question beyond temperature, one asks whether thermodyanics can be applied to a small system that can never be truely "equilibrated" due to large fluctuations? Nevertheless, it has been practically used so far (such as many many MD simulations) possible due to the following reasons: (1) even though metastable, their life time is so long that the nanostructures can be considered at "equilibrium"; (2) cases where fluctuations are not too large to confuse the issue; (3) There is no other better way to treat it, so we do the best we can for now...
nanoscale-size and fluctuating non-equilibrium
nanoscale-size and fluctuating non-equilibrium, seems to be the characteristic of nanoscale thermodynamics.
Entropy and temperature are concepts for a continuum
Entropy and temperature are concepts for a continuum.
Two choices for a nanoscale system:
we can either abandon these continuum concepts by describe the system discretely, or establish some continuum-atomistic coupled models.
Entropy and temperature are not concepts limited to a continuum
Dear Henry:
I'm not sure entropy and temperature are concepts for a continuum. Let us look at the entropy first. For an isolated system, the entropy is simply the logarithm of the number of quantum states of the system:
S = logΩ.
For example, a hydrogen atom can be an isolated system, and we can speak of its entropy. The values of its entropy are listed elsewhere in this thread.
A more general definition seems to belong to Gibbs. I described this definition in my notes on entropy. As I remarked in my response to Sukumar a while back, one can define entropy simply as a property of any probability distribution. Thus, one can speak of the entropy of rolling a die, or entropy of whether tomorrow will rain, for example.
For an isolated system, the fundamental postulate says that every quantum state is equally probable. Then Gibbs's definition is reduced to S = logΩ. This much I did in my notes. What I didn't have time to do in the notes was to develop this line of reasoning into a useful idea. In any case, the entropy has nothing to do with continuum.
We have talked about temperature extensively in this thread of discussion. In particular, one way to hold a small system at a fixed temperature is to allow it to exchange energy with a reservoir of energy. In this picture, one does not speak of the temperature of the system, but speaks of the fluctuation of the system among various quantum states.
As an ancient example of a small system, consider a vacancy in a crystal lattice. We hold the vacancy to a fixed temperature simply by holding the crystal at a fixed temperature. The vacancy can trade energy with the crystal. We can then speak of various states this vacancy is in, e.g., whether it is energetic enough to move to another lattice site.
Perhaps a key to apply thermal physics to small systems is to carefully define an excess quantity. For it is not obvious how to privatize energy to a vacancy. Which part of the energy belongs to the crystal, and which part of the energy belongs to the vacancy?
what is the temperature of an empty space?
You bring a fun, but very important, topic to discuss:
For your ancient example of small system, suppose the vacancy is a vacuum withou anything, what is the temperatur of this vacancy?
Can we still hold this vacancy (purely empty space) to a fixed temperature simply by holding the crystal at a fixed temperature?
Statistical mechanics is a bridge
Dear Zhigang,
Here I used continuum to mean macroscopic matter.
Although temperature and entropy can be defined for a small system (even for a single electron or a single atom), but in practice (applications) statistical mechanics is used as a bridge between the behavior of macroscopic matters and the laws of nature governing microscopic dynamics of their constituents.
How temperature affects the viscoelastic behaviour?
How temperature affects the viscoelastic behaviour? especially viewed from the behaviour of molecular movements?
time-temperature equivalence for a viscouselastic material
How does the time-temperature equivalence for a viscouselastic material be viewed at molecular scale?
Temperature is an important issue in electronic components
Temperature is an important issue in electronic components because of the trend towards miniaturization, which means that the heat is generated over a very small area.
The temperatures outside the working range of electronic circuitry might cause damage.
Nanotechnology: world's smallest thermometer
I checked the nanotechnology development, and found that the world's smallest thermometer used a single carbon nanotube filled with liquid gallium. (My initial question and argument seem funny here -:)
Liquid gallium is used in the nanothermometer because the gallium volume changes linearly with temperature - rising up and down the tube - at a consistent rate when the tube was exposed to different temperatures. It maintained this consistency between 50 and 500 °C.
The instrument is so sensitive that it can measure the temperature change that occur when small groups of molecules react with each other.
research proposals
I am sure that some of the above discussed topics can be polished and further be developed into nice research proposals (the current hit of this blog entry has reached to 1572).
If succeed, can we share the funding?
Nanotubes may have no 'temperature'
An interesting news headline in nanotechwire.com
Physicists have made a bizarre discovery: the concept of temperature is meaningless in some tiny objects. Although the concept of temperature is known to break down on the scale of individual atoms, research now suggests that it may also fail to apply in rather larger entities, such as carbon nanotubes.
The blossoming field of nanotechnology relies on being able to manipulate materials that are made from just a few thousand atoms. Carbon nanotubes, for example, are tiny cylinders that could be used to make miniature electronic devices.
Ortwin Hess from the University of Surrey, Guildford, UK and colleagues say that if you took the temperature at one end of a 10-micrometre nanotube, it would not necessarily have the same temperature as the other end, no matter how long it was left to reach a thermal equilibrium. Such a nanotube is about as long as a sheet of paper is thick.
Ortwin Hess
Professor Ortwin Hess
Department of Physics
University of Surrey
His recent interests include nano-thermodynamics.
temperature at the tip of the nano-indenter
Nanoindentation is a fundamental, evolving, and complementary discipline (Michelle, http://imechanica.org/node/1237).
It iis an interesting topic among imechanicians from many different backgrounds:
Experimental Nanomechanics (Xiaodong, http://imechanica.org/node/606);
Viscoelastic Contacts (Michelle, http://imechanica.org/node/842);
On the uniqueness of measuring elastoplasticproperties from indentation (Xiaodong, http://imechanica.org/node/1222).
The nanoindentation measurements can be even more interesting, when accounting for the temperature at the tip of the nano-indenter.
How can we use the concept of temperature for few atoms
Very interesting topic!
I read the first parts of the book Thermal physics written by C.Kittel under the suggestion of Prof. Suo. I post this comment to explain what I learn form that book.
First, the thermal contact plays a signifcant role in the definition of the temperature and entropy. As for two systems, we can obtain the total degeneracy of all the accessible configurations after the thermal contact. If the number of particles in at least one of the two systems is very large, the numbers of that total configurations can be replaced by the number of the states in the most probable configuration. Only in this case, the additivity of the entropy is valid.
As defined in the lectures of Prof. Suo:1/T = change in the logarithm of the number of quantum states divided by the change in the energy of the system, everything else being fixed. The introduction of temperature is to describe the equilibrium state of two systems under thermal contact. It is noted that this equilibrium state is just the most probable configuration. The formalism of T is also derived from the maximum of total degeneracy of all the accessible configurations. In this sense, we can think T is corresponding to the most probable configuration. However, the states expect the most probable configuration can be observed only when the number of particles in at least one of the two systems is very large. If the two systems are both small, then we can see that many different states expect of the most probable configuration which can be represented by the temperature.
Thus, for a small system with only few atoms, we can define the temperature of this kind system via letting it contact with a very large system. However, when we make two small systems together, how can we obtain the final temperature of these two systems, even though we know the temperature of them before contact. If we make they contact with a large system, this may destroy the states of the real systems and make them have the same temperature of the large system itself.
I am not sure whether my understanding is reasonable or not, however, I hope this can make any help for this topic.
Best regards
Teng Zhang
"thermal contact" of a one-atom system?
For a one-atom, or several atoms, system, how are you going to define the "thermal contact", which is the kernel of the concept of temperature?
temperature without thermal contact
For an isolated ergodic Hamiltonian system with kinetic energy quadratic in the momenta (all standard assumptions), there is a clear definition of the temperature based on the derived result of equipartition. This does not require the notion of thermal contact for the definition, and an entropy for such a system can be defined (non-extensive) to be consistent with the macroscopic thermodynamic relation between reciprocal temperature and the derivative of the entropy w.r.t energy.
Now how well this definition corresponds with the 'level of hotness' we physically perceive, and think we measure and also think as understand as temperature, that I have not decided in my mind with certainty (I think the question may be undecidable), but there is a clear definition to hang on to without involving thermal contact.
From having skimmed over this voluminous thread, it seems that many here do not like this definition (most must be aware of it since this is a standard notion?).
I would like to know any thoughts on this anyone might have.
Incidentally, in the attachment to the post
I summarize some basic statistical mechanics in the microcanonical ensemble, all learnt from the book by Berdichevsky referred to in the paper.
I recommend the book highly to students of mechanics - Berdichevsky, being a student of Sedov's and having degrees in both solid and fluid mechanics writes like a mechanician, and after a long search I finally found a book where the fundamentals are laid out clearly - no philosophy. He also makes the connection between statistical mechanics in the microcanonical and canonical distributions in the limit of large N and there are nice connections with when fluctuations become important, a fact that can be captured by working in the microcanonical setting.
- Amit
Welcome to Manchester foundation year students
Some of the Manchester foundation year students will join in this discussion. Welcome!
Foundation year project title: Thermodynamics of nanoscale small systems
This project explores the thermodynamics of nanoscale small systems and its possible applications. For a system going to the scale of a few (say less than 100,000) atoms, which is possible for today's technology, one cannot even define the temperature. Is this true or not? This is a bizarre discovery: some concepts for large systems, like temperature, are meaningless in some tiny objects.
I skimmed over much of this discussion, but I would suggest you read up on the work of the pioneers in this field, e.g. Terrell Hill, Ali Mansoori, also possibly Gian Beretta's thermodynamics
textbook, and his work on single particle system quantum thermodynamics variables,
if I remember correctly. Here's a starter page:
Also authors who publish on so-called violations of the second law are all individuals who have never read Clausius' textbook and are aiming to disprove the Boltzmann version of the second law:
Re: Nanothermo: Thermodynamics of small isolated systems
An interesting paper on this subject was published by Mandelbrot in 1962. Check out
The Role of Sufficiency and of Estimation in Thermodynamics
Benoit Mandelbrot
Source: Ann. Math. Statist. Volume 33, Number 3
(1962), 1021-1038.
The purpose of this paper is to point out (and to
use) the relations of certain statistical concepts with "statistical" thermodynamics.
(A) It is observed that Gibbs's "canonical distribution"of energy is precisely what statisticians have later labeled a "distribution of the exponential type". It follows that a rigorous treatment of the canonical law can be based upon the concept of "sufficiency", which is thereby related to the physical idea of "thermal equilibrium" and to the "zero-th principle of thermodynamics". In other words, the theory of physical fluctuations can be based upon "principles" very similar to those of the "phenomenological", or "classical, non-statistical" thermodynamics. Naturally, our results will be less detailed than those of statistical mechanics. However, the foundations of the latter theory still raise a host of unanswered
problems, and it seems good in the meantime to show that the less powerful phenomenological theory has a wider scope than is commonly thought (see also [15]). The possibility of a purely phenomenological approach to statistical thermodynamics is not in itself a new idea. A procedure somewhat similar to ours has indeed been long ago suggested in Szilard's admirable, but very difficult and neglected, paper [18]--not to be confused with his [19]. Of course, Szilard used a quite different vocabulary; but, with hindsight, one may now say that he has co-invented the concept of sufficiency with R. A. Fisher; by showing that, under certain regularity conditions, Gibbs's canonical law is the only probability distribution with a single scalar sufficient statistic, Szilard also anticipated the results of G. Darmois [2], B. O. Koopman [10] and E. J. G. Pitman [16], but was partly anticipated by Poincare [17].
(B) The second thesis of the paper is independent of Szilard, and concerns the concept of temperature. For systems with a canonical
energy, the temperature is the parameter of the Gibbs distribution; as such it is undefined for isolated systems with a determined energy. However, it is necessary to generalize the concept of temperature to isolated systems. Several definitions have been proposed and, although they all safely converge mutually for the usual very large systems, the temperature remains athematically ambiguous for small isolated systems; it also becomes physically meaningless. We shall show that the temperature for systems-in-isolation should be viewed as a statistical estimate of the parameter of a conjectural canonical distribution, from which the presently isolated system may be presumed to have once been drawn. This interpretation explains the nature of the ambiguity of the concept of temperature; it also meets the actual practice of physicists; finally, some of the a priori conditions, which the physicists impose upon their "estimators", turn out to correspond to the statistical conditions of consistency, unbiasedness, and efficiency. Physicists also use two very interesting variants of consistency and unbiasedness, which we shall study under the names of "self-consistency" and "self-unbiasedness". The most commonly used temperature, due to Ludwig Boltzmann, turns out to be the maximum likelihood estimator. In summary, we hope to show that it is a great pity that mathematical and physical statistics should have developed largely independently of each other, while using the same concepts. By combining the rigor of modern statistics with the intuitive vigor of thermodynamics, both should be served well. However, as things stand, the mathematical statistician should not hope to unearth in the literature of physics any result as yet unknown to him. An important open problem suggested by this paper is the following. When sufficiency and estimation are defined in the most general terms, it seems that one should also be able to generalize the scope of thermodynamics. However, an approach such as that of P. R. Halmos and L. J. Savage [5] could not be applied to thermodynamics without substantial restrictions, as we shall show in Section 7. It remains to study these restrictions in greater detail, before one can assert that a non-void generalization of thermodynamics is possible. The problem is addressed to both mathematicians and physicists. We shall strive to reduce to the minimum the detailed knowledge of physics required to read this paper. If the reader's appetite for information about thermodynamics has been awakened, he could do no better than to make use of references [11] and [20].


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What's included:
- One Classic Ice Cream Hardware Kit
- One Pizza Cutter Kit
- Two 5/16" Threaded Inserts
Customer Reviews
2 Review(s)View All
Made these sets as Christmas gifts....Posted December 26, 2011
Made these sets as Christmas gifts. Had to change the threaded insert for a t-nut as we had 3 unsuccessful tries with enlarged bit/placing insert prior to turning, etc., absolutely could not get Marblewood to work. Worked on Black Walnut, Mahogany, Rosewood and Olivewood, Maple will work as well. So LOVE this hardware! Ice Cream Scoops work fabulous. Plan on making more for our local Farmer's Market. Well worth getting this set. Avid woodworker with years of experience.
The Pizza Cutter is incredible...very heavy...Posted November 28, 2011
The Pizza Cutter is incredible...very heavy duty! The specified drill size for hardwood handles is way too small and the nut insert cracked both my tiger eye maple and burled walnut handles. I finally used a 1/2" bit successfully...the threads still had plenty of grip and there was no need for epoxy.
Customer Reviews
2 Review(s)


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Judicial Officers of the Court of Chancery
The Honorable Leo E. Strine, Jr. was confirmed as Chancellor of the Court of Chancery on June 22, 2011, having previously served as a Vice Chancellor since 1998. Chancellor Strine also has long-standing positions as the Austin Wakeman Scott Lecturer in Law at the Harvard Law School, Senior Fellow at the Harvard Program of Corporate Governance, and Adjunct Professor of Law at the University of Pennsylvania and Vanderbilt University Law Schools. He also serves as the Special Judicial Consultant to the Corporate Laws Committee of the American Bar Association. Before joining the Court of Chancery, Chancellor Strine was Counsel to Governor Thomas R. Carper. Before his position with Governor Carper, Chancellor Strine served as a corporate litigator at Skadden, Arps, Slate, Meagher & Flom and as law clerk to Judge Walter K. Stapleton of the U.S. Court of Appeals for the Third Circuit and Chief Judge John F. Gerry of the U.S. District Court for the District of New Jersey.
Chancellor Strine graduated magna cum laude from the University of Pennsylvania Law School, and received his Bachelor's Degree summa cum laude from the University of Delaware. He was selected as a Harry S Truman Scholar and a Crown Fellow of the Aspen Institute.
Vice Chancellor J. Travis Laster
The Honorable J. Travis Laster was sworn in as Vice Chancellor of the Court of Chancery on October 9, 2009. Prior to his appointment, he was one of the founding partners of Abrams & Laster LLP, a corporate law boutique specializing in high stakes litigation involving Delaware corporations and other business entities, and advising on transactional matters carrying a significant risk of litigation. Before forming Abrams & Laster, he was a director in the Corporate Department of Richards, Layton & Finger P.A. Before joining Richards Layton & Finger, he clerked for the Honorable Jane R. Roth of the United States Court of Appeals for the Third Circuit.
Vice Chancellor Laster received his A.B summa cum laude from Princeton University and his J.D. and M.A. from the University of Virginia, where he served on the Virginia Law Review, was a member of the Order of the Coif, and received the Law School Alumni Association Award for Academic Excellence for having the best academic record in his graduating class. He is a member of the American Bar Association, Delaware State Bar Association, and the Rodney Inn of Court.
Vice Chancellor Sam Glasscock, III
The Honorable Sam Glasscock, III was appointed as Vice Chancellor in 2011 after having served as Master in Chancery from 1999 to 2011. He was born in Erie, Pennsylvania and spent most of his youth in Lewes, Delaware. He received a B.A. in History from the University of Delaware in 1979, a J.D. from Duke University in 1983 and a Master's Degree in Marine Policy from the University of Delaware in 1989. Before coming to the Court of Chancery, he worked as a judicial clerk, as an associate at Prickett, Jones, Elliott, Kristol & Schnee in the litigation section, as a Superior Court special discovery master and as a Deputy Attorney General in the Appeals Unit of the Department of Justice.
Abigail LeGrow became a Master in Chancery in October 2011. Before joining the Court of Chancery, she was an associate in the Corporate Group of Potter Anderson & Corroon LLP and a judicial law clerk to the Honorable Jack B. Jacobs of the Delaware Supreme Court. She graduated summa cum laude from the Penn State Dickinson School of Law, and also received her B.A. in Political Science from Susquehanna University.


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Selling our Leaders In the Rs 2000 Crore Scramble
By Santwana Bhattacharya, Piya Singh and Pratul Sharma - NEW DELHI
Published: 16th Feb 2014 07:53:03 AM
It's raining political ads and copywriters are reaping the whirlwind. All major political parties, national and regional, have recruited advertising agencies to sell them in the coming Lok Sabha polls. The size of the election publicity pie is Rs 1,000 crore, estimates Group M, an international media investment arm of the WPP group which may well escalate to Rs 2,000 crore. The Congress is spending the most, around Rs 700 crore, mostly with Dentsu India, a Japanese public relations-cum-advertising agency. The BJP's campaign revolves singularly around Narendra Modi, though party treasurer Piyush Goel maintains that the party hasn't finalised any agency. It's an indicator of the changing times that Mayawati's BSP is also hiring a professional ad agency to mount a catchy poll campaign. Three agencies have been shortlisted and the result will be out in the next few days. Ironically, the strong-woman of UP politics had famously declared that she does not need the media to do her politics. In UP, Chief Minister Akhilesh Yadav is overseeing the party's publicity campaign himself, assisted by loyal babus. He has commissioned two TV channels, ETV UP and ZEE News, to make short films about his and his father Mulayam Singh's political achievements. Sources say he's a "bit cagey about handing over the entire account to a single agency'', the way the big parties with deep pockets, Congress and BJP, do. Without political campaign spends, in this slump year, Indian advertising would have grown at around 9 per cent only and not at the current estimate of 11.6 per cent.
LOCAL TALENT LAUNCHPADS: Other political parties in the fray are using local talent and state television channels to promote their leaders, who monitor the work with eagle eyes. While the BJD has a team of five senior party leaders working on the campaign text, slogans, manifesto and audio visuals, Chief Minister Naveen Patnaik "does not let anything go out without his approval''. For audio-visuals, the party is depending on local agencies. In Tamil Nadu, AIADMK and DMK have their own TV channels to propagate their campaigns and counter-campaigns.
In an increasingly multi-cornered contest where every other leader worth a vote bank is entertaining hopes of becoming the next occupier of the prime ministerial bungalow at 7 Race Course Road, nothing can be left to chance. "Catching the maximum eyeballs is the name of the game now,'' a young ad-executive waiting outside Congress treasurer Motilal Vora's office says. His company attached to a media house deals in online ads for parties in the heartland states, especially Uttar Pradesh. But Prasoon Joshi, President South Asia of McCann feels that the "Congress was the first-mover; it was the fastest to get its campaign off the ground."
THE BIG SPENDER: The Congress has belatedly realised that Modi's meticulously planned across-the-range publicity campaign—TV screens at street corners, holograms and public engagement initiatives like chai pe charcha—has set the agenda, forcing the Congress to react. But the on-air commercials touting the UPA's achievements and positioning Rahul Gandhi as the next PM have drawn mixed reviews. Copy errors have crept into regional print ads. Tweeples, cartoonists and commentators in the capital have been sniggering at the poster of Gandhi standing in the middle centre of ten youthful faces—it is very similar to the Modi campaign. Its slogan "Main Nahin, Hum (Not I, we)," which, the BJP immediately pointed out, had been a 2011 Modi line for a "Chintan Shivir". Rohit Ohri, executive chairman of Dentsu declined to comment quoting a non-disclosure agreement. The Congress is targeting the youth through a specific campaign with 120 million new citizens eligible to vote for the first time using a time-tested marketing strategy of segmentation.
Party treasurer Motilal Vora is shelling out the big bucks. Rural Development minister Jairam Ramesh's task is to devise "the line to be followed''. The rest is being left to Dentsu India. Sonia Gandhi has strictly banned any mention of 'aam aadmi' any more in any Congress ads after its arch enemy, AAP appropriated the moniker. The 'Congress ki haath, Aam Aadmi ke saath' slogan had brought the grand old party back to power in 2004. Vora says, "We've lot of work to do and professionals are better equipped to do these kind of things now." The reason Dentsu was chosen over JWT which had done the Congress campaign in 2009, was "because the people moved from JWT to the Japanese firm", according to Vora.
UPHILL CONNECT: Senior ad executives in Mumbai who were closely involved in Congress campaign—expected to roll out in 14 languages—would speak only on the condition of anonymity. "The Congress campaign was a result of several brainstorming sessions with Rahul and the top party leadership like Digvijay Singh that moved the positioning from "Congress Ka Haath Aam Aadmi Ke Saath" to empowerment through " Har Haath Shakti, Har Haath Tarakki," (Every Hand is powerful, every Hand leads to progress)" says an ad guru, who was present at the sessions as part of a group of media representatives. Another executive confirmed that leadership right up to Rahul had vetted the campaigns before being released. Industry insiders say that the slogans would keep changing until the elections. A recent Hindi ad featuring a youth activist from Goa got mired in an online controversy; she got hate mails following her appearance in an ad titled, Kattar Soch Nahi, Yuva Josh (Not fanaticism, youthful energy) which was aimed at an image makeover for Rahul Gandhi.
If ads alone can get congress to power,let there be ads. To some extent BJP's is localized , appealing to the people . All others are copying . Is there one party that can come up with truth that we have failed in the service of the people . With what face congress thinks it can win with all the scams name it it is there, tagged to them . BJP's in season and out of season blame throwing on AAP reveals its nervousness . The imposition of president's rule on Delhi is another way to prevent AAP to form Govt. as they will come back with higher nos , even crossing the 50% . It is political chickanery played by Congress and BJP. Inspite of this , congress and BJP will be wiped out in Delhi. Rahul's electioneering thru ads which is followed by SP and BSP is going to fall on deaf years . The only campaign that will be effective is Modi's
Posted by N.S.Srinivasan at 02/16/2014 09:19 Reply to this Report abuse
Good comment
Posted by KoodaMooda at 02/16/2014 11:19 Reply to this Report abuse
The bigger question is whether these advertisements make any impact on public? Personally, it never influenced me except the professionalism of the creator...
Posted by Muhammed Rafeeque at 02/16/2014 10:33 Reply to this Report abuse
They looted the country for the last 10 years perpetrating one mega scam after another. Now he wants to eradicate corruption. Corruption is in the flesh and blood of every Congressi. Even God cannot eradicate Corruption from the Congressis as it is so ingrained in their character. First let them bring back the looted money deposited in foreign banks, wherever it may be, then talk about eradication of corruption. Sorry, you cannot fool us any more.
Posted by KSV SUBRAMANIAN at 02/16/2014 12:06 Reply to this Report abuse
We will empower the poor, we will empower women , we will empower agriculturists - all this after 2014 polls. then there will be no corruption in India. First give us your votes to serve you": well
Posted by P.S.Arunachalam at 02/16/2014 12:28 Reply to this Report abuse
Narendra Modi should be whipped and hanged for giving a bouquet of roses to an American diplomat in exchange for a strip search and cavity search of an Indian diplomat. You do not shake hands with any representative of a country whose population will be made to eat one another till no one remains alive. NuclearSupremacyForIndiaOverUSDOTblogspotDOTcom
Posted by SatishChandra at 02/16/2014 19:30 Reply to this Report abuse


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1996 Israel My Jerusalem Silver Medal ASW 2.0
We provide all our customers with a refund, return and/or exchange policy on everything we sell including all bullion and certified coins. If for any reason you have a problem, please feel free to call our offices. We will always do our best to accommodate you.
|Bid: $19.51
|Ask: $19.61
Volume Pricing
Quantity Notification
Product Description
The obverse of this Silver Medal depicts many of the sites in Jerusalem including the Broad Wall from the First Temple Period, the Burnt House (Katres House) and the Western Wall. The reverse shows a lion, which is the symbol of the city, surrounded by the word Jerusalem in twenty different languages. The word Jerusalem in Hebrew means "City of Peace".
The medal is made of .999-fine Silver and weighs 2 oz. This beautiful medal comes in the original box with the certificate of authenticity from the Holy Land Mint.
Learn why you should buy Silver, and learn how to buy Silver as an investment. Get started today! Call our Account Managers toll-free or chat with us live online. APMEX is where to buy Silver!
APMEX stands behind every product it sells with a satisfaction guarantee.
Product Specifications
|Product ID:
|50 mm


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Denver >Lodging > Renaissance Denver
3801 Quebec Street, Denver, CO | Directions 8020739.770032 -104.904360
Daily 24 Hours
Neighborhoods: Northeast Denver
I normally donâÂ?Â?t write reviews, but I – I normally donâ??t write reviews, but I felt that I had to for this hotel, especially since I wish I had known what I know now after staying here. After checking in, I had a decent dinner and slept ok, but then I was woken up early in the morning by about 10 or 15 people that started yelling through bullhorns on the sidewalk outside of the hotel. At first I thought it was some kind of rally or a union thing, but then realized that there is some kind of clinic for women next door. They were yelling all sorts of mean and nasty things at anyone coming in to the parking area of the building. I tried to sit on the balcony and enjoy a cup of coffee and the nice warm sunrise, but I could not stand the constant shouting and what appeared to be harsh bullying of everyone that came down the street. It was terrible to listen to and watch.
I even tried to block out the noise with music on my ipod and headphones, but I could still hear them. I called the front desk and they were not very helpful, but offered to move me to a room that faced the busy street instead of the mountain view, which I did not want. The big story at breakfast amongst all of my colleagues was how everyone was awoken by the annoying continuous shouting of the people outside and that they ruined the beauty of the hotel and view, so I wasnâ??t the only one. This bullhorn noise and yelling woke me up every day of my visit. A couple of my colleagues who went for walk around the block after breakfast came back and said it was like a freak show and many of them had nasty signs with bloody images, Jesus and sin and even bloody baby dolls hanging from trees up and down the street. Many of my coworkers had also complained to the hotel but no one at the hotel cared to do anything about it, although one of the front desk people did say they would call the local police. Another hotel employee told us that the people that were out there yelling were anti-birth control and anti-abortion protesters and they are out there almost every day of the month, have been there for years and that everyone complained about them, but that the city or county didnâ??t seem to want to do anything. It didnâ??t really seem like anyone, even the manager of the hotel, even cared. Two local Denver sheriff/police cars and an SUV showed up on at least two separate occasions, but they did not do anything about the protesters or noise, just chatted with some security guards in the parking lot for a while and then left.
I was looking forward to staying the weekend to check out things to do in the Denver area, but even MORE of these loud people were out there just after 7:00 am on SATURDAY, and one of them was even blowing loud noises through a trumpet! That was it for me! I took a shower, packed up and left to go to another hotel, since my flight wasnâ??t until Monday. The hotel never apologized or anything to any of us.
My company routinely books all of us at Renaissance hotels, but after we returned to work and told the rest of the office and our corporate travel agent about our experience, they all agreed this would be our last stay at this hotel brand. At least the travel agent apologized and gave us some credit back.
If you are looking for a place to stay with a nice view of the Denver mountains, find someplace else because they obviously donâ??t do anything about the constant daily yelling and screaming outside at this hotel or this part of the city.
Good night's sleep...ya right. – Very beautiful inside, clean as well. Fire alarm went off at 4 AM! Found out this happens frequently, no fire. 12 flights of stairs in a huge crowd. Finally back to bed 2 hours later, awakened to their Maid knocking at 9 AM wondering if we would be leaving soon??? Unbelievable, they would not even give us a free nights stay or a discount. Sits in the industrial part of the city, with trains near as well. Will we be staying here again? I think not!
Stunning hotel remodel-think Luxor in Vegas ! Beautiful hotel, friendly staff, pool, loved the new gym. – Impressed! The hotel was completly remodeled for the DNC 8/08 a staff member told me. Wonderful decor, lobby is stunning,Starbucks coffee bar, new beds/linens were luxurious! Our room was quiet & relaxing. Will have to agree with previous review that the hotel reminded me of the LUXOR in Vegas.Staff was kind, friendly, and very helpful. Loved the new gym! Manager sent a fun little basket after I mentioned my husbands birthday. Nice little extra touch. Will return next trip into Denver.
Do not stay here – This hotel is very old and located among a train shipyard. If you are looking to be woken up by the whistling of the train signals in the middle of the night then I recommend staying elsewhere. Valet service is horrible and the staff not so friendly either.
The rooms were so dirty that I checked into a different hotel just after one night.
An executive-friendly hotel with all the amenities for the business traveler. – The Scene
This 400-room hotel is a popular conference venue for both out-of-town business travelers and locals. Twenty-four meeting rooms are the main draw. A soaring, 12-story, plant-filled atrium adds architectural interest to this otherwise conventional property.
The Details
Each of the comfortable rooms is equipped with all the basics. In addition, they have work desks with good task lamps and phones with voicemail and data ports. Club level guests enjoy complimentary continental breakfast and hot afternoon snacks. Freebies include newspapers delivered Monday through Friday and a shuttle to downtown (6 miles) and the Denver International Airport (17 miles). Two on-site restaurants, The Brasserie and The Lounge, are open for breakfast, lunch and dinner. Laundry and dry-cleaning valet, as well as self-service laundry, are available.
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Looking for used extractor under $200
Looking for used extractor under $200
how many frames to extract at once do you need? Pigeon Mountain Trading has some that are even less than that (and new) if you only need 2 frames at a time.
I have a two frame galvanized. $150+ you pay shipping. Roch NY
Rmns 1:16/Prv.3:5,6/ Beegan BK May 09/ Zone 5b
I have NOT failed. I have only found many many ways that do not work!


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The third-ranked (Class A) Minneota volleyball team won two matches Saturday at the Apple Valley October Classic to finish in ninth place out of 16 teams at the two-day event.
The Vikings opened the day with a 25-21, 25-22 win over Cambridge-Isanti. Taylor Reiss had 10 kills, seven digs and an ace block in the match. Megan Larson added 22 set assists and nine digs.
In its final match of the tournament, Minneota easy handled Edina 25-18, 25-15. Reiss again led the attack with 12 kills. She also had three ace serves.
Payton Boerboom and Molly Hennen each had eight digs in the match, and Larson again had 22 set assists.
The Vikings play tonight in the Camden Conference championship match against Dawson-Boyd in Dawson.
Cambridge-Isanti13 22
Minneota25 25
Serving (good-att-aces): Shelby Corbin 9-9-0, Analisa Buysse 7-7-0, Faith Laleman 8-8-0.
Kills: Taylor Reiss 10, Molly Hennen 8, Corbin 4.
Digs: Megan Larson 9, Reiss 7, Laleman 6.
Set Assists: Larson 22.
Blocks: Hanna Prellwitz, Larson, Reiss.
Edina18 15
Minneota25 25
Serving (good-att-aces): Laleman 14-14-2, Reiss 11-12-3.
Kills: Reiss 12, Hennen 7, Prellwitz 5, Corbin 3.
Digs: Payton Boerboom 8, Hennen 8, Larson 7, Corbin 6.
Set Assists: Larson 22.
Blocks: Prellwitz 2, Hennen, Reiss.


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Accelerating Sales: Driving Traffic
In the preface that I published last week, I talked about the fact that you and your sales team need to be very clear regarding the results that are produced by your products and services when a customer contracts with you. If you don't understand the quantity of results (as measured by the client) and the value of results (again, from the customer's point of view), then you are doomed to pitching your features and prices. Obviously, this is an unprofitable way to go to market.
The Preface To Accelerating Sales
Welcome to my nine-week sales acceleration program. During the next nine weeks, this newsletter will publish one chapter from a book that I am developing. Our overarching purpose in writing this book is to help the 21st-century sales professional understand that the rules of the road have clearly changed and that our old strategies and tactics don't work.
8 Mobile Computer Must-Haves Your Customers Can't Do Without
You knew this day would come. Your customers' need for greater mobility and advanced applications has moved from a nice to have to a critical business requirement. Their legacy systems can't keep up with rapidly evolving customer, technology and business demands. Inefficiencies are costing them time and money. From the front office to the distribution center and all points in between, mobile technology creates the foundation on which successful, profitable businesses are now built. And the time to invest is now.
6 Reasons Tablet POS Systems Are Here To Stay
Retailers often spend significant time determining the layout, décor, and other aesthetic aspects of their shops. They rightly focus on ensuring a consistent brand experience exists for customers throughout the store. Yet businesses that have wanted their countertop devices to fit in with their brand image often have limited options.
Help Your Brick-And-Mortar Retail Customers Make Mobile Work For Them
It's no secret that mobile technology has changed our lives. We are now able to be in contact with anyone and access the tiniest minutia of information from nearly anywhere in the world using our increasingly sophisticated smartphones and tablets. And increasingly, these mobile capabilities are also transforming another aspect of modern life: how consumers shop.
How To Focus IP Video Surveillance On The Needs Of Education, Courts
Features and functions of video surveillance systems vary, depending on the application. Below is information on K-12 education, university and higher education, and courthouse and remote arraignment applications.
3 Ways Hospitals Can Help Ensure HIPAA Compliance
The Health Information Portability and Accountability Act (HIPAA) is 13 years old. During that time, the acronym, HIPAA, has become synonymous with patient privacy. Every patient receives the doctor or hospital's privacy policy during an initial visit and terms like protected health information (PHI) have become part of the everyday healthcare vernacular.
IP Cameras 101: Megapixels Don't Matter — Image Usability Does
The physical security practitioner has a myriad of electronic devices at their disposal to detect, deter, and deny adversaries from harming people or property. Video surveillance is one such countermeasure used for deterrence and, more importantly, as an assessment tool to verify the events of a given scene and situation. The quality of that video could mean the difference between identifying a suspect or not.
The Value Of A Payment Gateway
There's no way around it. No matter what size your business is or what industry you work in, if you accept credit cards, keeping up with the latest requirements is difficult at best. Credit card security has become an even greater challenge for merchants with the advent of the Payment Card Industry Data Security Standard put forth by The PCI Security Standards Council.
Bar & Grill Streamlines Operations And Provides Excellent Support With New POS Solution
Harbortouch has helped this popular restaurant streamline operations while providing excellent support along the way.