text:
A microfluidic embedded nanoelectromechanical system (NEMs) force sensor provides an electrical readout. The force sensor contains a deformable member that is integrated with a strain sensor. The strain sensor converts a deformation of the deformable member into an electrical signal. A microfluidic channel encapsulates the force sensor, controls a fluidic environment around the force sensor, and improves the read out. In addition, a microfluidic embedded vacuum insulated biocalorimeter is provided. A calorimeter chamber contains a parylene membrane. Both sides of the chamber are under vacuum during measurement of a sample. A microfluidic cannel (built from parylene) is used to deliver a sample to the chamber. A thermopile, used as a thermometer is located between two layers of parylene.
1. A microfluidic embedded nanoelectromechanical system (NEMs) force sensor comprising:
(a) a force sensor comprising a deformable member that is integrated with a strain sensor, wherein:
(i) the strain sensor converts a deformation of the deformable member into an electrical signal;
(ii) the deformable member comprises a doubly clamped beam;
(iii) the strain sensor comprises a piezo resistive strain sensor that is patterned asymmetrically in a horizontal plane of the doubly clamped beam so as to couple to regions of tensile or compressive strain; and
(iv) the piezo resistive strain sensor is used for measuring in-plane forces; and
(b) a microfluidic channel that encapsulates the force sensor, wherein the microfluidic channel controls a fluidic environment around the force sensor and improves an electrical read out of the electrical signal from the force sensor.
2. The force sensor of
3. The force sensor of
4. The force sensor of
5. The force sensor of
6. A microfluidic embedded nanoelectromechanical system (NEMs) force sensor comprising:
(a) a force sensor comprising a deformable member that is integrated with a strain sensor, wherein:
(i) the strain sensor converts a deformation of the deformable member into an electrical signal;
(ii) the force sensor comprises the deformable member and a transducer used for reading out the electrical signal;
(iii) the deformable member comprises a doubly-clamped beam made from two polymer layers;
(iv) the transducer comprises a metal wire sandwiched between the two polymer layers;
(v) the force sensor is fabricated on a silicon-nitride coated silicon wafer and suspended over an opening etched in the wafer;
(vi) the opening comprises part of the microfluidic channel that surrounds the force sensor; and
(vii) the force sensor is suspended from the wafer's surface over a hole etched through the wafer's backside; and
(b) a microfluidic channel that encapsulates the force sensor, wherein the microfluidic channel controls a fluidic environment around the force sensor and improves an electrical read out of the electrical signal from the force sensor.
7. The force sensor of
the strain sensor comprises a piezo resistive strain sensor that is patterned asymmetrically through the doubly clamped beam so as to couple to regions of tensile or compressive strain.
8. The force sensor of
the piezo resistive strain sensor is patterned asymmetrically in a horizontal plane of the doubly clamped beam; and
the piezo resistive strain sensor is used for measuring in-plane forces.
9. The force sensor of
the strain sensor comprises a piezo resistive strain sensor that is patterned symmetrically through the doubly clamped beam using a straight line pattern to measure out-of-plane forces.
10. The force sensor of
11. The force sensor of
12. The force sensor of
13. A method for fabricating a microfluidic embedded nanoelectromechanical system (NEMS) force sensor, comprising:
depositing a first polymer layer onto a silicon-nitride layer coating a silicon wafer;
depositing a metal wire that comprises a piezo-resistive element of a strain sensor on the first polymer layer;
depositing a second polymer layer on the metal wire and the first polymer layer;
etching a hole through the wafer's backside;
defining the NEMS force sensor by creating a polymer structure, from the first polymer layer and second polymer layer, that encapsulates the metal wire, and that is suspended over the hole, by removing the silicon-nitride layer from a portion of the wafer, without damaging the first polymer layer and the second polymer layer.
14. The method of
15. The method of
16. The method of
17. The method of
18. The method of
This application claims the benefit under 35 U.S.C. Section 119(e) of the following co-pending and commonly-assigned U.S. provisional patent application(s), which is/are incorporated by reference herein:
Provisional Application Ser. No. 60/834,253, filed on Jul. 28, 2006, by Michael L. Roukes, Chung-Wah Fon, Wonhee Lee, and Hongxing Tang, entitled "Vacuum-insulating polymer-based micro-biocalorimeter integrated with microfluidics";
Provisional Application Ser. No. 60/834,052, filed on Jul. 28, 2006, by Blake W. Axelrod, Michael L. Roukes, and John Tan, entitled "Plastic NEMs for cell physiology"; and
Provisional Application Ser. No. 60/834,288, filed on Jul. 28, 2006, by Blake W. Axelrod, Michael L. Roukes, and John Tan, entitled "Microfabricated cell positioning system";
The invention was made with Government support under Grant No. N66001-02-1-8914 awarded by NAVY-SPAWAR Systems Center San Diego, and Grant No. W911NF-04-1-0171 awarded by ARO-US Army Robert Morris Acquisition Center. The Government has certain rights in this invention.
1. Field of the Invention
The present invention relates generally to nanoscale electromechanical (NEMs) devices, and in particular, to a method, apparatus, and device for a micro-fluidic embedded polymer NEMs force sensor and vacuum insulated polymer based micro-biocalorimeter integrated with microfluidics.
2. Description of the Related Art
(Note: This application references a number of different publications as indicated throughout the specification by reference numbers enclosed in brackets, e.g., [x]. A list of these different publications ordered according to these reference numbers can be found below in the section entitled "References." Each of these publications is incorporated by reference herein.)
The development of microcantilever force sensors has enabled development in the field of atomic force microscopy (AFM). AFMs are important tools in nanoscience and have further led to the development of cantilever based sensing, including a wide range of scanning probe microscopies (SPM), and many different forms of static (that is non-scanned) sensing. SPMs are used to image local forces arising from magnetic and magnetic resonance interactions; forces from local electrostatics, surface potentials, surface temperatures, and chemical bonding; and forces from many other local origins. Similarly, applications for non-scanned microcantilever sensors are equally diverse, including infrared imaging, nanocalorimetry, vapor- and liquid-phase chemisensing, electrometry, mass detection, etc.
However, at microscale dimensions, there are limits with respect to the level of frequency achievable and the level of sensitivity attainable. In this regard, the standard approaches used to make microelectromechanical systems (MEMS) cannot provide access to the nanoscale, where very large improvements in sensitivity can be attained [1]. Recent demonstrations and applications of the unprecedented sensitivity available from nanoelectromechanical (NEMS) devices include milestones such as sub-single-charge electrometry[2], single-electron-spin paramagnetic resonance [3], zeptogram-scale mass sensing [4], zeptonewton-scale force sensing [5] and subfemtometre displacement sensing [6]. In fact, with these continuing advances, NEMS sensors are rapidly converging towards the ultimate, quantum limits of force and displacement detection [7].
However, in contrast to MEMS, NEMS devices are still largely pursued only within the province of specialists. A current barrier to their practical development and widespread use is the difficulty of achieving sensitive displacement transduction at the nanoscale. Beyond the initial challenges of fabricating ultra-small mechanical devices, successful realization of NEMS involves addressing the doubly hard challenge of realizing very high frequency displacement sensing while attaining extreme subnanometre resolution. This is not straightforward; approaches to displacement transduction commonly used for MEMS generally are not applicable to NEMS [8]. For example, the efficiency of capacitive detection precipitously decreases at the nanoscale, and the signal is typically overwhelmed by uncontrollable parasitic effects.
Existing prior art techniques used to measure forces exerted by biological structures have been primarily limited to optical measurements. For optical readouts, diffraction effects become pronounced when device dimensions are scaled far below the wavelength of the illumination used. Furthermore, existing readouts for scanned probe microscopy cantilevers are predominantly based upon external (that is, off-chip) displacement sensing systems that, typically, greatly exceed the size scale of the cantilever sensors themselves. The most common SPM readouts are optically based, involving simple optical beam deflection or more sensitive interferometry. By comparison, only a relatively small subset of efforts has focused upon development of self-sensing nanocantilevers.
In addition to the above, the ability to measure forces exerted by biological specimens have encountered significant limitations. In this regard, prior art techniques have focused on optical measurement techniques. In such an environment, the amount of resolution attainable is limited. Further, prior art techniques fail to provide an efficient mechanism to deliver individual cells to specific force sensors and fail to precisely control the chemical environment around a cell under study. In addition, prior art delivery and control systems fail to maintain the viability of the biological sample under study while providing a mechanism to extract signals from a force sensor to a computer for readout and analysis.
In view of the above, what is needed is a NEMs force sensor for use in biological applications that can be used in an efficient and controlled environment.
In addition to the above, calorimeters are used in the prior art to detect enthalpy change of chemical and biological reactions. However, measurement sensitivity of microfabricated calorimeters/thermometers fail to achieve the measurement sensitivity compatible to that of large scale calorimeters. Such a lack of measurement sensitivity is determined by the sensitivity of the thermometer and capability to maximize the signal with good thermal isolation. However, the prior art has failed to increase sensitivity to minimize the heat loss of the sample. Accordingly, what is needed is a microcalorimeter that is useful in biological applications and that provides sufficient measurement sensitivity.
One or more embodiments of the invention encompasses a force sensing nanoscale electromechanical (NEMs) device for biological applications, such as the contraction of a cell's lamellipodia. The force sensor is a doubly clamped beam fabricated from a polymer, such as SU-8, with a piezoresistive strain sensor patterned asymmetrically through the beam so as to integrate over the regions of maximum tensile strain. The piezoresistive strain sensor is made from a conductor, such as a metal like gold. The force sensor can be positioned next to a ledge or suspended bridge for supporting a single cell and performing force measurements on cell contraction. If the entire device is mounted on a flexible substrate the force-sensing beam can also be used to exert force back on a cell by flexing the substrate parallel to the beam. Furthermore, the stiffness of the force sensor can be tuned by flexing the substrate perpendicular to the beam.
In addition, one or more embodiments of the invention provide calorimeter capable of detection of enthalpy change of chemical and biological reaction, such as enzyme activity and protein-ligand binding, in a 3.5 nanoliter (nL) volume. The calorimeter is embedded in parylene microfluidic system and can be coupled to other lab-on-a-chip microfluidic devices. Microfabrication of the calorimeter array and the accompanying microfluidic circuitry has enabled rapid and parallel implementation of calorimetric measurement. The reduction in scale also reduces the time and sample quantity required for such measurement. Sophisticated thermal insulation is engineered to maximize the measurement sensitivity. While a batch calorimeter is demonstrated, the calorimeter can be modified to perform isothermal titration, differential scanning and flow calorimetry.
Referring now to the drawings in which like reference numbers represent corresponding parts throughout:
In the following description, reference is made to the accompanying drawings which form a part hereof, and which is shown, by way of illustration, several embodiments of the present invention. It is understood that other embodiments may be utilized and structural changes may be made without departing from the scope of the present invention.
Overview—Microfluidic Embedded Polymer NEMs Force Sensor
As described above, prior art techniques have attempted to measure the forces exerted by biological samples (e.g., single cells). In this regard, adherence cells (i.e., cells that adhere or have adhering properties with respect to adjacent surfaces), may exert forces when diffused across a surface. Prior art mechanisms attempted to measure such forces primarily utilizing optical means. In this regard, prior art mechanisms were based on optical measurements of deflected substrates or members. For example, cells (e.g., monocyte or macrophage cells), may be placed superior to polydimethylsiloxane (PDMS) (e.g., PDMS pillars/structures) and any resulting deformation in the PDMS structure was optically measured. However, the resolution of such measurements was insufficient. In this regard, prior art mechanisms were insufficient for measuring the displacement/deformation of single cell structures. Further, such optical measurement techniques are expensive and cell delivery and control is difficult.
To overcome the disadvantages of the prior art, one or more embodiments of the invention utilize a microfluidic embedded polymer NEMs force sensor. To more easily understand the invention, a description of the overview of the force sensor and microfluidics are followed with independent descriptions of the force sensor and the microfluidic aspects of the invention.
One or more embodiments of the invention provide a force sensor for biological applications, e.g. measuring forces exerted by a single cell. The force sensor may consist of a doubly clamped beam fabricated from a polymer (e.g., plastic) with a piezo resistive strain sensor patterned asymmetrically through the beam so as to couple to regions of maximum tensile or compressive strain. Beams can be fabricated using the following polymers: SU Polymer family (e.g., SU8 2000, SU-8 3000, etc.) Polylmide, Parylene. The piezo resistive strain sensor can be made from any conductive material (e.g., a metal such as gold with a very thin titanium or chromium adhesion layer).
Beams can been fabricated for measuring in-plane forces by patterning the piezo-resistive strain sensor 102 asymmetrically in the horizontal plane using a c-shape and symmetrically out of the plane by sandwiching the strain sensor 102 between two layers of polymer (e.g., plastic) of the same thickness.
Beams have also been fabricated for measuring to out-of-plane forces by patterning the piezo-resistive strain sensor 102 symmetrically in the horizontal plane using a straight line pattern and asymmetrically out of the plane by placing the strain sensor 102 on top of or on the bottom of the polymer/plastic layers or by sandwiching the strain sensor 102 between two layers of polymer/plastic of different thickness.
For applications in fluid, particularly buffered solutions used in biological applications, it is advantageous to sandwich the strain sensor 102 between two layers of polymer (e.g., plastic) in order to electrically isolate the strain sensor 102 from the fluid. Such isolation insulates the force/strain sensor 102 and isolates the sensor 102 from any conductivity present in the buffered solution/fluid.
The force sensors can be encapsulated in PDMS (poly-dimethylsiloxane) microfluidics for use in fluid. Multi-layer microfluidics with control valves may be mounted on the front side of the chip with the force sensor. A glass cover slip can also be mounted on the backside of the chip and sealed with a thin layer of PDMS. The glass cover slip enables high resolution microscopy simultaneously with use of the force sensor.
Polymer NEMs Force Sensor
Described below is a detailed description of the force sensor used in accordance with embodiments of the invention.
Various symbols may be used in the description that follows. The following presents a list of such symbols and their intended meaning.
α—material dependent hooge parameter
E—Young's modulus
ζ—thickness of piezoresistive wire
G—tension force
I—moment of intertia
K—spring constant
kB—Boltzmann's constant
κ—transducer responsivity
l—substrate length
L—length of beam
λ—filter setting
N—number of carriers
n—carrier density
πl—longitudinal piezoresistance coefficient
δR—change in resistance
r(x)—radius of curvature
{right arrow over (r)}—Cartesian vector
{right arrow over (ρ)}—Cartesian vector
STh—thermal noise voltage spectral density
SH—hooge noise voltage spectral density
σ0—surface stress distribution
T—substrate thickness
t—thickness of beam
τ—time constant
V0—input voltage
δV—voltage signal
υ—poison ratio, width of piezoresistive wire
w—width of beam
ΔX(r)—displacement of surface at r in x direction
ΔY(x)—displacement of centerline of beam in y direction
δz—vertical displacement
I. Device: Clamped Beam with Piezoresistive Strain Gauge
a. Beam Displacement and Spring Constant
The displacement of the center line of a doubly clamped beam due to a force exerted at the beam's mid point is given by:
The effective spring constant, K, is defined by the displacement at the midpoint, x=L/2:
b. Strain in Piezoresistor
A strain gauge is integrated into the beam by patterning a u-shaped piezoresistive (PZR) conductor of width υ and thickness ζ symmetrically across the four quarters of the beam, shown
c. Wheatstone Bridge and Transducer Responsivity
The strain gauge will use the piezoresistance effect to convert the induced strain, eq (6), into a change in resistance:
The force sensing beam may be integrated into an on chip Wheatstone bridge with one suspended reference beam and two supported balance resistors. When optimally balanced the Wheatstone bridge converts a change in resistance into a voltage signal according to:
d. Electrical Noise
There will be four electrical contributions to the noise: amplifier voltage noise en, amplifier current noise in, Johnson noise, and 1/f noise. The voltage spectral density of Johnson noise is frequency independent:
The force noise is determined by combing equations (9) and (13):
The bandwidth, fmin and fmax, is determined by the lock-in amplifier used, in particular the source frequency f, the time constant τ, and the low pass filter roll-off. For the following I assume a SRS 830 lock-in with source frequency of 100 kHz, a minimum time-constant of 10 μs and low pass filter settings of 6 db/oct, 12 db/oct, 18 db/oct or 24 db/oct. The time resolution δ will be determined by the time constant and low pass filter settings, Table 2 summarizes the relationship between these three variables.
For a given filter setting, λ, and source frequency, f, one can determine the force noise and thus force resolution as a function of the time resolution):
One may apply the noise analysis embodied in eq. (15) and table (2) with the appropriate optimized bandwidth and filter settings for an SRS 560 pre-amp and SRS 830 lock-in amplifier to the 36 different combinations of materials, beam dimensions and PZR strain gauge dimensions listed in table (3).
The principle piece missing from this analysis is an optimization of the input voltage applied to the Wheatstone bridge. Fluidic noise, which will be discussed in the following section is also missing from this analysis, but is expected to be negligible. The estimated force resolution for the Su8 beams is plotted in
The results of this noise analysis indicate that beams #20 & 21, made of Su8 with length 100 μm, width 1 μm, thickness 400 nm, PZR thickness 50 nm and PZR widths 200 nm and 100 nm respectively, yield the best force and time resolution: 120 pN at 10 μs, 20 pN at 100 μs and 6.5 pN at 1 ms. The best silicon beams, by comparison, are #34 & 35 which offer force resolution of 2 nN at 10 μs, 280 pN at 100 μs and 80 pN at 1 ms; roughly a factor of 15 worse than the best Su8 beams.
The dynamic range of this measurement can be determined by the onset of non-linearity within the beam.
e. Demonstration of Strain Sensor
Polymer (e.g., plastic) strain sensors (as described above) have been successfully fabricated with a length of 100 microns, a width of 4 microns, a thickness of 530 nm and with a gold piezoresistive strain gauge that is 500 nm wide and 40 nm thick.
The device of
f. Force Application by Device
The plastic, SU-8, beams may be attached to a flexible substrate and then by bending the substrate it is possible to either change the distance between the beam and the ledge or to apply a tension to the beam, depending on whether the bending axis is parallel or perpendicular to the beam.
Application of equation (3) to the geometry in
The derivation of equation (24) is shown in
By combining equations (23) and (24) one obtains the displacement in terms of the vertical displacement, δz, which is the relevant experimental variable:
This result differs from a similar derivation by Ruitenbeek et. al [P23] by a factor of 2 in which the neutral surface is assumed to be at the bottom surface of the flexible substrate.
In the experimental setup described herein, the vertical displacement may be controlled by a piezoelectric stage such as a long-travel piezo flexure stage (e.g., part number P-290 available from Physik Instrumente (PI) GmbH & Co. KG) which has a maximum travel of 1000 μm and an open-loop displacement resolution of 20 nm. The displacement resolution is limited by the voltage noise of the amplifier used to drive the piezoelectric stage. Potential substrates include number 1 cover glass (T=250 μm) or stiff plastic (T=1000 μm)—cover glass will enable high resolution microscopy, whereas the plastic will enable greater force application. A substrate width, l, of 2 cm is necessary to enable electronic and fluidic integration/fanout.
The force exerted on the cell by displacing the beam as described above will depend on the spring constant of the beam, given by equation (2), and Hook's law:
g. Device Stiffening: Tuning the Spring Constant
The previous section detailed how bending of the substrate can be used to move the beam with respect to the ledge and thus exert a force on the cell under study. The same principle can be used to apply a tension to the beam that will increase the beam's effective spring constant by bending the substrate around an axis perpendicular to the beam. Replacing the beam to ledge distance, x, in equation (25) with the length of the beam, L, one obtains an expression for the change in length of the beam as a function of the vertical extension, δz:
The tension induced from this extension of the beam is:
The displacement of the center line of a doubly clamped beam under tension force, G, due to a force, F, exerted at the beam's mid point is given by:
Similar to the analysis in section (a) of the beam without tension, one can define the effective spring constant, K, by the displacement at the midpoint, x=L/2:
Equation (30) may be simplified with the observation that wl3<<3 L l2√(Tδz):
II. Device Fabrication
Prior art techniques describe optically patterning SU-8 cantilevers and metal wires to use as piezo-resistive strain sensors (e.g., deformable members), made from polymers, with transducers for converting deformation into an electrical signal. Additionally, the prior art describes a sacrificial chrome release layer and SU-8 plastic chip that were used in early versions of plastic NEMS, but not in more recent versions (see Thaysen [P2]). However, the prior art cantilevers are intended for use in Atomic Force Microscopes (AFM) and are not embedded in microfluidics. In addition, the prior art utilizes a polymer layer as a "handle" or substrate.
In view of the above, prior art techniques for force measurements were primarily obtained based on optical measurements of deflected substrates or members. Further, prior art techniques do not utilize microfluidics. For example, some prior art techniques utilize soft substrates embedded with fluorescent beads, optical detection of deformation of substrate by cell, an optical readout, heavy computation requirements to extract probabilistic force maps, limited force resolution due to optical readout, limited time resolution due to optical readout & substrate stiffness, and very limited throughput due to computation requirements (see Lo [P18]).
Further, Tan [P19] describes soft posts marked with fluorescent dye, optical detection of deformation of posts by cell, optical readout, limited force resolution due to optical readout, and limited time resolution due to optical readout & substrate stiffness.
One or more embodiments of the present invention overcome the disadvantages of the prior art. In this regard, embodiments of the present invention utilize electrical detection of the deformation, electrical readout, and micro-fluidics. Further, embodiments may utilize stand alone chips as force sensors, may embed force sensors in the micro-fluidics and utilize the force sensors for/in biological applications. In addition, while early designs of the invention may have used an all polymer method, embodiments of the present invention may build polymer force sensors on top of a silicon wafer with openings through the wafer to suspend the force sensors. Also, MPTS adhesion promoters may be utilized. Further, embodiments may use a hot, dilute hydrofluoric acid to selectively etch silicon-nitride in the presence of the polymer force sensors. Such differences between embodiments of the present invention and the prior art may be better understood with a detailed explanation of the fabrication techniques that may be utilized.
The force sensors can be fabricated using an all SU-8 process that produces a finished chip which is all plastic and thus flexible. The fabrication steps for this process are as follows:
1. Deposition of a sacrificial chrome layer onto a silicon wafer. Typically a Ti/Au layer is included below the chrome to aid in the removal of the chrome.
2. Deposition of the first polymer layer for the force sensor. The polymer can be any polymer in the SU-8 polymer family (e.g., SU-8 2000 or SU-8 3000). The polymer layer can be patterned using a direct write of ebeam lithography or photolithography—typically a combination of both is used. Or the layer can remain unpatterned until later—see step 6.
3. Deposition of the metal wire that makes up the piezo-resistive element of the strain sensor. The wire is patterned in PMMA (polymethyl methacrylate) using electron-beam lithography and deposited using electron-beam or thermal evaporation and lift-off in solvent—acetone, tricholorethylene. Typically gold is used as the metal with a thin titanium or chromium adhesion layer. A spin-on organic titanate (AP300) is used to aid adhesion to the polymer layer.
4. Deposition of the second polymer layer for the force sensor. SU-8 2000 or SU-8 3000. The polymer layer can be patterned using a direct write of ebeam lithography or photolithography—typically a combination of both is used. Or the layer can remain unpatterned.
5. Optional patterning and deposition of a metal layer for controlling cell adhesion to the force sensor by creating differences in hydrophobicity between this metal layer and the surrounding polymer or by utilizing surface chemistry differences between the metal layer and surrounding polymer. Patterned in PMMA using electron-beam lithography and deposited using electron-beam or thermal evaporation and lift-off in solvent—acetone, tricholorethylene. Typically gold is used as the metal with a thin titanium or chromium adhesion layer. A spin-on organic titanate (AP300) is used to aid adhesion to the polymer layer.
6. Optional patterning of the polymer layers if they were not directly patterned using lithography in steps 2 & 4. The polymer layers are patterned using an oxygen based plasma etch with a mask to protect the regions which are to remain as structural elements on the force sensor. Typically a metal such as chrome or titanium is used as the etch mask and patterned using electron-beam lithography in PMMA. Electron-beam sensitive polymers such as PMMA and UVN-30 have also been used as etch masks.
7. Patterning and deposition of metal layer for fan-out. A thick metal layer, typically gold with a thin titanium or chrome adhesion layer, is patterned using a bi-layer resist, photolithography and lift-off. Typically 500-1000 nm of metal is necessary to protect wires from breaking when chip flexes.
8. Deposition and patterning of thick polymer layer that will make up the structural support layer of the final chip. Typically 60-80 microns thick SU-8 2000 or SU-8 3000. Vias are patterned with photolithography so that the force sensors will be suspended over openings in the thick polymer layer. It is important that this layer have very low internal stress, low baking temperatures and long baking times are used to achieve low stress.
9. Release of the polymer chip from the silicon wafer by wet etching the sacrificial chrome layer. Best results are achieved by drying the released chips using a critical point drier.
The force sensors can also be fabricated using a silicon-nitride coated silicon wafer as a substrate. This process results in a rigid finished chip, but gives much higher yields. The fabrication steps for this process are as follows:
1. Optional patterning and deposition of a metal layer for controlling cell adhesion to the force sensor by creating differences in hydrophobicity between this metal layer and the surrounding polymer or by utilizing surface chemistry differences between the metal layer and surrounding polymer. Patterned in PMMA using electron-beam lithography and deposited using electron-beam or thermal evaporation and lift-off in solvent—acetone, tricholorethylene. Gold is used as the metal with an organic mercapto-silane monolayer as an adhesion layer. The organic adhesion layer is deposited from an aqueous solution after developing the PMMA and prior to evaporating the metal.
2. Deposition of the first polymer layer for the force sensor. SU-8 2000, SU-8 3000, Poly-Imide or parylene can be used. Typically the layer is left unpatterned. However, the SU-8 resists can be directly patterned using electron-beam or photo lithography at this stage.
3. Deposition of the metal wire that makes up the piezo-resistive element of the strain sensor. The wire is patterned in PMMA using electron-beam lithography and deposited using electron-beam or thermal evaporation and lift-off in solvent—acetone, tricholorethylene. Typically gold is used as the metal with a thin titanium or chromium adhesion layer. A spin-on organic titanate (AP300) is used to aid adhesion to the polymer layer.
4. Deposition of the second polymer layer for the force sensor. SU-8 2000, SU-8 3000, Poly-Imide or parylene can be used. Typically the layer is left unpatterned. However, the SU-8 resists can be directly patterned using electron-beam or photo lithography at this stage.
5. Optional patterning of the polymer layers if they were not directly patterned using lithography in steps 2 & 4. The polymer layers are patterned using an oxygen based plasma etch with a mask to protect the regions which are to remain as structural elements on the force sensor. Typically a metal such as chrome or titanium is used as the etch mask and patterned using electron-beam lithography in PMMA. Electron-beam sensitive polymers such as PMMA and UVN-30 have also been used as etch masks.
6. Patterning and deposition of metal layer for fan-out. A thick metal layer, typically gold with a thin titanium or chrome adhesion layer, is patterned using a bi-layer resist, photolithography and lift-off. Typically 200-300 nm of metal is used.
7. Through wafer silicon etch to open vias below the device regions. The backside of the wafer is patterned using photolithography and a window is opened in the silicon-nitride layer using a fluorine based plasma etch. A hot KOH etch is used to etch holes through the silicon wafer leaving only silicon nitride membranes beneath the plastic force sensors.
9. The plastic force sensors are released by preferentially etching the silicon-nitride membrane without damaging the plastic beams. A fluorine based plasma is used to thin the membrane from the back side of the wafer. The membrane removal is finished using a hot, dilute hydrofluoric acid bath which etches silicon nitride without damaging the plastic and metal that comprise the force sensor. After the silicon-nitride membrane has been removed the devices are dried using a critical point drier.
In view of the above described fabrication techniques,
The force sensors have been fabricated on a silicon-nitride coated silicon wafer and suspended over an opening etched in the wafer. This opening makes up part of the fluidic channel that surrounds the force sensor. The rest of the fluidic channel is made from silicone rubber (Poly-DiMethyl-Siloxane or PDMS) based micro-fluidics that are not shown in this image.
The force sensors have been suspended from the wafer's surface by etching a hole through the wafer from the backside using a potassium hydroxide etch to remove the silicon and a combination of a fluorine based plasma etch and a hot, dilute hydrofluoric acid etch to remove the silicon-nitride layer.
The hot, dilute hydrofluoric acid etch is important because it selectively and specifically etches the silicon-nitride without damaging the polymer and metal that comprise the force sensor. The use of hot, dilute hydrofluoric acid to etch silicon-nitride is described in Knotter[P4] which focuses on selecting the etching of silicon-nitride over silicon-dioxide in CMOS process. Accordingly, embodiments of the invention provide for the use of hot, dilute hydrofluoric acid to etch silicon-nitride for the purpose of suspending polymer structures without damaging those polymer.
In the particular instance of a force sensor for measuring forces from a cell, the hot, dilute hydrofluoric acid etch serves a second purpose: the hydrofluoric acid leaves the polymer surface hydrophobic and exposed gold regions hydrophilic. The hydrophobic and hydrophilic nature of these surfaces is critical for the surface chemistry techniques described below.
In the particular instance of a force sensor for measuring forces from a cell with cell contact pads using a titanium adhesion layer, the hot, dilute hydrofluoric acid etch serves a third purpose: the hydrofluoric acid selectively removes the titanium adhesion layer to expose the gold pad without damaging the gold surface. Removal of the titanium adhesion layer is critical to the surface chemistry techniques described below.
In addition to the above, the force sensors may be intended for use measuring forces exerted by individual adherent cells on their surroundings. This requires a cell contact area in close proximity to the force sensors. The cell contact area is a relatively rigid area adjacent to the force sensor upon which an adherent cell can make contact and spread. In one or more embodiments, the cell contact area is defined by a grid of metal (gold) squares. The gold squares can be used to control where the cell attaches utilizing the surface chemistry techniques. Similar gold squares have been patterned on each force sensor in order to control the cell's attachment to the force sensor using the same surface chemistry techniques.
Two types of surface chemistry may be provided in accordance with embodiments of the invention: The first type utilizes the hydrophobic nature of the polymer and the hydrophilic nature of the metal pads. Such techniques may be set forth in further detail in Tan [P5]. The second type utilizes thiol-gold chemistry to form Self-Assembled Monolayers (SAMS) on the metal pads. Such a type is described in Mrksich [P6].
The gold squares that make up the cell contact area on the relatively rigid area and on the force sensors are initially deposited on silicon-nitride and the polymer layers that make up the force sensor are deposited on top of the gold squares. When the force sensors are suspended using the hot, dilute hydrofluoric acid etch described above, the surface of the gold squares to be used for the surface chemistry described above is exposed. The cleanliness and hydrophilic nature of the gold surface is critical for the surface chemistry. There are a couple of techniques that are critical for ensuring the cleanliness and hydrophilic nature of the gold surface.
An adhesion layer must be used to ensure the gold adheres to the silicon-nitride during fabrication. Titanium is a commonly used adhesion promoter for gold on silicon-nitride. However, after the force sensor is suspended the titanium adhesion layer must be removed in order to expose the gold pad. The hot, dilute hydrofluoric acid etch selectively removes the titanium without removing or damaging the gold.
An alternative to the titanium adhesion layer is an organic molecule containing a sulfur atom and a silane group, such as mercapto-tri-methoxy-silane (MPTS). Typically the MPTS is blanket deposited over a silicon or silicon-derivative surface using a solvent solution (such a toluene). The gold layer is then blanket deposited over the surface and patterning of the gold follows using lithography and a gold etch process. These techniques are described in Ling [P7].
The above-described techniques may be insufficient for this process and application for two reasons: first, it may be necessary to pattern sub-micron features in the gold pads which is hard to do using an etch method—liftoff is preferable. Second, there is a layer of gold alignment marks on the wafer that are needed for multiple layer steps, and the etch process would remove those alignment marks as well. To solve these problems, embodiments of the invention utilize a MPTS deposition process that is compatible with metal deposition and patterning by lift-off. The critical step is to deposit the MPTS layer after developing the resist using an aqueous solution with 0.1% acetic acid, which is described in a data sheet available from the Gelest Corporation (also see [P20-P22]). The aqueous solution does not damage the resist layer. This process works well with electron beam resists such at PMMA and with i and g line photoresists such at AZ5214e. Accordingly, embodiments of the invention deposit MPTS from an aqueous solution for this purpose.
Microfluidic valve and pump systems such as those used in embodiments of the invention have been described before and have also been used to implement a cell sorting system [P8]-[P18]. In this regard, references [P8]-[P18] describe a technology used to build multilayer silicone based microfluidics with multiple flow channels, flow modalities and integrated, and computer driven pneumatic controls.
However, none of the prior art systems have encapsulated a polymer NEMS force sensor in microfluidics. In this regard, embodiments of the invention provide for integrating microfluidics with NEMS force sensors.
The microfluidics serve a number of critical functions. Firstly, microfluidics enable delivery of individual cells to specific force sensors. Secondly, microfluidics provide/enable precise control of the chemical environment around the cell/s under study. Precise control is necessary for cell culture (keeping the cells alive). Additionally, precise control adds precision and control when perturbing the cells with pharmacological agents. Third, significant "fan-out" wiring and electronics are needed to extract signals from the force sensors out to a computer for readout and analysis. The microfluidics decouple the "fan-out" wiring from the fluid necessary for cells and biological studies in general.
A minimal microfluidics system can be very simple, consisting of just a few parts and very basic function: In this regard, embodiments of the invention provide for encapsulation of the force sensor to enclose, minimize and control the volume around the force sensor. Further, embodiments may merely comprise a single inlet and a single outlet.
Particular fabrication methods may include partial flow channels that pass completely through the NEMS chip. For this reason, these NEMS devices require encapsulation from two sides. One side of the NEMS device is encapsulated by a glass cover slip with a thin layer of silicone that acts as a glue and seal. The glass cover slip serves a dual purpose: it encapsulates the device and enables high resolution optical microscopy that is compatible with use of the NEMS devices. The other side of the NEMS device, which has the "fan-out" wiring and NEMS devices is encapsulated with multilayer silicone based microfluidics with multiple flow channels, flow modalities and integrated, computer driven pneumatic controls.
A list of the features of the multilayer silicone based microfluidics used on the NEMS force sensor follows. The parts are labeled in
The Incubator Layer also contains a zig-zaging through line which can be used to flow gases through the silicone. Flowing mixtures of air and carbon dioxide through the silicone is sometimes necessary for culturing cells within the microfluidics.
The second layer, referred to as the "Flow Layer" and referred to in the drawings as flow lines and outlet lines, contains 12 inlets lines and 3 outlet lines. There are two classes of inlet lines: low fluidic resistance lines with large diameter for flowing cells and the fast flowing of liquids and high fluidic resistance lines with small diameter for slowly flowing liquids. Cells are very sensitive to fluidic shear forces so it is necessary to feed and perturb cells by slowly flowing liquids.
The flow lines are connected to the devices on the NEMS chip by way of "vias" that travel vertically through the third and fourth layers of the chip.
The third layer on the chip, the "Control Layer," contains 34 pneumatic valves which are used to control the flow in the flow layer. The valves are used at flow inlets, outlets, to isolate lines that connect to the individual force sensors, and in combinations to make a peristaltic pump which can be used to precisely meter flow through the flow lines both forward and backward.
There are also "vias" through the control layer that are vertical flow channels that connect the flow layer to the fourth layer and the NEMS chip.
The fourth layer, the "base layer," is in contact with the NEMS chip and contains flow channels which run parallel to the channels in the NEMS chip and encapsulate the NEMS device while leaving it suspended.
The channels in the base layer contain vertical portions that connect to the "vias" through the control layer and horizontal portions, which run along the NEMS chip.
The base layer also includes a set of high resistance flow channels that allow slow liquid flow to pass by the NEMS force sensor perpendicular to the plane in which the sensor senses forces and out of the plane of the sensor. The purpose of this "out of plane" flow network is to enable fluid flow and reagent exchange for cells on the force sensor that does not mechanically perturb the NEMS force sensor.
Thus, as described above, a microfluidic system is used for various purposes. In addition to that stated above, the microfluidic system may be used to position a cell where desired.
The target location for positioning can be any small object or surface upon which it is desirable to place a single cell. It can range in size from as small as ˜100 square microns up to 10,000 square microns or larger.
A microfluidic channel must pass over the target area. The microfluidic channel confines the fluid flow, and thus cell location, in two directions. The confined geometry of the microfluidic channel reduces the Reynolds number for flow through the channel below 1. Thus the flow through the channel is laminar and the cell can be moved back and forth—reversibly—along a flow line without convective flow moving the cell in an uncontrolled manner.
In one or more embodiments, the valves may be positioned along the flow channel so that the region around the target location can be sealed off from the rest of the microfluidic system once the cell has been positioned over the target area. Sealing a small region around the target area ensures that unintended flow with not move the cell away from the target area while it is settling.
Further, as described above, a peristaltic pump, integrated into the microfluidic channel, may be used to control the fluid flow and thus the cell's location. The pump can be operated forward or reverse to move the cell forwards and backwards along a flow line until it is located over the target area. Clearly the cell must be on a flow line which passes over the target area, if the target area is centered in the microfluidic channel this is not a difficult condition to meet. The minimum resolution of the cell positioning system is determined by the displacement volume of one of the valves in the peristaltic pump and the channel cross section over the target area.
Once the cell has been positioned over the target location, valves are used to seal off the flow channel around the target area. Gravity will gently lower the cell onto the target location.
Force Measurement Results
As described above, one or more embodiments of the invention may provide for fabricating a device and high yields have been demonstrated (>60%). Successful micro-fluidic encapsulation is routine and consistently performed at very high yields, (>90%). The force sensing capabilities of the devices have been tested and calibrated by perturbing the force sensors with glass micro-needles mounted on piezo-electric actuators, data shown in
Data of force measurement from a single cell have shown a stable force in growth media, collapse of that force when the cytoskeleton disrupting agent Cytochalasin D is introduced, and the recovery of the force when the Cytochalasin D is removed. Such measurements were performed with 200 pN force resolution—an improvement of 25 fold over prior art—and 10 ms time resolution—and improvement of 300 fold over prior art.
Vacuum Insulating Polymer-Based Micro-Biocalorimeter Integrated with Microfluidics
In addition to the above described force sensors, one or more embodiments of the invention further provide for the use of a micro-biocalorimeter that is vacuum insulated, polymer based, and integrated within microfluidics.
As described above, a calorimeter is a device for the measurement of the heat capacity of materials and the enthalpy change in chemical reactions. Calorimetry is a technique widely used by the pharmaceutical industry, biologists and chemists to study the kinetics of biochemical reactions and the reaction of living organisms and tissues to chemicals (e.g., drugs). In this regard, calorimeters have been used in diverse research areas in biology, such as studies of thermodynamic properties, structure and interactions of proteins because of universal nature of heat generation in biochemical reaction and simple preparation of samples.
However, the use of calorimeters has been limited due to its large consumption of sample and long measurement time, typically >1 mL and 1 hour. Microfabrication techniques have made it possible to build small scale calorimeters to overcome these disadvantages. In these calorimeters, samples are prepared as either droplets on micro-size sensing regions or flow through microfluidic channels. Microfabricated thermometers are used to achieve very good temperature sensitivity. Measurement sensitivity of these calorimeters, however, are not as good as large scale calorimeters, due to large device heat capacity and thermal conductance. There has been no serious attempt to increase sensitivity by minimizing the heat loss of the sample.
One or more embodiments of the invention provide a fabrication and operation of a highly sensitive heat conduction calorimeter with vacuum insulation, which can detect enthalpy change of reactions from ˜3.5 nanoliter (nL) liquid sample. In this regard, a parylene polymer-based micro-biocalorimeter is integrated with microfluidics (also referred to as a "CIT calorimeter") that is capable of performing batch, isothermal titration and differential scanning calorimetric measurements on 50 picoliter (pL) to 100 nanoliter (nL) volumes of chemical reagents and living tissues. The calorimeter could also be configured as a detector of chemicals and hazardous reagents. The major advantages of the CIT calorimeter over existing biocalorimeters are the following:
1. Small reagents volume: The volume of reagents used in the CIT biocalorimeter is significantly lower than that in conventional commercial biocalorimeters such as a MicroCal VP-IT C [CIT 1] which uses ˜1 micro liter (μL) of reagents. For many applications, this is very useful because reagents (such as a newly synthesized protein) could be very expensive and scarce.
2. Liquid delivery by microfluidics: The use of a microfluidics system with on-chip pumping and valves enables automated delivery of liquid over other biocalorimeters that require manual injection. [CIT 1] [CIT 2]. It also provides efficient delivery of small amounts of liquid at relatively low cost compared to the traditional, "robotic-pipette" systems such as that used by the MiDiCal microplate system developed by Vivactis. It furthermore allows easy interfacing with existing pipelines (e.g., a water distribution system) from which it could draw samples for analysis. Devices including sensor and microfluidic controls can be packed in very small volume and be easily developed as a hand-held detector.
3. Simultaneous operation of multiple calorimeters: Because the calorimeters are produced on inexpensive glass substrates by standard semiconductor processing technologies, the user could obtain and operate multiple (e.g., 100 to 1000) calorimeters simultaneously. This greatly improves the efficiency of calorimetric measurement. Moreover, this low cost calorimeter is disposable, easy to use and saves cost on cleaning.
4. Large bandwidth: The microcalorimeter promises a fast response at ˜1 kHz. It could be used to trace the reaction of a cell to its surroundings.
Overview—Design of the CIT Calorimeter
The three major building blocks of the calorimeter are the thermometry, the microfluidics and the thermal isolated reagents compartment.
The main microfluidic body is built with parylene. Microfluidic control, such as on chip pumps and valves, can be made in different ways. One way is to build a PDMS microfluidic control and combine the control with a parylene channel. Another way is making on-chip electrostatic-actuated pumps and valves on silicon or glass substrates by optical lithography and parylene and metal deposition.
The thermometry is used to determine the temperature change due to the reactions of biochemical reagents. Thermopile thermometry of two thermoelectric components, such as gold and nickel, can be used which is easy to fabricate and reliable. The thermopile thermometry with metallic thermoelements generally provides a responsivity of 200 to 500 μV/K. This is corresponded to a temperature sensitivity of ˜0.1 mK.
The most critical part of a calorimeter to achieve pL-scale reagent volumes is the design of the compartment for reagents. Because of the small volume of reagents and/or living tissues involved, the enthalpy change due to the biochemical reactions is very low. The typical power of a biochemical reaction is 1 to 10 nW for 100 pL of reagents. To generate a resolvable temperature gradient from the power, the total thermal conductance of the compartment to the environment must be very low at ˜1 μW/K. Thus, the average conductivity of the constructing material is ˜0.03 W/m K.
The most common forms of thermal isolation used for calorimeters are thermally resistive enclosures, [CIT 1] air cushions (generated by membranes)[CIT 2][CIT 3] and insulating substrates. Such techniques are not readily applicable to a 100 pL calorimeter. A resistive enclosure for a 100 pL volume has to be made as small as the volume itself. The silicon nitride membranes used by the existing calorimeter are themselves too conductive (thermal conductivity of silicon nitride is 30 W/m K). Finally, everyday insulating materials such as foam are composed of air sacs that are as big as the calorimeter itself and could not be used as the substrate.
In one or more embodiments of the invention, a multi-layered parylene structure is used for vacuum isolation, the suspended parylene structure is fabricated by standard semiconductor processing techniques and extends outward for ˜500 μm.
An inexpensive mechanical pump is applied to create a vacuum 1804 of 1 mbar. This is possible because of the low gas permeability of parylene 1802. The 1 mbar vacuum, coupled with the small dimensions of the layer, has a thermal conductivity of 0.0005 W/m K. The resultant compartment has a thermal conductance of 0.1 μW/K from the vacuum 1804 (residual air) and 0.4 μW/K from the parylene membrane 1802. Thus, the total thermal conductance of the compartment is 0.5 μW/K.
One can emphasize the unique nature of parylene for construction of the compartment because of its low thermal conductivity, gas permeability and available valve structures. Many polymers, such as SU-8, could form similar structures. However, since they could not form valves, the reagent compartment is not cut off from the fluidic channels, which results in large thermal leaks. On the other hand, common microfluidics materials, such as PDMS, are highly permeable to gas and very soft, and so could not support a vacuum.
In addition, a prototype of a parylene microcalorimeter is illustrated in
Detailed Description—CIT Calorimeter
The above description provides an overview of a parylene microcalorimeter in accordance with embodiments of the invention. A detailed description of such a calorimeter follows.
The calorimeter consists of thin film thermopile, parylene-polydimethylsiloxane (PDMS) hybrid microfluidic system and vacuum insulation structure.
Both sides of the parylene membrane 2002 are under vacuum during measurement. Thermopile 2004 is buried between two parylene layers 2002 and protected from the sample, which is placed into the chamber 2006. Au/Ni metallic thermopile 2004 is chosen as a thermometer because of fabrication convenience and low electric noise. 5 thermocouple junctions are connected in parallel to give ˜110 μV/K temperature coefficient (ε).
Referring again to
PDMS peristaltic pumps are used to move liquid through the channel. For a batch mode measurement, a reactant is used to fill up to half of the reaction chamber 2006, and then second reactant is delivered to the reaction chamber 2006 (e.g., via the microfluidic channel created via PDMS 2008, SU-8 2010 and parylene 2002. The second reactant is merged with the first reactant.
Reaction from reactants in the channel may be ignored because its volume is very small compared to total chamber volume. Reactants far from chambers are considered as not participating in reaction due to long diffusion time.
For a microscale calorimeter, it's very challenging to keep the heat capacity of addenda small while reducing the sample volume. For instance, when the sample is surrounded by bulky microfluidic material, much of sensitivity is lost due to huge heat loss to chamber wall. Parylene microfluidic channels can have only ˜1 μm thick wall, so it can reduce heat loss significantly and even replace SiN membrane, which is used for the most of microscale calorimeter even though it is quite conductive. Even more reduction of the heat loss can be accomplished by accommodating on-chip vacuum capability. Parylene thin film 2002 can give very low gas permeability and mechanical strength, which enables the application of vacuum insulation on the device. With nanoliter scale sample volume, the surface to volume ratio of the sample becomes significantly large, resulting in significant heat loss from the surface. This implies that even heat loss through air to the environment can significantly affect the sensitivity.
To calibrate the thermometer signal, thermoelectric voltage response was measured over electric power applied on the gold heater. The heat power sensitivity (SP), which is defined as voltage output over applied power, was 5V/W. Since SP=ε/G, both increase in ε, for example use high Seebeck coefficient material and decrease in G can give better sensitivity. However, materials with a high Seebeck coefficient, such as doped Si, usually has high electric resistivity and give large electric noise on thermoelectric voltage measurement. The resistance of Ni/Au thermopile was ˜1.1 kΩ and the noise at 1 Hz was ˜10 nVrms/√Hz, which corresponds to equivalent power noise of ˜2 nW/√Hz.
Thermal conductance was 22 μW/K. According to the finite element simulation, it can be as small as 5 μW/K if the air conductance was minimized. This result implies the vacuum insulation did not reach its best with only one layer of vacuum sac. Multiple layers of vacuum sac or higher vacuum is expected to improve the overall sensitivity by lowering the thermal conductance.
In view of the above, embodiments of the invention provide a highly sensitive microfluidic embedded calorimeter. Integration of a microfabricated thermal sensing element, microfluidic system and on-chip vacuum structure enable the ability to measure the nanocalorie scale heat of reactions from 3.5 nl samples.
Device sensitivity on thermometer side has not pushed to its limit. Thermopile material with high Seebeck coefficient and multiplication of signal by increasing number of thermocouple junction may provide increased temperature sensitivity. In addition, careful balancing of thermal conductance of each element may provide a further reduction in thermal conductance.
Although single device operation are described herein, multiple devices may also used to increase throughput or to be deployed as detector array. All of the fabrication steps are compatible with mass production. The device concept can also be applicable to different type of calorimeters such as isothermal titration calorimeter (ITC), differential scanning calorimeter (DSC) and flow calorimeter, with simple geometry change.
Fabrication and Use—CIT Calorimeter
To make a suspended parylene membrane, one first builds a 1.5 mm square SiN membrane with a double side polished SiN wafer. This SiN membrane is removed by Reactive Ion Etch (RIE) at the end of fabrication steps. 1 μm thick parylene is deposited on the SiN with PDS 2010 LABCOTER® 2, parylene coater. As a thermometer and a resistive heater, 90 nm thick Ni and 80 nm thick Au are e-beam evaporated on parylene. 4 nm thick Ti is evaporated as adhesion layer for both Ni and Au. They are patterned by photolithography and chemical wet etch. A 1 μm thick 2nd parylene layer is coated as a protective layer. The parylene microfluidic channel can be built in conventional method. A 15 μm thick photoresist is spun and patterned into the microfluidic chamber and the channel structure. A 3rd parylene layer, 2 μm thick, is deposited on the photoresist to build the parylene microfluidic channel. A ˜80 μm thick SU-8 structure is built on top of the parylene microfluidic structure to planarize the surface and to construct the vacuum chamber.
Several etching steps can be conducted by RIE. First, the parylene microfluidic channel opening area was etched (O2 plasma 150 mT, 140 W). The photoresist filling inside the channel is removed using propylene glycol methyl ether acetate (PGMEA). After the microfluidic channel is cleared, parylene covering the electric contact area is etched (O2 plasma 150 mT, 140 W). Finally, the parylene membrane is suspended alone by etching away SiN underneath (CF4 plasma 120 mT, 140 W). The vacuum chamber region is sealed with a glass slide using UV curable glue.
Electrical Measurements may be obtained using the device described herein. Thermal conductance and the device time constant is measured by applying step function heating voltage to the heater. Calorimeter temperature response to applied power can be represented as
The deformable member may be a doubly clamped beam and the strain sensor may be a piezo resistive strain sensor that is patterned asymmetrically through the doubly clamped beam so as to couple to regions of maximum tensile or compressive strain. The piezo resistive strain sensor may be a c-shape that is patterned in the horizontal plane of the doubly clamped beam and is used to measure in-place forces. Alternatively, the strain sensor may be patterned using a straight line pattern to measure out-of-plane forces.
The force sensor may be fabricated from a polymer. In this regard, the strain sensor may be sandwiched between two layers of polymer to electrically isolate the strain sensor from the fluid in the fluidic environment.
In addition to the above, the force sensor may consist of the deformable member and a transducer used for reading out the electrical signal. In such an embodiment, the deformable member may be a doubly-clamped beam made from two polymer layers and the transducer may be a gold wire sandwiched between the two polymer layers. Further, the force sensor may be fabricated on a silicon-nitride coated silicon wafer and suspended over an opening etched in the wafer. Such an opening comprises part of the microfluidic channel that surrounds the force sensor. Also, the force sensor is suspended from the wafer's surface over a hole etched through the wafer's backside. A contact area on the force sensor may also be defined by a metal region or a grid of metal regions that control where a biological sample exerts a force on the force sensor. The metal layer may adhere to the silicon substrate using an organic adhesion promoter and is patterned using metal liftoff.
In terms of fabricating the force sensor, multiple steps may be involved. A first polymer layer may be deposited onto a silicon-nitride layer coating a silicon wafer. A metal wire may then be deposited (on the first polymer layer) that provides a piezo-resistive element of a strain sensor. A second polymer layer is deposited on the metal wire and the first polymer layer. A hole can then be etched through the wafer's backside. The force sensor can then be defined by creating a polymer structure, from the first polymer layer and second polymer layer, that encapsulates the metal wire, and that is suspended over the hole, by removing the silicon-nitride layer from a portion of the wafer, without damaging the first polymer layer and the second polymer layer. The opening may define part of a fluidic channel that surrounds the force sensor. Further, the hole may be etched through the wafer's backside using potassium hydroxide. The silicon-nitride layer can be removed from a portion of the wafer using a combination of a flourine based plasma and a hot dilute hydrofluoric acid.
A further part of the fabrication process may include depositing a metal layer for controlling cell adhesion to the force sensor. Such a metal layer may consist of a grid of metal squares that control where a biological sample exerts a force on the force sensor.
At step 2604, the force sensor is encapsulated in a microfluidic channel. The channel serves to control a fluidic environment around the force sensor and improves an electrical read out (or enables a precise electrical readout) of the electrical signal from the force sensor.
At step 2606, the force sensor is used to measure the force exerted (e.g., by a biological sample/single cell).
At step 2702, a calorimeter chamber is created using a parylene membrane. Both sides of the calorimeter chamber are under vacuum during measurement of a sample. Thus, the calorimeter chamber may consist of two regions. A first region adjacent the parylene member can be defined by SU-8 on a first side and glass on a second side. The second region is adjacent the parylene member and can be formed by potassium hydroxide (KOH) etching for a SiN (Silicon nitride) membrane that is sealed.
At step 2704, a microfluidic channel is created. Such a channel is used to deliver a sample to the calorimeter chamber. Further, the channel is built from the parylene membrane.
At step 2704, a thermopile (e.g., a nickel/gold), used as a thermometer, is encapsulated/located between two layers of the parylene membrane and is protected from the sample. Further, multiple layers of vacuum can be utilized to provide further insulation of the sample.
At step 2708, the biocalorimeter is used to measure the enthalpy change of biological samples in the chamber. A PDMS (parylene-polydimethylsiloxane) peristaltic pump can be used to move the sample in liquid along the microfluidic channel to obtain the measurement.
The foregoing description of the preferred embodiment of the invention has been presented for the purposes of illustration and description. It is not intended to be exhaustive or to limit the invention to the precise form disclosed. Many modifications and variations are possible in light of the above teaching. It is intended that the scope of the invention be limited not by this detailed description, but rather by the claims appended hereto.
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Interview: Alexander Payne on Nebraska
The Oscar-winning writer and director on his new film, shooting in black-and-white, and transforming movie stars into actors.
There are few surer signs of awards season than the imminent release of a new Alexander Payne movie. The writer-director of Election, About Schmidt, Sideways and The Descendants is a darling of the year-end circuit, picking up two screenplay Oscars and guiding many of his performers to acting nods along the way. Payne's latest, the alternately droll and sentimental father-son road trip Nebraska, has already earned star Bruce Dern the best actor prize at this year's Cannes festival and should factor among the accolades distributed in the coming months. It's a stripped-back performance of quiet detail from Dern, framed by Payne's stark, almost haunted black-and-white lensing of a disappearing America. Here, the director chats to RT about the film.
This is the first film in which you weren't directly involved in the original screenplay. What drew you to Bob Nelson's script?
Alexander Payne: Well, you saw the movie, so you can imagine -- not to be obvious -- I liked the setting, I liked the characters, I liked that it would give me a chance to explore parts of my beloved home state that I didn't really know. And it was just pretty funny. It had a pretty Nebraskan, dead-pan sense of humor that I liked a lot, and it was an interesting -- you know, the corny stuff -- father-son story, how they're so distant but they're reconnected and achieve a type of understanding by the end. That's kind of a nice story. It's about kindness. I liked that it was about kindness, ultimately, in a way. That's it. Plus, I'm always so f--king desperate for something to make a movie about. [Laughs] By now I've read, you know, so many thousands of scripts praying that I'd want to make one, it was just such a relief to find one that I could stand to make.
And that you didn't have to write for once.
Well, I rewrote it toward the end, before shooting, and stuff, but it's very much that guy's vision.
One of the things that's constant in your career is that you seem attracted to stories about characters in transition, if not outright life crisis. Is there a particular appeal to that kind of scenario?
Am I really alone in that? Aren't all great stories about characters in transition? Isn't it always about character revealed through times of major or minor life crisis?
A lot of great movies, yes, but not all of them. You're right in that you're not alone in that, it just seems like a very defining trait across your films.
I don't know what to say about it. I'll think about it. [Laughs] I appreciate the observation but yeah, I don't know. What's a movie that doesn't have that? Even, you know, I just saw Gravity -- I'm just pulling this out of a hat because I saw it the other day -- and it's Sandra Bullock in the haunted house, right, but in space?
But even her they imbued with -- whether you thought it was corny or not -- that she had lost a daughter, and this was a way of literally and figuratively getting her feet back on the ground. Even that they had to put that sort of backstory in to add to that. I don't know.
Characters are usually more interesting in a state of change, I guess.
Right, yeah. And the last movie I saw before that was Eric Rohmer's 1986 The Green Ray, and there's that gal -- she's in a crisis of loneliness and solitude, and is on holiday with nobody to go on holiday with. Anyway. Stuff to think about.
Point taken. An immediately remarkable thing about this film is the way it looks. It evokes so many things for me, particularly, as you've said, early Jim Jarmusch and Stranger Than Paradise, Ansel Adams, a bit of Wim Wenders's Alice, The Last Picture Show -- and the most obvious thing that came to my mind, the cover of Bruce Springsteen's Nebraska. Did shooting in black and white, and that kind of visual sense, inform the mood of the film and the circumstances of the performances?
It did. I didn't conceive of shooting the film in color, at all. When we had difficulty in getting it financed in black and white, I walked away from it. And even my DP was saying, "Oh, we could do it in a very desaturated color" and all that crap, and I was like "No! This movie should be in black and white." [Laughs] "And when you see the movie when it's done you'll know why. I can't explain it to you." And I could say all those things, like it certainly didn't hurt Spielberg and Scorsese and Woody Allen and all those guys to shoot their movie in black and white -- those are arguably some of their best films -- and look, most of the movies I watch are in black and white. It never left fine art photography as a choice; nobody asks Sebasti�o Salgado "Why do you shoot in black and white?" I knew that whenever I was gonna make a black and white film it would have to be cheap, and this one was -- under $14 million bucks, for Pete's sake. And it just felt right.
But along with the black and white and the CinemaScope widescreen format, I definitely wanted Autumn in Nebraska, with the corn stubble in the fields and those leafless trees, so you can see the skeletons of the trees. I was trying to see the skeletons of the people and the skeletons of the trees, things really, really stripped back to their essence. Also, by the time we made the film -- I read the script nine years ago -- we were in the midst, and still at the tail-end, we hope, of that economic crisis. So in small-town America the film, just because of the time we were shooting, becomes a Depression-era film; the black and white on a contemporary movie kind of suggests a Depression-era film, so I thought that was kind of fitting.
It definitely has the sense of a film out of time. I wanted to talk a little bit about Bruce. It's an interesting performance, especially given his long screen history and the types of characters he usually plays. He's said he didn't want to be "Bruce Dern" in this movie, so what was it like for the both of you to get to that performance, to strip back a screen persona to what we see on screen?
It's because they want to do that. Working with Nicholson 10 years ago, and working with this guy -- they wanna be somebody else. Especially Nicholson, who was so often asked to be that commercial version of himself. He's trained as an actor. And you know, he can have fun with that commercial version of himself -- the devilish guy with the smile and the raised eyebrows and all that -- but he's a wonderful actor who wants to disappear into a part. And the same thing with Dern. They are anxious to become the guy suggested by the screenplay.
You did that with Clooney, too. You seem to have a knack of taking someone with a very high profile, very particular public persona and getting a real actor performance out of them. What's the trick there? Is it, as you say, because they want to disappear into the roles?
They want to not just be stars, they want to be actors -- and they are; the good ones, of course. I mean, it's so common in Hollywood where you cast a star, and then in the moment of casting the star, you begin tailoring the screenplay to the expected, or the commercial version of that star's persona. I never do that. I want the star to become an actor and become the guy suggested in the screenplay, period. And the moment they do that they -- I hope -- cease to be themselves and their public personae and become the actor, become the person. Then it's up to the audience to determine with what success that happened or not.
You mentioned Gravity before, and one of the things that was problematic for me was that George Clooney was just being George Clooney. It was a very "Clooney" performance, which you didn't see in your film.
Yeah. It's Cary Grant. He's totally Cary Grant there.
This is your second collaboration with the Dern family now. Are there any similarities between working with Laura [on Payne's 1996 debut, Citizen Ruth] and now, her dad?
Both Derns are interested in doing the process that I just described, which is really, really becoming that character -- to use a hackneyed phrase -- warts and all. Especially warts and all. With Laura in Citizen Ruth many years ago, and now with her dad, they are not interested in their own vanity. They don't care about maintaining dignity or stupid, vain beauty at the cost of some bitter truth about the character they're playing. They want to go full-bore, and I like that about them.
Nebraska screens this week as part of the New York Film Festival and opens in theaters on November 22.

subset: commoncrawl


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- Willamette
- College of Law
- News
- Library
- 2011
- International child abduction expert lectures at the law school
International child abduction expert lectures at the law school
Thousands of child abductions occur each year by parents wishing to bring their offspring to their native countries, says child abduction expert Ana Grammaticaki-Alexiou, despite an international treaty designed to compel the return of those children to their homes.
Professor Grammaticaki-Alexiou, who teaches conflicts of laws at Aristotelian University of Thessaloniki School of Law in Greece, is on campus this week to deliver two lectures. One is on international child abduction and the second is about cultural heritage and human rights. She has been a visiting professor at Loyola Law and Tulane Law schools in New Orleans, served as a judge on the Greek Special Supreme Court for three years and served as vice chairperson of the Greek Delegation in the Civil Law Commission of the Council of the European Union. She also has published widely in the areas of conflicts of law, international protection of cultural property, international child abduction and the law applicable to individual employment contracts.
"The bi-national marriages we encounter more and more every day are the reason for the child abduction phenomenon we see," Prof. Grammaticaki-Alexiou told Prof. Kathy Graham's family law class. "Ninety-five percent of the cases are between such parents."
The Hague Convention on Civil Aspects of Child Abduction was adopted in 1980 and has been ratified by 84 nations including the United States. It is intended to prevent one parent from obtaining custody by taking their child to a country that would be likely to grant it.
Prof. Grammaticaki-Alexiou said the idea of the treaty is to return children as quickly as possible to their country of "habitual residence." Delays of a year or two are harmful to young children, she told Prof. Graham's class.
"Think of a baby or a toddler. After a few years they become a completely different person," she said. "You don't want that person to suffer being taken from place to place, as if they were a box."
She highlighted several abduction cases: One involved a Greek couple living in New York. The father was a doctor who worked long hours and rarely saw their baby boy. When the family took the child to Greece for a visit, the mother refused to return to the U.S. The father, who was agreeable at first, later claimed his wife had abducted their child. But a court sided with the mother, noting the father's many hours away from the baby.
Another custody battle in Greece involved a British mother and a Greek father. The mother had taken one of their children to Great Britain but was ordered to bring the child back to Greece. A judge ordered the couple to share a house – with the mother living on one side with their daughter and the father living on the opposite side with their son. Not a good decision, Prof. Grammaticaki-Alexiou said.
Prof. Grammaticaki-Alexiou is visiting the U.S. as part of the Alexander S. Onassis Public Benefit Foundation. The foundation finances scholars from around the world to lecture at universities in North and Latin America on topics that relate to Hellenic civilization.


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Beaumont City Council on Tuesday plans to "discuss and deliberate" negotiations with an unnamed business entity in connection with development of a hotel and water park at Ford Park.
The deliberations are scheduled for council's executive session, which is closed to the public.
Jefferson County built Ford Park almost 15 year ago and has wanted an adjacent hotel to help attract conventions.
Council also will consider offering financial incentives to the OCI project to build a chemical plant on Texas 347 that could be valued at $1 billion to begin.


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Tazo® Rococo Mug - Purple, 12 fl oz
Have more fun with your tea or coffee with this elegant ceramic mug with a Rococo-inspired vine-leaf handle. Designed exclusively for Tazo, the 12-fl oz mug has a matte purple exterior and cream interior. Dishwasher and microwave safe.
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$11.95 / 12 count
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$37.95 / 50 count
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I absolutely love the ergonomics of this coffee cup. I wish all coffee cup handles were like this one. It fits your hand so perfectly you can carry and hold it comfortably for a long time and it's beautiful as well. The overall quality of the cup is top flight too. The only thing I wasn't too thrilled with was the color. It's supposed to be purple, but it's so dull it looks more like a charcoal grey. The other cups I've seen in this style had somewhat odd colors as well...not very appetizing. I'd love it if they would continue to make this style, but amp up the colors (more true, rich colors) and add some interesting graphics to some (stripes, floral or other beautiful patterns). This should be their premier cup line. It would be 5+ stars then!
It was too annoying to return so I now have a nice medium blue mug. Great shape, pretty handle detail.


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ASU's newest solar project changes the way students use the outdoors
PHOENIX -- Thanks in large part to Arizona Public Service and Strategic Solar Energy, anyone on the Arizona State University campus can now enjoy Mother Nature, regardless of the temperature outside.
The two newest PowerParasol solar structures provide shade for people and sunlight for plants, as well as unique lighting and security features, while producing clean renewable energy.
The structures are located near a prominent parking entrance to the Gammage Auditorium, as well as over Pedestrian Mall near Cady Fountain and the Memorial Union.
PowerParasol President Bob Boscamp is thrilled with the project.
"I went to school (there) a long time ago, and nothing had changed in that mall," he said. "No one would ever sit in the mall, unless you were sitting in the fountain hanging your feet in to cool off, and then as soon as you got out, you'd race to go inside the M.U. to get the air conditioning."
He said these new structures provide a venue for students to entertain themselves or hold gatherings before or after events at Gammage. Some even feel it's an ideal place to conduct higher education.
"Some of the professors are already talking about holding class out under the PowerParasol, adjacent to the music school and College of Education," said Boscamp.
The 25-foot-high structures are higher than a traditional carport or canopy solar installation. Construction elements include advertising and promotional signage opportunities.
The first PowerParasol structure was constructed in Lot 59 near Sun Devil Stadium. Fans use that area to tailgate before and after games, and students use it for shaded parking.


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LISTEN CLOSELY TO YOUR INTUITION, so that you can start to make smarter decisions.
Always listen carefully and take notice of the signals coming from your own intuition/Higher Awareness. Learn to TRUST what your intuition is trying to tell you.
There will be times when you receive conflicting messages - when your intuition says one thing while the conscious mind says another. When this happens, don't try to decipher. TRUST your intuition!
Decision making will become easier when you TRUST your own "Gut Feelings." So, learn to take some time for yourself, relax and reflect (meditate), and you will soon hear the answers you seek. When the answer comes, you must act quickly... so there is no time in which to doubt your intuition.
If something doesn't feel right, or something feels wrong, then you need to stop and take a closer look at the details of the situation. You must TRUST your intuition, but NOT BLINDLY TRUST, while making an important decision! Nor, should you blindly trust the words of a psychic/medium when making an important decision. Learn to TRUST your own intuition! Start to work on wakening up your own HIGHER SENSORY PERCEPTION (HSP). God has blessed each and every one of us with a mind (psyche) therefore, WE ARE ALL PSYCHIC!!


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thanks for the help, and it is the bought version not the steam one, and i agree it is far too short, but mayb it is restricted cause the scenario is supposed to be night raids??
---------- Post added at 07:58 AM ---------- Previous post was at 07:52 AM ----------
also, how do i unpack it? so far i can just rid the .pbo and view some of it in microsoft word, do i need any specific program to do
(argh i hate being tech-illiterate :S)
ohk, opned it with my ancient version of word and edited it, but the file can no longer be recognised as a valid pbo file. tried using notepad but it for some reason crashes notepad and doesnt work? :S gah! curse vista and all of its satanic offspring! XS


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Shooting in Newtown, Connecticut Elementary School
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Join Date: Mar 2012
Location: Kent, United Kingdom
Posts: 4,884
Re: Shooting in Newtown, Connecticut Elementary School
There are armed Police in the UK but, as Bad Tempered Clavier says, they are an unusual sight. In the capital, they are usually there as a response to a security alert or to protect a high-value individual such as the Queen or members of the government. Walking around the capital (and I live very close to it, I was in London today, in fact) I have never seen a beat officer wearing a firearm and I don't wish to. The last time I saw an armed officer in the UK was in Gatwick Airport - which obviously has a specific security requirement.
The armed Police in the UK are a very small subset (5%) of officers. Those 5% receive intensive training and are generally only called for in specific instances when life is in immediate danger. Unfortunately, even with this approach to armed Policing, there have been cases in the last few years of officers mistakenly killing civilians, just as there have been cases of civilians killing unarmed officers but these
are incredibly rare
Quite simply, guns are not a topic of everyday British culture. When somebody owns a gun, it is usually on the quiet. I know one civilian that owns a rifle (quite a few own shotguns and the licence is very different) and that is stored at a rifle club, which is practically the only way to own a rifle in the UK. The Section 5 licence - which is required to own anything in a 'military' calibre (e.g. 5.56, 7.62, .223 (same as 5.56 essentially), .308 (same as 7.62 essentially), .303 (old British standard), etc are incredibly stringent to the point that the vast majority of the population could not own a firearm of significant power. Handguns are outright banned. I, for instance, could not privately hold a rifle due to my medical record unless it was stored at a club and everything was logged - including the ammunition.
I find it hard to understand the American attitude towards firearms but I do know a bit about the US Constitution. Nowhere does it say that anybody has the right to own a gun. If they own a weapon, they are supposed to be members of a militia. I doubt that many people in the US that privately hold weapons are members of an organised militia, or have indeed actually studied the Constitutional Amendment. The Second Amendment is actually based on a British writ that says much the same, except with the caveat that any ownership of arms must adhere to other laws - no such caveat is applied in the US Constitution.
As a result, I find it very amusing when people speak of the 'right' to own a gun. The Constitution actually says no such thing! 'Arm' is not a synonymous term and the membership of a militia should be enforceable - but it's not enforced.
The first step in every social change is education and awareness. Of course anybody motivated enough to commit a crime will do so and this may involve a firearm - this is true in any country but in the US the ease of access to firearms is second-to-none in the Western World, with the exception of Switzerland for reasons Henri explained. Guns may not kill people but guns make it a Hell of a lot easier for an individual to commit mass murder should they be motivated. If the same individual had entered the school with a Katana or a Machete, I doubt the death toll would have been anything like as tragic as that which transpired. Trying to bury heads in the sand and deny that gun control is a problem is a deep disrespect to all of those killed in these tragic incidents, at home, work, or school.
From an outsider's perspective, the American attitude towards guns is absolutely crazy. Would I like to own a rifle for target shooting in a controlled environment? Sure. It's fun. Would I like to own a rifle at home for no reason other than my own soundness of mine against some ephemeral 'bad guys'? Hell no.
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Search continues for missing mother, children
WALHALLA - Oconee County sheriff's deputies are continuing to ask for help finding a mother who has not returned her four children, ages 6 to 10, to their father as a required part of a custody agreement.
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Hang tight!
Recipe by FASTWELLIES
"A delicious way of serving beetroot, that can be eaten hot or cold. You may need to adjust the sugar and vinegar to taste. This is better left for the next day, and reheated."
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1/2 pound
3 tablespoons
vegetable oil
onion, diced
1 tablespoon
all-purpose flour
1 cup
chicken broth
2 tablespoons
brown sugar
6 tablespoons
malt vinegar
salt and pepper to taste
We loved this! I cut down a little on the oil, only used enough to saute the onions, and I added a clove of chopped garlic with the onions. Apart from that, followed the recipe exactly. Thank you - will definately make this again!
I needed a way to use up some leftover beets and these were delicious!! The only problem I had was that I used half white vinegar and half red wine vinegar and they were a little more sour than sweet! I will definatley make them again with malt vinegar.
10 Ratings
These were pretty good. A little too sweet. Also I added a clove of garlic after reading the other review. Next time I'll leave that out. I didn't really think it belonged there and I love garlic. Next time i will hold back on a little of the brown sugar and not add any garlic. Also, I used cider vinegar and it worked just fine. Thanks for the recipe. The 4 stars is based on the sweetness. Not my mistake of adding garlic. UPDATE: Made this again with a little less sugar and they were perfect for our tastes.
This was my first experience with fresh beets, and I'm pleased with how they turned out. Here in amish country we must grow things big because the beets took closer to 30 min to cook. I didn't have malt vinegar, but read other reviews and decided to try with cider vinegar- when I reached for the bottle, realized there was only about 1Tbsp in it, and resorted to white, and cut back to 4Tbsp of the vinegar- I tasted the sauce/juice and it was still on the sour side, so just added an extra Tbsp of brwn. sugar. Rated 5 stars because I'm sure if I had the apple cider or malt vinegar, that the sour and sweet would balance! Good recipe despite my purple fingers!!!
These were great! My boyfriend loved them. I love finding new beet recipies, we grow them. This one is a keeper!
Very tasty! I made this vegetarian, so I put vegetable stock instead of chicken broth, and I used 3/4 pounds beets instead of 1/2 a pound, and the flavor came out very nicely.
This is my new favorite recipe for beets. It is just wonderful! Thank you for sharing.
* Percent Daily Values are based on a 2,000 calorie diet.
Sweet and Sour Beetroot
Serving Size: 1/4 of a recipe
Servings Per Recipe: 4
Amount Per Serving
** Calories: 167
** Calories from Fat: 93
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Let me get this straight....Teachers do all the work, student achievement goes up, and principals get extra pay. ?????? Really????
What great timing for any school officials - admins, teachers - to be unable to go and hear what she has to say. Oh wait, our thoughts do not matter to anyone!!!
"AEA bought an election," Johnson said. "I don't think there's any question of that."
What a sore looser!! If by AEA he means teachers, maybe that means teachers did not support him! Sorry, but there are not that many AEA members in District 2! Mrs. Bates is an involved member of the community, and that is what "bought" her the election!
Someone should check on their son! Most of his schooling was spent in alternative school for attacking and harming a school counselor. He was then moved to another school (sound familiar?) Now I believe he is in a permanent detention facility for the same type crime. I also heard suspicion of abuse was reported many years ago by a school official.
"charter schools, which are free of many of the regulations of regular schools"
Idiot! Why not free the public schools of some of the regulations, and let the teachers teach??? If the SD of Ed would stop trying to tell teachers what to teach and how to teach and what day to teach it, and quit hiring specailists to come up with new ways to do old strategies, teachers could actually teach!!! Get discipline back into schools, stop running from problems!!! There are so many people trying to justify their new jobs that teachers aren't allowed to teach any more, just test and look at DATA!!!!
When will we start arresting the parents of all these teens getting arrested??? I think that will stop a lot of problems with society. Parents should be held responsible!!!
All candidates received questions from the board in advance.
Really? I could pass all my tests if I were given the questions in advance!!
google Les Bivens.....strange how he made it into the finals.
Why would a sitting appointed super want a job that, if he wants to keep it, will have to run for election in 3 years? Would it be just to get some time in another state retirement system?
I will be voting for Dan Nash!!!
Dan Nash is a most wonderful man! He has my vote! He will have the best interest of the students in mind at all times. He truely cares about people!!!
Yep, that's one in the same!
"I probably know as much about the programs in the schools as anybody."
He is a joke!! A bully is not needed on the school board. I just pray people know who he really is and vote for who ever runs against him!!! He only cares about himself!!!
and so is education...due to the fact that people keep getting involved that have never been inside a classroom.....................................
When and if they make the needed changes, the law should say elected and appointed emplyees of the state. Teachers are neither! I plan to donate money to my child's teacher's classroom account. Then she can buy the needed supplies for her classes.
As far as $50 an hour, that may be if you only count the time your teacher spends with your child. Teachers to not get paid for the work they do after school hours, weekends, and even in the summer. Please come walk a mile in a teacher's shoes!
we shouldn't be in this situation. He was elected and took money to run for the term. Just to spend more time with family is not a reason to leave an elected office. He should have planned better before running. He should have to return all contributions to his campaign! All elected officials should be held accountable!!! He made a promise and then changed his mind. BOO HOO
I think it is time to charge the over-weight people extra! I smoke, I go to the doctor once a year for a physical. So far so good! If smoking was banned, what would that tax to recoup the lost taxes paid by the smokers? Sodas? Candy? McDonald's? French Fries? Ice Cream? I just don't thin smokers should be targeted. I pay the extra now. I just do not like to be targeted.


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Our family hails from Central Travancore area in Kerala - Pathanamthitta originally, but stay largely in Cochin when we visit. Our quaint family of four has been settled in Alberta for past 30 years, and have semi-modern, but mostly traditional values. My wife and I are employed and working in the Oil & Natural Gas Industry. And have a younger daughter as well, who is completing her undergraduate studies in Medicine too. We belong to the Orthodox - Christian denomination, and are all active members in church and in the community.
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