| United States Patent Application |
20080022513
|
| Kind Code
|
A1
|
|
Liu; Chang
;   et al.
|
January 31, 2008
|
Method of fabricating an artificial haircell
Abstract
Method of fabricating an artificial haircell. A cilium, a strain gauge
connected to the cilium, and a ductile hinge are microfabricated on a
substrate by surface micromachining. The cilium and the strain gauge are
raised with respect to the substrate by application of a magnetic field,
thus bending the hinge.
| Inventors: |
Liu; Chang; (Champaign, IL)
; Chen; Jack; (Urbana, IL)
; Engel; Jonathan; (Champaign, IL)
|
| Correspondence Name and Address:
|
GREER, BURNS & CRAIN
300 S WACKER DR
25TH FLOOR
CHICAGO
IL
60606
US
|
| Serial No.:
|
880131 |
| Series Code:
|
11
|
| Filed:
|
July 20, 2007 |
| U.S. Current Class: |
29/621.1; 374/E7.023; 73/756 |
| U.S. Class at Publication: |
029/621.1; 073/756 |
| Intern'l Class: |
H01C 17/28 20060101 H01C017/28 |
Goverment Interests
STATEMENT OF GOVERNMENT INTEREST
[0002] The invention was made with Government assistance under NSF Grant
Nos. IIS-00-80639 and IIS-99-84954, AFOSR Grant F49620-01-1-0496, and
NASA Grant No. NAG5-8781. The Government has certain rights in the
invention.
Claims
1. A method of fabricating an artificial haircell comprising:
microfabricating a cilium, a strain gauge connected to the cilium, and a
ductile hinge on a substrate by surface micromachining; raising the
cilium and the strain gauge with respect to the substrate by application
of a magnetic field, wherein the hinge is bent.
2. The method of claim 1 further comprising: electroplating the hinge.
3. The method of claim 1 further comprising: forming a layer of permalloy
on the cilium before said raising.
4. The method of claim 1 wherein said microfabricating comprises: forming
a sacrificial layer on the substrate; forming the cilium on the
sacrificial layer; forming the strain gauge on the cilium; forming the
hinge on the cilium and on at least one of the substrate and a support
rigidly connected to the substrate; removing the sacrificial layer.
Description
PRIORITY CLAIM
[0001] The present application is a division of U.S. patent application
Ser. No. 10/861,096, filed Jun. 4, 2004, which claims the benefit of U.S.
Provisional Application Ser. No. 60/476,672, filed Jun. 6, 2003, under 35
U.S.C. .sctn.119.
FIELD OF THE INVENTION
[0003] The invention concerns sensors. The invention relates generally to
the field of microscale sensors.
BACKGROUND OF THE INVENTION
[0004] Humans and other animals are able to perceive and process
environmental conditions using various sensory attributes. For example,
animal skin and hair act to provide tactile and flow sensing for
perception in land and/or water environments. Man-made devices rely on
sensors constructed on many different physical principles, for example
heat and resistance, to obtain similar information. Animal sensory
systems have attributes that are more elegant and efficient than known
sensors.
SUMMARY OF THE INVENTION
[0005] Embodiments of the present invention provide, among other things, a
method of fabricating an artificial haircell. An exemplary method
comprises microfabricating a cilium, a strain gauge connected to the
cilium, and a ductile hinge on a substrate by surface micromachining. The
cilium and the strain gauge are raised with respect to the substrate by
application of a magnetic field, thus bending the hinge.
BRIEF DESCRIPTION OF THE DRAWINGS
[0006] FIG. 1 shows an exemplary tactile sensor node incorporated into a
sensor chip, according to a preferred embodiment of the present
invention;
[0007] FIG. 2 shows a flexed sensor chip, according to a preferred
embodiment of the present invention;
[0008] FIGS. 3A and 3B show a cross section of a hardness sensor, and the
hardness sensor in contact with an object, respectively, according to a
preferred embodiment of the present invention;
[0009] FIG. 4 shows a differential response between the membrane hardness
sensor and a reference sensor versus object hardness, with a linear fit
line;
[0010] FIG. 5 shows a preferred embodiment of a thermal conductivity
sensor, according to an embodiment of the present invention;
[0011] FIG. 6 shows a relationship between thermal conductivity and a time
constant, in which step power input to a gold heater of a thermal
conductivity sensor generates a signal at a nickel temperature sensor,
with a time constant that varies with contact object thermal
conductivity;
[0012] FIG. 7 shows a response of a skin mapping sensor to skin curvature,
according to an embodiment of the present invention;
[0013] FIGS. 8A-8E show an exemplary process for manufacturing a sensor
chip having sensors, according to a preferred embodiment of the present
invention;
[0014] FIG. 9 shows a membrane hardness sensor with a nichrome string
gauge, and a reference bulk sensor, respectively;
[0015] FIG. 10 shows an exemplary flow sensory node, according to another
embodiment of the present invention;
[0016] FIG. 11 shows a silicon based artificial haircell, according to an
embodiment of the present invention;
[0017] FIG. 12 shows a preferred artificial haircell (AHC), according to a
preferred embodiment of the present invention;
[0018] FIGS. 13A and 13B show steps in a preferred process for
manufacturing the AHC of FIG. 12, according to a preferred embodiment of
the present invention;
[0019] FIG. 14 illustrates a post release Ni plating set up, in which an
external magnetic field is used to raise the AHC of FIG. 12, according to
a preferred embodiment of the present invention;
[0020] FIGS. 15A and 15B show a plastically deformed Au hinge without and
with electroplating, respectively;
[0021] FIG. 16 shows an array of AHCs, having different heights and
widths;
[0022] FIG. 17 shows resistance change versus deflection for an 850 .mu.m
long and 200 .mu.m wide cilium;
[0023] FIG. 18 shows airflow response of AHCs inside a wind tunnel, having
various cilium widths and lengths;
[0024] FIG. 19 shows a multidimensional array of AHCs;
[0025] FIG. 20 shows a three-dimensional array of hot wire anemometers,
according to an embodiment of the present invention;
[0026] FIG. 21 shows a polymer membrane diaphragm supporting metal leads
for a pressure sensor and a shear stress sensor, according to a preferred
embodiment of the present invention;
[0027] FIG. 22 shows an exemplary cluster of sensor nodes disposed about a
data processor;
[0028] FIGS. 23A-23C show methods for placing a data processor on a
polymer substrate;
[0029] FIG. 24 shows a flexible silicon chip; and
[0030] FIG. 25 shows steps in an exemplary process for forming an
elastomer skin with embedded silicon islands.
DETAILED DESCRIPTION
[0031] For machines such as robotics to replace or serve as extensions of
humans in dangerous, delicate, or remote applications, such machines
should have sensory input at least comparable to human senses. One of the
most important senses for performing varied complex and precise tasks
autonomously or remotely is the sense of touch.
[0032] Human beings, for example, employ a flexible, robust sensory skin
with a distributed architecture to achieve accurate object identification
and dexterous manipulation. Tactile feedback from human skin provides a
multitude of information, including force, temperature, hardness,
texture, and thermal conductivity. However, conventionally, machines have
not had the sensing capability to provide an equivalent sense of "touch".
[0033] Providing artificial tactile and/or flow sensors that provide rich
sensor data incurs significant challenges. For example, an optimal
artificial sensor would provide multiple sensing modalities, mechanical
flexibility and robustness, efficient signal processing, and high density
of integration with signal readout and electronics. Further, it would be
preferred that such an artificial sensor would be capable of being
manufactured with high efficiency and relatively low cost.
[0034] Artificial sensors have been created to provide force imaging and
measurement. Such sensors have included silicon-based sensors, using
piezoresistive or capacitive sensing, and polymer-based approaches that
use piezoelectric polymer films for sensing. Others have combined some of
the strengths of silicon with polymer-based devices, such as by embedding
silicon sensing elements in polymer skins, or by covering silicon-based
devices in a protective polymer layer. Other devices have been used to
measure contact force and object thermal properties.
[0035] A fundamental difficulty faced in creating artificial sensors such
as "sensing skins" is that the sensors in operation would directly
contact a variety of objects and contaminants under any number of loading
conditions. As a result, devices that incorporate brittle sensing
elements such as silicon-based diaphragms or piezoresistors, even
embedded in protective polymers, typically cannot be used as an interface
"skin" between a robotic manipulator and the manipulated object. Devices
made with pressure-sensitive rubbers that can withstand contact have been
provided, but they require serial manual assembly and provide limited
independent sensing modes.
[0036] According to preferred embodiments of the present invention, an
artificial sensor chip (or a large-area patch) is provided on a
polymer-based substrate, forming a skin. Preferably, the sensor chip is
flexible, providing a sensory skin that can be, for example, mounted on
curved or other non-flat surfaces easily and can withstand mechanical
flexure and movement.
[0037] The sensor chip incorporates one or more metal film sensors. This
provides many functional advantages and uses. The sensors preferably are
distributed in an array, such as a two-dimensional array, having high
spatial density and integrated signal processing capabilities. The sensor
chip and sensor components thereon preferably are sufficiently robust to
survive mechanical contact with an external harsh environment.
[0038] Unlike sensors in an integrated circuit chip that are packaged in
enclosed environments, individual sensors according to a preferred sensor
chip are exposed. Also, it is preferred that a frontal surface of the
sensor chip be relatively smooth and free from mechanical protrusions,
etch holes, exposed wiring, or other flaws and design compromises that
would allow environmental contamination or accelerated wear and failure
of the device.
[0039] In a preferred sensor chip, the distributed sensors are connected
using signal processing circuitry that is distributed spatially and can
accommodate multiple streams of analog sensor output with minimal
footprint and power. Local, distributed signal amplification and
analog-digital conversion are preferred to preserve signal-to-noise ratio
(before a signal is broadcasted through wire leads). Local signal
processing avoids the routing bottleneck associated with long wire leads.
[0040] The density of integration of the sensors on a preferred sensor
chip may reach as high as, for example., 1-10/mm.sup.2. The maximum
density on a preferred chip may be determined not only by sensor sizes
but also by the footprint of signal processing circuits.
[0041] Also, in preferred methods of manufacturing the sensor chip, the
cost of manufacture should be as low as possible to allow widespread use,
especially if large continuous sensor chip surfaces are required.
Manufacturing processes are preferably integrated and efficient.
Particularly, monolithic integration is preferred because costs can be
reduced through batch fabrication. It is also preferred that the efforts
for calibrating three-dimensional sensor positions should be minimized to
streamline their use.
[0042] Preferred sensor chips include multi-modal sensor nodes that are
for tactile sensing and/or for flow sensing. For example, a multi-modal
tactile sensing node may be provided.
[0043] A preferred multi-modal tactile sensor node can successfully
incorporate multiple sensor modalities for evaluating one or more of
contact forces, and the relative hardness, thermal conductivity, and/or
temperature of a contacted object.
[0044] Traditional microfabricated tactile sensors suffer from a number of
significant disadvantages. For example, they are typically based on
silicon, which is usually a rigid and fragile material from a mechanical
point of view. Exposing the sensors presents problems if silicon is used,
because silicon is easy to fracture upon mechanical impact and
over-loading. For example, many silicon micromachined tactile sensors do
not stand force loading well.
[0045] The individual sensors of each multi-modal sensory node are
fabricated on the polymer-based substrate using surface micromachining.
Thin-film metal elements are used, for example, as piezoresistors,
heaters, and temperature sensors. Preferred methods for manufacturing the
individual sensors involve a relatively low temperature and do not
involve bulk micromachining. In this way, all of the sensors can be
formed on the polymer-based substrate.
[0046] Also, traditional silicon sensors only sense surface roughness
features and contact forces. By contrast, a preferred tactile sensing
node may contain one or more of surface roughness, contact force
measurement, thermal conductivity, hardness, temperature, and/or
proximity sensors. Such additional modalities preferably allow a
preferred tactile sensor node to characterize an object in a more
comprehensive fashion.
[0047] Another exemplary multi-modal sensor node that may be formed on a
surface of the sensor chip is a flow sensor node. A preferred multi-modal
flow sensor node can characterize a boundary-layer flow field in a
comprehensive fashion, with high spatial and temporal resolution. Such
exemplary multi-modal flow sensor nodes may be used, for example, in
real-time monitoring of a flow field in underwater vehicles and
structures, and in characterizing flow fields around models in
experimental wind or water tunnels.
[0048] Traditional flow sensors are based on hot-wire anemometry for
measuring flow speed, or diaphragms for measuring pressure distribution.
Such different sensors typically have been based on specific structures
that are significantly incompatible with fabrication processes and
materials. Accordingly, it has been impossible to measure several flow
parameters locally and with a distributed array. By contrast, a preferred
multi-modal flow sensor node includes one or more of various flow
sensors, including, for example, surface micromachined artificial
haircell sensors (for flow rate), surface micromachined hot-wire
anemometers (for flow speed distribution, preferably along three axes),
and surface micromachined diaphragms, preferably manufactured from
Parylene, for pressure sensors and shear stress sensors (for vortex and
drag detection).
[0049] A preferred sensor chip substrate is manufactured primarily from
polymer-based materials, as opposed to silicon. Because silicon is a
relatively fragile material for sensors, sensor chips made out of polymer
material offer desirable mechanical flexibility and robustness compared
with silicon counterparts. However, most existing polymer materials such
as silicone elastomer, polyimide, and plastics cannot host signal
processing electronics like silicon substrates do.
[0050] Hence, a preferred sensor chip integrates flexible polymer devices
with discrete silicon chips for signal processing. The silicon chips
(islands) are selected and designed so as not to significantly impede the
overall mechanical flexibility and surface integrity of the sensor chip,
and so that they can be integrated in efficient manufacturing processes
without significantly compromising cost.
[0051] Exemplary applications of a preferred sensor chip include, but are
not limited to, smart tactile skins for sensor-rich surgical tools,
robotics manipulators, computer periphery input devices, and smart toys
having sensor input. Preferred sensor chips having flow sensors may be
useful for, e.g., smart flow sensing skins for underwater robots (e.g.,
for exploration or mine detection), underwater vehicles and
infrastructures (e.g., oil drilling stations in deep sea), and scientific
exploration and measurement (e.g., wind tunnels). Preferred embodiments
of the sensory chip have the potential to make a significant impact on a
broad range of applications for industry, exploration, military, and
security, as nonlimiting examples.
[0052] Referring now to FIG. 1, an exemplary sensor chip 10 is shown,
embodied in a flexible polymer-based substrate 12 forming a skin, and
including a plurality of multi-modal sensor nodes 14, shown as
multi-modal tactile sensor nodes. As shown in FIG. 1, the multi-modal
sensor nodes 14 are repeated over an n.times.n array (as shown,
3.times.3) to form the sensor chip 10. A preferred multimodal tactile
sensor node, for example, includes multiple sensor modalities (hardness,
thermal conductivity, temperature, contact force, surface roughness).
These nodes 14 in an exemplary embodiment are repeated with a spatial
frequency of approximately 1 per 1 cm.sup.2, though this repetition or
particular distribution is not necessary. For example, individual nodes
may have the same number of sensors or a significantly different number
and/or type of sensor. Also, the spatial frequency of the nodes can vary,
and may be greater or fewer than 1 per 1 cm.sup.2.
[0053] The multi-modal sensor node 14, a tactile sensor node, includes a
temperature sensor 16, a thermal conductivity (thermal flux) sensor 18,
and a contact force and measured hardness sensor 20. The multi-modal
sensor node 14 also includes a reference hardness sensor 22 for use with
the contact force and measured hardness sensor 20. Sensors may also be
implemented for such tasks as object identification and impending
slippage detection. In the preferred tactile sensor node 14, a reference
nickel resistance temperature device (RTD) of the temperature sensor 16
provides temperature measurement and compensation, a gold heater 24 and
nickel RTD 26 pair provides thermal conductivity measurement for the
thermal conductivity sensor 18, and the membrane NiCr (nichrome)
strain-gauge based contact force and hardness sensor 20 with the
reference contact hardness sensor 22 measures hardness.
[0054] The substrate 12 is preferably made of a polymer-based material. In
an exemplary sensor chip 10, the substrate is a 2 mil thick Kapton HN200
polyimide film, manufactured by E.I. DuPont de Nemours and Co. The
polymer substrate allows flexibility, robustness, and low material cost.
Flex channels 30 are provided in the substrate along two dimensions by
forming indentations in the substrate 12. The flex channels 30 provide
enhanced and controlled flexibility to the substrate 12.
[0055] In addition, the contour of the substrate 12 is sensed in an
integrated fashion using mapping sensors 32 embodied in microscale strain
gauges, also preferably made of NiCr, and dispersed between the sensory
nodes 14 (as shown in FIG. 1, the tactile sensor node). The mapping
sensors 32 are dispersed between the sensory nodes 14 to sense bending of
the substrate. In this way, the contour of a bent skin is sensed in an
integrated fashion using the mapping sensors 32. For example, when the
sensor chip 10 is mounted on a curved or compliant surface (e.g., a
robotic finger tip), as shown by example in FIG. 2, the spatial relation
of the multi-modal sensor nodes 14 is mapped to coordinate manipulation
in three-dimensional space.
[0056] Individual sensing elements will now be described in more detail.
As shown in FIG. 1, a preferred temperature sensor 16, for example,
includes a nickel resistance temperature device (RTD) 34 that is used to
measure the temperature of the operating environment as well as contact
objects. This information is important for temperature compensation of
the measurements of the other sensors as well as providing contact object
information. The temperature sensor 16 and other sensor components are
connected to other parts of the sensor chip, such as a processor, by
leads 36.
[0057] Because all the sensors 16, 18, 20, 22 incorporated on the
exemplary tactile sensing node are based on thin film metal resistors,
all of them will function as RTDs to one extent or another based on the
TCR (thermal coefficient of resistance) of the base material. This value
is low for NiCr, making it a good choice for rejecting thermal
disturbances, but is high for nickel and gold. Gold is not used for a
preferred RTD due to its low resistivity. By using nickel, a high TCR is
provided with the added benefit of increased resistivity to decrease the
effect of parasitic resistances. The TCR of each sensor is characterized
to allow temperature compensation by calibrating the reference nickel
RTD, for example, by heating the sensor chip 10 and observing the changes
in resistance with temperature, then calculating the base metal TCR.
[0058] Hardness of a contact object is an important parameter for object
identification and manipulation. This measurement modality is lacking in
most conventional tactile sensors. Existing micromachined hardness
sensors require that the applied force be known, use a known calibrated
integral actuator force, or use changing resonant frequency under
ultrasonic vibration. The required assumptions, complexity, and size
limitations of such approaches do not lend themselves to a distributed
multi-modal sensor chip. By contrast, a preferred hardness sensor 40
shown in FIGS. 3A-3B is a passive hardness sensor that does not rely on
actuation or knowledge of contact force.
[0059] Referring now to FIGS. 3A-3B, the passive hardness sensor 40, which
may be incorporated into the multi-modal sensory node 14, derives a
hardness of a contact object using two contact sensors of different
support stiffness: the contact force and measured hardness sensor 20 and
the reference hardness sensor 22. The preferred hardness sensor does not
rely on knowledge of contact force. In a preferred embodiment, the
measurement sensor 20 is mounted on a polymer membrane, while the
reference sensor 22 is built on the bulk substrate 12. Both the
measurement sensor 20 and the reference sensor 22 include a strain gauge
42, which may be made from NiCr, for example, to measure response. A
differential response between the measurement sensor 20 and the reference
sensor 22 is used to measure the hardness of a contact object 43.
[0060] The structure of the preferred hardness sensor 40 within the sensor
node 14 is shown in FIG. 3A and in cross section in FIG. 3B. The
exemplary hardness sensor 40 includes the measurement sensor 20 on a
square polymer diaphragm 45 and a reference sensor 22 on the bulk polymer
substrate 12. Both sensors 20, 22 include a contact mesa 46 with the
strain gauges 42 situated on the periphery of these mesas. The square of
a diaphragm 45 of the measurement sensor 20 has a relatively low
stiffness and for a given maximum central displacement requires a uniform
pressure according to clamped-clamped plate theory as shown in Eq. 1.
q plate = z max .times. E .times. .times. t 3 ( 0.0138 )
.times. b 4 ( 1 )
[0061] In Eq. 1, z.sub.max is the peak vertical deflection in the center
of the diaphragm 45, q.sub.plate is the pressure applied to the plate, b
is the length of the square sides, E is the material modulus, and t is
the plate thickness.
[0062] The preferred reference sensor 22 does not use a diaphragm; rather
the contact mesa 44 and the strain gauges 42 are positioned over full
thickness bulk polymer 12. The stiffness of the bulk reference sensor 22
is thus much higher than the measurement sensor diaphragm 45. The
preferred reference sensor 22 requires a uniform pressure for a given
deflection according to Eq. 2. q bulk = z max .times. E (
2.24 ) .times. a .function. ( 1 - v 2 ) ( 2 )
[0063] In Eq. 2, .nu. is the bulk material Poisson's ratio, a is the
contact mesa 46 width, and q.sub.bulk is the pressure applied to the bulk
sensor contact mesa. This model assumes that the reference sensor 22
behaves like a semi-infinite block under a uniform pressure over the area
of the contact mesa.
[0064] When the sensor chip 10 is in contact with the object 43, changes
in resistance are observed at both the measurement and reference sensor
strain gauges 42. The measured resistance changes are converted to a peak
deflection (z.sub.max) with calibrated resistance versus displacement
data and used to find the apparent pressures q.sub.plate and q.sub.bulk
with Eqs. 1 and 2. The contact object hardness 43 is related to the ratio
of apparent pressures.
[0065] Measurement of contact forces can also be performed using the
measurement sensor 20 and the reference sensor 22. Based on the known
geometry of the devices, the pressures can be equated to normal force.
The differential stiffness of the two sensors 20, 22 allows two different
ranges of contact forces to be measured.
[0066] In an experimental operation of the hardness sensor 40, a number of
polymer samples were placed in contact with the sensor skin 12. A range
of reference samples of sorbothane and polyurethane rubber with known
hardnesses ranging from 10 to 80 Shore A were cut into 5 mm by 5 mm
squares and pressed onto the sensor skin 12 using a fixed mass (147 g).
The change in resistance of each sensor 20, 22 was converted to an
equivalent displacement using calibration data. Calibration data was
generated by measuring the change in resistance of the measurement
membrane sensor 20 and the bulk reference sensor 22 in response to a
known normal displacement provided by a micromanipulator probe coupled to
a precision linearly variable differential transformer (LVDT).
[0067] The proportionality between pressure ratio and object hardness is
shown in the graph of FIG. 4. A large amount of scatter was observed in
the hardness data as can be seen in the graph. This is attributable to
the surface roughness of the rubber samples. Nevertheless, a clear
overall trend is observed when a large number of data points are averaged
as in FIG. 4, showing an increase in pressure ratio with object hardness.
[0068] The thermal conductivity of the contact object 43 is another
important piece of data for object identification. The thermal
conductivity sensor 18 operates by observing the changing resistance of
the nickel RTD 26 in response to an input to the gold heater 24. The
thermal conductivity of the contacting object 43 is a useful measure for
object discrimination, and in concert with other sensing modes can expand
the capabilities of the overall sensor chip 12 by helping to distinguish
between equally "hard" objects for example.
[0069] As shown, the value is derived by measuring heat flux between the
heater 24 and the temperature sensor 26, which are disposed on the
polyimide substrate 12. The heater 24, preferably manufactured from gold
as described above, is disposed on a bump 48 (FIG. 5) formed on the
substrate 12, and is situated near, yet separated from, the temperature
sensor 26. The exemplary temperature sensor 26 is embodied in an Ni RTD
thermoresistor, also disposed on the bump 48. The heat transfer between
the heater 24 and the temperature sensor 26 is altered when the contact
object 43 contacts the surface of the sensor chip 12 over the thermal
conductivity sensor 18, which changes the thermal transfer path. The heat
flux travels through the contact object 43 as well as the substrate 12,
which changes the signal measured at the temperature sensor 26. A stepped
power input to the heater generates a signal at the temperature sensor
with a time constant that varies with the thermal conductivity of the
contact object.
[0070] When not in contact with the object 43, the only route for the heat
input of the heater 24 to reach the RTD of the temperature sensor 26 is
through the polyimide substrate 12 and the surrounding air. When the
object 43 comes in contact with the thermal conductivity sensor 18, the
low efficiency heat path through the air is replaced by solid conduction,
changing the character of the signal measured at the temperature sensor
26. Using an Ni RTD as the temperature sensor 26, for example, with a
square wave voltage input to the heater, the temperature of the
temperature sensor can be modeled as a simple first order system
according to Eq. 3. T.sub.RTD(t)=1-e.sup.-t/.tau. (3)
[0071] Where T is the time constant of the first order system, giving a
measure of how quickly the system responds to an input. The time constant
of the temperature of the temperature sensor 26 is found to be a function
of contact object thermal conductivity. This method was found to
correlate well to contact object thermal conductivity.
[0072] In an exemplary operation, characterization of the performance of
the thermal conductivity sensor is performed at room temperature
(.about.22.degree. C.) by inputting a 0-2VDC square wave at 0.3 Hz to the
gold heater 24 and measuring the resulting change in resistance of the
nearby Ni RTD 26. The resistance of the RTD is sampled at 10 Hz using an
Agilent 33410A multi-meter and GPIB interface.
[0073] The thermal conductivity sensor 18 preferably should behave as a
first order system with a time constant related to the object thermal
conductivity. FIG. 6 shows the result of testing, where contact objects
of various thermal conductivities (nylon 6, soda-lime glass, single
crystal silicon, 300-series stainless steel, aluminum, and ambient air)
were placed in contact with the surface of the thermal conductivity
sensor 18, and the time constant of the resulting signal at the
temperature sensor 26 was obtained through curve fitting. It was observed
that the time constant decreases and the step response of the temperature
of the temperature sensor 26 is faster with increasing thermal
conductivity. Scatter is observed and expected due to changes in contact
configuration from test to test due to surface roughness. The
relationship between object thermal conductivity and time constant is
found to be approximately logarithmic based on a curve fit of FIG. 6. As
shown, more conductive objects result in faster response and smaller time
constant.
[0074] Another type of sensing measures curvature of the substrate using
the mapping sensor 32 described above. The mapping sensor 32 preferably
embodied in integrated NiCr strain gauges dispersed between the sensor
nodes 14 measures the x- and y-direction curvature of the flexible
substrate 12. The mapping sensors 32 are positioned over the flex
channels (trenches) 30 etched in the back of the polyimide substrate 12
to allow the substrate to preferentially bend in these regions.
Processing of these measurements into bending angles using calibrated
data allows a three-dimensional mapping of skin curvature state. The skin
mapping sensors 32 are found to perform linearly (R.sup.2=0.996) with
respect to curvature with sensitivity of 44.25 ppm.
[0075] Skin curvature calibration is accomplished by flexing the substrate
12 under known displacement using a micromanipulator coupled to a
precision linearly variable differential transformer (LVDT). Measurements
are taken while bending and relaxing to assess viscoelastic hysteresis
and plastic deformation. A resulting response of the mapping sensors 32
versus skin flex for a number of tests is seen in FIG. 7.
[0076] The processing steps preferably do not have to involve high
temperature steps or bulk micromachining, therefore they can be substrate
neutral. Specifically, the microfabrication process can be carried out
directly on flexible and low cost polymer substrates.
[0077] A description of an exemplary fabrication process follows for the
sensory chip and the tactile sensory node, referring to FIGS. 8A-8E. A
polyimide film substrate 60, for example a 50 mm square sheet cut from a
sheet of DuPont Kapton HN200 polyimide film is provided. This film 60 is
preferably about 50 .mu.m thick, though other thicknesses may be used.
During the fabrication of the polyimide film 60, one surface of the film
is in contact with a roller and the other is untouched. In practice,
measurements with an optical vertical scanning interferometer (VEECO
LM1000) showed very small roughness differences between the free and
roller faces (197 nm and 243 nm Rq respectively). Prior to
photolithography, the polyimide film substrate 60 is cleaned and then
baked at 350.degree. C. under nitrogen at 1 Torr for 2 h.
[0078] Once the polyimide film substrate 60 has been cured, an aluminum
etch mask 62 is deposited and patterned via lift off on the "rough"
roller side of the film (FIG. 8A). The film substrate 60 is then etched
in an oxygen plasma reactive ion etcher at 350 W with 300 mT oxygen
pressure (FIG. 8B) to define the flex channels 30 and the membrane sensor
diaphragms 45. The film 60 preferably is etched 40 .mu.m down at a rate
of 330 nm per minute. This plasma-etching step preferably is performed
first to avoid erosion of backside metal layers that may otherwise occur.
[0079] With the sensor node 14 regions and contact force membranes
defined, a 2-.mu.m-thick layer of photo-definable polyimide (for example,
HD Microsystems HD4000) is spun on the smoother top skin surface and
patterned to define contact mesas 46 for the thermal conductivity 18 and
reference RTD sensors 22 (FIG. 8C). FIGS. 9A-9B show exemplary RTD strain
gauges on a membrane hardness sensor 20 and a reference bulk sensor 20,
respectively. This layer is aligned to the backside features via
alignment marks visible due to the optical clarity of the HN200 film.
Once patterned, the polyimide layer is cured under 1 Torr of nitrogen at
350.degree. C. for 2 hours.
[0080] Next, nickel RTDs 26 are patterned and deposited on the contact
mesas 46. For example, nickel (e.g., 500 .ANG. Ni) 64 is thermally
evaporated via e-beam on top of a 100 A chrome adhesion layer (not
shown). Then, 750 .ANG. of NiCr 68 is deposited and lifted off to define
the strain gauges for the force 20, curvature (mapping) 32, and hardness
sensors 22. Preferably, no adhesion layer is used. In order to achieve
the relatively high resolution required for the minimum NiCr (10 .mu.m)
and Ni (15 .mu.m) feature widths on a flexible polymer substrate, in a
preferred embodiment, the Kapton film 12 is temporarily attached to a
Pyrex substrate via surface tension by wetting the substrate with a drop
of deionized water. The RTDs 26 are patterned preferably via liftoff
using standard image reversal photolithography. The last metal layer
comprises 1500 .ANG. of gold 70 on a 100 .ANG. chrome adhesion layer that
is thermally evaporated and lifted off (FIG. 8D), forming wiring 36.
Before each metal deposition step 60, the film substrate is placed in
oxygen planar plasma for 3 minutes at 300 W to remove photoresist residue
from image reversal and to improve metal adhesion to the polymer film.
[0081] The final step is to spin on and pattern the tactile contact bumps
46 for the force and hardness sensors (FIG. 8E). The bumps 46 are defined
from an 8-.mu.m-thick layer of HD4000 photo-definable polyimide in the
center of each sensor. The polyimide is cured for 2 hours at 350.degree.
C. and 1 Torr nitrogen.
[0082] Another embodiment of the present invention includes a sensor node
for flow sensing. The substrate may be polymer-based as in the substrate
supporting the tactile sensor node 14.
[0083] Comprehensive flow sensing in the fluid boundary layer involves
measurement of, for example, pressure, shear stress (drag and vortex),
temperature, and three-axis flow rates. The spatial and temporal
evolution of surface flow features is extremely difficult to obtain due
to limitations of scientific instruments.
[0084] Conventional flow sensing instruments such as hot-wire anemometers
are singular point measurement devices only. They suffer from a number of
bottlenecks: their sizes are large and may change the characteristics of
the flow; it is extremely difficult to measure multiple flow parameters
including vector speed, pressure, and shear stress, which is proportional
to the gradient of velocity in the boundary layer; and it is difficult to
characterize a flow field within a thin boundary layer (thickness on the
order of 1 mm).
[0085] Microfabricated flow sensing surfaces with multiple sensing
modalities to record pressure, shear stress, and flow rates would be
useful for experimental fluid mechanical studies and for underwater
vehicles and platforms. Such sensors preferably would be fabricated using
efficient, low cost techniques. They preferably would allow integration
of microelectronics signal processing units, and should be relatively
mechanically robust.
[0086] Potential application scenarios for multi-modal flow sensors may
include, but are not limited to: comprehensive monitoring of liquid flow
field for underwater vehicles and structures, such as autonomous
underwater vehicles, deep-sea drilling stations, and military vehicles
for possible drag reduction; and comprehensive monitoring of air flow
conditions for aircrafts and unmanned vehicles.
[0087] A large sensitive skin could be used to cover an object with a
large area and curved surfaces. For example, an aerodynamic model used in
an experimental wind- or water-tunnel may be covered with the sensitive
skin in strategic regions to provide direct experimental characterization
of flow field. Such flow field data has been prohibitively difficult to
obtain in the past. Such comprehensive results can be used to validate
and improve theoretical models or provide aerodynamic design insights.
[0088] The diagram of an exemplary single sensor node is illustrated in
FIG. 10. According to an embodiment of the present invention, the node
70, which may be disposed on a flexible, polymer-based substrate 72, is
provided with one or more of the following sensing units: an artificial
haircell 74 for measuring three-dimensional flow velocity, one or more
hot-wire anemometers 76 along one or more dimensions for measuring the
velocity of flow at different distance to the boundary layer, a pressure
sensor 78 for monitoring pressure variation, and a shear stress sensor 80
for measuring surface vortex. Various sensors may be integrated together
on the polymer substrate using novel material and fabrication processes
as described herein.
[0089] Fish and many underwater animals utilize multimodal sensitive skin
that can detect flow, pressure distribution, electrical potential and
field, and local vortex. The lateral line is a primary sensing organ for
fish. It usually spans the length of the fish body. Its main functions
include (1) detection of water flow around the fish body, allowing a fish
to maintain stability within turbulent currents and (2) detection of
distant objects such as obstacles, prey and predators using direct or
reflected waves. Linearly distributed along the lateral line are
clustered haircell bundles embedded in a gel-like dome called a
neuromast. Water flowing past the neuromasts imparts forces to the
haircells and causes them to bend, with the extent of the bending
determined by the speed of the flow. In certain species, the haircells
lie outside of the epidermis; in others, they are embedded in sub-dermal
canals for added protection against wearing and damages.
[0090] Artificial haircell sensors may be used for mimicking the lateral
line system of fish. A schematic diagram of an exemplary haircell sensor
82, made of single crystal silicon substrate 83, is shown in FIG. 11. The
haircell sensor 82 consists of an in-plane fixed-free cantilever 84 with
a vertical artificial cilium 86 attached at the distal, free end.
External flow parallel to the sensor substrate 83 impacts upon the
vertical cilium 86. Due to rigid connection between the in-plane
cantilever 84 and the vertical cilium 86, a mechanical bending moment is
transferred to the horizontal cantilever beam, inducing strain at the
base of the cantilever beam, which is detected using a strain sensor 88,
such as a piezoelectric sensor producing a signal that is transmitted by
conductive contacts 90. The magnitude of the induced strain can be sensed
by many means, for example by using integrated piezoresistive sensors.
[0091] The vertical cilium 86 preferably is realized using a
three-dimensional assembly technique called plastic deformation magnetic
assembly (PDMA). A description of the PDMA process is provided in J. Zou,
J. Chen, C. Liu, and J. Schutt-Aine, "Plastic Deformation Magnetic
Assembly (PDMA) of Out-of-Plane Microstructures: Technology and
Application; IEEE/ASME J. of Microelectromechanical Systems, Vol. 10, No.
2, pp. 302-309, June 2001, which is incorporated in its entirety by
reference. A preferred assembly process allows reliable formation of
three-dimensional structures in large array format. Multiple structures
can be achieved at wafer-scale by a globally applied magnetic field.
Position and height of the cilia can be controlled.
[0092] A preferred polymer based haircell device is also provided, as
shown by example in FIG. 12. An artificial haircell (AHC) 92 includes a
vertical beam 94 (cilium) rigidly attached to the substrate 92. The
vertical cilium 94 is made of surface micromachined polymer, and more
preferably includes a stiff permalloy plating.
[0093] As shown in FIG. 12, the vertical cilium 94 is rigidly attached to
the substrate 72 by one or more rigid metal supports 95. The substrate 72
can be any of various substrates, but preferably is a polymer-based
substrate. Attached at the base of the vertical cilium 94, between the
cilium and the substrate, is a strain gauge 96. The strain gauge 96
includes a thin film nichrome (NiCr) resistor on a thicker polyimide
backing that runs the length of the cilium 94. The piezoresistive strain
sensors 96 are located on the piece that is assembled (i.e., the vertical
cilium 94) using three-dimensional assembly.
[0094] When an external force is applied to the vertical cilium 94, either
through direct contact with another object (functioning as a tactile
sensor) or by the drag force from fluid flow (flow sensing), the beam
will deflect and cause the strain gauge 96 to stretch or compress. The
strain gauge region is treated as being rigidly attached to the substrate
72, while the cilium 94 is free. The magnitude of the induced strain (e)
is largest at the base, where the strain gauge is located, = M
.times. .times. t PI 2 .times. .times. EI ( 4 )
[0095] where M is the moment experienced at the base, t.sub.PI is the
polyimide thickness, and E and I are the modulus of elasticity of and the
moment of inertia of the polyimide. The very thin nichrome resistor of
the strain gauge 96 is not taken into account.
[0096] The vertical cilium preferably is surface micromachined and
deflected out of plane using magnetic 3D assembly, such as PDMA, and can
be conducted on a wafer scale. The vertical cilium 94 remains in
deflected position due to plastic deformation at the joint.
[0097] A preferred fabrication method includes a series of metallization
and polymer deposition steps. Referring to FIG. 13A, first, on a
substrate 100 a 0.5-.mu.m Al sacrificial layer 102 is evaporated and
patterned. Then, a 5.5-.mu.m photodefinable polyimide 104 (e.g., HD-4000
from HD Microsystems) is spun-on and patterned photolithographically. The
polyimide 104 is cured at 350.degree. C. in a 1 Torr N.sub.2 vacuum for 2
hours. Preferably, this is the highest temperature used in the process,
allowing the AHC to be fabricated on various substrates 100, including
polymer-based substrates.
[0098] Afterwards, a 750-.ANG.-thick NiCr layer 106 used for the strain
gauge 96 is deposited by electron beam evaporation. This is followed by a
0.5-.mu.m-thick Au/Cr evaporation 108 used for electrical leads 110 and
the bending hinge. The Au/Cr layer 108 is then used as a seed layer to
electroplate approximately 5 .mu.m of permalloy 112 before being removed
by lift-off. The resulting structure is shown in FIG. 13A. The final
surface micromachining step is another 2.7-.mu.m polyimide film (not
shown) to serve as a protective coating for the permalloy cilium and the
NiCr strain gauge.
[0099] The Al sacrificial layer 102 is then etched in a TMAH solution for
over a day to free the structure. The sample is then carefully rinsed and
placed in an electroplating bath 113, where an external magnetic field is
applied that interacts with the permalloy 112 to raise the vertical
cilium 94 out of plane.
[0100] For example, in a post-release Ni plating setup, shown by example
in FIG. 14, an external magnetic field 1.14 is applied with an
electromagnet 115 during the electroplating process. Preferably, the
entire process is done under a microscope. After a few minutes of
plating, the magnetic field 114 is removed and the cilium remains
permanently out of plane.
[0101] While the external field is being applied, Ni 116 is electroplated
on the Au hinge using a nickel anode 118, which rigidly fixes the
structure out-of-plane to the substrate and reinforces the ductile Au
hinge, as shown in FIG. 13B. The Ni electroplating is done on the
substrate globally, preferably lasting about 20 minutes to achieve a
thickness of approximately 10 mm. The actual thickness is difficult to
measure and control, but is not important as long as it is rigid relative
to the polyimide film.
[0102] SEM images of the hinge are shown in FIG. 15A-15B, showing the
difference between a deformed Au hinge with and without Ni plating. An
array of AHCs 92 with different vertical cilium and strain gauge geometry
is shown in FIG. 16, showing the parallel nature of the preferred
fabrication process. Again, it is preferred that overall, the fabrication
method does not exceed temperature over 3500 Celsius, allowing it to be
completed on a skin-like thin film polymer substrate on other substrates.
Silicon, glass, and Kapton film, for example, can be used as a substrate
for this process. The resistance of devices tested ranges from 1.2 kW to
3.2 kW, and TCR measurement of the as-deposited NiCr film in an exemplary
AHC has a value of -25 ppm/.degree. C., which is very small and should
not contribute to anemometric effects during airflow testing.
[0103] In an exemplary operation of the AHC 92, the resistance change due
to external displacement is shown in FIG. 17 for an 850 .mu.m tall
vertical cilium. A micromanipulator is used to deflect the distal end of
the vertical cilium. The resistance change is measured by a multimeter,
and is linear to the beam deflection. The gauge factor GF can be
calculated from the slope of the curve, GF = dR / R PI (
5 )
[0104] where dR/R is the percent resistance change, and e.sub.PI is the
calculated strain from a fixed-free beam (See Eq. (4)) undergoing a
deflection x. The plastically deformed hinge, after being plated with
approximately 10 .mu.m of Ni, is very rigid. The modulus of elasticity
for the nickel is approximately two orders of magnitude larger than
polyimide (200 Gpa versus 3.5 Gpa). Therefore, an assumption of a
fixed-free cantilever model should be valid. The measured gauge factor
for an exemplary strain gauge configuration is about 1.4, which is lower
than expected. This could be attributed to the strain gauge not being
located at the point of maximum strain.
[0105] Several fabricated AHCs were then tested as airflow transducers in
a wind tunnel. The airflow with velocity U impinging on the cilium
results in a drag force acting normal to the paddle, leading to a moment
on the strain gauge M = .intg. 0 I .times. C D .times. 1 2
.times. .rho. .times. .times. U 2 .times. wy .times. d y (
6 )
[0106] where CD is the drag coefficient, r is the density of air, w
and/are the width and length of the cilium. Because strain is
proportional to the applied moment, and resistance change is proportional
to strain, Equation (6) suggests a quadratic relationship between airflow
and resistance change. In addition, by systematically varying the height
and width of the cilium, the response can be tailored to different ranges
of air velocity. The polarity of resistance change is dependant on the
direction of the airflow.
[0107] The wind tunnel measurement of three AHCs with different cilia
geometry is plotted in FIG.18. The AHCs tested were fabricated on a
silicon substrate to allow wire bonding to the sample. The AHC with the
longest cilium length of 1500 .mu.m is the most sensitive, with dR/R
reaching 600 ppm at around 10 m/s. The device with the shortest cilium,
even with a greater width, does not have the 600 ppm resistance change
until 30 m/s. The sign of resistance change can be indicative of the
direction of air velocity. However, the response in various directions
does not seem to be symmetrical. This is because it is difficult for the
PDMA assembly process to orient the cilium at exactly 90.degree. to the
substrate. The characteristic lengths of individual MEMS devices range
from 1 .mu.m to 1 mm, although distributed Microsystems containing arrays
of devices could have larger overall sizes.
[0108] The artificial haircell, for example, may be used to realize other
sensing modalities, including but not limited to vibration sensing. By
varying the geometry and mass of the vertical cilium, the haircell can be
made more responsive to inertia forces created by vibration. For example,
a three-axis acceleration sensor may be provided, as shown by example in
FIG. 19.
[0109] Among other flow sensor components, the hot-wire sensor 76 uses an
electrical wire placed in the flow field. The wire is heated using ohmic
heating and the resistance of the wire (which is a function of
temperature) is monitored. Flow imparts forced convection on the wire to
induce cooling. The temperature of the wire indicates the flow speed.
[0110] Existing hot-wire sensors are all supplied as individual devices.
Their sizes are relatively large. Even micromachined hot-wire anemometers
are supplied as singular units. They cannot measure the distribution of
flow in a distributed field. By contrast, a hot-wire sensor can be made
using surface micromachining process and three-dimensional assembly
method. It can be made on polymer substrates with large two-dimensional
array formats. Examples of hot wire anemometers formed on a substrate and
fabrication methods for them are provided in J. Chen and C. Liu,
"Development and Characterization of Surface Micromachined, Out-of-Plane
Hot-Wire Anemometer," in Journal of Microelectomechanical Systems, Vol.
12, No. 6, December 2003, pp. 979-988, and in J. Chen, J. Zou, and C.
Liu, "A Surface Micromachined, Out-of-Plane Anemometer," in Proceedings
MEMS, Las Vegas, 2002, pp. 332-335, which are incorporated by reference
in its entirety herein. FIG. 20 shows a three-dimensional array of
hot-wire anemometers, which can be formed by selecting fabricating
individual anemometers and raising them out of plane.
[0111] Conventional pressure and shear stress sensors employ a membrane.
In the case of a pressure sensor, the diaphragm bends in response to
applied pressure difference. In the case of shear stress for measuring
fluid stress, the membrane supports a heated hot-wire element. Referring
to FIG. 10, the pressure sensor 78 may include, for example, an NiCr
strain gauge 120 disposed on a Parylene film 122 forming a raised
diaphragm for measuring deflection of the Parylene film in response to
pressure. The shear stress sensor 80 may include a raised Parylene
membrane with a heated hot-wire element such as a nickel thermoresistor
126 for measuring fluid stress.
[0112] According to another embodiment of the present invention, a
microfabrication sequence for a Parylene membrane, shown by example in
FIG. 21, with patterned metal on the membrane is provided, in which a
preferably polymer membrane diaphragm supports metal leads used for a
pressure sensor and for a shear stress sensor. The metal leads can be
used for both pressure sensing and shear sensing (temperature sensing).
The location preferably determines the principal use of a particular
metal lead. For example, the metal leads closer to the center of the
membrane may be better located for shear sensing, while the metal leads
closer to the edge of the membrane may be better located for pressure
sensing.
[0113] In an exemplary fabrication process, a photoresist layer is
deposited and patterned as a sacrificial layer to define a membrane
cavity. A layer of Parylene is deposited, preferably having a thickness
in the 0.2 to 5 .mu.m range. A metal thin film is deposited and patterned
to form a resistor that can respond to stress (piezoresistor). The gauge
factor of such resistors is typically approximately 1-5. Metals that can
be used include NiCr (nichrome), Pt, Au, Cu, Al, and others.
[0114] Another layer of Parylene is deposited on top of the metal thin
film, passivating the resistors and reducing or preventing damage by
environmental elements over the long run. The photoresist is removed
through spatially placed holes on or around the membrane. The cavity is
dried and sealed using one or more of a variety of methods. One exemplary
method to seal the cavity is to deposit another thin layer of Parylene.
The deposition process is performed at low pressure (e.g., 40 mtorr), and
the cavity is therefore sealed under low pressure.
[0115] In another embodiment of the present invention, exemplary methods
are provided for integrating silicon chips (containing signal processing
functions such as amplification, multiplexing, and analog-to-digital
conversion) with a polymer sensor chip (with tactile or flow sensing
components) and within the fabrication flow. FIG. 22 shows an overview of
a skin architecture showing a cluster of sensor nodes connected to a
local cluster processor.
[0116] A first method includes bonding a silicon chip, such as a
commercially obtained chip 130 (e.g., ADC chip with internal clock from
National Semiconductors) onto a polymer sensor skin 132. The chip may be,
for example, an application-specific IC chip. A schematic diagram of this
bonding approach is shown in FIG. 23A. In a preferred bonding process, a
blank slot 134 on the back surface of the sensor skin 132 is opened for
the microelectronic chip 130 to rest. A through-wafer electrical
interconnect 138 is provided so that the silicon chip 130 rests on the
backplane and not the front plane, where the chip may interface with
surface roughness. Chip-to-polymer metal bonding technology using low
melting temperature metal thin films provides flip-chip bonding.
[0117] The assembly is repeated across the skin 132 with additional
circuits that handle multiple clusters for a distributed system. FIG. 23A
shows an embedded sensor 139 and wiring 140 with an ASIC flip chip 130
bonded to backside vias 138 with solder bumps 142.
[0118] A second method, shown by example in FIG. 23B, includes thinning a
semiconductor wafer 144 that contains analog/digital electronics at the
top surface 146 to the point that the semiconductor wafer becomes
flexible and yet still maintains electronics functionalities. For
example, a chip having a small die size (e.g., less than 1 cm.sup.2) with
thickness on the order of 10-30 micrometers, may be used. An exemplary
thinned silicon wafer is shown in FIG. 24. The silicon dies flex with the
polymer substrate 132 and therefore preserve the mechanical flexibility.
As shown in FIG. 23B, thin dies may be flip-chip bonded to bonding sites
148 on polymer sensor skin 132. The chip-to-polymer electrical connection
may be achieved, for example, using low temperature metal reflow. The top
surface 146 can be further protected and mechanically enhanced using
conformal chemical vapor deposition of a plastic 150 such as Parylene,
which is stress free, relatively soft, and does not damage the
microelectronics or the sensor.
[0119] In a third method, shown by example in FIG. 23C and FIG. 25, both
circuit elements 152 and sensor elements 154 are built on a silicon wafer
156 first. The sensors 154 are preferably formed on the wafer 156 after
the circuit elements 152 are formed (step (a) in FIG. 25). This is
feasible since the sensor elements 154 preferably can be formed under low
processing temperatures. An exemplary method uses a silicon wafer 156
having preformed circuit elements, on which the sensor elements 154 are
formed. Such silicon wafers 156 may contain, for example, op-amps,
multiplexors, and/or A/D conversion functions.
[0120] Post-process steps are performed to build interconnect wires 158
(step (b)) and the tactile or flow sensor elements 154. Next, the
backside of the wafer 156 is patterned and etched (step (c)) to form
trenches 160. An elastomer precursor 162 is poured and cured (step (d)),
to encase resulting silicon islands 164 in a elastomer back-filled skin.
The front surface of the skin can be further protected, for example, by
depositing a protective layer such as Parylene using chemical vapor
deposition. These steps provide a flexible sensor chip 166, as shown
flexed at step (e).
[0121] While specific embodiments of the present invention have been shown
and described, it is to be understood that other modifications,
substitutions, and alternatives will be apparent to those of ordinary
skill in the art. Such modifications, substitutions, and alternatives can
be made without departing from the spirit and scope of the present
invention, which should be determined from the appended claims.
[0122] Various features of the invention are set forth in the appended
claims.
* * * * *