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AU2016292465B2 - Method and device for electrical force measurement by means of an insulating thin layer - Google Patents

Method and device for electrical force measurement by means of an insulating thin layer Download PDF

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Publication number
AU2016292465B2
AU2016292465B2 AU2016292465A AU2016292465A AU2016292465B2 AU 2016292465 B2 AU2016292465 B2 AU 2016292465B2 AU 2016292465 A AU2016292465 A AU 2016292465A AU 2016292465 A AU2016292465 A AU 2016292465A AU 2016292465 B2 AU2016292465 B2 AU 2016292465B2
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Prior art keywords
force
insulating film
thin insulating
measuring
metal
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AU2016292465A1 (en
Inventor
Jan Klemm
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Priority claimed from DE102015111425.9A external-priority patent/DE102015111425B4/en
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01LMEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
    • G01L1/00Measuring force or stress, in general
    • G01L1/20Measuring force or stress, in general by measuring variations in ohmic resistance of solid materials or of electrically-conductive fluids; by making use of electrokinetic cells, i.e. liquid-containing cells wherein an electrical potential is produced or varied upon the application of stress
    • G01L1/22Measuring force or stress, in general by measuring variations in ohmic resistance of solid materials or of electrically-conductive fluids; by making use of electrokinetic cells, i.e. liquid-containing cells wherein an electrical potential is produced or varied upon the application of stress using resistance strain gauges
    • G01L1/225Measuring circuits therefor
    • G01L1/2262Measuring circuits therefor involving simple electrical bridges
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01LMEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
    • G01L1/00Measuring force or stress, in general
    • G01L1/18Measuring force or stress, in general using properties of piezo-resistive materials, i.e. materials of which the ohmic resistance varies according to changes in magnitude or direction of force applied to the material
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01LMEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
    • G01L1/00Measuring force or stress, in general
    • G01L1/20Measuring force or stress, in general by measuring variations in ohmic resistance of solid materials or of electrically-conductive fluids; by making use of electrokinetic cells, i.e. liquid-containing cells wherein an electrical potential is produced or varied upon the application of stress
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01LMEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
    • G01L1/00Measuring force or stress, in general
    • G01L1/20Measuring force or stress, in general by measuring variations in ohmic resistance of solid materials or of electrically-conductive fluids; by making use of electrokinetic cells, i.e. liquid-containing cells wherein an electrical potential is produced or varied upon the application of stress
    • G01L1/22Measuring force or stress, in general by measuring variations in ohmic resistance of solid materials or of electrically-conductive fluids; by making use of electrokinetic cells, i.e. liquid-containing cells wherein an electrical potential is produced or varied upon the application of stress using resistance strain gauges
    • G01L1/2268Arrangements for correcting or for compensating unwanted effects
    • G01L1/2281Arrangements for correcting or for compensating unwanted effects for temperature variations
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01LMEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
    • G01L1/00Measuring force or stress, in general
    • G01L1/26Auxiliary measures taken, or devices used, in connection with the measurement of force, e.g. for preventing influence of transverse components of force, for preventing overload

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Force Measurement Appropriate To Specific Purposes (AREA)
  • Pressure Sensors (AREA)
  • Measurement Of Force In General (AREA)

Abstract

The invention relates to a device for electrically measuring a force (F) acting at least between two pressed-together metal electrodes (1) and metal electrode (3), characterised in that: the metal electrodes, made of hard metal, steel or low-resistance metal layers on ceramic, glass or plastic bodies with an electrical resistance in the region of a few milliohm to less than or equal to 10 ohm, and an average roughness depth R

Description

Device for Electrically Measuring a Force
The invention relates to a device for electrically measuring a
force built between at least two metal electrodes, wherein at
least one thin insulating film acts as a sensor element, the
electrical conductivity of which describes an unambiguous and
exactly traceable function of the acting force.
In general, the invention relates to the field of force
measurement technology, wherein a novel application variety is
achieved over the prior art by creating a simplified design of
the force sensors without deformation bodies. A configuration
feature used here is the application of at least one or more
homogeneous thin insulating films onto the planar or free-form
[5 surfaces of the mechanical force transmission elements,
whereby between the electrically insulated force transmission
elements and the metal electrodes a sensor design becomes
possible which, directly and without noteworthy deformation of
these elements, generates an electrical signal in the form of
a force-dependent change in voltage at a given current, the
signal describing the bijective, high-resolution and
continuous representation of the applied force on a direct
mechanical and electrical route.
This technology makes it possible to create sensors that have
high temperature stability, depending on the selected thin
insulating film, and a miniaturized design, which is to say in
an installation space of less than one cubic millimeter for
force measurement in the millinewton range, and furthermore in an arbitrarily large macro design in the newton to meganewton
range, wherein, depending on the measuring task, an arbitrary
geometric configuration of the mechanical force transmission
elements comprising applied thin insulating films a free selection with regard to installation space, force application direction and mechanical amplification ratios is achieved.
For example, as a result of being able to freely select the
cone slope of the inner and outer truncated cones, to the
outer cone lateral surface of which a thin insulating layer
was applied, free design selection of the measuring
sensitivity to be achieved is made possible, wherein tension
or compression sensor becomes possible, depending on the
geometric configuration. An additional degree of freedom in
the mechanical and electrical configuration of the force
sensors is the material selection, the design and the chemical
composition of the thin insulating film, or of the layer
system, applied to the force transmission elements, wherein
[5 the temperature stability and the measuring sensitivity of the
thin insulating film can be freely selected depending on the
requirements of the measuring task. Additionally, it becomes
possible to configure miniaturized and larger combinations of
multiple force sensors by way of thin insulating films in the
design of a combined sensor unit, for example so as to detect,
without interactions, the action of the force and the
direction of the force with respect to the 3 spatial
dimensions of width (x component), length (y component) and
depth (z component) in the space.
In general, the piezoresistive effect is sufficiently known
from the related art and first publications that became known
as early as 1920. The piezoresistive effect describes a change
in the electrical resistance of a material as a result of the application of a high external force or pressure. This effect
occurs in all materials that are moderately to highly
electrically conducting; however, compared to metals the
pressure sensitivity of semiconductors is several times greater. In principle, it should be noted that this pressure sensitivity based on the change in resistance due to the application of an external force can be increased in semiconductors by deliberately adapting the orientation of the monocrystal, which means the direction of flow of the electrical current, and the doping with impurity atoms in the carrier material.
The piezoresistive effect can also be observed on the example
of amorphous carbon layers having a diamond-like lattice
structure, as is described in patent DE 199 54 164 B4, wherein
it should be noted that it is not only possible to influence
the intensity of the piezoresistive effect in amorphous carbon
layers by way of a specific chemical composition and
[5 configuration of the lattice structure, but great
intensification of the piezoresistive effect is likewise
achieved with other thin films or multilayer systems, such as
aluminum-titanium-nitrite, aluminum-chromium-nitrite,
zirconium-oxide-nitrite or aluminum-chromium-nitrite-oxide,
and many others, by integrating impurity atoms or molecule
structures as grains in a nanocomposite carrier layer. This
means that the sensitivity of the change in electrical
resistance with respect to the degree of the force or pressure
mechanically applied from the outside is drastically increased
since, depending on the material combination and introduced
impurities, additional charge carriers in the form of ions
and/or electrons are released in the semiconductors as a
function of the pressure. This effect has been known since
1920; however, technical progress and continued development regarding the use and production of layer systems has yielded
novel material combinations and layer systems that, on the one
hand, can be applied to a wide variety of materials, such as
metal, ceramic, glass or plastic surfaces, and, on the other hand, have a material composition that comes very close to semiconductors with respect to the electrical properties.
Such piezoresistive layers, however, exhibit very strong temperature-dependent drift of the resistance, which as a
relative temperature-dependent change in resistance is in a
range of -0.4 percent to approximately -1.2 percent per kelvin
increase in temperature, which has likewise been described in
the related art. Such layers and structures, for example,
allow discrete electronic components and circuits to be
configured on planar carrier materials, for example glass,
such as are used in the production of modern flat screen
monitors. Surfaces thus coated are also characterized by
extreme mechanical strength exceeding that of hard metals,
[5 having compressive strength of more than 2 gigapascals and
temperature stability in the range of minus 100 degrees
Celsius up to 1200 degrees Celsius, depending on the selection
of the carrier body and the applied layer system.
DE 10 2010 024 808 Al describes a sensor design comprising a
piezoresistive thin carbon film having a structured
arrangement and measurement electronics. Only carbon (diamond
like carbon, DLC) layers are used. Such layers have very low
resistance. The piezoelectric functional layer is structured,
resulting in high manufacturing complexity for creating the
force entry surfaces. Additionally, the functional layer made
of DLC is coated with a wear protection layer, which can cause
electrical disturbance variables in the measuring system.
US 2003/0164047 Al describes a load sensor comprising a load
detecting element and a temperature compensating element,
wherein these two elements are made of the same material and
have the same dimensions.
DE 102 53 178 Al describes the use of a layer made of diamond
like carbon as a temperature sensor, which is preferably used
in areas of machines subject to tribology. Furthermore, the
option of simultaneously measuring pressure and temperature at
different locations of layer regions is mentioned.
List of Appendices
FIG. 1: shows a sectional illustration of the thin insulating
film load cell comprising a thin reference insulating
film for temperature compensation, serving as an
electrical half measuring bridge;
FIG. 2: shows a sectional illustration of the thin insulating
film load cell comprising a thin reference film for
temperature compensation for resistance measurement;
FIG. 3: shows a sectional illustration of the thin insulating
film load cell comprising a thin reference insulating
film for temperature compensation in a double design,
serving as a highly sensitive full measuring bridge;
FIG. 4: shows a sectional illustration of the thin insulating
film load cell for simultaneously detecting two force
directions F x and Fy comprising a thin reference
insulating film for temperature compensation for
electrical multi-channel resistance measurement;
FIG. 5: shows the composition and measuring circuit of an N
dimensional thin insulating film force sensor
comprising an n-fold measuring circuit having a multi-channel thin reference insulating film for temperature compensation; top - sectional illustration of a 2D insulating film sensor segment; bottom - rotational segment arrangement as an exemplary embodiment comprising n=4 times 2D sensor blocks and 4x2=8 measuring channels so as to measure the direction of the force and the magnitude thereof in a component-based manner;
Legend:
El-i and El-2: electrode pair Fy+Fx rotation angle
0°; E2-1 and E2-2: electrode pair Fy+Fx rotation angle
450;
E3-1 and E3-2: electrode pair Fy+Fx rotation angle
900;
E4-1 and E4-2: electrode pair Fy+Fx rotation angle
135°;
FIG. 6: shows a force-resistance characteristic curve of the
thin insulating film measuring cell, comprising an
uncoated hard metal electrode and a type_01 coated
hard metal electrode;
FIG. 7: shows a force-resistance characteristic curve of the
thin insulating film measuring cell, comprising an
uncoated hard metal electrode and a type_03 coated
hard metal electrode;
FIG. 8: shows a force-resistance characteristic curve of the
thin insulating film measuring cell, comprising an
uncoated hard metal electrode and a type_01 coated
hard metal electrode;
FIG. 9: shows a force-resistance characteristic curve of the
thin insulating film measuring cell, comprising two
uncoated hard metal electrodes, which is to say the resistance between the contact surfaces is in the
lower milliohm range at +/- 1 mOhm;
FIG. 10: shows a force-resistance characteristic curve of the
thin insulating film measuring cell, comprising two
uncoated hard metal electrodes, which is to say the
resistance between the contact surfaces is in the
lower milliohm range at +/- 1 mOhm;
FIG. 11: shows a force-resistance characteristic curve of the
[5 thin insulating film measuring cell, comprising two
coated hard metal electrodes having different
roughness levels [SiC_05 polished on SiC_03
unpolished]; and
FIG. 12: shows a force-resistance characteristic curve of the
thin insulating film measuring cell, comprising two
coated hard metal electrodes having different
roughness levels [SiC_05 polished on SiC_03
unpolished].
The invention relates, in general, to a device for
electrically measuring a force F, which acts at least between
two compressed metal electrodes 1 and a metal electrode 3. The
metal electrodes are made of hard metal, steel or low
resistance metal layers on ceramic, glass or plastic bodies
having electrical resistance in the range of a few milliohms
to less than or equal to ten ohms, and having a mean roughness
value Ra of less than or equal to 400 nanometers, and have
force-independent conductivity on the contact surfaces. The
force acts directly on a thin insulating film 2 or a thin
multi-layer insulating film 2 disposed between a metal
electrode 1 and a metal electrode 3 in a form-locked manner,
which is made of zinc oxide or stochastically reduced aluminum
oxide Al 2 0x, where x=2.4 to x=2.8, or silicon carbide or a DLC
(diamond-like carbon) layer, under the slightest relative
deformation in the range of smaller than or equal to 0.1h of
the metal electrode 1 and the metal electrode 3. Due to the
identical thin insulating film 2 or the thin multi-layer
insulating film 2 exhibiting exactly the same physical
behavior, a reference metal electrode 4, which is disposed
independently of the flow of the force to be measured and
fixed under the constant holding force of a fastening element
5, acts electrically on the metal electrode 3, so that this
reference resistance of the thin insulating film between the
metal electrode 3 and the metal electrode 4 is applied under a
constant pressing force for complete temperature compensation
of the measuring system as a half bridge or a full bridge, in
that a defined current of a high-precision power source 6
flows on the current path in a series connection via the metal
electrode 1 across the thin insulating film 2 to the metal
electrode 3 across the thin insulating film 2 to the metal
electrode 4, so that a force-dependent voltage 8 drops across
the thin insulating film between the metal electrode 1 and the metal electrode 3, and a reference voltage 9 drops between the metal electrode 3 and the metal electrode 4 of a thin reference insulating film 2, the voltage ratio thereof being temperature-independent, wherein the resulting bridge voltage of the measuring bridge or the directly measured voltage ratio defines a continuous, high-resolution and exactly describable and repeatable function of the acting force, regardless of the operating temperature of the device for electrically measuring a force, wherein the temperature-compensated voltage ratio or the measured bridge voltage is directly supplied to a signal processing and evaluation unit via an electrical connection, whereby an electrically decoupled and mechanically robust design of the force measuring device according to the invention is achieved. A geometry of the metal electrodes 1, 2
[5 and 3 can be freely selected in the form of planar surfaces or
free-form surfaces.
One embodiment of the device is characterized in that, during
the creation of the contact surfaces of the at least two metal
electrodes having a mean surface roughness Ra of less than or
equal to 400 nanometers, a form fit in the range of less than
4 micrometers across the entire contact surface is achieved,
whereby the electrical resistance between the contact surfaces
of the at least two or more metal electrodes 1, metal
electrodes 3 and metal electrodes 4 without thin insulating
film, which are produced, for example, from hard metal or
high-strength steel, or by way of metal injection molding, or
low-resistance metal layers on ceramic, glass or plastic
bodies having electrical resistance in the range of less than a few milliohms to less than or equal to ten ohms, regardless
of the applied force at which these metal bodies are pressed
together, remains constant within the tolerance range of
plus/minus 3 milliohms and, depending on the material used and the surface area of the contact surface, is established in the range between 20 milliohms and no more than 160 milliohms, whereby the metrological condition is created that only the thin insulating film 2 detects a force-dependent change in resistance.
One embodiment of the device is characterized in that the thin
insulating film 2 is applied to hard metal electrodes, steel
electrodes or metal layer electrodes on ceramic, glass or
plastic bodies having electrical resistance in the range of
less than a few milliohms to less than or equal to ten ohms,
so that the electrode base body of the metal electrode 1,
metal electrode 3 and metal electrode 4 has at least the same
strength as, or greater strength than, the thin insulating
[5 film 2, whereby deformation and damage of the thin insulating
film in relation to the carrier material due to pressing or
flaking is avoided, and the measuring system are not deformed
by the application of the force, or to an extremely small
degree, which is to say a relative deformation of less than
0.1o, so that the entire force measuring system operates
without displacement due to deformations of the mechanical
metal electrodes 1, the metal electrodes 3 and the metal
electrodes 4, and the application of the force on the thin
insulating film is thus converted into a direct change in
resistance, which is an unambiguous, high-resolution and
continuous function of the force.
One embodiment of the device is characterized in that the
mechanical transmission elements, serving as metal electrodes 1, metal electrodes 3 and metal electrodes 4 for passing on
the force between the outer force application site to the thin
insulating film 2 of the force measuring device and the thin
reference insulating film 2, which is disposed between the metal electrodes 3 and metal electrodes 4, are made of high strength steels or hard metals, by way of metal injection molding, ceramic or glass materials, having special high strength layers or layer systems applied, which are made of silicon carbide, DLC (diamond-like carbon), zinc oxide or stochastically reduced aluminum oxide Al 20x having an oxygen ratio of x equal to or greater than 2.4 to 2.8, whereby very high mechanical and chemical robustness, dimensional stability and freedom from wear of the elements of the measuring cell, comprising the metal electrodes 1, the metal electrodes 3 and the metal electrodes 4 and the thin insulating layer 2, is achieved, and this measuring cell withstands thermal loading of the thin insulating film 2 and the electrical contact with the electronic measurement evaluation circuit of the
[5 components (6, 7 to 17) in the vicinity of the measuring
device at a spatial distance of less than or equal to 200
millimeters, so that the measuring system is operated in the
temperature range of less than -80°C to +3000C, wherein far in
excess of one hundred thousand operating cycles do not result
in any change of the unambiguous force-resistance function of
the thin insulating film 2 or the thin multi-layer insulating
film 2.
One embodiment of the device is characterized in that the load
cell, comprising the metal electrodes 1, the metal electrodes
3 and the metal electrodes 4 and at least one thin insulating
film 2, are implemented as high-temperature applications in
the temperature range of -80°C to +11000C, and up to +12000C
in isolated cases, by using a temperature-resistant electrical connection between the thin insulating film 2 and the
electronic evaluation unit of the components (6, 7 to 17),
wherein the metallic conductor and insulator and the contact
surfaces of the connection system are temperature-resistant up to 12000C, having line lengths of greater than 20 millimeters up to 5 meters, due to the specific selection of the insulating film system 2 [SiC, Al 2 0,, ZnO].
One embodiment of the device, which is configured in a
miniaturized and compact design for electrically measuring a
force F in the millinewton to meganewton range, is
characterized in that a composition of the force measuring
system that is very robust and tolerates dynamic loads is
achieved as a result of the mechanical design of the metal
electrodes 1 the metal electrodes 3 and the metal electrodes
4, wherein the mean roughness value Ra of the metal electrode
contact surfaces 1 and the metal electrode contact surfaces 4
at a ratio of 30:1 to 2:1 are rougher compared to the mean
[5 roughness of the metal electrodes 3 of Ra equal to or less
than 200 nanometers, whereby the increase in the continuous
force-resistance characteristic curve of the measuring cell is
deliberately defined in an application-specific manner in that
a roughness ratio of 1:1 of the electrodes produces a
significantly lower increase in the force-resistance
characteristic curve compared to a higher ratio of X:1, where
X = 1.5 to 30.0, which causes a significantly steeper increase
in the force-resistance characteristic curve. Furthermore, the
metal electrode contact surface is configured as a shaped
part, wherein planar surfaces or free-form surfaces are used,
having defined surface roughness, which increases the adhesion
of the high-strength coatings on the force transmission
surfaces, whereby a strength of the thin insulating film 2 or
of the thin multi-layer insulating film 2 and of the base bodies of the metal electrode 1, the metal electrode 3 and the
metal electrode 4 the pressure load-bearing capacity of hard
metals of up to 2 gigapascals or of high-strength steels of up
to 1.2 gigapascal is achieved. Due to the selection the production method of the thin insulating film 2 in terms of the material selection and material treatment using available coating techniques, specific resistance characteristic values or working ranges of the force-dependent insulating behavior in the milliohm, ohm to several hundred kiloohm range are established, which in a smaller design having an installation space of a few cubic millimeters operate for the millinewton range, in an average size in the range up to one hundred cubic centimeters operate in the newton to kilonewton range, and in a large design below one cubic meter operate in the meganewton range.
One embodiment of the device is characterized in that the
measuring device of the elements (1, 2, 3 to 17) is
[5 electrically operated in the form of a half or full measuring
bridge by combining multiple thin insulating films 2 or thin
multi-layer insulating films 2, so that the measuring
sensitivity is increased several times over specifically by
the electrical interconnection. As a result of one or more
respective reference metal electrodes 4 per load cell, the
temperature-related resistance deviation is entirely
compensated for. Furthermore, a spatial arrangement of the one
measuring cell combination, comprising metal electrodes 1 and
metal electrodes 3, thin insulating films 2 and reference
metal electrodes 4, in the direction of the force application
to be measured, and a second spatial arrangement of the
elements (1, 2, 3 and 4) of the second measuring cell
combination in the direction of the interfering force
component, which is caused as a mechanically superimposed oscillation in the system, for example, make it possible to
operate a half or full measuring bridge as an electrical
differential connection, whereby disturbing signals can be deliberately reduced, or entirely compensated for, by parasitic mechanical oscillations.
One embodiment of the device is characterized in that the measuring device is electrically operated as a multiple series
connection of multiple measuring channels by way of one or
more half or full measuring bridges by combining multiple thin
insulating films (2.1 corresponds to channel one, and 2.2
corresponds to channel two) or thin multi-layer insulating
films (2.1, 2.2 to 2.n), the spatial or geometric arrangement
of the bridges being designed in such a way that the magnitude
and direction of the forces to be measured can be exactly and
simultaneously determined as a vector quantity for each
associated measuring channel by separately detecting the force
[5 application as vector components in the at least three spatial
dimensions of the Cartesian coordinate system, having a width
X, length-Y, and height-Z, and/or additionally in the polar
coordinate system of the rotational axis about the normal
vector of the X-Y plane, the Z axis and a further rotational
axis, which bijectively describe the angle of inclination with
respect to the X-Y plane.
One embodiment of the device is characterized in that both
simple and complex mechanical designs of the elements, these
being the metal electrodes 1, the thin insulating films 2, the
metal electrodes 3 and the reference metal electrodes 4, are
created as the electrical force measuring device, which by way
of the thin insulating films 2 are composed as a combination
of one or more electrical force measuring devices, comprising single layers (2) or multiple layers (2 or 2.n) applied to a
few shaped parts as planar or free-form surfaces, in a macro
design, which is to say in the range of greater than 10 mm, as
well as as a miniaturization in a micro design, which is to say in the sub-millimeter range, wherein multiple metal and/or ceramic and/or glass components are disposed in a force-fit or form-locked manner and detect moments as well as forces in a temperature-compensated manner, wherein, as a result of the application of high-resistance insulating layers in the megaohm range, these components are operated as metal electrodes 1, 3 and 4 in a manner that is electrically insulated with high resistance with respect to the external environment and sufficiently electrically insulated with respect to one another, and mechanically as well as electrically decoupled from one another without interactions.
One embodiment of the device is characterized in that the
establishment of the measuring sensitivity of the electrical
[5 force measuring device is defined with respect to the force
measuring range in the millinewton to meganewton range, and
that furthermore the direction of force is predefined by the
geometric configuration of the metal electrodes 1, the metal
electrodes 3 and the reference metal electrodes 4, in that
these are designed and manufactured as insertable bodies
having freely selectable ruled geometries as positive and
negative shapes, the dimensional deviation of which is smaller
than or equal to 6 micrometers at a mean roughness value of
the electrode contact surface of Ra smaller than or equal to
400 nanometers, for example as an inside truncated cone and an
outside truncated cone of lateral surfaces having the same
shape for measuring tensile or compressive forces, having the
thin insulating film 2 applied to the lateral surface, wherein
the cone angle, and thus the mechanical multiplication ratio of the compression or tension measuring cell, can be freely
selected. Furthermore, as a result of cylinder surfaces,
inserted into one another, of the outer cylinder and inner
cylinder having thin insulating films applied to the cylinder lateral surface, it is achieved that the radial tension force is detected, and thus the radial and axial force transmission capacity of shrink joints between cylindrical tensioning systems is measured directly, wherein this is linearly detected as a force acting between two bodies. In a further exemplary embodiment, it is possible, for the design freedom in terms of the configuration of this measuring system, to directly measure axial tensile or compressive forces with the aid of stepped cylinders, wherein the thin insulating film 2 of the two or more shaped parts is applied to the end face of the cylinder rings, and thus the axially acting tensile or compressive force of the pressed-on shaped parts is directly linearly detected in a linear manner, and likewise the direct measurement of torque is made possible in that, due to a
[5 planar bearing surface between the metal electrodes 1 and the
metal electrodes 3 and the interposed thin insulating film 2,
having a normal vector pointing tangentially to the direction
of rotation, of the mutually engaging, rotationally
symmetrical shaped parts, wherein the thin insulating film is
applied to a planar surface or free-form surface of a shaft,
the normal vector of which points in the direction of the
force to be measured acting on the cylinder circumference of
the two bodies as a rotation.
One embodiment of the device is characterized in that the
metal electrodes are electrically insulated from one another
by one or more thin insulating layers (2 or 2.n) and,
mechanically, they are designed as a ruled geometry or free
form geometry in such a way that at least two-channel or multi-channel simultaneous measurement of compressive and
tensile forces is possible by applying the thin insulating
film to the circumferential surface of two mutually connected
truncated cones on the outer surface of the respective inner electrode, which are mounted respect to the precisely fitting casing, which is to say with a surface roughness having a mean roughness value of less than 400 nanometers and dimensional tolerance of less than 6 micrometers, as two outer electrodes that are electrically insulated from one another as a negative shape, wherein no deformation or an extremely small relative deformation of less than 0.01% takes place of the metal electrodes 1, the metal electrodes 3 and the reference metal electrodes 4, which are made of hard metal for example, and the thin insulating film 2 on the truncated cone having a tip in the direction of the force application measures a compressive force, and the truncated cone having the tip counter to the force application measures the tensile force, and this electrical force measuring device thus simultaneously
[5 allows a force measurement in opposite force directions as
positively and negatively acting forces.
During the electrical measurement of a force by way of the
thin insulating layer 2 using the above-described device, an
electronic precision signal generator is used as the power
source 6, which operates either in the operating mode of a
regulated direct current source or furthermore in the
operating mode of an alternating current signal source, so
that clearly defined output current signals, usable as an
exact reference, in the form of sinusoidal, square wave or
triangular signals, for example, are supplied, with freely
selectable amplitudes and frequencies of the resistance
measuring circuit. Furthermore, a signal processing and
evaluation circuit is matched to the respective operating mode so that, depending on the application, electrical disturbance
variables from the surrounding environment, which is to say
strong electrical or electromagnetic fields, are deliberately
suppressed or compensated by way of signal filtering using a band pass filter or a band stop filter, having cut-off frequencies that are designed with the specific application in mind. Likewise, a reduction in the energy consumption of such a measuring system by more than 2 to 4 powers of ten is achieved in pulse/no pulse mode.
The dynamics of the thin film force measuring system,
comprising the metal electrodes 1, the thin insulating films
2, the metal electrodes 3 and the reference metal electrodes
4, or of the combination of electrical force measuring devices
by way of thin insulating films of the elements (1, 2, 3 and
4), supplies a temporal resolution in the megahertz range of
force curves that takes place exclusively as a result of the
design of the thin insulating films 2 and the thin reference
[5 films 4 as low-resistance measuring resistors in the range of
less than or equal to one hundred ohms to one ohm. In this
way, the increase in the measuring currents, and in particular
the edge steepness of the detected measuring voltage, which is
detected as a voltage drop across the thin insulating film
resistor and achieved in the lower microsecond to ten
nanosecond range. The measurement electronics is electrically
adapted to detect the voltage drops across the thin insulating
films (2 or 2n) with a resolution to no less than the three
digit microvolt range at a time delay of less than eight
hundred nanoseconds, so that the performance capability of the
entire measuring system with respect to the time response and
sensitivity is determined exclusively by this adaptation, and
thus temporal high-resolution and deformation-free force
measurement is made possible, which is carried out on bearing shells of turbines or high-voltage generators, for example.
The mechanical transmission elements for passing on the force
to the metal electrodes 1, the metal electrodes 3 and the reference metal electrodes between the outer force application site to the thin insulating film 2 are made of strong plastic materials or high-strength composite materials in the form of shaped parts, wherein the electrical force measuring system is created on the carrier material of the electrode base bodies made of plastic material or composite material of the metal electrodes (1, 3 and 4) as a result of the application of high-strength metal layers as the electrically conducting metal electrode of the elements (1, 3 and 4), the application of the thin insulating films (2 and 2.n) onto these metal electrodes (1, 3 and 4), and furthermore as a low-resistance electrical contact of these electrodes with the electronic measuring system in the resistance range of less than fifty milliohms of the elements (6, 7, to 17).
The metal electrodes 1, the metal electrodes 3 and the metal
electrodes 4 are electrically insulated from one another by a
thin insulating film 2, so that the capacitance and/or the
resistance of this electrical measuring cell, comprising the
elements (1, 2, 3 to 17), represents an unambiguous and
continuous function of the applied pressure force acting on
the measuring cell from the outside, wherein, for the purpose
of electrically measuring the force-dependent capacitance C or
the impedance Z, an electronic precision signal generator,
which operates in the operating mode of a regulated
alternating current signal source, is used as the power
source, so that clearly defined output current signals, usable
as an exact reference, in the form of sinusoidal, square wave
or triangular signals, for example, are supplied, with freely selectable amplitudes and frequencies of the capacitance or
impedance measuring circuit, and these, serving as an
oscillating circuit, provide excitation at the resonant
frequency, wherein the oscillating circuit is detuned as a result of the force acting between the metal electrodes (1, 3 and 4) due to a change in capacitance and/or impedance, and likewise the amplitude of the alternating current measuring signal drops across the capacitive-resistive resistance of the thin insulating film 2, the curve of which describes a bijective and continuous function with respect to the applied pressure force, and the electronic signal processing and evaluation circuit, by way of application-specific band stop filters or band pass filters, achieves almost complete suppression or compensation of disturbance signals as a result of parasitic mechanical oscillations or electrical fields from the surrounding environment.
The metal electrodes 1, the metal electrodes 3 and the metal
[5 electrodes 4 are electrically insulated from one another by a
thin insulating film 2, so that the impedance Z, which is to
say the inductive AC resistance or capacitive AC resistance,
of this electrical measuring cell represents an unambiguous
and continuous function of the applied pressing force acting
on the measuring cell from the outside, wherein, for the
purpose of electrically measuring the force-dependent
inductance L or capacitance C, an electronic precision signal
generator, which operates in the operating mode of a regulated
alternating current signal source, is used as the power
source, so that clearly defined output current signals, usable
as an exact reference, in the form of sinusoidal, square wave
or triangular signals, for example, are supplied, with freely
selectable amplitudes and frequencies of the capacitance or
inductance measuring circuit, and these, serving as an oscillating circuit, provide excitation at the resonant
frequency.
According to the invention, the measurement of forces is
achieved, as shown as exemplary embodiments in FIG. 1, FIG. 2
and FIG. 3, in that an insulating thin film (2) is applied
between at least two mechanical force transmission elements (1
and 3), which are designed as electrodes electrically
insulated from one another, the electrical resistance of the
thin insulating film being a clearly traceable function of the
acting force F, and furthermore a reference metal electrode
(4) is disposed in the vicinity outside the power flow, the
mounting of which fixes this electrode (4) at a constant
retaining force with respect to the source electrode (3).
In this way, a half or full measuring bridge can be created,
which fully compensates for the temperature dependence of the
[5 measuring system, whereby the resulting bridge voltage
describes a bijectively traceable function of the force
application between the electrodes (1 and 3), regardless of
the ambient temperature. For this purpose, the at least two
electrodes (1 and 3), or the shared source electrode (Eq or 3
), and the adjoining sensor electrodes (En) thereof, are
electrically connected to the power source (6), so that the
given and known current Iq of the regulated power source (6),
which is measured as a current I by way of an ammeter (7),
resulting in a voltage drop U or U n across the thin
insulating film on the multidimensional sensor, which is
measured in a high-resolution manner by way of a voltmeter (8)
and transferred as a bridge voltage with respect to one or
more reference measuring electrodes (4 or U.ref(n)) using a
half or full measuring bridge, whereby complete compensation of the temperature dependence of the thin insulating film
resistance or of the measuring system is achieved.
In opposition to previously known solutions of force measuring
sensors and, among other things, with respect to patents DE
199 54 164 B4 and DE 10 2006 019 942 Al, it should be cited
that:
• none of the force measuring systems based on piezoresistive
thin insulating film systems described in the prior art
comprises a device for fully and with high precision
compensating for temperature-dependent drift of the
insulation resistance;
• a wide variety of thin insulating films and multi-layer
systems having semiconductor behavior are employed, wherein
the sensitivity thereof with respect to the force-dependent
electrical conductivity or electrical resistance
deliberately by way of specific manufacturing methods,
[5 chemical substance combinations and the introduction of
impurities releasing additional electrical charge carriers,
which considerably increase the force-dependent
piezoresistive effect. Examples of such thin insulating
films or thin insulating film combinations are aluminum
titanium-nitrite, aluminum-chromium-nitrite, zirconium
oxide-nitrite or aluminum-chromium-nitrite-oxide, and many
others, which, serving as semiconductors, exhibit strong
sensitivity to the force-dependent change in resistance;
with respect to geometry and material selection, the
mechanical force transmission elements are configured in
such a way that no change in geometry or negligible
deformation of the mechanical force transmission elements
takes place, and thus a force measurement is directly
converted into an electrically measurable signal without travel or displacement errors, which is to say the thin
insulating film is the only sensor coupling member, and no
other component tolerances and mechanical disturbances enter
the measuring chain; furthermore, for example in the sensor design comprising hard metal force transmission elements serving as the electrodes (1 and 3), electrically exactly defined contact resistances are achieved between the interfaces of the metal electrodes (1 and 3), the contact resistance of which in the milliohm range is exactly constant, regardless of the applied force under which these elements are pressed together;
• the arbitrary, even miniaturized, design of the force
measuring sensors or force measuring sensor combinations,
serving as a multidimensional force measuring unit, makes an
extremely rapid, high-resolution measuring unit possible,
wherein the physical boundaries of this system are solely
electrically limited by the charge/discharge times of the
[5 measuring currents or changes in voltage of the measuring
circuit to the analog-to-digital converter. Modern
electronic signal amplification and processing circuits open
up an unprecedented performance level in dynamic force
measurement;
depending on the selected thin insulating film or thin
multi-layer insulating film system and the material
composition thereof and accordingly robust force
transmission elements, unprecedented temperature stability
of such sensors in the range of less than one hundred
degrees Celsius to 1200 degrees Celsius becomes possible;
• energy-saving applications and very cost-effective
miniaturized force measuring systems, operated by battery
over many years, become possible since the measuring
currents can be switched only briefly in active sleep mode with extremely long sleep phases, wherein very short
settling phases of the measurement system enable a very
short active duration; the mechanical robustness and wear resistance of the thin insulating film exceeds the load limit of the mechanical coupling elements, for example 2 gigapascals of compressive strength for hard metal.
The option to implement multifaceted configurations, combined
with the very high degree of freedom regarding
miniaturization, normal sizes for mechanical standard
elements, for example connecting elements such as bolts,
screws, thrust washers and the like, all the way to
applications in heavy equipment construction, is possible as a
result of this measuring technology using thin insulating
films.
[5 The exemplary embodiment at the bottom of FIG. 4 shows a
sectional illustration of the force measurement in one
direction, and that at the top of FIG. 4 shows the component
based force measurement in two directions, which is to say in
the two-dimensional space (2D) with the force components F x
and Fy.
The further exemplary embodiment according to FIG. 5 shows a
multi-dimensional sensor design by way of example, wherein
electrical force measurement takes place in a component-based
manner in the two times four dimensional space from 4
different rotation angles in the 3D space (Fx + Fy). This
electrical measuring circuit and the selected sensor design
are shown in the form of a sectional illustration, wherein an
arbitrary number of rotationally added (n-) sensor elements can be assembled; however, in the specific example here, n=4
separate units are determined for 4 rotation angles and are
intended to show the freedom of design with respect to the mechanical design and electronic evaluation options by way of example.
Description of legend
(1) electrode or shared electrode in the case of multidimensional measuring cells
(2) thin insulating film (2-n or 2.n in the case of a multidimensional design), which is to say nth thin insulating film
(3) electrode or nth electrode in the case of multidimensional sensors (3-n or 3.n in the case of a multidimensional design)
(4) reference metal electrode or nth electrode in the case of multidimensional sensors (4-n or 4.n in the case of a multidimensional design)
(5) mounting for reference metal electrode, which with a
[5 constant retaining force fixes the reference metal electrode at a constant retaining force from the two opposite directions
(6) power source I_q
(7) ammeter I or, in the case of a multidimensional design, nth ammeter of the respective force component (direction) and the associated nth current measuring channel
(8) voltmeter U or U n or, in the case of a multidimensional design, nth voltmeter of the respective force component (direction) and the associated nth voltage measuring channel (8-n or 8.n in the case of a multidimensional design)
(9) reference voltmeter U ref or U ref-m or, in the case of a multidimensional design, mth voltmeter of the respective force component (direction) and the associated mth reference voltage measuring channel (9-m or 9.m in the case of a multidimensional design)
(9) reference ammeter I ref or I ref-m or, in the case of a
multidimensional design, mth reference ammeter of the
respective force component (direction) and the associated
mth reference current measuring channel (9-m or 9.m in
the case of a multidimensional design)
(11) fixed resistance R_1 = constant of the half measuring
bridge
(12) fixed resistance R_2 = constant of the half measuring
bridge
(13) insulating film resistance R_1 of the full measuring
bridge
(14) insulating reference resistance R ref-1 of the full
[5 measuring bridge
(15) insulating resistance R_2 of the full measuring bridge
(16) insulating reference resistance R ref-2 of the full
measuring bridge
(17) insulating film resistance R_17 between the two measuring
cells placed on top of one another to make the full
measuring bridge possible [R_ >= 500 * R_1 ]
EDITORIAL NOTE
Patent No. 2016292465 Please notionally renumber claims pages as 28 to 32
Claims - PCT Article 34
1. A device for electrically measuring a force (F) comprising:
- a load cell comprising
o a first metal electrode (1) and a second metal
electrode (3) disposed opposite thereof in the
direction of the force (F) to be measured, each
being made of hard metal, steel or low-resistance
metal layers on ceramic, glass or or plastic bodies
and having contact surfaces by way of which the
force (F) to be measured can be impressed, and
having electrical resistance in the range of a few
milliohms to less than or equal to ten ohms and a
mean roughness value (Ra) of less than or equal to
400 nanometers, for forming force-independent
[5 conductivity,
o a thin insulating film (2), which is disposed between
the metal electrodes (1, 3) in a form-locked manner
and made of a material selected from the group
consisting of:
• zinc oxide,
• stochastically reduced aluminum oxide Al 2 0
where x = 2.4 to 2.8,
• silicon carbide,
• a DLC layer (diamond-like carbon),
o a reference metal electrode (4), which is disposed on
a section of the thin insulating film (2) in a
manner that is force-decoupled from the first metal
electrode (1) and tensioned with respect to the
second metal electrode (3) at a constant retaining
force by a fastening element (5);
a measuring circuit designed as a half bridge or a full
bridge, wherein
" a current path fed from a power source (6) in a
series connection runs across the first metal
electrode (1), the thin insulating layer (2) to the
second metal electrode (3), and onward across the
thin insulating layer (2) to the reference metal
electrode (4),
o a force-dependent voltage (8) is tapped between the
first metal electrode (1) and the second metal
electrode (3), the voltage dropping across the thin
insulating film (2),
o a reference voltage (9) is tapped between the second
metal electrode (3) and the reference metal
electrode (4),
o the measuring circuit forms a voltage ratio from the
[5 force-dependent voltage (8) and the reference
voltage (9), the voltage ratio representing a value
of the impressed force.
2. The device according to claim 1, characterized in that the
thin insulating film (2) is designed as a thin multi-layer
insulating film (2).
3. The device according to claim 1 or 2, characterized in that
the contact surfaces of the first and second metal
electrodes (1, 3) is designed a form fit in the range of
less than 4 micrometers across the entire contact surface.
4. The device according to one or more of claims 1 to 3,
characterized in that the first metal electrode (1), the
second metal electrode (3) and the metal electrode (4) have
at least the same strength as, or greater strength than,
the thin insulating film (2).
5. The device according to one or more of claims 1 to 4,
characterized in that a spatial distance of less than or
equal to 200 millimeters exists between the measuring
circuit and the load cell.
6. The device according to one or more of claims 1 to 5,
characterized in that the mean roughness value Ra of the
contact surfaces of the first metal electrode (1) and of
the reference metal electrode (4) are rougher at a ratio of
30:1 to 2:1 compared to the mean roughness value of the
contact surface of the second metal electrode (3), which
has a mean roughness value Ra of less than or equal to 200
nanometers.
7. The device according to one or more of claims 1 to 6,
characterized in that multiple reference metal electrodes
[5 (4) are provided on the load cell.
8. The device according to one or more of claims 1 to 7,
characterized by comprising a second load cell having the
same design, which can be positioned in the direction of an
interfering force component.
9. The device according to one or more of claims 1 to 8,
characterized in that the load cell comprises a plurality
of thin insulating films (2.1, 2.2), which electrically are
associated with a plurality of measuring circuits, and the
spatial or geometry arrangement is designed in such a way
that the magnitude and direction of the forces to be
measured are simultaneously detected as a vector quantity.
10. The device according to one or more of claims 1 to 9,
characterized in that the metal electrodes (1, 3) and the

Claims (1)

  1. reference metal electrode (4) are manufactured as
    insertable bodies having freely selectable ruled geometries
    as positive and negative shapes.
    11. The device according to claim 10, characterized in that the insertable bodies are selected from the following group:
    - designed as an inside truncated cone and an outside
    truncated cone comprising lateral surfaces having the
    same shape, the thin insulating film (2) being applied
    to the lateral surface;
    - designed as cylinder surfaces, inserted into one
    another, of the outer cylinder and inner cylinder having
    thin insulating films applied to the cylinder lateral
    surface, the thin insulating film (2) being applied to
    the end face of the cylinder rings.
    12. The device according to one or more of claims 1 to 11,
    characterized in that the thin insulating film (2) is
    applied to the circumferential surface of two mutually
    connected truncated cones on the outer surface of the
    respective inner electrode, which are mounted respect to a
    precisely fitting casing made of two outer electrodes that
    are electrically insulated from one another as a negative
    shape.
    13. The device according to one or more of claims 1 to 12,
    characterized in that an electronic signal generator is
    used as the power source (6), which in a first operating
    mode operates as a regulated direct current source or in a
    second operating mode as an alternating current signal
    source, and that furthermore the measuring circuit can be
    set to the respective operating mode.
    14. The device according to one or more of claims 1 to 13,
    characterized in that mechanical transmission elements for
    passing on the force to the metal electrodes (1, 3) and the
    reference metal electrode (4) are provided, which are
    designed as shaped parts made of strong plastic materials
    or high-strength composite materials.
    15. The device according to one or more of claims 1 to 14,
    characterized in that the measuring circuit furthermore
    comprises band stop filters or band pass filters.
AU2016292465A 2015-07-14 2016-07-09 Method and device for electrical force measurement by means of an insulating thin layer Active AU2016292465B2 (en)

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
DE102015111425.9 2015-07-14
DE102015111425.9A DE102015111425B4 (en) 2014-07-18 2015-07-14 Method and device for electrical force measurement by means of insulating thin film
PCT/DE2016/100305 WO2017008784A1 (en) 2014-07-18 2016-07-09 Method and device for electrical force measurement by means of an insulating thin layer

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AU2016292465B2 true AU2016292465B2 (en) 2020-10-29

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Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20030164047A1 (en) * 2002-01-18 2003-09-04 Toyoda Koki Kabushiki Kaisha Load sensor, temperature compensation method for the load sensor and manufacturing method of the load sensor
DE10253178B4 (en) * 2002-09-10 2004-08-19 Fraunhofer-Gesellschaft zur Förderung der angewandten Forschung e.V. Use a layer of diamond-like carbon
DE102010024808A1 (en) * 2010-06-23 2011-12-29 Deutsches Zentrum für Luft- und Raumfahrt e.V. Piezoresistive force sensor

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20030164047A1 (en) * 2002-01-18 2003-09-04 Toyoda Koki Kabushiki Kaisha Load sensor, temperature compensation method for the load sensor and manufacturing method of the load sensor
DE10253178B4 (en) * 2002-09-10 2004-08-19 Fraunhofer-Gesellschaft zur Förderung der angewandten Forschung e.V. Use a layer of diamond-like carbon
DE102010024808A1 (en) * 2010-06-23 2011-12-29 Deutsches Zentrum für Luft- und Raumfahrt e.V. Piezoresistive force sensor

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EA039446B1 (en) 2022-01-27
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AU2016292465A1 (en) 2018-03-01
EA201890310A1 (en) 2018-05-31

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