modern instrumentation phys 533/chem 620 lecture 11 light, force, strain, and pressure sensors amin...
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Modern InstrumentationPHYS 533/CHEM 620
Lecture 11Light, Force, Strain, and Pressure Sensors
Amin JazaeriFall 2007
Classification of Sensors• Proprioceptive (Internal state) v.s.
Exteroceptive (external state) – measure values internally to the system (robot), e.g.
battery level, wheel position, joint angle, etc,– observation of environments, objects
• Active v.s. Passive – emitting energy into the environment, e.g., radar,
sonar– passively receive energy to make observation, e.g.,
camera• Contact v.s. non-contact• Visual v.s. non-visual
– vision-based sensing, image processing, video camera
Light energy• For a sensor, we’re interested in the light power
that falls on a unit area, and how well the sensor converts that into a signal.
• A common unit is the lux which measures apparent brightness (power multiplied by the human eye’s sensitivity).
• 1 lux of yellow light is about 0.0015 W/m2.• 1 lux of green light (50% eff.) is 0.0029 W/m2.• Sunlight corresponds to about 50,000 lux • Artificial light typically 500-1000 lux
Electromagnetic SpectrumElectromagnetic SpectrumVisible Spectrum
700 nm 400 nm
Light sensors• Simplest light sensor is an LDR (Light-
Dependent Resistor).• Optical characteristics close to human eye. • Can be used to feed an A/D directly without
amplification (one resistor in a voltage divider).• Common material is CdS
Sensitivity: dark 1 M,10 lux 40 k,1000 lux 400 .
(a) General block diagram of an optical instrument. (b) Highest efficiency is obtained by using an intense lamp, lenses to gather and focus the light on the sample in the cuvette, and a sensitive detector. (c) Solid-state lamps and detectors may simplify the system.
Light sources and detectors
Sources
• Incandescent bulb
• Light emitting diode (LED)
• Gas and solid state lasers
• Arc lamp
• Fluorescent source
Detectors
• Thermal detector (pyroelectric)
• Photodiode
• Phototransistor
• Charge-coupled device (CCD)
• Photoconductive cell
• Photomultiplier tube
• Block diagram of a single beam spectrophotometer. The prism serves as the dispersing device while the monochromator refers to the dispersing device (prism), entrance slit, and exit slit. The exit slit is moveable in the vertical direction so that those portions of the power spectrum produced by the power source (light source) that are to be used can be selected.
Readoutdevice
Detector
Cuvette
Exit slit
Red
VioletPrism
Monochromator
Entrance slit
Light source
I0
I
Photoemissive Sensors
Photomultiplier An incoming photon strikes the photocathode and liberates an electron. This electron is accelerated toward the first dynode, which is 100 V more positive than the cathode. The impact liberates several electrons by secondary emission. They are accelerated toward the second dynode, which is 100 V more positive than the first dynode, This electron multiplication continues until it reaches the anode, where currents of about 1 A flow through RL. Time response < 10 nsec
Phototube: have photocathode coated with alkali metals. A radiation photon with energy cause electron to jump from cathode to anode.Photon energies below 1 eV are not large enough to overcome the work functions, so wavelength over 1200nm cannot be detected.
Photoconductive CellsPhotoresistors: a photosensitive crystalline materials such as cadmium Sulfide (CdS) or lead sulfide (PbS) is deposited on a ceramic substance.
The resistance decrease of the ceramic material with input radiation. This is true if photons have enough energy to cause electron to move from the valence band to the conduction band.
light-dependent resistors (LDRs) are slow, but respond like the human eye
Photojunction SensorsPhotojunction sensors are formed from p-n junctions and are usually made of silicon. If a photon has enough energy to jump the band gap, hole-electron pairs are produced that modify the junction characteristics.
Voltage-current characteristics of irradiated silicon p-n junction. For 0 irradiance, both forward and reverse characteristics are normal. For 1 mW/cm2, open-circuit voltage is 500 mV and short-circuit current is 8 A.
Photodiode: With reverse biasing, the reverse photocurrent increases linearly with an increase in radiation.
Phototransistor: radiation generate base current which result in the generation of a large current flow from collector to emitter.Response time = 10 microsecond
Photovoltaic SensorsPhotovoltaic sensors is a p-n junction where the voltage increases as the radiation increases.
Spectral characteristics of detectors, (c) Detectors. The S4 response is a typical phototube response. The eye has a relatively narrow response, with colors indicated by VBGYOR. CdS plus a filter has a response that closely matches that of the eye. Si p-n junctions are widely used. PbS is a sensitive infrared detector. InSb is useful in far infrared. Note: These are only relative responses. Peak responses of different detectors differ by 107.
Photovoltaic Sensors
• Photovoltaic– light falling on a pn-junction
can be used to generate electricity from light energy (as in a solar cell)
– small devices used as sensors are called photodiodes
– fast acting, but the voltage produced is not linearly related to light intensity A typical photodiode
Photodiode vs. Photoresistor
• Photoresistor: simple but slow
• Photodiode/phototransistor: complex but fast– Phototransistor vs. Photodiode:
• Higher current• Slower (100KHz)• Higher dark current
Light sensors – high end• At the cutting edge of light sensor sensitivity are
Avalanche photodiodes. • Large voltages applied to these diodes
accelerate electrons to “collide” with the semiconductor lattice, creating more charges.
• These devices have quantum efficienciesaround 90% and extremely low noise.
• They are now made withlarge collection areas andknown as LAAPDs (Large-Area Avalanche Photo-Diode)
Light sensors – cameras• Two solid-state camera types: CCD and CMOS.• CCD is the more mature technology, and has
the widest performance range. – 8 Mpixel size for cameras– Low noise/ high efficiency for astronomy etc. – Good sensitivity (low as 0.0003 lux, starlight)
• CCDs require several chips,but are still cheap ($50 +)
• Most CCDs work in near infraredand can be used for night visionif an IR light source is used.
Light sensors – cameras• CMOS cameras are very compact and
inexpensive, but haven’t matched CCDs in most performance dimensions.
• Start from $20(!)
• Custom CMOS camerasintegrate image processingright on the camera.
• Allow special functions likemotion detection, recognition.
Polarized Light
• Normal light: light wave travels at all orientation (w.r.t. horizon)
• Polarized light: all the light traveling in a given orientation.
• Two normal filters => no passing light
• The amount of light can be controlled
Applications
• object presence detection
• object distance detection
• surface feature detection (finding/following markers/tape)
• wall/boundary tracking
• rotational shaft encoding
• bar code decoding
Sensor limitations
• Light reflectivity:– Surface color
• Black: does not reflect• White: reflects
– Texture• Ambient light:
– Measure with and w/o emitter– Subtract from each other
• Sensor calibration– Calibration to be done repeatedly. Why?
• => Partially observable
Force Sensing
AF Strain Sensing:
APF Pressure Sensing:
amF Acceleration Sensing:
xkF Elastic Sensing:
Sensing Element in Force Sensing Element in Force SensorsSensors
There are many types of sensors can
be used to measure force (or torque)!
Resistive type force sensors, such as
strain gages ands load cells, are very
commonly used in force
measurements.
Load Cell Load Cell (Example of Spec. Items)
PerformancePerformance Load range: 5 to 250 lbs Non-Linearity: 0.05% F.S. Hysteresis: 0.03% F.S. Non-Repeatability: 0.03% F.S. Output: 3 mV/V Resolution: InfiniteEnvironmentalEnvironmental Temp. operating: 0 to 130 °F Temp. compensated: 30 to 130 °FMechanicalMechanical Static overload: 50% over capacity
FullScale
Force sensors - Strain Gauges
• Strain gauge - The main tool in sensing force.• Strain gauges, measure strain• Strain can be related to stress, force, torque and
a host of other stimuli including displacement, acceleration or position.
• At the heart of all strain gauges is the change in resistance of materials due to change in their length due to strain.
Strain GagesStrain Gages
Characteristics:
1) able to measure strains of m/m2) small in size and light in weight3) able to response to high frequency signals4) wide range of linear response5) has stable calibration constant (gage factor)6) flexible in use and wide range applications7) low in cost8) easy compensation to various factors
Fundamentals of Strain Fundamentals of Strain GagesGages
(strain) e
(stress) E
eL
eT
FF
llA
Elastic Modulus:
LT ee
The resistance of a strain gage:Al
R
Material resistivity
Element length
Cross section area
When a strain gage is strained, the change in resistance is:
R
AAR
llR
R
Poisson’sratio
Axialstrain
Transversestrain
Strain GagesStrain Gages
Relative change in resistance:
Because:
Define a Gage factor G:
Gage factor of a strain gage:
LeR
RG
)e(2e2D
D2
A
ALT
Then:
;el
lL
Poisson’sratio
Example Specs of Strain Example Specs of Strain GagesGages
Temperature RangeTemperature RangeNormal: -100 to +350 FShort-Term: -320 to +400 F
Strain RangeStrain Range+3% for gage lengths under 1/8 in+5% for 1/8 in and over
Fatigue LifeFatigue Life105 cycles at +1500 microstrain 106 cycles at +1500 microstrain
with low modulus solder.
Strain Gauge
• For any given strain gauge the gauge factor is a constant
• Ranges between 2 to 6 for most metallic strain gauges
• From 40-200 for semiconductor strain gauges. • The strain gauge relation gives a simple linear
relation between the change in resistance of the sensor and the strain applied to it.
Stress and Strain
Two-axis strain gauge
120 degree rosette
45 degree rosette
45 degree stacked rosette
membrane rosette
Semiconductor strain gauges
• Operate like resistive strain gauges • Construction and properties are different. • The gauge factor for semiconductors is much
higher than for metals. • The change in conductivity due to strain is much
larger than in metals. • Are typically smaller than metal types • Often more sensitive to temperature variations
(require temperature compensation).
Semiconductor strain gauges
• All semiconductor materials exhibit changes in resistance due to strain
• The most common material is silicon because of its inert properties and ease of production.
• The base material is doped, by diffusion of doping materials (usually boron or arsenide for p or n type) to obtain a base resistance as needed.
• The substrate provides the means of straining the silicon chip and connections are provided by deposition of metal at the ends of the device.
Amplification for Strain Amplification for Strain GagesGages
Sensitive instrumentation is required to measure the small changes in resistance produced by strain gauges.
Wheatstone bridgeWheatstone bridge is typically used to measure resistances accurately and dynamically over a very large range (1 to 1,000,000
Application of Strain GagesApplication of Strain Gages
+e
x l
-eF
Strain gages are used in cantilever type load cells
w
t
-
R4 R3
R1 R2
V0
Vs
+
-
R1 R3
R2
R4
4
4
2
2
1
1
3
32
32
32s0 R
R
R
R
R
R
R
R
)RR(
RRVV
Application of Strain GagesApplication of Strain Gages
Strain gages are used in pillar type load cells
LT
L
eEA
Fe
EEA
Fe
F
eT
eL
R3
, R4
, R1
R2
F Poisson’sratio
Application of Strain GagesApplication of Strain Gages
Strain gages are used in torque cells :
3142 eeee
31 rG
Te
3
gage1gage
0
rG
TFeF
V
V
ulusmodShear)1(2
EG
factorGageF
TorqueT
gage
Strainedcompressed
Common Strain Gage Common Strain Gage ArrangementsArrangements
+ -
R4 R3
R1 R2
VS + -
R4 R3
R1 R2
VS
+ -
R4 R3
R1 R2
VS + -
R4 R3
R1 R2
VS
Practical Implementation of Practical Implementation of Strain GagesStrain Gages
Strain gages Bridge Amplifier / filter ComputerForce Input
Preparation:• clean with sandpaper• degreaser solvent • glue = adhesive + curing agent• clams for curing cycle (24 h)
Parallel
Most critical step !
Practical Implementation of Practical Implementation of Strain GagesStrain Gages
Wheatstone bridge and amplification circuit
RF
-
+
V1
Vout
R1
A
B
R3
V2
R2
-
R4 R3
R1 R2
V0
Specifications:• Chip 741• R1 = R2 • R3 = RF • Gain: RF / R1
Tactile sensors
• Tactile sensors are force sensors but: • Definition of “tactile” action is broader, the
sensors are also more diverse. • One view is that tactile action as simply sensing
the presence of force. Then:– A simple switch is a tactile sensor– This approach is commonly used in keyboards – Membrane or resistive pads are used – The force is applied against the membrane or a
silicon rubber layer.
Tactile sensors
• In many tactile sensing applications it is often important to sense a force distribution over a specified area (such as the “hand” of a robot).
• Either an array of force sensors or • A distributed sensor may be used. • These are usually made from piezoelectric films
which respond with an electrical signal in response to deformation (passive sensors).
A tactile sensor
Tactile sensors
• Operation:• The polyvinylidene fluoride (PVDF) film is
sensitive to deformation. • The lower film is driven with an ac signal • It contracts and expands mechanically and
periodically. • When the upper film is deformed, its signal
changes from normal and the amplitude and or phase of the output signal is now a measure of deformation (force).
Pressure Sensors
What is pressure?
Pressure = force per area in fluids
1 N/m2 = 1 Pa Pascal
Engineers use the bar1 bar = 105 Pa = 1 athmosphere ~ 10 m of water column
Ranges of pressure measurement:Athmosphere: 1 barHydraulics, pneumatics: 6 -10 barCar industry 1 - 5 bar (tyre), 20 bar (air conditioning)Medicine: Blood: 100 mbar; in the human body 10 to 100 mbarDeep sea level: 4.000m ~ 400 barThin film processes: 1 to 1000 Pa (0,01 to 10 mbar)Rough vacuum: 10 Pa (changing pumps) High vacuum: down to 10-8 Pa
Pressure sensors
• Pressure sensors come in four basic types :• Absolute pressure sensors (PSIA): pressure sensed
relative to absolute vacuum.• Differential pressure sensors (PSID): the difference
between two pressures on two ports of the sensor is sensed.
• Gage pressure sensors (PSIG): the pressure relative to ambient pressure is sensed. (Most common)
• Sealed gage pressure sensor (PSIS): the pressure relative to a sealed pressure chamber (usually 1 atm at sea level or 14.7 psi) is sensed.
Piezoresistive pressure sensors
• Piezoresistor is a semiconductor strain gauge• Most modern pressure sensors use it rather than
the conductor type strain gauge. • Resistive (metal) strain gauges are used only at
higher temperature or for specialized applications
• May be fabricated of silicon– simplifies construction – allows on board temperature compensation,
amplifiers and conditioning circuitry.
Piezoresistive pressure sensors
• Basic structure: – two gauges are parallel to one dimension of
the diaphragm– The two gauges can be in other directions
Piezoresistive pressure sensors
• The change in resistance of the two piezoresistos is:
R1R1
= R2R2
= 12 y x
is an average sensitivity (gauge) coefficient andx and y are the stresses in the transverse directions
Piezoresistive pressure sensors
• Piezoresistors and the diaphragm are fabricated of silicon.
• A vent is provided, making this a gage sensor. • If the cavity under the diaphragm is
hermetically closed and the pressure in it is P0, the sensor becomes a sealed gage pressure sensor sensing the pressure P-P0.
• A differential sensor is produced by placing the diaphragm between two chambers, each vented through a port (figure).
Differential pressure sensor
Piezoresistive pressure sensors
• A different approach is to use a single strain gauge
• A current passing through the strain gauge
• Pressure applied perpendicular to the current.
• The voltage across the element is measured as an indication of the stress and therefore pressure.
Construction
• Many variations
• Body of sensor is particularly important
• Silicon, steel, stainless steel and titanium are most commonly used
• Ports are made with various fittings
• The contact material is specified (gas, fluid, corrosivity, etc.)
Various pressure sensors
Miniature pressure sensors
Pitran pressure sensors (absolute)
150 psi differential pressure sensor
100 psi absolute pressure sensor (TO5 can)
15 and 30 psi differential pressure sensors
Capacitive pressure sensors
• The deflection of the diaphragm constitutes a capacitor in which the distance between the plates is pressure sensitive.
• The basic structure (not shown) consists of two metalic plates
• These sensors are very simple and are particularly useful for sensing of very low pressure.
• At low pressure, the deflection of the diaphragm may be insufficient to cause large strain but can be relatively large in terms of capacitance.
Capacitive pressure sensors
• The capacitance may be part of an oscillator,• The change in its frequency may be quite large making
for a very sensitive sensor. • Other advantages
– less temperature dependent – stops on motion of the plate may be incorporated, - not sensitive
to overpressure.
• Overpressures of 2-3 orders of magnitude larger than rated pressure may be easily tolerated without ill effects.
• The sensors are linear for small displacement but at larger pressures the diaphragm tends to bow causing nonlinear output
Magnetic( Inductive) pressure sensors
• A number of methods are used • In large deflection sensors an inductive position
sensor may be used or an LVDT attached to the diaphragm.
• For low pressures, variable reluctance pressure sensor is more practical.
• The diaphragm is made of a ferromagnetic material and is part of the magnetic circuit shown in Figure 6.32.
Variable reluctance pressure sensor
Magnetic pressure sensors
• The reluctance is directly proportional to the length of the air gap between the diaphragm and the E-core.
• Gap changes with pressure and the inductance of the two coils changes and sensed directly.
• A very small deflection can cause a very large change in inductance of the circuit making this a very sensitive device.
• Magnetic sensors are almost devoid of temperature sensitivity allowing these sensors to operate at elevated temperatures.
Other pressure sensors
• Optoelectronic pressure sensors - Fabri-Perot optical resonator to measure small displacements. – light reflected from a resonant optical cavity is measured
by a photodiode to produce a measure of pressure sensed.
• A very old method of sensing low pressures (often called vacuum sensors) is the Pirani gauge. – based on measuring the heat loss from gases which is
dependent on pressure. The temperature is sensed and correlated to pressure, usually in an absolute pressure sensor arrangement.
Pressure sensors - properties
• Semiconductor based sensors can only operate at low temperatures (50 to +150C).
• Temperature dependent errors can be high unless properly compensated (externally or internally).
• The range of sensors can exceed 50,000 psi and can be as small as a fraction of psi.
• Impedance is anywhere between a few hundred Ohms to about 100 k, depending on device.
• Linearity is between 0.1 to 2% typically
Pressure sensors - properties
• Other speciffications include:– Maximum pressure, burst pressure and proof pressure
(overpressure) – electrical output - either direct (no internal circuitry) or after
conditioning and amplification. – Digital outputs are also available. – Materials used (silicon, stainless steel, etc.) and compatibility
with gases and liquids are specified – port sizes and shapes, connectors, venting ports – cycling of the pressure sensors is also specified – hysteresis (usually below 0.1% of full scale) – repeatability (typically less than 0.1% of full scale).
How to construct a pressure sensor
Pressure is transformed into deflection of a membrane
Tasks to do:
• Understand the elastic deformation of a membrane
• Construct a membrane
• Sense the deflection
• Construct a sensor housing
• Build an electronic circuit
Metal membrane pressure sensor
Figure from: Hesse, Schnell: Sensoren für die Prozess- und Fabrikautomation
Capacitive pressure sensor
Capacity of two plates
d
AC r0
Advantages:
• Sensitive
• Stable, small T-drift (ceramic technology)
• Small, E.g. 2mm Si chip size for eye pressure sensor
Disadvantages:
• Nonlinear (1/d)
• Electronics complicated
• Capacitive bridge circuit
• C - Frequency conversion
A: Area; d: distance
Inductive pressure sensor
Inductive bridge circuit
Very T-stable
Large devices,
large membranes for
small differential pressure
Si micromachined pressure sensor
Why Si technology?
• Batch process: >1000 chips on a wafer
• Precise control of technology
• k-factor in Si is ~ 100 (>>2!)
• Monolithic integration with electronics
• Very advanced and available technology
• Housing processes well known
Piezoresistive effect in Si
Semiconductors: deformation changes band structure
large change in conductivity
k positive or negative
k sensitive on temperature, doping and crystal orientation
Longitudinal: Current parallel to strain: i
Transversal: Current vertical to strain: i
Rule of thumb for p-doped Si:
Longitudinal: k~ +100
Transversal: k~ -100
Principle of Si p-sensor
A: longitudinal
B: transversal
Silicon piezoresistive pressure sensor
Figure from: Bonfig, Sensoren
Si
Si
Pyrex glass
Metal socket
NitrideMetal
Oxide Piezoresistor
Low pressure: vacuum gauges
Ranges:
Rough vacuum at 1 Pa to 100 Pa. In this range, mechanical pumping is switched to turbo pumping for high vacuum. A sensor is needed to trigger the valves.
High vacuum below 0,1 Pa. This is measured for process control.
Usually, a vacuum system has one sensor for control of the pumping down and pump control (pirani type) and one sensor for the control of the final pressure (ionisation type).
Quartz Pressure Sensor
• A typical Quartz crystal sensor with inbuilt micro-electric circuitry and a diaphragm.
• These sensors measure dynamic pressures, and are not generally used for static pressure sensing.
• Proper and accurate alignment of the sensor is very important for higher sensitivity.
• Sensors used in high temperature conditions(e.g. combustion chamber of an engine) use either recess mounting, baffled diaphragm or thermal protection coatings to reduce negative signal effects.
Pros and Cons
• Have a high Stiffness value and produce a high output with very little strain.
• Ideal for rugged use.• Excellent linearity over a
wide amplitude.• Ideal for continuous
online condition monitoring smart systems.
• Can be used only for dynamic pressure sensing as in case of static sensing the signals will decay away.
• Operation over long cables may affect frequency response and introduce noise and distortion, the cables need to be protected.
Typical Application-Combustion Monitoring• Pressures developed during
the combustion process is continuously measured by sensors mounted on the cylinder heads.
• Continuous Pressure monitor(CPM) systems are the basic data acquisition and data reduction software and hardware units.