Variable Capacitance Transducers The Capacitance of a two plate capacitor is given by A –...
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Transcript of Variable Capacitance Transducers The Capacitance of a two plate capacitor is given by A –...
Variable Capacitance Transducers
• The Capacitance of a two plate capacitor is given by
CkA
x
A – Overlapping Area
x – Gap width
k – Dielectric constant
rk 0 0 rPermitivity of vacuum Relative permitivity
• A change in any one of these parameters may be used for sensing
• Examples - Transverse displacement, rotation, and fluid level
• A capacitance bridge can be used to measure the change in the capacitance
• Other methods include measuring a change in charge
• Charge – charge amplifier
• Voltage – high impedance device in parallel
• Current – low impedance device in series
• Or inductance capacitance oscillator circuit
DC Outputvo
CapacitanceBridge
Rotating Plate
A
Fixed Plate
Rotation
Capacitive Rotation Sensor
• One plate rotates and the other is stationary
• Common area is proportional to the angle
θ
KC • The relationship is linear and K is the sensor constant
• Sensitivity isK
CS
Moving Plate(e.g., Diaphragm)
Position x
vo
Fixed Plate
Capacitive Displacement Sensor
• One plate is attached to the moving object and the other is kept stationary
• Capacitance is and sensitivity is
x
KC
• This relationship is nonlinear but can be linearized by using an op amp circuit
2x
K
x
CS
Outputvo
SupplyVoltage
vref
+
−
Cref
C = K/x
+
−A
+
−
Op amp
CapacitanceBridge
xK
Cvv refref
o
k
vo
Fixed Plate
Levelh
Liquid
Displacement Measurement by changing Dielectric
• Displacement can be measured by attaching the moving object to a solid dielectric element placed in between the plates
• Liquid level as shown below can be measured as the dielectric medium between the plates changes with the liquid level
CapacitanceBridge
Outputvo
SupplyVoltage
vref
+
−
R +
−
i
Displacement Measurement
id
dtCv
v v
Roref o
x
KC
v
v RKj xo
ref
1
1
xRK
M
1 12
From magnitude From phase
x RK tan
SupplyVoltage
vref
+
−
i CurrentSensor
+
−
Capacitive Angular Velocity Sensor
id
dtCv v
dC
dtref ref
C
d
dt
i
Kvref
Capacitive Sensor Applications
• Mechanical loading effects are negligible
• Variations in dielectric properties due to humidity, temperature, pressure, and impurities can cause errors
• Capacitance bridge can compensate for these effects
• Sensitivity – 1pF per mm
+
AC Excitation
vref
CompensatorZ1
SensorZ2
Bridge Completion
Z3 Z4
BridgeOutput
vo
v
v v
Z
v v
Zref o
1 2
0
v
Z Z Z Z
Z Zvo ref
4 3 2 1
4 31
/ /
/
Z
Z
Z
Z2
1
4
3
vv
Z Z ZZo
ref1 4 31 /
Capacitance Bridge Circuit
v v
Z
v
Zref
3 4
00
For a balanced circuit Bridge output due to sensor change
ChargeSource
q
EquivalentCapacitance
C
Piezoelectric Sensors• Substances such as BaTiO3 (barium titanate),SiO2 (quartz in crystalline), and
lead zirconate titanate can generate an electric charge when subjected to stress (strain)
• Applications include
• Pressure and strain measuring devices
• Touch screens
• Accelerometers
• Torque/Force sensors
• Piezoelectric materials deform when a voltage is applied. Applications include
• Piezoelectric valves
• Microactuators and MEMS
CjZ
1
• Output impedance of a piezoelectric sensor is very high
• It varies with the frequency ~MΩ at 100Hz
Sensitivity
• Charge sensitivity For a surface area A (pressure applied – stress)
• Voltage sensitivity – change in voltage due to unit increment in pressure per unit thickness (d is the thickness)
• k is the dielectric constant of the crystal capacitor
Sq
Fq
SA
q
pq 1
Sd
v
pv 1
q C v
vq kSS
Material Charge Sensitivity Sq (pC/N)
Voltage SensitivitySv (mV.m/N)
Lead Zirconate Titanate (PZT)Barium Titanate
QuartzRochelle Salt
1101402.5275
106
5090
Piezoelectric Material Sensitivities
Piezoelectric Accelerometer
Outputvo
Direction ofSensitivity
(Input)
Spring
Inertia Mass
PiezoelectricElement
Electrodes
• Inertia force caused by the acceleration produces a voltage
• Light weight, high frequency response (1MHz)
• High output impedance – small voltages ~1mV
• High spring stiffness – natural frequency or resonant frequency is high (20kHz)
• Useful frequency range – 5kHz
Acc
eler
omet
er
Sig
nal (
dB)
Frequency (Hz)
5,000 20,000
Useful Range
1
Resonance
Frequency response curve of a piezoelectric accelerometer
• Typical accelerometer sensitivities – 10 pC/g (pico Coulomb per gravity) or 5mV/g
• Sensitivity depends on the piezoelectric properties and the way the inertia force is applied
• Large mass would result in a large force and a large output signal but
• Load the measurand
• Lower the resonant frequency
Charge Amplifier
Outputvo
Cf
vo/K +
−A
+
−Charge
Amplifier
Rf
CcC
PiezoelectricSensor
Cable
q
K
• Impedance matching
• Reduce speed of charge leakage
0o o o o oc f o
f
v v v v v Kq C C C v
K K K R
R Cdv
dtv R
dq
dtf fo
o f
v s
q s
R s
R C so f
f f
1
v j
q j
R j
R C jo f
f f
1
c f fR C