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Variable Capacitance Transducers

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Presentation on theme: "Variable Capacitance Transducers"— Presentation transcript:

1 Variable Capacitance Transducers
The Capacitance of a two plate capacitor is given by A – Overlapping Area x – Gap width k – Dielectric constant Permitivity 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

2 Capacitive Rotation Sensor
One plate rotates and the other is stationary Common area is proportional to the angle The relationship is linear and K is the sensor constant Sensitivity is Capacitance Bridge DC Output vo Fixed Plate Rotation A θ Rotating Plate

3 Capacitive Displacement Sensor
One plate is attached to the moving object and the other is kept stationary Capacitance is and sensitivity is This relationship is nonlinear but can be linearized by using an op amp circuit C = K/x Capacitance Bridge vo Cref A Supply Voltage vref + + Fixed Plate + Output vo Op amp Position x Moving Plate (e.g., Diaphragm)

4 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 Capacitance Bridge vo Fixed Plate Liquid Level h k

5 Displacement Measurement
Output vo Supply Voltage vref + R i From magnitude From phase

6 Capacitive Angular Velocity Sensor
Supply Voltage vref + i Current Sensor

7 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

8 Capacitance Bridge Circuit
Compensator Z1 Sensor Z2 AC Excitation Bridge Output vo v vref + Z3 Z4 Bridge Completion For a balanced circuit Bridge output due to sensor change

9 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 Charge Source q Equivalent Capacitance C

10 Sensitivity 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

11 Piezoelectric Material Sensitivities
Charge Sensitivity Sq (pC/N) Voltage Sensitivity Sv (mV.m/N) Lead Zirconate Titanate (PZT) Barium Titanate Quartz Rochelle Salt 110 140 2.5 275 10 6 50 90

12 Piezoelectric Accelerometer
Spring Direction of Sensitivity (Input) Inertia Mass Piezoelectric Element Output vo 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

13 Frequency response curve of a piezoelectric accelerometer
Resonance Accelerometer Signal (dB) Useful Range 1 5,000 20,000 Frequency (Hz) 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

14 Charge Amplifier Impedance matching Reduce speed of charge leakage Rf
Cf A vo/K K + + q C Cc Output vo Piezoelectric Sensor Cable Charge Amplifier Impedance matching Reduce speed of charge leakage

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