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Acceleration, Shock and Vibration Sensors

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<strong>Acceleration</strong>, <strong>Shock</strong> <strong>and</strong> <strong>Vibration</strong> <strong>Sensors</strong><br />

A built-in electronic circuit is required for proper operation of a capacitive accelerometer.<br />

In the simplest sense, the built-in circuit serves two primary functions:<br />

(1) allow changes in capacitance to be useful for measuring both static <strong>and</strong> dynamic<br />

events, <strong>and</strong> (2) convert this change into a useful voltage signal compatible with<br />

readout instrumentation.<br />

A representative circuit is shown<br />

in Figure 5.2.13 <strong>and</strong> Figure 5.2.14,<br />

which graphically depicts operation<br />

in the time domain, resulting from<br />

static measur<strong>and</strong> input.<br />

The following explanation starts<br />

from the beginning of the circuit <strong>and</strong><br />

Circuit Schematic<br />

continues through to the output, <strong>and</strong><br />

describes the operation of the circuit.<br />

To begin, the supply voltage is routed<br />

through a voltage regulator, which<br />

provides a regulated dc voltage to the<br />

circuit. The device assures “clean”<br />

power for operating the internal<br />

circuitry <strong>and</strong> fixes the amplitude of<br />

a built-in oscillator, which typically<br />

operates at >1 MHz. By keeping the<br />

amplitude of the oscillator signal<br />

Response from Circuit due to applied +1g Static <strong>Acceleration</strong><br />

(x-axis = time <strong>and</strong> y-axis = voltage)<br />

Figures 5.2.13 <strong>and</strong> 5.2.14: Operation of builtin<br />

circuit for capacitive accelerometer.<br />

constant, the output sensitivity of the device becomes fixed <strong>and</strong> independent of the<br />

supply voltage. Next, the oscillator signal is directed into the capacitance-bridge as<br />

indicated by Point 1 in Figure 5.2.13. It then splits <strong>and</strong> passes through each arm of the<br />

bridge, which each act as divider networks. The divider networks cause the oscillator<br />

signal to vary in direct proportion to the change in capacitance in C 2 <strong>and</strong> C 4. (C 2 <strong>and</strong><br />

C 4 electrically represent the mechanical sensing element.) The resulting amplitudemodulated<br />

signals appear at Points 2 <strong>and</strong> 3. Finally, to “demodulate” these signals,<br />

they are passed through individual rectification/peak-picking networks at Points 4 <strong>and</strong><br />

5, <strong>and</strong> then summed together at Point 6. The result is an electrical signal proportional<br />

to the physical input.<br />

It would be sufficient to complete the circuit at this point; however, additional features<br />

are often added to enhance its performance. In this case, a “st<strong>and</strong>ardization” ampli-<br />

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