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handbook of modern sensors

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178 5 Interface Electronic Circuits<br />

integrator can be built for the applications, where the stimulus needs to be integrated<br />

over a certain time. The counter accumulates pulses over the gated interval rather<br />

than as an average number <strong>of</strong> pulses per counting cycle.<br />

Another useful feature <strong>of</strong> a V/F converter is that its pulses can be easily transmitted<br />

through communication lines. The pulsed signal is much less susceptible to a<br />

noisy environment than a high-resolution analog signal. In the ideal case, the output<br />

frequency f out <strong>of</strong> the converter is proportional to the input voltage V in :<br />

f out<br />

f FS<br />

= V in<br />

V FS<br />

, (5.25)<br />

where f FS and V FS are the full-scale frequency and input voltage, respectively. For<br />

a given linear converter, ratio f FS /V FS = G is constant and is called a conversion<br />

factor; then,<br />

f out = GV in . (5.26)<br />

There are several known types <strong>of</strong> V/F converters. The most popular <strong>of</strong> them are the<br />

multivibrator and the charge-balance circuit.<br />

A multivibrator V/F converter employs a free-running square-wave oscillator<br />

where charge–discharge currents <strong>of</strong> a timing capacitor are controlled by the input<br />

signal (Fig. 5.23). The input voltage V in is amplified by a differential amplifier (e.g.,<br />

an instrumentation amplifier) whose output signal controls two voltage-to-current<br />

converters (transistors U 1 and U 2 ). A precision multivibrator alternatively connects<br />

timing capacitor C to both current converters. The capacitor is charged for a half <strong>of</strong><br />

period through transistor U 1 by the current i a . During the second half <strong>of</strong> the timing<br />

period, it is discharged by the current i b through transistor U 2 . Because currents i a and<br />

i b are controlled by the input signal, the capacitor charging and discharging slopes<br />

vary accordingly, thus changing the oscillating frequency. An apparent advantage <strong>of</strong><br />

this circuit is its simplicity and potentially very low power consumption; however,<br />

its ability to reject high-frequency noise in the input signal is not as good as in the<br />

charge-balance architecture.<br />

Fig. 5.23. Multivibrator type <strong>of</strong> voltage-to-frequency converter.

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