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handbook of modern sensors

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78 3 Physical Principles <strong>of</strong> Sensing<br />

conduction. The bottom electrode may be given a heat-absorbing coating, such as<br />

goldblack or organic paint. As a result <strong>of</strong> heat absorption, the bottom side becomes<br />

warmer (the new temperature is T 1 ), which causes the bottom side <strong>of</strong> the material to<br />

expand. The expansion leads to flexing <strong>of</strong> the sensor, which, in turn, produces stress<br />

and a change in dipole orientation. Being piezoelectric, stressed material generates<br />

electric charges <strong>of</strong> opposite polarities across the electrodes. Hence, we may regard<br />

a secondary pyroelectricity as a sequence <strong>of</strong> events: a thermal radiation → a heat<br />

absorption → a thermally induced stress → an electric charge.<br />

The dipole moment, M, <strong>of</strong> the bulk pyroelectric sensor is<br />

M = µAh, (3.72)<br />

where µ is the dipole moment per unit volume, A is the sensor’s area, and h is the<br />

thickness. The charge, Q a , which can be picked up by the electrodes, develops the<br />

dipole moment across the material:<br />

M must be equal to M 0 , so that<br />

M 0 = Q a h. (3.73)<br />

Q a = µA. (3.74)<br />

As the temperature varies, the dipole moment also changes, resulting in an induced<br />

charge.<br />

Thermal absorption may be related to a dipole change, so that µ must be considered<br />

as a function <strong>of</strong> both temperature, T a , and an incremental thermal energy, W,<br />

absorbed by the material<br />

Q a = Aµ(T a ,W). (3.75)<br />

Figure 3.27 shows a pyroelectric detector (pyrosensor) connected to a resistor R b ,<br />

which represents either the internal leakage resistance or a combined input resistance<br />

<strong>of</strong> the interface circuit which is connected to the sensor. The equivalent electrical<br />

circuit <strong>of</strong> the sensor is shown at the right. It consists <strong>of</strong> three components: (1) the<br />

current source generating a heat induced current, i (remember that a current is a<br />

movement <strong>of</strong> electric charges), (2) the sensor’s capacitance, C, and (3) the leakage<br />

resistance, R b .<br />

The output signal from the pyroelectric sensor can be taken in the form <strong>of</strong> either<br />

charge (current) or voltage, depending on the application. Being a capacitor, the<br />

pyroelectric device is discharged when connected to a resistor, R b . Electric current<br />

Fig. 3.27. Pyroelectric sensor and its equivalent circuit.

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