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6.4 Triboelectric Detectors 237<br />

6.4 Triboelectric Detectors<br />

Any object can accumulate static electricity on its surface. These naturally occurring<br />

charges arise from the triboelectric effect (i.e., a process <strong>of</strong> charge separation due to<br />

object movements, friction <strong>of</strong> clothing fibers, air turbulence, atmosphere electricity,<br />

etc.) (see Section 3.1 <strong>of</strong> Chapter 3). Usually, air contains either positive or negative<br />

ions that can be attracted to the human body, thus changing its charge. Under the<br />

idealized static conditions, an object is not charged: Its bulk charge is equal to zero. In<br />

reality, any object which at least temporarily is isolated from the ground can exhibit<br />

some degree <strong>of</strong> its bulk charge imbalance. In other words, it becomes a carrier <strong>of</strong><br />

electric charges.<br />

Any electronic circuit is made up <strong>of</strong> conductors and dielectrics. If a circuit is not<br />

shielded, all <strong>of</strong> its components exhibit a certain capacitive coupling to the surrounding<br />

objects. In practice, the coupling capacitance may be very small—on the order <strong>of</strong> 1 pF<br />

or less. A pickup electrode can be added to the circuit’s input to increase its coupling<br />

to the environment, very much like in the capacitive detectors discussed in Section<br />

6.3. The electrode can be fabricated in the form <strong>of</strong> a conductive surface which is well<br />

isolated from the ground.<br />

An electric field is established between the surrounding objects and the electrode<br />

whenever at least one <strong>of</strong> them carries electric charges. In other words, all distributed<br />

capacitors formed between the electrode and the environmental objects are charged<br />

by the static or slow-changing electric fields. Under the no-occupancy conditions, the<br />

electric field in the electrode vicinity is either constant or changes relatively slowly.<br />

If a charge carrier (a human or an animal) changes its position (moves away or<br />

a new charge carrying an object enters into the vicinity <strong>of</strong> the electrode), the static<br />

electric field is disturbed. This results in a redistribution <strong>of</strong> charges between the<br />

coupling capacitors, including those which are formed between the input electrode<br />

and the surroundings. The charge magnitude depends on the atmospheric conditions<br />

and the nature <strong>of</strong> the objects. For instance, a person in dry man-made clothes walking<br />

along a carpet carries a million times stronger charge than a wet intruder who has come<br />

from the rain. An electronic circuit can be adapted to sense these variable charges at<br />

its input. In other words, it can be made capable <strong>of</strong> converting the induced variable<br />

charges into electric signals that may be amplified and further processed. Thus, static<br />

electricity, which is a naturally occurring phenomenon, can be utilized to generate<br />

alternating signals in the electronic circuit to indicate the movement <strong>of</strong> objects.<br />

Figure 6.8 shows a monopolar triboelectric motion detector. It is composed <strong>of</strong><br />

a conductive electrode connected to an analog impedance converter made with a<br />

MOS transistor Q 1 a bias resistor R 1 , an input capacitance C 0 , a gain stage, and a<br />

window comparator [4]. Whereas the rest <strong>of</strong> the electronic circuit may be shielded, the<br />

electrode is exposed to the environment and forms a coupling capacitor C p with the<br />

surrounding objects. In Fig. 6.8, static electricity is exemplified by positive charges<br />

distributed along the person’s body. Being a charge carrier, the person generates an<br />

electric field, having intensity E. The field induces a charge <strong>of</strong> the opposite sign in the<br />

electrode. Under static conditions, when the person does not move, the field intensity<br />

is constant and the input capacitance C 0 is discharged through a bias resistor R 1 . That

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