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handbook of modern sensors

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3.1 Electric Charges, Fields, and Potentials 39<br />

(A)<br />

(B)<br />

Fig. 3.1. (A) Positive test charge in the vicinity <strong>of</strong> a charged object and (B) the electric field <strong>of</strong><br />

a spherical object.<br />

perfect isolator, the isolating ability <strong>of</strong> fused quartz is about 10 25 times as great as<br />

that <strong>of</strong> copper, so that for practical purposes, many materials are considered perfect<br />

isolators. The semiconductors are intermediate between conductors and isolators in<br />

their ability to conduct electricity. Among the elements, silicon and germanium are<br />

well-known examples. In semiconductors, the electrical conductivity may be greatly<br />

increased by adding small amounts <strong>of</strong> other elements; traces <strong>of</strong> arsenic or boron are<br />

<strong>of</strong>ten added to silicon for this purpose.<br />

Figure 3.1A shows an object which carries a positive electric charge q. If a small<br />

positive electric test charge q 0 is positioned in the vicinity <strong>of</strong> a charged object, it will<br />

be subjected to a repelling electric force. If we place a negative charge on the object, it<br />

will attract the test charge. In vector form, the repelling (or attracting) force is shown<br />

as f. The boldface indicates a vector notation. A fact that the test charge is subjected<br />

to force without a physical contact between charges means that the volume <strong>of</strong> space<br />

occupied by the test charge may be characterized by a so-called electric field.<br />

The electric field in each point is defined through the force as<br />

E = f q 0<br />

. (3.1)<br />

Here, E is vector in the same direction as f because q 0 is scalar. Formula (3.1) expresses<br />

an electric field as a force divided by a property <strong>of</strong> a test charge. The test charge must<br />

be very small not to disturb the electric field. Ideally, it should be infinitely small;<br />

however, because the charge is quantized, we cannot contemplate a free test charge<br />

whose magnitude is smaller than the electronic charge: e = 1.602 × 10 −19 C.<br />

The field is indicated in Fig. 3.1A by the field lines which in every point <strong>of</strong> space<br />

are tangent to the vector <strong>of</strong> force. By definition, the field lines start on the positive<br />

plate and end on the negative. The density <strong>of</strong> field lines indicates the magnitude <strong>of</strong><br />

the electric field E in any particular volume <strong>of</strong> space.

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