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where C is the capacitance in pF, A is the area of the plates in mm2 , and x is the (variable) distance in mm It is important to observe that the change in capacitance caused by the displacement of one of the plates is nonlinear, since the capacitance varies as the inverse of the displacement For small displacements, however, the capacitance varies approximately in a linear fashion The sensitivity, S, of this motion transducer is de ned as the slope of the change in capacitance per change in displacement, x, according to the relation dC 8854 10 3 A pF = dx 2x 2 mm Thus, the sensitivity increases for small displacements This behavior can be veri ed by plotting the capacitance as a function of x and noting that as x approaches zero, the slope of the nonlinear C(x) curve becomes steeper (thus the greater sensitivity) Figure 46 depicts this behavior for a transducer with area equal to 10 mm2 S= This simple capacitive displacement transducer actually nds use in the popular capacitive (or condenser) microphone, in which the sound pressure waves act to displace one of the capacitor plates The change in capacitance can then be converted into a change in voltage or current by means of a suitable circuit An extension of this concept that permits measurement of differential pressures is shown in simpli ed form in Figure 47 In the gure, a three-terminal variable capacitor is shown to be made up of two xed surfaces (typically, spherical depressions ground into glass disks and coated

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200 150 C (pF) 100 50 0 1

Of twenty-eight offspring examined, all were consistent with the predictions of the Punnett square in gure 6.14. Those of class 8 (lower right box) with the colored, waxy phenotype all had a knobbed interchange chromosome as well as a normal homologue. Those with the colorless, waxy phenotype (class 4) had a knobless interchange chromosome. All of the colored, non-

5 6 x (mm)

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Thin deflecting plate Fixed surfaces vS (t) + _ R2 c c b d d R1 a_

mhkl = kG hkl , where k is a constant Porat [28] has studied the value of the shear modulus on different planes of a diamond, and the summary of the minimum shear modulus is as given in Table 26

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with a conducting material) and of a de ecting plate (typically made of steel) sandwiched between the glass disks Pressure inlet ori ces are provided, so that the de ecting plate can come into contact with the uid whose pressure it is measuring When the pressure on both sides of the de ecting plate is the same, the capacitance between terminals b and d, Cbd , will be equal to that between terminals b and c, Cbc If any pressure differential exists, the two capacitances will change, with an increase on the side where the de ecting plate has come closer to the xed surface and a corresponding decrease on the other side This behavior is ideally suited for the application of a bridge circuit, similar to the Wheatstone bridge circuit illustrated in Example 212, and also shown in Figure 47 In the bridge circuit, the output voltage, vout , is precisely balanced when the differential pressure across the transducer is zero, but it will deviate from zero whenever the two capacitances are not identical because of a pressure differential across the transducer We shall analyze the bridge circuit later

The McGraw Hill Companies, 2001

The Ideal Inductor The ideal inductor is an element that has the ability to store energy in a magnetic eld Inductors are typically made by winding a coil of wire around a core, which can be an insulator or a ferromagnetic material, as shown in Figure 48 When a

1(X) 0.0 1.2 1.5 5.5 7.5 13.7 18.9 20.1 21.0 27.7 32.0 33.0 36.1

current ows through the coil, a magnetic eld is established, as you may recall from early physics experiments with electromagnets2 In an ideal inductor, the resistance of the wire is zero, so that a constant current through the inductor will ow freely without causing a voltage drop In other words, the ideal inductor acts as a short circuit in the presence of DC currents If a time-varying voltage is established across the inductor, a corresponding current will result, according to the following relationship: diL dt

Summary of the minimum shear modulus [28]

3 1.4 2.0

(49)

i (t) L + vL (t) = Ldi dt _

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