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Callister - An introduction - 8th edition

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770 • Chapter 18 / Electrical Properties<br />

Equation Summary<br />

• This polarization phenomenon accounts for the ability of the dielectrics to<br />

increase the charge-storing capability of capacitors.<br />

• Capacitance is dependent on applied voltage and quantity of charge stored<br />

according to Equation 18.24.<br />

• The charge-storing efficiency of a capacitor is expressed in terms of a dielectric<br />

constant or relative permittivity (Equation 18.27).<br />

• For a parallel-plate capacitor, capacitance is a function of the permittivity of the<br />

material between the plates, as well as plate area and plate separation distance<br />

per Equation 18.26.<br />

• The dielectric displacement within a dielectric medium depends on the applied<br />

electric field and the induced polarization according to Equation 18.31.<br />

• For some dielectric materials, the polarization induced by an applied electric field<br />

is described by Equation 18.32.<br />

Types of Polarization<br />

Frequency Dependence of the Dielectric Constant<br />

• Possible polarization types include electronic (Figure 18.32a), ionic (Figure<br />

18.32b), and orientation (Figure 18.32c); not all types need be present in a particular<br />

dielectric.<br />

• For alternating electric fields, whether a specific polarization type contributes to<br />

the total polarization and dielectric constant depends on frequency; each polarization<br />

mechanism ceases to function when the applied field frequency exceeds<br />

its relaxation frequency (Figure 18.34).<br />

Other Electrical Characteristics of Materials<br />

• Ferroelectric materials exhibit spontaneous polarization—that is, they polarize in<br />

the absence of an electric field.<br />

• <strong>An</strong> electric field is generated when mechanical stresses are applied to a piezoelectric<br />

material.<br />

Equation<br />

Page<br />

Number Equation Solving for Number<br />

18.1 V IR<br />

Voltage (Ohm’s law) 721<br />

18.2 r RA Electrical resistivity 721<br />

l<br />

18.4 s 1 r<br />

Electrical conductivity 721<br />

18.5 J se<br />

Current density 722<br />

18.6 e V Electric field intensity 722<br />

l<br />

18.8, 18.16<br />

s nem e<br />

Electrical conductivity (metal); conductivity for n-type<br />

extrinsic semiconductor<br />

727, 737<br />

18.9 r total r t r i r d For metals, total resistivity (Matthiessen’s rule) 729<br />

18.10 r t r 0 aT<br />

Thermal resistivity contribution 729

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