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Chapter V Dielectric Study of ……<br />

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5.2 Fundamentals of Dielectric Studies<br />

Materials, which are electric insulators or in which an electric field can<br />

be sustained with a minimum dissipation power are known as dielectric<br />

materials. The dielectric includes all materials except condensed states of<br />

metals. A dielectric is characterized by its dielectric constant r, which relates<br />

the charge density to the electric field by the following relation,<br />

D = E = 0.rE (5.1)<br />

Where, = 0.r, 0 is the permittivity of free space and r is the relative<br />

permittivity or dielectric constant of the material (r = /0).<br />

In the earlier experiments Faraday found that by inserting a dielectric<br />

material between the capacitor plates, the capacitance was increased by a<br />

factor of r. The reason is the appearance of charges on the surface of the<br />

dielectric necessitating the arrival of fresh charges from the battery in order to<br />

keep the voltage constant. This is described in a schematic diagram of figure<br />

(5.1).<br />

In vacuum the surface charge density (D0) on the condenser plate is<br />

represented as<br />

D0= = 0E (5.2)<br />

Where, d is the distance between the plates.<br />

In the presence of dielectric, the surface charge density (D) of<br />

dielectrics increase to<br />

D =<br />

= 0.r E (5.3)<br />

The dipole moment per unit volume of dielectric (polarization- P) is<br />

equal to the surface charge density of dielectrics, therefore,<br />

P = 0.r E (5.4)<br />

186

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