09.03.2013 Views

Download (4Mb) - Etheses - Saurashtra University

Download (4Mb) - Etheses - Saurashtra University

Download (4Mb) - Etheses - Saurashtra University

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

Chapter V Dielectric Study of ……<br />

-<br />

electric field. For anisotropic dielectrics the relationship between P and E is<br />

tensorical.<br />

Usually, the dielectric constant for a given material is defined as the<br />

ratio of a capacitance of capacitor containing a given dielectric (C) to a<br />

capacitance of vacuum capacitor (C0) of identical dimensions. This can be<br />

represented by the following relationship,<br />

r = (5.7)<br />

For a given charge distribution, the dielectric constant expresses the<br />

ratio of electric field strength in vacuum to that in a dielectric, the later field<br />

being reduced by the polarization of the dielectric medium.<br />

5.2.1 Polar and Non-polar Dielectrics<br />

Dielectrics can be divided into two classes<br />

(i) Polar dielectrics<br />

(ii) Non-polar dielectrics<br />

This classification is extremely important when electrical, general physical<br />

and chemical properties of materials are considered.<br />

A molecule of any material consists of atoms or ions having definite<br />

positive or negative electric charges. Even in the absence of external electric<br />

field if the molecule exhibits electric dipole (figure: 5.1-c) with dipole moment<br />

different from zero, it is referred to as a permanent dipole and the molecule is<br />

called as polar dielectric. The magnitude of the electric dipole moment of a<br />

molecule is,<br />

µ = q.l (5.8)<br />

Where, q is the magnitude of positive or negative electric charge of a<br />

molecule and l is the length of the dipole. Here, µ is the intrinsic electric<br />

188

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!