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Chapter V Dielectric Study of ……<br />

-<br />

dipole moment of a molecule exhibited in the absence of external electric<br />

field.<br />

Irrespective of the results obtained in the study of electrical properties<br />

of materials, its polarity can be judged from the chemical structure of its<br />

molecules. An experimental definition of the dipole moment µ leads to very<br />

important conclusions regarding the structure of the molecules of materials.<br />

The atom has a positively charged nucleus surrounded by an electron cloud.<br />

Due to symmetry in non-polar dielectric substance, in the absence of electric<br />

field, the centers of positive and negative charges coincide. As a result of this<br />

l = 0 in the molecules of non-polar dielectric material and hence µ = 0.<br />

Conversely, the asymmetric molecules are always polar dielectric.<br />

Figure: 5.2 Formation of dipole in non-polar dielectric in electric field.<br />

Figure (5.2) shows formation of dipole in non-polar dielectric material<br />

when placed in electric field. When an electric field is applied, the centers of<br />

positive and negative charges are separated from each other due to the<br />

influence of electric force acting on them in mutually opposite directions. This<br />

induces an electric dipole.<br />

Figure: 5.3 Molecules structure of (a) KI, (b) CO2 and (c) H2O.<br />

The mono-atomic molecules (He, Ne, Ar, Kr, Xe) and molecules<br />

consisting of two identical atoms linked by a homo-polar bond (H2, N2, Cl2) are<br />

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