Classical Electrodynamics |
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Page 116
E 4.66 p (# a'EO ( ) 4.6 Molecular Polarizability and Electric Susceptibility In this
section and the next we will consider the relation between molecular properties
and the macroscopically defined parameter, the electric susceptibility X. Our ...
E 4.66 p (# a'EO ( ) 4.6 Molecular Polarizability and Electric Susceptibility In this
section and the next we will consider the relation between molecular properties
and the macroscopically defined parameter, the electric susceptibility X. Our ...
Page 126
If, however, the dielectric properties are altered, e(x) → e(x) + 6e(x) (4.100) the
contributions in (4.99) are not necessarily the same. In fact, we have just
calculated the change in energy brought about by introducing a dielectric body
into an ...
If, however, the dielectric properties are altered, e(x) → e(x) + 6e(x) (4.100) the
contributions in (4.99) are not necessarily the same. In fact, we have just
calculated the change in energy brought about by introducing a dielectric body
into an ...
Page 216
7.5 Reflection and Refraction of Electromagnetic Waves at a Plane Interface
between Dielectrics The reflection and refraction of light at a plane surface
between two media of different dielectric properties are familiar phenomena. The
various ...
7.5 Reflection and Refraction of Electromagnetic Waves at a Plane Interface
between Dielectrics The reflection and refraction of light at a plane surface
between two media of different dielectric properties are familiar phenomena. The
various ...
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Contents
Introduction to Electrostatics | 1 |
References and suggested reading | 23 |
Multipoles Electrostatics of Macroscopic Media | 98 |
Copyright | |
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