Classical Electrodynamics |
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Page 116
Fortunately, the simpler properties of dielectrics are amenable to classical
analysis. Before examining how the detailed properties of the molecules are
related to the susceptibility we must make a distinction between the fields acting
on the ...
Fortunately, the simpler properties of dielectrics are amenable to classical
analysis. Before examining how the detailed properties of the molecules are
related to the susceptibility we must make a distinction between the fields acting
on the ...
Page 126
If , however , the dielectric properties are altered , € ( x ) = f ( x ) + de ( 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 ...
If , however , the dielectric properties are altered , € ( x ) = f ( x ) + de ( 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 ...
Page 216
( 1 ) Kinematic properties : ( a ) Angle of reflection equals angle of incidence . sin
i n ' ( 6 ) Snell ' s law : = - , where i , r are the angles of incidence and refraction ,
while n , n ' are the corresponding indices of refraction . ( 2 ) Dynamic properties ...
( 1 ) Kinematic properties : ( a ) Angle of reflection equals angle of incidence . sin
i n ' ( 6 ) Snell ' s law : = - , where i , r are the angles of incidence and refraction ,
while n , n ' are the corresponding indices of refraction . ( 2 ) Dynamic properties ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
RelativisticParticle Kinematics and Dynamics | 391 |
Copyright | |
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