## Classical ElectrodynamicsProblems after each chapter |

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Page 116

Fortunately , the simpler

analysis . Before examining how the detailed

related to the susceptibility we must make a distinction between the fields acting

on the ...

Fortunately , the simpler

**properties**of dielectrics are amenable to classicalanalysis . Before examining how the detailed

**properties**of the molecules arerelated to the susceptibility we must make a distinction between the fields acting

on the ...

Page 126

From ( 4.86 ) it is evident that the change in energy accompanying the changes

dp ( x ) and 80 ( x ) in charge density and potential is δW = 3 [ ρδΦ + Φδρ ] d8α (

4.99 ) Comparison with ( 4.87 ) shows that , if the dielectric

From ( 4.86 ) it is evident that the change in energy accompanying the changes

dp ( x ) and 80 ( x ) in charge density and potential is δW = 3 [ ρδΦ + Φδρ ] d8α (

4.99 ) Comparison with ( 4.87 ) shows that , if the dielectric

**properties**...Page 216

( 1 ) Kinematic

i n ' ( b ) Snell's law : where i , r are the angles of incidence sin r and refraction ,

while n , n ' are the corresponding indices of refraction . ( 2 ) Dynamic

( 1 ) Kinematic

**properties**: ( a ) Angle of reflection equals angle of incidence . sini n ' ( b ) Snell's law : where i , r are the angles of incidence sin r and refraction ,

while n , n ' are the corresponding indices of refraction . ( 2 ) Dynamic

**properties**...### What people are saying - Write a review

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

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