## Classical ElectrodynamicsProblems after each chapter |

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Page 116

Fortunately , the simpler

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 ...Page 126

From ( 4.86 ) it is evident that the change in energy accompanying the changes p ( x ) and db ( x ) in charge density and potential is 3 ] [ ρδΦ + Φδρ ] dr ( 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 p ( x ) and db ( x ) in charge density and potential is 3 ] [ ρδΦ + Φδρ ] dr ( 4.99 ) Comparison with ( 4.87 ) shows that , if the dielectric

**properties**...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

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

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

TimeVarying Fields Maxwells Equations Con | 169 |

Copyright | |

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