## 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 ...Page 126

If , however , the dielectric

If , however , the dielectric

**properties**are altered , € ( x ) + f ( x ) + de ( x ) ( 4.100 ) the contributions in ( 4.99 ) are not necessarily the same .Page 216

( 1 ) Kinematic

( 1 ) Kinematic

**properties**: ( a ) Angle of reflection equals angle of incidence . sin i n ' ( b ) Snell's law : where i , r are the angles of incidence sin ...### What people are saying - Write a review

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### Contents

Introduction to Electrostatics | 1 |

Greens theorem | 14 |

BoundaryValue Problems in Electrostatics I | 26 |

Copyright | |

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### Common terms and phrases

acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge charged particle classical collisions compared component conducting Consequently consider constant coordinates cross section cylinder defined density dependence derivative determine dielectric dimensions dipole direction discussed distance distribution effects electric field electromagnetic electron electrostatic energy equal equation example expansion expression factor force frame frequency function given gives incident inside integral involved limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative relativistic result satisfy scalar scattering shown in Fig shows side solution sphere spherical surface transformation unit vanishes vector velocity volume wave written