## Classical ElectrodynamicsProblems after each chapter |

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Page 51

PROBLEMS 2.1 A point charge q is brought to a position a distance d away from an infinite

PROBLEMS 2.1 A point charge q is brought to a position a distance d away from an infinite

**plane**conductor held at zero potential .Page 220

E PARALLEL TO

E PARALLEL TO

**PLANE**OF INCIDENCE E. EO = 2 € sin 2 i μ'ε ' ' sin 2r + M 2 cos i sin r sin ( i + r ) cos ( i – r ) sin 2i M ( 7.60 ) sin 2i sin 2r E. " E.Page 307

9.7 A linearly polarized

9.7 A linearly polarized

**plane**wave of amplitude E , and wave number k is incident on a circular opening of radius a in an otherwise perfectly conducting ...### 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