## Classical ElectrodynamicsProblems after each chapter |

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of the shape of the guide we can obtain the order of magnitude of the attenuation constant B , and exhibit completely its

of the shape of the guide we can obtain the order of magnitude of the attenuation constant B , and exhibit completely its

**frequency**dependence .Page 310

When the

When the

**frequency**of the applied fields is comparable to v ... Unfortunately at these same**frequencies**the description of collisions in terms of a ...Page

Consequently its spectrum will contain only a narrow range of

Consequently its spectrum will contain only a narrow range of

**frequencies**centered around yulb . In collision problems we must sum the**frequency**spectra ...### 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