## Classical ElectrodynamicsProblems after each chapter |

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Page 52

2.7 A line charge with linear charge density is placed parallel to , and a distance R away from , the axis of a conducting

2.7 A line charge with linear charge density is placed parallel to , and a distance R away from , the axis of a conducting

**cylinder**of radius b held at fixed voltage such that the potential vanishes at infinity .Page 259

8.8 Dielectric Wave Guides In Sections 8.2-8.5 we considered wave guides made of hollow metal

8.8 Dielectric Wave Guides In Sections 8.2-8.5 we considered wave guides made of hollow metal

**cylinders**with fields only ... which arise because of the very different boundary conditions to be satisfied at the surface of the**cylinder**.Page 260

The axial propagation constant k must be the same inside and outside the

The axial propagation constant k must be the same inside and outside the

**cylinder**in order to satisfy boundary conditions at all points on the surface at all times . In the usual way , inside the dielectric**cylinder**the transverse ...### What people are saying - Write a review

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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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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 light limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means modes 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 shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written