## 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 ...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 inside the hollow .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 ...### 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