## Classical ElectrodynamicsProblems after each chapter |

### From inside the book

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Page 234

Just

Just

**inside**the dielectric the boundary values of the tangential electric field and its normal derivative are u ( 0 , 1 ) = 0 ( t ) e - et cos wot ди . won ...Page 236

Then , just as in the static case , there is no electric field

Then , just as in the static case , there is no electric field

**inside**the conductors . The charges**inside**a perfect conductor are assumed to be so mobile ...Page 639

... 9, 110 and electrostatic force, 23 effective magnetic, 159 on conducting sphere, 29, 34 on perfect conductor, 236 on sphere with line charge

... 9, 110 and electrostatic force, 23 effective magnetic, 159 on conducting sphere, 29, 34 on perfect conductor, 236 on sphere with line charge

**inside**, ...### 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 | |

9 other sections not shown

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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