## Classical ElectrodynamicsProblems after each chapter |

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For neutral particles with no detectable electromagnetic interactions it is clearly impossible to obtain their relativistic transformation ... A

For neutral particles with no detectable electromagnetic interactions it is clearly impossible to obtain their relativistic transformation ... A

**charged particle**can be thought of as a very localized distribution of charge and mass .Page

The sudden creation of a fast electron in nuclear beta decay , for example , can be viewed for our purposes as the violent acceleration of a

The sudden creation of a fast electron in nuclear beta decay , for example , can be viewed for our purposes as the violent acceleration of a

**charged particle**initially at rest to some final velocity in a very short time interval ...Page

It exploits the similarity between the fields of a rapidly moving

It exploits the similarity between the fields of a rapidly moving

**charged particle**and the fields of a pulse of radiation ( see Section 11.10 ) and correlates the effects of the collision of the relativistic**charged particle**with some ...### 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 space sphere spherical surface transformation unit vanishes vector velocity volume wave written