## Classical ElectrodynamicsProblems after each chapter |

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Page 24

If

If

**equal**and opposite charges are placed on the conductors , there will be a certain difference of potential between them . The ratio of the magnitude of the charge on one conductor to the magnitude of the potential difference is called ...Page 358

From ( 11.19 ) the length in K ' is 22 21 L Lo = zz ' – 2 ' ( 11.22 ) v2 c2 c2 which is just the FitzGerald - Lorentz result ( 11.10 ) . Note that in the system K the length is defined at

From ( 11.19 ) the length in K ' is 22 21 L Lo = zz ' – 2 ' ( 11.22 ) v2 c2 c2 which is just the FitzGerald - Lorentz result ( 11.10 ) . Note that in the system K the length is defined at

**equal**times t .Page

This magnetic field becomes almost

This magnetic field becomes almost

**equal**to the transverse electric field E , as ß → 1. Even at nonrelativistic velocities where y - 1 , this magnetic induction is equivalent to B ~ чухг ( 11.119 ) с p3 which is just the Ampère - Biot ...### 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 | |

11 other sections not shown

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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 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