## Classical Electrodynamics |

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Page 24

Use symmetry arguments and Gauss's law to prove that (a) the surface-charge

densities on the adjacent faces are

densities on the outer faces of the two sheets are the same; (c) the magnitudes of

...

Use symmetry arguments and Gauss's law to prove that (a) the surface-charge

densities on the adjacent faces are

**equal**and opposite; (b) the surface-chargedensities on the outer faces of the two sheets are the same; (c) the magnitudes of

...

Page 382

This magnetic field becomes almost

— 1. Even at nonrelativistic velocities where y o 1, this magnetic induction is

This magnetic field becomes almost

**equal**to the transverse electric field E, as B— 1. Even at nonrelativistic velocities where y o 1, this magnetic induction is

**equivalent**to B ~4 V × { (11.119) c ro which is just the Ampère-Biot–Savart ...Page 597

It is desirable to have an

order, has no grossly ... The smaller the particle's charge, the smaller the self-

fields, and the smaller the radiative effects, other things being

external ...

It is desirable to have an

**equivalent**equation of motion which is of the correctorder, has no grossly ... The smaller the particle's charge, the smaller the self-

fields, and the smaller the radiative effects, other things being

**equal**. If theexternal ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

References and suggested reading | 50 |

Copyright | |

16 other sections not shown

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acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge 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 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