## Classical ElectrodynamicsProblems after each chapter |

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Since the Green's function , as a function of one of its variables , is a

Since the Green's function , as a function of one of its variables , is a

**potential**due to a unit point charge , this symmetry merely represents the ...Page 94

The segments are kept at fixed

The segments are kept at fixed

**potentials**V , alternately . ( a ) Set up a series representation for the**potential**inside the sphere for the general case of ...Page 95

3.5 A hollow sphere of inner radius a has the

3.5 A hollow sphere of inner radius a has the

**potential**specified on its surface to be Q = V ( 0 ° ) . Prove the equivalence of the two forms of solution ...### 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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### 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