## Classical ElectrodynamicsProblems after each chapter |

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Page 31

2.3 Point Charge in the Presence of a Charged , Insulated , Conducting

2.3 Point Charge in the Presence of a Charged , Insulated , Conducting

**Sphere**In the previous section we considered the problem of a point charge q near a ...Page 39

As a very simple example of the solution of a potential problem by inversion we consider an isolated conducting

As a very simple example of the solution of a potential problem by inversion we consider an isolated conducting

**sphere**of radius R with a total charge Q on ...Page 638

**Spherical**wave expansion, of E and B, 546 Stokes's theorem, 9 Stored energy in ... by conducting**sphere**, at long wavelengths, 569 f. by conducting**sphere**, ...### 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