## Classical ElectrodynamicsProblems after each chapter |

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on one small charged body by a number of the other small charged bodies placed around it was the vector sum of the individual two - body

on one small charged body by a number of the other small charged bodies placed around it was the vector sum of the individual two - body

**forces**of Coulomb .Page 30

2.4 The

2.4 The

**force**acting on the charge q can be calculated in different ways . One ( the easiest ) way is to write down immediately the**force**between the charge ...Page 32

2.5 The

2.5 The

**force**on a point charge q due to an insulated , conducting sphere of radius a carrying a total charge Q. Positive values mean a repulsion , negative ...### What people are saying - Write a review

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### Contents

Introduction to Electrostatics | 1 |

References and suggested reading | 23 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

6 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 light limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means modes 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