## Classical ElectrodynamicsProblems after each chapter |

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Page 161

The nonlinear

The nonlinear

**relation**( 5.87 ) and the phenomenon of hysteresis allow the creation of permanent magnets . We can solve equations ( 5.112 ) for one**relation**...Page 234

Write the other dispersion

Write the other dispersion

**relation**, expressing the imaginary part as an integral over the real . ( b ) Show by direct calculation with the dispersion ...Page

... 512 Classical electron radius , 490 , 589 Clausius - Mossotti

... 512 Classical electron radius , 490 , 589 Clausius - Mossotti

**relation**, 119 Closure , see Completeness**relation**Collisions , between charged particles ...### 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 | |

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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