## Classical ElectrodynamicsProblems after each chapter |

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Page 91

The general theory of dual

The general theory of dual

**integral**equations is complicated and not highly ... by using certain discontinuous**integrals**involving Bessel functions .Page 284

To do this we make use of the following easily proved identities connecting surface

To do this we make use of the following easily proved identities connecting surface

**integrals**over a closed surface Sto volume**integrals**over the interior ...Page 301

respectively ; the shadow

respectively ; the shadow

**integral**will be large and the**integral**from the illuminated region will go to zero . As the scattering angle departs from the ...### 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 sphere spherical surface transformation unit vanishes vector velocity volume wave written