## Classical ElectrodynamicsProblems after each chapter |

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The multiple - scattering

The multiple - scattering

**distribution**for the projected angle of scattering is 1 A12 PM ( 0 ' ) de ' = exp do ' ( 13.112 ) 7 ( 02 ) where both positive and ...Page

has inside of it a uniform volume

has inside of it a uniform volume

**distribution**of charge totaling Q. The small parameter ß varies harmonically in time at frequency w .Page

Quadrupole moment , nuclear , 102 of oscillating source , 275 see also Multipole moment Power , radiated , angular

Quadrupole moment , nuclear , 102 of oscillating source , 275 see also Multipole moment Power , radiated , angular

**distribution**of quadrupole , 275 , 552 ...### 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