## Classical ElectrodynamicsProblems after each chapter |

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Make a sketch of I as a function of X for fixed Z. ( c ) Use the vector formula ( 9.82 ) to obtain a

Make a sketch of I as a function of X for fixed Z. ( c ) Use the vector formula ( 9.82 ) to obtain a

**result**equivalent to that of part ( a ) .Page

ot be below which our approximate

ot be below which our approximate

**result**( 13.2 ) must be replaced by a more exact expression which tends to ( 13.5 ) as b 0. It can be shown ( Problem 13.1 ) ...Page

O angular dependence which is a wellknown

O angular dependence which is a wellknown

**result**. We note from ( 14.18 ) that the radiation is polarized in the plane containing ý and n .### 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