## Classical ElectrodynamicsProblems after each chapter |

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Page 86

If we let x ' → 0 , only the m = 0 term survives , and we

If we let x ' → 0 , only the m = 0 term survives , and we

**obtain**the integral representation : 1 2 cos kz Kolkp ) dk ( 3.150 ) p2 + 2 za If we replace p in ( 3.150 ) by R2 = pa + ...Page 403

NI O ' it is a straightforward , although tedious , matter to

NI O ' it is a straightforward , although tedious , matter to

**obtain**the result : ma ) ? ? – ma ( El + mo ) ( m , E , + 2 , – ? mg m ? 2 ( E2 + m2 ) ? – pe cosa 0 , Eg ( 12.53 ) Only the values of ( 12.53 ) greater than my have physical ...Page 498

Then we

Then we

**obtain**e " diw ) dΩ In x v2 v ( ** ) ai ( 14.127 ) 03 с The integral is a Dirac delta function . Then di ( 0 ) exe'p2 sin 0 18 ( 1 – ( " ß cos 0 ) 2 ( 14.128 ) dΩ where 0 is measured relative to the velocity v .### 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 | |

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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