## Classical ElectrodynamicsProblems after each chapter |

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Page 63

If the point x is on the z

If the point x is on the z

**axis**, the right - hand side reduces to ( 3.38 ) , while the left - hand side becomes : 1 1 | x – X'l 1 ir – p ' !Page 166

( c ) Show that at the end of a long solenoid the magnetic induction near the

( c ) Show that at the end of a long solenoid the magnetic induction near the

**axis**has components 20NI πΝΙ B , - B , – > El ...Page 422

The speed of the particle is constant so that at any position along the z

The speed of the particle is constant so that at any position along the z

**axis**v ,? + v2 = 0 v 2 ( 12.126 ) where v.2 = 0.02 + 0,10 % 2 is the square of the ...### 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