## Classical ElectrodynamicsProblems after each chapter |

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Page 12

This can be seen by letting the

double layer . The double layer is now imagined to consist of two parts , one

being a small disc directly under the

small ...

This can be seen by letting the

**observation**point come infinitesimally close to thedouble layer . The double layer is now imagined to consist of two parts , one

being a small disc directly under the

**observation**point . The disc is sufficientlysmall ...

Page 292

Then the

away from the diffracting system . The near - zone fields are complicated in

structure and of little interest . Points many wavelengths away from the diffracting

system ...

Then the

**observation**point may be in the near zone , less than a wavelengthaway from the diffracting system . The near - zone fields are complicated in

structure and of little interest . Points many wavelengths away from the diffracting

system ...

Page 531

It is easy to show that on averaging over this precession sin in ( 15.81 ) becomes

equal to its average value of s , independent of

angular and frequency spectrum becomes diw ) e2 hos ) ( 15.82 ) dΩ 87 ° c \ mco

...

It is easy to show that on averaging over this precession sin in ( 15.81 ) becomes

equal to its average value of s , independent of

**observation**direction . Thus theangular and frequency spectrum becomes diw ) e2 hos ) ( 15.82 ) dΩ 87 ° c \ mco

...

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### Contents

Introduction to Electrostatics | 1 |

References and suggested reading | 23 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

6 other sections not shown

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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