## Classical ElectrodynamicsProblems after each chapter |

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Page 12

This can be seen by letting the

This can be seen by letting the

**observation**point come infinitesimally close to the double layer . The double layer is now imagined to consist of two parts , one being a small disc directly under the**observation**point .Page 292

Then the

Then the

**observation**point may be in the near zone , less than a wavelength away from the diffracting system . The near - zone fields are complicated in structure and of little interest . Points many wavelengths away from the ...Page 531

Then , in the dipole approximation , the appropriate intensity distribution is di ( w ) d92 09 40 % C3 S. - nx Meiwt dll ( 15.80 ) This gives dl ( 0 ) dΩ w2 sin 47 % C342 ( 15.81 ) where is the angle between de and the

Then , in the dipole approximation , the appropriate intensity distribution is di ( w ) d92 09 40 % C3 S. - nx Meiwt dll ( 15.80 ) This gives dl ( 0 ) dΩ w2 sin 47 % C342 ( 15.81 ) where is the angle between de and the

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

TimeVarying Fields Maxwells Equations Con | 169 |

Copyright | |

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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