## Classical Electrodynamics |

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Page 12

This can be seen by letting the

inner side of the double layer . Then ( 1 . 26 ) says that the potential is 0 , = - 27D

since all of the solid angle comes from the immediate neighborhood of the point ...

This can be seen by letting the

**observation**point come infinitesimally close to theinner side of the double layer . Then ( 1 . 26 ) says that the potential is 0 , = - 27D

since all of the solid angle comes from the immediate neighborhood of the point ...

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 479

62 ) 872c ) J - 00 Since the

region of space where the acceleration occurs , the unit vector n is sensibly

constant in time . Furthermore the distance R ( t ' ) can be approximated as R ( t ' )

= x ...

62 ) 872c ) J - 00 Since the

**observation**point is assumed to be far away from theregion of space where the acceleration occurs , the unit vector n is sensibly

constant in time . Furthermore the distance R ( t ' ) can be approximated as R ( t ' )

= x ...

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### Contents

Introduction to Electrostatics | 1 |

References and suggested reading | 50 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

10 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 coefficients 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 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 space sphere spherical surface transformation unit vanishes vector velocity volume wave written