## Classical Electrodynamics |

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Page 258

x (Geometrical

total surface area. The Q of a cavity is evidently, apart from a geometrical

the ratio of the volume occupied by the fields to the volume of the conductor into ...

x (Geometrical

**factor**) (8.92)* pu,\Sö where V is the volume of the cavity, and S itstotal surface area. The Q of a cavity is evidently, apart from a geometrical

**factor**,the ratio of the volume occupied by the fields to the volume of the conductor into ...

Page 301

As the scattering angle departs from the forward direction the shadow integral will

vanish rapidly, both the exponential and the vector

the same tendency. On the other hand, the integral from the illuminated region ...

As the scattering angle departs from the forward direction the shadow integral will

vanish rapidly, both the exponential and the vector

**factor**in the integrand havingthe same tendency. On the other hand, the integral from the illuminated region ...

Page 606

... the same Lorentz shape as the scattering cross section, but is larger by a

T/T. At high frequencies T, -- oor, so that the absorption cross section approaches

the constant Thomson value (we have again ignored or compared to unity).

... the same Lorentz shape as the scattering cross section, but is larger by a

**factor**T/T. At high frequencies T, -- oor, so that the absorption cross section approaches

the constant Thomson value (we have again ignored or compared to unity).

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

5 other sections not shown

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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 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