## Classical Electrodynamics |

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Page 299

9.10 Scattering by a Conducting Sphere in the Short-Wavelength

type of problem which is essentially diffraction is the scattering of waves by an

obstacle. We will consider the scattering of a plane electromagnetic wave by a ...

9.10 Scattering by a Conducting Sphere in the Short-Wavelength

**Limit**Anothertype of problem which is essentially diffraction is the scattering of waves by an

obstacle. We will consider the scattering of a plane electromagnetic wave by a ...

Page 447

We will content ourselves with the extreme relativistic

since ... Consequently we can approximate the Bessel functions by their small

argument

is ...

We will content ourselves with the extreme relativistic

**limit**(3 - 1). Furthermore,since ... Consequently we can approximate the Bessel functions by their small

argument

**limits**(3.103). Then in the relativistic**limit**the Fermi expression (13.70)is ...

Page 598

The first integral is therefore et/7 C r mW(t) = “s e-"F(t') dt' (17.50) T J t The minus

sign of the preceding line has been absorbed by making the lower

integral the indefinite one. The constant of integration C is to be determined on ...

The first integral is therefore et/7 C r mW(t) = “s e-"F(t') dt' (17.50) T J t The minus

sign of the preceding line has been absorbed by making the lower

**limit**of theintegral the indefinite one. The constant of integration C is to be determined on ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

BoundaryValue Problems in Electrostatics II | 54 |

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 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 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