## Classical Electrodynamics |

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Page 299

9.10

type of problem which is essentially diffraction is the

obstacle. We will consider the

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 anobstacle. We will consider the

**scattering**of a plane electromagnetic wave by a ...Page 458

The multiple-

6') d6' = #) d6' (13.112) 1 — exp (– Vm (0°) (0°) where both positive and negative

values of 0' are considered. The smallangle Rutherford formula (13.92) can be ...

The multiple-

**scattering**distribution for the projected angle of**scattering**1S r2 PM(6') d6' = #) d6' (13.112) 1 — exp (– Vm (0°) (0°) where both positive and negative

values of 0' are considered. The smallangle Rutherford formula (13.92) can be ...

Page 569

16.9

wave of electromagnetic radiation is incident on a spherical obstacle, as

indicated schematically in Fig. 16.5, it is

scatterer the ...

16.9

**Scattering**of Electromagnetic Waves by a Conducting Sphere If a planewave of electromagnetic radiation is incident on a spherical obstacle, as

indicated schematically in Fig. 16.5, it is

**scattered**so that far away from thescatterer the ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

Multipoles Electrostatics of Macroscopic Media | 98 |

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 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