## 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

But for reasonable thicknesses such that the particle does not lose appreciable

energy, the Gaussian will still be peaked at very small forward angles. The

multiple-

= exp ...

But for reasonable thicknesses such that the particle does not lose appreciable

energy, the Gaussian will still be peaked at very small forward angles. The

multiple-

**scattering**distribution for the projected angle of**scattering**PM(6') dQ' = -J= exp ...

Page 459

13.8 Multiple and single

of plural

the small-angle multiple

13.8 Multiple and single

**scattering**distributions of projected angle. In the regionof plural

**scattering**(a ~ 2-3) the dotted curve indicates the smooth transition fromthe small-angle multiple

**scattering**(approximately Gaussian in shape) to the ...### What people are saying - Write a review

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### Contents

Introduction to Electrostatics | 1 |

Scalar potential | 7 |

Greens theorem | 14 |

Copyright | |

17 other sections not shown

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### Common terms and phrases

4-vector acceleration angular distribution approximation assumed atomic average axis behavior Bessel functions boundary conditions bremsstrahlung calculate Chapter charge density charge q charged particle classical coefficients collisions component conductor Consequently consider coordinates cross section current density cylinder defined delta function dielectric constant diffraction dimensions dipole direction discussed effects electric field electromagnetic fields electron electrostatic emitted energy loss expansion expression factor force equation frequency given Green's function impact parameter incident particle inside integral Laplace's equation limit linear Lorentz invariant Lorentz transformation macroscopic magnetic field magnetic induction magnitude Maxwell's equations meson molecules momentum multipole multipole expansion nonrelativistic obtain orbit oscillations parallel perpendicular photon plane wave plasma point charge polarization power radiated problem quantum quantum-mechanical radiative radius region relativistic result scalar scattering shown in Fig shows solid angle solution spectrum spherical surface theorem transverse vanishes vector potential wave equation wave number wavelength written zero