## Classical electrodynamics |

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Page 258

For p = 0 modes, (8.91) must be multiplied by 2 and £, replaced by 2fA. This

expression for Q has an intuitive physical interpretation when written in the form :

Q = -I — I X (Geometrical

its ...

For p = 0 modes, (8.91) must be multiplied by 2 and £, replaced by 2fA. This

expression for Q has an intuitive physical interpretation when written in the form :

Q = -I — I X (Geometrical

**factor**) (8.92)* where Kis the volume of the cavity, and Sits ...

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

We see that near the resonant frequency eo0 the absorption cross section has

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

</F. At high frequencies F< — »• MZT, so that the absorption cross section ...

We see that near the resonant frequency eo0 the absorption cross section has

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

**factor**F</F. At high frequencies F< — »• MZT, so that the absorption cross section ...

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### Contents

Introduction to Electrostatics | 1 |

Scalar potential | 7 |

Greens theorem | 14 |

Copyright | |

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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