## Classical electrodynamics |

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Page 182

Comparison of (6.47) with (6.49) shows that V— =47rJ, (6.51) dt Therefore the

source for the wave equation for A can be expressed entirely in terms of the

the ...

Comparison of (6.47) with (6.49) shows that V— =47rJ, (6.51) dt Therefore the

source for the wave equation for A can be expressed entirely in terms of the

**transverse**current (6.50): VA-l^.--^, (6.52) c2 dr c This is, of course, the origin ofthe ...

Page 243

Consequently the fields divide themselves into two distinct categories :

\s = 0

is dBt ...

Consequently the fields divide themselves into two distinct categories :

**TRANSVERSE**MAGNETIC (TM) B2 = 0 everywhere The boundary condition is Et\s = 0

**TRANSVERSE**ELECTRIC (TE) E, = 0 everywhere The boundary conditionis dBt ...

Page 639

containment of, by magnetic mirrors, 423 on transmission lines, 264, 265

wave guide, 263 spherical, 545

...

containment of, by magnetic mirrors, 423 on transmission lines, 264, 265

**Transverse**magnetic (TM) waves, ... 243 in cylindrical cavity, 254 in dielectricwave guide, 263 spherical, 545

**Transverse**waves, in conducting medium, 223 in...

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### Contents

Introduction to Electrostatics | 1 |

Scalar potential | 7 |

Greens theorem | 14 |

Copyright | |

19 other sections not shown

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### Common terms and phrases

4-vector acceleration angular distribution approximation assumed atomic 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 inversion 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 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