## Classical electrodynamics |

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Page 283

9.6 Vector Equivalents of Kirchhoff Integral To obtain vector equivalents to the

Kirchhoff integral (9.63) we first note that with the definition, 1 e*R G(x, x') = j- e—

(9.66) 477r R the scalar form (9.63) can be

...

9.6 Vector Equivalents of Kirchhoff Integral To obtain vector equivalents to the

Kirchhoff integral (9.63) we first note that with the definition, 1 e*R G(x, x') = j- e—

(9.66) 477r R the scalar form (9.63) can be

**written**f y(x) = 9 [Gn • V'y; — y>n • V'G]...

Page 377

4-vectors will be denoted by A^ with (A^, At, A3) the components of a space

vector A and At = iA0. This correspondence will sometimes be

(11.95) Sometimes the subscript on the 4-vector will be omitted, e.g. f(x) means /(

x,/).

4-vectors will be denoted by A^ with (A^, At, A3) the components of a space

vector A and At = iA0. This correspondence will sometimes be

**written**Afl = (\JA0)(11.95) Sometimes the subscript on the 4-vector will be omitted, e.g. f(x) means /(

x,/).

Page 395

The conservation of energy and momentum in the two-body decay can be

as a 4-vector equation : P = pl+p2 (12.17) where the 4-vector subscript fj. on each

symbol has been suppressed. The squares of the 4-vector momenta are the ...

The conservation of energy and momentum in the two-body decay can be

**written**as a 4-vector equation : P = pl+p2 (12.17) where the 4-vector subscript fj. on each

symbol has been suppressed. The squares of the 4-vector momenta are the ...

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### Contents

Introduction to Electrostatics | 1 |

Scalar potential | 7 |

Greens theorem | 14 |

Copyright | |

18 other sections not shown

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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 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