## Classical electrodynamics |

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Page 241

For simplicity, the cross-sectional size and shape are

the cylinder axis. With a sinusoidal time dependence e~lwt for the fields inside

the cylinder, Maxwell's equations take the form: V x E = i - B V • B VxB=— /ue-E

V-E ...

For simplicity, the cross-sectional size and shape are

**assumed**constant alongthe cylinder axis. With a sinusoidal time dependence e~lwt for the fields inside

the cylinder, Maxwell's equations take the form: V x E = i - B V • B VxB=— /ue-E

V-E ...

Page 297

The dimensions of the hole are

wavelength of the electromagnetic fields which are

of the sheet. The problem is to calculate the diffracted fields on the other side of

the ...

The dimensions of the hole are

**assumed**to be very small compared to awavelength of the electromagnetic fields which are

**assumed**to exist on one sideof the sheet. The problem is to calculate the diffracted fields on the other side of

the ...

Page 451

Then (13.83) becomes fdE\ dx'ieDl»l TT V Jo \e(w) W We shall take the simple

dielectric constant (7.93), augmented by some damping: e(ut) = 1 - "P2 (13.86) «2

+ The damping constant F will be

...

Then (13.83) becomes fdE\ dx'ieDl»l TT V Jo \e(w) W We shall take the simple

dielectric constant (7.93), augmented by some damping: e(ut) = 1 - "P2 (13.86) «2

+ The damping constant F will be

**assumed**small compared to wp. The necessary...

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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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### 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 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