## Classical electrodynamics |

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Page 210

7.5 A harmonic wave train of finite extent and its Fourier spectrum in

different frequency or

7.5 A harmonic wave train of finite extent and its Fourier spectrum in

**wave****number**. The pulse shown at t = 0 in Fig. 7.5 begins to move as time goes on. Thedifferent frequency or

**wave**-**number**components in it move at different phase ...Page 245

There will be a spectrum of eigenvalues yŁ and corresponding solutions yk A = 1,

2, 3, . . . , which form an orthogonal set. These different solutions are called the

modes of the guide. For a given frequency a>, the

There will be a spectrum of eigenvalues yŁ and corresponding solutions yk A = 1,

2, 3, . . . , which form an orthogonal set. These different solutions are called the

modes of the guide. For a given frequency a>, the

**wave number**k is determined ...Page 340

It is only for

10.106) («') that appreciable departures of the frequency from ODV occur. For

...

It is only for

**wave numbers**comparable to the Dehye**wave number**kD, kj = ^ (10.106) («') that appreciable departures of the frequency from ODV occur. For

**wave numbers**k < kD, the phase and group velocities of the longitudinal plasma...

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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