## Classical electrodynamics |

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Page 310

When the

time to accelerate and decelerate between collisions. Then inertia! effects enter

and the conductivity becomes complex. Unfortunately at these same

...

When the

**frequency**of the applied fields is comparable to v, the electrons havetime to accelerate and decelerate between collisions. Then inertia! effects enter

and the conductivity becomes complex. Unfortunately at these same

**frequencies**...

Page 477

14.7 Radiating particle illuminates the detector at O only for a time Ar. The

arbitrary motion it plays the role of a fundamental

14.50) ...

14.7 Radiating particle illuminates the detector at O only for a time Ar. The

**frequency**spectrum thus contains**frequencies**up to a maximum wc ~ (Ar)~'. forarbitrary motion it plays the role of a fundamental

**frequency**of motion. Equation (14.50) ...

Page 485

Then we find (14.85) This critical

estimate (14.50) of Section 14.4. If the motion of the charge is truly circular, then c

/p is the fundamental

Then we find (14.85) This critical

**frequency**is seen to agree with our qualitativeestimate (14.50) of Section 14.4. If the motion of the charge is truly circular, then c

/p is the fundamental

**frequency**of rotation, w0. Then we can define a critical ...### What people are saying - Write a review

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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 Babinet's principle behavior 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 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 screen shown in Fig shows solid angle solution spectrum spherical surface theorem transverse unit vanishes vector potential wave equation wave number wavelength written zero