## Classical electrodynamics |

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Page 313

The effects are both electromagnetic and mechanical. We first consider the

electromagnetic effects. We will see that, depending on the conductivity, quite

different behaviors of the fields occur. The time dependence of the

can be ...

The effects are both electromagnetic and mechanical. We first consider the

electromagnetic effects. We will see that, depending on the conductivity, quite

different behaviors of the fields occur. The time dependence of the

**magnetic field**can be ...

Page 382

induction in the xz direction. This

transverse electric field Łt as /S -»• 1. Even at nonrelativistic velocities where y ~

1, this magnetic induction is equivalent to „ a v x r B ~ c r3 (11.119) which is just

the ...

induction in the xz direction. This

**magnetic field**becomes almost equal to thetransverse electric field Łt as /S -»• 1. Even at nonrelativistic velocities where y ~

1, this magnetic induction is equivalent to „ a v x r B ~ c r3 (11.119) which is just

the ...

Page 427

12.9 A particle of mass m and charge e moves in the laboratory in crossed, static,

uniform, electric and

// axis. (a) For |E/ < /B| make the necessary Lorentz transformation described in ...

12.9 A particle of mass m and charge e moves in the laboratory in crossed, static,

uniform, electric and

**magnetic fields**. E is parallel to the x axis; B is parallel to the// axis. (a) For |E/ < /B| make the necessary Lorentz transformation described 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