## Classical electrodynamics |

### From inside the book

Results 1-3 of 84

Page 427

E is

necessary Lorentz transformation described in Section 12.8 to obtain explicitly

parametric equations for the particle's trajectory. (b) Repeat the calculation of (a)

for ...

E is

**parallel**to the x axis; B is**parallel**to the ,</ axis. (a) For |E| < |B| make thenecessary Lorentz transformation described in Section 12.8 to obtain explicitly

parametric equations for the particle's trajectory. (b) Repeat the calculation of (a)

for ...

Page 476

comparable

component is negligible (of order I/y2) compared to that from the perpendicular

component.

**parallel**to and perpendicular to the velocity. But we have just seen that forcomparable

**parallel**and perpendicular forces the radiation from the**parallel**component is negligible (of order I/y2) compared to that from the perpendicular

component.

Page 575

16.3 The uniform charge density of Problem 16.2 is replaced by a uniform density

of intrinsic magnetization

M. With the same approximations as above calculate the nonvanishing ...

16.3 The uniform charge density of Problem 16.2 is replaced by a uniform density

of intrinsic magnetization

**parallel**to the z axis and having total magnetic momentM. With the same approximations as above calculate the nonvanishing ...

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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