## Classical electrodynamics |

### From inside the book

Results 1-3 of 80

Page 220

E

,. sin (i + r) cos (i — r) r sin 2r + — sin 2i „ „ — sin 2i — sin 2r ,. . £0 _ j« _ tan (i — r

) • i sin 2r , i" • -•• tan(i + r) + — sin 2i (7.60) Again the results on the right apply ...

E

**PARALLEL**TO PLANE OF INCIDENCE £,/ _ 0 / pe sin 2i 2 cos i sin r ,«'e' • , . u .,. sin (i + r) cos (i — r) r sin 2r + — sin 2i „ „ — sin 2i — sin 2r ,. . £0 _ j« _ tan (i — r

) • i sin 2r , i" • -•• tan(i + r) + — sin 2i (7.60) Again the results on the right apply ...

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/ > ...

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 /E/ > ...

Page 476

comparable

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

component.

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### Contents

Introduction to Electrostatics | 1 |

Scalar potential | 7 |

Greens theorem | 14 |

Copyright | |

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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