## Classical electrodynamics |

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Page 220

E

2/ C°S '' ~ „ „ — sin 2i — sin 2r ,. £0 - f< _ tan (i — r) ~ ~»• sin 2r + sin 2/ tan (7.60)

Again the results on the right apply for p = p. For normal incidence (/ = 0), both ...

E

**PARALLEL**TO PLANE OF INCIDENCE £,/ - I fie sin 2i 2 cos i sin r sin 2r + . A*'2/ C°S '' ~ „ „ — sin 2i — sin 2r ,. £0 - f< _ tan (i — r) ~ ~»• sin 2r + sin 2/ tan (7.60)

Again the results on the right apply for p = p. For normal incidence (/ = 0), both ...

Page 412

The motion described by (12.93) is a circular motion perpendicular to B and a

uniform translation

v(0 = vfo + roaafo - ieje-***' (12.95) where e3 is a unit vector

The motion described by (12.93) is a circular motion perpendicular to B and a

uniform translation

**parallel**to B. The solution for the velocity is easily shown to bev(0 = vfo + roaafo - ieje-***' (12.95) where e3 is a unit vector

**parallel**to the field, ...Page 476

comparable

component is negligible (of order 1/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 1/y2) compared to that from the perpendicular

component ...

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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