## Classical Electrodynamics |

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Page 213

This means that at times immediately before t = 0 the wave consisted of two

pulses, both moving towards the

shape given by (7.38). Clearly at later times we expect each pulse to re-emerge

on ...

This means that at times immediately before t = 0 the wave consisted of two

pulses, both moving towards the

**origin**, such that at t = 0 they coalesced into theshape given by (7.38). Clearly at later times we expect each pulse to re-emerge

on ...

Page 436

Consequently AE = es V - E dt (13.22) where v = x, and in the dipole

approximation E is the field of the incident particle at the

Fourier representations (13.16) and (13.17), as well as that for a delta function (

2.52), and the ...

Consequently AE = es V - E dt (13.22) where v = x, and in the dipole

approximation E is the field of the incident particle at the

**origin**O. Using theFourier representations (13.16) and (13.17), as well as that for a delta function (

2.52), and the ...

Page 482

... loss of generality to lie in the z-z plane, making an angle 6 (the colatitude) with

the r axis. Only for very small 0 will there be appreciable radiation intensity. The

... loss of generality to lie in the z-z plane, making an angle 6 (the colatitude) with

the r axis. Only for very small 0 will there be appreciable radiation intensity. The

**origin**of time is chosen so that at t = 0 the particle is at the**origin**of coordinates.### What people are saying - Write a review

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### Contents

Introduction to Electrostatics | 1 |

References and suggested reading | 23 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

6 other sections not shown

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