## Classical Electrodynamics |

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E

sin 2r + * sin 2i o" (i + r.) cos (i — r) pr * sin 2i — sin 2r - (7.60) Eo" — 4 -> tan (i —

r) * in 2, 14 in 2: "( t ) Au Again the results on the right apply for u' = u. For normal

...

E

**PARALLEL**TO PLANE OF INCIDENCE * = 2 Le sin 2i —o- 2 cos i sin r Eo **sin 2r + * sin 2i o" (i + r.) cos (i — r) pr * sin 2i — sin 2r - (7.60) Eo" — 4 -> tan (i —

r) * in 2, 14 in 2: "( t ) Au Again the results on the right apply for u' = u. For normal

...

Page

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 r axis; B is**parallel**to the y 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

comparable

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

component.

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### Contents

Introduction to Electrostatics | 1 |

Nš 3 | 3 |

Greens theorem | 14 |

Copyright | |

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### Common terms and phrases

acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge classical collisions compared component conducting conductor Consequently consider constant coordinates cross section cylinder defined density depends derivative determine dielectric dimensions dipole direction discussed distance distribution effects electric field electromagnetic electron electrostatic energy equal equation example expansion expression factor force frame frequency function given gives incident inside integral involved limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative result satisfy scalar scattering shows side simple solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written