## Classical Electrodynamics |

### From inside the book

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Page 209

25 ) , our subsequent discussion can apply equally well to electromagnetic

represents a harmonic

shows that ...

25 ) , our subsequent discussion can apply equally well to electromagnetic

**waves**, sound**waves**, de Broglie matter**waves**, etc . For the ... 27 ) If u ( x , 0 )represents a harmonic

**wave**eikot for all x , the orthogonality relation ( 2 . 52 )shows that ...

Page 363

The relativistic Doppler shift formulas can be obtained from the fact that the phase

of a light

invariant under a Lorentz transformation , the reason being that the phase can ...

The relativistic Doppler shift formulas can be obtained from the fact that the phase

of a light

**wave**is an invariant quantity . Actually , the phase of any plane**wave**isinvariant under a Lorentz transformation , the reason being that the phase can ...

Page 640

Transverse

204 Traveling

209, 215 use of, to obtain quantum-mechanical modifications, 440, 442, 453, 455

, ...

Transverse

**waves**, in magnetohydrodynamics, 331 in plasma, 226, 339 plane,204 Traveling

**wave**solutions, 203, 212 in**wave**guide, 244 Uncertainty principle,209, 215 use of, to obtain quantum-mechanical modifications, 440, 442, 453, 455

, ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

RelativisticParticle Kinematics and Dynamics | 391 |

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 charged particle classical collisions compared component conducting Consequently consider constant coordinates cross section cylinder defined density dependence 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 light limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means modes momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative relativistic result satisfy scalar scattering shown in Fig shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written