## Classical Electrodynamics |

### From inside the book

Results 1-3 of 82

Page 172

If the circuit C is

, the total time derivative in ( 6 . 4 ) must take into account this motion . The flux

through the circuit may change because ( a ) the flux changes with time at a point

...

If the circuit C is

**moving**with a velocity v in some direction , as shown in Fig . 6 . 2, the total time derivative in ( 6 . 4 ) must take into account this motion . The flux

through the circuit may change because ( a ) the flux changes with time at a point

...

Page 503

( Note that for a real circuit the stationary positive ions in the conductors will

produce an electric field which just cancels that due to the

13 Assume that the instantaneous power spectrum radiated by an electron in a ...

( Note that for a real circuit the stationary positive ions in the conductors will

produce an electric field which just cancels that due to the

**moving**charges . ) 14 .13 Assume that the instantaneous power spectrum radiated by an electron in a ...

Page 630

... Radiation Fresnel diffraction, see Diffraction Fresnel formula for velocity of light

in

219, 220 Fresnel integrals and diffraction, 306 Galilean invariance, 348, 369 and

...

... Radiation Fresnel diffraction, see Diffraction Fresnel formula for velocity of light

in

**moving**media, 349 Fresnel formulas for reflected and refracted plane waves,219, 220 Fresnel integrals and diffraction, 306 Galilean invariance, 348, 369 and

...

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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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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