## Classical Electrodynamics |

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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,

or (b) ...

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,

or (b) ...

Page 503

14.12 As an idealization of steady-state currents flowing in a circuit, consider a

system of N identical charges q

accelerations) in an arbitrary closed path. Successive charges are separated by

a ...

14.12 As an idealization of steady-state currents flowing in a circuit, consider a

system of N identical charges q

**moving**with constant speed v (but subject toaccelerations) in an arbitrary closed path. Successive charges are separated by

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 |

References and suggested reading | 50 |

Copyright | |

16 other sections not shown

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