## Classical Electrodynamics |

### From inside the book

Results 1-3 of 75

Page 24

Use symmetry arguments and Gauss's law to prove that (a) the surface-charge

densities on the adjacent faces are

densities on the outer faces of the two sheets are the same; (c) the magnitudes of

...

Use symmetry arguments and Gauss's law to prove that (a) the surface-charge

densities on the adjacent faces are

**equal**and opposite; (b) the surface-chargedensities on the outer faces of the two sheets are the same; (c) the magnitudes of

...

Page 358

... at the same time t. From (11.19) the length in K' is which is moving with uniform

velocity v relative to the. r 22 – 21 L J - J -o C C which is just the FitzGerald-

Lorentz result (11.10). Note that in the system K the length is defined at

times t.

... at the same time t. From (11.19) the length in K' is which is moving with uniform

velocity v relative to the. r 22 – 21 L J - J -o C C which is just the FitzGerald-

Lorentz result (11.10). Note that in the system K the length is defined at

**equal**times t.

Page

This magnetic field becomes almost

— 1. Even at nonrelativistic velocities where y c 1, this magnetic induction is

equivalent to B ~ 17 × { (11.119) c ro which is just the Ampère-Biot–Savart

expression ...

This magnetic field becomes almost

**equal**to the transverse electric field El as B— 1. Even at nonrelativistic velocities where y c 1, this magnetic induction is

equivalent to B ~ 17 × { (11.119) c ro which is just the Ampère-Biot–Savart

expression ...

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### Contents

Introduction to Electrostatics | 1 |

Nº 3 | 3 |

Greens theorem | 14 |

Copyright | |

30 other sections not shown

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