## Classical Electrodynamics |

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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 334

But, if v 4 » c, then the phase velocity is

point of view of electromagnetic waves, the transverse Alfvén wave can be

thought of as a wave in a medium with an index of refraction given by u_4 = i (

10.85) Thus ...

But, if v 4 » c, then the phase velocity is

**equal**to the velocity of light. From thepoint of view of electromagnetic waves, the transverse Alfvén wave can be

thought of as a wave in a medium with an index of refraction given by u_4 = i (

10.85) Thus ...

Page 382

This magnetic field becomes almost

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

equivalent to B ~ 4 V × 5. - (11.119) c ro which is just the Ampère-Biot–Savart ...

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 ~ 4 V × 5. - (11.119) c ro which is just the Ampère-Biot–Savart ...

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### Contents

Introduction to Electrostatics | 1 |

References and suggested reading | 23 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

6 other sections not shown

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