## Classical Electrodynamics |

### From inside the book

Results 1-3 of 73

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 263

Hence the lowest “cutoff” frequency for TEo, waves is given by =-“– (8.109) (t) 01

Vel – so a At this frequency B" = 0, but the axial wave number k is still real and

the ...

Hence the lowest “cutoff” frequency for TEo, waves is given by =-“– (8.109) (t) 01

Vel – so a At this frequency B" = 0, but the axial wave number k is still real and

**equal**to its free-space value Vevolc. Immediately below this “cutoff.” frequency,the ...

Page 382

This magnetic field becomes almost

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

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

This magnetic field becomes almost

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

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

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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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