## Classical ElectrodynamicsProblems after each chapter |

### From inside the book

Results 1-3 of 70

Page 155

5.9 , Gauss's theorem can be applied to V. B = 0 to yield ( B , – B ) : n = 0 ( 5.88 )

where n is the unit

the subscripts refer to values at the surface in the two media . If we now consider

...

5.9 , Gauss's theorem can be applied to V. B = 0 to yield ( B , – B ) : n = 0 ( 5.88 )

where n is the unit

**normal**to the surface directed from region 1 into region 2 , andthe subscripts refer to values at the surface in the two media . If we now consider

...

Page 238

If n is the unit

inward into the conductor , then the gradient operator can be written a af

neglecting the other derivatives when operating on the fields within the conductor

.

If n is the unit

**normal**outward from the conductor and Ğ is the**normal**coordinateinward into the conductor , then the gradient operator can be written a af

neglecting the other derivatives when operating on the fields within the conductor

.

Page 298

But far away from the hole ( in terms of its dimensions ) , although still “ near the

conducting plane , ” the fields will be the same as if the hole were not there ,

namely ,

shown ...

But far away from the hole ( in terms of its dimensions ) , although still “ near the

conducting plane , ” the fields will be the same as if the hole were not there ,

namely ,

**normal**E , and tangential B .. The electric field lines might appear asshown ...

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### Contents

Introduction to Electrostatics | 1 |

References and suggested reading | 23 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

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