## Classical Electrodynamics |

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Page 10

23 ) Is lx – x ' Another problem of interest is the potential due to a

distribution on a surface S . A

letting the surface S have a surface - charge density g ( x ) on it , and another ...

23 ) Is lx – x ' Another problem of interest is the potential due to a

**dipole**- layerdistribution on a surface S . A

**dipole**layer can be imagined as being formed byletting the surface S have a surface - charge density g ( x ) on it , and another ...

Page 274

33 ) where m is the magnetic

= 20 J The fields can be determined by noting that the vector potential ( 9 . 33 ) is

proportional to the magnetic induction ( 9 . 18 ) for an electric

33 ) where m is the magnetic

**dipole**moment , m = s . u & r = [ xx J ) de ( 9 . 34 ) m= 20 J The fields can be determined by noting that the vector potential ( 9 . 33 ) is

proportional to the magnetic induction ( 9 . 18 ) for an electric

**dipole**.Page 628

... see Time dilatation Dimensions, discussion of, 611

energy loss, 435 in radiation problems, 271, 274, 507

100 magnetostatic, 143, 147 of conducting sphere, 34 of dielectric sphere, 115 of

...

... see Time dilatation Dimensions, discussion of, 611

**Dipole**approximation, inenergy loss, 435 in radiation problems, 271, 274, 507

**Dipole**fields, electrostatic,100 magnetostatic, 143, 147 of conducting sphere, 34 of dielectric sphere, 115 of

...

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### Contents

Introduction to Electrostatics | 1 |

References and suggested reading | 23 |

Wave Guides and Resonant Cavities | 235 |

Copyright | |

5 other sections not shown

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