## Classical Electrodynamics |

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Page 193

Evidently the terms in the volume integral (6.93) transform like

momentum, instead of the vectorial form (6.93), the tensor can be handled within

the framework of

tensor ...

Evidently the terms in the volume integral (6.93) transform like

**vectors**. ... ofmomentum, instead of the vectorial form (6.93), the tensor can be handled within

the framework of

**vector**operations by introducing a corresponding dyadic. If atensor ...

Page 307

Make a sketch of I as a function of X for fixed Z. (c) Use the

to obtain a result equivalent to that of part (a). Compare the two expressions. A

linearly polarized plane wave of amplitude Eo and wave number k is incident on

a ...

Make a sketch of I as a function of X for fixed Z. (c) Use the

**vector**formula (9.82)to obtain a result equivalent to that of part (a). Compare the two expressions. A

linearly polarized plane wave of amplitude Eo and wave number k is incident on

a ...

Page 640

... 199

harmonics, 556, 568 Wave packets, spreading in time, 215 Waves, Alfven, 331,

344.

... 199

**Vector**Green's theorem, 283 f.**Vector**potential, for time-varying fields, 179**Vector**theorem, with surface and volume integrals, 284 with**vector**sphericalharmonics, 556, 568 Wave packets, spreading in time, 215 Waves, Alfven, 331,

344.

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### Contents

Introduction to Electrostatics | 1 |

Greens theorem | 14 |

BoundaryValue Problems in Electrostatics I | 26 |

Copyright | |

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