## 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

cartesian coordinates, 141 of localized oscillating source, 269 f. of magnetic

dipole, 146 of oscillating electric dipole, 271 of oscillating electric quadrupole,

275 of ...

**Vector**potential, for time-varying fields, 179 in magnetostatics, 139 f. in non-cartesian coordinates, 141 of localized oscillating source, 269 f. of magnetic

dipole, 146 of oscillating electric dipole, 271 of oscillating electric quadrupole,

275 of ...

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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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