## Classical Electrodynamics |

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Page 269

The electromagnetic potentials and fields are assumed to have the same time

(x, t) in the Lorentz gauge is A(x, t) = Jersar J(x', t') •(r + B = <! — i) (9.2) c c |x — x"|

...

The electromagnetic potentials and fields are assumed to have the same time

**dependence**. It was shown in Chapter 6 that the solution for the vector potential A(x, t) in the Lorentz gauge is A(x, t) = Jersar J(x', t') •(r + B = <! — i) (9.2) c c |x — x"|

...

Page 296

Both formulas contain the same “diffraction” distribution factor [J.(kaš)|kaśl and

the same

.

Both formulas contain the same “diffraction” distribution factor [J.(kaš)|kaśl and

the same

**dependence**on wave number. But the scalar result has no azimuthal**dependence**(apart from that contained in 5), whereas the vector expression does.

Page 553

Furthermore, we assume that the time

Fourier components, and we consider only harmonically varying sources, - p(x)e^

*, J(x)e^*', M(x)e^* (16.76) where it is understood that we take the real part of

such ...

Furthermore, we assume that the time

**dependence**can be analyzed into itsFourier components, and we consider only harmonically varying sources, - p(x)e^

*, J(x)e^*', M(x)e^* (16.76) where it is understood that we take the real part of

such ...

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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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