## Classical Electrodynamics |

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Page 315

In the limit of very large conductivity it is convenient to relate the current density J

in the

infinite conductivity expression (10.9) to eliminate E from Faraday's law to yield ...

In the limit of very large conductivity it is convenient to relate the current density J

in the

**force equation**to the magnetic induction B via Ampère's law and to use theinfinite conductivity expression (10.9) to eliminate E from Faraday's law to yield ...

Page 337

an independent equation, but may be derived by combining the last two

equations in (10.91). Since the

magnetic field, we suspect that there exist solutions of a purely electrostatic

nature, with B = 0.

an independent equation, but may be derived by combining the last two

equations in (10.91). Since the

**force equation**in (10.91) is independent ofmagnetic field, we suspect that there exist solutions of a purely electrostatic

nature, with B = 0.

Page

Consequently to complete our discussion we must consider the covariant

formulation of the Lorentz

momentum and energy. The Lorentz

unit volume ...

Consequently to complete our discussion we must consider the covariant

formulation of the Lorentz

**force equation**and the conservation laws ofmomentum and energy. The Lorentz

**force equation**can be written as a force perunit volume ...

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### Contents

Introduction to Electrostatics | 1 |

Nº 3 | 3 |

Greens theorem | 14 |

Copyright | |

30 other sections not shown

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