## Classical Electrodynamics |

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Page 150

The potential energy of a permanent magnetic moment (or dipole) in an external

we interpret the force as the negative gradient of a potential energy U, we find U ...

The potential energy of a permanent magnetic moment (or dipole) in an external

**magnetic field**can be obtained from either the force (5.69) or the torque (5.72). Ifwe interpret the force as the negative gradient of a potential energy U, we find U ...

Page 313

10.3 Magnetic Diffusion, Viscosity, and Pressure The behavior of a fluid in the

presence of electromagnetic fields is , governed to a large ... The time

dependence of the

the form: 2 ...

10.3 Magnetic Diffusion, Viscosity, and Pressure The behavior of a fluid in the

presence of electromagnetic fields is , governed to a large ... The time

dependence of the

**magnetic field**can be written, using (10.8) to eliminate E, inthe form: 2 ...

Page 382

This

— 1. Even at nonrelativistic velocities where y c 1, this magnetic induction is

equivalent to B ~ 4 V × 5. - (11.119) c ro which is just the Ampère-Biot–Savart ...

This

**magnetic field**becomes almost equal to the transverse electric field El as B— 1. Even at nonrelativistic velocities where y c 1, this magnetic induction is

equivalent to B ~ 4 V × 5. - (11.119) c ro which is just the Ampère-Biot–Savart ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

BoundaryValue Problems in Electrostatics II | 54 |

Copyright | |

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