## Electrodynamics of continuous mediaCovers the theory of electromagnetic fields in matter, and the theory of the macroscopic electric and magnetic properties of matter. There is a considerable amount of new material particularly on the theory of the magnetic properties of matter and the theory of optical phenomena with new chapters on spatial dispersion and non-linear optics. The chapters on ferromagnetism and antiferromagnetism and on magnetohydrodynamics have been substantially enlarged and eight other chapters have additional sections. |

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Page 40

sphere in the form <pie) — (£ - r + A(£ - r/r3; the first term is the potential of the

required change in potential due to the sphere (cf. §3, Problem 1, solution).

Inside the ...

sphere in the form <pie) — (£ - r + A(£ - r/r3; the first term is the potential of the

**external field**imposed, and the second, which vanishes at infinity, gives therequired change in potential due to the sphere (cf. §3, Problem 1, solution).

Inside the ...

Page 184

The total energy of the magnetic

integral | (H2/%n) d V, taken over all space ... If the ring is in an

the ...

The total energy of the magnetic

**field**of the superconductor is given by theintegral | (H2/%n) d V, taken over all space ... If the ring is in an

**external**magnetic**field**, the total magnetic flux <J> is composed of the flux LJ/c and the flux <t>e ofthe ...

Page 185

The state of an n-ply connected system in the absence of an

completely determined by the n — 1 total currents Ja. The relation (54.5)

becomes the system of equations XL^ + <&„<«> = 4>fl0. (54.6) b These equations

hold, not ...

The state of an n-ply connected system in the absence of an

**external field**iscompletely determined by the n — 1 total currents Ja. The relation (54.5)

becomes the system of equations XL^ + <&„<«> = 4>fl0. (54.6) b These equations

hold, not ...

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### Contents

ELECTROSTATICS OF CONDUCTORS 1 The electrostatic field of conductors | 1 |

2 The energy of the electrostatic field of conductors | 3 |

3 Methods of solving problems in electrostatics | 8 |

Copyright | |

118 other sections not shown

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### Common terms and phrases

angle anisotropy anisotropy energy antiferromagnetic atoms averaging axes axis body boundary conditions calculation charge circuit coefficient components conducting conductor constant coordinates corresponding cross-section crystal Curie point curl H current density denote depends derivative determined dielectric differential diffraction dipole direction discontinuity dispersion dissipation distance e(co effect electric field electromagnetic electrons ellipsoid equilibrium expression external field factor ferroelectric ferromagnet field H fluctuations fluid formula free energy frequency function given gives grad Hence incident induction integral isotropic Laplace's equation layer Let us consider linear magnetic field magnitude Maxwell's equations medium neglected non-zero normal obtain optical particle permittivity perpendicular perturbation phase piezoelectric plane polarization Problem propagated properties pyroelectric quantities refraction relation respect result rotation satisfied scattering Solution sphere Substituting suffixes superconducting surface symmetry tangential temperature tensor theory thermodynamic equilibrium thermodynamic potential transition uniaxial uniform values variable velocity wave vector wire z-axis zero