## Electrodynamics of Continuous MediaCovers the theory of electromagnetic fields in matter, and the theory of 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. |

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Page 152

In the transition layer, M rotates over half a circular cone with its axis along the f/-

axis; M, = constant = 1/^/2, so that div M - Mr' = 0, as it should be (the prime

In the transition layer, M rotates over half a circular cone with its axis along the f/-

axis; M, = constant = 1/^/2, so that div M - Mr' = 0, as it should be (the prime

**denotes**differentiation with respect to 7;). Let <p**denote**the angle between the ...Page 240

Thus PiVln = p2v2n, where the suffixes 1 and 2 refer to the two sides of the

discontinuity, and the suffix n

surface. In what follows we shall

...

Thus PiVln = p2v2n, where the suffixes 1 and 2 refer to the two sides of the

discontinuity, and the suffix n

**denotes**the component of a vector normal to thesurface. In what follows we shall

**denote**the difference between the values of any...

Page 423

The equation is therefore valid for the unresolved field in the scattered wave,

which we shall

<|E'|2> " SWS? <|C|!>si"Je * TW <|G|'>si"'e' where 0 is the angle between k and G,

...

The equation is therefore valid for the unresolved field in the scattered wave,

which we shall

**denote**by the same letter E'. Using the solution (117.7), we obtain<|E'|2> " SWS? <|C|!>si"Je * TW <|G|'>si"'e' where 0 is the angle between k and G,

...

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### Contents

ELECTROSTATICS OF CONDUCTORS 51 The electrostatic field of conductors | 1 |

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

3 Methods of solving problems in electrostatics | 9 |

Copyright | |

122 other sections not shown

### Common terms and phrases

absorption amplitude angle anisotropy antiferromagnetic atoms averaging axes axis body boundary conditions calculation charge Cherenkov radiation coefficient components conductor constant coordinates corresponding cos2 cross-section crystal Curie point curl H denote density dependence derived determined dielectric diffraction direction discontinuity dissipation distance e(co effect electric field electron ellipsoid equation expression external field factor ferroelectric ferromagnet fluctuations fluid formula Fourier free energy frequency function given gives grad Hence incident wave induction integral intensity isotropic Laplace's equation linear macroscopic magnetic field magnitude Maxwell's equations medium monochromatic non-linear normal obtain optical particle permittivity perpendicular perturbation phase plane polarization Problem propagated properties pyroelectric quantities radiation refraction relation respect result rotation satisfied scalar scattering solution spatial dispersion sphere Substituting suffixes superconducting surface symmetry temperature tensor theory thermodynamic potential transition uniaxial upper half-plane values variable velocity wave vector waveguide z-axis zero