## 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 41

The existence of such a

as we saw above in the examples of the sphere and the cylinder. To determine a

and b we notice that, in the trivial particular case £<" = 1, we have simply E = D ...

The existence of such a

**relation**follows from the form of the boundary conditions,as we saw above in the examples of the sphere and the cylinder. To determine a

and b we notice that, in the trivial particular case £<" = 1, we have simply E = D ...

Page 106

which is analogous to the

Although H is, by analogy with E, usually called the magnetic field, it must be

remembered that the true mean field is really B and not H. To see the physical ...

which is analogous to the

**relation**between the electric field E and induction D.Although H is, by analogy with E, usually called the magnetic field, it must be

remembered that the true mean field is really B and not H. To see the physical ...

Page 266

Hence the

general linear

previous instants can be written in the integral form D(f) = E(t)+ |/(t)E(r-t)dT. (77.3)

o It ...

Hence the

**relation**between D and E can always be taken to be linear.f The mostgeneral linear

**relation**between D(f) and the values of the function E(f) at allprevious instants can be written in the integral form D(f) = E(t)+ |/(t)E(r-t)dT. (77.3)

o It ...

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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

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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