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 288
... frequency , but also with respect to the wave vector ; we shall return to this topic in §105 . Lastly , suppose that within the broad transparency region there is a narrow absorption line near some frequency wo . Let us consider a ...
... frequency , but also with respect to the wave vector ; we shall return to this topic in §105 . Lastly , suppose that within the broad transparency region there is a narrow absorption line near some frequency wo . Let us consider a ...
Page 372
... frequencies . For example , if a monochromatic wave with frequency @ , is incident on such a medium , then , as it is propagated in the medium , waves with frequencies mo , ( m being an integer ) are generated ; if there is initially a ...
... frequencies . For example , if a monochromatic wave with frequency @ , is incident on such a medium , then , as it is propagated in the medium , waves with frequencies mo , ( m being an integer ) are generated ; if there is initially a ...
Page 414
... frequency w ' of the scattered wave and of the primary frequency w . The fact that a and ẞ are tensors does not , of course , contradict the assumed isotropy of the medium . Only the fully averaged properties of the medium are isotropic ...
... frequency w ' of the scattered wave and of the primary frequency w . The fact that a and ẞ are tensors does not , of course , contradict the assumed isotropy of the medium . Only the fully averaged properties of the medium are isotropic ...
Contents
ELECTROSTATICS OF CONDUCTORS | 1 |
2 The energy of the electrostatic field of conductors | 7 |
4 A conducting ellipsoid | 27 |
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angle anisotropy anisotropy energy antiferromagnetic atoms averaging axes axis body boundary conditions calculation charge coefficient components conductor constant coordinates corresponding cross-section crystal Curie point curl H denote depends derivative determined dielectric diffraction direction discontinuity dispersion E₁ E₂ electric field electromagnetic electrons ellipsoid expression external field factor ferroelectric ferromagnet field H fluctuations fluid flux formula free energy frequency function given gives grad H₁ H₂ Hence incident induction integral isotropic Laplace's equation linear magnetic field magnetic moment Maxwell's equations medium normal obtain optical particle permittivity perpendicular perturbation phase plane polarization PROBLEM propagated properties pyroelectric quantities refraction relation respect result rotation satisfied scattering sin² SOLUTION sphere suffixes superconducting surface symmetry temperature tensor theory thermodynamic potential transition uniaxial values variable velocity volume wave vector z-axis zero Απ