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 340
... propagated in a uniaxial crystal . With respect to one type , called ordinary waves , the crystal behaves like an isotropic body with refractive index n = √1 . The magnitude of the wave vector is on / c whatever its direction , and the ...
... propagated in a uniaxial crystal . With respect to one type , called ordinary waves , the crystal behaves like an isotropic body with refractive index n = √1 . The magnitude of the wave vector is on / c whatever its direction , and the ...
Page 346
... propagated in the crystal , in which n is a complex vector but its real and imaginary parts are in the same direction : n = nv , where v is a real unit vector , n = n ( w ) a complex quantity . For a given v , the dispersion equation ...
... propagated in the crystal , in which n is a complex vector but its real and imaginary parts are in the same direction : n = nv , where v is a real unit vector , n = n ( w ) a complex quantity . For a given v , the dispersion equation ...
Page 369
... propagated in the medium . When ẞ > 0 ( Fig . 58a ) , the upper continuous curve enters the region w > wo , and this gives rise to an additional wave which would not exist without spatial dispersion ; when w > wo , two different ...
... propagated in the medium . When ẞ > 0 ( Fig . 58a ) , the upper continuous curve enters the region w > wo , and this gives rise to an additional wave which would not exist without spatial dispersion ; when w > wo , two different ...
Contents
ELECTROSTATICS OF CONDUCTORS | 1 |
2 The energy of the electrostatic field of conductors | 7 |
4 A conducting ellipsoid | 27 |
Copyright | |
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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