Electrodynamics of Continuous Media, Volume 8Covers 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 335
... wave vector . ( The principal values are functions of frequency , and so are , in some cases ( see §99 ) , the directions of the principal axes of the tensor & . ) For monochromatic waves , however , w , and therefore all the e ) , are ...
... wave vector . ( The principal values are functions of frequency , and so are , in some cases ( see §99 ) , the directions of the principal axes of the tensor & . ) For monochromatic waves , however , w , and therefore all the e ) , are ...
Page 336
... vector of a wave with given n is that of the normal at the corresponding point of the wave - vector surface . It is easy to see that the reverse is also true : the normal to the ray surface gives the direction of the corresponding wave ...
... vector of a wave with given n is that of the normal at the corresponding point of the wave - vector surface . It is easy to see that the reverse is also true : the normal to the ray surface gives the direction of the corresponding wave ...
Page 340
... vector is that of n . In waves of the second type , called extraordinary waves , the magnitude of the wave vector depends on the angle 0 which it makes with the optical axis . By ( 98.2 ) 1 sin20 cos20 + n2 ( 98.5 ) The ray vector in an ...
... vector is that of n . In waves of the second type , called extraordinary waves , the magnitude of the wave vector depends on the angle 0 which it makes with the optical axis . By ( 98.2 ) 1 sin20 cos20 + n2 ( 98.5 ) The ray vector in an ...
Contents
ELECTROSTATICS OF CONDUCTORS 1 The electrostatic field of conductors 13892 | 1 |
2 The energy of the electrostatic field of conductors | 7 |
3 Methods of solving problems in electrostatics | 17 |
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Electrodynamics of Continuous Media: Volume 8 L D Landau,E.M. Lifshitz,L. P. Pitaevskii Snippet view - 1995 |
Common terms and phrases
angle anisotropy anisotropy energy antiferromagnetic atoms averaging axes axis body boundary conditions calculation charge circuit coefficient components conductor constant coordinates corresponding cross-section crystal Curie point curl H denote depends derivative determined dielectric diffraction direction discontinuity dispersion E₁ 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