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 241
... discontinuity occurs . In reality , however , it is found that essentially different types of discontinuity again occur ( F. de Hoffmann and E. Teller , 1950 ) . Let us consider , first of all , discontinuities for which j = 0. This ...
... discontinuity occurs . In reality , however , it is found that essentially different types of discontinuity again occur ( F. de Hoffmann and E. Teller , 1950 ) . Let us consider , first of all , discontinuities for which j = 0. This ...
Page 244
... discontinuities cannot exist indefinitely , even if the conditions ( 71.14 ) are fulfilled . Although no turbulence occurs , the sharp discontinuity is replaced by a gradually widening transitional region , in which the velocity and the ...
... discontinuities cannot exist indefinitely , even if the conditions ( 71.14 ) are fulfilled . Although no turbulence occurs , the sharp discontinuity is replaced by a gradually widening transitional region , in which the velocity and the ...
Page 251
... discontinuity , u , < H , / 4rj = v l n Noting also that by the continuity of the mass flux P1 Un1 = P2 n2 , we deduce from p1 < P2 that 12 11 Un1 > Un2 , ( 73.8 ) and hence , from ( 73.6 ) , H12 < H11 : in a slow shock wave , the ...
... discontinuity , u , < H , / 4rj = v l n Noting also that by the continuity of the mass flux P1 Un1 = P2 n2 , we deduce from p1 < P2 that 12 11 Un1 > Un2 , ( 73.8 ) and hence , from ( 73.6 ) , H12 < H11 : in a slow shock wave , the ...
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