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 61
... Hence we have finally the following expression for the stress tensor : σik = [ F – p ( † Ƒ / ĉp ) ET ] dik + E¡Dx / 4π . ( 15.7 ) In isotropic media , which are those here considered , E and D are parallel . Hence EDED , and the tensor ...
... Hence we have finally the following expression for the stress tensor : σik = [ F – p ( † Ƒ / ĉp ) ET ] dik + E¡Dx / 4π . ( 15.7 ) In isotropic media , which are those here considered , E and D are parallel . Hence EDED , and the tensor ...
Page 187
... Hence , in particular , Her ( 7 ) must tend continuously to zero at T = Ter . We know from the general theory of second - order phase transitions † that the change in the thermodynamic potential near the transition point is proportional ...
... Hence , in particular , Her ( 7 ) must tend continuously to zero at T = Ter . We know from the general theory of second - order phase transitions † that the change in the thermodynamic potential near the transition point is proportional ...
Page 197
... Hence the magnetic moment per unit length in the z - direction and per boundary surface of the superconducting layer is - OCD H 4π y ds , ds = √ ( dx2 + dy2 ) . If the layer did not emerge at the surface , there would be no segment OC ...
... Hence the magnetic moment per unit length in the z - direction and per boundary surface of the superconducting layer is - OCD H 4π y ds , ds = √ ( dx2 + dy2 ) . If the layer did not emerge at the surface , there would be no segment OC ...
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