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 181
... flow in a superconductor . It should be emphasized that in a superconductor the conduction current cannot meaningfully be isolated from pv as it can in an ordinary conductor . For the same reason the magnetization M , and therefore H ...
... flow in a superconductor . It should be emphasized that in a superconductor the conduction current cannot meaningfully be isolated from pv as it can in an ordinary conductor . For the same reason the magnetization M , and therefore H ...
Page 182
... flow of current on a superconductor is possible even if no electric field is present . This means that no dissipation of energy occurs , whose replacement would involve work being done by an external field . This property of a ...
... flow of current on a superconductor is possible even if no electric field is present . This means that no dissipation of energy occurs , whose replacement would involve work being done by an external field . This property of a ...
Page 231
... flow , in comparison with that of the viscosity , is described by the quantity G = a / d = ( a H / c ) √ ( o / n ) , I called the Hartmann number . When G < 1 we have v = v 。( 1 - z2 / a2 ) , v = ( AP / l ) a2 / 3n , ( 67.5 ) ( 67.6 ) ...
... flow , in comparison with that of the viscosity , is described by the quantity G = a / d = ( a H / c ) √ ( o / n ) , I called the Hartmann number . When G < 1 we have v = v 。( 1 - z2 / a2 ) , v = ( AP / l ) a2 / 3n , ( 67.5 ) ( 67.6 ) ...
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