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 28
... plane = O and the potential is zero , as it should be . At large distances r = √ ( z2 + p2 ) from the aperture we ... plane . The distribution of charge on the conducting plane is given by σ = + 1 еф 4π 02 a аф & = = + = ± z = 0 [ a a ...
... plane = O and the potential is zero , as it should be . At large distances r = √ ( z2 + p2 ) from the aperture we ... plane . The distribution of charge on the conducting plane is given by σ = + 1 еф 4π 02 a аф & = = + = ± z = 0 [ a a ...
Page 139
... plane ( the basal plane of the crystal ) ; such ferromagnet is said to be of the " easy - plane " type . † The expression ( 40.2 ) is isotropic in the xy - plane . This isotropy , however , does not occur in the higher - order terms in ...
... plane ( the basal plane of the crystal ) ; such ferromagnet is said to be of the " easy - plane " type . † The expression ( 40.2 ) is isotropic in the xy - plane . This isotropy , however , does not occur in the higher - order terms in ...
Page 344
... plane to the ray surface . This plane is perpendicular to ON , and touches the ray surface not at one point but along a curve , which is found to be a circle . In Fig . 55 the trace of this plane is shown by ab . This follows at once ...
... plane to the ray surface . This plane is perpendicular to ON , and touches the ray surface not at one point but along a curve , which is found to be a circle . In Fig . 55 the trace of this plane is shown by ab . This follows at once ...
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 |
Copyright | |
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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