Electrodynamics of Continuous Media: Volume 8Covers the theory of electromagnetic fields in matter, and the theory of 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. |
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Page 138
... anisotropy energy As already mentioned , the anisotropy of the magnetic properties of ferromagnets is due to the relativistic interactions between their atoms , and these interactions are comparatively weak . In the macroscopic theory ...
... anisotropy energy As already mentioned , the anisotropy of the magnetic properties of ferromagnets is due to the relativistic interactions between their atoms , and these interactions are comparatively weak . In the macroscopic theory ...
Page 139
... anisotropy in the basal plane . In a hexagonal crystal , the anisotropy energy contains only one fourth - order term , proportional to ( m ̧2 + m , 2 ) 2 ; in this approximation , 2 Uaniso = K1 sin20 + K2 sin1 0 , 1 ( 40.3 ) the ...
... anisotropy in the basal plane . In a hexagonal crystal , the anisotropy energy contains only one fourth - order term , proportional to ( m ̧2 + m , 2 ) 2 ; in this approximation , 2 Uaniso = K1 sin20 + K2 sin1 0 , 1 ( 40.3 ) the ...
Page 141
... anisotropic in the xy - plane , are neglected in the anisotropy energy ) . We take this as the xz - plane . The thermodynamic potential , including the anisotropy energy , is § 2 - μ = Þ 。( M ) + { ßM ̧2 – M · H - H2 / 8 ′′ = - Þ 。( M ) ...
... anisotropic in the xy - plane , are neglected in the anisotropy energy ) . We take this as the xz - plane . The thermodynamic potential , including the anisotropy energy , is § 2 - μ = Þ 。( M ) + { ßM ̧2 – M · H - H2 / 8 ′′ = - Þ 。( M ) ...
Contents
ELECTROSTATICS OF CONDUCTORS | 1 |
2 The energy of the electrostatic field of conductors | 7 |
3 Methods of solving problems in electrostatics | 17 |
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angle anisotropy anisotropy energy antiferromagnetic atoms averaging axes axis body boundary conditions calculation charge coefficient components conductor constant coordinates corresponding cross-section crystal Curie point curl H denote depends derivative determined dielectric diffraction direction discontinuity dispersion E₁ E₂ electric field electromagnetic electrons ellipsoid equation expression external field 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 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