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 144
... magnitude . This happens , for instance , in uniaxial crystals . Marked deformations resulting from a change in the direction of M occur in fields H ~ BM ; the change in the magnitude M is considerable when H ~ 4πM . If these two values ...
... magnitude . This happens , for instance , in uniaxial crystals . Marked deformations resulting from a change in the direction of M occur in fields H ~ BM ; the change in the magnitude M is considerable when H ~ 4πM . If these two values ...
Page 145
... magnitude o ~ a / μ , where a and μ are the orders of magnitude of the coefficients aikim and the elastic coefficients respectively . In this sense , the magnetoelastic energy ( per unit volume , as usual ) is of the order of a2 / μ ...
... magnitude o ~ a / μ , where a and μ are the orders of magnitude of the coefficients aikim and the elastic coefficients respectively . In this sense , the magnetoelastic energy ( per unit volume , as usual ) is of the order of a2 / μ ...
Page 242
... magnitude of H itself and its angle to the surface are likewise continuous . Formulae ( 71.3 ) – ( 71.6 ) give all the properties of the discontinuities under consideration . The thermodynamic quantities are continuous , but the ...
... magnitude of H itself and its angle to the surface are likewise continuous . Formulae ( 71.3 ) – ( 71.6 ) give all the properties of the discontinuities under consideration . The thermodynamic quantities are continuous , but the ...
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