Electrodynamics of Continuous MediaCovers 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
... Substituting the above expressions in ( 15.4 ) and using also the fact that dh = 52 = § ⋅n , we obtain 1 aF σik Šink = ( n.D ) ( E ) - np . • + § • nF Απ др OF Ρ θρ = { E , D + Απ Sik + FSik ( Š¡1k Hence we have finally the following ...
... Substituting the above expressions in ( 15.4 ) and using also the fact that dh = 52 = § ⋅n , we obtain 1 aF σik Šink = ( n.D ) ( E ) - np . • + § • nF Απ др OF Ρ θρ = { E , D + Απ Sik + FSik ( Š¡1k Hence we have finally the following ...
Page 82
... substituting Poz = Po from ( 19.16 ) , we find the longitudinal polarization P - PoE / 4a ( T - T ) and the transverse polarization Px = BE / aC ( T - T ) ( 19.17 ) ( 19.18 ) ( and similarly for P , ) . Above the transition point , in ...
... substituting Poz = Po from ( 19.16 ) , we find the longitudinal polarization P - PoE / 4a ( T - T ) and the transverse polarization Px = BE / aC ( T - T ) ( 19.17 ) ( 19.18 ) ( and similarly for P , ) . Above the transition point , in ...
Page 419
... substituting for a and b the corresponding terms in ( 117.17 ) . In scalar scattering of linearly polarized light , the scattered light too is completely polarized , and its angular intensity distribution is given by I = 3sin20 ...
... substituting for a and b the corresponding terms in ( 117.17 ) . In scalar scattering of linearly polarized light , the scattered light too is completely polarized , and its angular intensity distribution is given by I = 3sin20 ...
Contents
ELECTROSTATICS OF CONDUCTORS | 1 |
2 The energy of the electrostatic field of conductors | 7 |
4 A conducting ellipsoid | 27 |
Copyright | |
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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 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