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 71
... zero components are those with three different suffixes : Yxyz Yz.xy Vy , zx ( The other non - zero components are equal to these , since Yi , ki = Yi , lk- ) Accordingly , the piezoelectric part of the thermodynamic potential is † pie ...
... zero components are those with three different suffixes : Yxyz Yz.xy Vy , zx ( The other non - zero components are equal to these , since Yi , ki = Yi , lk- ) Accordingly , the piezoelectric part of the thermodynamic potential is † pie ...
Page 72
... zero in the class C1 , and by a choice of the x and y axes one more component can be made zero in the classes C ,, C2 , C3 ; in C1 and C6 , the expression E is invariant under rotation through any angle about the z axis , and therefore ...
... zero in the class C1 , and by a choice of the x and y axes one more component can be made zero in the classes C ,, C2 , C3 ; in C1 and C6 , the expression E is invariant under rotation through any angle about the z axis , and therefore ...
Page 416
Лев Давидович Ландау, Evgeniĭ Mikhaĭlovich Lifshit︠s︡, Lev Petrovich Pitaevskiĭ. which is not zero . Since E ' is perpendicular to k ' , the tensor lik has non - zero components only in the plane perpendicular to k ' . These components ...
Лев Давидович Ландау, Evgeniĭ Mikhaĭlovich Lifshit︠s︡, Lev Petrovich Pitaevskiĭ. which is not zero . Since E ' is perpendicular to k ' , the tensor lik has non - zero components only in the plane perpendicular to k ' . These components ...
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