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 3
... integral being taken over the whole surface . The potential distribution in the electrostatic field has the following remarkable property : the function ( x , y , z ) can take maximum and minimum values only at boundaries of regions ...
... integral being taken over the whole surface . The potential distribution in the electrostatic field has the following remarkable property : the function ( x , y , z ) can take maximum and minimum values only at boundaries of regions ...
Page 49
... integral this follows at once from the equations div D = 0 and div = 0 which the induction in the dielectric and the field in the vacuum must respectively satisfy . The surface integral is taken over the surfaces of the conductors which ...
... integral this follows at once from the equations div D = 0 and div = 0 which the induction in the dielectric and the field in the vacuum must respectively satisfy . The surface integral is taken over the surfaces of the conductors which ...
Page 149
... integral ∞ = ∞ [ { x , ( M , 2 + M ; 2 ) + { BM , 2 ] dx = { M2 ( ( x , 0'2 + ẞ sin20 ) dx , ( 43.4 ) where the prime denotes differentiation with respect to x . The remaining terms in the free energy are independent of the structure ...
... integral ∞ = ∞ [ { x , ( M , 2 + M ; 2 ) + { BM , 2 ] dx = { M2 ( ( x , 0'2 + ẞ sin20 ) dx , ( 43.4 ) where the prime denotes differentiation with respect to x . The remaining terms in the free energy are independent of the structure ...
Contents
ELECTROSTATICS OF CONDUCTORS | 1 |
2 The energy of the electrostatic field of conductors | 7 |
4 A conducting ellipsoid | 27 |
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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