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 63
... grad & can be written as Then ( 15.12 ) becomes grad ɛ = ( ĉɛ / ♂T ) , grad T + ( ĉɛ / ĉp ) , grad p . Ρ E2 θε f = -grad P. ( p.7 ) + { grad [ E2 ( ? ) , ] - E ( G ) , T ) + 8π grad T. ( 15.15 ) If the temperature also is constant ...
... grad & can be written as Then ( 15.12 ) becomes grad ɛ = ( ĉɛ / ♂T ) , grad T + ( ĉɛ / ĉp ) , grad p . Ρ E2 θε f = -grad P. ( p.7 ) + { grad [ E2 ( ? ) , ] - E ( G ) , T ) + 8π grad T. ( 15.15 ) If the temperature also is constant ...
Page 99
... grad p was included in ( 26.2 ) or ( 26.4 ) . The existence of such terms would , in fact , contradict the law of the increase of entropy : the integrand in ( 26.5 ) would then contain terms in the products j grad p and grad 7 · grad p ...
... grad p was included in ( 26.2 ) or ( 26.4 ) . The existence of such terms would , in fact , contradict the law of the increase of entropy : the integrand in ( 26.5 ) would then contain terms in the products j grad p and grad 7 · grad p ...
Page 127
... grad Po + 8π Brad [ H3p ( CH ) ] - Ομ H2 8π μ grad μ - 8π μ grad H2 + ( H⚫grad ) H . Απ By a well - known formula of vector analysis , ( H · grad ) H = 1⁄2 grad H2 - H × curl H = = grad H2 + 4лj × Н / c . Thus 1 f = - grad P。 + - grad ...
... grad Po + 8π Brad [ H3p ( CH ) ] - Ομ H2 8π μ grad μ - 8π μ grad H2 + ( H⚫grad ) H . Απ By a well - known formula of vector analysis , ( H · grad ) H = 1⁄2 grad H2 - H × curl H = = grad H2 + 4лj × Н / c . Thus 1 f = - grad P。 + - grad ...
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