Electrodynamics of Continuous Media, Volume 8Covers 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 288
... incident on the boundary of the medium at time t = 0 , so that at x = 0 the field ( E or H ) of the incident wave is E = 0 for t < 0 , E x e - iwol for t > 0. Expanding this field as a Fourier integral with respect to time , we reduce ...
... incident on the boundary of the medium at time t = 0 , so that at x = 0 the field ( E or H ) of the incident wave is E = 0 for t < 0 , E x e - iwol for t > 0. Expanding this field as a Fourier integral with respect to time , we reduce ...
Page 354
... incident ray they are n ̧ sin 0 , n , = 0. Substituting these values in ( 1 ) , we find the x and y components of the unit vector s / s , which give immediately the directions of the refracted rays : 1 1 sin e ' cos o ' = sin 0+ no 2n62 ...
... incident ray they are n ̧ sin 0 , n , = 0. Substituting these values in ( 1 ) , we find the x and y components of the unit vector s / s , which give immediately the directions of the refracted rays : 1 1 sin e ' cos o ' = sin 0+ no 2n62 ...
Page 414
... incident wave will be denoted by the unprimed letters E , H. In the present chapter we always suppose the incident wave to be monochromatic with frequency w . In the propagation of the scattered wave we have the relation D ' = ɛ ( w ...
... incident wave will be denoted by the unprimed letters E , H. In the present chapter we always suppose the incident wave to be monochromatic with frequency w . In the propagation of the scattered wave we have the relation D ' = ɛ ( w ...
Contents
ELECTROSTATICS OF CONDUCTORS 1 The electrostatic field of conductors 13892 | 1 |
2 The energy of the electrostatic field of conductors | 7 |
3 Methods of solving problems in electrostatics | 17 |
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Electrodynamics of Continuous Media: Volume 8 L D Landau,E.M. Lifshitz,L. P. Pitaevskii Snippet view - 1995 |
Common terms and phrases
angle anisotropy anisotropy energy antiferromagnetic atoms averaging axes axis body boundary conditions calculation charge circuit coefficient components conductor constant coordinates corresponding cross-section crystal Curie point curl H denote depends derivative determined dielectric diffraction direction discontinuity dispersion E₁ 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 sinē SOLUTION sphere suffixes superconducting surface symmetry temperature tensor theory thermodynamic potential transition uniaxial values variable velocity volume wave vector z-axis zero Απ