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 43
... averaged equation div D = 0 we have, as far as small terms of the first order, - div (E+óc)(E+6E)] = EdivöE + E. gradóe = 0. (9.4) The averaging of the product 68óE in (9.3) is done in two stages. We first average over the volume of ...
... averaged equation div D = 0 we have, as far as small terms of the first order, - div (E+óc)(E+6E)] = EdivöE + E. gradóe = 0. (9.4) The averaging of the product 68óE in (9.3) is done in two stages. We first average over the volume of ...
Page 56
... averaging over physically infinitesimal volumes, it is reasonable to consider that the position of the faces relative to the crystal lattice is averaged also. In consequence of this averaging, Do vanishes in any non-pyroelectric finite ...
... averaging over physically infinitesimal volumes, it is reasonable to consider that the position of the faces relative to the crystal lattice is averaged also. In consequence of this averaging, Do vanishes in any non-pyroelectric finite ...
Page 59
... averaging with respect to the Gibbs distribution w, = exp{(370 – E.")/T}. The term V, in formula (142), which is linear in the field, is zero except in pyroelectric bodies. The quadratic change in the free energy, which is of interest ...
... averaging with respect to the Gibbs distribution w, = exp{(370 – E.")/T}. The term V, in formula (142), which is linear in the field, is zero except in pyroelectric bodies. The quadratic change in the free energy, which is of interest ...
Page 81
... averaged over such portions. Its component P. can evidently take values in the range between the ordinates of a and a' in Fig. 14, i.e. – V[(T-T)a/2B]<P = V/[(T-T)a/2B]. (19.13) In other words, if P in Fig. 14 is taken as the ...
... averaged over such portions. Its component P. can evidently take values in the range between the ordinates of a and a' in Fig. 14, i.e. – V[(T-T)a/2B]<P = V/[(T-T)a/2B]. (19.13) In other words, if P in Fig. 14 is taken as the ...
Page 92
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Contents
1 | |
34 | |
CHAPTER III STEADY CURRENT | 86 |
CHAPTER IV STATIC MAGNETIC FIELD | 105 |
CHAPTER V FERROMAGNETISM AND ANTIFERROMAGNETISM | 130 |
CHAPTER VI SUPERCONDUCTIVITY | 180 |
CHAPTER VII QUASISTATIC ELECTROMAGNETIC FIELD | 199 |
CHAPTER VIII MAGNETOHYDRODYNAMICS | 225 |
CHAPTER XI ELECTROMAGNETIC WAVES IN ANISOTROPIC MEDIA | 331 |
CHAPTER XII SPATIAL DISPERSION | 358 |
CHAPTER XIII NONLINEAR OPTICS | 372 |
CHAPTER XIV THE PASSAGE OF FAST PARTICLES THROUGH MATTER | 394 |
CHAPTER XV SCATTERING OF ELECTROMAGNETIC WAVES | 413 |
CHAPTER XVI DIFFRACTION OF XRAYS IN CRYSTALS | 439 |
CURVILINEAR COORDINATES | 452 |
INDEX | 455 |
CHAPTER IX THE ELECTROMAGNETIC WAVE EQUATIONS | 257 |
CHAPTER X THE PROPAGATION OF ELECTROMAGNETIC WAVES | 290 |
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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
According angle anisotropy assumed averaging axes axis becomes body boundary conditions calculation called charge coefficient compared components condition conducting conductor consider constant continuous coordinates corresponding crystal curl denote density depends derivative determined dielectric direction discontinuity distance distribution effect electric field ellipsoid energy equal equation expression external factor ferromagnet fluid flux follows force formula frequency function given gives grad Hence incident increases independent induction integral linear magnetic field mean medium neglected normal obtain occur parallel particle particular permittivity perpendicular phase plane polarization positive potential present PROBLEM propagated properties quantities range regarded region relation respect result rotation satisfied scattering simply solution sphere Substituting surface symmetry taken temperature tensor theory thermodynamic transition uniform unit values variable vector volume wave write zero