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 41
... write out the formulae for the field outside the ellipsoid. The uniform field inside the ellipsoid can be found without actually writing out the boundary conditions, by using some results already known. Let us first suppose that the ...
... write out the formulae for the field outside the ellipsoid. The uniform field inside the ellipsoid can be found without actually writing out the boundary conditions, by using some results already known. Let us first suppose that the ...
Page 42
... + In these three Problems the body is assumed to be in a vacuum. : In a longitudinal field the solution is clearly E3 = (#. We write the local field as E = E +6E, 42 Electrostatics of Dielectrics §9. The permittivity of a mixture.
... + In these three Problems the body is assumed to be in a vacuum. : In a longitudinal field the solution is clearly E3 = (#. We write the local field as E = E +6E, 42 Electrostatics of Dielectrics §9. The permittivity of a mixture.
Page 43
... write the local field as E = E +6E, and the local permittivity as E+ 68, where # = (1/V) edy (9.2) is obtained by averaging over the volume. Then the mean induction is D = (E+ 6e)(E+6E) = BE+ 6edE, (9.3) since the mean values of 68 and ...
... write the local field as E = E +6E, and the local permittivity as E+ 68, where # = (1/V) edy (9.2) is obtained by averaging over the volume. Then the mean induction is D = (E+ 6e)(E+6E) = BE+ 6edE, (9.3) since the mean values of 68 and ...
Page 45
... write 1 1 - :- - - - e := - - - V. ôR = p 6e 47t job df 47t jawood The last integral is taken over the whole volume outside the conductor. Since the varied field, like the original field, must satisfy the field equations, we have div 6D ...
... write 1 1 - :- - - - e := - - - V. ôR = p 6e 47t job df 47t jawood The last integral is taken over the whole volume outside the conductor. Since the varied field, like the original field, must satisfy the field equations, we have div 6D ...
Page 47
... write out also, for future reference, formulae for the entropy density S and the chemical potential £, which follow from (10.15). 6F D” (68 S :- - - - T - (#). So( *#(#) E* / 68 6F E* / de :-(#).--To-#(£). (10.19) These quantities, of ...
... write out also, for future reference, formulae for the entropy density S and the chemical potential £, which follow from (10.15). 6F D” (68 S :- - - - T - (#). So( *#(#) E* / 68 6F E* / de :-(#).--To-#(£). (10.19) These quantities, of ...
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