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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Results 1-5 of 65
Page 23
... Substituting (422) in Laplace's equation (4.6), we obtain for F(£) the equation d°F dF d 2 dć” +: log (R&ta )] = 0. One solution of this equation is F = constant, and the other is dć F (&) = A –#–. 4.23 (#) |G: (423) & The upper limit ...
... Substituting (422) in Laplace's equation (4.6), we obtain for F(£) the equation d°F dF d 2 dć” +: log (R&ta )] = 0. One solution of this equation is F = constant, and the other is dć F (&) = A –#–. 4.23 (#) |G: (423) & The upper limit ...
Page 26
... Substituting (4.24) and using the fact that |: # | JC | v. = | T-- * | 3-2T 5 hi déJ:= 0 2a'h, J. = 0 we have a = (#v./4tn” when the external field is in the x-direction. When the direction of the external field is arbitrary this ...
... Substituting (4.24) and using the fact that |: # | JC | v. = | T-- * | 3-2T 5 hi déJ:= 0 2a'h, J. = 0 we have a = (#v./4tn” when the external field is in the x-direction. When the direction of the external field is arbitrary this ...
Page 30
... Substituting (2.2), we find that % and 7 differ only in sign. & = – W. (5.6) The force F, is obtained by differentiating % with respect to q for constant potentials, i.e. F. = -(6%/āq) = (6%/64). (5.7) Thus the forces acting on a ...
... Substituting (2.2), we find that % and 7 differ only in sign. & = – W. (5.6) The force F, is obtained by differentiating % with respect to q for constant potentials, i.e. F. = -(6%/āq) = (6%/64). (5.7) Thus the forces acting on a ...
Page 33
... Substituting in these two relations & = ae"T" and p = Ae" "e" (q) satisfies the equation Aq) = 0) and eliminating a and A, we find the required relation between k and a . o' = k(gp–4:too'k + ak')/p. (1) If the surface of the liquid is ...
... Substituting in these two relations & = ae"T" and p = Ae" "e" (q) satisfies the equation Aq) = 0) and eliminating a and A, we find the required relation between k and a . o' = k(gp–4:too'k + ak')/p. (1) If the surface of the liquid is ...
Page 34
... Substituting p from (6.3) and again integrating over a volume which includes the whole body we have | rod V = – Jr div PdV = – $r(df. P)+ j (P. grad)rd V. The integral over the surface is zero, and in the second term we have (P - grad)r ...
... Substituting p from (6.3) and again integrating over a volume which includes the whole body we have | rod V = – Jr div PdV = – $r(df. P)+ j (P. grad)rd V. The integral over the surface is zero, and in the second term we have (P - grad)r ...
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