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. |
From inside the book
Results 6-10 of 86
Page 18
... integral, we have taken the limits as those of the region d 4 x < VS. Hence we find the capacitance L., VS S C = +:-5 log 4nd "812" d —?" *o/4 (o) -2'- - - - - - - - - - - 3=O —2 =-2, 2 96 (b) 2-#" |2-0 FIG. 7 t See §23. In formula ...
... integral, we have taken the limits as those of the region d 4 x < VS. Hence we find the capacitance L., VS S C = +:-5 log 4nd "812" d —?" *o/4 (o) -2'- - - - - - - - - - - 3=O —2 =-2, 2 96 (b) 2-#" |2-0 FIG. 7 t See §23. In formula ...
Page 22
... integral of the first kind. The surface of the conductor corresponds to # = 0, and so the capacitance of the ... integrals (4.14), (4.15) degenerate and can be expressed in terms of elementary functions. For a prolate spheroid (a > b = c ...
... integral of the first kind. The surface of the conductor corresponds to # = 0, and so the capacitance of the ... integrals (4.14), (4.15) degenerate and can be expressed in terms of elementary functions. For a prolate spheroid (a > b = c ...
Page 23
... integral is an elliptic integral of the second kind. We must have p = constant on the surface of the ellipsoid. For this condition to be satisfied with & = 0 and arbitrary n, &, the constant value of p must be zero. Determining the ...
... integral is an elliptic integral of the second kind. We must have p = constant on the surface of the ellipsoid. For this condition to be satisfied with & = 0 and arbitrary n, &, the constant value of p must be zero. Determining the ...
Page 27
... integral in formula (4.24), q = -ex. _tanh "V(a'-b')/(# a')]–VI(a' #" tanh-'y(1–b°/a")-V(1-5°/a") The coordinate ... integrals in (4.24). Then _V[(a'-c')(#c')]-tan 'V[(a'-c')(: * V(a'/c'–1)-tan" </(a'/c”–1) q = -e: where the coordinate ...
... integral in formula (4.24), q = -ex. _tanh "V(a'-b')/(# a')]–VI(a' #" tanh-'y(1–b°/a")-V(1-5°/a") The coordinate ... integrals in (4.24). Then _V[(a'-c')(#c')]-tan 'V[(a'-c')(: * V(a'/c'–1)-tan" </(a'/c”–1) q = -e: where the coordinate ...
Page 34
... integral equation, which must be valid for a body of any shape, means that the average charge density can be written ... integral rod V. Substituting p from (6.3) and again integrating over a volume which includes the whole body we have ...
... integral equation, which must be valid for a body of any shape, means that the average charge density can be written ... integral rod V. Substituting p from (6.3) and again integrating over a volume which includes the whole body we have ...
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 |
Other editions - View all
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