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 84
Page 2
... relation is obtained from the general electrostatic equation div e = 4tp, which on averaging gives div E = 4tp, (1.8) p being the mean charge density. The meaning of the integrated form of this equation is well known: the flux of the ...
... relation is obtained from the general electrostatic equation div e = 4tp, which on averaging gives div E = 4tp, (1.8) p being the mean charge density. The meaning of the integrated form of this equation is well known: the flux of the ...
Page 4
... relations between them. Since the field equations in a vacuum are linear and homogeneous, these relations must also be linear, i.e. they must be given by equations of the form e =X.C., b, (2.3) b where the quantities C, C, have the ...
... relations between them. Since the field equations in a vacuum are linear and homogeneous, these relations must also be linear, i.e. they must be given by equations of the form e =X.C., b, (2.3) b where the quantities C, C, have the ...
Page 7
... relation e = C(42 – p1), and the energy of the system is given in terms of C by 4 = }e^/C. Comparing with (29), we obtain 1/C = CT'11–2CT*12 +CT"22 = (C.11 + 2C12 +C22)/(C11C22– C12*). PROBLEM 2. A point charge e is situated at O, near ...
... relation e = C(42 – p1), and the energy of the system is given in terms of C by 4 = }e^/C. Comparing with (29), we obtain 1/C = CT'11–2CT*12 +CT"22 = (C.11 + 2C12 +C22)/(C11C22– C12*). PROBLEM 2. A point charge e is situated at O, near ...
Page 11
... relation r = R*r'/r”, we find that the magnitudes of the small differences or and Ör' = r" — r"o are related by (ór)* ... relations between the derivatives of p and A are, mathematically, just the wellknown Cauchy–Riemann conditions, which ...
... relation r = R*r'/r”, we find that the magnitudes of the small differences or and Ör' = r" — r"o are related by (ór)* ... relations between the derivatives of p and A are, mathematically, just the wellknown Cauchy–Riemann conditions, which ...
Page 12
... relations (3.14), according to which 64, 6A 64, 6A : 5; +5, Gy-" Both the real and the imaginary part of an analytic ... relation w = w(z) constitutes a conformal mapping of the plane of the complex variable z on the plane of the complex ...
... relations (3.14), according to which 64, 6A 64, 6A : 5; +5, Gy-" Both the real and the imaginary part of an analytic ... relation w = w(z) constitutes a conformal mapping of the plane of the complex variable z on the plane of the complex ...
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