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 48
... present case, when D and E are linearly related, all the field equations and their boundary conditions are also linear. Hence the potentials of the conductors must (as for the field in a vacuum) be linear functions of their charges, and ...
... present case, when D and E are linearly related, all the field equations and their boundary conditions are also linear. Hence the potentials of the conductors must (as for the field in a vacuum) be linear functions of their charges, and ...
Page 49
... present there, and not on the field which would be present if the body were removed. If the external field (£ is uniform, then 6% = -6&. [PdV = -2°.6G, (11.4) where 3° is the total electric dipole moment of the body. Hence the ...
... present there, and not on the field which would be present if the body were removed. If the external field (£ is uniform, then 6% = -6&. [PdV = -2°.6G, (11.4) where 3° is the total electric dipole moment of the body. Hence the ...
Page 58
... present case, however, we are considering a change in the field but no change in the sources. This term therefore vanishes, leaving 6% = - | (68/e”)(D+/87)d V = – | 68(E*/87)d V. (14.1) From this formula it follows that any increase in ...
... present case, however, we are considering a change in the field but no change in the sources. This term therefore vanishes, leaving 6% = - | (68/e”)(D+/87)d V = – | 68(E*/87)d V. (14.1) From this formula it follows that any increase in ...
Page 63
... present; an allowance for the change in p is beyond the accuracy of formulae which assume the linear relation D = & E. Then, equating to zero f from (15.15), we obtain the equilibrium condition at constant temperature in the form Po(p ...
... present; an allowance for the change in p is beyond the accuracy of formulae which assume the linear relation D = & E. Then, equating to zero f from (15.15), we obtain the equilibrium condition at constant temperature in the form Po(p ...
Page 67
... present in it. SOLUTION. Assuming go, a1, a2 constant and using the equations curl E = 0, div D = 80 div E = 4tpex, we have from (16.4) 6a, ća", GE2 a 1 f = − = — – (#a1 + a2)- + 1 - -] pe. E. - 87t CX, 280 $17. Piezoelectrics The ...
... present in it. SOLUTION. Assuming go, a1, a2 constant and using the equations curl E = 0, div D = 80 div E = 4tpex, we have from (16.4) 6a, ća", GE2 a 1 f = − = — – (#a1 + a2)- + 1 - -] pe. E. - 87t CX, 280 $17. Piezoelectrics The ...
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