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 68
... the crystal, we have D = Doi + 8, Ek +4ty, aga. (17.6) Corresponding additional terms appear in the thermodynamic quantities. The thermodynamic potential of a non-piezoelectric crystal in the absence of a 68 Electrostatics of Dielectrics.
... the crystal, we have D = Doi + 8, Ek +4ty, aga. (17.6) Corresponding additional terms appear in the thermodynamic quantities. The thermodynamic potential of a non-piezoelectric crystal in the absence of a 68 Electrostatics of Dielectrics.
Page 71
... corresponding coordinates. Hence, for example, from # = xx-yy+2ixy, we have a # = a, -a, +2io, The result is (b where a = 2iy,...; and b = 2y: are real constants. The relations between the componentsy, a in the coordinates x, y, z are ...
... corresponding coordinates. Hence, for example, from # = xx-yy+2ixy, we have a # = a, -a, +2io, The result is (b where a = 2iy,...; and b = 2y: are real constants. The relations between the componentsy, a in the coordinates x, y, z are ...
Page 82
... corresponding components oil (see 17.4)):8 us, = #P.+ uq, (1922) In the non-pyroelectric phase when E is small we can neglect the term in P.” in (1921): E = 2a(T–T.)P – ya Substituting P. in (1922), we find xy" 2 'y y = — E - * * * = AU ...
... corresponding components oil (see 17.4)):8 us, = #P.+ uq, (1922) In the non-pyroelectric phase when E is small we can neglect the term in P.” in (1921): E = 2a(T–T.)P – ya Substituting P. in (1922), we find xy" 2 'y y = — E - * * * = AU ...
Page 84
... corresponding component of the vector P. and the theory based on the thermodynamic potential (19.1) is applicable to them. The components of P in a plane perpendicular to the principal axis of symmetry in a uniaxial crystal are ...
... corresponding component of the vector P. and the theory based on the thermodynamic potential (19.1) is applicable to them. The components of P in a plane perpendicular to the principal axis of symmetry in a uniaxial crystal are ...
Page 87
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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