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 6-10 of 66
Page 30
... identity states that 64//de. = p, and 64//ćq = - F. Using the variables p, instead of ea, we have d? = –X e.dp, - F.dq, (5.9) which gives (5.7). At the end of $2 we have discussed the energy 30 Electrostatics of Conductors.
... identity states that 64//de. = p, and 64//ćq = - F. Using the variables p, instead of ea, we have d? = –X e.dp, - F.dq, (5.9) which gives (5.7). At the end of $2 we have discussed the energy 30 Electrostatics of Conductors.
Page 46
... variables. Such are * * U = U – E. D/4t, F = F – E. D/4t. (10.8) On differentiating these we have dU = TaS+ (dp – D dE/4t, | (10.9) dF = – SdT+&dp – D dE/4t. Hence, in particular, D = -47(OU/CE), = -47(ČF/óE), (10.10) It should be ...
... variables. Such are * * U = U – E. D/4t, F = F – E. D/4t. (10.8) On differentiating these we have dU = TaS+ (dp – D dE/4t, | (10.9) dF = – SdT+&dp – D dE/4t. Hence, in particular, D = -47(OU/CE), = -47(ČF/óE), (10.10) It should be ...
Page 56
... and in a pyroelectric one is independent of the face configuration. # In Problems 2–6 the anisotropic dielectric is assumed to be non-pyroelectric. By the introduction of new variables x = x/x/8", y' 56 Electrostatics of Dielectrics.
... and in a pyroelectric one is independent of the face configuration. # In Problems 2–6 the anisotropic dielectric is assumed to be non-pyroelectric. By the introduction of new variables x = x/x/8", y' 56 Electrostatics of Dielectrics.
Page 68
... variables in (17.2) include the components of the tensor up. It is sometimes convenient to use instead the components oil. To do so, we must introduce the thermodynamic potential, defined as d = F – unan. (17.3) For the differential of ...
... variables in (17.2) include the components of the tensor up. It is sometimes convenient to use instead the components oil. To do so, we must introduce the thermodynamic potential, defined as d = F – unan. (17.3) For the differential of ...
Page 72
... variables, instead of oil. We write F in the form * 1 1 F = Fo + *****". - *FF, 47 E. Doi + B.M.E. uti, whence Oik = 6F/ău, = Mianu, +/h." E. The equations of motion from the theory of elasticity are - - dois dut, 6E. i = - = Alivia ...
... variables, instead of oil. We write F in the form * 1 1 F = Fo + *****". - *FF, 47 E. Doi + B.M.E. uti, whence Oik = 6F/ău, = Mianu, +/h." E. The equations of motion from the theory of elasticity are - - dois dut, 6E. i = - = Alivia ...
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