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 86
Page 1
... result from the molecular structure of matter. For example, instead of the actual “microscopic” value of the electric field e, we discuss its averaged value, denoted by E. e = E. (1.1) The fundamental equations of the electrodynamics of ...
... result from the molecular structure of matter. For example, instead of the actual “microscopic” value of the electric field e, we discuss its averaged value, denoted by E. e = E. (1.1) The fundamental equations of the electrodynamics of ...
Page 6
... resulting from the introduction of the uncharged conductor with the energy of the fictitious field in which there are no ... result can also be formulated thus: an uncharged conductor remote from a system of given charges is attracted ...
... resulting from the introduction of the uncharged conductor with the energy of the fictitious field in which there are no ... result can also be formulated thus: an uncharged conductor remote from a system of given charges is attracted ...
Page 17
... result that [. log sin p dot = – t log2. In the integral which contains the difference r (z') – t (2), we can neglect the a term in R, since it no longer causes the integral to diverge. Thus t t(z') — t(z) , , (#z = r(z)log4(l” – z*)/a ...
... result that [. log sin p dot = – t log2. In the integral which contains the difference r (z') – t (2), we can neglect the a term in R, since it no longer causes the integral to diverge. Thus t t(z') — t(z) , , (#z = r(z)log4(l” – z*)/a ...
Page 28
... result is (£ - * =#|V(i+b)+ V.I./nl. where we now take V& positive and the two signs + correspond to the regions z > 0 and z < 0. - - - At large distances from the slit we have in the upper half-space & = y + 2* = r^, and the potential ...
... result is (£ - * =#|V(i+b)+ V.I./nl. where we now take V& positive and the two signs + correspond to the regions z > 0 and z < 0. - - - At large distances from the slit we have in the upper half-space & = y + 2* = r^, and the potential ...
Page 29
... result in §3, Problem 3, for the case 60 < 1. $5. The forces on a conductor In an electric field certain forces act on the surface of a conductor. These forces are easily calculated as follows. The momentum flux density in an electric ...
... result in §3, Problem 3, for the case 60 < 1. $5. The forces on a conductor In an electric field certain forces act on the surface of a conductor. These forces are easily calculated as follows. The momentum flux density in an electric ...
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