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 80
Page 1
... distributed on its surface, however, in such a way that the fields which they produce in its interior are mutually ... distribution of charges on their surfaces. At any point far from the surface of the body, the mean field E in the ...
... distributed on its surface, however, in such a way that the fields which they produce in its interior are mutually ... distribution of charges on their surfaces. At any point far from the surface of the body, the mean field E in the ...
Page 3
... distribution of charges over the surface of the conductor is given by the formula 4ta = E = – 6 b/ón, (1.9) the derivative of the potential being taken along the outward normal to the surface. The total charge on the conductor is 1 [ćp ...
... distribution of charges over the surface of the conductor is given by the formula 4ta = E = – 6 b/ón, (1.9) the derivative of the potential being taken along the outward normal to the surface. The total charge on the conductor is 1 [ćp ...
Page 5
... that another inequality which must be satisfied if the form (2.9) is positive is C.C. P. Cab'. charge distribution on the conductors undergoes an infinitesimal change (the $2 The energy of the electrostatic field of conductors 5.
... that another inequality which must be satisfied if the form (2.9) is positive is C.C. P. Cab'. charge distribution on the conductors undergoes an infinitesimal change (the $2 The energy of the electrostatic field of conductors 5.
Page 6
... distribution on the conductors undergoes an infinitesimal change (the total charge on each conductor remaining unaltered), in which the charges may penetrate into the conductors; we ignore the fact that such a charge distribution cannot ...
... distribution on the conductors undergoes an infinitesimal change (the total charge on each conductor remaining unaltered), in which the charges may penetrate into the conductors; we ignore the fact that such a charge distribution cannot ...
Page 8
... distributed along the axis of the wire (for a right cylinder, it would be exactly the same). Hence the potential of the ring is _ e £dl 2nb fr' 'b. where r is the distance from a point on the surface of the ring to an element dl of the ...
... distributed along the axis of the wire (for a right cylinder, it would be exactly the same). Hence the potential of the ring is _ e £dl 2nb fr' 'b. where r is the distance from a point on the surface of the ring to an element dl of 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 |
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