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 80
Page 9
... distribution of surface charge induced on the bounding plane by the point charge e is given by 1 | 6p & Cl O ... distributed over the large surface of the conductor. Next, let us consider a more difficult problem, that of the field due ...
... distribution of surface charge induced on the bounding plane by the point charge e is given by 1 | 6p & Cl O ... distributed over the large surface of the conductor. Next, let us consider a more difficult problem, that of the field due ...
Page 14
... distribution of charge on the surface of the sphere is given by a = – (1/4").[ād)ór]. - R = (3G/4t) cos 6. The total charge e = 0. The dipole moment of the sphere is most easily found by comparing b1 with the potential 4° r/r” of an ...
... distribution of charge on the surface of the sphere is given by a = – (1/4").[ād)ór]. - R = (3G/4t) cos 6. The total charge e = 0. The dipole moment of the sphere is most easily found by comparing b1 with the potential 4° r/r” of an ...
Page 16
... projection. Determine the charge distribution on the surface. SOLUTION. In the field determined in Problem 1, whose potential is R3 q = constant X 2 (1 --> ), r the plane z = 0 with a projection r = 16 Electrostatics of Conductors.
... projection. Determine the charge distribution on the surface. SOLUTION. In the field determined in Problem 1, whose potential is R3 q = constant X 2 (1 --> ), r the plane z = 0 with a projection r = 16 Electrostatics of Conductors.
Page 17
... distribution on the plane part of the surface is given by |#| --(1-#) of = - — || – = Go || 1 - - ); 4: Lóz J._o r we have taken the constant in p as – 4too, so that go is the charge density far from the projection. On the surface of ...
... distribution on the plane part of the surface is given by |#| --(1-#) of = - — || – = Go || 1 - - ); 4: Lóz J._o r we have taken the constant in p as – 4too, so that go is the charge density far from the projection. On the surface of ...
Page 18
... distribution of charge over them is not uniform. To determine the required correction in a first approximation, we consider points which are at distances x from the edge such that d 4 x < \/S. For example, taking the upper layer (at ...
... distribution of charge over them is not uniform. To determine the required correction in a first approximation, we consider points which are at distances x from the edge such that d 4 x < \/S. For example, taking the upper layer (at ...
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