Electrodynamics of Continuous Media, Volume 8Covers 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. |
From inside the book
Results 1-3 of 75
Page 213
... variable currents in the circuits : 1 dJb ( 61.16 ) RaJa + Σ = Lab dt a The sum over b includes the self - inductance term ( b = a ) , and 8 , is the e.m.f. produced in the ath circuit by sources external to the system of currents ...
... variable currents in the circuits : 1 dJb ( 61.16 ) RaJa + Σ = Lab dt a The sum over b includes the self - inductance term ( b = a ) , and 8 , is the e.m.f. produced in the ath circuit by sources external to the system of currents ...
Page 265
... variable in time must necessarily be variable in space also . For a frequency w , the spatial periodicity is characterized by a wavelength ~ c / w . As the frequency increases , & eventually becomes comparable with the atomic dimensions ...
... variable in time must necessarily be variable in space also . For a frequency w , the spatial periodicity is characterized by a wavelength ~ c / w . As the frequency increases , & eventually becomes comparable with the atomic dimensions ...
Page 266
... variable as well as for static fields . Thus in any variable field , even if dispersion is present , the vector P = ( D - E ) / 4π retains its physical significance : it is the electric moment per unit volume . In rapidly varying fields ...
... variable as well as for static fields . Thus in any variable field , even if dispersion is present , the vector P = ( D - E ) / 4π retains its physical significance : it is the electric moment per unit volume . In rapidly varying fields ...
Contents
ELECTROSTATICS OF CONDUCTORS 1 The electrostatic field of conductors 13892 | 1 |
2 The energy of the electrostatic field of conductors | 7 |
3 Methods of solving problems in electrostatics | 17 |
Copyright | |
118 other sections not shown
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
angle anisotropy anisotropy energy antiferromagnetic atoms averaging axes axis body boundary conditions calculation charge circuit coefficient components conductor constant coordinates corresponding cross-section crystal Curie point curl H denote depends derivative determined dielectric diffraction direction discontinuity dispersion E₁ electric field electromagnetic electrons ellipsoid expression external field factor ferroelectric ferromagnet field H fluctuations fluid flux formula free energy frequency function given gives grad H₁ H₂ Hence incident induction integral isotropic Laplace's equation linear magnetic field magnetic moment Maxwell's equations medium normal obtain optical particle permittivity perpendicular perturbation phase plane polarization PROBLEM propagated properties pyroelectric quantities refraction relation respect result rotation satisfied scattering sin² SOLUTION sphere suffixes superconducting surface symmetry temperature tensor theory thermodynamic potential transition uniaxial values variable velocity volume wave vector z-axis zero Απ