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 2
... derivative ch / êt also vanishes on averaging , and we find that the static electric field in the vacuum satisfies the usual equations div E = 0 , curl E = 0 , i.e. it is a potential field with a potential and satisfies Laplace's ...
... derivative ch / êt also vanishes on averaging , and we find that the static electric field in the vacuum satisfies the usual equations div E = 0 , curl E = 0 , i.e. it is a potential field with a potential and satisfies Laplace's ...
Page 96
... derivatives are taken at constant area S. To calculate these , we express , in terms of the thermodynamic potential ... derivative to be positive becomes 10 or de2 J2gos дег = аф de = do / dp > 0 . 10ф > 0 , S do ( 25.7 ) This result ...
... derivatives are taken at constant area S. To calculate these , we express , in terms of the thermodynamic potential ... derivative to be positive becomes 10 or de2 J2gos дег = аф de = do / dp > 0 . 10ф > 0 , S do ( 25.7 ) This result ...
Page 220
... derivative of B with respect to axes fixed in a rotating body . For the sum of the first two terms is the " substantial " time derivative ( derivative following the motion ) dB / dt , which gives the rate of change of B at a point ...
... derivative of B with respect to axes fixed in a rotating body . For the sum of the first two terms is the " substantial " time derivative ( derivative following the motion ) dB / dt , which gives the rate of change of B at a point ...
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