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. |
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Page 97
... electrons . This means not only that the temperature must be constant throughout the body , but also that the sum eo + should be constant , where 5 , is the chemical potential of the conduction electrons in the metal ( for = 0 ) . If ...
... electrons . This means not only that the temperature must be constant throughout the body , but also that the sum eo + should be constant , where 5 , is the chemical potential of the conduction electrons in the metal ( for = 0 ) . If ...
Page 398
... electrons ) ionization energy of an atom is usually almost independent of its interaction with other atoms , being determined mainly by the electrons of the inner shells , which are almost unaffected by that interaction . Moreover ...
... electrons ) ionization energy of an atom is usually almost independent of its interaction with other atoms , being determined mainly by the electrons of the inner shells , which are almost unaffected by that interaction . Moreover ...
Page 439
... electron in the field of the electromagnetic wave as mv ' = eE , i.e. the electrons may be regarded as free ( see §78 ) . ( 124.1 ) From ( 124.1 ) we find the additional velocity acquired by the electron under the action of the wave ...
... electron in the field of the electromagnetic wave as mv ' = eE , i.e. the electrons may be regarded as free ( see §78 ) . ( 124.1 ) From ( 124.1 ) we find the additional velocity acquired by the electron under the action of the wave ...
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 |
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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