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 394
... particle and individual atoms . In a solid or liquid medium , however , several atoms may interact simultaneously with the particle . The effect of this on the energy loss by the particle can be macroscopically regarded as resulting ...
... particle and individual atoms . In a solid or liquid medium , however , several atoms may interact simultaneously with the particle . The effect of this on the energy loss by the particle can be macroscopically regarded as resulting ...
Page 405
... particle increases , the condition » wo is ultimately fulfilled in any medium , i.e. whatever the electron density N ( even in a gas ) . The velocity required is , however , the greater , the smaller N , i.e. the more rarefied the ...
... particle increases , the condition » wo is ultimately fulfilled in any medium , i.e. whatever the electron density N ( even in a gas ) . The velocity required is , however , the greater , the smaller N , i.e. the more rarefied the ...
Page 406
... particle moving in it . The distinction between the two types of radiation appears with particular clarity when the particle has a very large mass : the bremsstrahlung disappears , but the Cherenkov radiation is unaffected . The wave ...
... particle moving in it . The distinction between the two types of radiation appears with particular clarity when the particle has a very large mass : the bremsstrahlung disappears , but the Cherenkov radiation is unaffected . 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