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 51
... isotropic dielectrics For a solid dielectric in an electric field the concept of pressure cannot be defined as for an isotropic body in the absence of a field , because the forces acting on a dielectric ( which we shall determine in ...
... isotropic dielectrics For a solid dielectric in an electric field the concept of pressure cannot be defined as for an isotropic body in the absence of a field , because the forces acting on a dielectric ( which we shall determine in ...
Page 347
... isotropic body in the zero - order approximation , we have Ɛik ( 0 ) 8 . There can be no terms in ε which are of the first order in the field , since in an isotropic body there is no constant vector with which a tensor of rank two ...
... isotropic body in the zero - order approximation , we have Ɛik ( 0 ) 8 . There can be no terms in ε which are of the first order in the field , since in an isotropic body there is no constant vector with which a tensor of rank two ...
Page 366
... isotropic medium , Bikim must be expressed in terms of the unit tensor only , i.e. must have the form Bikim = B1SikSim + 1⁄2ẞ 2 ( §¡18 km + 8μdim ) ; Im il it contains only two independent components . In an isotropic body we also have ...
... isotropic medium , Bikim must be expressed in terms of the unit tensor only , i.e. must have the form Bikim = B1SikSim + 1⁄2ẞ 2 ( §¡18 km + 8μdim ) ; Im il it contains only two independent components . In an isotropic body we also have ...
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