Electrodynamics of Continuous Media: Volume 8Covers the theory of electromagnetic fields in matter, and the theory of 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. |
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Page 106
... relation between the electric field E and induction D. Although H is , by analogy with E , usually called the ... relation between H and B in order to complete the system of equations . For example , in non - ferromagnetic bodies in ...
... relation between the electric field E and induction D. Although H is , by analogy with E , usually called the ... relation between H and B in order to complete the system of equations . For example , in non - ferromagnetic bodies in ...
Page 266
... relation between D and E can always be taken to be linear . † The most general linear relation between D ( t ) and the values of the function E ( t ) at all previous instants can be written in the integral form ∞ D ( t ) = E ( t ) + ...
... relation between D and E can always be taken to be linear . † The most general linear relation between D ( t ) and the values of the function E ( t ) at all previous instants can be written in the integral form ∞ D ( t ) = E ( t ) + ...
Page 348
... relation E = G. The relation E , nik Dk between the = E ; = ( nik ' + ie iki G1 ) Dx = Nik ' Dx + i ( D × G ) ;. ( 101.7 ) There is a similar linear relation D ; = & ik ' Ex + i ( E × g ) ;. ( 101.8 ) The connection between the ...
... relation E = G. The relation E , nik Dk between the = E ; = ( nik ' + ie iki G1 ) Dx = Nik ' Dx + i ( D × G ) ;. ( 101.7 ) There is a similar linear relation D ; = & ik ' Ex + i ( E × g ) ;. ( 101.8 ) The connection between the ...
Contents
ELECTROSTATICS OF CONDUCTORS | 1 |
2 The energy of the electrostatic field of conductors | 7 |
3 Methods of solving problems in electrostatics | 17 |
Copyright | |
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angle anisotropy anisotropy energy antiferromagnetic atoms averaging axes axis body boundary conditions calculation charge coefficient components conductor constant coordinates corresponding cross-section crystal Curie point curl H denote depends derivative determined dielectric diffraction direction discontinuity dispersion E₁ E₂ electric field electromagnetic electrons ellipsoid equation expression external field 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 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