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 37
... medium with permittivity & 1 , is the same as for a body with permittivity & 2 / 1 , surrounded by a vacuum . Let us consider how the results obtained in Chapter I for the electrostatic field of conductors will be modified if these ...
... medium with permittivity & 1 , is the same as for a body with permittivity & 2 / 1 , surrounded by a vacuum . Let us consider how the results obtained in Chapter I for the electrostatic field of conductors will be modified if these ...
Page 392
... medium , the coefficients x2 , B2 and 2 are , like ɛ2 , real , and the tensor ( 112.4 ) is Hermitian . When w1 → 0 and accordingly E , is real , it includes as a particular case double refraction in a static electric field , described ...
... medium , the coefficients x2 , B2 and 2 are , like ɛ2 , real , and the tensor ( 112.4 ) is Hermitian . When w1 → 0 and accordingly E , is real , it includes as a particular case double refraction in a static electric field , described ...
Page 426
... medium goes from a specified initial state ( suffix n ) to any final state ( ƒ ) is ( see QM , ( 40.5 ) ) 2 d3k ' dw ... medium gives the required result . PROBLEMS PROBLEM 1. Find the general form of the polarization dependence for ...
... medium goes from a specified initial state ( suffix n ) to any final state ( ƒ ) is ( see QM , ( 40.5 ) ) 2 d3k ' dw ... medium gives the required result . PROBLEMS PROBLEM 1. Find the general form of the polarization dependence for ...
Contents
ELECTROSTATICS OF CONDUCTORS | 1 |
2 The energy of the electrostatic field of conductors | 7 |
3 Methods of solving problems in electrostatics | 17 |
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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 sinē SOLUTION sphere suffixes superconducting surface symmetry temperature tensor theory thermodynamic potential transition uniaxial values variable velocity volume wave vector z-axis zero Απ