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 54
... tensor of rank two , called the permittivity tensor ( or the dielectric tensor ) . The inhomogeneous term Do in ( 13.1 ) does not , however , appear for all crystals . The majority of the types of crystal symmetry do not admit this ...
... tensor of rank two , called the permittivity tensor ( or the dielectric tensor ) . The inhomogeneous term Do in ( 13.1 ) does not , however , appear for all crystals . The majority of the types of crystal symmetry do not admit this ...
Page 347
... tensor of rank two linear in E could be constructed . The next terms in the expansion of & must therefore be quadratic in the field . From the components of the vector E we can form two symmetrical tensors of rank two , E281 and EE ...
... tensor of rank two linear in E could be constructed . The next terms in the expansion of & must therefore be quadratic in the field . From the components of the vector E we can form two symmetrical tensors of rank two , E281 and EE ...
Page 416
... tensor IB in that plane ( Greek suffixes take two values ) . The tensor Ig is , by definition , Hermitian : Lap = Ipa * . It can be diagonalized , and the ratio of its two principal values gives the degree of depolarization , while ...
... tensor IB in that plane ( Greek suffixes take two values ) . The tensor Ig is , by definition , Hermitian : Lap = Ipa * . It can be diagonalized , and the ratio of its two principal values gives the degree of depolarization , while ...
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 sinē SOLUTION sphere suffixes superconducting surface symmetry temperature tensor theory thermodynamic potential transition uniaxial values variable velocity volume wave vector z-axis zero Απ