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 54
... tensor of rank two , called the permittivity tensor ( or the dielectric tensor ) . The inhomogeneous term D。 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 D。 in ( 13.1 ) does not , however , appear for all crystals . The majority of the types of crystal symmetry do not admit this ...
Page 64
... tensor & ¡ . The state of a slightly deformed body is described by the strain tensor Wik = 1 / du¡ дик ( ou + 2 dxk axi where u ( x , y , z ) is the displacement vector for points in the body . Since these quantities are small , only ...
... tensor & ¡ . The state of a slightly deformed body is described by the strain tensor Wik = 1 / du¡ дик ( ou + 2 dxk axi where u ( x , y , z ) is the displacement vector for points in the body . Since these quantities are small , only ...
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 E¡E ...
... 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 E¡E ...
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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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