Electrodynamics of Continuous MediaCovers 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 81
... Let us consider ferroelectrics which belong ( in the non - pyroelectric phase ) to the cubic system . The cubic symmetry admits two independent fourth - order invariants formed from the components of the vector P , which may be taken as ...
... Let us consider ferroelectrics which belong ( in the non - pyroelectric phase ) to the cubic system . The cubic symmetry admits two independent fourth - order invariants formed from the components of the vector P , which may be taken as ...
Page 352
... Let us consider the purely quadratic effect ( called the Cotton - Mouton effect ) which occurs when n and g are perpendicular . In equations ( 101.11 ) and ( 101.12 ) we have G2 = 0 , and 1 / no12 , 1 / n022 are respectively 7 , 71 ...
... Let us consider the purely quadratic effect ( called the Cotton - Mouton effect ) which occurs when n and g are perpendicular . In equations ( 101.11 ) and ( 101.12 ) we have G2 = 0 , and 1 / no12 , 1 / n022 are respectively 7 , 71 ...
Page 446
... Let us now consider another case , where the incident wave is monochromatic but its components have varying directions of k which differ by rotation about some axis ; † let 1 be a unit vector along that axis , and the angle of rotation ...
... Let us now consider another case , where the incident wave is monochromatic but its components have varying directions of k which differ by rotation about some axis ; † let 1 be a unit vector along that axis , and the angle of rotation ...
Contents
ELECTROSTATICS OF CONDUCTORS | 1 |
2 The energy of the electrostatic field of conductors | 7 |
4 A conducting ellipsoid | 27 |
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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 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