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 77
... direction of the spontaneous polarization here requires only a slight reconstruction of the lattice and can occur quite easily . The actual nature of the ferroelectric properties of a body depends on its crystal symmetry . The direction ...
... direction of the spontaneous polarization here requires only a slight reconstruction of the lattice and can occur quite easily . The actual nature of the ferroelectric properties of a body depends on its crystal symmetry . The direction ...
Page 320
... directions of the vector E in a plane perpendicular to the direction of propagation of the incident wave ( i.e. perpendicular to its wave vector k ) . Denoting by 9 and the polar angle and the azimuth of the direction of n relative to k ...
... directions of the vector E in a plane perpendicular to the direction of propagation of the incident wave ( i.e. perpendicular to its wave vector k ) . Denoting by 9 and the polar angle and the azimuth of the direction of n relative to k ...
Page 340
... direction , and the direction of the ray vector is that of n . In waves of the second type , called extraordinary waves , the magnitude of the wave vector depends on the angle 0 which it makes with the optical axis . By ( 98.2 ) 1 sin20 ...
... direction , and the direction of the ray vector is that of n . In waves of the second type , called extraordinary waves , the magnitude of the wave vector depends on the angle 0 which it makes with the optical axis . By ( 98.2 ) 1 sin20 ...
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