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 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 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 ...
... 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 ...
Page 351
... direction of n , we can write this formula , to the same accuracy , in the vector form 1 2 nt g 2n0 = no2 . ( 101.20 ) Hence we see that the wave - vector surface in this case consists of two spheres with radius no , whose centres are ...
... direction of n , we can write this formula , to the same accuracy , in the vector form 1 2 nt g 2n0 = no2 . ( 101.20 ) Hence we see that the wave - vector surface in this case consists of two spheres with radius no , whose centres are ...
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