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 56
... symmetry transformations , and that this will be the direction of the con- stant vector Do. This condition is satisfied only by those symmetry groups which consist of a single axis together with planes of symmetry which pass through the ...
... symmetry transformations , and that this will be the direction of the con- stant vector Do. This condition is satisfied only by those symmetry groups which consist of a single axis together with planes of symmetry which pass through the ...
Page 84
... symmetry in a uniaxial crystal are transformed by a two - dimensional irreducible representation and can serve as the order parameter for that representation . Lastly , in crystals with cubic symmetry , all three components of the ...
... symmetry in a uniaxial crystal are transformed by a two - dimensional irreducible representation and can serve as the order parameter for that representation . Lastly , in crystals with cubic symmetry , all three components of the ...
Page 131
... symmetry groups of the current distribution j ( x , y , z ) ? This symmetry contains , first of all , the usual rotations , reflections and translations , and so the possible symmetry groups of j always include the usual 230 ...
... symmetry groups of the current distribution j ( x , y , z ) ? This symmetry contains , first of all , the usual rotations , reflections and translations , and so the possible symmetry groups of j always include the usual 230 ...
Contents
ELECTROSTATICS OF CONDUCTORS | 1 |
2 The energy of the electrostatic field of conductors | 7 |
4 A conducting ellipsoid | 27 |
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 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