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 39
... field is small, i.e. < - 5 mT. To maintain simplicity in the equations used in the following analyses, volume susceptibility k, volume magnetization M, and the field H ... field. In an anisotropic medium the magnetization is not in general ...
... field is small, i.e. < - 5 mT. To maintain simplicity in the equations used in the following analyses, volume susceptibility k, volume magnetization M, and the field H ... field. In an anisotropic medium the magnetization is not in general ...
Page 264
... FIELDS - > = x Let I : TM → TM be the identity map . Thus we can regard I as a vector field I over the projection II ( cf. Section 2.0 ) . Similarly we regard the restriction I。 of I to + as a vector field over E. A vector field H on ...
... FIELDS - > = x Let I : TM → TM be the identity map . Thus we can regard I as a vector field I over the projection II ( cf. Section 2.0 ) . Similarly we regard the restriction I。 of I to + as a vector field over E. A vector field H on ...
Page 11
... field , that the actual field within the metal shall be uniform all through it even though not the same as the im- pressed field - so that I and H. and H , shall all three differ from zero , and the resultant H of H. and H ; shall be ...
... field , that the actual field within the metal shall be uniform all through it even though not the same as the im- pressed field - so that I and H. and H , shall all three differ from zero , and the resultant H of H. and H ; shall be ...
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