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 333
... perpendicular . Moreover , H is perpendicular to E , and so the three vectors D , E , k , being all perpendicular to H , must be coplanar . Fig . 51 ( p . 334 ) shows the relative position of all these vectors . With respect to the ...
... perpendicular . Moreover , H is perpendicular to E , and so the three vectors D , E , k , being all perpendicular to H , must be coplanar . Fig . 51 ( p . 334 ) shows the relative position of all these vectors . With respect to the ...
Page 336
... perpendicular to any vector n - no in the plane . Since s , and no are So related by sono = 1 , we can write the equation as So ' n = 1 . ( 97.14 ) Hence it follows that 1 / s 。 is the length of the perpendicular from the origin to the ...
... perpendicular to any vector n - no in the plane . Since s , and no are So related by sono = 1 , we can write the equation as So ' n = 1 . ( 97.14 ) Hence it follows that 1 / s 。 is the length of the perpendicular from the origin to the ...
Page 437
... perpendicular to that plane . Since E is perpendicular to k , it is easy to see that in the first case the component of G in the plane perpendicular to k ' is zero . Thus transverse sound waves polarized in the plane of k and k ' do not ...
... perpendicular to that plane . Since E is perpendicular to k , it is easy to see that in the first case the component of G in the plane perpendicular to k ' is zero . Thus transverse sound waves polarized in the plane of k and k ' do not ...
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