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 108
... infinite , and in particular is finite on a surface separating two media . Hence the term on the right of ( 30.2 ) ... infinite at the boundary . The field equations are simpler in the two - dimensional problem of finding the magnetic ...
... infinite , and in particular is finite on a surface separating two media . Hence the term on the right of ( 30.2 ) ... infinite at the boundary . The field equations are simpler in the two - dimensional problem of finding the magnetic ...
Page 271
... infinite medium . SOLUTION . With the tensor from ( 1 ) , equation ( 79.6 ) becomes 224 dx2 dy2 22 ) = 0 . az2 ( 2 ) Puttinger , we find μ ( w ) = −cot20 , where 0 is the angle between k and the easy - magnetization axis ( the z- axis ) ...
... infinite medium . SOLUTION . With the tensor from ( 1 ) , equation ( 79.6 ) becomes 224 dx2 dy2 22 ) = 0 . az2 ( 2 ) Puttinger , we find μ ( w ) = −cot20 , where 0 is the angle between k and the easy - magnetization axis ( the z- axis ) ...
Page 299
... infinite media of the substances in regions 2 and 3 . SOLUTION . We denote by A , and A , the amplitudes of the field ( E or H , whichever is parallel to the layer ) in the incident and reflected waves . The field in the layer consists ...
... infinite media of the substances in regions 2 and 3 . SOLUTION . We denote by A , and A , the amplitudes of the field ( E or H , whichever is parallel to the layer ) in the incident and reflected waves . The field in the layer consists ...
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