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 149
... layer ; the direction of M depends only on x . The rotation of the vector M across the layer must take place in the yz - plane , i.e. M1 = 0 everywhere . This is seen as follows . The non - uniformity and anisotropy energies in a ...
... layer ; the direction of M depends only on x . The rotation of the vector M across the layer must take place in the yz - plane , i.e. M1 = 0 everywhere . This is seen as follows . The non - uniformity and anisotropy energies in a ...
Page 194
... layers , i.e. to increase their thickness . The energy of emergence of the layers at the free surface of the body has the opposite tendency . The layer thickness increases with the size of the body , and consequently ( for the same ...
... layers , i.e. to increase their thickness . The energy of emergence of the layers at the free surface of the body has the opposite tendency . The layer thickness increases with the size of the body , and consequently ( for the same ...
Page 299
... layer ) in the incident and reflected waves . The field in the layer consists of the refracted wave ( amplitude A2 ) and the wave reflected from region 3 ( amplitude A2 ' ) . The boundary condition between regions 1 and 2 gives A2 = a ...
... layer ) in the incident and reflected waves . The field in the layer consists of the refracted wave ( amplitude A2 ) and the wave reflected from region 3 ( amplitude A2 ' ) . The boundary condition between regions 1 and 2 gives A2 = a ...
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