Electrodynamics of Continuous Media, Volume 8Covers 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 77
... polarization also is small ) . For this reason the change in direction of the spontaneous polarization here requires only a slight reconstruction of the lattice and can occur quite easily . The actual nature of the ferroelectric ...
... polarization also is small ) . For this reason the change in direction of the spontaneous polarization here requires only a slight reconstruction of the lattice and can occur quite easily . The actual nature of the ferroelectric ...
Page 81
... polarization P averaged over such portions . Its component P , can evidently take values in the range between the ordinates of a and a ' in Fig . 14 , i.e. -√ [ ( T. - T ) a / 2B ] < P2 < √ / [ ( T. − T ) a / 2B ] . ( 19.13 ) In ...
... polarization P averaged over such portions . Its component P , can evidently take values in the range between the ordinates of a and a ' in Fig . 14 , i.e. -√ [ ( T. - T ) a / 2B ] < P2 < √ / [ ( T. − T ) a / 2B ] . ( 19.13 ) In ...
Page 83
... polarization results in a certain deformation of the body . If there are no internal stresses and the field E is zero , the strain u ,, is proportional to Po , i.e. varies with temperature as √ ( T ̧ − T ) . If the symmetry ( cubic ...
... polarization results in a certain deformation of the body . If there are no internal stresses and the field E is zero , the strain u ,, is proportional to Po , i.e. varies with temperature as √ ( T ̧ − T ) . If the symmetry ( cubic ...
Contents
ELECTROSTATICS OF CONDUCTORS 1 The electrostatic field of conductors 13892 | 1 |
2 The energy of the electrostatic field of conductors | 7 |
3 Methods of solving problems in electrostatics | 17 |
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Electrodynamics of Continuous Media: Volume 8 L D Landau,E.M. Lifshitz,L. P. Pitaevskii Snippet view - 1995 |
Common terms and phrases
angle anisotropy anisotropy energy antiferromagnetic atoms averaging axes axis body boundary conditions calculation charge circuit coefficient components conductor constant coordinates corresponding cross-section crystal Curie point curl H denote depends derivative determined dielectric diffraction direction discontinuity dispersion E₁ 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