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 188
... obtain the difference of the specific heats ( at constant pressure ) of the two phases . The terms involving the thermal - expansion coefficient and the compressibility are usually very small in comparison with the remaining terms ...
... obtain the difference of the specific heats ( at constant pressure ) of the two phases . The terms involving the thermal - expansion coefficient and the compressibility are usually very small in comparison with the remaining terms ...
Page 336
... obtain SD = 8Hxn + Hxon , SH = n × 8E + dn × E. ( 97.15 ) We take the scalar product of the first equation with E and of the second with H , obtaining · E SDH SH + ExH 8n , = H.SH = • D SE + EXH⚫dn . But D.SE = & ik ExSE ; E · 8D , and ...
... obtain SD = 8Hxn + Hxon , SH = n × 8E + dn × E. ( 97.15 ) We take the scalar product of the first equation with E and of the second with H , obtaining · E SDH SH + ExH 8n , = H.SH = • D SE + EXH⚫dn . But D.SE = & ik ExSE ; E · 8D , and ...
Page 417
... obtain three equations , from which the significance of the coefficients in ( 117.13 ) becomes evident : Go = √ ( a ( 1 ) a ( 2 ) * > dv , Gs ( 1 ) Sik ( 2 ) * > dV , = G2 = < a1a ( 2 ) * > dV . Ga = These quantities are real and ...
... obtain three equations , from which the significance of the coefficients in ( 117.13 ) becomes evident : Go = √ ( a ( 1 ) a ( 2 ) * > dv , Gs ( 1 ) Sik ( 2 ) * > dV , = G2 = < a1a ( 2 ) * > dV . Ga = These quantities are real and ...
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 |
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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