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 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 317
... obtain the required damping coefficient a . With this definition , a gives the rate of damping of the wave amplitude , which decreases along the waveguide as e - az . Expressing all quantities in terms of E , or H , by means of formulae ...
... obtain the required damping coefficient a . With this definition , a gives the rate of damping of the wave amplitude , which decreases along the waveguide as e - az . Expressing all quantities in terms of E , or H , by means of formulae ...
Page 336
... obtain SD = 8Hxn + Hx8n , SH = nx8E + 8nxE . ( 97.15 ) We take the scalar product of the first equation with E and of the second with H , obtaining = E.SD H.SH + ExH 8n , • H.SHD.SE + ExH 8n . But D.SE = & ix ExSE¡ = E · SD , and so ...
... obtain SD = 8Hxn + Hx8n , SH = nx8E + 8nxE . ( 97.15 ) We take the scalar product of the first equation with E and of the second with H , obtaining = E.SD H.SH + ExH 8n , • H.SHD.SE + ExH 8n . But D.SE = & ix ExSE¡ = E · SD , and so ...
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