Electrodynamics of Continuous Media: Volume 8Covers the theory of electromagnetic fields in matter, and the theory of 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. |
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Page 116
... field . One of the thermodynamic properties of this quantity is that the change in it gives the work done by the ... H.SH ) dV / 4π = - [ ( H - H ) · 8HdV / 4л - [ В · ( ¿ H - ƐH ) dν / 4π - √ ( в - Н ) · ¿ HdV / 4π . Introducing the ...
... field . One of the thermodynamic properties of this quantity is that the change in it gives the work done by the ... H.SH ) dV / 4π = - [ ( H - H ) · 8HdV / 4л - [ В · ( ¿ H - ƐH ) dν / 4π - √ ( в - Н ) · ¿ HdV / 4π . Introducing the ...
Page 182
... field is present . This means that no dissipation of energy occurs , whose replacement would involve work being done by an external field ... H ̧ = H sin 182 Superconductivity §54 The superconductivity current.
... field is present . This means that no dissipation of energy occurs , whose replacement would involve work being done by an external field ... H ̧ = H sin 182 Superconductivity §54 The superconductivity current.
Page 230
... field is only slightly perturbed by the motion of the fluid . If the unperturbed field is independent of time ( as we shall assume ) , the change H ' in this field in the moving fluid may be estimated by comparing the two terms on the ...
... field is only slightly perturbed by the motion of the fluid . If the unperturbed field is independent of time ( as we shall assume ) , the change H ' in this field in the moving fluid may be estimated by comparing the two terms on the ...
Contents
ELECTROSTATICS OF CONDUCTORS | 1 |
2 The energy of the electrostatic field of conductors | 7 |
3 Methods of solving problems in electrostatics | 17 |
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 equation expression external field 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 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