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 1
... field of conductors MACROSCOPIC electrodynamics is concerned with the study of electromagnetic fields in space that ... electric field e , we discuss its averaged value , denoted by E : ĕ = E. ( 1.1 ) The fundamental equations of the ...
... field of conductors MACROSCOPIC electrodynamics is concerned with the study of electromagnetic fields in space that ... electric field e , we discuss its averaged value , denoted by E : ĕ = E. ( 1.1 ) The fundamental equations of the ...
Page 44
... field which equals the mean field E. Assuming the particles spherical and using formula ( 8.2 ) , we obtain for the ... electric field The question of the change in thermodynamic properties owing to the presence of an electric field does ...
... field which equals the mean field E. Assuming the particles spherical and using formula ( 8.2 ) , we obtain for the ... electric field The question of the change in thermodynamic properties owing to the presence of an electric field does ...
Page 347
... electric field An isotropic body becomes optically anisotropic when placed in a static electric field . This anisotropy may be regarded as the result of a change in the permittivity due to the static field . Although this change is ...
... electric field An isotropic body becomes optically anisotropic when placed in a static electric field . This anisotropy may be regarded as the result of a change in the permittivity due to the static field . Although this change is ...
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