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 200
... equations ( 58.1 ) and ( 58.4 ) , E is the induced electric field resulting from the variation of the magnetic field . When H is known , the field E can be immediately determined by equation ( 58.4 ) . The equation for H is obtained by ...
... equations ( 58.1 ) and ( 58.4 ) , E is the induced electric field resulting from the variation of the magnetic field . When H is known , the field E can be immediately determined by equation ( 58.4 ) . The equation for H is obtained by ...
Page 241
... equation ( 70.5 ) we can take Voutside the brackets and divide this equation by equation ( 70.4 ) , obtaining and j = H√ ( 4π V ) [ v , ] = √ ( V / 4π ) [ H , ] , ( 71.4 ) ( 71.5 ) In equation ( 70.2 ) we put w = & + PV ; since V is ...
... equation ( 70.5 ) we can take Voutside the brackets and divide this equation by equation ( 70.4 ) , obtaining and j = H√ ( 4π V ) [ v , ] = √ ( V / 4π ) [ H , ] , ( 71.4 ) ( 71.5 ) In equation ( 70.2 ) we put w = & + PV ; since V is ...
Page 305
... equations can be solved in a general form in the important case where the con- ditions of propagation approximate to those of geometrical optics . In what follows we shall assume that the function ε ( z ) is real . † In equation ( 88.3 ) ...
... equations can be solved in a general form in the important case where the con- ditions of propagation approximate to those of geometrical optics . In what follows we shall assume that the function ε ( z ) is real . † In equation ( 88.3 ) ...
Contents
ELECTROSTATICS OF CONDUCTORS | 1 |
2 The energy of the electrostatic field of conductors | 7 |
3 Methods of solving problems in electrostatics | 17 |
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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