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 240
... tangential to the surface . Finally , the normal component of the magnetic field and the tangential component of the electric field must be continuous . If the conductivity of the medium is infinite , the induced electric field is given ...
... tangential to the surface . Finally , the normal component of the magnetic field and the tangential component of the electric field must be continuous . If the conductivity of the medium is infinite , the induced electric field is given ...
Page 242
... tangential and rotational discontinuities form two different types , there are also discontinuities having the properties of both . These discontinuities are such that v and H are tangential in direction and continuous in magnitude . In ...
... tangential and rotational discontinuities form two different types , there are also discontinuities having the properties of both . These discontinuities are such that v and H are tangential in direction and continuous in magnitude . In ...
Page 251
... tangential magnetic field becomes weaker . In a fast wave , however , v , > H2 / 4лj , and from ( 73.6 ) it follows that H12 > H11 , the tangential magnetic field thus becoming stronger . 119 n A particular case of shock waves is that ...
... tangential magnetic field becomes weaker . In a fast wave , however , v , > H2 / 4лj , and from ( 73.6 ) it follows that H12 > H11 , the tangential magnetic field thus becoming stronger . 119 n A particular case of shock waves is that ...
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