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 128
... expression ( 35.4 ) H is the true value of the magnetic field due both to external sources and to the currents themselves on which the force ( 35.4 ) acts . In calculating the total force from ( 35.5 ) , however , we can take H to be ...
... expression ( 35.4 ) H is the true value of the magnetic field due both to external sources and to the currents themselves on which the force ( 35.4 ) acts . In calculating the total force from ( 35.5 ) , however , we can take H to be ...
Page 218
... expression j2 / σ as for a conductor at rest . The expression j⚫E , however , is replaced byt j2σ = j • ( E + v × B / c ) . Thus , in a moving conductor , the sum E + vx B / c acts as an " effective " electric field producing the ...
... expression j2 / σ as for a conductor at rest . The expression j⚫E , however , is replaced byt j2σ = j • ( E + v × B / c ) . Thus , in a moving conductor , the sum E + vx B / c acts as an " effective " electric field producing the ...
Page 449
... expression gibb1 . This expression is the product of 1 / K2 and a fairly involved function of the direction of the vector K with respect to the crystal axes . For scattering near a principal maximum the diffusely scattered intensity is ...
... expression gibb1 . This expression is the product of 1 / K2 and a fairly involved function of the direction of the vector K with respect to the crystal axes . For scattering near a principal maximum the diffusely scattered intensity is ...
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