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 64
... Formula ( 16.3 ) is valid whatever the relation between D and E. For a body which is neither pyroelectric nor piezoelectric , so that D ; = & ik Ek , F is given by formula ( 13.4 ) and the required derivatives are dƑ / du¡k = dƑ 。/ du ...
... Formula ( 16.3 ) is valid whatever the relation between D and E. For a body which is neither pyroelectric nor piezoelectric , so that D ; = & ik Ek , F is given by formula ( 13.4 ) and the required derivatives are dƑ / du¡k = dƑ 。/ du ...
Page 123
... formula also to a solenoid whose length h is finite , but large compared with b . Then the self - inductance is L ... formula ( 33.2 ) . On account of the assumed surface distribution of the current , the integral in this formula becomes ...
... formula also to a solenoid whose length h is finite , but large compared with b . Then the self - inductance is L ... formula ( 33.2 ) . On account of the assumed surface distribution of the current , the integral in this formula becomes ...
Page 397
... formula , and the result ist - Ĵ am 2лiNе2 ( dw ωη " ( ω ) δω = = 2π2 Ne2 / m . m W σ We define a mean frequency of the motion of the atomic electrons by 00 I wn " ( w ) log w dw ( 113.10 ) log @ = ∞ S wn " ( w ) dw m = 2n2 Ne2 wn ...
... formula , and the result ist - Ĵ am 2лiNе2 ( dw ωη " ( ω ) δω = = 2π2 Ne2 / m . m W σ We define a mean frequency of the motion of the atomic electrons by 00 I wn " ( w ) log w dw ( 113.10 ) log @ = ∞ S wn " ( w ) dw m = 2n2 Ne2 wn ...
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