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 322
... cos2 9 ( cos2 + 1712 sin2 ) } do , where and 9 are the angles shown in Fig . 47. In scattering of unpolarized light we have do = ( a * w * / c * ) { } [ 1 + | y | 2 ] [ 1 + cos2 9 ] − ( y + y * ) cos 9 } do , - and the degree of ...
... cos2 9 ( cos2 + 1712 sin2 ) } do , where and 9 are the angles shown in Fig . 47. In scattering of unpolarized light we have do = ( a * w * / c * ) { } [ 1 + | y | 2 ] [ 1 + cos2 9 ] − ( y + y * ) cos 9 } do , - and the degree of ...
Page 445
... cos2 9 ) [ nb2 ( nb2 / k ) 2 df . As n → 0 this formula becomes ( 124.19 ) . If { nb2Z / k » 1 ( which is compatible with ŋ « 1 ) , the squared sine can be replaced by its mean value , and we have e2 21+ cos2 9 σ = 4π2 mc n2b + Inol2s ...
... cos2 9 ) [ nb2 ( nb2 / k ) 2 df . As n → 0 this formula becomes ( 124.19 ) . If { nb2Z / k » 1 ( which is compatible with ŋ « 1 ) , the squared sine can be replaced by its mean value , and we have e2 21+ cos2 9 σ = 4π2 mc n2b + Inol2s ...
Page 448
... cos2 9 ) < | b · u exp ( − iK · r ) d V | 2 > do ' , ( 126.2 ) where K = k ' - k - b . The scattered intensity is large for directions where K « b . The integral Suexp ( − iK · r ) dV gives the Fourier space component of u whose wave ...
... cos2 9 ) < | b · u exp ( − iK · r ) d V | 2 > do ' , ( 126.2 ) where K = k ' - k - b . The scattered intensity is large for directions where K « b . The integral Suexp ( − iK · r ) dV gives the Fourier space component of u whose wave ...
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