Electrodynamics of Continuous Media |
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Page 266
... frequency , ( 2 ) gives or , conversely , 1 = € ( w ) √ F ( x ) eiuz dx , F ( t ) = 1 00 1 2π ε ( w ) -iwt dw . To estimate this integral for large t , we displace the path of integration into the lower half- plane of w , where the ...
... frequency , ( 2 ) gives or , conversely , 1 = € ( w ) √ F ( x ) eiuz dx , F ( t ) = 1 00 1 2π ε ( w ) -iwt dw . To estimate this integral for large t , we displace the path of integration into the lower half- plane of w , where the ...
Page 357
... frequency w occurs if the velocity of the particle exceeds the phase velocity of waves of that frequency in the medium concerned . Let be the angle between the direction of motion of the particle and the direction of emission . We have ...
... frequency w occurs if the velocity of the particle exceeds the phase velocity of waves of that frequency in the medium concerned . Let be the angle between the direction of motion of the particle and the direction of emission . We have ...
Page 385
... frequency . We shall denote wi by w simply , and the small difference w2w1 by Aw ( < w ) , and put for brevity dh12 / do2 dw2 I ( w , Aw ) . In the non - exponential factors ew2 in ... frequency $93 Scattering with small change of frequency.
... frequency . We shall denote wi by w simply , and the small difference w2w1 by Aw ( < w ) , and put for brevity dh12 / do2 dw2 I ( w , Aw ) . In the non - exponential factors ew2 in ... frequency $93 Scattering with small change of frequency.
Contents
ELECTROSTATICS OF CONDUCTORS 1 The electrostatic field of conductors | 1 |
2 The energy of the electrostatic field of conductors | 3 |
3 Methods of solving problems in electrostatics | 9 |
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Electrodynamics of Continuous Media: Volume 8 L D Landau,E.M. Lifshitz,L. P. Pitaevskii Snippet view - 1995 |
Common terms and phrases
angle anisotropy atoms averaging axes axis body boundary condition calculated charge circuit co-ordinates coefficient components conducting conductor constant corresponding cross-section crystal Curie point curl H current density denote depends derivative determined dielectric permeability diffraction dipole direction discontinuity distance effect electric field electromagnetic electrons electrostatic ellipsoid entropy equation div expression external field ferroelectric ferromagnetic field H fluid flux force formula free energy frequency function given gives grad H₂ Hence incident induction integral isotropic Laplace's equation layer linear macroscopic magnetic field magnetic moment magnetisation magnitude Maxwell's equations medium metal normal obtain optical particle perpendicular piezoelectric plane polarisation PROBLEM propagation properties pyroelectric quantities refraction relation respect result rotation scalar scattering SOLUTION sphere suffixes superconducting surface symmetry tangential temperature theory thermodynamic potential tion unit volume values variable velocity wave vector wire z-axis zero