Electrodynamics of Continuous Media |
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Page 305
... diffraction occurs , namely that it is perfectly con- ducting , and therefore perfectly reflecting . The following remark may be made here . It might seem reasonable to solve the diffraction problem on the assumption that the surface of ...
... diffraction occurs , namely that it is perfectly con- ducting , and therefore perfectly reflecting . The following remark may be made here . It might seem reasonable to solve the diffraction problem on the assumption that the surface of ...
Page 309
... diffraction are moderately large ( this region overlaps the region of small angles in which the ordinary Fresnel - diffraction formulae are valid ) . The result is in the form of an integral along the edge of the screen , analogously to ...
... diffraction are moderately large ( this region overlaps the region of small angles in which the ordinary Fresnel - diffraction formulae are valid ) . The result is in the form of an integral along the edge of the screen , analogously to ...
Page 310
... diffraction problem for the aperture in the screen is given by E = ( Eo + E ' ) , H = ( Ho + H ' ) for ≈ < 0 ... diffraction by an aperture in a screen with e = ∞ is equivalent to a problem of diffraction by a complementary screen with ...
... diffraction problem for the aperture in the screen is given by E = ( Eo + E ' ) , H = ( Ho + H ' ) for ≈ < 0 ... diffraction by an aperture in a screen with e = ∞ is equivalent to a problem of diffraction by a complementary screen with ...
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