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Page 258
... factor ) ( 8.92 ) * where Vis the volume of the cavity , and S its total surface area . The Q of a cavity is evidently , apart from a geometrical factor , the ratio of the volume occupied by the fields to the volume of the conductor ...
... factor ) ( 8.92 ) * where Vis the volume of the cavity , and S its total surface area . The Q of a cavity is evidently , apart from a geometrical factor , the ratio of the volume occupied by the fields to the volume of the conductor ...
Page 559
... factor is of the order of unity for electrons . With a ~ ao / Zeff 137 ( h / mcZeff ) , we see that the magnetic Ith multipole rate is a factor ( Zeff / 137 ) 2 smaller than the corresponding electric multipole rate . We conclude that ...
... factor is of the order of unity for electrons . With a ~ ao / Zeff 137 ( h / mcZeff ) , we see that the magnetic Ith multipole rate is a factor ( Zeff / 137 ) 2 smaller than the corresponding electric multipole rate . We conclude that ...
Page 606
... factor / г . At high frequencies I , → w2 , so that the absorption cross section approaches the constant Thomson ... factor ( w2 / w62 ) represents the incident radiation . For scattering a second factor ( w2 / w62 ) appears , while for ...
... factor / г . At high frequencies I , → w2 , so that the absorption cross section approaches the constant Thomson ... factor ( w2 / w62 ) represents the incident radiation . For scattering a second factor ( w2 / w62 ) appears , while for ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain oscillations P₁ parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ