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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 301
... factor involving ( 1 cos 0 ) can be set equal to unity , since at small angles its exponent is a factor 0/2 smaller than the other exponent . The integral over ẞ is 2πJo ( ka sin 0 sin x ) . Hence / 2 -4a3E [ ** J ( kað sin x ) cos x ...
... factor involving ( 1 cos 0 ) can be set equal to unity , since at small angles its exponent is a factor 0/2 smaller than the other exponent . The integral over ẞ is 2πJo ( ka sin 0 sin x ) . Hence / 2 -4a3E [ ** J ( kað sin x ) cos x ...
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... factor / г . At high frequencies T → 2 , so that the absorption cross section approaches the constant Thomson value ... factor ( w2 / w2 ) T represents the incident radiation . For scattering a second factor ( 2/2 ) г appears , while ...
... factor / г . At high frequencies T → 2 , so that the absorption cross section approaches the constant Thomson value ... factor ( w2 / w2 ) T represents the incident radiation . For scattering a second factor ( 2/2 ) г appears , while ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ