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Page 258
... factor ) ( 8.92 ) * where V is 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 V is 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 ∞ ) . Hence C # / 2 Fsh ~ —4πa3E , ( * Jo ( kað ...
... 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 ∞ ) . Hence C # / 2 Fsh ~ —4πa3E , ( * Jo ( kað ...
Page 561
... factor is typically of the order of g ~ 3 because of their anomalous magnetic moments . Then , with the source size estimate a ~ R = 1.24 % × 10-13 cm , we find 1 7 0.3 1 TM ( 1 ) A TE ( ) ( 16.109 ) The numerical factor ranges from 4 x ...
... factor is typically of the order of g ~ 3 because of their anomalous magnetic moments . Then , with the source size estimate a ~ R = 1.24 % × 10-13 cm , we find 1 7 0.3 1 TM ( 1 ) A TE ( ) ( 16.109 ) The numerical factor ranges from 4 x ...
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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 coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ 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