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... angular distribution ( 14.39 ) can be written approximately 8e22 dP ( t ' ) ΔΩ 28 ( 20 ) 2 π C3 ( 1+ y202 ) 5 ( 14.41 ) The natural angular unit is evidently y1 . The angular distribution is shown in Fig . 14.5 with angles measured in ...
... angular distribution ( 14.39 ) can be written approximately 8e22 dP ( t ' ) ΔΩ 28 ( 20 ) 2 π C3 ( 1+ y202 ) 5 ( 14.41 ) The natural angular unit is evidently y1 . The angular distribution is shown in Fig . 14.5 with angles measured in ...
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... angular dependence , but have polarizations at right angles to one another . Thus the multipole order can be determined by measurement of the angular distribution of radiated power , but the character of the radiation ( electric or ...
... angular dependence , but have polarizations at right angles to one another . Thus the multipole order can be determined by measurement of the angular distribution of radiated power , but the character of the radiation ( electric or ...
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... angular and frequency dis- tribution , for charge in periodic motion , 501 angular and frequency distribution , for magnetic moments , 481 angular and frequency distribution , for ultrarelativistic particle , 481 f . angular and ...
... angular and frequency dis- tribution , for charge in periodic motion , 501 angular and frequency distribution , for magnetic moments , 481 angular and frequency distribution , for ultrarelativistic particle , 481 f . angular and ...
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Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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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