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Page 474
... angular distribution ( 14.39 ) can be written approximately dP ( t ' ) 8 e2 2 28 ΦΩ c3 π ( 20 ) 2 ( 1 + y202 ) 5 ( 14.41 ) The natural angular unit is evidently y1 . The angular distribution is shown in Fig . 14.5 with angles measured ...
... angular distribution ( 14.39 ) can be written approximately dP ( t ' ) 8 e2 2 28 ΦΩ c3 π ( 20 ) 2 ( 1 + y202 ) 5 ( 14.41 ) The natural angular unit is evidently y1 . The angular distribution is shown in Fig . 14.5 with angles measured ...
Page 549
... angular momentum per photon of energy ho . In further analogy with quantum mechanics we would expect the ratio of the magnitude of the angular momentum to the energy to have the value , 2 M ( a ) ( M2 + M , 2 + M , 2 ) √1 ( 1 + 1 ) ...
... angular momentum per photon of energy ho . In further analogy with quantum mechanics we would expect the ratio of the magnitude of the angular momentum to the energy to have the value , 2 M ( a ) ( M2 + M , 2 + M , 2 ) √1 ( 1 + 1 ) ...
Page 636
... 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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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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