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Page 474
... angular distribution ( 14.39 ) can be written approximately dP ( t ' ) dQ 8 622 28 пс3 ( 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 in ...
... angular distribution ( 14.39 ) can be written approximately dP ( t ' ) dQ 8 622 28 пс3 ( 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 in ...
Page 635
... angular momentum of , 201 , 569 Pinch effect , and instabilities , 326 dynamic models of , 322 scaling law for , 325 ... angular distribution of dipole , 272 radiated , angular distribution of half- and full - wave antenna , 279 radiated ...
... angular momentum of , 201 , 569 Pinch effect , and instabilities , 326 dynamic models of , 322 scaling law for , 325 ... angular distribution of dipole , 272 radiated , angular distribution of half- and full - wave antenna , 279 radiated ...
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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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ