Classical ElectrodynamicsProblems after each chapter |
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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 575
... angular distribution of radiation , and the total power radiated . 16.3 The uniform charge density of Problem 16.2 is replaced by a uniform density of intrinsic magnetization parallel to the z axis and having total magnetic moment M ...
... angular distribution of radiation , and the total power radiated . 16.3 The uniform charge density of Problem 16.2 is replaced by a uniform density of intrinsic magnetization parallel to the z axis and having total magnetic moment M ...
Page 636
John David Jackson. Power , radiated , angular distribution of quadrupole , 275 , 552 radiated , by charged particle ... angular and frequency dis- tribution , for charge in periodic motion , 501 angular and frequency distribution , for ...
John David Jackson. Power , radiated , angular distribution of quadrupole , 275 , 552 radiated , by charged particle ... angular and frequency dis- tribution , for charge in periodic motion , 501 angular and frequency distribution , for ...
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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