Classical ElectrodynamicsProblems after each chapter |
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Page 458
... distribution for the projected angle : Ps ( 0 ' ) do ' = Nt do ' = Ni do do ' π 2zZe22 do ' Nt 2 pu 0'3 ( 13.113 ) ( 13.114 ) The single - scattering distribution is valid only for angles large compared to ( 2 ) , and contributes a tail ...
... distribution for the projected angle : Ps ( 0 ' ) do ' = Nt do ' = Ni do do ' π 2zZe22 do ' Nt 2 pu 0'3 ( 13.113 ) ( 13.114 ) The single - scattering distribution is valid only for angles large compared to ( 2 ) , and contributes a tail ...
Page 575
... 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. With the ...
... 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. With the ...
Page 636
... distribution , for magnetic moments , 481 angular and frequency distribution , for ultrarelativistic particle , 481 f . angular and frequency distribution , general result for accelerated charge , 480 angular distribution of , for ...
... distribution , for magnetic moments , 481 angular and frequency distribution , for ultrarelativistic particle , 481 f . angular and frequency distribution , general result for accelerated charge , 480 angular distribution of , 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