Classical ElectrodynamicsProblems after each chapter |
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Page 458
... distribution for the projected angle : Ps ( 0 ' ) do ' = Nt do ' = Nt do do ' 2 2zZe2 2 do ' pv 0/3 ( 13.113 ) ( 13.114 ) The single - scattering distribution is valid only for angles large compared to ( 2 ) , and contributes a tail to ...
... distribution for the projected angle : Ps ( 0 ' ) do ' = Nt do ' = Nt do do ' 2 2zZe2 2 do ' pv 0/3 ( 13.113 ) ( 13.114 ) The single - scattering distribution is valid only for angles large compared to ( 2 ) , and contributes a tail to ...
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 ...
Contents
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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