Classical Electrodynamics |
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Page 145
... Distribution ; Magnetic Moment We now consider the properties of a general current distribution which is localized in a small region of space , " small " being relative to the scale of length of interest to the observer . The proper ...
... Distribution ; Magnetic Moment We now consider the properties of a general current distribution which is localized in a small region of space , " small " being relative to the scale of length of interest to the observer . The proper ...
Page 458
... distribution for the projected angle : ( 13.113 ) = Ps ( 0 ' ) d0 ' Nt do ' = do = NI Nt do ' Ni ( 22Ze2 ) ° do ( 2zZe22 do ' 2 ρυ 0.3 ( 13.114 ) The single - scattering distribution is valid only for angles large compared to ( 2 ) ...
... distribution for the projected angle : ( 13.113 ) = Ps ( 0 ' ) d0 ' Nt do ' = do = NI Nt do ' Ni ( 22Ze2 ) ° do ( 2zZe22 do ' 2 ρυ 0.3 ( 13.114 ) The single - scattering distribution is valid only for angles large compared to ( 2 ) ...
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 ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss factor force equation frame 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 P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result 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