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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 ' ) do ' = Nt do do ' π 2zZe2 2 do ' do ' = Nt 2 pu 013 ( 13.114 ) The single - scattering distribution is valid only for angles large compared to ( 2 ) , and contributes a tail ...
... distribution for the projected angle : ( 13.113 ) Ps ( 0 ' ) do ' = Nt do do ' π 2zZe2 2 do ' do ' = Nt 2 pu 013 ( 13.114 ) The single - scattering distribution is valid only for angles large compared to ( 2 ) , and contributes a tail ...
Page 474
... distribution ( 14.39 ) can be written approximately 8e22 dP ( t ' ) ΦΩ C3 ᅲ 28 . ( 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 these ...
... distribution ( 14.39 ) can be written approximately 8e22 dP ( t ' ) ΦΩ C3 ᅲ 28 . ( 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 these ...
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ