Classical Electrodynamics |
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Page 429
... Consequently the path is much less straight . After a short distance , electrons tend to diffuse into the material , rather than go in a rectilinear path . The subject of energy loss and scattering is an important one and is discussed ...
... Consequently the path is much less straight . After a short distance , electrons tend to diffuse into the material , rather than go in a rectilinear path . The subject of energy loss and scattering is an important one and is discussed ...
Page 430
John David Jackson. presented . Consequently our discussion will emphasize the physical ideas involved , rather than ... Consequently the momentum impulse Ap is in the transverse direction 430 Classical Electrodynamics Energy transfer in ...
John David Jackson. presented . Consequently our discussion will emphasize the physical ideas involved , rather than ... Consequently the momentum impulse Ap is in the transverse direction 430 Classical Electrodynamics Energy transfer in ...
Page 447
... Consequently we can approximate the Bessel functions by their small argument limits ( 3.103 ) . Then in the relativistic limit the Fermi expression ( 13.70 ) is dE dx / b > a 2 ( ze ) 2 пс2 Re 00 ίω \ ε ( w ) - < [ in ( 1.123 ) - In ( 1 ...
... Consequently we can approximate the Bessel functions by their small argument limits ( 3.103 ) . Then in the relativistic limit the Fermi expression ( 13.70 ) is dE dx / b > a 2 ( ze ) 2 пс2 Re 00 ίω \ ε ( w ) - < [ in ( 1.123 ) - In ( 1 ...
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