Classical ElectrodynamicsProblems after each chapter |
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Page 193
... Consequently , if they are to be combined into the divergence of some quantity , that quantity must be a tensor of the second rank . While it is possible to deal with rectangular components of momentum , instead of the vectorial form ...
... Consequently , if they are to be combined into the divergence of some quantity , that quantity must be a tensor of the second rank . While it is possible to deal with rectangular components of momentum , instead of the vectorial form ...
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 8 Re X ίω € ( w ) 1 [ In ( 1.123c ) - 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 8 Re X ίω € ( w ) 1 [ In ( 1.123c ) - In ( 1 ...
Page 508
... consequently that of Aẞ , are not known . Consequently the plane containing the incident beam direction and the direction of the radiation is a natural one with respect to which one specifies the state of polarization of the radiation ...
... consequently that of Aẞ , are not known . Consequently the plane containing the incident beam direction and the direction of the radiation is a natural one with respect to which one specifies the state of polarization of the radiation ...
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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