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Page 439
... classical result . The important quantum effects are ( 1 ) discreteness of the possible energy transfers , and ( 2 ) limitations due to the wave nature of the particles and the uncertainty principle . The problem of the discrete nature ...
... classical result . The important quantum effects are ( 1 ) discreteness of the possible energy transfers , and ( 2 ) limitations due to the wave nature of the particles and the uncertainty principle . The problem of the discrete nature ...
Page 510
... classical limits on the impact parameters can be found by arguments analogous to those of Section 13.1 . The classical minimum impact param- eter is [ see ( 13.5 ) – ( 13.7 ) ] : ( c ) = zZe2 Mv2 ( 15.13 ) while the maximum value is ...
... classical limits on the impact parameters can be found by arguments analogous to those of Section 13.1 . The classical minimum impact param- eter is [ see ( 13.5 ) – ( 13.7 ) ] : ( c ) = zZe2 Mv2 ( 15.13 ) while the maximum value is ...
Page 593
... classical theory . The origins and fundamental nature of the Poincaré stresses are , of course , unknown . The stresses were merely postulated to meet the obvious experimental facts that charged particles do exist as stable entities ...
... classical theory . The origins and fundamental nature of the Poincaré stresses are , of course , unknown . The stresses were merely postulated to meet the obvious experimental facts that charged particles do exist as stable entities ...
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Common terms and phrases
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