In order to determine the range of validity of Gryzinski's classical theory for inelastic electron-atom scattering, we evaluate exactly the classical cross section for the electron ionization of atomic hydrogen. At large electron-impact energies the exact classical cross section disagrees with the experimental cross section. This is due to the inability of the classical theory to describe an electron-atom collision if the energy of the incident electron is large. For low-impact energies the classical description of a collision becomes valid. The electron energy at which the classical theory becomes applicable is in good agreement with the energy predicted by the uncertainty principle.
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A E Kingston (1964) studied this question.
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