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Exact expressions for the ionization due to the emission of alpha-particles from radioactive solids are set up and the results of their graphical integration are given. The total ionization per cm² of surface, both with and without absorbers; the variation of ionization with height above the radioactive surface; the ionization from thin films; the ionization from substances containing all members of the U, Th and Ac series, both with and without absorbers; and the counting rate for alpha-particle counting chambers, are given in equations accompanied by appropriate graphs and tables. The older approximate theories break down for actual alpha-particles, particularly those of short range. If q is ion pairs per cm² per sec. formed above the surface of a radioactive solid; N, the number of alpha-particles per sec. per cm³ emitted in the solid; k, ion pairs per alpha-particle of range R in air; and R^', the alpha-particle range in the solid: then q=εNkR^', and the numerical coefficient ε has values between 0.114 and 0.150 for the alpha-particles from all known radioactive substances.
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Robley D. Evans (1934) studied this question.
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