The Theory of Ionization of Gases By Collision Microform
The Theory of Ionization of Gases By Collision Microform
John Townsend
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TABLE XII. I 2 4 6 8 1-0 1-1 q 2-86 8-3 24-2 81 373 2250 e z 1 2*86 8-2 23-4 66-5 190 322 (a-/3)>- 8 ) Z 1 0. 07 C. Q 04. 0 80 380 2150 A (-) a pe v 1 See papers in Electrician, April 3, 1903, and Philosophical Magazine, November, 1903, on "The Genesis of Ions by the Motion of Positive Ions in a Gas. " loNIZATION BY POSITIVE loNS 43 The currents are given in arbitrary units, and the values of a and /3 may be found from the ratios of the currents at three distances. The agreement between the exp...ression for n involving a and /3 and the currents over several distances shows that the experiments are accurately explained by the theory. The above example of currents developed in air, in which p=l, X=350, a=5*25, and /3 = '0141, may be compared with the results of an experiment in which p=%, X=700, since according to the theory a and /3 should in this case have twice the above values, and the current corresponding to any distance should be the same as that at double the distance in the previous experiment.
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