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- 3 - X 14.3 X 106 X .05 - 7.15 X 105 atoms of radon will be present in the ionization chamber, and of this number, the fraction, 2.1 X 10-6 disintegrates per second. -6 Carrying out the multiplication of 7.15 X 105 x 2.1 X 10-6 we obtain 1.5 for the number of atoms of radon disintegrating per second. As we have shown, a net drift of 1 division per second.of the leaf requires a transformation of approximately 250 atoms of radon per second, including its short-lived products. Hence the expected net drift will be very small indeed, namely, 1.5 = 0.006 divisions per second, 250 a value of the same order of magnitude as the natural drift of the instrument used in our experiments. An increase in drift of this magnitude when identified as produced by radon can safely be made the basis for approximate quantitative determinations. In this connec- tion it should be emphasized that observed increase in drift will be only one-sixth the the above value, or 0.001 divisions per second when standard sized ionization chamber of one- half liter volume is used for testing expired air for the presence of radon. DETECTION OF RADON---SCINTILLATION METHOD. The lens used in commercial spinthariscopes has a magnification of 7 times, and covers a field of 20 mm diameter at best. Hence the area of the luminous zinc sulfide soreen on which the scintillations can be observed is limited to 3.1 square centimeters. By means of the special mounting and lens which we have employed in our experimental arrangement, a screen area of 6 sq. eme may come under observation. This screen area will still be slightly less than 2 per cent of the surface area of a cylindrical chamber 8 centimeters in diameter and 10 centimeters high, whose volume is approximately 500 cubic centimeters. Now the total number of alpha particles expelled per second from the emanation contained in 500 00 of expired air exhaled by a subject bearing 20 micrograms of r adium will be only 0.25, or in one minute not more than 15 alpha particles will strike the walls of the counting chamber. At best but 2 per cent of the alpha particles will fall on the screen, which is equivalent to saying that one would expect to observe a single scintillation at intervals of about three minutes. Since the natural number of scintillations observed by us on samples of phosphorescent

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    "ocrText": "- 3 -\nX\n14.3 X 106 X .05 - 7.15 X 105 atoms of radon will be present in the ionization\nchamber, and of this number, the fraction, 2.1 X 10-6 disintegrates per second.\n-6\nCarrying out the multiplication of 7.15 X 105 x 2.1 X 10-6 we obtain 1.5 for the\nnumber of atoms of radon disintegrating per second. As we have shown, a net drift of\n1 division per second.of the leaf requires a transformation of approximately 250 atoms of\nradon per second, including its short-lived products. Hence the expected net drift will\nbe very small indeed, namely,\n1.5 = 0.006 divisions per second,\n250\na\nvalue\nof the same order of magnitude as the natural drift of the instrument used in our\nexperiments. An increase in drift of this magnitude when identified as produced by radon\ncan safely be made the basis for approximate quantitative determinations. In this connec-\ntion it should be emphasized that observed increase in drift will be only one-sixth the\nthe\nabove value, or 0.001 divisions per second when standard sized ionization chamber of one-\nhalf liter volume is used for testing expired air for the presence of radon.\nDETECTION OF RADON---SCINTILLATION METHOD. The lens used in commercial spinthariscopes\nhas a magnification of 7 times, and covers a field of 20 mm diameter at best. Hence the\narea of the luminous zinc sulfide soreen on which the scintillations can be observed is\nlimited to 3.1 square centimeters. By means of the special mounting and lens which we\nhave employed in our experimental arrangement, a screen area of 6 sq. eme may come under\nobservation. This screen area will still be slightly less than 2 per cent of the surface\narea of a cylindrical chamber 8 centimeters in diameter and 10 centimeters high, whose\nvolume is approximately 500 cubic centimeters. Now the total number of alpha particles\nexpelled per second from the emanation contained in 500 00 of expired air exhaled\nby\na\nsubject bearing 20 micrograms of r adium will be only 0.25, or in one minute not more than\n15 alpha particles will strike the walls of the counting chamber. At best but 2 per cent\nof the alpha particles will fall on the screen, which is equivalent to saying that one\nwould expect to observe a single scintillation at intervals of about three minutes.\nSince the natural number of scintillations observed by us on samples of phosphorescent"
}