Condensation of Vapor As Induced By Nuclei And Ions Third Report

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6 5 03 IO 9 W = 3-6 ....
3-6 3-7 ....
3-7 ....
dp/p= d = . 219 . Oigow- 1 / 3 . 219 . Oigow" 1 / 3 . 224 . OI92W" 1 / 3 . 224 . OI92W- 1 / 3 s = . I68rtV 3 . I68V 3 . I67V ....
. I67W 1 / 3 ....
62 CONDENSATION OF VAPOR AS INDUCED BY NUCLEI AND IONS To reduce the other tables to the same standards (remembering that n varies as m, while d and 5 are independent of it), is not necessary for the present comparisons. In table 18, however, 10 w 6 = 2. I should be replaced by io 6 m = 2 . 3, where dp/
...p = o. 133. In table 19, dpjp 0. 2 73, io 6 m = 4. I is to be replaced by io 8 ^ = 4. 3. In all cases the initial nucleations are thus increased. The new values for m are referred to 20 C. And the temperature coefficient is about 2 per cent per degree.
35. Wilson's* data and conclusions. The following table (24) con- tains Wilson's exhaustions (v^/v) at 18 to 19 C. And the correspond- ing disk colors as I interpret them. It also contains the equivalent relative drop of pressure dp/p used above. From these and the colors, the diameters of fog particles (d) may be estimated, provided the series in which these colors lie is known ; hence d, A 2 refers to the probable case of the occurrence of the third and second series, d 2 1 to the very im- probable case of the occurrence of the second and first series.


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