. Carnegie Institution of Washington publication. 20 CONDENSATION OF VAPOR AS INDUCED BY NUCLEI AND IONS. Compared with the graph n and [dp]', table 7, where the upper limit only is varied, the graph n and [dp^ lies in the main above it, in the smaller exhaustions, and it should be remembered that the range of variation is here smaller. But it does not lie as much above n and [dp]' throughout as would be expected, seeing that only the upper points. FIG. 6.—Nucleation of dust-free air for different drops of pressure 8p = p — p2', [dp]' denoting that the upper limits, [], that the lower limit of
. Carnegie Institution of Washington publication. 20 CONDENSATION OF VAPOR AS INDUCED BY NUCLEI AND IONS. Compared with the graph n and [dp]', table 7, where the upper limit only is varied, the graph n and [dp^ lies in the main above it, in the smaller exhaustions, and it should be remembered that the range of variation is here smaller. But it does not lie as much above n and [dp]' throughout as would be expected, seeing that only the upper points. FIG. 6.—Nucleation of dust-free air for different drops of pressure 8p = p — p2', [dp]' denoting that the upper limits, [], that the lower limit of the drop of pressure dp is varied. Also corresponding curve referred to the exhaustion dp/p. Three series. Larger ranges of nucleation than in fig. 5. should coincide, intimating that there is some variation as compared with fig. 6 not accounted for. This becomes specially evident when the two graphs for [dp] in figs. 5 and 6 are compared, as shown in the Please note that these images are extracted from scanned page images that may have been digitally enhanced for readability - coloration and appearance of these illustrations may not perfectly resemble the original Carnegie Institution of Washington. Washington, Carnegie Institution of Washington
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