. Carnegie Institution of Washington publication. . 66. 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 work.. Carnegie Institution of Washington. Washington, Carnegie Institution of Washington

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RFRG65

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RM2AKNDHK–Carnegie Institution of Washington publication . Diver shortened. Long diver. Long interval. time-interval to reach rigorously normal conditions of equilibrium, theresult is patent that the true diffusion rates do not appear until the time-interval has been prolonged sometimes as much as five or six weeks. Even Table 22.—Air-air through water. Vessel H (double tube). Constants as in table23. Date. Oct. 26 28 2C)30 Nov. 1 2 456 78 9111213 Barom- t eter. 75-66 O 22.7 j • 76.20 21.8 76.58 20.6 75.80 21.9 75-91 20.0 75.62 20.7 ; 77-33 18.3 76.89 20.8 7682 22.4 76.02 24.2 7507 24.0 ; 75-55 19.3 76.

RM2AKNCCJ–Carnegie Institution of Washington publication . Fig. 27.—Chart showing loss of standardvolumes of gas in diver in lapse ofdays. Diffusion of air through CaCl2solution. Table 31.—Air-air through CaClj solution (13.9 grams in 100 grams water). VesselC (single tube). Constants as in table 30. pw = 1. 105 at 230. Date. Barom-eter. I H Vo Date. Barom-eter. t H Vo Oct. 26 • 75-66 022.5 65.64 5-797 i Nov. 7 76. 02 024.0 64.91 5-707 28 76.20 21.3 65.27 5 786 8 • 75-07 23.9 65.00 5-77 29 . 76.58 20.2 64.92 5 774 9 • 75-55 19.0 63.95 5.709 30 . 75.80 21.7 65.09 5 763 11 • 76.33 IQ.O 63.62 5.6S0 Nov. 1

RM2AKNDB2–Carnegie Institution of Washington publication . 24.50. Date. Barom-eter. t v0 Date. Barom-eter. / // to Sept. 18.. 76.06 019.8 67.32 15.223 Oct. 7.. 75-68 019.2 64.78 14.675 19. 7585 21.2 66.54 14.981 8. 76.34 19.6 64 <)5 33 14 633 25. 76.72 17.8 64.74 4-731 14. 76.88 22.6 65 23 4 622 26.. 76.54 17.8 64.70 14.722 15. 76.08 22.5 65 11 »4 600 27.. 76.31 17.8 64.62 14.703 16.. 76.92 19.8 64 43 14 570 28. 77.04 19.2 64.95 8 14 494 3-- 76.33 20.2 65.02 14.684 22. 77.08 2! . I 64 36 14 495 4-. 76.10 22.7 65.50 14.691 23.. 76.05 22-4 64 so U 486 5-. 76.69 20.8 65.20 14.699. hept.1% 23 fflGefS Fig

$. Carnegie Institution of Washington publication. 63 -55 structed graphically (n—i+K for solution as abscissa and for submergedglass as ordinate), the results (figs. 65 and 66) show a very definite trendand show also that slight interpolation would be possible. It would behasty, however, to infer that the intersection at a of the graph for submergedglass with the line at 45° through the origin is the index of refraction of theglass, in so far as the data for the liquid are trustworthy. The methodseems to be deserving of notice; but before discussing the matter furtherit will be necessary to de Stock Photo$

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