Carnegie Institution of Washington publication . Date. Barom-eter. t v0 Date. Barom-eter. / // to Sept. Oct. 75-68 19. 7585 8. 64 <)5 33 14 633 25. 4-731 14. 65 23 4 622 15. 65 11 »4 600 64 43 14 570 28. 8 14 494 3-- 22. 2! . I 64 36 14 495 4-. 22-4 64 so U 486 5-. 23 fflGefS Fig
Carnegie Institution of Washington publication . Date. Barom-eter. t v0 Date. Barom-eter. / // to Sept. Oct. 75-68 19. 7585 8. 64 <)5 33 14 633 25. 4-731 14. 65 23 4 622 15. 65 11 »4 600 64 43 14 570 28. 8 14 494 3-- 22. 2! . I 64 36 14 495 4-. 22-4 64 so U 486 5-. 23 fflGefS Fig. 22.—Chart showing loss of standard volumesof gas in diver in lapse of days. Diffusionof air through KC1 solution. 7r = 7r(i —) for KC1. Hence these data for KC1 in the table must becorrected before the diffusion coefficients are computed, as follows: Theerror of w being 57r = , its effect on va will be dvo ,_ 8tt This correction is to be supplied in the summary. For brine, by graphicinterpolation, using either Dietericis or Smitss observations, the correctionis 7r = 7r (1—), and this is provisionally used in table 24 and fig. 22. LIQUIDS AND ALLIED EXPERIMENTS. 69 The diffusion of air through strong KC1 shows at the outset a peculiarlyrapid march. This is probably due to the fact that, to remove air bubbles,the water was placed under a relatively high partial vacuum. The rapiddiffusion observed is in correspondence with the restoration of a normalamount of air to the water. Thereafter the march of results is fairlyregular, apart from the
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Keywords: ., bookauthorcarnegie, bookcentury1900, bookdecade1910, bookyear1913
