. Carnegie Institution of Washington publication. 44 CONDENSATION OF VAPOR AS INDUCED BY NUCLEI AND IONS. tion therefore varies in geometric progression with the number of ex- haustions, apart from necessary corrections. The observations were made in time series by two observers, Miss L. B. Joslin assisting me with. FIG. ii.—Fog chamber F, and vacuum chamber V. the work. Details will be given in connection with the data. The initial isothermal (T) pressures p and pf of the fog and vacuum chambers and the final isothermal (T) pressure p3, when in communication after exhaustion, were carefully d
. Carnegie Institution of Washington publication. 44 CONDENSATION OF VAPOR AS INDUCED BY NUCLEI AND IONS. tion therefore varies in geometric progression with the number of ex- haustions, apart from necessary corrections. The observations were made in time series by two observers, Miss L. B. Joslin assisting me with. FIG. ii.—Fog chamber F, and vacuum chamber V. the work. Details will be given in connection with the data. The initial isothermal (T) pressures p and pf of the fog and vacuum chambers and the final isothermal (T) pressure p3, when in communication after exhaustion, were carefully determined previous to the experiment with coronas. These were needed for the computation of the amount of water precipitated per cubic centimeter in each of the series of exhaus- tions. In addition to this the pressure [^>2] for finding the ratio of the geometric sequence was necessary and found as follows: In each exhaustion the stopcock was opened suddenly at the beginning of each. 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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