. Carnegie Institution of Washington publication. 10 iz 14 is ib ao ^^ ^4 ^6 aa 30 Fig. 55.—Aperture of coronas (s), observed at different exhaustions (dp), in media of alcohol-air, water-air, energized or non-energized. Table 46. I4C0 1200 ICOO BOO 600 400 ZOO 10 IZ 14 16 18 ZO ZZ Z4 Z6 Z8 30 32 34 36 38 Fig. 56.—Efficient nucleation n in energized or non-energized media of alcohol-air and water-air, at different exhaustions {dp). Table 46. the saturated vapor which furnishes the colloidal nuclei and that the gas is only secondarily involved. 81. Data for alcohol vapor.—The behavior of alcoho
. Carnegie Institution of Washington publication. 10 iz 14 is ib ao ^^ ^4 ^6 aa 30 Fig. 55.—Aperture of coronas (s), observed at different exhaustions (dp), in media of alcohol-air, water-air, energized or non-energized. Table 46. I4C0 1200 ICOO BOO 600 400 ZOO 10 IZ 14 16 18 ZO ZZ Z4 Z6 Z8 30 32 34 36 38 Fig. 56.—Efficient nucleation n in energized or non-energized media of alcohol-air and water-air, at different exhaustions {dp). Table 46. the saturated vapor which furnishes the colloidal nuclei and that the gas is only secondarily involved. 81. Data for alcohol vapor.—The behavior of alcohol vapor is shown in the usual way in table 46, where dp is the sudden fall in pressure from atmospheric pressure producing the corona of the angular diameter 5/30, when the eye and the source of light are at distances 40 and 250 cm. on the opposed sides of the fog chamber. The nucleation n is com- puted in the way given above, section 79, and indicates the number of. 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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