2007
DOI: 10.1063/1.2731780
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Influence of vapor depletion on nucleation rate

Abstract: During condensation in finite systems part of molecules is transformed from supersaturated mother phase to a new one and depletion of the mother phase occurs. Kinetic equations describing homogeneous nucleation process including decrease of supersaturation are solved numerically. It is shown that dependency of nucleation rate on nucleus size reaches some maximum, which decreases with time and moves to higher nucleus sizes. Nucleation rate is negative for undercritical size of nuclei.

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Cited by 15 publications
(13 citation statements)
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“…Unfortunately, typical transient time of nucleation process for condensation is too short (in order of 10 −7 s) and thus direct comparison with experimental data is not possible due to lack of experimental data. Similarly as in our previous works (Koíšek & Demo, 2005;Koíšek et al, 2006;Koíšek & Demo, 2007) we have chosen as a model system condensation of ethanol vapor at T = 260 K, P 0 = 598.26 Pa, = 0.025 J m −2 , and = 817.5 kg m −3 . Condensation of ethanol vapor was measured to determine the stationary nucleation rate (Kacker & Heist, 1985;Peters & Paikert, 1989;Schmitt, Adams, & Zalabsky, 1982;Strey & Viisanen, 1993) or critical supersaturation (Katz & Ostermier, 1967).…”
Section: Resultsmentioning
confidence: 99%
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“…Unfortunately, typical transient time of nucleation process for condensation is too short (in order of 10 −7 s) and thus direct comparison with experimental data is not possible due to lack of experimental data. Similarly as in our previous works (Koíšek & Demo, 2005;Koíšek et al, 2006;Koíšek & Demo, 2007) we have chosen as a model system condensation of ethanol vapor at T = 260 K, P 0 = 598.26 Pa, = 0.025 J m −2 , and = 817.5 kg m −3 . Condensation of ethanol vapor was measured to determine the stationary nucleation rate (Kacker & Heist, 1985;Peters & Paikert, 1989;Schmitt, Adams, & Zalabsky, 1982;Strey & Viisanen, 1993) or critical supersaturation (Katz & Ostermier, 1967).…”
Section: Resultsmentioning
confidence: 99%
“…In a closed system and at higher initial supersaturations, the nucleation rate does not reach its stationary limit, as in the standard theory. After reaching some extremal value the nucleation rate falls to zero and system tends to equilibrium state (Chesnokov & Krasnoperov, 2002;Koíšek & Demo, 2007).…”
Section: Introductionmentioning
confidence: 97%
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“…In the standard model with a constant supersaturation under the same conditions, one gets for the time delay (corresponding to an appropriate critical size) = 0.42 s at S = 3 and = 0.087 s at S = 5 (time delay decreases with increasing supersaturation). If one takes into account a decrease in the supersaturation for the high initial supersaturation, the nucleation rate does not necessarily reach its stationary value and for sufficiently long times approaches zero (Koíšek & Demo, 2007). If one compares a dimensionless nucleation rate (nucleation rate normalized to its stationary value) for various initial supersaturations (see Figs.…”
Section: Resultsmentioning
confidence: 99%
“…Negative nucleation rates mean a decrease of the number density of nuclei for subcritical sizes. Detailed discussion about negative nucleation rates in closed systems can be found in Koíšek and Demo (2007). At t = 6 s ( Fig.…”
Section: Resultsmentioning
confidence: 99%