Research output: Contribution to journal › Article
Nucleation stage in supersaturated vapor with inhomogeneities due to nonstationary diffusion onto growing droplets. / Kuchma, A.; Markov, M.; Shchekin, A.
In: Physica A: Statistical Mechanics and its Applications, Vol. 402, 2014, p. 255-265.Research output: Contribution to journal › Article
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TY - JOUR
T1 - Nucleation stage in supersaturated vapor with inhomogeneities due to nonstationary diffusion onto growing droplets
AU - Kuchma, A.
AU - Markov, M.
AU - Shchekin, A.
PY - 2014
Y1 - 2014
N2 - An analytical description of the nucleation stage in a supersaturated vapor with instantly created supersaturation is given with taking into account the vapor concentration inhomogeneities arising as a result of depletion due to nonstationary diffusion onto growing droplets. This description is based on the fact, that the intensity of the nucleation of new droplets is suppressed in spherical diffusion regions of a certain size surrounding previously nucleated droplets, and remains at the initial level in the remaining volume of the vapor–gas medium. The value of the excluded volume (excluded from nucleation) depends on the explicit form of the vapor concentration profile in the space around the growing droplet, and we use for that the unsteady self-similar solution of the time-dependent diffusion equation with a convective term describing the flow of the gas–vapor mixture caused by the moving surface of the single growing droplet. The main characteristics of the phase transition at the end of the nucleation s
AB - An analytical description of the nucleation stage in a supersaturated vapor with instantly created supersaturation is given with taking into account the vapor concentration inhomogeneities arising as a result of depletion due to nonstationary diffusion onto growing droplets. This description is based on the fact, that the intensity of the nucleation of new droplets is suppressed in spherical diffusion regions of a certain size surrounding previously nucleated droplets, and remains at the initial level in the remaining volume of the vapor–gas medium. The value of the excluded volume (excluded from nucleation) depends on the explicit form of the vapor concentration profile in the space around the growing droplet, and we use for that the unsteady self-similar solution of the time-dependent diffusion equation with a convective term describing the flow of the gas–vapor mixture caused by the moving surface of the single growing droplet. The main characteristics of the phase transition at the end of the nucleation s
KW - Phase transitions Kinetics Nucleation Droplets Nonstationary diffusion
U2 - 10.1016/j.physa.2014.02.005
DO - 10.1016/j.physa.2014.02.005
M3 - Article
VL - 402
SP - 255
EP - 265
JO - Physica A: Statistical Mechanics and its Applications
JF - Physica A: Statistical Mechanics and its Applications
SN - 0378-4371
ER -
ID: 6994806