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Dependence of Surface Tension of a Droplet Formed on the Molecular Condensation Nucleus or Ion on the Droplet Radius. / Lebedeva, T. S.; Suh, D.; Shchekin, A. K.

In: Mechanics of Solids, Vol. 55, No. 1, 01.2020, p. 55-61.

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@article{23d17d8e90284a3da0dae4b23cf6f76f,
title = "Dependence of Surface Tension of a Droplet Formed on the Molecular Condensation Nucleus or Ion on the Droplet Radius",
abstract = "Abstract—The dependence of the thermodynamic surface tension of a small droplet formed on a molecular-size condensation nucleus on the droplet size, nucleus size, molecular field parameters, and nuclear charge in the case of an ion is investigated. Calculations have been performed for molecules of supersaturated argon vapor at different values of the chemical potential of the molecules in the framework of the gradient density functional theory (DFT) and the Carnahan–Starling model to take into account the contribution of hard spheres. The interaction of argon molecules with an uncharged condensation nucleus has been described by the Lennard–Jones potential. In the case of an ion, the long-range Coulomb potential of electric forces is additionally taken into account. The dielectric constant is defined as a function of the local density of the number of argon molecules. As a variable describing the size of the droplet, the radius of the equimolecular surface of the droplet is chosen. The obtained dependences of the surface tension of the droplets have been compared with the dependence of the surface tension on the size of droplet without a condensation nucleus. When the effect of the solvation layer is discarded, the dependence of the surface tension on the radius of the equimolecular surface of a small droplet with a condensation nucleus exhibits similar behavior as in the absence of the nucleus with almost the same negative Tolman correction. The effect of the rigidity constant, however, is clearly influenced by the existence of a condensation nucleus. It is shown that when the first solvation layer is divided around the condensation nucleus, the dependence of surface tension on the radius of the equimolecular surface of a small droplet with a condensation nucleus exhibits similar behavior with almost the same negative Tolman correction as in the absence of a nucleus, but with a different correction, namely, with effective rigidity constant for the surface layer.",
keywords = "condensation nucleus, density functional theory, droplet, heterogeneous nucleation, statistical thermodynamics and mechanics, surface tension, VAPOR, CHARGED NUCLEI, STRONG FIELD, THERMODYNAMIC CHARACTERISTICS, BARRIERLESS NUCLEATION, TERMS",
author = "Lebedeva, {T. S.} and D. Suh and Shchekin, {A. K.}",
note = "Lebedeva, T.S., Suh, D. & Shchekin, A.K. Dependence of Surface Tension of a Droplet Formed on the Molecular Condensation Nucleus or Ion on the Droplet Radius. Mech. Solids 55, 55–61 (2020). https://doi.org/10.3103/S0025654420010161",
year = "2020",
month = jan,
doi = "10.3103/S0025654420010161",
language = "English",
volume = "55",
pages = "55--61",
journal = "Mechanics of Solids",
issn = "0025-6544",
publisher = "Allerton Press, Inc.",
number = "1",

}

RIS

TY - JOUR

T1 - Dependence of Surface Tension of a Droplet Formed on the Molecular Condensation Nucleus or Ion on the Droplet Radius

AU - Lebedeva, T. S.

AU - Suh, D.

AU - Shchekin, A. K.

N1 - Lebedeva, T.S., Suh, D. & Shchekin, A.K. Dependence of Surface Tension of a Droplet Formed on the Molecular Condensation Nucleus or Ion on the Droplet Radius. Mech. Solids 55, 55–61 (2020). https://doi.org/10.3103/S0025654420010161

PY - 2020/1

Y1 - 2020/1

N2 - Abstract—The dependence of the thermodynamic surface tension of a small droplet formed on a molecular-size condensation nucleus on the droplet size, nucleus size, molecular field parameters, and nuclear charge in the case of an ion is investigated. Calculations have been performed for molecules of supersaturated argon vapor at different values of the chemical potential of the molecules in the framework of the gradient density functional theory (DFT) and the Carnahan–Starling model to take into account the contribution of hard spheres. The interaction of argon molecules with an uncharged condensation nucleus has been described by the Lennard–Jones potential. In the case of an ion, the long-range Coulomb potential of electric forces is additionally taken into account. The dielectric constant is defined as a function of the local density of the number of argon molecules. As a variable describing the size of the droplet, the radius of the equimolecular surface of the droplet is chosen. The obtained dependences of the surface tension of the droplets have been compared with the dependence of the surface tension on the size of droplet without a condensation nucleus. When the effect of the solvation layer is discarded, the dependence of the surface tension on the radius of the equimolecular surface of a small droplet with a condensation nucleus exhibits similar behavior as in the absence of the nucleus with almost the same negative Tolman correction. The effect of the rigidity constant, however, is clearly influenced by the existence of a condensation nucleus. It is shown that when the first solvation layer is divided around the condensation nucleus, the dependence of surface tension on the radius of the equimolecular surface of a small droplet with a condensation nucleus exhibits similar behavior with almost the same negative Tolman correction as in the absence of a nucleus, but with a different correction, namely, with effective rigidity constant for the surface layer.

AB - Abstract—The dependence of the thermodynamic surface tension of a small droplet formed on a molecular-size condensation nucleus on the droplet size, nucleus size, molecular field parameters, and nuclear charge in the case of an ion is investigated. Calculations have been performed for molecules of supersaturated argon vapor at different values of the chemical potential of the molecules in the framework of the gradient density functional theory (DFT) and the Carnahan–Starling model to take into account the contribution of hard spheres. The interaction of argon molecules with an uncharged condensation nucleus has been described by the Lennard–Jones potential. In the case of an ion, the long-range Coulomb potential of electric forces is additionally taken into account. The dielectric constant is defined as a function of the local density of the number of argon molecules. As a variable describing the size of the droplet, the radius of the equimolecular surface of the droplet is chosen. The obtained dependences of the surface tension of the droplets have been compared with the dependence of the surface tension on the size of droplet without a condensation nucleus. When the effect of the solvation layer is discarded, the dependence of the surface tension on the radius of the equimolecular surface of a small droplet with a condensation nucleus exhibits similar behavior as in the absence of the nucleus with almost the same negative Tolman correction. The effect of the rigidity constant, however, is clearly influenced by the existence of a condensation nucleus. It is shown that when the first solvation layer is divided around the condensation nucleus, the dependence of surface tension on the radius of the equimolecular surface of a small droplet with a condensation nucleus exhibits similar behavior with almost the same negative Tolman correction as in the absence of a nucleus, but with a different correction, namely, with effective rigidity constant for the surface layer.

KW - condensation nucleus

KW - density functional theory

KW - droplet

KW - heterogeneous nucleation

KW - statistical thermodynamics and mechanics

KW - surface tension

KW - VAPOR

KW - CHARGED NUCLEI

KW - STRONG FIELD

KW - THERMODYNAMIC CHARACTERISTICS

KW - BARRIERLESS NUCLEATION

KW - TERMS

UR - http://www.scopus.com/inward/record.url?scp=85089852219&partnerID=8YFLogxK

UR - https://www.mendeley.com/catalogue/f41eb990-b6ca-3ecf-af75-ee950949ee27/

U2 - 10.3103/S0025654420010161

DO - 10.3103/S0025654420010161

M3 - Article

AN - SCOPUS:85089852219

VL - 55

SP - 55

EP - 61

JO - Mechanics of Solids

JF - Mechanics of Solids

SN - 0025-6544

IS - 1

ER -

ID: 62012157