Properties of liquid clusters in large-scale molecular dynamics nucleation simulations

被引:35
|
作者
Angelil, Raymond [1 ]
Diemand, Juerg [1 ]
Tanaka, Kyoko K. [2 ]
Tanaka, Hidekazu [2 ]
机构
[1] Univ Zurich, Inst Theoret Phys, CH-8057 Zurich, Switzerland
[2] Hokkaido Univ, Inst Low Temp Sci, Sapporo, Hokkaido 0600819, Japan
来源
JOURNAL OF CHEMICAL PHYSICS | 2014年 / 140卷 / 07期
基金
瑞士国家科学基金会;
关键词
HOMOGENEOUS NUCLEATION; COMPUTER-SIMULATION; INTERFACE; PLANAR;
D O I
10.1063/1.4865256
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
We have performed large-scale Lennard-Jones molecular dynamics simulations of homogeneous vapor-to-liquid nucleation, with 10(9) atoms. This large number allows us to resolve extremely low nucleation rates, and also provides excellent statistics for cluster properties over a wide range of cluster sizes. The nucleation rates, cluster growth rates, and size distributions are presented in Diemand et al. [J. Chem. Phys. 139, 74309 (2013)], while this paper analyses the properties of the clusters. We explore the cluster temperatures, density profiles, potential energies, and shapes. A thorough understanding of the properties of the clusters is crucial to the formulation of nucleation models. Significant latent heat is retained by stable clusters, by as much as Delta kT = 0.1 epsilon for clusters with size i = 100. We find that the clusters deviate remarkably from spherical-with ellipsoidal axis ratios for critical cluster sizes typically within b/c = 0.7 +/- 0.05 and a/c = 0.5 +/- 0.05. We examine cluster spin angular momentum, and find that it plays a negligible role in the cluster dynamics. The interfaces of large, stable clusters are thinner than planar equilibrium interfaces by 10%-30%. At the critical cluster size, the cluster central densities are between 5% and 30% lower than the bulk liquid expectations. These lower densities imply larger-than-expected surface areas, which increase the energy cost to form a surface, which lowers nucleation rates. (C) 2014 AIP Publishing LLC.
引用
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页数:15
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