Gibbs free energies of Fe clusters can be approximated by Tolman correction to accurately model cluster nucleation and growth

Alexander Khrabry, Louis E. S. Hoffenberg, Igor D. Kaganovich, Yuri Barsukov, David B. Graves
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Abstract

Accurate Gibbs free energies of Fe clusters are required for predictive modeling of Fe cluster growth during condensation of a cooling vapor. We present a straightforward method of calculating free energies of cluster formation using the data provided by molecular dynamics (MD) simulations. We apply this method to calculate free energies of Fe clusters having from 2 to 100 atoms. The free energies are verified by comparing to an MD-simulated equilibrium cluster size distribution in a sub-saturated vapor. We show that these free energies differ significantly from those obtained with a commonly used spherical cluster approximation - which relies on a surface tension coefficient of a flat surface. The spherical cluster approximation can be improved by using a cluster size-dependent Tolman correction for the surface tension. The values for the Tolman length and effective surface tension were derived, which differ from the commonly used experimentally measured surface tension based on the potential energy. This improved approximation does not account for geometric magic number effects responsible for spikes and troughs in densities of neighbor cluster sizes. Nonetheless, it allows to model cluster formation from a cooling vapor and accurately reproduce the condensation timeline, overall shape of the cluster size distribution, average cluster size, and the distribution width. Using a constant surface tension coefficient resulted in distorted condensation dynamics and inaccurate cluster size distributions. The analytical expression for cluster nucleation rate from classical nucleation theory (CNT) was updated to account for the size-dependence of cluster surface tension.
铁簇的吉布斯自由能可用托尔曼修正法近似,以准确模拟铁簇的成核和生长过程
要对冷却蒸汽凝结过程中铁簇的生长进行预测建模,就必须获得铁簇的精确吉布斯自由能。我们提出了一种利用分子动力学(MD)模拟提供的数据计算团簇形成自由能的直接方法。我们用这种方法计算了 2 到 100 个原子的铁簇的自由能。通过与亚饱和蒸汽中的 MD 模拟平衡团簇大小分布进行比较,验证了自由能。我们发现,这些自由能与通常使用的球形团簇近似方法(该方法依赖于平面的表面张力系数)得到的自由能有很大不同。球团近似可以通过使用与团块大小相关的托尔曼表面张力校正来改进。我们得出的托尔曼长度和有效表面张力值与常用的基于势能的实验测量表面张力值不同。这种改进的近似方法并没有考虑到几何魔数效应,这种效应会导致相邻团簇大小的密度出现尖峰和低谷。尽管如此,它仍能模拟冷却水蒸气的团簇形成,并准确再现凝结时限、团簇大小分布的整体形状、平均团簇大小和分布宽度。使用恒定的表面张力系数会导致冷凝动力学失真和不准确的团簇大小分布。更新了经典成核理论(CNT)中的团簇成核率分析表达式,以考虑团簇表面张力的大小依赖性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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