Errington Jeffrey R, Kofke David A
Department of Chemical and Biological Engineering, University at Buffalo, The State University of New York, Buffalo, New York 14260, USA.
J Chem Phys. 2007 Nov 7;127(17):174709. doi: 10.1063/1.2795698.
We examine the performance of several molecular simulation techniques aimed at evaluation of the surface tension through its thermodynamic definition. For all methods explored, the surface tension is calculated by approximating the change in Helmholtz free energy associated with a change in interfacial area through simulation of a liquid slab at constant particle number, volume, and temperature. The methods explored fall within three general classes: free-energy perturbation, the Bennett acceptance-ratio scheme, and the expanded ensemble technique. Calculations are performed for both the truncated Lennard-Jones and square-well fluids at select temperatures spaced along their respective liquid-vapor saturation lines. Overall, we find that Bennett and expanded ensemble approaches provide the best combination of accuracy and precision. All of the methods, when applied using sufficiently small area perturbation, generate equivalent results for the Lennard-Jones fluid. However, single-stage free-energy-perturbation methods and the closely related test-area technique recently introduced by Gloor et al. [J. Chem. Phys. 123, 134703 (2005)] generate surface tension values for the square-well fluid that are not consistent with those obtained from the more robust expanded ensemble and Bennett approaches, regardless of the size of the area perturbation. Single-stage perturbation methods fail also for the Lennard-Jones system when applied using large area perturbations. Here an analysis of phase-space overlap produces a quantitative explanation of the observed inaccuracy and shows that the satisfactory results obtained in these cases from the test-area method arise from a cancellation of errors that cannot be expected in general. We also briefly analyze the variation in method performance with respect to the adjustable parameters inherent to the techniques.
我们研究了几种旨在通过表面张力的热力学定义来评估其性能的分子模拟技术。对于所有探索的方法,表面张力是通过在恒定粒子数、体积和温度下模拟液体平板,近似与界面面积变化相关的亥姆霍兹自由能变化来计算的。探索的方法分为三大类:自由能微扰法、贝内特接受率方案和扩展系综技术。在沿着各自的液-气饱和线分布的选定温度下,对截断的 Lennard-Jones 流体和方阱流体进行了计算。总体而言,我们发现贝内特方法和扩展系综方法提供了精度和准确性的最佳组合。当使用足够小的面积微扰应用所有方法时,对于 Lennard-Jones 流体产生等效结果。然而,单阶段自由能微扰法以及 Gloor 等人最近引入的密切相关的测试面积技术 [《化学物理杂志》123, 134703 (2005)] 对方阱流体产生的表面张力值与从更稳健的扩展系综和贝内特方法获得的值不一致,无论面积微扰的大小如何。当使用大面积微扰应用时,单阶段微扰法对于 Lennard-Jones 系统也会失败。这里对相空间重叠的分析对观察到的不准确性给出了定量解释,并表明在这些情况下从测试面积法获得的令人满意的结果源于误差的抵消,而这种抵消一般是无法预期的。我们还简要分析了方法性能相对于技术固有可调参数的变化。