Ichiye Toshiko, Tan Ming-Liang
Department of Chemistry, Georgetown University, Washington, DC 20057, USA.
J Chem Phys. 2006 Apr 7;124(13):134504. doi: 10.1063/1.2161201.
A new, efficient potential energy function for liquid water is presented here. The new model, which is referred here as the soft sticky dipole-quadrupole-octupole (SSDQO) model, describes a water molecule as a Lennard-Jones sphere with point dipole, quadrupole, and octupole moments. It is a single-point model and resembles the hard-sphere sticky dipole potential model for water by Bratko et al. [J. Chem. Phys. 83, 6367 (1985)] and the soft sticky dipole model by Ichiye and Liu [J. Phys. Chem. 100, 2723 (1996)] except now the sticky potential consists of an approximate moment expansion for the dimer interaction potential, which is much faster than the true moment expansion. The object here is to demonstrate that the SSDQO potential energy function can accurately mimic the potential energy function of a multipoint model using the moments of that model. First, the SSDQO potential energy function using the dipole, quadruple, and octupole moments from SPC/E, TIP3P, or TIP5P is shown to reproduce the dimer potential energy functions of the respective multipoint model. In addition, in Monte Carlo simulations of the pure liquid at room temperature, SSDQO reproduces radial distribution functions of the respective model. However, the Monte Carlo simulations using the SSDQO model are about three times faster than those using the three-point models and the long-range interactions decay faster for SSDQO (1/r(3) and faster) than for multipoint models (1/r). Moreover, the contribution of each moment to the energetics and other properties can be determined. Overall, the simplicity, efficiency, and accuracy of the SSDQO potential energy function make it potentially very useful for studies of aqueous solvation by computer simulations.
本文提出了一种新的、高效的液态水势能函数。这种新模型,在此称为软粘性偶极 - 四极 - 八极(SSDQO)模型,将水分子描述为具有点偶极、四极和八极矩的 Lennard - Jones 球。它是一个单点模型,类似于 Bratko 等人 [《化学物理杂志》83, 6367 (1985)] 提出的水的硬球粘性偶极势模型以及 Ichiye 和 Liu [《物理化学杂志》100, 2723 (1996)] 提出的软粘性偶极模型,只是现在粘性势由二聚体相互作用势的近似矩展开组成,这比真实的矩展开要快得多。这里的目的是证明 SSDQO 势能函数能够使用该模型的矩准确地模拟多点模型的势能函数。首先,使用来自 SPC/E、TIP3P 或 TIP5P 的偶极、四极和八极矩的 SSDQO 势能函数被证明可以重现相应多点模型的二聚体势能函数。此外,在室温下纯液体的蒙特卡罗模拟中(此处有误,原文是在室温下纯液体的分子动力学模拟中),SSDQO 重现了相应模型的径向分布函数。然而,使用 SSDQO 模型的分子动力学模拟比使用三点模型的模拟快约三倍,并且 SSDQO 的长程相互作用衰减更快(1/r³ 及更快),而多点模型的长程相互作用衰减较慢(1/r)。此外,可以确定每个矩对能量学和其他性质的贡献。总体而言,SSDQO 势能函数的简单性、效率和准确性使其在通过计算机模拟研究水合作用方面可能非常有用。 (注:原文中“Monte Carlo simulations of the pure liquid at room temperature”表述有误,结合上下文应该是“分子动力学模拟”,翻译时已按正确理解翻译)