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Computing the free energy of molecular solids by the Einstein molecule approach: Ices XIII and XIV, hard-dumbbells and a patchy model of proteins

机译:通过爱因斯坦分子方法计算分子固体的自由能:Ices XIII和XIV,硬哑铃和蛋白质的斑块模型

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The recently proposed Einstein molecule approach is extended to compute the free energy of molecular solids. This method is a variant of the Einstein crystal method of Frenkel and Ladd [J. Chem. Phys. 81, 3188 (1984)]. In order to show its applicability, we have computed the free energy of a hard- dumbbell solid, of two recently discovered solid phases of water, namely, ice XIII and ice XIV, where the interactions between water molecules are described by the rigid nonpolarizable TIP4P/2005 model potential, and of several solid phases that are thermodynamically stable for an anisotropic patchy model with octahedral symmetry which mimics proteins. Our calculations show that both the Einstein crystal method and the Einstein molecule approach yield the same results within statistical uncertainty. In addition, we have studied in detail some subtle issues concerning the calculation of the free energy of molecular solids. First, for solids with noncubic symmetry, we have studied the effect of the shape of the simulation box on the free energy. Our results show that the equilibrium shape of the simulation box must be used to compute the free energy in order to avoid the appearance of artificial stress in the system that will result in an increase in the free energy. In complex solids, such as the solid phases of water, another difficulty is related to the choice of the reference structure. As in some cases there is no obvious orientation of the molecules; it is not clear how to generate the reference structure. Our results will show that, as long as the structure is not too far from the equilibrium structure, the calculated free energy is invariant to the reference structure used in the free energy calculations. Finally, the strong size dependence of the free energy of solids is also studied. (C) 2008 American Institute of Physics. [DOI: 10.1063/1.2971188]
机译:最近提出的爱因斯坦分子方法已扩展为计算分子固体的自由能。该方法是弗伦克尔和拉德[E.化学物理81,3188(1984)]。为了显示其适用性,我们计算了硬哑铃固体的自由能,该硬哑铃固体的水是最近发现的两个水固相,即冰XIII和冰XIV,其中水分子之间的相互作用由刚性非极化TIP4P来描述。 / 2005模型势,以及具有模拟蛋白质的八面体对称性的各向异性斑块模型在热力学上稳定的几个固相。我们的计算表明,在统计不确定性范围内,爱因斯坦晶体方法和爱因斯坦分子方法都能产生相同的结果。此外,我们还详细研究了有关分子固体自由能计算的一些细微问题。首先,对于非立方对称的固体,我们研究了模拟盒形状对自由能的影响。我们的结果表明,必须使用模拟盒的平衡形状来计算自由能,以避免在系统中出现会导致自由能增加的人造应力。在复杂的固体(例如水的固相)中,另一个困难与参考结构的选择有关。在某些情况下,分子没有明显的取向;目前尚不清楚如何生成参考结构。我们的结果将表明,只要结构与平衡结构之间的距离不太远,所计算的自由能就不会随自由能计算中使用的参考结构而变化。最后,还研究了固体自由能的强烈尺寸依赖性。 (C)2008美国物理研究所。 [DOI:10.1063 / 1.2971188]

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