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Biasing the center of charge in molecular dynamics simulations with empirical valence bond models: free energetics of an excess proton in a water droplet

机译:用分子动力学模拟偏向电荷中心   经验价键模型:水中过量质子的自由能量学   水滴

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摘要

Multistate empirical valence bond (EVB) models provide an accuratedescription of the energetics of proton transfer and solvation in complexmolecular systems and can be efficiently used in molecular dynamics computersimulations. Within such models, the location of the moving protonic charge canbe specified by the so called center of charge, defined as a weighted averageover the diabatic states of the EVB model. In this paper, we use first orderperturbation theory to calculate the molecular forces that arise if a biaspotential is applied to the center of charge. Such bias potentials are oftennecessary when molecular dynamics simulations are used to determine freeenergies related to proton transfer and not all relevant proton positions aresampled with sufficient frequency during the available computing time. Theforce expressions we derive are easy to evaluate and do not create anysignificant computational cost compared with unbiased EVB-simulations. As anillustration of the method, we study proton transfer in a small liquid waterdroplet consisting of 128 water molecules plus an excess proton. Contrary topredictions of continuum electrostatics but in agreement with previous computersimulations of similar systems, we observe that the excess proton ispredominantly located at the surface of the droplet. Using the formalismdeveloped in this paper, we calculate the reversible work required to carry theprotonic charge from the droplet surface to its core finding a value of roughly4 $k_{\rm B}T$.
机译:多态经验价键(EVB)模型提供了对复杂分子系统中质子转移和溶剂化能的准确描述,可以有效地用于分子动力学计算机模拟。在此类模型中,可以通过所谓的电荷中心(定义为EVB模型的非绝热状态的加权平均值)来指定运动质子电荷的位置。在本文中,我们使用一阶扰动理论来计算将偏置电势施加到电荷中心时产生的分子力。当使用分子动力学模拟来确定与质子转移相关的自由能并且在可用计算时间内并非所有相关质子位置都以足够的频率进行采样时,此类偏置电位通常是必需的。与无偏EVB仿真相比,我们得出的力表达式易于评估,并且不会产生任何可观的计算成本。作为该方法的例证,我们研究了质子在包含128个水分子和过量质子的小水滴中的质子转移。连续静电的相反预测,但与类似系统的先前计算机模拟一致,我们观察到过量的质子主要位于液滴的表面。使用本文开发的形式主义,我们计算了将质子电荷从液滴表面传递到其核心所需的可逆功,得出的值约为4 $ k _ {\ rm B} T $。

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