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探索疏水界面处水合过量质子的行为。

Exploring the behaviour of the hydrated excess proton at hydrophobic interfaces.

作者信息

Kumar Revati, Knight Chris, Voth Gregory A

出版信息

Faraday Discuss. 2013;167:263-78. doi: 10.1039/c3fd00087g.

Abstract

The affinity of the excess proton for the aqueous solution-hydrophobic interface was examined for two specific examples, the air-water and hydrophobic wall-water cases, using a multiconfigurational molecular dynamics algorithm. The use of a reactive simulation method is important as it allows for a realistic description of the excess proton, namely, its propensity to hop between water molecules via the Grotthuss mechanism. The free energy profile reveals a minimum at these interfaces due to a favourable enthalpic term that outweighs the entropic penalty. The key factors that contribute to this enthalpic minimum were examined using a generalization of a scheme that decomposes the interaction energy into separate terms arising from various local environments [Otten et al., Proc. Natl. Acad. Sci. USA, 109, 701 (2012)] (coordination shell, bulk, and interface) and the delocalization energy (which allows the proton to hop). For both systems, it was observed that the energetic penalty for loss of coordinating water molecules as the excess proton moves toward the hydrophobic interface is more than compensated by the displacement of unfavourable interfacial water molecules. In addition, the ion becomes more delocalized, more Zundel-like, and therefore possesses a larger effective radius as it moves to the interface. The fluctuations of the instantaneous interface were reduced near the vicinity of the ion, thereby giving rise to an entropic penalty. This paper will discuss the application of energy decomposition schemes to multiconfigurational simulations and the resulting consequences realized for the excess proton at hydrophobic interfaces.

摘要

使用多构型分子动力学算法,针对两个具体实例,即气 - 水界面和疏水壁 - 水界面,研究了过量质子与水溶液 - 疏水界面之间的亲和力。采用反应性模拟方法很重要,因为它能够对过量质子进行真实描述,即其通过Grotthuss机制在水分子间跳跃的倾向。自由能分布显示,由于有利的焓项超过熵罚,在这些界面处存在一个最小值。使用一种将相互作用能分解为源自各种局部环境([Otten等人,《美国国家科学院院刊》,109, 701 (2012)](配位层、本体和界面))以及离域能(使质子能够跳跃)的单独项的方案的推广,研究了促成该焓最小值的关键因素。对于这两个系统,均观察到当过量质子向疏水界面移动时,失去配位水分子的能量代价被不利的界面水分子的位移所充分补偿。此外,离子在向界面移动时变得更加离域,更像Zundel离子,因此具有更大的有效半径。离子附近瞬时界面的波动减小,从而产生熵罚。本文将讨论能量分解方案在多构型模拟中的应用以及在疏水界面处过量质子所产生的结果。

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