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石墨烯壁之间的纳米限域抑制了离子液体[BMIM][PF]的近壁扩散。

Nanoconfinement between Graphene Walls Suppresses the Near-Wall Diffusion of the Ionic Liquid [BMIM][PF].

作者信息

Shao Cheng, Ong Wee-Liat, Shiomi Junichiro, McGaughey Alan J H

机构信息

Department of Mechanical Engineering, Carnegie Mellon University, Pittsburgh, Pennsylvania 15213, United States.

University of Michigan-Shanghai Jiao Tong University Joint Institute, Shanghai Jiao Tong University, Shanghai 200240, China.

出版信息

J Phys Chem B. 2021 May 6;125(17):4527-4535. doi: 10.1021/acs.jpcb.1c02562. Epub 2021 Apr 22.

Abstract

We identify two distinct regimes for the diffusion of the ionic liquid [BMIM][PF] confined between parallel graphene walls using molecular dynamics simulations. Within 2 nm of the wall, the cations and anions form a well-defined layered structure. In this region, the in-plane diffusion coefficients are suppressed when compared to their bulk values and increase monotonically with the distance away from the wall. Beyond 2 nm from the wall, the density profile and in-plane diffusion coefficients recover their bulk values. The channel-averaged in-plane diffusion coefficients increase monotonically with wall separation and recover the bulk values at a separation of 15 nm. A simple semianalytical model is proposed that mirrors this trend. The results also highlight the importance of applying a finite-size correction to molecular dynamics-predicted diffusion coefficients of confined liquids, which may otherwise be unusually larger than their bulk values.

摘要

我们通过分子动力学模拟确定了限制在平行石墨烯壁之间的离子液体[BMIM][PF]扩散的两种不同状态。在壁面2纳米范围内,阳离子和阴离子形成了明确的层状结构。在该区域,面内扩散系数与其本体值相比受到抑制,并随着与壁面距离的增加而单调增加。在距壁面超过2纳米处,密度分布和面内扩散系数恢复到其本体值。通道平均面内扩散系数随着壁间距的增加而单调增加,并在15纳米的间距处恢复到本体值。提出了一个简单的半解析模型来反映这种趋势。结果还强调了对受限液体的分子动力学预测扩散系数应用有限尺寸校正的重要性,否则这些扩散系数可能会异常大于其本体值。

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