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水-纳米管相互作用如何影响纳米通道中的水流?

How does water-nanotube interaction influence water flow through the nanochannel?

机构信息

Key Laboratory for Biomedical Effects of Nanomaterials & Nanosafety, National Center for Nanosciences and Technology of China, Beijing100191, China.

出版信息

J Chem Phys. 2012 May 7;136(17):175101. doi: 10.1063/1.4707346.

Abstract

Water permeation across various nitrogen-doped double-walled carbon nanotubes (N-DWCNT) has been studied with molecular dynamics simulations to better understand the influence of water-nanopore interaction on the water permeation rate. There exists a threshold interaction energy at around -34.1 kJ/mol. Over the threshold energy, the water flow through N-DWCNT decreases monotonically with the strengthening of the water-nanotube interaction. The effect on the water flow across the channel is found to be negligible when the interaction energy is weaker than the threshold. The water-nanotube interaction energy can be controlled by doping nitrogen atoms into the nanotube walls. Although the van der Waals interaction energy is much stronger than the electrostatic interaction energy, it is less sensitive to the proportion of doped nitrogen atoms. On the other hand, the electrostatic interaction energy weakens after the initial strengthening when the percentage of doped nitrogen atoms increases to ~25%. The doped nitrogen atoms make less influence on the overall electrostatic interaction energy when the proportion is over 25%, due to the repulsions among themselves. Thus, the monotonous strengthening of the van der Waals interaction energy seems to dominate the overall trend of the total interaction energy, whereas the change of the long-range electrostatic interaction energy characterizes the shape of the correlation curve, as the percentage of doped nitrogen atoms increases.

摘要

采用分子动力学模拟研究了不同氮掺杂双壁碳纳米管(N-DWCNT)的水渗透,以更好地理解水-纳米孔相互作用对水渗透速率的影响。存在一个约为-34.1 kJ/mol 的阈值相互作用能。超过该能量阈值,随着水-纳米管相互作用的增强,水在 N-DWCNT 中的流动呈单调递减。当相互作用能弱于阈值时,发现其对通道中水流动的影响可以忽略不计。氮原子掺杂到纳米管壁可以控制水-纳米管的相互作用能。虽然范德华相互作用能远强于静电相互作用能,但它对掺杂氮原子的比例不太敏感。另一方面,当掺杂氮原子的比例增加到约 25%时,静电相互作用能在初始增强后会减弱。当比例超过 25%时,掺杂氮原子之间的排斥作用会使它们对整体静电相互作用能的影响减小。因此,范德华相互作用能的单调增强似乎主导了总相互作用能的总体趋势,而随着掺杂氮原子比例的增加,长程静电相互作用能的变化则体现了相关曲线的形状。

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