Department of Chemistry and Biochemistry, University of Arkansas, Fayetteville, Arkansas 72701, USA.
J Chem Phys. 2017 Feb 7;146(5):054702. doi: 10.1063/1.4974921.
A pairwise additive atomistic potential was developed for modeling liquid water on graphene. The graphene-water interaction terms were fit to map the PAW-PBE-D3 potential energy surface using the adaptive force matching method. Through condensed phase force matching, the potential developed implicitly considers the many-body effects of water. With this potential, the graphene-water contact angle was determined to be 86° in good agreement with a recent experimental measurement of 85° ± 5° on fully suspended graphene. Furthermore, the PAW-PBE-D3 based model was used to study contact line hysteresis. It was found that the advancing and receding contact angles of water do agree on pristine graphene, however a long simulation time was required to reach the equilibrium contact angle. For water on suspended graphene, sharp peaks in the water density profile disappear when the flexibility of graphene was explicitly considered. The water droplet induces graphene to wrap around it leading to a slightly concave contact interface.
我们为模拟石墨烯上水的结构开发了一种对原子相互作用的双体加和型经验势函数。我们使用自适应力匹配方法拟合了石墨烯-水相互作用项,以映射 PAW-PBE-D3 势能面。通过凝聚相力匹配,所开发的势能隐含地考虑了水的多体效应。利用该势能,我们确定石墨烯-水的接触角为 86°,这与最近在完全悬浮的石墨烯上测量的 85°±5°的实验结果非常吻合。此外,我们还使用基于 PAW-PBE-D3 的模型研究了接触线滞后现象。结果表明,在原始石墨烯上,前进和后退接触角是一致的,但是需要很长的模拟时间才能达到平衡接触角。对于悬浮石墨烯上的水,当明确考虑石墨烯的柔韧性时,水的密度分布中的尖锐峰消失了。水滴会导致石墨烯围绕它包裹,从而导致接触界面略微凹陷。