Center of Smart Interfaces, Technische Universität Darmstadt, Petersenstrasse 17, D-64287, Darmstadt, Germany.
Langmuir. 2013 Feb 5;29(5):1457-65. doi: 10.1021/la304645w. Epub 2013 Jan 24.
Although experimental and theoretical studies have addressed the question of the wetting properties of graphene, the actual value of the contact angle of water on an isolated graphene monolayer remains unknown. While recent experimental literature indicates that the contact angle of water on graphite is in the range 90-95°, it has been suggested that the contact angle on graphene may either be as high as 127° or moderately enhanced in comparison with graphite. With the support of classical molecular dynamics simulations using empirical force-fields, we develop an argumentation to show that the value of 127° is an unrealistic estimate and that a value of the order of 95-100° should be expected. Our study establishes a connection between the variation of the work of adhesion of water on graphene-based surfaces and the interaction potential between individual water molecules and these surfaces. We show that a variation of the contact angle from 90° on graphite to 127° on graphene would imply that both of the first two carbon layers of graphite contribute approximately the same interaction energy with water. Such a situation is incompatible with the short-range nature of the interaction between water and this substrate. We also show that the interaction potential energy between water and the graphene-based substrates is the main contribution to the work of adhesion of water with a relative magnitude that is independent of the number of graphene layers. We introduce the idea that the remaining contribution is entropic in nature and is connected to the fluctuations in the water-substrate interaction energy.
虽然实验和理论研究已经解决了石墨烯润湿性的问题,但孤立石墨烯单层上水的接触角的实际值仍然未知。尽管最近的实验文献表明,水在石墨上的接触角在 90-95°范围内,但有人认为,水在石墨烯上的接触角要么高达 127°,要么与石墨相比适度增强。在使用经验力场的经典分子动力学模拟的支持下,我们提出了一个论点,表明 127°的值是不现实的估计,而应该预期在 95-100°左右的值。我们的研究建立了水在基于石墨烯的表面上的粘附功变化与单个水分子与这些表面之间的相互作用势能之间的联系。我们表明,水在石墨烯上的接触角从石墨上的 90°变化到 127°,这意味着石墨的前两层都对与水的相互作用贡献了大约相同的能量。这种情况与水和这种基底之间的短程相互作用性质不兼容。我们还表明,水与基于石墨烯的基底之间的相互作用势能是水与基底粘附功的主要贡献,其相对大小与石墨烯层的数量无关。我们提出了这样的想法,即剩余的贡献是熵的性质,并与水-基底相互作用能量的波动有关。