Vlcek Lukas, Zhang Zhan, Machesky Mike L, Fenter Paul, Rosenqvist Jorgen, Wesolowski David J, Anovitz Larry M, Predota Milan, Cummings Peter T
Department of Chemical Engineering, Vanderbilt University, Nashville, Tennessee 37235-1604, USA.
Langmuir. 2007 Apr 24;23(9):4925-37. doi: 10.1021/la063306d. Epub 2007 Mar 24.
The structure of water at the (110) surface of cassiterite (alpha-SnO2) at ambient conditions was studied by means of molecular dynamics simulations and X-ray crystal truncation rod experiments and interpreted with the help of the revised MUSIC model of surface protonation. The interactions of the metal oxide in the simulations were described by a recently developed classical force field based on the SPC/E model of water. Two extreme cases of completely hydroxylated and nonhydroxylated surfaces were considered along with a mixed surface with 50% dissociation. To study the dependence of the surface properties on pH, neutral and negatively charged variants of the surfaces were constructed. Axial and lateral density distributions of water for different types of surfaces were compared to each other and to experimental axial density distributions found by X-ray experiments. Although significant differences were found between the structures of the studied interfaces, the axial distances between Sn and O atoms are very similar and therefore could not be clearly distinguished by the diffraction technique. The explanation of structures observed in the density distributions was provided by a detailed analysis of hydrogen bonding in the interfacial region. It revealed qualitatively different hydrating patterns formed at neutral hydroxylated and nonhydroxylated surfaces and suggested a preference for the dissociative adsorption of water. At negatively charged surfaces, however, the situation can be reversed by the electric field stabilizing a hydrogen bond network similar to that found at the neutral nonhydroxylated surface. Comparison with previously studied rutile (alpha-TiO2) surfaces provided insight into the differences between the hydration of these two metal oxides, and an important role was ascribed to their different lattice parameters. A link to macroscopic properties was provided by the revised MUSIC surface protonation model. Explicit use of the Sn-O bond lengths based on ab initio calculations and H-bond configurations as inputs led to the prediction of a pH of zero net-proton induced surface charge (pHpzc) that agrees very well with those determined experimentally (about 4.4 at 298 K).
通过分子动力学模拟和X射线晶体截断棒实验研究了锡石(α-SnO₂)在环境条件下(110)表面的水结构,并借助表面质子化的修正MUSIC模型进行了解释。模拟中金属氧化物的相互作用由基于水的SPC/E模型最近开发的经典力场描述。考虑了完全羟基化和非羟基化表面的两种极端情况以及50%解离的混合表面。为了研究表面性质对pH的依赖性,构建了表面的中性和带负电变体。比较了不同类型表面水的轴向和横向密度分布,并与X射线实验发现的实验轴向密度分布进行了比较。尽管在所研究的界面结构之间发现了显著差异,但Sn和O原子之间的轴向距离非常相似,因此无法通过衍射技术清楚地区分。通过对界面区域氢键的详细分析,对密度分布中观察到的结构进行了解释。结果表明,在中性羟基化和非羟基化表面形成了性质不同的水合模式,并表明水倾向于解离吸附。然而,在带负电的表面,电场可以稳定类似于中性非羟基化表面的氢键网络,从而使情况发生逆转。与先前研究的金红石(α-TiO₂)表面的比较提供了对这两种金属氧化物水合差异的深入了解,并且它们不同的晶格参数被认为起着重要作用。修正的MUSIC表面质子化模型提供了与宏观性质的联系。明确使用基于从头算计算的Sn-O键长和氢键构型作为输入,导致预测的零净质子诱导表面电荷pH(pHpzc)与实验测定的值(298 K时约为4.4)非常吻合。