Chowdhary Janamejaya, Ladanyi Branka M
Department of Chemistry, Colorado State University, Fort Collins, Colorado 80523, USA.
Phys Rev E Stat Nonlin Soft Matter Phys. 2008 Mar;77(3 Pt 1):031609. doi: 10.1103/PhysRevE.77.031609. Epub 2008 Mar 24.
Within the capillary-wave model (CWM), the liquid-vapor interface is a hypothetical two-dimensional surface whose deviations from planarity are represented as long wavelength capillary waves. We modify the CWM for liquid-liquid interfaces and treat them as two harmonically interacting surfaces (model 1). Corrections to the model are proposed to prevent the usual divergence of the capillary-wave broadening in the thermodynamic limit by introducing a surface-bulk coupling (model 2) and to incorporate the curvature of the two surfaces (model 3). Expressions for the capillary-wave contribution to the surface tension of the interface are obtained. Molecular dynamics simulations are performed for two series of water-hydrocarbon interfacial systems (a) n -pentane, 2-methyl pentane, and 2,2,4-trimethyl pentane (constant chain length) and (b) n -octane, 2-methyl heptane, and 2,2,4-trimethyl pentane (constant molecular mass). A simple procedure to identify the molecular sites at the surface is utilized for a molecular representation of the surface. The distribution of these surface sites as well as the wave-vector dependence of surface fluctuations are analyzed in order to extract the parameters required for model 2. A small length scale is identified above which surface fluctuations correspond to capillary-wave fluctuations thereby connecting the molecular and mesoscopic scales. This approach is applied to all interfacial systems studied here and predictions based on the parameters found to be in good agreement with independent simulation results for surface tension and interfacial widths. Hydrocarbon branching has a small effect on model parameters.
在毛细波模型(CWM)中,液 - 气界面是一个假设的二维表面,其与平面的偏差被表示为长波长毛细波。我们对液 - 液界面的CWM进行了修改,并将它们视为两个谐波相互作用的表面(模型1)。通过引入表面 - 体相耦合(模型2)来提出对该模型的修正,以防止在热力学极限下毛细波展宽的通常发散,并纳入两个表面的曲率(模型3)。获得了毛细波对界面表面张力贡献的表达式。对两个系列的水 - 烃界面系统进行了分子动力学模拟:(a)正戊烷、2 - 甲基戊烷和2,2,4 - 三甲基戊烷(恒定链长),以及(b)正辛烷、2 - 甲基庚烷和2,2,4 - 三甲基戊烷(恒定分子量)。利用一种简单的方法来识别表面的分子位点,以对表面进行分子表示。分析这些表面位点的分布以及表面涨落的波矢依赖性,以提取模型2所需的参数。确定了一个小长度尺度,在该尺度以上表面涨落对应于毛细波涨落,从而连接了分子尺度和介观尺度。这种方法应用于此处研究的所有界面系统,基于所发现参数的预测与表面张力和界面宽度的独立模拟结果高度吻合。烃类支化对模型参数的影响较小。