H H Wills Physics Laboratory, University of Bristol, Tyndall Avenue, Bristol BS8 1TL, UK.
J Phys Condens Matter. 2010 Aug 18;22(32):325108. doi: 10.1088/0953-8984/22/32/325108. Epub 2010 Jul 29.
Using a fundamental measure density functional theory we investigate both bulk and inhomogeneous systems of the binary non-additive hard sphere model. For sufficiently large (positive) non-additivity the mixture phase separates into two fluid phases with different compositions. We calculate bulk fluid-fluid coexistence curves for a range of size ratios and non-additivity parameters and find that they compare well to simulation results from the literature. Using the Ornstein-Zernike equation, we investigate the asymptotic, [Formula: see text], decay of the partial pair correlation functions, g(ij)(r). At low densities a structural crossover occurs in the asymptotic decay between two different damped oscillatory modes with different wavelengths corresponding to the two intra-species hard-core diameters. On approaching the fluid-fluid critical point there is a Fisher-Widom crossover from exponentially damped oscillatory to monotonic asymptotic decay. Using the density functional we calculate the density profiles for the planar free fluid-fluid interface between coexisting fluid phases. We show that the type of asymptotic decay of g(ij)(r) not only determines the asymptotic decay of the interface profiles, but is also relevant for intermediate and even short-ranged behaviour. We also determine the surface tension of the free fluid interface, finding that it increases with non-additivity, and that on approaching the critical point mean-field scaling holds.
我们采用基本测量密度泛函理论研究了二元非加和硬球模型的体相和非均匀体系。对于足够大的(正)非加和性,混合物会分相成具有不同组成的两种流体相。我们计算了一系列尺寸比和非加和参数的体相流体-流体共存曲线,并发现它们与文献中的模拟结果吻合较好。我们利用奥恩斯坦-泽尼克方程研究了部分关联函数 g(ij)(r)的渐近,[公式:见文本],衰减。在低密度下,在两个不同的阻尼振荡模式之间会发生结构交叉,这两种模式具有不同的波长,对应于两种内部分子的硬球直径。在接近流体-流体临界点时,会发生从指数衰减振荡到单调渐近衰减的费希尔-怀道交叉。我们利用密度泛函计算了共存流体相之间的平面自由流体-流体界面的密度分布。我们表明,g(ij)(r)的渐近衰减类型不仅决定了界面分布的渐近衰减,而且与中间甚至短程行为也有关。我们还确定了自由流体界面的表面张力,发现它随非加和性的增加而增加,并且在接近临界点时,平均场标度成立。