Krishna Rajamani
Van't Hoff Institute for Molecular Sciences, University of Amsterdam, Science Park 904, 1098 XH Amsterdam, The Netherlands.
Phys Chem Chem Phys. 2015 Nov 7;17(41):27428-36. doi: 10.1039/c5cp04520g.
This work investigates the transient equilibration process when partially miscible ternary liquid mixtures of two different compositions are brought into contact with each other. Diffusional coupling effects are shown to become increasingly significant as the mixture compositions approach the meta-stable regions of the phase equilibrium diagrams. The proper modelling of coupled diffusion phenomena requires the use of a Fick diffusivity matrix [D], with inclusion of non-zero off-diagonal elements. The primary objective of this article is to develop a simple, robust, procedure for the estimation of the matrix [D], using the Maxwell-Stefan (M-S) formulation as a convenient starting point. In the developed simplified approach, the Fick diffusivity matrix [D] is expressed as the product of a scalar diffusivity and the matrix of thermodynamic correction factors [Γ]. By detailed examination of experimental data for the matrix [D] in a wide variety of ternary mixtures, it is deduced that the major contribution of diffusional coupling arises from the contributions of non-ideal solution thermodynamics, quantified by the matrix of thermodynamic correction factors [Γ]. An important consequence of strong thermodynamic coupling is that equilibration trajectories are serpentine in shape and may exhibit incursions into meta-stable zones opening up the possibility of spontaneous emulsification and the Ouzo effect. If diffusional coupling effects are ignored, the equilibration trajectory is linear in composition space. For a wide variety of partially miscible ternary mixtures, it is demonstrated that the corresponding linear equilibration trajectories do not anticipate the possibility of emulsification.
本研究探讨了两种不同组成的部分互溶三元液体混合物相互接触时的瞬态平衡过程。结果表明,随着混合物组成接近相平衡图的亚稳区域,扩散耦合效应变得越来越显著。对耦合扩散现象进行恰当建模需要使用包含非零非对角元素的菲克扩散率矩阵[D]。本文的主要目标是开发一种简单、稳健的程序,以麦克斯韦-斯蒂芬(M-S)公式为便利的起点来估计矩阵[D]。在开发的简化方法中,菲克扩散率矩阵[D]表示为标量扩散率与热力学校正因子矩阵[Γ]的乘积。通过详细考察各种三元混合物中矩阵[D]的实验数据,推断出扩散耦合的主要贡献源于非理想溶液热力学的贡献,由热力学校正因子矩阵[Γ]量化。强热力学耦合的一个重要结果是平衡轨迹呈蛇形,可能会侵入亚稳区,从而引发自发乳化和奥祖效应。如果忽略扩散耦合效应,平衡轨迹在组成空间中是线性的。对于各种部分互溶三元混合物,证明相应的线性平衡轨迹无法预测乳化的可能性。