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Transport phenomena and microscopic structure in partially miscible binary fluids: A simulation study of the symmetrical Lennard-Jones mixture

机译:部分混溶的运输现象和微观结构   二元流体:对称Lennard-Jones混合物的模拟研究

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摘要

Static and dynamic structure factors and various transport coefficients arecomputed for a Lennard-Jones model of a binary fluid (A,B) with a symmetricalmiscibility gap, varying both temperature and relative concentration of themixture. The model is first equilibrated by a semi-grandcanonical Monte Carlomethod, choosing the temperature and chemical potential difference $\Delta \mu$between the two species as the given independent variables. Varying for $\Delta\mu=0$ the temperature and particle number $N$ over a wide range, the locationof the coexistence curve in the thermodynamic limit is estimated.Well-equilibrated configurations from these Monte Carlo runs are used asinitial states for microcanonical Molecular Dynamics runs, in order to studythe microscopic structure and the behavior of transport coefficients as well asdynamic correlation functions along the coexistence curve. Dynamic structurefactors $S_{\alpha \beta} (q,t)$ (and the corresponding static functions$S_{\alpha \beta} (q)$) are recorded ($\alpha, \beta, \in$ A,B), $q$ being thewavenumber and $t$ the time, as well as the mean square displacements of theparticles (to obtain the self-diffusion constants $D_{\rm A}$, $D_{\rm B}$) andtransport coefficients describing collective transport, such as theinterdiffusion constant and the shear viscosity. The minority species is foundto diffuse a bit faster than the majority species. Despite the presence ofstrong concentration fluctuations in the system the Stokes-Einstein relation isa reasonable approximation.
机译:对于具有对称溶混间隙,同时改变混合物温度和相对浓度的二元流体(A,B)的Lennard-Jones模型,计算了静态和动态结构因子以及各种传输系数。首先通过半大模型蒙特卡洛方法对模型进行平衡,选择两个物种之间的温度和化学势差$ \ Delta \ mu $作为给定的独立变量。在$ \ Delta \ mu = 0 $的温度和粒子数$ N $在很宽的范围内变化时,估算了共存曲线在热力学极限中的位置。这些蒙特卡洛试验的均衡平衡构型被用作微规范的初始状态。为了研究微观结构和沿着共存曲线的传输系数以及动态相关函数,进行了分子动力学研究。记录了动态结构因子$ S _ {\ alpha \ beta}(q,t)$(以及相应的静态函数$ S _ {\ alpha \ beta}(q)$)($ \ alpha,\ beta,\ in $ A, B),$ q $是波数,$ t $是时间,还有粒子的均方位移(以获得自扩散常数$ D _ {\ rm A} $,$ D _ {\ rm B} $)以及描述集体输运的输运系数,例如相互扩散常数和剪切粘度。发现少数种比多数种扩散得快。尽管系统中存在强烈的浓度波动,但斯托克斯-爱因斯坦关系还是一个合理的近似值。

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