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首页> 外文期刊>The Journal of Chemical Physics >Structure of penetrable-rod fluids:Exact properties and comparison between Monte Carlo simulations and two analytic theories
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Structure of penetrable-rod fluids:Exact properties and comparison between Monte Carlo simulations and two analytic theories

机译:渗透棒流体的结构:蒙特卡洛模拟与两种解析理论的精确性质和比较

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Bounded potentials are good models to represent the effective two-body interaction in some colloidal systems,such as the dilute solutions of polymer chains in good solvents.The simplest bounded potential is that of penetrable spheres,which takes a positive finite value if the two spheres are overlapped,being 0 otherwise.Even in the one-dimensional case,the penetrable-rod model is far from trivial,since interactions are not restricted to nearest neighbors and so its exact solution is not known.In this paper the structural properties of one-dimensional penetrable rods are studied.We first derive the exact correlation functions of the penetrable-rod fluids to second order in density at any temperature,as well as in the high-temperature and zero-temperature limits at any density.It is seen that,in contrast to what is generally believed,the Percus-Yevick equation does not yield the exact cavity function in the hard-rod limit.Next,two simple analytic theories are constructed:a high-temperature approximation based on the exact asymptotic behavior in the limit T->infinity and a low-temperature approximation inspired by the exact result in the opposite limit T-> 0.Finally,we perform Monte Carlo simulations for a wide range of temperatures and densities to assess the validity of both theories.It is found that they complement each other quite well,exhibiting a good agreement with the simulation data within their respective domains of applicability and becoming practically equivalent on the borderline of those domains.A comparison with numerical solutions of the Percus-Yevick and the hypernetted-chain approximations is also carried out.Finally,a perspective on the extension of our two heuristic theories to the more realistic three-dimensional case is provided.
机译:有界电势是表示某些胶体系统中有效两体相互作用的良好模型,例如在良溶剂中聚合物链的稀溶液。最简单的有界电势是可渗透球体的势能,如果这两个球体都具有正的有限值重叠,否则为0。即使在一维情况下,可穿透杆模型也并非微不足道,因为相互作用不限于最近的邻居,因此它的精确解还未知。首先,我们得出了在任何温度下以及在任何密度下的高温和零温极限下,可渗透棒流体的精确相关函数与二阶密度的精确相关函数。与通常认为的相反,Percus-Yevick方程无法在硬杆极限中产生确切的腔函数。接下来,构建了两个简单的解析理论:根据极限T->无穷大的精确渐近行为进行重新近似,并根据相反极限T-> 0的精确结果启发进行低温近似。最后,我们对各种温度和密度进行了蒙特卡洛模拟评估这两种理论的有效性。发现它们很好地互补,在各自适用范围内与仿真数据显示出良好的一致性,并且在这些领域的边界上几乎等效。最后,对我们的两种启发式理论扩展到更现实的三维情况提供了一个视角。

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