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首页> 外文期刊>The Journal of Chemical Physics >Phase behavior and percolation in mixed patchy colloids
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Phase behavior and percolation in mixed patchy colloids

机译:混合斑块胶体中的相行为和渗透

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Patchy colloids can be modeled as hard spheres with directional conical association sites. A variety of physical phenomena have been discovered in the patchy colloid system due to its short range and directional interactions. In this work, we combined a cluster distribution theory with generalized Flory and Stockmayer percolation theory to investigate the interplay between phase behavior and percolation for a binary patchy colloid system. The binary patchy colloid system consists of solute molecules with spherically symmetric bonding sites and solvents with two singly bondable sites. Wertheim's first order thermodynamic perturbation theory (TPT1) has been widely applied to the patchy colloids system and it has been combined with percolation theory to study the percolation threshold. However, due to assumptions behind TPT1, it will lose accuracy for a system in which particles have multiple association sites or multiply bondable sites. A recently proposed cluster distribution theory accurately models association at sites that can form multiple bonds. In this work, we investigate the comparison among cluster distribution theory, TPT1, and Monte Carlo simulation for the bonding states of this binary system in which cluster distribution theory shows excellent agreement with Monte Carlo simulation, while TPT1 has a large deviation with the simulation. Cluster distribution theory was further combined with the Flory and Stockmayer percolation theory to investigate the interplay between phase behavior and percolation threshold. We found that the reduced density and the relative bonding strength of solvent-solvent association and solute-solvent association are key factors for the phase behavior and percolation. Percolation can form at low density and low temperature in the vapor phase of this binary system, where the star-like molecules with 12 long branches formed.
机译:斑片状胶体可以模拟为具有定向锥形结合位点的硬球。由于短程和定向相互作用,在斑片状胶体系统中发现了多种物理现象。在这项工作中,我们将团簇分布理论与广义Flory和Stockmayer渗流理论相结合,研究了二元斑块胶体系统的相行为和渗流之间的相互作用。二元斑片状胶体体系由具有球对称键合位点的溶质分子和具有两个单键合位点的溶剂组成。Wertheim的一阶热力学微扰理论(TPT1)已广泛应用于斑片状胶体体系,并与渗流理论相结合来研究渗流阈值。然而,由于TPT1背后的假设,对于粒子具有多个缔合位点或多个可键合位点的系统,它将失去准确性。最近提出的簇分布理论精确地模拟了可以形成多个键的位点上的关联。在这项工作中,我们研究了团簇分布理论、TPT1和Monte Carlo模拟对该二元体系键态的比较,其中团簇分布理论与Monte Carlo模拟非常一致,而TPT1与模拟有很大的偏差。将团簇分布理论与Flory和Stockmayer渗流理论进一步结合,研究了相行为与渗流阈值之间的相互作用。我们发现,溶剂-溶剂缔合和溶质-溶剂缔合的还原密度和相对键合强度是影响相行为和渗流的关键因素。在这个双星系统的汽相中,低密度和低温下可以形成渗流,在那里形成了具有12个长分支的星形分子。

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