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Phase equilibria of lattice polymers from histogram reweighting Monte Carlo simulations

机译:直方图加权加权蒙特卡洛模拟的晶格聚合物相平衡

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摘要

Histogram reweighting Monte Carlo simulations were used to obtain polymer/solvent phase diagrams for lattice homopolymers of chain lengths up to r = 1000 monomers. The simulation technique was based on performing a series of grand canonical Monte Carlo calculations for a small number of state points and combining the results to obtain the phase behavior of a system over a range of temperatures and densities. Critical parameters were determined from mixed-field finite-size scaling concepts by matching the order parameter distribution near the critical point to the distribution for the three-dimensional Ising universality class. Calculations for the simple cubic lattice (coordination number z = 6) and for a high coordination number version of the same lattice (z = 26) were performed for chain lengths significantly longer than those in previous simulation studies. The critical temperature was found to scale with a chain length following the Flory-Huggins functional form. For the z = 6 lattice, the extrapolated infinite chain length critical temperature is 3.71 +/- 0.01, in excellent agreement with previous calculations of the temperature at which the osmotic second virial coefficient is zero and the mean end-to-end distance proportional to the number of bonds. This confirms that the three alternative definitions of the Theta temperature are equivalent in the limit of long chains. The critical volume fraction scales with a chain length with an exponent equal to 0.38 +/- 0.01, in agreement with experimental data but in disagreement with polymer solution theories. The width of the coexistence curve prefactor was tentatively found to scale with a chain length with an exponent of 0.20 +/- 0.03 for z = 6 and 0.22 +/- 0.03 for z = 26. These values are near the lower range of values obtained from experimental data. [References: 23]
机译:使用直方图重加权蒙特卡罗模拟来获得链长最高为r = 1000个单体的晶格均聚物的聚合物/溶剂相图。该模拟技术基于对少量状态点执行一系列大正则蒙特卡罗计算,并将结果组合在一起,以获得在一定温度和密度范围内系统的相态。通过将临界点附近的阶次参数分布与三维Ising通用性类别的分布进行匹配,可以从混合域有限尺寸缩放概念确定关键参数。对于简单立方晶格(配位数z = 6)和相同晶格的高配位数版本(z = 26)的计算,其链长明显比以前的模拟研究更长。发现临界温度与遵循弗洛里-哈金斯功能形式的链长成比例。对于z = 6晶格,外推的无限链长临界温度为3.71 +/- 0.01,与先前计算的渗透第二维里系数为零且平均端对端距离成正比的温度计算非常吻合债券数量。这证实了Theta温度的三个替代定义在长链的极限内是等效的。与实验数据一致但与聚合物溶液理论不同的是,临界体积分数的链长与指数相等,为0.38 +/- 0.01。初步发现,共存曲线前置因子的宽度与链长成比例关系,z = 6时指数为0.20 +/- 0.03,z = 26时指数为0.22 +/- 0.03。这些值接近所得值的下限根据实验数据[参考:23]

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