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首页> 外文期刊>The Journal of Chemical Physics >Local and chain dynamics in miscible polymer blends: A Monte Carlo simulation study
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Local and chain dynamics in miscible polymer blends: A Monte Carlo simulation study

机译:混溶性聚合物共混物中的局部和链动力学:蒙特卡洛模拟研究

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Local chain structure and local environment play an important role in the dynamics of polymer chains in miscible blends. In general, the friction coefficients that describe the segmental dynamics of the two components in a blend differ from each other and from those of the pure melts. In this work, we investigate polymer blend dynamics with Monte Carlo simulations of a generalized bond fluctuation model, where differences in the interaction energies between nonbonded nearest neighbors distinguish the two components of a blend. Simulations employing only local moves and respecting a no bond crossing condition were carried out for blends with a range of compositions, densities, and chain lengths. The blends investigated here have long time dynamics in the crossover region between Rouse and entangled behavior. In order to investigate the scaling of the self-diffusion coefficients, characteristic chain lengths N-c are calculated from the packing length of the chains. These are combined with a local mobility mu determined from the acceptance rate and the effective bond length to yield characteristic self-diffusion coefficients D-c=mu/N-c. We find that the data for both melts and blends collapse onto a common line in a graph of reduced diffusion coefficients D/D-c as a function of reduced chain length N/N-c. The composition dependence of dynamic properties is investigated in detail for melts and blends with chains of length N=20 at three different densities. For these blends, we calculate friction coefficients from the local mobilities and consider their composition and pressure dependence. The friction coefficients determined in this way show many of the characteristics observed in experiments on miscible blends.
机译:局部链结构和局部环境在混溶共混物中聚合物链的动力学中起重要作用。通常,描述混合物中两种组分的分段动力学的摩擦系数彼此不同,而与纯熔体的摩擦系数不同。在这项工作中,我们使用广义键涨落模型的蒙特卡洛模拟研究聚合物共混物动力学,其中未键合的最近邻之间相互作用能的差异区分了共混物的两种成分。对于具有一定范围的组成,密度和链长的共混物,仅采用局部运动并遵守无键交叉条件进行了模拟。此处研究的混合物在唤醒和纠缠行为之间的过渡区域中具有长时间的动力学。为了研究自扩散系数的标度,从链的堆积长度计算特征链长度N-c。将它们与根据接受率和有效键长确定的局部迁移率μ组合,以产生特征性的自扩散系数D-c = mu / N-c。我们发现,熔体和共混物的数据在减少的扩散系数D / D-c随减少的链长N / N-c的函数图中崩溃到一条公共线上。对于在三种不同密度下长度为N = 20的链的熔体和共混物,详细研究了其动态性能的成分依赖性。对于这些混合物,我们从局部流动性计算摩擦系数,并考虑其组成和压力依赖性。以这种方式确定的摩擦系数显示出在混溶共混物实验中观察到的许多特性。

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