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嵌段共聚链的链动力学与聚(甲基丙烯酸甲酯)共混物中的聚(氧化乙烯):耦合模型分析。

Interchain coupled chain dynamics of poly(ethylene oxide) in blends with poly(methyl methacrylate): coupling model analysis.

机构信息

CNR-IPCF, Dipartimento di Fisica, Università di Pisa, Largo Bruno Pontecorvo 3, I-56127 Pisa, Italy.

出版信息

J Chem Phys. 2011 Nov 21;135(19):194902. doi: 10.1063/1.3662130.

Abstract

Quasielastic neutron scattering and molecular dynamics simulation data from poly(ethylene oxide) (PEO)/poly(methyl methacrylate) (PMMA) blends found that for short times the self-dynamics of PEO chain follows the Rouse model, but at longer times past t(c) = 1-2 ns it becomes slower and departs from the Rouse model in dependences on time, momentum transfer, and temperature. To explain the anomalies, others had proposed the random Rouse model (RRM) in which each monomer has different mobility taken from a broad log-normal distribution. Despite the success of the RRM, Diddens et al. [Eur. Phys. Lett. 95, 56003 (2011)] extracted the distribution of friction coefficients from the MD simulations of a PEO/PMMA blend and found that the distribution is much narrower than expected from the RRM. We propose a simpler alternative explanation of the data by utilizing alone the observed crossover of PEO chain dynamics at t(c). The present problem is just a special case of a general property of relaxation in interacting systems, which is the crossover from independent relaxation to coupled many-body relaxation at some t(c) determined by the interaction potential and intermolecular coupling/constraints. The generality is brought out vividly by pointing out that the crossover also had been observed by neutron scattering from entangled chains relaxation in monodisperse homopolymers, and from the segmental α-relaxation of PEO in blends with PMMA. The properties of all the relaxation processes in connection with the crossover are similar, despite the length scales of the relaxation in these systems are widely different.

摘要

聚环氧乙烷(PEO)/聚甲基丙烯酸甲酯(PMMA)共混物的准弹性中子散射和分子动力学模拟数据表明,在短时间内,PEO 链的自动力学遵循 Rouse 模型,但在更长的时间 t(c) = 1-2 ns 后,它的速度变慢,并在时间、动量传递和温度的依赖性上偏离 Rouse 模型。为了解释这些异常,其他人提出了随机 Rouse 模型(RRM),其中每个单体的迁移率都取自广泛的对数正态分布。尽管 RRM 取得了成功,但 Diddens 等人[Eur. Phys. Lett. 95, 56003 (2011)]从 PEO/PMMA 共混物的 MD 模拟中提取了摩擦系数分布,发现分布比 RRM 预期的要窄得多。我们通过利用 PEO 链动力学在 t(c)处的观察到的交叉,提出了一个更简单的替代解释。目前的问题只是相互作用系统中弛豫的一般性质的一个特殊情况,即在某些由相互作用势和分子间耦合/约束决定的 t(c)处,从独立弛豫到耦合多体弛豫的交叉。通过指出中子散射也已经观察到从单分散均聚物中缠结链弛豫,以及从 PEO 与 PMMA 的混合物中的分段α弛豫,这生动地说明了这种普遍性。尽管这些系统中的弛豫的长度尺度差异很大,但与交叉相关的所有弛豫过程的性质都是相似的。

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