Cao Xue-Zheng, Merlitz Holger, Forest M Gregory
Departments of Mathematics and Applied Physical Sciences, University of North Carolina at Chapel Hill, Chapel Hill, North Carolina 27599-3250, United States.
Department of Physics, Xiamen University, Xiamen 361005, P.R. China.
J Phys Chem Lett. 2019 Sep 5;10(17):4968-4973. doi: 10.1021/acs.jpclett.9b01954. Epub 2019 Aug 14.
We combine molecular dynamics simulations, imaging and data analysis, and the Green-Kubo summation formula for the relaxation modulus () to elicit the structure and rheology of unentangled polymer-nanoparticle composites distinguished by small NPs and strong NP-monomer attraction, ε ≫ . A reptation-like plateau emerges in () beyond a terminal relaxation time scale as the volume fraction, , of NPs increases, coincident with a structure transition. A condensed phase of NP-aggregates forms, tightly interlaced with thin sheets of polymer chains, the remaining phase consisting of free chains void of NPs. Rouse mode analyses are applied to the two individual phases, revealing that long-wavelength Rouse modes in the aggregate phase are the source of reptation-like relaxation. Imaging reveals chain motion confined within the thin sheets between NPs and exhibits a 2D analogue of classical reptation. In the NP-free phase, Rouse modes relax indistinguishable from a neat polymer melt. The Fourier transform of () reveals a sol-gel transition across a broad frequency spectrum, tuned by and ε above critical thresholds, below which all structure and rheological transitions vanish.
我们结合分子动力学模拟、成像与数据分析,以及用于松弛模量()的格林-库博求和公式,以揭示由小纳米粒子和强纳米粒子-单体吸引力(ε≫)所区分的非缠结聚合物-纳米粒子复合材料的结构与流变学。随着纳米粒子的体积分数增加,在超过终端松弛时间尺度时,()中会出现类似爬杆的平台期,这与结构转变同时发生。形成了纳米粒子聚集体的凝聚相,与聚合物链薄片紧密交织,其余相由不含纳米粒子的自由链组成。对两个单独的相进行了Rouse模式分析,结果表明聚集相中的长波长Rouse模式是类似爬杆松弛的来源。成像显示链运动局限于纳米粒子之间的薄片内,并呈现出经典爬杆的二维类似物。在无纳米粒子相,Rouse模式的松弛与纯聚合物熔体无法区分。()的傅里叶变换揭示了在宽频谱上的溶胶-凝胶转变,该转变由高于临界阈值的和ε调节,低于该阈值时所有结构和流变转变均消失。