热塑性淀粉纳米复合材料的 MARTINI 粗粒度力场

IF 2.9 2区 化学 Q3 CHEMISTRY, PHYSICAL
Ankit Patidar*,  and , Gaurav Goel*, 
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引用次数: 0

摘要

热塑性淀粉(TPS)是一种优良的成膜材料,添加填料(如四甲基铵蒙脱石(TMA-MMT)粘土)后,它在包装领域的应用大大扩展。我们首先使用全原子 (AA) 模拟来预测 TPS 熔体和 TPS-TMA-MMT 复合材料的几种宏观(杨氏模量、玻璃化转变温度、密度)和微观(沿 1-4 和 1-6 糖苷键的构象、复合材料形态)特性。聚合物-表面(弱排斥性)、增塑剂-表面(吸引力)和聚合物-增塑剂(弱吸引力)相互作用的相互作用导致了构象和动力学特性,这些特性不同于具有吸引力或排斥性聚合物-表面相互作用的体系。AA 特性子集被用于参数化熔体和复合体系的 MARTINI-2 粗粒度(CG)力场(FF)。利用 AA TPS 熔体中的二体过量熵、密度、键和角分布,确定了淀粉和直链淀粉的缺失键参数以及 1-4 和 1-6 连接的 α-D 葡萄糖的珠类型。这种新的 MARTINI-2 CG 模型还与 TPS 熔体的 MARTINI-3 模型进行了比较。然而,由于需要可极化的水模型,因此复合体系必须使用 MARTINI-2 FF 模型。这种基于液液分配的 FF 显示聚合物链在粘土表面附近冻结和压实,TPS 聚合物的高共价配位环单元对与蒙脱石薄片之间的分散相互作用降低,进一步加剧了聚合物链的冻结和压实。通过对 TPS-MMT 交叉相互作用的有效分散成分进行重定标,对复合系统的 MARTINI-2 FF 进行了优化,并将长 AA 模拟获得的结构(链尺寸分布)、热力学(链构象熵和密度)和动力学(自扩散系数)特性作为优化的约束条件。获得的 CG FF 参数为参数估计中未使用的熔体和复合材料系统的其他一些特性提供了极好的估计值,从而确定了所开发模型的稳健性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

MARTINI Coarse-Grained Force Field for Thermoplastic Starch Nanocomposites

MARTINI Coarse-Grained Force Field for Thermoplastic Starch Nanocomposites

Thermoplastic starch (TPS) is an excellent film-forming material, and the addition of fillers, such as tetramethylammonium-montmorillonite (TMA-MMT) clay, has significantly expanded its use in packaging applications. We first used an all-atom (AA) simulation to predict several macroscopic (Young’s modulus, glass transition temperature, density) and microscopic (conformation along 1–4 and 1–6 glycosidic linkages, composite morphology) properties of TPS melt and TPS–TMA-MMT composite. The interplay of polymer-surface (weakly repulsive), plasticizer-surface (attractive), and polymer-plasticizer (weakly attractive) interactions leads to conformational and dynamics properties distinct from those in systems with either attractive or repulsive polymer-surface interactions. A subset of AA properties was used to parametrize the MARTINI-2 coarse-grained (CG) force field (FF) for the melt and composite systems. The missing bonded parameters of amylose and amylopectin and the bead types for 1–4 and 1–6 linked α-D glucose were determined using two-body excess entropy, density, and bond and angle distributions in the AA TPS melt. This new MARTINI-2 CG model was also compared with the MARTINI-3 model for the TPS melt. However, the requirement of a polarizable water model necessitates the use of MARTINI-2 FF for the composite system. This liquid–liquid partitioning-based FF shows freezing and compaction of polymer chains near the clay surface, further accentuated by lowering of dispersive interactions between pairs of high-covalent-coordination ring units of TPS polymers and the montmorillonite sheet. A rescaling of the effective dispersive component of TPS–MMT cross interactions was used to optimize the MARTINI-2 FF for the composite system with structural (chain size distribution), thermodynamic (chain conformational entropy and density), and dynamic (self-diffusion coefficient) properties obtained from long AA simulations forming the constraints for optimization. The obtained CG FF parameters provided excellent estimates for several other properties of the melt and composite systems not used in parameter estimation, thus establishing the robustness of the developed model.

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来源期刊
CiteScore
5.80
自引率
9.10%
发文量
965
审稿时长
1.6 months
期刊介绍: An essential criterion for acceptance of research articles in the journal is that they provide new physical insight. Please refer to the New Physical Insights virtual issue on what constitutes new physical insight. Manuscripts that are essentially reporting data or applications of data are, in general, not suitable for publication in JPC B.
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