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首页> 外文期刊>Journal of chemical theory and computation: JCTC >Simulation of interaction forces between nanoparticles: End-grafted polymer modifiers
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Simulation of interaction forces between nanoparticles: End-grafted polymer modifiers

机译:纳米颗粒之间的相互作用势的模拟:末端接枝聚合物改性剂

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摘要

The interaction forces between nanoscale colloidal particles coated with end-grafted Lennard-Jones homopolymers are calculated using off-lattice Monte Carlo simulations in the NVT ensemble. The focus of this work is on grafted polymers that are of approximately the same size as the nanoparticle, a regime intermediate to the star-polymer and Derjaguin limits. The effects of chain length (N), nanoparticle diameter (sigma(c)), grafting density (rho(a)), and colloid-polymer and polymer-polymer interaction energies (epsilon cp and epsilon pp) on the polymer-induced force between the nanoparticles are explored. The inclusion of attractive dispersion interactions between the particle and polymeric modifier results in either long-ranged attraction and short-ranged repulsion or pure repulsion, depending on the molecular parameters. The polymer-induced attraction occurs even under good solvent conditions below a threshold grafting density (rho a) and chain length (N) and could be attributed to both bridging (colloid-polymer) and intersegmental (polymer-polymer) attraction. Above the threshold rho(a) and N values, chain entropy and excluded volume effects begin to dominate and lead eventually to polymer-induced repulsion and, consequently, nanoparticle stabilization. These results point to the importance of considering dispersion attractions between grafted segments and the nanoparticle surface in modeling these high-curvature colloid interactions.
机译:纳米级胶体颗粒之间的相互作用力在NVT集合中使用偏离格子蒙特卡罗模拟计算。这项工作的重点是嫁接聚合物,其与纳米粒子大致相同的大小,该方案中间体与星形聚合物和Derjaguin限制的含量。链长(n),纳米颗粒直径(σ),接枝密度(rho(a))和胶体 - 聚合物和聚合物 - 聚合物相互作用能量(εcp和epsilon pp)对聚合物诱导的力的影响探索纳米颗粒之间。将颗粒和聚合物改性剂之间的吸引性分散相互作用在一起导致长距离的吸引力和短途排斥或纯排斥,这取决于分子参数。即使在低于阈值接枝密度(RHO A)和链长(N)的良好溶剂条件下也发生聚合物诱导的吸引力,并且可归因于桥接(胶体聚合物)和基于聚合物(聚合物 - 聚合物)吸引物。高于阈值rhO(a)和n值,链熵和排除的体积效应开始占据主导地位并最终导致聚合物诱导的排斥,并且因此,纳米粒子稳定性。这些结果指出了考虑接枝段和纳米颗粒表面之间的分散景点在模拟这些高曲率胶体相互作用时的重要性。

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