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首页> 外文期刊>Langmuir: The ACS Journal of Surfaces and Colloids >Simulation of Interaction Forces between Nanoparticles in the Presence of Lennard-Jones Polymers:Freely Adsorbing Homopolymer Modifiers
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Simulation of Interaction Forces between Nanoparticles in the Presence of Lennard-Jones Polymers:Freely Adsorbing Homopolymer Modifiers

机译:Lennard-Jones聚合物存在下纳米粒子之间相互作用力的模拟:自由吸附均聚物改性剂

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摘要

The force between two nanoscale colloidal particles dispersed in a solution of freely adsorbing Lennard-Jones homopolymer modifiers is calculated using the expanded grand canonical Monte Carlo simulation method.We investigate the effect of polymer chain length (N),nanoparticle diameter (sigma_c),and colloid-polymer interaction energy (epsilon_(cp)) on polymer adsorption (GAMMA) and polymer-induced forces (F_p(r)) between nanoparticles in the full thermodynamic equilibrium condition.There is a strong correlation between polymer adsorption and the polymer-mediated nanoparticle forces.When the polymer adsorption is weak,as in the case of smaller diameters and short polymer chain lengths (sigma_c = 5,N = 10),the polymers do not have any significant effect on the bare nanoparticle interactions.The adsorbed amount increases with increasing particle diameter,polymer chain length,and colloid-polymer interaction energy.In general,for strong polymer-particle adsorption the polymer-governed force profiles between nanoparticles show short-range repulsion and long-ranged attraction,suggesting that homopolymers would not be ideal for achieving stabilization in nanoparticle dispersions.The attraction is likely due to bridging,as well as polymer segment-segment interactions.The location and magnitude of attractive minimum in the force profile can be controlled by varying N and epsilon_(cp)- The results show partial agreement and some marked differences with previous theoretical and experimental studies of forces in the limit of flat walls in an adsorbing polymer solution.The difference could be attributed to incorporation of long-ranged colloid-polymer potential in our simulations and the influence of the curvature of the nanoparticles.
机译:使用扩展的大正则蒙特卡罗模拟方法计算了分散在自由吸附的Lennard-Jones均聚物改性剂溶液中的两个纳米级胶体颗粒之间的力。我们研究了聚合物链长(N),纳米颗粒直径(sigma_c)和在完全热力学平衡条件下,胶体-聚合物在聚合物吸附(GAMMA)上的相互作用能(ε_(cp))和纳米颗粒之间的聚合物诱导力(F_p(r))。聚合物吸附与聚合物介导之间存在很强的相关性当聚合物吸附较弱时,如较小的直径和较短的聚合物链长(sigma_c = 5,N = 10),聚合物对裸露的纳米颗粒相互作用没有任何显着影响。吸附量增加随粒径,聚合物链长和胶体-聚合物相互作用能的增加而增加。通常,对于强的聚合物-颗粒吸附,聚合物控制的力纳米粒子之间的分布图显示了短程排斥和长程吸引力,这表明均聚物不是实现纳米粒子分散体稳定的理想选择。吸引力可能是由于桥接以及聚合物链段之间的相互作用所致。可以通过改变N和epsilon_(cp)来控制力分布中的最小吸引力-结果表明,与以前的理论和实验研究(在吸附性聚合物溶液中,平板壁的极限)存在部分一致性和明显差异。这归因于在我们的模拟中结合了长程胶体聚合物电势以及纳米粒子曲率的影响。

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