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Ordering of anisotropic nanoparticles in diblock copolymer lamellae : simulations with dissipative particle dynamics and a molecular theory

机译:二嵌段共聚物薄片中各向异性纳米粒子的有序性:耗散粒子动力学和分子理论的模拟

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摘要

Local distribution and orientation of anisotropic nanoparticles in microphase-separated symmetric diblock copolymers has been simulated using dissipative particle dynamics and analyzed with a molecular theory. It has been demonstrated that nanoparticles are characterized by a non-trivial orientational ordering in the lamellar phase due to their anisotropic interactions with isotropic monomer units. In the simulations, the maximum concentration and degree of ordering are attained for non-selective nanorods near the domain boundary. In this case, the nanorods have a certain tendency to align parallel to the interface in the boundary region and perpendicular to it inside the domains. Similar orientation ordering of nanoparticles located at the lamellar interface is predicted by the molecular theory which takes into account that the nanoparticles interact with monomer units via both isotropic and anisotropic potentials. Computer simulations enable one to study the effects of the nanorod concentration, length, stiffness, and selectivity of their interactions with the copolymer components on the phase stability and orientational order of nanoparticles. If the volume fraction of the nanorods is lower than 0.1, they have no effect on the copolymer transition from the disordered state into a lamellar microstructure. Increasing nanorod concentration or nanorod length results in clustering of the nanorods and eventually leads to a macrophase separation, whereas the copolymer preserves its lamellar morphology. Segregated nanorods of length close to the width of the diblock copolymer domains are stacked side by side into smectic layers that fill the domain space. Thus, spontaneous organization and orientation of nanorods leads to a spatial modulation of anisotropic composite properties which may be important for various applications.
机译:使用耗散粒子动力学模拟了微相分离的对称二嵌段共聚物中各向异性纳米粒子的局部分布和取向,并用分子理论进行了分析。已经证实,由于纳米颗粒与各向同性单体单元的各向异性相互作用,其在层状相中具有非平凡的取向次序。在模拟中,在畴边界附近获得了非选择性纳米棒的最大浓度和有序度。在这种情况下,纳米棒具有一定的趋势,该趋势平行于边界区域中的界面并垂直于区域内。通过考虑到纳米颗粒通过各向同性和各向异性电势与单体单元相互作用的分子理论来预测位于层状界面处的纳米颗粒的相似取向次序。计算机模拟使人们能够研究纳米棒的浓度,长度,刚度及其与共聚物组分的相互作用的选择性对纳米颗粒的相稳定性和取向顺序的影响。如果纳米棒的体积分数小于0.1,则它们对共聚物从无序状态到层状微结构的转变没有影响。纳米棒浓度或纳米棒长度的增加导致纳米棒的聚集,并最终导致宏观相分离,而共聚物保留了其层状形态。将长度接近于二嵌段共聚物域的宽度的分离的纳米棒并排堆叠成填充该域空间的近晶层。因此,纳米棒的自发组织和取向导致各向异性复合特性的空间调节,这对于各种应用而言可能是重要的。

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