State Key Laboratory of Supramolecular Structure and Materials, Laboratory of Theoretical and Computational Chemistry, Institute of Theoretical Chemistry, Jilin University, Changchun 130021, China.
Soft Matter. 2019 Jan 30;15(5):890-900. doi: 10.1039/c8sm02472c.
The effect of different lengths of solvophilic A and C blocks on the assembled configuration of intermediate solvophobic B-blocks in both ABA and ABC polymer brush systems is investigated via dissipative particle dynamics simulations. For the AB diblock copolymer brush with solvophilic A-blocks being grafted to the surface, B-blocks self-assemble into spherical micelle structures that are immersed in a layer formed by the A-blocks. Tethering a very small solvophilic block A(C) at the free end of the polymer brush pulls the B-blocks toward the polymer brush/solvent interface and increases their local density which can significantly change the B-block self-assembled structure from spherical micelles to ripples. By increasing the length of the outermost solvophilic blocks, the lateral density distribution of B-blocks can be further changed, resulting in the domain size of the ripple structure first decreasing and then increasing. Compared to the ABA system, the incompatibility between the A and C blocks can effectively reduce the vertical domain separation caused by the fusion of the upper and lower A blocks. Then, based on an AB diblock copolymer brush system with self-assembled spherical micelles, we introduce extremely short free solvophilic blocks A(C) in dilute solution that can be tethered to the free ends of the polymer brush by using a reaction model [Liu et al., J. Chem. Phys., 2007, 127, 144903]. We find that the micelles' coalescence is mainly affected by the content of tethered reactive solvophilic blocks, and only weakly affected by the reaction rate of the reversible reactions. This strategy of tethering solvophilic blocks to the ends of polymer brushes can be an effective way for the fabrication of stimuli-responsive surfaces and for adjusting nanoscopic surface patterns.
通过耗散粒子动力学模拟研究了不同长度的亲溶剂 A 和 C 嵌段对 AB 和 ABC 两亲聚合物刷体系中中间疏溶剂 B 嵌段组装构型的影响。对于接枝有亲溶剂 A 嵌段的 AB 两亲嵌段共聚物刷,B 嵌段自组装成浸入 A 嵌段形成的层中的球形胶束结构。在聚合物刷的自由端接上非常小的亲溶剂 A(C)嵌段会将 B 嵌段拉向聚合物刷/溶剂界面,并增加其局部密度,这会显著改变 B 嵌段的自组装结构,从球形胶束变为波纹。通过增加最外层亲溶剂块的长度,可以进一步改变 B 嵌段的横向密度分布,从而导致波纹结构的畴尺寸先减小后增大。与 ABA 体系相比,A 和 C 嵌段之间的不相容性可以有效地减少由于上下 A 嵌段融合引起的垂直畴分离。然后,基于具有自组装球形胶束的 AB 两亲嵌段共聚物刷体系,我们在稀溶液中引入了极短的自由亲溶剂 A(C)嵌段,这些嵌段可以通过反应模型[Liu 等人,J. Chem. Phys.,2007,127,144903]与聚合物刷的自由端连接。我们发现胶束的聚结主要受连接的反应性亲溶剂嵌段的含量影响,而受可逆反应的反应速率的影响较弱。这种将亲溶剂嵌段连接到聚合物刷末端的策略可以是制造刺激响应表面和调整纳米级表面图案的有效方法。