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Poly(methyl methacrylate)-block-poly(n-butyl methacrylate) Diblock Copolymer Micelles in an Ionic Liquid: Scaling of Core and Corona Size with Core Block Length

机译:离子液体中的聚(甲基丙烯酸甲酯)-嵌段-聚(甲基丙烯酸正丁酯)二嵌段共聚物胶束:核和电晕尺寸随核嵌段长度的变化

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The structure of poly(methyl methacrylate)-block-poly(n-butyl methacrylate) (PMMA-b-PnBMA) micelles in the room temperature ionic liquid 1-ethyl-3-methylimidazolium bis(trifluoromethylsulfonyl)imide ([EMIM][TFSI]), a selective solvent for the PMMA block, has been studied using dynamic light scattering (DLS) and small-angle X-ray scattering (SAXS). A series of seven PMMA-b-PnBMA diblock copolymers, were prepared by reversible addition-fragmentation chain-transfer (RAFT) polymerization, in which the degree of polymerization of the PMMA block was kept constant while the PnBMA block length was varied. All the polymers formed spherical micelles at ambient temperature in dilute solution; their hydrodynamic radius (R-h) and core radius (R-c) were obtained by DLS and SAXS, respectively. It was found that R-c and the degree of polymerization of the core block, N-B, followed a power law relationship in which R-c similar to N-B(0.71 +/- 0.01). The corona thickness (L-corona), given by the difference of R-h and R-c, does not show any apparent dependence on N-B. These results were compared to scaling theory, and were found to be only in partial agreement with the star model proposed by Halperin et al. However, the mean-field calculations of micellar dimensions by Nagarajan and Ganesh were in excellent agreement with the, data. This comprehensive experimental study, provides precise quantification of the R-c and L-corona dependence on core block:lengths, due to the use of seven different block copolymers with identical corona block lengths.
机译:室温离子液体1-乙基-3-甲基咪唑双(三氟甲基磺酰基)酰亚胺([EMIM] [TFSI)中的聚(甲基丙烯酸甲酯)-嵌段-聚(甲基丙烯酸正丁酯)(PMMA-b-PnBMA)胶束的结构]),一种用于PMMA嵌段的选择性溶剂,已使用动态光散射(DLS)和小角度X射线散射(SAXS)进行了研究。通过可逆加成-断裂链转移(RAFT)聚合制备了一系列七个PMMA-b-PnBMA二嵌段共聚物,其中PMMA嵌段的聚合度保持不变,而PnBMA嵌段的长度却变化。所有的聚合物在室温下在稀溶液中形成球形胶束。它们的流体动力学半径(R-h)和芯半径(R-c)分别通过DLS和SAXS获得。发现R-c和核心嵌段的聚合度N-B遵循幂律关系,其中R-c类似于N-B(0.71 +/- 0.01)。由R-h和R-c之差得出的电晕厚度(L-电晕)对N-B没有明显的依赖性。这些结果与比例理论进行了比较,发现仅与Halperin等人提出的恒星模型部分吻合。但是,由Nagarajan和Ganesh进行的胶束尺寸平均场计算与这些数据非常吻合。这项全面的实验研究,由于使用了七个具有相同电晕嵌段长度的不同嵌段共聚物,因此可以精确定量R-c和L-电晕对核心嵌段长度的依赖性。

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