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Self-assembly in block polyelectrolytes

机译:嵌段聚电解质的自组装

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The self-consistent field theory (SCFT) complemented with the Poisson-Boltzmann equation is employed to explore self-assembly of polyelectrolyte copolymers composed of charged blocks A and neutral blocks B. We have extended SCFT to dissociating triblock copolymers and demonstrated our approach on three characteristic examples: (1) diblock copolymer (AB) melt, (2) symmetric triblock copolymer (ABA) melt, (3) triblock copolymer (ABA) solution with added electrolyte. For copolymer melts, we varied the composition (that is, the total fraction of A-segments in the system) and the charge density on A blocks and calculated the phase diagram that contains ordered mesophases of lamellar, gyroid, hexagonal, and bcc symmetries, as well as the uniform disordered phase. The phase diagram of charged block copolymer melts in the charge density - system composition coordinates is similar to the classical phase diagram of neutral block copolymer melts, where the composition and the Flory mismatch interaction parameter XAB are used as variables. We found that the transitions between the polyelectrolyte mesophases with the increase of charge density occur in the same sequence, from lamellar to gyroid to hexagonal to bcc to disordered morphologies, as the mesophase transitions for neutral diblocks with the decrease of XAB. In a certain range of compositions, the phase diagram for charged triblock copolymers exhibits unexpected features, allowing for transitions from hexagonal to gyroid to lamellar mesophases as the charge density increases. Triblock polyelectrolyte solutions were studied by varying the charge density and solvent concentration at a fixed copolymer composition. Transitions from lamellar to gyroid and gyroid to hexagonal morphologies were observed at lower polymer concentrations than the respective transitions in the similar neutral copolymer, indicating a substantial influence of the charge density on phase behavior.
机译:用自洽场论(SCFT)补充Poisson-Boltzmann方程来探索由带电嵌段A和中性嵌段B组成的聚电解质共聚物的自组装。我们将SCFT扩展到解离三嵌段共聚物,并论证了我们在三种方法上的方法特征示例:(1)二嵌段共聚物(AB)熔体;(2)对称三嵌段共聚物(ABA)熔体;(3)含电解质的三嵌段共聚物(ABA)溶液。对于共聚物熔体,我们改变了组成(即系统中A段的总分数)和A嵌段上的电荷密度,并计算了包含层状,螺旋形,六边形和bcc对称的有序中间相的相图,以及统一的无序阶段。带电荷的嵌段共聚物熔体在电荷密度-系统组成坐标下的相图类似于中性嵌段共聚物熔体的经典相图,其中组成和弗洛里错配相互作用参数XAB被用作变量。我们发现,随着电荷密度的增加,聚电解质中间相之间的转变以相同的顺序发生,从层状到螺旋状再到六角形到bcc到无序形态,随着XAB的减少,中性二嵌段的中间相转变。在一定范围的组成中,带电三嵌段共聚物的相图表现出出乎意料的特征,随着电荷密度的增加,允许从六方中间相,螺旋状中间相过渡到层状中间相。通过改变固定共聚物组成下的电荷密度和溶剂浓度,研究了三嵌段聚电解质溶液。在比相似的中性共聚物中的相应转变低的聚合物浓度下观察到了从层状到螺旋状和从螺旋状到六角形的转变,这表明电荷密度对相行为的显着影响。

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