Kyrylyuk A V, Fraaije J G E M
Soft Condensed Matter Group, Leiden Institute of Chemistry, Leiden University, P. O. Box 9502, 2300 RA Leiden, The Netherlands.
J Chem Phys. 2004 Nov 8;121(18):9166-71. doi: 10.1063/1.1806132.
A mean-field dynamic density functional theory is used to describe a phase diagram of concentrated solutions of weakly charged flexible block polyelectrolytes in a film. Electrostatics is taken into account by applying the local electroneutrality constraint (the Donnan membrane equilibrium approach). In the Donnan limit it is assumed that a salt added to the solution perfectly screens long-range electrostatic interactions. The phase diagram of a solution of a triblock polyelectrolyte in a film as a function of the solvent concentration and the charge of the polyelectrolyte (solvophilic) block is calculated for a given film thickness. The phase behavior of the block polyelectrolyte film arises from the interplay between surface-induced alignment and the electrostatically-driven structure formation. The observed mesoscopic structures (lamellar, perforated lamellar, cylindrical, micellar, and mixed phases) are oriented parallel to the surfaces for the considered case of morphologies unfrustrated by the film thickness. Structures with connections between parallel layers (bicontinuous, etc.) are not formed. As a result of surface-induced ordering, the region of ordered phases in a film is wider than in bulk and the phase boundary between ordered and disordered phases is more diffuse. As in the case of unconfined block polyelectrolyte solution, the solution in a film does not follow the lyotropic sequence of phases of such a block copolymer upon increase in the charge of the polyelectrolyte block. Upon changing the charge of the solvophilic copolymer block, transformations of copolymer morphology take place via change in curvature of polymeric domains. Due to confinement of a polyelectrolyte film, no swelling of solvophilic domains is observed.
采用平均场动态密度泛函理论来描述薄膜中弱电荷柔性嵌段聚电解质浓溶液的相图。通过应用局部电中性约束(唐南膜平衡方法)来考虑静电作用。在唐南极限情况下,假定添加到溶液中的盐能完美屏蔽长程静电相互作用。对于给定的薄膜厚度,计算了三嵌段聚电解质溶液在薄膜中的相图,该相图是溶剂浓度和聚电解质(亲溶剂)嵌段电荷的函数。嵌段聚电解质薄膜的相行为源于表面诱导排列与静电驱动结构形成之间的相互作用。在所考虑的形态未受薄膜厚度阻碍的情况下,观察到的介观结构(层状、穿孔层状、柱状、胶束状和混合相)与表面平行排列。未形成平行层之间有连接的结构(双连续等)。由于表面诱导有序化,薄膜中有序相的区域比本体中的更宽,有序相和无序相之间的相界更弥散。与无约束嵌段聚电解质溶液的情况一样,随着聚电解质嵌段电荷的增加,薄膜中的溶液并不遵循此类嵌段共聚物的溶致相序列。改变亲溶剂共聚物嵌段的电荷时,共聚物形态的转变通过聚合物域曲率的变化发生。由于聚电解质薄膜的限制,未观察到亲溶剂域的溶胀。