化学学报 ›› 2017, Vol. 75 ›› Issue (9): 884-892.DOI: 10.6023/A17050235 上一篇    下一篇

研究论文

环型嵌段高分子的强分凝理论方法

柳明, 杨颖梓, 邱枫   

  1. 复旦大学高分子科学系 聚合物分子工程国家重点实验室 上海 200433
  • 投稿日期:2017-05-29 发布日期:2017-08-07
  • 通讯作者: 杨颖梓 E-mail:yang_yingzi@fudan.edu.cn
  • 基金资助:

    国家自然科学基金(Nos.21320102005,21304020)资助.

A Strong Segregation Theory for Ring Block Copolymers

Liu Ming, Yang Yingzi, Qiu Feng   

  1. State Key Laboratory of Molecular Engineering of Polymers, Department of Macromolecular Science, Fudan University, Shanghai 200433
  • Received:2017-05-29 Published:2017-08-07
  • Contact: 10.6023/A17050235 E-mail:yang_yingzi@fudan.edu.cn
  • Supported by:

    Project supported by the National Natural Science Foundation of China (Nos. 21320102005, 21304020).

环型嵌段高分子没有自由端,分相结构会存在两种嵌段共混相区,使经典的线型嵌段高分子强分凝理论不能适用.在强分凝极限下,推导了两个共混相区之间的界面能,并结合两端固定在不同界面上的链的拉伸能,从而建立了环型嵌段高分子的强分凝理论研究方法.将此理论应用于环型两嵌段高分子体系,发现环型链比等链长的线型链更难相分离,且相结构周期远小于线型链.这与自洽场理论的结果一致.将此理论应用于环型三嵌段高分子,发现三元相图中心附近出现多种无共混相区的砖块堆积结构,而在靠近相图边缘部分,即组分比例较不对称时,含共混相区的层状和柱状结构占优势.

关键词: 强分凝理论, 强分凝极限, 环型嵌段高分子, 相图, 界面能

Due to the ring structure with no free ends, the traditional strong-segregation theory for linear chains is not adequate for ring block copolymers. We developed the strong-segregation theory for ring block copolymers (SST-ring), by modifying both the entropic free energy term and the interfacial energy term. The ring block copolymer can only form two types of conformations, i.e., the loops on one side of an interface and the bridges connecting two interfaces. For the entropic energy originating from the stretching of the chain conformation under strong-segregation limit, we employ the strategy for calculating the entropic energy of looping and bridging chains connecting interfaces. Since the mixing of components is unavoidable for the ring triblock copolymers to adapt to the classical morphologies, we start from the propagating function of the self-consistent field theory, and deduce the formula of the interfacial energy between two two-component domains under the strong-segregation limit. The formula is reminiscent to the interfacial energy between two single-component domains, except that the Flory-Huggins parameter χAB between two components on each side of the interface is replaced by an effective parameter, χeff, which is a function of the composite fractions and the Flory-Huggins parameters between each components. The application of SST-ring to ring diblock copolymers is successful to describe the decreased characteristic length and the lifted order-disorder transition point, compared with the corresponding linear diblock copolymers with the same segment number N. We find that the critical χABN value of the ordered-disordered transition is 1.59 times that of the linear diblock polymers, and the characteristic lengths of the ring diblock copolymers are always 0.63 times of those of linear diblock copolymers. This agrees qualitatively with the predictions of the self-consistent theory, with slight quantitative difference originating from the strong-segregation limit assumption. For the SST-ring calculations for ring triblock copolymers in two-dimensions, corresponding to the film with the thickness much smaller than the radius of gyration of the polymer, we consider two types of micro phase structures:the classical morphologies (lamellae and cylinders) with multi-component domains, and the tiling-brick structures ([6,6,6] and[8,8,4], where the numbers denote the side numbers of the bricks) consisting of the single-component domains. SST-ring predicts that the ternary diagram consists of both types of the micro phase structures. When the Flory-Huggins parameters between any two components are equal, the phase diagram has a three-fold rotational symmetry to the center of the regular triangle, and three mirror symmetric axis crossing three vertices of the triangle, respectively. Our SST-ring theory is easy to be applied to different morphologies of ring block copolymers.

Key words: strong segregation theory, strong segregation limit, ring block copolymers, phase diagram, interfacial energy