Schmid Friederike, Li Bing
Institut für Physik, Johannes Gutenberg-Universität Mainz, D 55099 Mainz, Germany.
Polymers (Basel). 2020 Sep 25;12(10):2205. doi: 10.3390/polym12102205.
The self-consistent field theory is a popular and highly successful theoretical framework for studying equilibrium (co)polymer systems at the mesoscopic level. Dynamic density functionals allow one to use this framework for studying dynamical processes in the diffusive, non-inertial regime. The central quantity in these approaches is the mobility function, which describes the effect of chain connectivity on the nonlocal response of monomers to thermodynamic driving fields. In a recent study, one of us and coworkers have developed a method to systematically construct mobility functions from reference fine-grained simulations. Here we focus on melts of linear chains in the Rouse regime and show how the mobility functions can be calculated semi-analytically for multiblock copolymers with arbitrary sequences without resorting to simulations. In this context, an accurate approximate expression for the single-chain dynamic structure factor is derived. Several limiting regimes are discussed. Then we apply the resulting density functional theory to study ordering processes in a two-length scale block copolymer system after instantaneous quenches into the ordered phase. Different dynamical regimes in the ordering process are identified: at early times, the ordering on short scales dominates; at late times, the ordering on larger scales takes over. For large quench depths, the system does not necessarily relax into the true equilibrium state. Our density functional approach could be used for the computer-assisted design of quenching protocols in order to create novel nonequilibrium materials.
自洽场理论是一种流行且非常成功的理论框架,用于在介观层面研究平衡(共)聚物体系。动态密度泛函使人们能够将该框架用于研究扩散、非惯性区域中的动力学过程。这些方法的核心量是迁移率函数,它描述了链连接性对单体对热力学驱动场的非局部响应的影响。在最近的一项研究中,我们中的一人及同事开发了一种从参考细粒度模拟中系统构建迁移率函数的方法。在此,我们关注Rouse区域中线性链的熔体,并展示如何在不借助模拟的情况下,对具有任意序列的多嵌段共聚物半解析地计算迁移率函数。在这种情况下,推导了单链动态结构因子的精确近似表达式。讨论了几种极限情况。然后,我们应用所得的密度泛函理论来研究两长度尺度嵌段共聚物体系在瞬间淬火进入有序相后的有序化过程。确定了有序化过程中的不同动力学区域:在早期,短尺度上的有序化占主导;在后期,更大尺度上的有序化占主导。对于大的淬火深度,系统不一定会弛豫到真正的平衡态。我们的密度泛函方法可用于计算机辅助设计淬火方案,以创造新型非平衡材料。