Sumi Tomonari, Kobayashi Kazuhiko, Sekino Hideo
Department of Knowledge-based Information Engineering, Toyohashi University of Technology, Tempaku-cho, Toyohashi 441-8580, Japan.
J Chem Phys. 2007 Oct 28;127(16):164904. doi: 10.1063/1.2793778.
The behavior of a polymer chain immersed in a binary solvent mixture is investigated via a single-polymer simulation using an effective Hamiltonian, where the solvent effects are taken into account through a density-functional theory for polymer-solvent admixtures. The liquid-liquid phase separation of the binary solvent mixture is modeled as that of a Lennard-Jones binary fluid mixture with weakly attractive interactions between the different components. Two types of energetic preferences of the polymer chain for the better solvent-(A) no preferential solvophilicity and (B) strong preferential solvophilicity-are employed as polymer-solvent interaction models. The radius of gyration and the polymer-solvent radial distribution functions are determined from the simulations of various molar fractions along an isotherm slightly above the critical temperature of the liquid-liquid phase separation. These quantities near the critical point conspicuously depend on the strength of the preferential solvophilicity. In the case where the polymer exhibits a strong preferential solvophilicity, a remarkable expansion of the polymer chain is observed near the critical point. On the other hand, in the case where the polymer has no preferential solvophilicity, no characteristic variation of the polymer conformation is observed even near the critical point. These results indicate that the expansion of a polymer chain enhances the local phase separation around it, acting as a nucleus of demixing in the vicinity of the critical point. This phenomenon in binary solvents near the liquid-liquid critical point is similar to the expansion of the polymer chain in one-component supercritical solvents near the liquid-vapor critical point, which we have reported [T. Sumi and H. Sekino J. Chem. Phys. 122, 194910 (2005)].
通过使用有效哈密顿量的单聚合物模拟,研究了浸入二元溶剂混合物中的聚合物链的行为,其中通过聚合物 - 溶剂混合物的密度泛函理论考虑溶剂效应。将二元溶剂混合物的液 - 液相分离模拟为具有不同组分之间弱吸引相互作用的 Lennard - Jones 二元流体混合物的相分离。聚合物链对良溶剂的两种能量偏好类型——(A)无优先亲溶剂性和(B)强优先亲溶剂性——被用作聚合物 - 溶剂相互作用模型。在略高于液 - 液相分离临界温度的等温线上,通过对各种摩尔分数的模拟确定了回转半径和聚合物 - 溶剂径向分布函数。临界点附近的这些量明显取决于优先亲溶剂性的强度。在聚合物表现出强优先亲溶剂性的情况下,在临界点附近观察到聚合物链的显著膨胀。另一方面,在聚合物没有优先亲溶剂性的情况下,即使在临界点附近也未观察到聚合物构象的特征变化。这些结果表明,聚合物链的膨胀增强了其周围的局部相分离,在临界点附近起到了混合核的作用。二元溶剂在液 - 液临界点附近的这种现象类似于我们之前报道的 [T. Sumi 和 H. Sekino J. Chem. Phys. 122, 194910 (2005)] 单组分超临界溶剂中聚合物链在液 - 气临界点附近的膨胀。