Wang Yongmei
Department of Chemistry, The University of Memphis, Memphis, Tennessee 38152-3550, USA.
J Chem Phys. 2004 Aug 22;121(8):3898-904. doi: 10.1063/1.1777222.
Lattice Monte Carlo simulations of polymer solutions confined between two parallel plates were performed. The confinement free energy Deltamicro(conf) per chain and the radius of gyrations of the chains parallel and perpendicular to the plates were obtained. When the concentration of the confined solution is above the overlap concentration, Deltamicro(conf) is found to scale with Na/D in a power law, betaDeltamicro(conf) approximately (Na/D)(m), with an exponent m=1.10+/-0.02 for athermal walls where N is the number of monomers in a chain, D is the slit width, and a is the lattice spacing. The presence of a weak attractive polymer/wall interaction epsilon(w) does not change the scaling variable, but the exponent m increases slightly. Extrapolating the results to melt would suggest that the predictions made by de Gennes [C. R. Acad. Sci. Paris II 305, 1181 (1987)] about the confinement free energy cost per chain in polymer melt is correct as far as the scaling variable is concerned, but is incorrect about the exponent m observed. The implication of this result on the predicted force between plates immersed in polymer melt is discussed. The parallel dimensions of the confined chain is expanded when the slit width D is narrow, however, the expansion is reduced at high concentration. It is conceivable that in melt the chain is not expanded when confined in a repulsive slit.
对限制在两个平行板之间的聚合物溶液进行了格子蒙特卡罗模拟。得到了每条链的限制自由能Δμ(conf)以及平行于和垂直于平板的链的回转半径。当受限溶液的浓度高于重叠浓度时,发现Δμ(conf)与Na/D呈幂律关系,βΔμ(conf)≈(Na/D)^m,对于无热壁,指数m = 1.10±0.02,其中N是链中单体的数量,D是狭缝宽度,a是晶格间距。弱吸引性聚合物/壁相互作用ε(w)的存在不会改变标度变量,但指数m会略有增加。将结果外推到熔体表明,就标度变量而言,德热纳 [《法国科学院院报》II 305, 1181 (1987)] 对聚合物熔体中每条链的限制自由能成本的预测是正确的,但观察到的指数m是不正确的。讨论了这一结果对浸入聚合物熔体中的平板间预测力的影响。当狭缝宽度D较窄时,受限链的平行尺寸会增大,然而,在高浓度下这种增大减小。可以想象,在熔体中,当链被限制在排斥性狭缝中时不会增大。