The James Franck Institute, The University of Chicago, Chicago, Illinois 60637, USA.
J Chem Phys. 2012 Feb 14;136(6):064902. doi: 10.1063/1.3681257.
The lattice cluster theory (LCT) for the thermodynamics of a wide array of polymer systems has been developed by using an analogy to Mayer's virial expansions for non-ideal gases. However, the high-temperature expansion inherent to the LCT has heretofore precluded its application to systems exhibiting strong, specific "sticky" interactions. The present paper describes a reformulation of the LCT necessary to treat systems with both weak and strong, "sticky" interactions. This initial study concerns solutions of linear telechelic chains (with stickers at the chain ends) as the self-assembling system. The main idea behind this extension of the LCT lies in the extraction of terms associated with the strong interactions from the cluster expansion. The generalized LCT for sticky systems reduces to the quasi-chemical theory of hydrogen bonding of Panyioutou and Sanchez when correlation corrections are neglected in the LCT. A diagrammatic representation is employed to facilitate the evaluation of the corrections to the zeroth-order approximation from short range correlations.
晶格团簇理论(LCT)已被开发用于广泛的聚合物系统的热力学,其使用了与 Mayer 非理想气体的维里膨胀的类比。然而,LCT 固有的高温展开迄今为止排除了其在表现出强烈、特定的“粘性”相互作用的系统中的应用。本文描述了一种对 LCT 的重新表述,这对于处理具有弱和强“粘性”相互作用的系统是必要的。这项初步研究涉及作为自组装系统的线性遥爪链(在链末端带有粘性物)的溶液。这种 LCT 扩展背后的主要思想在于从团簇展开中提取与强相互作用相关的项。当在 LCT 中忽略相关修正时,粘性系统的广义 LCT 简化为 Panyioutou 和 Sanchez 的氢键准化学理论。采用图示表示法来促进从短程相关中评估对零阶近似的修正。