Sgouros Aristotelis P, Revelas Constantinos J, Lakkas Apostolos T, Theodorou Doros N
School of Chemical Engineering, National Technical University of Athens (NTUA), GR-15780 Athens, Greece.
J Phys Chem B. 2022 Sep 29;126(38):7454-7474. doi: 10.1021/acs.jpcb.2c05306. Epub 2022 Sep 15.
Predicting the distribution of a chemical species across multiple phases is of critical importance to environmental protection, pharmaceuticals, and high added-value chemicals. Computationally, this problem is addressed by determining the free energy of solvation of the species in the different phases using a well-established thermodynamic formulation. Following recent developments in sterically stabilized colloids and nanocomposite materials, the solvation of polymer-grafted nanoparticles in different solvents or polymer melts has become relevant. We develop a Self-Consistent Field theoretical framework to determine the solvation free energy of grafted particles inside a molten polymer matrix phase at low concentrations. The solvation free energy is calculated based on the notion of a pseudochemical potential introduced by Ben-Naim. Grafted and matrix chains are taken to be of the same chemical constitution, but their lengths are varied systematically, as are the particle radius and the areal density of grafted chains. In addition, different affinities between the nanoparticle core and the polymer (contact angles) are considered. At very low or very high amounts of grafted material, solvation depends on the adhesion tension between the bare particle and the matrix or on the surface tension of the grafted polymer, respectively. The dependence of the solvation free energy on molecular characteristics is more complicated at intermediate grafting densities and high curvatures, where the contribution of the entropy of grafted chains becomes significant. In general, solvation is less favored in cases where the matrix chains are much shorter than the grafted ones. The former tend to penetrate and swell the brush, thus generating conformational and translational entropy penalties. This effect becomes more pronounced when considering large particles since the grafted chains have less available space and extend more. For extremely low amounts of grafted material, we observe the opposite trend, albeit weak. Based on our calculations, we propose a generic model for estimating the solvation free energies of grafted nanoparticles in polymer melts from their molecular characteristics. The model and associated SCF formulation, illustrated here for chemically identical grafted and matrix chains, can be extended to obtain partition coefficients of grafted nanoparticles between different polymer melts.
预测化学物质在多个相之间的分布对于环境保护、制药和高附加值化学品至关重要。从计算角度来看,这个问题是通过使用成熟的热力学公式来确定该物质在不同相中的溶剂化自由能来解决的。随着空间稳定胶体和纳米复合材料的最新发展,聚合物接枝纳米颗粒在不同溶剂或聚合物熔体中的溶剂化变得具有重要意义。我们开发了一个自洽场理论框架,以确定低浓度下熔融聚合物基质相中接枝颗粒的溶剂化自由能。溶剂化自由能是基于Ben-Naim引入的伪化学势的概念来计算的。接枝链和基质链被认为具有相同的化学组成,但它们的长度会系统地变化,接枝链的颗粒半径和面积密度也会变化。此外,还考虑了纳米颗粒核心与聚合物之间的不同亲和力(接触角)。在接枝材料含量非常低或非常高时,溶剂化分别取决于裸颗粒与基质之间的粘附张力或接枝聚合物的表面张力。在中等接枝密度和高曲率下,溶剂化自由能对分子特征的依赖性更为复杂,此时接枝链的熵贡献变得显著。一般来说,当基质链比接枝链短得多时,溶剂化不太有利。前者倾向于穿透并使刷状结构膨胀,从而产生构象和平动熵惩罚。当考虑大颗粒时,这种效应会变得更加明显,因为接枝链的可用空间更少且伸展得更多。对于极低含量的接枝材料,我们观察到相反的趋势,尽管很微弱。基于我们的计算,我们提出了一个通用模型,用于根据接枝纳米颗粒的分子特征估算其在聚合物熔体中的溶剂化自由能。这里针对化学性质相同的接枝链和基质链说明的模型及相关的自洽场公式可以扩展,以获得接枝纳米颗粒在不同聚合物熔体之间的分配系数。