Centro de Química-Física Molecular and IN-Institute of Nanoscience and Nanotechnology, Instituto Superior Técnico , 1049-001 Lisboa, Portugal.
J Phys Chem B. 2014 Mar 20;118(11):3192-206. doi: 10.1021/jp408390t. Epub 2014 Mar 10.
We have synthesized anionic multistimuli responsive core-shell polymer nanoparticles with low size dispersity composed of glassy poly(methyl methacrylate) (PMMA) cores of ca. 40 nm radius and poly(N-isopropylacrylamide) (PNIPAM) anionic brush-like shells with methacrylic acid comonomers. Using dynamic light scattering, we observed a volume phase transition upon an increase in temperature and this response was pH and ionic strength dependent. Already at room temperature we observed a pronounced polyelectrolyte effect, that is, a shift of the apparent pKa extracted from the degree of dissociation of the acids as a function of the pH. The multiresponsive behavior of the hydrophobic polyelectrolyte brush has been modeled using the Scheutjens-Fleer self-consistent field (SF-SCF) approach. Using a phenomenological relation between the Flory-Huggins χ parameter and the temperature, we confront the predicted change in the brush height with the observed change of the hydrodynamic radius and degree of dissociation and obtain estimates for the average chain lengths (number of Kuhn segments) of the corona chains, the grafting density and charge density distributions. The theory reveals a rich internal structure of the hydrophobic polyelectrolyte brush, especially near the collapse transition, where we find a microphase segregated structure. Considering this complexity, it is fair to state that the theoretical predictions follow the experimental data semiquantitatively, and it is attractive to attribute the observed disparity between theory and experiments to the unknown polydispersity of the chains, the unknown distribution of the charges, or other experimental complications. More likely, however, the deviations point to significant problems of the mean field theory, which focuses solely on the radial distributions and ignores the possibility of the formation of lateral (local) inhomogeneities in partially collapsed polyelectrolyte brushes. We argue that the PNIPAM brush at room temperature is already behaving nonideally.
我们合成了具有低尺寸分散性的阴离子多刺激响应核壳聚合物纳米粒子,其由约 40nm 半径的玻璃态聚甲基丙烯酸甲酯 (PMMA) 核和带有甲基丙烯酸共聚单体的聚 (N-异丙基丙烯酰胺) (PNIPAM) 阴离子刷状壳组成。使用动态光散射,我们观察到温度升高时发生体积相转变,这种响应依赖于 pH 值和离子强度。即使在室温下,我们也观察到明显的聚电解质效应,即从酸的离解度提取的表观 pKa 值随 pH 值的变化而变化。使用 Scheutjens-Fleer 自洽场 (SF-SCF) 方法对疏水性聚电解质刷的多响应行为进行了建模。使用 Flory-Huggins χ 参数与温度之间的经验关系,我们将预测的刷高变化与观察到的水动力半径和离解度变化进行了对比,并获得了冠链的平均链长(Kuhn 段数)、接枝密度和电荷密度分布的估计值。该理论揭示了疏水性聚电解质刷的丰富内部结构,特别是在崩溃转变附近,我们发现了微相分离结构。考虑到这种复杂性,可以公平地说,理论预测与实验数据具有半定量的一致性,并且将观察到的理论与实验之间的差异归因于链的未知多分散性、电荷的未知分布或其他实验复杂性是合理的。然而,更有可能的是,偏差指向了平均场理论的重大问题,该理论仅关注径向分布,忽略了部分坍塌的聚电解质刷中形成横向(局部)不均匀性的可能性。我们认为,室温下的 PNIPAM 刷已经表现出非理想行为。