Gindy Marian E, Prud'homme Robert K, Panagiotopoulos Athanassios Z
Department of Chemical Engineering, Princeton University, Princeton, New Jersey 08544 USA.
J Chem Phys. 2008 Apr 28;128(16):164906. doi: 10.1063/1.2905231.
The solution phase behavior of short, strictly alternating multiblock copolymers of type (A(n)B(n))(m) was studied using lattice Monte Carlo simulations. The polymer molecules were modeled as flexible chains in a monomeric solvent selective for block type A. The degree of block polymerization n and the number of diblock units per chain m were treated as variables. We show that within the regime of parameters accessible to our study, the thermodynamic phase transition type is dependent on the ratio of m / n. The simulations show microscopic phase separation into roughly spherical aggregates for m / n ratios less than a critical value and first-order macroscopic precipitation otherwise. In general, increasing m at fixed n, or n at fixed m, promotes the tendency toward macroscopic phase precipitation. The enthalpic driving force of phase change is found to universally scale with chain length for all multiblock systems considered and is independent of the existence of a true phase transition. For aggregate forming systems at low amphiphile concentrations, multiblock chains are shown to self-assemble into intramolecular, multichain clusters. Predictions for microstructural dimensions, including critical micelle concentration, equilibrium size, shape, aggregation parameters, and density distributions, are provided. At increasing amphiphile density, interaggregate bridging is shown to result in the formation of networked structures, leading to an eventual solution-gel transition. The gel is swollen and consists of highly interconnected aggregates of approximately spherical morphology. Qualitative agreement is found between experimentally observed physical property changes and phase transitions predicted by simulations. Thus, a potential application of the simulations is the design of multiblock copolymer systems which can be optimized with regard to solution phase behavior and ultimately physical and mechanical properties.
利用晶格蒙特卡罗模拟研究了(A(n)B(n))(m)型短链、严格交替多嵌段共聚物的溶液相行为。聚合物分子被建模为在对A嵌段具有选择性的单体溶剂中的柔性链。将嵌段聚合度n和每条链中二嵌段单元的数量m视为变量。我们表明,在我们研究可及的参数范围内,热力学相变类型取决于m/n的比值。模拟显示,当m/n比值小于临界值时,微观上相分离成大致球形的聚集体,否则为一级宏观沉淀。一般来说,在固定n时增加m,或在固定m时增加n,会促进宏观相沉淀的趋势。发现所有考虑的多嵌段体系中,相变的焓驱动力普遍与链长成比例,且与真正相变的存在无关。对于低两亲物浓度下形成聚集体的体系,多嵌段链显示会自组装成分子内的多链簇。给出了包括临界胶束浓度、平衡尺寸、形状、聚集参数和密度分布等微观结构尺寸的预测。在两亲物密度增加时,聚集体间的桥连显示会导致网络结构的形成,最终导致溶液-凝胶转变。凝胶是膨胀的,由近似球形形态的高度互连聚集体组成。实验观察到的物理性质变化与模拟预测的相变之间存在定性一致。因此,模拟的一个潜在应用是设计多嵌段共聚物体系,该体系可针对溶液相行为以及最终的物理和机械性能进行优化。