We present a kinetic model of crystal growth of polymers of finite molecularweight. Experiments help to classify polymer crystallization broadly into twokinetic regimes. One is observed in melts or in high molar mass polymersolutions and is dominated by nucleation control with $G \sim \exp(1/T \DeltaT)$, where $G$ is the growth rate and $\Delta T$ is the super-cooling. Theother is observed in low molar mass solutions (as well as for small molecules)and is diffusion controlled with $G \sim \Delta T$, for small $\Delta T$. Ourmodel unifies these two regimes in a single formalism. The model accounts forthe accumulation of polymer chains near the growth front and invokes anentropic barrier theory to recover both limits of nucleation and diffusioncontrol. The basic theory applies to both melts and solutions, and wenumerically calculate the growth details of a single crystal in a dilutesolution. The effects of molecular weight and concentration are also determinedconsidering conventional polymer dynamics. Our theory shows that entropicconsiderations, in addition to the traditional energetic arguments, can capturegeneral trends of a vast range of phenomenology. Unifying ideas oncrystallization from small molecules and from flexible polymer chains emergefrom our theory.
展开▼
机译:我们提出了有限分子量聚合物晶体生长的动力学模型。实验有助于将聚合物结晶大致分为两种动力学形式。在熔体或高摩尔质量的聚合物溶液中观察到一种,并以$ G \ sim \ exp(1 / T \ DeltaT)$进行成核控制,其中$ G $是增长率,$ \ Delta T $是超级-冷却。另一个在低摩尔质量溶液(以及小分子溶液)中观察到,并且受$ G \ sim \ Delta T $的扩散控制,对于$$ \ Delta T $的扩散。我们的模型将这两种制度统一在一个形式主义中。该模型说明了聚合物链在生长前沿附近的积累,并调用了熵垒理论来恢复成核和扩散控制的极限。基本理论适用于熔体和溶液,并通过数值计算单晶体在稀溶液中的生长细节。还考虑常规的聚合物动力学来确定分子量和浓度的影响。我们的理论表明,除了传统的精力充沛的论点之外,熵思考还可以捕捉到各种现象学的一般趋势。从小分子和柔性聚合物链中结晶的统一思想源于我们的理论。
展开▼