Key Laboratory of High-Performance Synthetic Rubber and Its Composite Materials , Changchun Institute of Applied Chemistry (CIAC), Chinese Academy of Sciences , Changchun 130022 , P. R. China.
School of Materials , Sun Yat-Sen University , 135 Xingang West , Guangzhou 510275 , P. R. China.
J Phys Chem B. 2019 Apr 11;123(14):3086-3095. doi: 10.1021/acs.jpcb.9b01491. Epub 2019 Mar 27.
Water in polymer matrixes is likely to show anomalous dynamics, a problem that has not been well understood yet. Here, we performed atomistic molecular dynamics simulations to study the water dynamics in a polyamide (PA) matrix, the bulk phase of well-known reverse osmosis membranes. For time-dependent ensemble average, water molecules experienced ballistic diffusion at a shorter time scale, followed by a crossover from subdiffusion to Brownian diffusion at a time scale ∼10 ns, and non-Gaussian diffusion, an indication of anomalous dynamics, sticks on even in the Brownian diffusion region. The anomalous dynamics mainly originates from two distinct motions including small-step continuous diffusion and jumping diffusion. The jumping motion has a mean length of 3.08 ± 0.31 Å and characteristic relaxation time of 0.218 ± 0.040 ns, which dominates the water diffusion in a fully hydrated PA matrix. It comprised low- and high-frequency jumps; the former is almost unchanged, and the latter remarkably increases with the increase of the hydration level. Surrounding neighbors of water strongly affect the jumping frequency, which exponentially or linearly decays with the increase in the number of atoms from the PA matrix. Although the PA matrix is flexible, associated with the water dynamics, the translocation of water is mainly through either tracing the position of neighboring water or jumping into the adjacent accommodation space.
聚合物基体中的水可能表现出异常的动力学行为,这是一个尚未得到很好理解的问题。在这里,我们进行了原子分子动力学模拟,以研究聚酰胺(PA)基体中的水动力学,这是众所周知的反渗透膜的体相。对于时变系综平均,水分子在更短的时间尺度上经历弹道扩散,然后在 10 ns 的时间尺度上从亚扩散转变为布朗扩散,并且非高斯扩散,表明异常动力学,甚至在布朗扩散区域也保持不变。异常动力学主要源于两种不同的运动,包括小步连续扩散和跳跃扩散。跳跃运动的平均长度为 3.08 ± 0.31 Å,特征弛豫时间为 0.218 ± 0.040 ns,这主导了完全水合 PA 基体中的水扩散。它由低频率跳跃和高频率跳跃组成;前者几乎不变,后者随着水合度的增加而显著增加。水的周围邻居强烈影响跳跃频率,其随距 PA 基体中原子数的增加呈指数或线性衰减。尽管 PA 基体是柔性的,但与水动力学相关,水的迁移主要是通过跟踪相邻水分子的位置或跳跃到相邻的容纳空间。