Stukalin Evgeny B, Cai Li-Heng, Kumar N Arun, Leibler Ludwik, Rubinstein Michael
Department of Chemistry, The University of North Carolina at Chapel Hill, Chapel Hill, NC 27599 USA.
Department of Chemistry, The University of North Carolina at Chapel Hill, Chapel Hill, NC 27599 USA ; Curriculum in Applied Sciences and Engineering, The University of North Carolina at Chapel Hill, Chapel Hill, NC 27599 USA.
Macromolecules. 2013 Sep 24;46(18). doi: 10.1021/ma401111n.
Self-healing polymeric materials are systems that after damage can revert to their original state with full or partial recovery of mechanical strength. Using scaling theory we study a simple model of autonomic self-healing of unentangled polymer networks. In this model one of the two end monomers of each polymer chain is fixed in space mimicking dangling chains attachment to a polymer network, while the sticky monomer at the other end of each chain can form pairwise reversible bond with the sticky end of another chain. We study the reaction kinetics of reversible bonds in this simple model and analyze the different stages in the self-repair process. The formation of bridges and the recovery of the material strength across the fractured interface during the healing period occur appreciably faster after shorter waiting time, during which the fractured surfaces are kept apart. We observe the slowest formation of bridges for self-adhesion after bringing into contact two bare surfaces with equilibrium (very low) density of open stickers in comparison with self-healing. The primary role of anomalous diffusion in material self-repair for short waiting times is established, while at long waiting times the recovery of bonds across fractured interface is due to hopping diffusion of stickers between different bonded partners. Acceleration in bridge formation for self-healing compared to self-adhesion is due to excess non-equilibrium concentration of open stickers. Full recovery of reversible bonds across fractured interface (formation of bridges) occurs after appreciably longer time than the equilibration time of the concentration of reversible bonds in the bulk.
自修复聚合物材料是一种在受损后能够恢复到原始状态,且机械强度能完全或部分恢复的系统。我们运用标度理论研究了一种非缠结聚合物网络自主自修复的简单模型。在该模型中,每条聚合物链的两个末端单体之一固定在空间中,模拟悬空链与聚合物网络的连接,而每条链另一端的粘性单体可以与另一条链的粘性末端形成成对的可逆键。我们研究了这个简单模型中可逆键的反应动力学,并分析了自修复过程中的不同阶段。在较短的等待时间后,愈合期间横跨断裂界面的桥接形成和材料强度的恢复明显加快,在此期间断裂表面保持分开。与自修复相比,当使两个具有平衡(非常低)密度的开放贴纸的裸露表面接触时,我们观察到自粘附的桥接形成最慢。确定了反常扩散在短等待时间内材料自修复中的主要作用,而在长等待时间时,横跨断裂界面的键的恢复是由于贴纸在不同键合伙伴之间的跳跃扩散。与自粘附相比,自修复中桥接形成的加速是由于开放贴纸的过量非平衡浓度。横跨断裂界面的可逆键的完全恢复(桥接的形成)发生的时间明显长于本体中可逆键浓度的平衡时间。