Sticky Rouse Time Features the Self-Adhesion of Supramolecular Polymer Networks
Sticky Rouse Time Features the Self-Adhesion of Supramolecular Polymer Networks
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DOI:
10.1021/acs.macromol.1c00335
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发表时间:
2021-05
期刊:
影响因子:
5.5
通讯作者:
Zhiqiang Shen;Huilin Ye;Qiming Wang;M. Kröger;Ying Li
中科院分区:
文献类型:
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作者:
Zhiqiang Shen;Huilin Ye;Qiming Wang;M. Kröger;Ying Li
Supramolecular polymers are fascinating materials due to their strikingly self-healing capabilities empowered by reversible bonds. However, due to the lack of knowledge about the molecular structure evolution at the fractured interfaces, there is no existing theory to explain and predict the diverse healing times of different supramolecular materials observed in experiments. Here, we systematically study the self-adhesion of both unentangled and entangled supramolecular polymer networks through molecular simulations. We find that the recovery of macroscopic interfacial strength almost linearly depends on the microscopic molecular formations at fractured interfaces of supramolecular polymers, including reversible bonds and entanglements (entangled systems only). More importantly, we place the healing time into the context of intrinsic relaxation timescales of supramolecular polymer networks. It is found that the intrinsic sticky Rouse time features the self-adhesion process of all fractured supramolecular polymers, representing the full recovery of interfacial strength. At this critical timescale, two things happened to guarantee the full recovery of fractured systems: (i) polymer chains have diffused across the fractured interface with a displacement comparable to their sizes; (ii) the crossed stickers and polymer chains have updated their reversible bonds and entanglements (entangled systems only), respectively. The clear molecular description and suggested characteristic self-adhesion time will help the molecular design of supramolecular polymers. ■ INTRODUCTION To mimic the self-repairing capability of human muscles and skins, numerous synthetic self-healable supramolecular polymers have been recently developed. The strikingly selfhealing properties of these polymers arise from reversible bonds (“r-bonds”) that cross-link polymer chains as a dynamic network. These r-bonds can autonomously reform after breaking or dissociation, which can be achieved through dynamic covalent bonds, hydrogen bonds, metal−ligand coordination, hydrophobic interactions, and ionic interactions. As a result of these r-bonds, supramolecular polymers can repair fracture or damage at the molecular or microscopic scale and restore their mechanical strength at the macroscopic scale. These polymers have been applied to a wide range of engineering applications, including flexible electronics, energy storage devices, biomaterials, soft robotics, and lattice structures. Considering their versatility, it is of paramount importance to study their required healing time and recovered interfacial strength for fractured supramolecular polymers. However, due to different r-bonds and polymer chains used in experiments, the reported characteristic healing times cover a wide range of values from a few seconds to a few days. For instance, Sitti and co-workers designed self-healing materials by programming biosynthetic proteins with tandem repeat peptides. These synthetic proteins can form a supramolecular network with flexible chains dynamically cross-linked by β-sheets. Through local heating above 43 °C near the fracture, their polypeptide materials can self-heal in a second with a mechanical strength of 2−23 MPa. Leibler and co-workers used fatty dimer acids to fabricate supramolecular material networking by hydrogen bonds between small molecules. The interfacial strength of their materials can recover to 2.5 MPa after a 6 h healing Received: February 11, 2021 Revised: May 5, 2021 Published: May 20, 2021 Article pubs.acs.org/Macromolecules © 2021 The Authors. Published by American Chemical Society 5053 https://doi.org/10.1021/acs.macromol.1c00335 Macromolecules 2021, 54, 5053−5064 D ow nl oa de d vi a 20 7. 15 1. 52 .1 65 o n Se pt em be r 28 , 2 02 1 at 1 9: 40 :4 5 (U T C ). Se e ht tp s: //p ub s. ac s. or g/ sh ar in gg ui de lin es f or o pt io ns o n ho w to le gi tim at el y sh ar e pu bl is he d ar tic le s.