4.6 Article

Intrinsic structure and dynamics of monolayer ring polymer melts

Journal

SOFT MATTER
Volume 17, Issue 47, Pages 10703-10715

Publisher

ROYAL SOC CHEMISTRY
DOI: 10.1039/d1sm01192h

Keywords

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Funding

  1. National Research Foundation of Korea [2019R1A2C208799011, 2021R1F1A1057023]
  2. Ministry of Trade, Industry, and Energy of Korea [20010276]
  3. Korea Evaluation Institute of Industrial Technology (KEIT) [20010276] Funding Source: Korea Institute of Science & Technology Information (KISTI), National Science & Technology Information Service (NTIS)
  4. National Research Foundation of Korea [2021R1F1A1057023] Funding Source: Korea Institute of Science & Technology Information (KISTI), National Science & Technology Information Service (NTIS)

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In a narrowly confined two-dimensional melt system, the stiffness of ring polymers increases, leading to an overall extended interpenetrated chain configuration. Compared to 3D systems, 2D ring and linear melts exhibit relatively similar structural and dynamical properties due to similar chain structures, less effective chain ends, and absence of complex topological constraints.
We present the general structural and dynamical characteristics of flexible ring polymers in narrowly confined two-dimensional (2D) melt systems using atomistic molecular dynamics simulations. The results are further analyzed via direct comparison with the 2D linear analogue as well as the three-dimensional (3D) ring and linear melt systems. It is observed that dimensional restriction in 2D confined systems results in an increase in the intrinsic chain stiffness of the ring polymer. Fundamentally, this arises from an entropic penalty on polymer chains along with a reduction in the available chain configuration states in phase space and spatial choices for individual segmental walks. This feature in combination with the intermolecular interactions between neighboring ring chains leads to an overall extended interpenetrated chain configuration for the 2D ring melt. In contrast to the generally large differences in structural and dynamical properties between ring and linear polymers in 3D melt systems, relatively similar local-to-global chain structures and dynamics are observed for the 2D ring and linear melts. This is attributed to the general structural similarity (i.e., extended double-stranded chain conformations), the less effective role of the chain ends, and the absence of complex topological constraints between chains (i.e., interchain entanglement and mutual ring threading) in the 2D confined systems compared with the corresponding 3D bulk systems.

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