a.State Key Laboratory of Polymer Physics and Chemistry, Changchun Institute of Applied Chemistry, Chinese Academy of Sciences, Changchun 130022, China
b.University of Science and Technology of China, Hefei 230026, China
yylu@ciac.ac.cn
收稿:2022-02-24,
修回:2022-3-23,
录用:2022-3-26,
网络首发:2022-06-20,
纸质出版:2023-04-01
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Mo, J. Y.; Wang, Z. H.; Lu, Y. Y.; An, L. J. Size and dynamics of ring polymers under different topological constraints. Chinese J. Polym. Sci. 2023, 41, 516–524
Jiang-Yang Mo, Zhen-Hua Wang, Yu-Yuan Lu, et al. Size and Dynamics of Ring Polymers under Different Topological Constraints[J]. Chinese Journal of Polymer Science, 2023, 41(4): 516-524.
Mo, J. Y.; Wang, Z. H.; Lu, Y. Y.; An, L. J. Size and dynamics of ring polymers under different topological constraints. Chinese J. Polym. Sci. 2023, 41, 516–524 DOI: 10.1007/s10118-022-2743-z.
Jiang-Yang Mo, Zhen-Hua Wang, Yu-Yuan Lu, et al. Size and Dynamics of Ring Polymers under Different Topological Constraints[J]. Chinese Journal of Polymer Science, 2023, 41(4): 516-524. DOI: 10.1007/s10118-022-2743-z.
It is inappropriate to treat the unknotting constraint free energy of the ring chains in the melts as the free energy contributed by the excluded volume interactions of polymers in a good solvent. And the intrachain constraints have little influence on the scaling relationship between self-diffusion coefficient and chain length.
The impact of ring polymer length
N
and the influence of interchain and intrachain interactions on the size and dynamic behaviors of ring polymers
including the structural relaxation time
τ
R
and self-diffusion coefficient
D
remain poorly understood at present due to a lack of systematic studies with relatively large
N
values. This work addressed this issue by applying dynamic Monte Carlo simulations with independently tuned interchain and intrachain interactions to investigate the size and dynamics of the ring melts with chain lengths over a wide range of 0.2
N
e
≤
N
≤80
N
e
(
N
e
is the entanglement length of corresponding linear chains) under different topological constraints
including all-crossing and inter-crossing systems. We found that it was inappropriate to treat the unknotting constraint free energy of the ring chains in the melts as the free energy contributed by the excluded volume interactions of polymers in a good solvent. Scaling exponents of 2.5 and 1.5 reflecting the
N
-dependence of
τ
R
were obtained for long ring chains in non-crossing and intra-crossing systems
respectively
suggesting that the ring chains behaved as individual clusters and exhibited Zimm-like dynamics in intra-crossing systems. A single scaling exponent of −2 reflecting the
N
-dependence of
D
was obtained for ring chains in non-crossing and intra-crossing systems
indicating that the intrachain constraints affected only the value of
D
and had little influence on the scaling relationship between
D
and
N
. Furthermore
the extended Stokes-Einstein relation broke down for the ring chains in the non-crossing and intra-crossing systems because the structural relaxation and translational diffusion were decoupled for the short ring systems
while both the translational diffusion and rotational relaxations
as well as diffusion at short and long time scales
were decoupled for long ring systems.
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