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Mixed equilibrium/nonequilibrium effects govern surface mobility in polymer glasses.
Xu, Jianquan; Ghanekarade, Asieh; Li, Li; Zhu, Huifeng; Yuan, Hailin; Yan, Jinsong; Simmons, David S; Tsui, Ophelia K C; Wang, Xinping.
Affiliation
  • Xu J; School of Chemistry and Chemical Engineering, Key Laboratory of Surface & Interface Science of Polymer Materials of Zhejiang Province, Zhejiang Sci-Tech University, Hangzhou 310018, China.
  • Ghanekarade A; Department of Chemical, Biological, and Materials Engineering, University of South Florida, Tampa, FL 33620.
  • Li L; School of Chemistry and Chemical Engineering, Key Laboratory of Surface & Interface Science of Polymer Materials of Zhejiang Province, Zhejiang Sci-Tech University, Hangzhou 310018, China.
  • Zhu H; School of Chemistry and Chemical Engineering, Key Laboratory of Surface & Interface Science of Polymer Materials of Zhejiang Province, Zhejiang Sci-Tech University, Hangzhou 310018, China.
  • Yuan H; Department of Physics, Hong Kong University of Science and Technology, Hong Kong Special Administrative Region 999077, China.
  • Yan J; Department of Physics, Hong Kong University of Science and Technology, Hong Kong Special Administrative Region 999077, China.
  • Simmons DS; Department of Chemical, Biological, and Materials Engineering, University of South Florida, Tampa, FL 33620.
  • Tsui OKC; Department of Physics, Hong Kong University of Science and Technology, Hong Kong Special Administrative Region 999077, China.
  • Wang X; William Mong Institute of Nano Science and Technology, Hong Kong University of Science and Technology, Hong Kong Special Administrative Region 999077, China.
Proc Natl Acad Sci U S A ; 121(41): e2406262121, 2024 Oct 08.
Article in En | MEDLINE | ID: mdl-39361647
ABSTRACT
Using angle-resolved X-ray photoelectron spectroscopy, sum-frequency generation vibrational spectroscopy, contact angle measurements, and molecular dynamics simulations, we verify that the glass transition temperature (Tg) of polymer glass is lower near the free surface. However, the experimental Tg-gradients showed a linear variation with depth (z) from the free surface, while the simulated equilibrium Tg-gradients exhibited a double exponential z-dependence. In typical simulations, Tg is determined based on the relaxation time of the system reaching a prescribed threshold value at equilibrium. Conversely, the experiments determined Tg by observing the unfreezing of molecular mobility during heating from a kinetically arrested, nonequilibrium glassy state. To investigate the impact of nonequilibrium effects on the Tg-gradient, we reduced the thermal annealing time in simulations, allowing the system to fall out of equilibrium. We observe a decrease in the relaxation time and the emergence of a modified z-dependence consistent with a linear Tg-gradient near the free surface. We further validate the impact of nonequilibrium effects by studying the dependence of the Tg on the heating/cooling rate for polymer films of varying thickness (h). Our experimental results reveal significant variations in the Tg-heating/cooling rate dependence with h below the bulk Tg, which are also observed in simulation when the simulated system is not equilibrated. We explain our findings by the reduction in mass density within the inner region of the system under nonequilibrium conditions, as observed in simulation, and recent research indicating a decrease in the local Tg of a polymer when placed next to a softer material.
Key words

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Proc Natl Acad Sci U S A Year: 2024 Document type: Article Affiliation country: China Country of publication: United States

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Proc Natl Acad Sci U S A Year: 2024 Document type: Article Affiliation country: China Country of publication: United States