The Relationship between Free Volume and Cooperative Rearrangement: From the Temperature-Dependent Neutron Total Scattering Experiment of Polystyrene

Although many theories have been proposed to describe the nature of glass formation, its microscopic picture is still missing. Here, by a combination of neutron scattering and molecular dynamics simulation, we present the temperature-dependent atomic structure variation of polystyrene at the glass f...

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Main Authors: Zehua Han, Guisheng Jiao, Changli Ma, Taisen Zuo, Charles C. Han, He Cheng
Format: Article
Language:English
Published: MDPI AG 2021-09-01
Series:Polymers
Subjects:
Online Access:https://www.mdpi.com/2073-4360/13/18/3042
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spelling doaj-76db3348109142099fccdfc6067372d92021-09-26T01:00:45ZengMDPI AGPolymers2073-43602021-09-01133042304210.3390/polym13183042The Relationship between Free Volume and Cooperative Rearrangement: From the Temperature-Dependent Neutron Total Scattering Experiment of PolystyreneZehua Han0Guisheng Jiao1Changli Ma2Taisen Zuo3Charles C. Han4He Cheng5Spallation Neutron Source Science Center, Dongguan 523808, ChinaShenzhen Key Laboratory of Polymer Science and Technology, Guangdong Research Center for Interfacial Engineering of Functional Materials, College of Materials Science and Engineering, Shenzhen University, Shenzhen 518055, ChinaSpallation Neutron Source Science Center, Dongguan 523808, ChinaSpallation Neutron Source Science Center, Dongguan 523808, ChinaInstitute for Advanced Study, Shenzhen University, Shenzhen 508060, ChinaSpallation Neutron Source Science Center, Dongguan 523808, ChinaAlthough many theories have been proposed to describe the nature of glass formation, its microscopic picture is still missing. Here, by a combination of neutron scattering and molecular dynamics simulation, we present the temperature-dependent atomic structure variation of polystyrene at the glass formation, free volume and cooperative rearrangement. When it is close to glass formation, the polymer is confined in tubes, whose diameter is the main chain–main chain distance, in a “static cage” from its neighbors. This definition can not only account for the kinetic pathway dependence of Williams-Landel-Ferry (WLF) free volume, but also be testified in a set of six polymers. However, the free volume which allows a monomer to move cannot be found in any frame of its real-space image. Monomers, thus, have to move cooperatively to be out of the cage. During glass formation, dynamic heterogeneity develops, and string-like cooperative rearrangement region (CRR) grows over a long range of time and length scales. All of these CRRs tend to walk through loose “static cages”. Our observation unifies the concepts of free volume and cooperative rearrangement. The former is a statistical average leading to a polydisperse “static cage” formation; while a loose “static cage” provides the way that CRRs move.https://www.mdpi.com/2073-4360/13/18/3042glass formationneutron scatteringmolecular dynamic simulationfree volumecooperative rearrangement
collection DOAJ
language English
format Article
sources DOAJ
author Zehua Han
Guisheng Jiao
Changli Ma
Taisen Zuo
Charles C. Han
He Cheng
spellingShingle Zehua Han
Guisheng Jiao
Changli Ma
Taisen Zuo
Charles C. Han
He Cheng
The Relationship between Free Volume and Cooperative Rearrangement: From the Temperature-Dependent Neutron Total Scattering Experiment of Polystyrene
Polymers
glass formation
neutron scattering
molecular dynamic simulation
free volume
cooperative rearrangement
author_facet Zehua Han
Guisheng Jiao
Changli Ma
Taisen Zuo
Charles C. Han
He Cheng
author_sort Zehua Han
title The Relationship between Free Volume and Cooperative Rearrangement: From the Temperature-Dependent Neutron Total Scattering Experiment of Polystyrene
title_short The Relationship between Free Volume and Cooperative Rearrangement: From the Temperature-Dependent Neutron Total Scattering Experiment of Polystyrene
title_full The Relationship between Free Volume and Cooperative Rearrangement: From the Temperature-Dependent Neutron Total Scattering Experiment of Polystyrene
title_fullStr The Relationship between Free Volume and Cooperative Rearrangement: From the Temperature-Dependent Neutron Total Scattering Experiment of Polystyrene
title_full_unstemmed The Relationship between Free Volume and Cooperative Rearrangement: From the Temperature-Dependent Neutron Total Scattering Experiment of Polystyrene
title_sort relationship between free volume and cooperative rearrangement: from the temperature-dependent neutron total scattering experiment of polystyrene
publisher MDPI AG
series Polymers
issn 2073-4360
publishDate 2021-09-01
description Although many theories have been proposed to describe the nature of glass formation, its microscopic picture is still missing. Here, by a combination of neutron scattering and molecular dynamics simulation, we present the temperature-dependent atomic structure variation of polystyrene at the glass formation, free volume and cooperative rearrangement. When it is close to glass formation, the polymer is confined in tubes, whose diameter is the main chain–main chain distance, in a “static cage” from its neighbors. This definition can not only account for the kinetic pathway dependence of Williams-Landel-Ferry (WLF) free volume, but also be testified in a set of six polymers. However, the free volume which allows a monomer to move cannot be found in any frame of its real-space image. Monomers, thus, have to move cooperatively to be out of the cage. During glass formation, dynamic heterogeneity develops, and string-like cooperative rearrangement region (CRR) grows over a long range of time and length scales. All of these CRRs tend to walk through loose “static cages”. Our observation unifies the concepts of free volume and cooperative rearrangement. The former is a statistical average leading to a polydisperse “static cage” formation; while a loose “static cage” provides the way that CRRs move.
topic glass formation
neutron scattering
molecular dynamic simulation
free volume
cooperative rearrangement
url https://www.mdpi.com/2073-4360/13/18/3042
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