Deep glassy state dynamic data challenge glass models: Elastic models
There is increasing experimental evidence that suggests that the dynamics of glass forming liquids do not diverge at finite temperature above zero Kelvin, at the same time there has been recent progress in the development of non-diverging glass transition models. In this work we examine two non-dive...
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doaj-45bcbd95bb314984817ae1f6bccac5b42021-10-01T05:10:51ZengElsevierJournal of Non-Crystalline Solids: X2590-15912021-09-0111100068Deep glassy state dynamic data challenge glass models: Elastic modelsDongjie Chen0Gregory B. McKenna1Department of Chemical Engineering, Texas Tech University, Lubbock, TX 79409, United States of AmericaDepartment of Chemical Engineering, Texas Tech University, Lubbock, TX 79409, United States of America; Department of Chemical and Biomolecular Engineering, North Carolina State University, Raleigh, NC 27695, United States of America; Corresponding author at: Department of Chemical Engineering, Texas Tech University, Lubbock, TX 79409, United States of America.There is increasing experimental evidence that suggests that the dynamics of glass forming liquids do not diverge at finite temperature above zero Kelvin, at the same time there has been recent progress in the development of non-diverging glass transition models. In this work we examine two non-diverging models: the elastically collective nonlinear Langevin equation theory (ECNLE) and the shoving model, both of which relate an energy barrier in the glass formation process with elastic motion at small scales. The models are evaluated in comparison with the non-diverging dynamic data obtained in the deep glassy state (very stable) for a 20-million-year-old (20 Ma) ancient amber and for a vapor deposited amorphous Teflon obtained previously. We find that although both models are in qualitative agreement with the dynamic data for the two stable glasses, they still overestimate the actual relaxation times for the deep glassy state below the nominal glass transition temperature and for conditions corresponding to the equilibrium state or in a state in which the glass relaxation times are upper bounds to the equilibrium values.http://www.sciencedirect.com/science/article/pii/S2590159121000091Glass transitionDiverging time-scalesNon-diverging time-scalesECNLE modelShoving modelGlass dynamics |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Dongjie Chen Gregory B. McKenna |
spellingShingle |
Dongjie Chen Gregory B. McKenna Deep glassy state dynamic data challenge glass models: Elastic models Journal of Non-Crystalline Solids: X Glass transition Diverging time-scales Non-diverging time-scales ECNLE model Shoving model Glass dynamics |
author_facet |
Dongjie Chen Gregory B. McKenna |
author_sort |
Dongjie Chen |
title |
Deep glassy state dynamic data challenge glass models: Elastic models |
title_short |
Deep glassy state dynamic data challenge glass models: Elastic models |
title_full |
Deep glassy state dynamic data challenge glass models: Elastic models |
title_fullStr |
Deep glassy state dynamic data challenge glass models: Elastic models |
title_full_unstemmed |
Deep glassy state dynamic data challenge glass models: Elastic models |
title_sort |
deep glassy state dynamic data challenge glass models: elastic models |
publisher |
Elsevier |
series |
Journal of Non-Crystalline Solids: X |
issn |
2590-1591 |
publishDate |
2021-09-01 |
description |
There is increasing experimental evidence that suggests that the dynamics of glass forming liquids do not diverge at finite temperature above zero Kelvin, at the same time there has been recent progress in the development of non-diverging glass transition models. In this work we examine two non-diverging models: the elastically collective nonlinear Langevin equation theory (ECNLE) and the shoving model, both of which relate an energy barrier in the glass formation process with elastic motion at small scales. The models are evaluated in comparison with the non-diverging dynamic data obtained in the deep glassy state (very stable) for a 20-million-year-old (20 Ma) ancient amber and for a vapor deposited amorphous Teflon obtained previously. We find that although both models are in qualitative agreement with the dynamic data for the two stable glasses, they still overestimate the actual relaxation times for the deep glassy state below the nominal glass transition temperature and for conditions corresponding to the equilibrium state or in a state in which the glass relaxation times are upper bounds to the equilibrium values. |
topic |
Glass transition Diverging time-scales Non-diverging time-scales ECNLE model Shoving model Glass dynamics |
url |
http://www.sciencedirect.com/science/article/pii/S2590159121000091 |
work_keys_str_mv |
AT dongjiechen deepglassystatedynamicdatachallengeglassmodelselasticmodels AT gregorybmckenna deepglassystatedynamicdatachallengeglassmodelselasticmodels |
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1716862081112735744 |