Creep behavior of a Twaron®/natural rubber composite
The creep behavior of a Twaron CT709® fabric/natural rubber composite under a uniaxial constant stress is studied using three viscoelasticity models with different levels of complexity and a newly developed para-rheological model. The three models employed are a one-term generalized Maxwell (GM n=1)...
Published in: | ASME International Mechanical Engineering Congress and Exposition, Proceedings (IMECE) |
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American Society of Mechanical Engineers (ASME)
2010
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2-s2.0-84881395259 David N.V.; Gao X.-L.; Zheng J.Q. Creep behavior of a Twaron®/natural rubber composite 2010 ASME International Mechanical Engineering Congress and Exposition, Proceedings (IMECE) 9 10.1115/IMECE2010-38079 https://www.scopus.com/inward/record.uri?eid=2-s2.0-84881395259&doi=10.1115%2fIMECE2010-38079&partnerID=40&md5=e1162a8a40d8e51a9225312d86223e0f The creep behavior of a Twaron CT709® fabric/natural rubber composite under a uniaxial constant stress is studied using three viscoelasticity models with different levels of complexity and a newly developed para-rheological model. The three models employed are a one-term generalized Maxwell (GM n=1) model (consisting of one Maxwell element and an additional spring in parallel), a two-term generalized Maxwell (GMn=2) model (including two parallel Maxwell elements and an additional spring in parallel), and a four-parameter Burgers model. The values of the parameters involved in each model are extracted from the experimental data obtained in this study. The creep tests reveal that the axial strain starts to increase exponentially during the primary stage and then continues to equilibrate linearly with time. The results show that the initial creep response of the composite is predicted fairly well by the GMn=2 model, while the secondary creep is more accurately described by the GMn=1 model. An implicit solution, together with a characteristic retardation time spectrum, obtained using the para-rheological model is found to provide more accurate predictions of the composite creep response than the three viscoelasticity models at both the primary and secondary stages. Copyright © 2010 by ASME. American Society of Mechanical Engineers (ASME) English Conference paper |
author |
David N.V.; Gao X.-L.; Zheng J.Q. |
spellingShingle |
David N.V.; Gao X.-L.; Zheng J.Q. Creep behavior of a Twaron®/natural rubber composite |
author_facet |
David N.V.; Gao X.-L.; Zheng J.Q. |
author_sort |
David N.V.; Gao X.-L.; Zheng J.Q. |
title |
Creep behavior of a Twaron®/natural rubber composite |
title_short |
Creep behavior of a Twaron®/natural rubber composite |
title_full |
Creep behavior of a Twaron®/natural rubber composite |
title_fullStr |
Creep behavior of a Twaron®/natural rubber composite |
title_full_unstemmed |
Creep behavior of a Twaron®/natural rubber composite |
title_sort |
Creep behavior of a Twaron®/natural rubber composite |
publishDate |
2010 |
container_title |
ASME International Mechanical Engineering Congress and Exposition, Proceedings (IMECE) |
container_volume |
9 |
container_issue |
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doi_str_mv |
10.1115/IMECE2010-38079 |
url |
https://www.scopus.com/inward/record.uri?eid=2-s2.0-84881395259&doi=10.1115%2fIMECE2010-38079&partnerID=40&md5=e1162a8a40d8e51a9225312d86223e0f |
description |
The creep behavior of a Twaron CT709® fabric/natural rubber composite under a uniaxial constant stress is studied using three viscoelasticity models with different levels of complexity and a newly developed para-rheological model. The three models employed are a one-term generalized Maxwell (GM n=1) model (consisting of one Maxwell element and an additional spring in parallel), a two-term generalized Maxwell (GMn=2) model (including two parallel Maxwell elements and an additional spring in parallel), and a four-parameter Burgers model. The values of the parameters involved in each model are extracted from the experimental data obtained in this study. The creep tests reveal that the axial strain starts to increase exponentially during the primary stage and then continues to equilibrate linearly with time. The results show that the initial creep response of the composite is predicted fairly well by the GMn=2 model, while the secondary creep is more accurately described by the GMn=1 model. An implicit solution, together with a characteristic retardation time spectrum, obtained using the para-rheological model is found to provide more accurate predictions of the composite creep response than the three viscoelasticity models at both the primary and secondary stages. Copyright © 2010 by ASME. |
publisher |
American Society of Mechanical Engineers (ASME) |
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language |
English |
format |
Conference paper |
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scopus |
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Scopus |
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1809678162082136064 |