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)...

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Published in:ASME International Mechanical Engineering Congress and Exposition, Proceedings (IMECE)
Main Author: David N.V.; Gao X.-L.; Zheng J.Q.
Format: Conference paper
Language:English
Published: American Society of Mechanical Engineers (ASME) 2010
Online Access:https://www.scopus.com/inward/record.uri?eid=2-s2.0-84881395259&doi=10.1115%2fIMECE2010-38079&partnerID=40&md5=e1162a8a40d8e51a9225312d86223e0f
id 2-s2.0-84881395259
spelling 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
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)
issn
language English
format Conference paper
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