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Cohesive zone length of metagabbro at supershear rupture velocity

We investigated the shear strain field ahead of a supershear rupture. The strain array data along the sliding fault surfaces were obtained during the large-scale biaxial friction experiments at the National Research Institute for Earth Science and Disaster Resilience. These friction experiments were...

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Autores principales: Fukuyama, Eiichi, Xu, Shiqing, Yamashita, Futoshi, Mizoguchi, Kazuo
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Springer Netherlands 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5270910/
https://www.ncbi.nlm.nih.gov/pubmed/28190969
http://dx.doi.org/10.1007/s10950-016-9588-2
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author Fukuyama, Eiichi
Xu, Shiqing
Yamashita, Futoshi
Mizoguchi, Kazuo
author_facet Fukuyama, Eiichi
Xu, Shiqing
Yamashita, Futoshi
Mizoguchi, Kazuo
author_sort Fukuyama, Eiichi
collection PubMed
description We investigated the shear strain field ahead of a supershear rupture. The strain array data along the sliding fault surfaces were obtained during the large-scale biaxial friction experiments at the National Research Institute for Earth Science and Disaster Resilience. These friction experiments were done using a pair of meter-scale metagabbro rock specimens whose simulated fault area was 1.5 m × 0.1 m. A 2.6-MPa normal stress was applied with loading velocity of 0.1 mm/s. Near-fault strain was measured by 32 two-component semiconductor strain gauges installed at an interval of 50 mm and 10 mm off the fault and recorded at an interval of 1 MHz. Many stick-slip events were observed in the experiments. We chose ten unilateral rupture events that propagated with supershear rupture velocity without preceding foreshocks. Focusing on the rupture front, stress concentration was observed and sharp stress drop occurred immediately inside the ruptured area. The temporal variation of strain array data is converted to the spatial variation of strain assuming a constant rupture velocity. We picked up the peak strain and zero-crossing strain locations to measure the cohesive zone length. By compiling the stick-slip event data, the cohesive zone length is about 50 mm although it scattered among the events. We could not see any systematic variation at the location but some dependence on the rupture velocity. The cohesive zone length decreases as the rupture velocity increases, especially larger than [Formula: see text] times the shear wave velocity. This feature is consistent with the theoretical prediction.
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spelling pubmed-52709102017-02-09 Cohesive zone length of metagabbro at supershear rupture velocity Fukuyama, Eiichi Xu, Shiqing Yamashita, Futoshi Mizoguchi, Kazuo J Seismol Original Article We investigated the shear strain field ahead of a supershear rupture. The strain array data along the sliding fault surfaces were obtained during the large-scale biaxial friction experiments at the National Research Institute for Earth Science and Disaster Resilience. These friction experiments were done using a pair of meter-scale metagabbro rock specimens whose simulated fault area was 1.5 m × 0.1 m. A 2.6-MPa normal stress was applied with loading velocity of 0.1 mm/s. Near-fault strain was measured by 32 two-component semiconductor strain gauges installed at an interval of 50 mm and 10 mm off the fault and recorded at an interval of 1 MHz. Many stick-slip events were observed in the experiments. We chose ten unilateral rupture events that propagated with supershear rupture velocity without preceding foreshocks. Focusing on the rupture front, stress concentration was observed and sharp stress drop occurred immediately inside the ruptured area. The temporal variation of strain array data is converted to the spatial variation of strain assuming a constant rupture velocity. We picked up the peak strain and zero-crossing strain locations to measure the cohesive zone length. By compiling the stick-slip event data, the cohesive zone length is about 50 mm although it scattered among the events. We could not see any systematic variation at the location but some dependence on the rupture velocity. The cohesive zone length decreases as the rupture velocity increases, especially larger than [Formula: see text] times the shear wave velocity. This feature is consistent with the theoretical prediction. Springer Netherlands 2016-06-02 2016 /pmc/articles/PMC5270910/ /pubmed/28190969 http://dx.doi.org/10.1007/s10950-016-9588-2 Text en © The Author(s) 2016 Open Access This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.
spellingShingle Original Article
Fukuyama, Eiichi
Xu, Shiqing
Yamashita, Futoshi
Mizoguchi, Kazuo
Cohesive zone length of metagabbro at supershear rupture velocity
title Cohesive zone length of metagabbro at supershear rupture velocity
title_full Cohesive zone length of metagabbro at supershear rupture velocity
title_fullStr Cohesive zone length of metagabbro at supershear rupture velocity
title_full_unstemmed Cohesive zone length of metagabbro at supershear rupture velocity
title_short Cohesive zone length of metagabbro at supershear rupture velocity
title_sort cohesive zone length of metagabbro at supershear rupture velocity
topic Original Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5270910/
https://www.ncbi.nlm.nih.gov/pubmed/28190969
http://dx.doi.org/10.1007/s10950-016-9588-2
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