Loading…
The seismic cycle at subduction thrusts: 2. Dynamic implications of geodynamic simulations validated with laboratory models
The physics governing the seismic cycle at seismically active subduction zones remains poorly understood due to restricted direct observations in time and space. To investigate subduction zone dynamics and associated interplate seismicity, we validate a continuum, visco‐elasto‐plastic numerical mode...
Saved in:
Published in: | Journal of geophysical research. Solid earth 2013-04, Vol.118 (4), p.1502-1525 |
---|---|
Main Authors: | , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
Tags: |
Add Tag
No Tags, Be the first to tag this record!
|
cited_by | cdi_FETCH-LOGICAL-a4828-52eddc26899cb9af2d5fef75b08e3aa5a629d54c4b93e84b67feb57ddb3858c43 |
---|---|
cites | cdi_FETCH-LOGICAL-a4828-52eddc26899cb9af2d5fef75b08e3aa5a629d54c4b93e84b67feb57ddb3858c43 |
container_end_page | 1525 |
container_issue | 4 |
container_start_page | 1502 |
container_title | Journal of geophysical research. Solid earth |
container_volume | 118 |
creator | van Dinther, Y. Gerya, T. V. Dalguer, L. A. Corbi, F. Funiciello, F. Mai, P. M. |
description | The physics governing the seismic cycle at seismically active subduction zones remains poorly understood due to restricted direct observations in time and space. To investigate subduction zone dynamics and associated interplate seismicity, we validate a continuum, visco‐elasto‐plastic numerical model with a new laboratory approach (Paper 1). The analogous laboratory setup includes a visco‐elastic gelatin wedge underthrusted by a rigid plate with defined velocity‐weakening and ‐strengthening regions. Our geodynamic simulation approach includes velocity‐weakening friction to spontaneously generate a series of fast frictional instabilities that correspond to analog earthquakes. A match between numerical and laboratory source parameters is obtained when velocity‐strengthening is applied in the aseismic regions to stabilize the rupture. Spontaneous evolution of absolute stresses leads to nucleation by coalescence of neighboring patches, mainly occurring at evolving asperities near the seismogenic zone limits. Consequently, a crack‐, or occasionally even pulse‐like, rupture propagates toward the opposite side of the seismogenic zone by increasing stresses ahead of its rupture front, until it arrests on a barrier. The resulting surface displacements qualitatively agree with geodetic observations and show landward and, from near the downdip limit, upward interseismic motions. These are rebound and reversed coseismically. This slip increases adjacent stresses, which are relaxed postseismically by afterslip and thereby produce persistent seaward motions. The wide range of observed physical phenomena, including back‐propagation and repeated slip, and the agreement with laboratory results demonstrate that visco‐elasto‐plastic geodynamic models with rate‐dependent friction form a new tool that can greatly contribute to our understanding of the seismic cycle at subduction zones.
Key points
Geodynamic simulations with rate‐dependent friction capture seismic thrust cycleSpontaneous, stress‐driven, mainly crack‐like rupture may re‐rupture hypocenterGPS displacements capture inter‐, co‐, and postseismic features via afterslip |
doi_str_mv | 10.1029/2012JB009479 |
format | article |
fullrecord | <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_miscellaneous_1642296673</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>1642296673</sourcerecordid><originalsourceid>FETCH-LOGICAL-a4828-52eddc26899cb9af2d5fef75b08e3aa5a629d54c4b93e84b67feb57ddb3858c43</originalsourceid><addsrcrecordid>eNp9kU9v1DAQxSMEElXbGx_AEhcOpHX8LzY3uqULVQWoKio3y7EnrIuz3toOJeLLk2VXFeLAXGY07_dGT5qqetHgkwYTdUpwQy7PMFasVU-qA9IIVSvKxdPHuaHPq-Oc7_Bccl417KD6dbMClMHnwVtkJxsAmYLy2LnRFh_XqKzSmEt-g8gJOp_WZsv5YRO8NVs9o9ijbxDdXsp-GMNe-WGCd6aAQw--rFAwXUymxDShIToI-ah61puQ4XjfD6svF-9uFu_rq0_LD4u3V7VhksiaE3DOEiGVsp0yPXG8h77lHZZAjeFGEOU4s6xTFCTrRNtDx1vnOiq5tIweVq92dzcp3o-Qix58thCCWUMcs24EI0QJ0dIZffkPehfHtJ7T_aEEE0LhmXq9o2yKOSfo9Sb5waRJN1hvn6H_fsaM0x3-4ANM_2X15fL6jGPM5Oyqdy6fC_x8dJn0Xc9JW65vPy71Ob5Y3H6ln_U1_Q06yJv1</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>1642646690</pqid></control><display><type>article</type><title>The seismic cycle at subduction thrusts: 2. Dynamic implications of geodynamic simulations validated with laboratory models</title><source>Wiley</source><source>Alma/SFX Local Collection</source><creator>van Dinther, Y. ; Gerya, T. V. ; Dalguer, L. A. ; Corbi, F. ; Funiciello, F. ; Mai, P. M.</creator><creatorcontrib>van Dinther, Y. ; Gerya, T. V. ; Dalguer, L. A. ; Corbi, F. ; Funiciello, F. ; Mai, P. M.</creatorcontrib><description>The physics governing the seismic cycle at seismically active subduction zones remains poorly understood due to restricted direct observations in time and space. To investigate subduction zone dynamics and associated interplate seismicity, we validate a continuum, visco‐elasto‐plastic numerical model with a new laboratory approach (Paper 1). The analogous laboratory setup includes a visco‐elastic gelatin wedge underthrusted by a rigid plate with defined velocity‐weakening and ‐strengthening regions. Our geodynamic simulation approach includes velocity‐weakening friction to spontaneously generate a series of fast frictional instabilities that correspond to analog earthquakes. A match between numerical and laboratory source parameters is obtained when velocity‐strengthening is applied in the aseismic regions to stabilize the rupture. Spontaneous evolution of absolute stresses leads to nucleation by coalescence of neighboring patches, mainly occurring at evolving asperities near the seismogenic zone limits. Consequently, a crack‐, or occasionally even pulse‐like, rupture propagates toward the opposite side of the seismogenic zone by increasing stresses ahead of its rupture front, until it arrests on a barrier. The resulting surface displacements qualitatively agree with geodetic observations and show landward and, from near the downdip limit, upward interseismic motions. These are rebound and reversed coseismically. This slip increases adjacent stresses, which are relaxed postseismically by afterslip and thereby produce persistent seaward motions. The wide range of observed physical phenomena, including back‐propagation and repeated slip, and the agreement with laboratory results demonstrate that visco‐elasto‐plastic geodynamic models with rate‐dependent friction form a new tool that can greatly contribute to our understanding of the seismic cycle at subduction zones.
Key points
Geodynamic simulations with rate‐dependent friction capture seismic thrust cycleSpontaneous, stress‐driven, mainly crack‐like rupture may re‐rupture hypocenterGPS displacements capture inter‐, co‐, and postseismic features via afterslip</description><identifier>ISSN: 2169-9313</identifier><identifier>EISSN: 2169-9356</identifier><identifier>DOI: 10.1029/2012JB009479</identifier><language>eng</language><publisher>Washington: Blackwell Publishing Ltd</publisher><subject>benchmark ; Coalescence ; Computer simulation ; Earthquakes ; Friction ; geodetic displacements ; Geodynamics ; Geophysics ; Laboratories ; Mathematical models ; numerical models ; rate-dependent friction ; Rupture ; Seismic activity ; seismic cycle ; Seismic phenomena ; Spontaneous ; Stresses ; subduction interplate earthquakes</subject><ispartof>Journal of geophysical research. Solid earth, 2013-04, Vol.118 (4), p.1502-1525</ispartof><rights>2012. American Geophysical Union. All Rights Reserved.</rights><rights>2013. American Geophysical Union. All Rights Reserved.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-a4828-52eddc26899cb9af2d5fef75b08e3aa5a629d54c4b93e84b67feb57ddb3858c43</citedby><cites>FETCH-LOGICAL-a4828-52eddc26899cb9af2d5fef75b08e3aa5a629d54c4b93e84b67feb57ddb3858c43</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>van Dinther, Y.</creatorcontrib><creatorcontrib>Gerya, T. V.</creatorcontrib><creatorcontrib>Dalguer, L. A.</creatorcontrib><creatorcontrib>Corbi, F.</creatorcontrib><creatorcontrib>Funiciello, F.</creatorcontrib><creatorcontrib>Mai, P. M.</creatorcontrib><title>The seismic cycle at subduction thrusts: 2. Dynamic implications of geodynamic simulations validated with laboratory models</title><title>Journal of geophysical research. Solid earth</title><addtitle>J. Geophys. Res. Solid Earth</addtitle><description>The physics governing the seismic cycle at seismically active subduction zones remains poorly understood due to restricted direct observations in time and space. To investigate subduction zone dynamics and associated interplate seismicity, we validate a continuum, visco‐elasto‐plastic numerical model with a new laboratory approach (Paper 1). The analogous laboratory setup includes a visco‐elastic gelatin wedge underthrusted by a rigid plate with defined velocity‐weakening and ‐strengthening regions. Our geodynamic simulation approach includes velocity‐weakening friction to spontaneously generate a series of fast frictional instabilities that correspond to analog earthquakes. A match between numerical and laboratory source parameters is obtained when velocity‐strengthening is applied in the aseismic regions to stabilize the rupture. Spontaneous evolution of absolute stresses leads to nucleation by coalescence of neighboring patches, mainly occurring at evolving asperities near the seismogenic zone limits. Consequently, a crack‐, or occasionally even pulse‐like, rupture propagates toward the opposite side of the seismogenic zone by increasing stresses ahead of its rupture front, until it arrests on a barrier. The resulting surface displacements qualitatively agree with geodetic observations and show landward and, from near the downdip limit, upward interseismic motions. These are rebound and reversed coseismically. This slip increases adjacent stresses, which are relaxed postseismically by afterslip and thereby produce persistent seaward motions. The wide range of observed physical phenomena, including back‐propagation and repeated slip, and the agreement with laboratory results demonstrate that visco‐elasto‐plastic geodynamic models with rate‐dependent friction form a new tool that can greatly contribute to our understanding of the seismic cycle at subduction zones.
Key points
Geodynamic simulations with rate‐dependent friction capture seismic thrust cycleSpontaneous, stress‐driven, mainly crack‐like rupture may re‐rupture hypocenterGPS displacements capture inter‐, co‐, and postseismic features via afterslip</description><subject>benchmark</subject><subject>Coalescence</subject><subject>Computer simulation</subject><subject>Earthquakes</subject><subject>Friction</subject><subject>geodetic displacements</subject><subject>Geodynamics</subject><subject>Geophysics</subject><subject>Laboratories</subject><subject>Mathematical models</subject><subject>numerical models</subject><subject>rate-dependent friction</subject><subject>Rupture</subject><subject>Seismic activity</subject><subject>seismic cycle</subject><subject>Seismic phenomena</subject><subject>Spontaneous</subject><subject>Stresses</subject><subject>subduction interplate earthquakes</subject><issn>2169-9313</issn><issn>2169-9356</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2013</creationdate><recordtype>article</recordtype><recordid>eNp9kU9v1DAQxSMEElXbGx_AEhcOpHX8LzY3uqULVQWoKio3y7EnrIuz3toOJeLLk2VXFeLAXGY07_dGT5qqetHgkwYTdUpwQy7PMFasVU-qA9IIVSvKxdPHuaHPq-Oc7_Bccl417KD6dbMClMHnwVtkJxsAmYLy2LnRFh_XqKzSmEt-g8gJOp_WZsv5YRO8NVs9o9ijbxDdXsp-GMNe-WGCd6aAQw--rFAwXUymxDShIToI-ah61puQ4XjfD6svF-9uFu_rq0_LD4u3V7VhksiaE3DOEiGVsp0yPXG8h77lHZZAjeFGEOU4s6xTFCTrRNtDx1vnOiq5tIweVq92dzcp3o-Qix58thCCWUMcs24EI0QJ0dIZffkPehfHtJ7T_aEEE0LhmXq9o2yKOSfo9Sb5waRJN1hvn6H_fsaM0x3-4ANM_2X15fL6jGPM5Oyqdy6fC_x8dJn0Xc9JW65vPy71Ob5Y3H6ln_U1_Q06yJv1</recordid><startdate>201304</startdate><enddate>201304</enddate><creator>van Dinther, Y.</creator><creator>Gerya, T. V.</creator><creator>Dalguer, L. A.</creator><creator>Corbi, F.</creator><creator>Funiciello, F.</creator><creator>Mai, P. M.</creator><general>Blackwell Publishing Ltd</general><scope>BSCLL</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7ST</scope><scope>7TG</scope><scope>8FD</scope><scope>C1K</scope><scope>F1W</scope><scope>FR3</scope><scope>H8D</scope><scope>H96</scope><scope>KL.</scope><scope>KR7</scope><scope>L.G</scope><scope>L7M</scope><scope>SOI</scope><scope>7TB</scope></search><sort><creationdate>201304</creationdate><title>The seismic cycle at subduction thrusts: 2. Dynamic implications of geodynamic simulations validated with laboratory models</title><author>van Dinther, Y. ; Gerya, T. V. ; Dalguer, L. A. ; Corbi, F. ; Funiciello, F. ; Mai, P. M.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a4828-52eddc26899cb9af2d5fef75b08e3aa5a629d54c4b93e84b67feb57ddb3858c43</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2013</creationdate><topic>benchmark</topic><topic>Coalescence</topic><topic>Computer simulation</topic><topic>Earthquakes</topic><topic>Friction</topic><topic>geodetic displacements</topic><topic>Geodynamics</topic><topic>Geophysics</topic><topic>Laboratories</topic><topic>Mathematical models</topic><topic>numerical models</topic><topic>rate-dependent friction</topic><topic>Rupture</topic><topic>Seismic activity</topic><topic>seismic cycle</topic><topic>Seismic phenomena</topic><topic>Spontaneous</topic><topic>Stresses</topic><topic>subduction interplate earthquakes</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>van Dinther, Y.</creatorcontrib><creatorcontrib>Gerya, T. V.</creatorcontrib><creatorcontrib>Dalguer, L. A.</creatorcontrib><creatorcontrib>Corbi, F.</creatorcontrib><creatorcontrib>Funiciello, F.</creatorcontrib><creatorcontrib>Mai, P. M.</creatorcontrib><collection>Istex</collection><collection>CrossRef</collection><collection>Environment Abstracts</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Technology Research Database</collection><collection>Environmental Sciences and Pollution Management</collection><collection>ASFA: Aquatic Sciences and Fisheries Abstracts</collection><collection>Engineering Research Database</collection><collection>Aerospace Database</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) 2: Ocean Technology, Policy & Non-Living Resources</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>Civil Engineering Abstracts</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) Professional</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Environment Abstracts</collection><collection>Mechanical & Transportation Engineering Abstracts</collection><jtitle>Journal of geophysical research. Solid earth</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>van Dinther, Y.</au><au>Gerya, T. V.</au><au>Dalguer, L. A.</au><au>Corbi, F.</au><au>Funiciello, F.</au><au>Mai, P. M.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The seismic cycle at subduction thrusts: 2. Dynamic implications of geodynamic simulations validated with laboratory models</atitle><jtitle>Journal of geophysical research. Solid earth</jtitle><addtitle>J. Geophys. Res. Solid Earth</addtitle><date>2013-04</date><risdate>2013</risdate><volume>118</volume><issue>4</issue><spage>1502</spage><epage>1525</epage><pages>1502-1525</pages><issn>2169-9313</issn><eissn>2169-9356</eissn><abstract>The physics governing the seismic cycle at seismically active subduction zones remains poorly understood due to restricted direct observations in time and space. To investigate subduction zone dynamics and associated interplate seismicity, we validate a continuum, visco‐elasto‐plastic numerical model with a new laboratory approach (Paper 1). The analogous laboratory setup includes a visco‐elastic gelatin wedge underthrusted by a rigid plate with defined velocity‐weakening and ‐strengthening regions. Our geodynamic simulation approach includes velocity‐weakening friction to spontaneously generate a series of fast frictional instabilities that correspond to analog earthquakes. A match between numerical and laboratory source parameters is obtained when velocity‐strengthening is applied in the aseismic regions to stabilize the rupture. Spontaneous evolution of absolute stresses leads to nucleation by coalescence of neighboring patches, mainly occurring at evolving asperities near the seismogenic zone limits. Consequently, a crack‐, or occasionally even pulse‐like, rupture propagates toward the opposite side of the seismogenic zone by increasing stresses ahead of its rupture front, until it arrests on a barrier. The resulting surface displacements qualitatively agree with geodetic observations and show landward and, from near the downdip limit, upward interseismic motions. These are rebound and reversed coseismically. This slip increases adjacent stresses, which are relaxed postseismically by afterslip and thereby produce persistent seaward motions. The wide range of observed physical phenomena, including back‐propagation and repeated slip, and the agreement with laboratory results demonstrate that visco‐elasto‐plastic geodynamic models with rate‐dependent friction form a new tool that can greatly contribute to our understanding of the seismic cycle at subduction zones.
Key points
Geodynamic simulations with rate‐dependent friction capture seismic thrust cycleSpontaneous, stress‐driven, mainly crack‐like rupture may re‐rupture hypocenterGPS displacements capture inter‐, co‐, and postseismic features via afterslip</abstract><cop>Washington</cop><pub>Blackwell Publishing Ltd</pub><doi>10.1029/2012JB009479</doi><tpages>24</tpages><oa>free_for_read</oa></addata></record> |
fulltext | fulltext |
identifier | ISSN: 2169-9313 |
ispartof | Journal of geophysical research. Solid earth, 2013-04, Vol.118 (4), p.1502-1525 |
issn | 2169-9313 2169-9356 |
language | eng |
recordid | cdi_proquest_miscellaneous_1642296673 |
source | Wiley; Alma/SFX Local Collection |
subjects | benchmark Coalescence Computer simulation Earthquakes Friction geodetic displacements Geodynamics Geophysics Laboratories Mathematical models numerical models rate-dependent friction Rupture Seismic activity seismic cycle Seismic phenomena Spontaneous Stresses subduction interplate earthquakes |
title | The seismic cycle at subduction thrusts: 2. Dynamic implications of geodynamic simulations validated with laboratory models |
url | http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-05T23%3A37%3A29IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=The%20seismic%20cycle%20at%20subduction%20thrusts:%202.%20Dynamic%20implications%20of%20geodynamic%20simulations%20validated%20with%20laboratory%20models&rft.jtitle=Journal%20of%20geophysical%20research.%20Solid%20earth&rft.au=van%20Dinther,%20Y.&rft.date=2013-04&rft.volume=118&rft.issue=4&rft.spage=1502&rft.epage=1525&rft.pages=1502-1525&rft.issn=2169-9313&rft.eissn=2169-9356&rft_id=info:doi/10.1029/2012JB009479&rft_dat=%3Cproquest_cross%3E1642296673%3C/proquest_cross%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-a4828-52eddc26899cb9af2d5fef75b08e3aa5a629d54c4b93e84b67feb57ddb3858c43%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_pqid=1642646690&rft_id=info:pmid/&rfr_iscdi=true |