Emergent anisotropy and flow alignment in viscous rock
-- A novel class of nonlinear, visco-elastic rheologies has recently been developed by MÜHLHAUS et al.(2002a, b). The theory was originally developed for the simulation of large deformation processes including folding and kinking in multi-layered visco-elastic rock . The orientation of the layer sur...
Gespeichert in:
Veröffentlicht in: | Pure and Applied Geophysics 2004-12, Vol.161 (11-12), p.2451-2463 |
---|---|
Hauptverfasser: | , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
container_end_page | 2463 |
---|---|
container_issue | 11-12 |
container_start_page | 2451 |
container_title | Pure and Applied Geophysics |
container_volume | 161 |
creator | MÜHLHAUS, H.-B MORESI, L CADA, M |
description | -- A novel class of nonlinear, visco-elastic rheologies has recently been developed by MÜHLHAUS et al.(2002a, b). The theory was originally developed for the simulation of large deformation processes including folding and kinking in multi-layered visco-elastic rock . The orientation of the layer surfaces or slip planes in the context of crystallographic slip is determined by the normal vector the so-called director of these surfaces. Here the model (MÜHLHAUS et al., 2002a, b) is generalized to include thermal effects; it is shown that in 2-D steady states the director is given by the gradient of the flow potential. The model is applied to anisotropic simple shear where the directors are initially parallel to the shear direction. The relative effects of textural hardening and thermal softening are demonstrated. We then turn to natural convection and compare the time evolution and approximately steady states of isotropic and anisotropic convection for a Rayleigh number Ra=5.64×10^sup 5^ for aspect ratios of the experimental domain of 1 and 2, respectively. The isotropic case has a simple steady-state solution, whereas in the orthotropic convection model patterns evolve continuously in the core of the convection cell, which makes only a near-steady condition possible. This near-steady state condition shows well aligned boundary layers, and the number of convection cells which develop appears to be reduced in the orthotropic case. At the moderate Rayleigh numbers explored here we found only minor influences in the change from aspect ratio one to two in the model domain.[PUBLICATION ABSTRACT] |
doi_str_mv | 10.1007/s00024-004-2575-5 |
format | Article |
fullrecord | <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_miscellaneous_815538719</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2165913091</sourcerecordid><originalsourceid>FETCH-LOGICAL-a355t-7cb2c70d9776f8ced056f5fc75b0b15dacd98cff1f7e6a7be6a796cb5cfce2793</originalsourceid><addsrcrecordid>eNpdkE9LxDAQxYMouK5-AG9FEE_RSdNpmqMs6x9Y8KLnkKbJ0rVt1qSr7Lc3ZRcELzMD897w5kfINYN7BiAeIgDkBQUoaI4CKZ6QGStyoJLx8pTMADinBSI_JxcxbgCYEChnpFz2NqztMGZ6aKMfg9_u09hkrvM_me7a9dBP23bIvtto_C5mwZvPS3LmdBft1bHPycfT8n3xQldvz6-LxxXVHHGkwtS5EdBIIUpXGdsAlg6dEVhDzbDRppGVcY45YUst6qnI0tRonLG5kHxO7g53t8F_7WwcVZ9S2K7Tg01ZVMXSS5Vgk_Lmn3Ljd2FI4ZTASvICpUgidhCZ4GMM1qltaHsd9oqBmjiqA0eVOKqJo8LkuT0e1tHozgU9mDb-GUsmJeaS_wKbaHLv</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>758934597</pqid></control><display><type>article</type><title>Emergent anisotropy and flow alignment in viscous rock</title><source>Springer Journals</source><creator>MÜHLHAUS, H.-B ; MORESI, L ; CADA, M</creator><creatorcontrib>MÜHLHAUS, H.-B ; MORESI, L ; CADA, M</creatorcontrib><description>-- A novel class of nonlinear, visco-elastic rheologies has recently been developed by MÜHLHAUS et al.(2002a, b). The theory was originally developed for the simulation of large deformation processes including folding and kinking in multi-layered visco-elastic rock . The orientation of the layer surfaces or slip planes in the context of crystallographic slip is determined by the normal vector the so-called director of these surfaces. Here the model (MÜHLHAUS et al., 2002a, b) is generalized to include thermal effects; it is shown that in 2-D steady states the director is given by the gradient of the flow potential. The model is applied to anisotropic simple shear where the directors are initially parallel to the shear direction. The relative effects of textural hardening and thermal softening are demonstrated. We then turn to natural convection and compare the time evolution and approximately steady states of isotropic and anisotropic convection for a Rayleigh number Ra=5.64×10^sup 5^ for aspect ratios of the experimental domain of 1 and 2, respectively. The isotropic case has a simple steady-state solution, whereas in the orthotropic convection model patterns evolve continuously in the core of the convection cell, which makes only a near-steady condition possible. This near-steady state condition shows well aligned boundary layers, and the number of convection cells which develop appears to be reduced in the orthotropic case. At the moderate Rayleigh numbers explored here we found only minor influences in the change from aspect ratio one to two in the model domain.[PUBLICATION ABSTRACT]</description><identifier>ISSN: 0033-4553</identifier><identifier>EISSN: 1420-9136</identifier><identifier>DOI: 10.1007/s00024-004-2575-5</identifier><identifier>CODEN: PAGYAV</identifier><language>eng</language><publisher>Basel: Springer</publisher><subject>Anisotropy ; Boundary layers ; Convection ; Earth sciences ; Earth, ocean, space ; Exact sciences and technology ; Rocks ; Studies ; Tectonics. Structural geology. Plate tectonics</subject><ispartof>Pure and Applied Geophysics, 2004-12, Vol.161 (11-12), p.2451-2463</ispartof><rights>2004 INIST-CNRS</rights><rights>Birkhäuser Verlag, Basel, 2004</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-a355t-7cb2c70d9776f8ced056f5fc75b0b15dacd98cff1f7e6a7be6a796cb5cfce2793</citedby></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>309,310,314,776,780,785,786,23909,23910,25118,27901,27902</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=16199529$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>MÜHLHAUS, H.-B</creatorcontrib><creatorcontrib>MORESI, L</creatorcontrib><creatorcontrib>CADA, M</creatorcontrib><title>Emergent anisotropy and flow alignment in viscous rock</title><title>Pure and Applied Geophysics</title><description>-- A novel class of nonlinear, visco-elastic rheologies has recently been developed by MÜHLHAUS et al.(2002a, b). The theory was originally developed for the simulation of large deformation processes including folding and kinking in multi-layered visco-elastic rock . The orientation of the layer surfaces or slip planes in the context of crystallographic slip is determined by the normal vector the so-called director of these surfaces. Here the model (MÜHLHAUS et al., 2002a, b) is generalized to include thermal effects; it is shown that in 2-D steady states the director is given by the gradient of the flow potential. The model is applied to anisotropic simple shear where the directors are initially parallel to the shear direction. The relative effects of textural hardening and thermal softening are demonstrated. We then turn to natural convection and compare the time evolution and approximately steady states of isotropic and anisotropic convection for a Rayleigh number Ra=5.64×10^sup 5^ for aspect ratios of the experimental domain of 1 and 2, respectively. The isotropic case has a simple steady-state solution, whereas in the orthotropic convection model patterns evolve continuously in the core of the convection cell, which makes only a near-steady condition possible. This near-steady state condition shows well aligned boundary layers, and the number of convection cells which develop appears to be reduced in the orthotropic case. At the moderate Rayleigh numbers explored here we found only minor influences in the change from aspect ratio one to two in the model domain.[PUBLICATION ABSTRACT]</description><subject>Anisotropy</subject><subject>Boundary layers</subject><subject>Convection</subject><subject>Earth sciences</subject><subject>Earth, ocean, space</subject><subject>Exact sciences and technology</subject><subject>Rocks</subject><subject>Studies</subject><subject>Tectonics. Structural geology. Plate tectonics</subject><issn>0033-4553</issn><issn>1420-9136</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2004</creationdate><recordtype>article</recordtype><sourceid>BENPR</sourceid><recordid>eNpdkE9LxDAQxYMouK5-AG9FEE_RSdNpmqMs6x9Y8KLnkKbJ0rVt1qSr7Lc3ZRcELzMD897w5kfINYN7BiAeIgDkBQUoaI4CKZ6QGStyoJLx8pTMADinBSI_JxcxbgCYEChnpFz2NqztMGZ6aKMfg9_u09hkrvM_me7a9dBP23bIvtto_C5mwZvPS3LmdBft1bHPycfT8n3xQldvz6-LxxXVHHGkwtS5EdBIIUpXGdsAlg6dEVhDzbDRppGVcY45YUst6qnI0tRonLG5kHxO7g53t8F_7WwcVZ9S2K7Tg01ZVMXSS5Vgk_Lmn3Ljd2FI4ZTASvICpUgidhCZ4GMM1qltaHsd9oqBmjiqA0eVOKqJo8LkuT0e1tHozgU9mDb-GUsmJeaS_wKbaHLv</recordid><startdate>20041201</startdate><enddate>20041201</enddate><creator>MÜHLHAUS, H.-B</creator><creator>MORESI, L</creator><creator>CADA, M</creator><general>Springer</general><general>Springer Nature B.V</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>3V.</scope><scope>7TG</scope><scope>7UA</scope><scope>7XB</scope><scope>88I</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>8FK</scope><scope>ABUWG</scope><scope>AEUYN</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>ATCPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>BHPHI</scope><scope>BKSAR</scope><scope>C1K</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>F1W</scope><scope>GNUQQ</scope><scope>H8D</scope><scope>H96</scope><scope>HCIFZ</scope><scope>KL.</scope><scope>L.G</scope><scope>L7M</scope><scope>M2P</scope><scope>P5Z</scope><scope>P62</scope><scope>PATMY</scope><scope>PCBAR</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PYCSY</scope><scope>Q9U</scope></search><sort><creationdate>20041201</creationdate><title>Emergent anisotropy and flow alignment in viscous rock</title><author>MÜHLHAUS, H.-B ; MORESI, L ; CADA, M</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a355t-7cb2c70d9776f8ced056f5fc75b0b15dacd98cff1f7e6a7be6a796cb5cfce2793</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2004</creationdate><topic>Anisotropy</topic><topic>Boundary layers</topic><topic>Convection</topic><topic>Earth sciences</topic><topic>Earth, ocean, space</topic><topic>Exact sciences and technology</topic><topic>Rocks</topic><topic>Studies</topic><topic>Tectonics. Structural geology. Plate tectonics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>MÜHLHAUS, H.-B</creatorcontrib><creatorcontrib>MORESI, L</creatorcontrib><creatorcontrib>CADA, M</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>ProQuest Central (Corporate)</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Water Resources Abstracts</collection><collection>ProQuest Central (purchase pre-March 2016)</collection><collection>Science Database (Alumni Edition)</collection><collection>Technology Research Database</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>ProQuest Central (Alumni) (purchase pre-March 2016)</collection><collection>ProQuest Central (Alumni)</collection><collection>ProQuest One Sustainability</collection><collection>ProQuest Central UK/Ireland</collection><collection>Advanced Technologies & Aerospace Collection</collection><collection>ProQuest Agriculture & Environmental Science Database</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest Natural Science Collection</collection><collection>Earth, Atmospheric & Aquatic Science Database</collection><collection>Environmental Sciences and Pollution Management</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central</collection><collection>ASFA: Aquatic Sciences and Fisheries Abstracts</collection><collection>ProQuest Central Student</collection><collection>Aerospace Database</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) 2: Ocean Technology, Policy & Non-Living Resources</collection><collection>SciTech Premium Collection</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) Professional</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Science Database</collection><collection>ProQuest advanced technologies & aerospace journals</collection><collection>ProQuest Advanced Technologies & Aerospace Collection</collection><collection>Environmental Science Database</collection><collection>ProQuest Earth, Atmospheric & Aquatic Science Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>Environmental Science Collection</collection><collection>ProQuest Central Basic</collection><jtitle>Pure and Applied Geophysics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>MÜHLHAUS, H.-B</au><au>MORESI, L</au><au>CADA, M</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Emergent anisotropy and flow alignment in viscous rock</atitle><jtitle>Pure and Applied Geophysics</jtitle><date>2004-12-01</date><risdate>2004</risdate><volume>161</volume><issue>11-12</issue><spage>2451</spage><epage>2463</epage><pages>2451-2463</pages><issn>0033-4553</issn><eissn>1420-9136</eissn><coden>PAGYAV</coden><abstract>-- A novel class of nonlinear, visco-elastic rheologies has recently been developed by MÜHLHAUS et al.(2002a, b). The theory was originally developed for the simulation of large deformation processes including folding and kinking in multi-layered visco-elastic rock . The orientation of the layer surfaces or slip planes in the context of crystallographic slip is determined by the normal vector the so-called director of these surfaces. Here the model (MÜHLHAUS et al., 2002a, b) is generalized to include thermal effects; it is shown that in 2-D steady states the director is given by the gradient of the flow potential. The model is applied to anisotropic simple shear where the directors are initially parallel to the shear direction. The relative effects of textural hardening and thermal softening are demonstrated. We then turn to natural convection and compare the time evolution and approximately steady states of isotropic and anisotropic convection for a Rayleigh number Ra=5.64×10^sup 5^ for aspect ratios of the experimental domain of 1 and 2, respectively. The isotropic case has a simple steady-state solution, whereas in the orthotropic convection model patterns evolve continuously in the core of the convection cell, which makes only a near-steady condition possible. This near-steady state condition shows well aligned boundary layers, and the number of convection cells which develop appears to be reduced in the orthotropic case. At the moderate Rayleigh numbers explored here we found only minor influences in the change from aspect ratio one to two in the model domain.[PUBLICATION ABSTRACT]</abstract><cop>Basel</cop><pub>Springer</pub><doi>10.1007/s00024-004-2575-5</doi><tpages>13</tpages></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0033-4553 |
ispartof | Pure and Applied Geophysics, 2004-12, Vol.161 (11-12), p.2451-2463 |
issn | 0033-4553 1420-9136 |
language | eng |
recordid | cdi_proquest_miscellaneous_815538719 |
source | Springer Journals |
subjects | Anisotropy Boundary layers Convection Earth sciences Earth, ocean, space Exact sciences and technology Rocks Studies Tectonics. Structural geology. Plate tectonics |
title | Emergent anisotropy and flow alignment in viscous rock |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-02-11T23%3A52%3A08IST&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=Emergent%20anisotropy%20and%20flow%20alignment%20in%20viscous%20rock&rft.jtitle=Pure%20and%20Applied%20Geophysics&rft.au=M%C3%9CHLHAUS,%20H.-B&rft.date=2004-12-01&rft.volume=161&rft.issue=11-12&rft.spage=2451&rft.epage=2463&rft.pages=2451-2463&rft.issn=0033-4553&rft.eissn=1420-9136&rft.coden=PAGYAV&rft_id=info:doi/10.1007/s00024-004-2575-5&rft_dat=%3Cproquest_cross%3E2165913091%3C/proquest_cross%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=758934597&rft_id=info:pmid/&rfr_iscdi=true |