Activation of Dissolution‐Precipitation Creep Causes Weakening and Viscous Behavior in Experimentally Deformed Antigorite
Antigorite occurs at seismogenic depth along plate boundary shear zones, particularly in subduction and oceanic transform settings, and has been suggested to control a low‐strength bulk rheology. To constrain dominant deformation mechanisms, we perform hydrothermal ring‐shear experiments on antigori...
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description | Antigorite occurs at seismogenic depth along plate boundary shear zones, particularly in subduction and oceanic transform settings, and has been suggested to control a low‐strength bulk rheology. To constrain dominant deformation mechanisms, we perform hydrothermal ring‐shear experiments on antigorite and antigorite‐quartz mixtures at temperatures between 20 and 500°C at 150 MPa effective normal stress. Pure antigorite is strain hardening, with frictional coefficient (μ) > 0.5, and developed cataclastic microstructures. In contrast, antigorite‐quartz mixtures (10% quartz) are strain weakening with μ decreasing with temperature from 0.36 at 200°C to 0.22 at 500°C. Antigorite‐quartz mixtures developed foliation similar to natural serpentinite shear zones. Although antigorite‐quartz reactions may form mechanically weak talc, we only find small, localized amounts of talc in our deformed samples, and room temperature friction is higher than expected for talc. Instead, we propose that the observed weakening at temperatures ≥200°C primarily results from silica dissolution leading to a lowered pore‐fluid pH that increases antigorite solubility and dissolution rate and thus the rate of dissolution‐precipitation creep. We suggest that under our experimental conditions, efficient dissolution‐precipitation creep coupled to grain boundary sliding results in a mechanically weak frictional‐viscous rheology. Antigorite with this rheology is much weaker than antigorite deforming frictionally, and strength is sensitive to effective normal stress and strain rate. The activation of dissolution‐precipitation in antigorite may allow steady or transient creep at low driving stress where antigorite solubility and dissolution rate are high relative to strain rate, for example, in faults juxtaposing serpentinite with quartz‐bearing rocks.
Plain Language Summary
Some major, plate‐boundary fault zones are very weak, and in some places this is thought to be because they contain the mineral serpentine. Antigorite is a common form of serpentine at depth, but in many rock deformation experiments, antigorite is found to be relatively strong. In natural fault zones, however, antigorite can be highly deformed at seemingly low stress. The motivation for this study was to explore whether antigorite can be weak also in the laboratory. Because laboratory experiments occur relatively fast, the mechanism of deformation may be different from in nature. To address this, we mixed antigorite with qua |
doi_str_mv | 10.1029/2024JB029053 |
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Plain Language Summary
Some major, plate‐boundary fault zones are very weak, and in some places this is thought to be because they contain the mineral serpentine. Antigorite is a common form of serpentine at depth, but in many rock deformation experiments, antigorite is found to be relatively strong. In natural fault zones, however, antigorite can be highly deformed at seemingly low stress. The motivation for this study was to explore whether antigorite can be weak also in the laboratory. Because laboratory experiments occur relatively fast, the mechanism of deformation may be different from in nature. To address this, we mixed antigorite with quartz, which changes the pH and promotes dissolution of antigorite. We found that when deforming antigorite mixed with quartz, the experimental fault was very weak, because the dissolution of antigorite removed sticking points ‐ a process that is also documented in natural faults. The experiments also produced minor talc, from the reaction of antigorite with quartz, but too little to affect strength. We suggest that it is the activation of dissolution and precipitation of antigorite which allows deformation of major serpentine‐bearing faults at low stress at temperatures of several hundred degrees Celsius.
Key Points
At 20°C and 500°C antigorite is strain‐hardening, develops cataclastic microstructures and has a frictional coefficient of ∼0.5
Samples of antigorite mixed with quartz are strain‐weakening, and the friction coefficient decreases from 0.36 at 200°C to 0.22 at 500°C
The weakness of quartz‐antigorite is associated with activation of dissolution‐precipitation creep</description><identifier>ISSN: 2169-9313</identifier><identifier>EISSN: 2169-9356</identifier><identifier>DOI: 10.1029/2024JB029053</identifier><language>eng</language><publisher>Washington: Blackwell Publishing Ltd</publisher><subject>Boundary shear ; Deformation ; Deformation effects ; Deformation mechanisms ; Dissolution ; dissolution‐precipitation creep ; Dissolving ; experimental rock deformation ; Experiments ; Fault lines ; Fault zones ; Faults ; frictional‐viscous flow ; Grain boundary sliding ; Laboratory experimentation ; Laboratory experiments ; microstructure ; Mixtures ; Normal stress ; Plate boundaries ; Plates (tectonics) ; Precipitation ; Quartz ; Rheological properties ; Rheology ; Rock deformation ; Rocks ; Room temperature ; Serpentine ; Serpentinite ; Shear ; Shear zone ; Silica ; Solifluction ; Solubility ; Strain ; Strain hardening ; Strain rate ; Subduction ; Subduction (geology) ; Talc</subject><ispartof>Journal of geophysical research. Solid earth, 2024-08, Vol.129 (8), p.n/a</ispartof><rights>2024. The Author(s).</rights><rights>2024. This article is published under http://creativecommons.org/licenses/by/4.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><orcidid>0000-0001-6335-8534 ; 0000-0001-9332-9662 ; 0000-0003-3983-9308</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1029%2F2024JB029053$$EPDF$$P50$$Gwiley$$Hfree_for_read</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1029%2F2024JB029053$$EHTML$$P50$$Gwiley$$Hfree_for_read</linktohtml><link.rule.ids>314,780,784,1417,27924,27925,45574,45575</link.rule.ids></links><search><creatorcontrib>Tulley, C. J.</creatorcontrib><creatorcontrib>ten Thij, L.</creatorcontrib><creatorcontrib>Niemeijer, A. R.</creatorcontrib><creatorcontrib>Hamers, M. F.</creatorcontrib><creatorcontrib>Fagereng, Å.</creatorcontrib><title>Activation of Dissolution‐Precipitation Creep Causes Weakening and Viscous Behavior in Experimentally Deformed Antigorite</title><title>Journal of geophysical research. Solid earth</title><description>Antigorite occurs at seismogenic depth along plate boundary shear zones, particularly in subduction and oceanic transform settings, and has been suggested to control a low‐strength bulk rheology. To constrain dominant deformation mechanisms, we perform hydrothermal ring‐shear experiments on antigorite and antigorite‐quartz mixtures at temperatures between 20 and 500°C at 150 MPa effective normal stress. Pure antigorite is strain hardening, with frictional coefficient (μ) > 0.5, and developed cataclastic microstructures. In contrast, antigorite‐quartz mixtures (10% quartz) are strain weakening with μ decreasing with temperature from 0.36 at 200°C to 0.22 at 500°C. Antigorite‐quartz mixtures developed foliation similar to natural serpentinite shear zones. Although antigorite‐quartz reactions may form mechanically weak talc, we only find small, localized amounts of talc in our deformed samples, and room temperature friction is higher than expected for talc. Instead, we propose that the observed weakening at temperatures ≥200°C primarily results from silica dissolution leading to a lowered pore‐fluid pH that increases antigorite solubility and dissolution rate and thus the rate of dissolution‐precipitation creep. We suggest that under our experimental conditions, efficient dissolution‐precipitation creep coupled to grain boundary sliding results in a mechanically weak frictional‐viscous rheology. Antigorite with this rheology is much weaker than antigorite deforming frictionally, and strength is sensitive to effective normal stress and strain rate. The activation of dissolution‐precipitation in antigorite may allow steady or transient creep at low driving stress where antigorite solubility and dissolution rate are high relative to strain rate, for example, in faults juxtaposing serpentinite with quartz‐bearing rocks.
Plain Language Summary
Some major, plate‐boundary fault zones are very weak, and in some places this is thought to be because they contain the mineral serpentine. Antigorite is a common form of serpentine at depth, but in many rock deformation experiments, antigorite is found to be relatively strong. In natural fault zones, however, antigorite can be highly deformed at seemingly low stress. The motivation for this study was to explore whether antigorite can be weak also in the laboratory. Because laboratory experiments occur relatively fast, the mechanism of deformation may be different from in nature. To address this, we mixed antigorite with quartz, which changes the pH and promotes dissolution of antigorite. We found that when deforming antigorite mixed with quartz, the experimental fault was very weak, because the dissolution of antigorite removed sticking points ‐ a process that is also documented in natural faults. The experiments also produced minor talc, from the reaction of antigorite with quartz, but too little to affect strength. We suggest that it is the activation of dissolution and precipitation of antigorite which allows deformation of major serpentine‐bearing faults at low stress at temperatures of several hundred degrees Celsius.
Key Points
At 20°C and 500°C antigorite is strain‐hardening, develops cataclastic microstructures and has a frictional coefficient of ∼0.5
Samples of antigorite mixed with quartz are strain‐weakening, and the friction coefficient decreases from 0.36 at 200°C to 0.22 at 500°C
The weakness of quartz‐antigorite is associated with activation of dissolution‐precipitation creep</description><subject>Boundary shear</subject><subject>Deformation</subject><subject>Deformation effects</subject><subject>Deformation mechanisms</subject><subject>Dissolution</subject><subject>dissolution‐precipitation creep</subject><subject>Dissolving</subject><subject>experimental rock deformation</subject><subject>Experiments</subject><subject>Fault lines</subject><subject>Fault zones</subject><subject>Faults</subject><subject>frictional‐viscous flow</subject><subject>Grain boundary sliding</subject><subject>Laboratory experimentation</subject><subject>Laboratory experiments</subject><subject>microstructure</subject><subject>Mixtures</subject><subject>Normal stress</subject><subject>Plate boundaries</subject><subject>Plates (tectonics)</subject><subject>Precipitation</subject><subject>Quartz</subject><subject>Rheological properties</subject><subject>Rheology</subject><subject>Rock deformation</subject><subject>Rocks</subject><subject>Room temperature</subject><subject>Serpentine</subject><subject>Serpentinite</subject><subject>Shear</subject><subject>Shear zone</subject><subject>Silica</subject><subject>Solifluction</subject><subject>Solubility</subject><subject>Strain</subject><subject>Strain hardening</subject><subject>Strain rate</subject><subject>Subduction</subject><subject>Subduction (geology)</subject><subject>Talc</subject><issn>2169-9313</issn><issn>2169-9356</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><sourceid>24P</sourceid><sourceid>WIN</sourceid><recordid>eNpNkEtOwzAQhi0EElXpjgNYYh2w87DjZV8UqkogxGMZOfGkuKR2sJNCxYYjcEZOQqoixGzmm5lfM6MfoVNKzikJxUVIwng-6ogk0QHqhZSJQEQJO_xjGh2jgfcr0kXatWjcQx_DotEb2WhrsC3xRHtvq3ZXfn9-3ToodK2b_XjsAGo8lq0Hj59AvoDRZomlUfhR-8K2Ho_gWW60dVgbPH2vwek1mEZW1RZPoLRuDQoPTaOX1ukGTtBRKSsPg9_cRw-X0_vxVbC4mV2Ph4tA0pQkAYWSKy5UkStZchlTliR5yHKiAAohWJHmPM6ZIpwzVkjFJaSQRyoRQhQ5L6M-OtvvrZ19bcE32cq2znQns4gIHlNCCetU0V71pivYZnX3u3TbjJJsZ2_2395sPrsbJWyHPzyJcrM</recordid><startdate>202408</startdate><enddate>202408</enddate><creator>Tulley, C. J.</creator><creator>ten Thij, L.</creator><creator>Niemeijer, A. R.</creator><creator>Hamers, M. F.</creator><creator>Fagereng, Å.</creator><general>Blackwell Publishing Ltd</general><scope>24P</scope><scope>WIN</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><orcidid>https://orcid.org/0000-0001-6335-8534</orcidid><orcidid>https://orcid.org/0000-0001-9332-9662</orcidid><orcidid>https://orcid.org/0000-0003-3983-9308</orcidid></search><sort><creationdate>202408</creationdate><title>Activation of Dissolution‐Precipitation Creep Causes Weakening and Viscous Behavior in Experimentally Deformed Antigorite</title><author>Tulley, C. J. ; ten Thij, L. ; Niemeijer, A. R. ; Hamers, M. F. ; Fagereng, Å.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a1805-1ef7d79dcbdaf7a41655b26b0deec996c8b74b6d07766cad7ae8eb3d5999cb7f3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><topic>Boundary shear</topic><topic>Deformation</topic><topic>Deformation effects</topic><topic>Deformation mechanisms</topic><topic>Dissolution</topic><topic>dissolution‐precipitation creep</topic><topic>Dissolving</topic><topic>experimental rock deformation</topic><topic>Experiments</topic><topic>Fault lines</topic><topic>Fault zones</topic><topic>Faults</topic><topic>frictional‐viscous flow</topic><topic>Grain boundary sliding</topic><topic>Laboratory experimentation</topic><topic>Laboratory experiments</topic><topic>microstructure</topic><topic>Mixtures</topic><topic>Normal stress</topic><topic>Plate boundaries</topic><topic>Plates (tectonics)</topic><topic>Precipitation</topic><topic>Quartz</topic><topic>Rheological properties</topic><topic>Rheology</topic><topic>Rock deformation</topic><topic>Rocks</topic><topic>Room temperature</topic><topic>Serpentine</topic><topic>Serpentinite</topic><topic>Shear</topic><topic>Shear zone</topic><topic>Silica</topic><topic>Solifluction</topic><topic>Solubility</topic><topic>Strain</topic><topic>Strain hardening</topic><topic>Strain rate</topic><topic>Subduction</topic><topic>Subduction (geology)</topic><topic>Talc</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Tulley, C. J.</creatorcontrib><creatorcontrib>ten Thij, L.</creatorcontrib><creatorcontrib>Niemeijer, A. R.</creatorcontrib><creatorcontrib>Hamers, M. F.</creatorcontrib><creatorcontrib>Fagereng, Å.</creatorcontrib><collection>Wiley Online Library Open Access</collection><collection>Wiley Online Library (Open Access Collection)</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><jtitle>Journal of geophysical research. Solid earth</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Tulley, C. J.</au><au>ten Thij, L.</au><au>Niemeijer, A. R.</au><au>Hamers, M. F.</au><au>Fagereng, Å.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Activation of Dissolution‐Precipitation Creep Causes Weakening and Viscous Behavior in Experimentally Deformed Antigorite</atitle><jtitle>Journal of geophysical research. Solid earth</jtitle><date>2024-08</date><risdate>2024</risdate><volume>129</volume><issue>8</issue><epage>n/a</epage><issn>2169-9313</issn><eissn>2169-9356</eissn><abstract>Antigorite occurs at seismogenic depth along plate boundary shear zones, particularly in subduction and oceanic transform settings, and has been suggested to control a low‐strength bulk rheology. To constrain dominant deformation mechanisms, we perform hydrothermal ring‐shear experiments on antigorite and antigorite‐quartz mixtures at temperatures between 20 and 500°C at 150 MPa effective normal stress. Pure antigorite is strain hardening, with frictional coefficient (μ) > 0.5, and developed cataclastic microstructures. In contrast, antigorite‐quartz mixtures (10% quartz) are strain weakening with μ decreasing with temperature from 0.36 at 200°C to 0.22 at 500°C. Antigorite‐quartz mixtures developed foliation similar to natural serpentinite shear zones. Although antigorite‐quartz reactions may form mechanically weak talc, we only find small, localized amounts of talc in our deformed samples, and room temperature friction is higher than expected for talc. Instead, we propose that the observed weakening at temperatures ≥200°C primarily results from silica dissolution leading to a lowered pore‐fluid pH that increases antigorite solubility and dissolution rate and thus the rate of dissolution‐precipitation creep. We suggest that under our experimental conditions, efficient dissolution‐precipitation creep coupled to grain boundary sliding results in a mechanically weak frictional‐viscous rheology. Antigorite with this rheology is much weaker than antigorite deforming frictionally, and strength is sensitive to effective normal stress and strain rate. The activation of dissolution‐precipitation in antigorite may allow steady or transient creep at low driving stress where antigorite solubility and dissolution rate are high relative to strain rate, for example, in faults juxtaposing serpentinite with quartz‐bearing rocks.
Plain Language Summary
Some major, plate‐boundary fault zones are very weak, and in some places this is thought to be because they contain the mineral serpentine. Antigorite is a common form of serpentine at depth, but in many rock deformation experiments, antigorite is found to be relatively strong. In natural fault zones, however, antigorite can be highly deformed at seemingly low stress. The motivation for this study was to explore whether antigorite can be weak also in the laboratory. Because laboratory experiments occur relatively fast, the mechanism of deformation may be different from in nature. To address this, we mixed antigorite with quartz, which changes the pH and promotes dissolution of antigorite. We found that when deforming antigorite mixed with quartz, the experimental fault was very weak, because the dissolution of antigorite removed sticking points ‐ a process that is also documented in natural faults. The experiments also produced minor talc, from the reaction of antigorite with quartz, but too little to affect strength. We suggest that it is the activation of dissolution and precipitation of antigorite which allows deformation of major serpentine‐bearing faults at low stress at temperatures of several hundred degrees Celsius.
Key Points
At 20°C and 500°C antigorite is strain‐hardening, develops cataclastic microstructures and has a frictional coefficient of ∼0.5
Samples of antigorite mixed with quartz are strain‐weakening, and the friction coefficient decreases from 0.36 at 200°C to 0.22 at 500°C
The weakness of quartz‐antigorite is associated with activation of dissolution‐precipitation creep</abstract><cop>Washington</cop><pub>Blackwell Publishing Ltd</pub><doi>10.1029/2024JB029053</doi><tpages>17</tpages><orcidid>https://orcid.org/0000-0001-6335-8534</orcidid><orcidid>https://orcid.org/0000-0001-9332-9662</orcidid><orcidid>https://orcid.org/0000-0003-3983-9308</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Boundary shear Deformation Deformation effects Deformation mechanisms Dissolution dissolution‐precipitation creep Dissolving experimental rock deformation Experiments Fault lines Fault zones Faults frictional‐viscous flow Grain boundary sliding Laboratory experimentation Laboratory experiments microstructure Mixtures Normal stress Plate boundaries Plates (tectonics) Precipitation Quartz Rheological properties Rheology Rock deformation Rocks Room temperature Serpentine Serpentinite Shear Shear zone Silica Solifluction Solubility Strain Strain hardening Strain rate Subduction Subduction (geology) Talc |
title | Activation of Dissolution‐Precipitation Creep Causes Weakening and Viscous Behavior in Experimentally Deformed Antigorite |
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