Extension of Aseismic Slip Propagation Theory to Slow Earthquake Migration

Natural faults host various types of migrating slow earthquake phenomena, with migration speeds much lower than seismic wave speeds and different moment‐duration scaling from regular earthquakes. To advance the obtained quantitative understanding of the migration process and long duration of slow ea...

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Veröffentlicht in:Journal of geophysical research. Solid earth 2022-07, Vol.127 (7), p.n/a
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description Natural faults host various types of migrating slow earthquake phenomena, with migration speeds much lower than seismic wave speeds and different moment‐duration scaling from regular earthquakes. To advance the obtained quantitative understanding of the migration process and long duration of slow earthquakes, I study a chain reaction model in a population of brittle asperities based on a rate‐ and state‐dependent friction on a 3‐D subduction plate boundary. Simulation results show that the migration speed is quantitatively related to frictional properties by an analytical relation derived here. By assuming that local pore water in front of the migration drives rapid tremor reversal and is so local as to hold a constant stress drop, the application of the analytical solution to observational results suggests that (a) the temporal changes of observed migration speeds for the rapid tremor reversal could be explained by about 70% reduction of the effective normal stress; (b) effective normal stress for the deeper extension of seismogenic segment in the western part of Shikoku is about 1.5 times greater than that in the central part. Applying rupture time delay between slow earthquake asperities for the duration longer than regular earthquake, I also conclude that (c) the characteristic slip distance of rate‐and‐state friction for low‐frequency earthquakes is roughly between 30 µm and 30 mm; (d) the stress and strength drops of very low‐frequency earthquakes is much smaller than 1 MPa. Plain Language Summary Previous computer simulations and a few observational studies suggest that large subduction earthquakes may be preceded by slow earthquakes (not felt by humans) whose migration speed increases as the occurrence of the large earthquake approaches. So far, this precursory process has only been discussed qualitatively. In this study, I consider a chain reaction model on a heterogeneous fault made of small brittle asperities embedded in a viscous matrix: when a small asperity breaks rapidly, it generates a wave of slow slip around it, which in turn triggers the rupture of neighboring asperities, and so on. I develop a theoretical relation between slow earthquake migration speed and frictional properties. The model helps explain why slow earthquakes are slow, and provides a basis for precursory slow earthquake migration phenomena. The theoretical relation also provides an estimate of the characteristic slip distance of slow earthquakes, a rock property that is d
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To advance the obtained quantitative understanding of the migration process and long duration of slow earthquakes, I study a chain reaction model in a population of brittle asperities based on a rate‐ and state‐dependent friction on a 3‐D subduction plate boundary. Simulation results show that the migration speed is quantitatively related to frictional properties by an analytical relation derived here. By assuming that local pore water in front of the migration drives rapid tremor reversal and is so local as to hold a constant stress drop, the application of the analytical solution to observational results suggests that (a) the temporal changes of observed migration speeds for the rapid tremor reversal could be explained by about 70% reduction of the effective normal stress; (b) effective normal stress for the deeper extension of seismogenic segment in the western part of Shikoku is about 1.5 times greater than that in the central part. Applying rupture time delay between slow earthquake asperities for the duration longer than regular earthquake, I also conclude that (c) the characteristic slip distance of rate‐and‐state friction for low‐frequency earthquakes is roughly between 30 µm and 30 mm; (d) the stress and strength drops of very low‐frequency earthquakes is much smaller than 1 MPa. Plain Language Summary Previous computer simulations and a few observational studies suggest that large subduction earthquakes may be preceded by slow earthquakes (not felt by humans) whose migration speed increases as the occurrence of the large earthquake approaches. So far, this precursory process has only been discussed qualitatively. In this study, I consider a chain reaction model on a heterogeneous fault made of small brittle asperities embedded in a viscous matrix: when a small asperity breaks rapidly, it generates a wave of slow slip around it, which in turn triggers the rupture of neighboring asperities, and so on. I develop a theoretical relation between slow earthquake migration speed and frictional properties. The model helps explain why slow earthquakes are slow, and provides a basis for precursory slow earthquake migration phenomena. The theoretical relation also provides an estimate of the characteristic slip distance of slow earthquakes, a rock property that is difficult to extrapolate it to actual fault from laboratory experiments to natural scales. Key Points I propose a quantitative relation between slow earthquake migration speed and friction properties with observed stress drop I attribute the long duration of slow earthquakes to rupture time delays due to aseismic slip between seismic slip patches Characteristic slip distance for low‐frequency events is estimated as 30 μm∼30 mm, which is derived from propagation speed</description><identifier>ISSN: 2169-9313</identifier><identifier>EISSN: 2169-9356</identifier><identifier>DOI: 10.1029/2021JB023800</identifier><language>eng</language><publisher>Washington: Blackwell Publishing Ltd</publisher><subject>Asperity ; Distance ; Duration ; Earthquake prediction ; Earthquakes ; Exact solutions ; Friction ; friction law ; Geological faults ; Geophysics ; Laboratory experimentation ; Laboratory experiments ; low‐frequency tremor ; Mathematical models ; megathrust earthquake ; multi‐scale simulation ; Observational studies ; P-waves ; Plate boundaries ; Pore water ; Precursors ; Properties ; Rupture ; Rupturing ; Scaling ; Seismic activity ; Seismic waves ; Slip ; Subduction ; Subduction (geology) ; subduction zone ; Temporal variations ; Tremors ; very low‐frequency earthquake</subject><ispartof>Journal of geophysical research. 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Solid earth</title><description>Natural faults host various types of migrating slow earthquake phenomena, with migration speeds much lower than seismic wave speeds and different moment‐duration scaling from regular earthquakes. To advance the obtained quantitative understanding of the migration process and long duration of slow earthquakes, I study a chain reaction model in a population of brittle asperities based on a rate‐ and state‐dependent friction on a 3‐D subduction plate boundary. Simulation results show that the migration speed is quantitatively related to frictional properties by an analytical relation derived here. By assuming that local pore water in front of the migration drives rapid tremor reversal and is so local as to hold a constant stress drop, the application of the analytical solution to observational results suggests that (a) the temporal changes of observed migration speeds for the rapid tremor reversal could be explained by about 70% reduction of the effective normal stress; (b) effective normal stress for the deeper extension of seismogenic segment in the western part of Shikoku is about 1.5 times greater than that in the central part. Applying rupture time delay between slow earthquake asperities for the duration longer than regular earthquake, I also conclude that (c) the characteristic slip distance of rate‐and‐state friction for low‐frequency earthquakes is roughly between 30 µm and 30 mm; (d) the stress and strength drops of very low‐frequency earthquakes is much smaller than 1 MPa. Plain Language Summary Previous computer simulations and a few observational studies suggest that large subduction earthquakes may be preceded by slow earthquakes (not felt by humans) whose migration speed increases as the occurrence of the large earthquake approaches. So far, this precursory process has only been discussed qualitatively. In this study, I consider a chain reaction model on a heterogeneous fault made of small brittle asperities embedded in a viscous matrix: when a small asperity breaks rapidly, it generates a wave of slow slip around it, which in turn triggers the rupture of neighboring asperities, and so on. I develop a theoretical relation between slow earthquake migration speed and frictional properties. The model helps explain why slow earthquakes are slow, and provides a basis for precursory slow earthquake migration phenomena. The theoretical relation also provides an estimate of the characteristic slip distance of slow earthquakes, a rock property that is difficult to extrapolate it to actual fault from laboratory experiments to natural scales. Key Points I propose a quantitative relation between slow earthquake migration speed and friction properties with observed stress drop I attribute the long duration of slow earthquakes to rupture time delays due to aseismic slip between seismic slip patches Characteristic slip distance for low‐frequency events is estimated as 30 μm∼30 mm, which is derived from propagation speed</description><subject>Asperity</subject><subject>Distance</subject><subject>Duration</subject><subject>Earthquake prediction</subject><subject>Earthquakes</subject><subject>Exact solutions</subject><subject>Friction</subject><subject>friction law</subject><subject>Geological faults</subject><subject>Geophysics</subject><subject>Laboratory experimentation</subject><subject>Laboratory experiments</subject><subject>low‐frequency tremor</subject><subject>Mathematical models</subject><subject>megathrust earthquake</subject><subject>multi‐scale simulation</subject><subject>Observational studies</subject><subject>P-waves</subject><subject>Plate boundaries</subject><subject>Pore water</subject><subject>Precursors</subject><subject>Properties</subject><subject>Rupture</subject><subject>Rupturing</subject><subject>Scaling</subject><subject>Seismic activity</subject><subject>Seismic waves</subject><subject>Slip</subject><subject>Subduction</subject><subject>Subduction (geology)</subject><subject>subduction zone</subject><subject>Temporal variations</subject><subject>Tremors</subject><subject>very low‐frequency earthquake</subject><issn>2169-9313</issn><issn>2169-9356</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNp9kEFPAjEQhRujiQS9-QOaeHW17XS72yMQRAlGo3huut0uFIEu7RLk37uIMZ6cy0zmfXkveQhdUXJLCZN3jDA67hMGOSEnqMOokImEVJz-3hTO0WWMC9JO3r4o76Dx8LOx6-j8GvsK96J1ceUMflu6Gr8EX-uZbg7idG592OPGt5Lf4aEOzXyz1R8WP7lZ-GYu0Fmll9Fe_uwuer8fTgcPyeR59DjoTRLNcoDECJkZqYuMAxSCmqzUTHCTccEEy3kJlJVEClqkBaFFyTm3hufGaFrxCriELro--tbBb7Y2Nmrht2HdRiomZApc0Jy01M2RMsHHGGyl6uBWOuwVJepQmPpbWIvDEd-5pd3_y6rx6LWfphkD-AKgr2p2</recordid><startdate>202207</startdate><enddate>202207</enddate><creator>Ariyoshi, Keisuke</creator><general>Blackwell Publishing Ltd</general><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><orcidid>https://orcid.org/0000-0002-6353-1082</orcidid></search><sort><creationdate>202207</creationdate><title>Extension of Aseismic Slip Propagation Theory to Slow Earthquake Migration</title><author>Ariyoshi, Keisuke</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a2833-c697c9ab7433b61c7da264c74626284d312d0961b5b01bd444ec48cca1f4f3493</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>Asperity</topic><topic>Distance</topic><topic>Duration</topic><topic>Earthquake prediction</topic><topic>Earthquakes</topic><topic>Exact solutions</topic><topic>Friction</topic><topic>friction law</topic><topic>Geological faults</topic><topic>Geophysics</topic><topic>Laboratory experimentation</topic><topic>Laboratory experiments</topic><topic>low‐frequency tremor</topic><topic>Mathematical models</topic><topic>megathrust earthquake</topic><topic>multi‐scale simulation</topic><topic>Observational studies</topic><topic>P-waves</topic><topic>Plate boundaries</topic><topic>Pore water</topic><topic>Precursors</topic><topic>Properties</topic><topic>Rupture</topic><topic>Rupturing</topic><topic>Scaling</topic><topic>Seismic activity</topic><topic>Seismic waves</topic><topic>Slip</topic><topic>Subduction</topic><topic>Subduction (geology)</topic><topic>subduction zone</topic><topic>Temporal variations</topic><topic>Tremors</topic><topic>very low‐frequency earthquake</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ariyoshi, Keisuke</creatorcontrib><collection>CrossRef</collection><collection>Environment Abstracts</collection><collection>Meteorological &amp; 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Solid earth</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ariyoshi, Keisuke</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Extension of Aseismic Slip Propagation Theory to Slow Earthquake Migration</atitle><jtitle>Journal of geophysical research. Solid earth</jtitle><date>2022-07</date><risdate>2022</risdate><volume>127</volume><issue>7</issue><epage>n/a</epage><issn>2169-9313</issn><eissn>2169-9356</eissn><abstract>Natural faults host various types of migrating slow earthquake phenomena, with migration speeds much lower than seismic wave speeds and different moment‐duration scaling from regular earthquakes. To advance the obtained quantitative understanding of the migration process and long duration of slow earthquakes, I study a chain reaction model in a population of brittle asperities based on a rate‐ and state‐dependent friction on a 3‐D subduction plate boundary. Simulation results show that the migration speed is quantitatively related to frictional properties by an analytical relation derived here. By assuming that local pore water in front of the migration drives rapid tremor reversal and is so local as to hold a constant stress drop, the application of the analytical solution to observational results suggests that (a) the temporal changes of observed migration speeds for the rapid tremor reversal could be explained by about 70% reduction of the effective normal stress; (b) effective normal stress for the deeper extension of seismogenic segment in the western part of Shikoku is about 1.5 times greater than that in the central part. Applying rupture time delay between slow earthquake asperities for the duration longer than regular earthquake, I also conclude that (c) the characteristic slip distance of rate‐and‐state friction for low‐frequency earthquakes is roughly between 30 µm and 30 mm; (d) the stress and strength drops of very low‐frequency earthquakes is much smaller than 1 MPa. Plain Language Summary Previous computer simulations and a few observational studies suggest that large subduction earthquakes may be preceded by slow earthquakes (not felt by humans) whose migration speed increases as the occurrence of the large earthquake approaches. So far, this precursory process has only been discussed qualitatively. In this study, I consider a chain reaction model on a heterogeneous fault made of small brittle asperities embedded in a viscous matrix: when a small asperity breaks rapidly, it generates a wave of slow slip around it, which in turn triggers the rupture of neighboring asperities, and so on. I develop a theoretical relation between slow earthquake migration speed and frictional properties. The model helps explain why slow earthquakes are slow, and provides a basis for precursory slow earthquake migration phenomena. The theoretical relation also provides an estimate of the characteristic slip distance of slow earthquakes, a rock property that is difficult to extrapolate it to actual fault from laboratory experiments to natural scales. Key Points I propose a quantitative relation between slow earthquake migration speed and friction properties with observed stress drop I attribute the long duration of slow earthquakes to rupture time delays due to aseismic slip between seismic slip patches Characteristic slip distance for low‐frequency events is estimated as 30 μm∼30 mm, which is derived from propagation speed</abstract><cop>Washington</cop><pub>Blackwell Publishing Ltd</pub><doi>10.1029/2021JB023800</doi><tpages>19</tpages><orcidid>https://orcid.org/0000-0002-6353-1082</orcidid></addata></record>
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subjects Asperity
Distance
Duration
Earthquake prediction
Earthquakes
Exact solutions
Friction
friction law
Geological faults
Geophysics
Laboratory experimentation
Laboratory experiments
low‐frequency tremor
Mathematical models
megathrust earthquake
multi‐scale simulation
Observational studies
P-waves
Plate boundaries
Pore water
Precursors
Properties
Rupture
Rupturing
Scaling
Seismic activity
Seismic waves
Slip
Subduction
Subduction (geology)
subduction zone
Temporal variations
Tremors
very low‐frequency earthquake
title Extension of Aseismic Slip Propagation Theory to Slow Earthquake Migration
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