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Role of pore fluids in the generation of seismic precursors to shear fracture
A SYSTEMATIC study of temporal changes in seismic b -values (defined as the log-linear slope of the earthquake frequency–magnitude distribution) has shown that large earthquakes are often preceded by an intermediate-term increase in b , followed by a decrease in the months to weeks before the earthq...
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Published in: | Nature (London) 1992-09, Vol.359 (6392), p.228-230 |
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creator | Sammonds, P. R Meredith, P. G Main, I. G |
description | A SYSTEMATIC study of temporal changes in seismic
b
-values (defined as the log-linear slope of the earthquake frequency–magnitude distribution) has shown that large earthquakes are often preceded by an intermediate-term increase in
b
, followed by a decrease in the months to weeks before the earthquake
1
. The onset of the
b
-value increase can precede earthquake occurrence by as much as 7 years. A recently proposed fracture mechanics model of the earthquake source
2
explains these temporal fluctuations in
b
in terms of the underlying physical processes of time-varying applied stress and crack growth. The model predicts two minima in
b
, separated by a short-lived maximum. Here we report the results of controlled laboratory deformation experiments, done in simulated upper-crustal conditions on both air-dried and water-saturated rock specimens. As found in previous experiments
3–5
, shear fracture in dry specimens is characterized by a decline in
b
during anelastic deformation to a single minimum reached just before failure. But in water-saturated specimens, when pore-fluid volume is kept constant by servo-control we also observe a second, intermediate-term
b
-value minimum, so reproducing the double
b
-value anomaly predicted by the model
2
. |
doi_str_mv | 10.1038/359228a0 |
format | article |
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b
-values (defined as the log-linear slope of the earthquake frequency–magnitude distribution) has shown that large earthquakes are often preceded by an intermediate-term increase in
b
, followed by a decrease in the months to weeks before the earthquake
1
. The onset of the
b
-value increase can precede earthquake occurrence by as much as 7 years. A recently proposed fracture mechanics model of the earthquake source
2
explains these temporal fluctuations in
b
in terms of the underlying physical processes of time-varying applied stress and crack growth. The model predicts two minima in
b
, separated by a short-lived maximum. Here we report the results of controlled laboratory deformation experiments, done in simulated upper-crustal conditions on both air-dried and water-saturated rock specimens. As found in previous experiments
3–5
, shear fracture in dry specimens is characterized by a decline in
b
during anelastic deformation to a single minimum reached just before failure. But in water-saturated specimens, when pore-fluid volume is kept constant by servo-control we also observe a second, intermediate-term
b
-value minimum, so reproducing the double
b
-value anomaly predicted by the model
2
.</description><identifier>ISSN: 0028-0836</identifier><identifier>EISSN: 1476-4687</identifier><identifier>DOI: 10.1038/359228a0</identifier><identifier>CODEN: NATUAS</identifier><language>eng</language><publisher>London: Nature Publishing Group UK</publisher><subject>Earth sciences ; Earth, ocean, space ; Earthquakes ; Earthquakes, seismology ; Engineering and environment geology. Geothermics ; Exact sciences and technology ; Humanities and Social Sciences ; Internal geophysics ; letter ; multidisciplinary ; Natural hazards: prediction, damages, etc ; Plate tectonics ; Science ; Science (multidisciplinary) ; Seismic activity</subject><ispartof>Nature (London), 1992-09, Vol.359 (6392), p.228-230</ispartof><rights>Springer Nature Limited 1992</rights><rights>1992 INIST-CNRS</rights><rights>Copyright Macmillan Journals Ltd. Sep 17, 1992</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-a427t-5ea989ca858010c3591e09f18adc8a4e9431edd0c066b2c980209d989ec0db7b3</citedby><cites>FETCH-LOGICAL-a427t-5ea989ca858010c3591e09f18adc8a4e9431edd0c066b2c980209d989ec0db7b3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,2727,27924,27925</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=5556012$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Sammonds, P. R</creatorcontrib><creatorcontrib>Meredith, P. G</creatorcontrib><creatorcontrib>Main, I. G</creatorcontrib><title>Role of pore fluids in the generation of seismic precursors to shear fracture</title><title>Nature (London)</title><addtitle>Nature</addtitle><description>A SYSTEMATIC study of temporal changes in seismic
b
-values (defined as the log-linear slope of the earthquake frequency–magnitude distribution) has shown that large earthquakes are often preceded by an intermediate-term increase in
b
, followed by a decrease in the months to weeks before the earthquake
1
. The onset of the
b
-value increase can precede earthquake occurrence by as much as 7 years. A recently proposed fracture mechanics model of the earthquake source
2
explains these temporal fluctuations in
b
in terms of the underlying physical processes of time-varying applied stress and crack growth. The model predicts two minima in
b
, separated by a short-lived maximum. Here we report the results of controlled laboratory deformation experiments, done in simulated upper-crustal conditions on both air-dried and water-saturated rock specimens. As found in previous experiments
3–5
, shear fracture in dry specimens is characterized by a decline in
b
during anelastic deformation to a single minimum reached just before failure. But in water-saturated specimens, when pore-fluid volume is kept constant by servo-control we also observe a second, intermediate-term
b
-value minimum, so reproducing the double
b
-value anomaly predicted by the model
2
.</description><subject>Earth sciences</subject><subject>Earth, ocean, space</subject><subject>Earthquakes</subject><subject>Earthquakes, seismology</subject><subject>Engineering and environment geology. Geothermics</subject><subject>Exact sciences and technology</subject><subject>Humanities and Social Sciences</subject><subject>Internal geophysics</subject><subject>letter</subject><subject>multidisciplinary</subject><subject>Natural hazards: prediction, damages, etc</subject><subject>Plate tectonics</subject><subject>Science</subject><subject>Science (multidisciplinary)</subject><subject>Seismic activity</subject><issn>0028-0836</issn><issn>1476-4687</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1992</creationdate><recordtype>article</recordtype><recordid>eNpt0E9LwzAYBvAgCs4p-AkkiAc9VN-kSZscZfgPJoLouWTp262ja2rSHvz2ZnTOi6cc8svz5n0IOWdwyyBVd6nUnCsDB2TCRJ4lIlP5IZkAcJWASrNjchLCGgAky8WEvL67BqmraOc80qoZ6jLQuqX9CukSW_Smr127BQHrsKkt7TzawQfnA-0dDSs0nlbe2H7weEqOKtMEPNudU_L5-PAxe07mb08vs_t5YgTP-0Si0Upbo6QCBjZ-mSHoiilTWmUEapEyLEuwkGULbrUCDrqMT9BCucgX6ZRcjrmdd18Dhr5Yu8G3cWTBQQjBNYeIrkdkvQvBY1V0vt4Y_10wKLZdFb9dRXq1yzPBmiau09o67L2UMgPGI7sZWYg37RL939h_Ii9G25ptM_usPfgBSiN-9A</recordid><startdate>19920917</startdate><enddate>19920917</enddate><creator>Sammonds, P. 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R</au><au>Meredith, P. G</au><au>Main, I. G</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Role of pore fluids in the generation of seismic precursors to shear fracture</atitle><jtitle>Nature (London)</jtitle><stitle>Nature</stitle><date>1992-09-17</date><risdate>1992</risdate><volume>359</volume><issue>6392</issue><spage>228</spage><epage>230</epage><pages>228-230</pages><issn>0028-0836</issn><eissn>1476-4687</eissn><coden>NATUAS</coden><abstract>A SYSTEMATIC study of temporal changes in seismic
b
-values (defined as the log-linear slope of the earthquake frequency–magnitude distribution) has shown that large earthquakes are often preceded by an intermediate-term increase in
b
, followed by a decrease in the months to weeks before the earthquake
1
. The onset of the
b
-value increase can precede earthquake occurrence by as much as 7 years. A recently proposed fracture mechanics model of the earthquake source
2
explains these temporal fluctuations in
b
in terms of the underlying physical processes of time-varying applied stress and crack growth. The model predicts two minima in
b
, separated by a short-lived maximum. Here we report the results of controlled laboratory deformation experiments, done in simulated upper-crustal conditions on both air-dried and water-saturated rock specimens. As found in previous experiments
3–5
, shear fracture in dry specimens is characterized by a decline in
b
during anelastic deformation to a single minimum reached just before failure. But in water-saturated specimens, when pore-fluid volume is kept constant by servo-control we also observe a second, intermediate-term
b
-value minimum, so reproducing the double
b
-value anomaly predicted by the model
2
.</abstract><cop>London</cop><pub>Nature Publishing Group UK</pub><doi>10.1038/359228a0</doi><tpages>3</tpages></addata></record> |
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subjects | Earth sciences Earth, ocean, space Earthquakes Earthquakes, seismology Engineering and environment geology. Geothermics Exact sciences and technology Humanities and Social Sciences Internal geophysics letter multidisciplinary Natural hazards: prediction, damages, etc Plate tectonics Science Science (multidisciplinary) Seismic activity |
title | Role of pore fluids in the generation of seismic precursors to shear fracture |
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