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  • 11
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    In:  Journal of Geophysical Research, Warszawa, Elsevier, vol. 103, no. B5, pp. 9691-9712, pp. 2382, (ISBN: 0-12-018847-3)
    Publication Date: 1998
    Keywords: Rheology ; Inelastic ; Laboratory measurements ; Physical properties of rocks ; JGR
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  • 12
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    In:  Tectonophys., Stockholm, Wissenschaftliche Buchgesellschaft, vol. 277, no. 1-3, pp. 57-81, pp. L15318, (ISSN: 1340-4202)
    Publication Date: 1997
    Keywords: Fault zone ; Rock mechanics ; Modelling ; Seismicity ; Fracture
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  • 13
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    In:  J. Geophys. Res., Tübingen, Europ. Ass. Exploration Geophys., vol. 99, no. Sonderband IV/2000, pp. 18159-18173, pp. 2017, (ISSN: 1340-4202)
    Publication Date: 1994
    Keywords: Fracture ; cracks and fractures (.NE. fracturing) ; JGR
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  • 14
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    Elsevier / Academic Press
    In:  Bull., Polar Proj. OP-O3A4, International Handbook of Earthquake and Engineering Seismology - Part A, Amsterdam, Elsevier / Academic Press, vol. 81A, no. 4, pp. 505-537, (ISBN 0080419208)
    Publication Date: 2002
    Keywords: Seismology ; Stress ; Fracture ; Rock mechanics ; Review article
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  • 15
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    American Geophysical Union
    In:  Bull., Polar Proj. OP-O3A4, Rock Physics & Phase Relations - A Handbook of Physical Constants, Washington, D.C., American Geophysical Union, vol. 1, no. 4, pp. 127-147, (ISBN 0080419208)
    Publication Date: 1995
    Keywords: Rock mechanics ; Geochemistry ; Physical properties of rocks ; Mineralogy ; Review article
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  • 16
    Publication Date: 2012-10-09
    Description: After nucleation, a large earthquake propagates as an expanding rupture front along a fault. This front activates countless fault patches that slip by consuming energy stored in Earth's crust. We simulated the slip of a fault patch by rapidly loading an experimental fault with energy stored in a spinning flywheel. The spontaneous evolution of strength, acceleration, and velocity indicates that our experiments are proxies of fault-patch behavior during earthquakes of moment magnitude (M(w)) = 4 to 8. We show that seismically determined earthquake parameters (e.g., displacement, velocity, magnitude, or fracture energy) can be used to estimate the intensity of the energy release during an earthquake. Our experiments further indicate that high acceleration imposed by the earthquake's rupture front quickens dynamic weakening by intense wear of the fault zone.〈br /〉〈span class="detail_caption"〉Notes: 〈/span〉Chang, J C -- Lockner, D A -- Reches, Z -- New York, N.Y. -- Science. 2012 Oct 5;338(6103):101-5. doi: 10.1126/science.1221195.〈br /〉〈span class="detail_caption"〉Author address: 〈/span〉Geology and Geophysics, University of Oklahoma, 100 East Boyd Street, Norman, OK 73019, USA.〈br /〉〈span class="detail_caption"〉Record origin:〈/span〉 〈a href="http://www.ncbi.nlm.nih.gov/pubmed/23042892" target="_blank"〉PubMed〈/a〉
    Keywords: *Acceleration ; *Earthquakes ; Laboratories
    Print ISSN: 0036-8075
    Electronic ISSN: 1095-9203
    Topics: Biology , Chemistry and Pharmacology , Computer Science , Medicine , Natural Sciences in General , Physics
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  • 17
    Publication Date: 2015-12-15
    Description: We performed flow-through laboratory experiments on 5 cylindrically cored samples of ultramafic rocks, in which we generated a well-mated through-going tensile fracture, to investigate evolution of fracture permeability during serpentinization. The samples were tested in a triaxial loading machine at a confining pressure of 50 MPa, pore pressure of 20 MPa, and temperature of 260 °C, simulating a depth of 2 km under hydrostatic conditions. A pore-pressure difference of up to 2 MPa was imposed across the ends of the sample. Fracture permeability decreased by one to two orders of magnitude during the 200 to 340 hour experiments. Electron microprobe and SEM data indicated the formation of needle-shaped crystals of serpentine composition along the walls of the fracture, and chemical analyses of sampled pore fluids were consistent with dissolution of ferro-magnesian minerals. By comparing the difference between fracture permeability and matrix permeability measured on intact samples of the same rock types, we concluded that the contribution of the low matrix permeability to flow is negligible and essentially all of the flow is focused in the tensile fracture. The experimental results suggest that the fracture network in long-lived hydrothermal circulation systems can be sealed rapidly as a result of mineral precipitation, and generation of new permeability resulting from a combination of tectonic and crystallization-induced stresses is required to maintain fluid circulation. This article is protected by copyright. All rights reserved.
    Electronic ISSN: 1525-2027
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Published by Wiley on behalf of American Geophysical Union (AGU).
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  • 18
    Publication Date: 2011-03-29
    Description: The San Andreas fault accommodates 28-34 mm yr(-1) of right lateral motion of the Pacific crustal plate northwestward past the North American plate. In California, the fault is composed of two distinct locked segments that have produced great earthquakes in historical times, separated by a 150-km-long creeping zone. The San Andreas Fault Observatory at Depth (SAFOD) is a scientific borehole located northwest of Parkfield, California, near the southern end of the creeping zone. Core was recovered from across the actively deforming San Andreas fault at a vertical depth of 2.7 km (ref. 1). Here we report laboratory strength measurements of these fault core materials at in situ conditions, demonstrating that at this locality and this depth the San Andreas fault is profoundly weak (coefficient of friction, 0.15) owing to the presence of the smectite clay mineral saponite, which is one of the weakest phyllosilicates known. This Mg-rich clay is the low-temperature product of metasomatic reactions between the quartzofeldspathic wall rocks and serpentinite blocks in the fault. These findings provide strong evidence that deformation of the mechanically unusual creeping portions of the San Andreas fault system is controlled by the presence of weak minerals rather than by high fluid pressure or other proposed mechanisms. The combination of these measurements of fault core strength with borehole observations yields a self-consistent picture of the stress state of the San Andreas fault at the SAFOD site, in which the fault is intrinsically weak in an otherwise strong crust.〈br /〉〈span class="detail_caption"〉Notes: 〈/span〉Lockner, David A -- Morrow, Carolyn -- Moore, Diane -- Hickman, Stephen -- England -- Nature. 2011 Apr 7;472(7341):82-5. doi: 10.1038/nature09927. Epub 2011 Mar 23.〈br /〉〈span class="detail_caption"〉Author address: 〈/span〉US Geological Survey, Menlo Park, California 94025, USA. dlockner@usgs.gov〈br /〉〈span class="detail_caption"〉Record origin:〈/span〉 〈a href="http://www.ncbi.nlm.nih.gov/pubmed/21441903" target="_blank"〉PubMed〈/a〉
    Print ISSN: 0028-0836
    Electronic ISSN: 1476-4687
    Topics: Biology , Chemistry and Pharmacology , Medicine , Natural Sciences in General , Physics
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  • 19
    Publication Date: 1994-09-09
    Description: The addition of hydrothermal fluids to heated, intact granite leads to permeability reductions in the temperature range of 300 degrees to 500 degrees C, with the rate of change generally increasing with increasing temperature. The addition of gouge enhances the rate of permeability reduction because of the greater reactivity of the fine material. Flow rate is initially high in a throughgoing fracture but eventually drops to the level of intact granite. These results support the fault-valve model for the development of mesothermal ore deposits, in which seals are formed at the base of the seismogenic zone of high-angle thrust faults. The lower temperature results yield varying estimates of mineral-sealing rates at shallower depths in fault zones, although they generally support the hypothesis that such seals develop in less time than the recurrence interval for moderate to large earthquakes on the San Andreas fault.〈br /〉〈span class="detail_caption"〉Notes: 〈/span〉Moore, D E -- Lockner, D A -- Byerlee, J D -- New York, N.Y. -- Science. 1994 Sep 9;265(5178):1558-61.〈br /〉〈span class="detail_caption"〉Record origin:〈/span〉 〈a href="http://www.ncbi.nlm.nih.gov/pubmed/17801532" target="_blank"〉PubMed〈/a〉
    Print ISSN: 0036-8075
    Electronic ISSN: 1095-9203
    Topics: Biology , Chemistry and Pharmacology , Computer Science , Medicine , Natural Sciences in General , Physics
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  • 20
    Publication Date: 2017-10-10
    Description: Coseismic frictional melting and the production of quenched glass called pseudotachylyte is a recurring process during earthquakes. To investigate how glassy materials affect the postseismic strength and stability of faults, obsidian gouges were sheared under dry and wet conditions from 200 °C to 300 °C at ~150 MPa effective normal stress. Dry glass exhibited a brittle rheology at all conditions tested, exhibiting friction values and microstructures consistent with siliciclastic materials. Likewise, wet glass at 200 °C exhibited a brittle rheology. In contrast, wet gouges at 300 °C transitioned from brittle sliding to linear-viscous (Newtonian) flow at strain rates 〈 3x10 -4 s -1 , indicating melt-like behavior. The viscosity ranged from 2x10 11 to 7.8x10 11 Pa-s. Microstructures show viscous gouges were fully welded with rod-shaped microlites rotated into the flow direction. Fourier transform infrared spectroscopy along with electron backscatter imaging demonstrate that hydration of the glass by diffusion of pore water was the dominant process reducing the viscosity and promoting viscous flow. As much as 5 wt% water diffused into the glass. These results may provide insight into postseismic-slip behaviors and challenge some interpretations of fault kinematics based on studies assuming pseudotachylyte formation and flow is solely coseismic.
    Print ISSN: 0094-8276
    Electronic ISSN: 1944-8007
    Topics: Geosciences , Physics
    Published by Wiley on behalf of American Geophysical Union (AGU).
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