Character and Origin of Cataclasite Developed Along the Low-Angle Whipple Detachment Fault, Whipple Mountains, California
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Significance of Brittle Deformation in the Footwall
Journal of Structural Geology 64 (2014) 79e98 Contents lists available at SciVerse ScienceDirect Journal of Structural Geology journal homepage: www.elsevier.com/locate/jsg Significance of brittle deformation in the footwall of the Alpine Fault, New Zealand: Smithy Creek Fault zone J.-E. Lund Snee a,*,1, V.G. Toy a, K. Gessner b a Geology Department, University of Otago, PO Box 56, Dunedin 9016, New Zealand b Western Australian Geothermal Centre of Excellence, The University of Western Australia, 35 Stirling Highway, Crawley, WA 6009, Australia article info abstract Article history: The Smithy Creek Fault represents a rare exposure of a brittle fault zone within Australian Plate rocks that Received 28 January 2013 constitute the footwall of the Alpine Fault zone in Westland, New Zealand. Outcrop mapping and Received in revised form paleostress analysis of the Smithy Creek Fault were conducted to characterize deformation and miner- 22 May 2013 alization in the footwall of the nearby Alpine Fault, and the timing of these processes relative to the Accepted 4 June 2013 modern tectonic regime. While unfavorably oriented, the dextral oblique Smithy Creek thrust has Available online 18 June 2013 kinematics compatible with slip in the current stress regime and offsets a basement unconformity beneath Holocene glaciofluvial sediments. A greater than 100 m wide damage zone and more than 8 m Keywords: Fault zone wide, extensively fractured fault core are consistent with total displacement on the kilometer scale. e Fluid flow Based on our observations we propose that an asymmetric damage zone containing quartz carbonate Hydrofracture echloriteeepidote veins is focused in the footwall. -
Deformation Mechanisms, Rheology and Tectonics Geological Society Special Publications Series Editor J
Deformation Mechanisms, Rheology and Tectonics Geological Society Special Publications Series Editor J. BROOKS J/iLl THIS VOLUME IS DEDICATED TO THE WORK OF HENDRIK JAN ZWART GEOLOGICAL SOCIETY SPECIAL PUBLICATION NO. 54 Deformation Mechanisms, Rheology and Tectonics EDITED BY R. J. KNIPE Department of Earth Sciences Leeds University UK & E. H. RUTTER Department of Geology Manchester University UK ASSISTED BY S. M. AGAR R. D. LAW Department of Earth Sciences Department of Geological Sciences Leeds University Virginia University UK USA D. J. PRIOR R. L. M. VISSERS Department of Earth Sciences Institute of Earth Sciences Liverpool University University of Utrceht UK Netherlands 1990 Published by The Geological Society London THE GEOLOGICAL SOCIETY The Geological Society of London was founded in 1807 for the purposes of 'investigating the mineral structures of the earth'. It received its Royal Charter in 1825. The Society promotes all aspects of geological science by means of meetings, speeiat lectures and courses, discussions, specialist groups, publications and library services. It is expected that candidates for Fellowship will be graduates in geology or another earth science, or have equivalent qualifications or experience. Alt Fellows are entitled to receive for their subscription one of the Society's three journals: The Quarterly Journal of Engineering Geology, the Journal of the Geological Society or Marine and Petroleum Geology. On payment of an additional sum on the annual subscription, members may obtain copies of another journal. Membership of the specialist groups is open to all Fellows without additional charge. Enquiries concerning Fellowship of the Society and membership of the specialist groups should be directed to the Executive Secretary, The Geological Society, Burlington House, Piccadilly, London W1V 0JU. -
Lithology and Internal Structure of the San Andreas Fault at Depth Based
1 1 Lithology and Internal Structure of the San Andreas Fault at depth based on 2 characterization of Phase 3 whole-rock core in the San Andreas Fault Observatory at 3 Depth (SAFOD) Borehole 4 By Kelly K. Bradbury1, James P. Evans1, Judith S. Chester2, Frederick M. Chester2, and David L. Kirschner3 5 1Geology Department, Utah State University, Logan, UT 84321-4505 6 2Center for Tectonophysics and Department of Geology and Geophysics, Texas A&M University, College Station, 7 Texas 77843 8 3Department of Earth and Atmospheric Sciences, St. Louis University, St. Louis, Missouri 63108 9 10 Abstract 11 We characterize the lithology and structure of the spot core obtained in 2007 during 12 Phase 3 drilling of the San Andreas Fault Observatory at Depth (SAFOD) in order to determine 13 the composition, structure, and deformation processes of the fault zone at 3 km depth where 14 creep and microseismicity occur. A total of approximately 41 m of spot core was taken from 15 three separate sections of the borehole; the core samples consist of fractured arkosic sandstones 16 and shale west of the SAF zone (Pacific Plate) and sheared fine-grained sedimentary rocks, 17 ultrafine black fault-related rocks, and phyllosilicate-rich fault gouge within the fault zone 18 (North American Plate). The fault zone at SAFOD consists of a broad zone of variably damaged 19 rock containing localized zones of highly concentrated shear that often juxtapose distinct 20 protoliths. Two zones of serpentinite-bearing clay gouge, each meters-thick, occur at the two 21 locations of aseismic creep identified in the borehole on the basis of casing deformation. -
Faults and Joints
133 JOINTS Joints (also termed extensional fractures) are planes of separation on which no or undetectable shear displacement has taken place. The two walls of the resulting tiny opening typically remain in tight (matching) contact. Joints may result from regional tectonics (i.e. the compressive stresses in front of a mountain belt), folding (due to curvature of bedding), faulting, or internal stress release during uplift or cooling. They often form under high fluid pressure (i.e. low effective stress), perpendicular to the smallest principal stress. The aperture of a joint is the space between its two walls measured perpendicularly to the mean plane. Apertures can be open (resulting in permeability enhancement) or occluded by mineral cement (resulting in permeability reduction). A joint with a large aperture (> few mm) is a fissure. The mechanical layer thickness of the deforming rock controls joint growth. If present in sufficient number, open joints may provide adequate porosity and permeability such that an otherwise impermeable rock may become a productive fractured reservoir. In quarrying, the largest block size depends on joint frequency; abundant fractures are desirable for quarrying crushed rock and gravel. Joint sets and systems Joints are ubiquitous features of rock exposures and often form families of straight to curviplanar fractures typically perpendicular to the layer boundaries in sedimentary rocks. A set is a group of joints with similar orientation and morphology. Several sets usually occur at the same place with no apparent interaction, giving exposures a blocky or fragmented appearance. Two or more sets of joints present together in an exposure compose a joint system. -
Song of the Year
General Field Page 1 of 15 Category 3 - Song Of The Year 015. AMAZING 031. AYO TECHNOLOGY Category 3 Seal, songwriter (Seal) N. Hills, Curtis Jackson, Timothy Song Of The Year 016. AMBITIONS Mosley & Justin Timberlake, A Songwriter(s) Award. A song is eligible if it was Rudy Roopchan, songwriter songwriters (50 Cent Featuring Justin first released or if it first achieved prominence (Sunchasers) Timberlake & Timbaland) during the Eligibility Year. (Artist names appear in parentheses.) Singles or Tracks only. 017. AMERICAN ANTHEM 032. BABY Angie Stone & Charles Tatum, 001. THE ACTRESS Gene Scheer, songwriter (Norah Jones) songwriters; Curtis Mayfield & K. Tiffany Petrossi, songwriter (Tiffany 018. AMNESIA Norton, songwriters (Angie Stone Petrossi) Brian Lapin, Mozella & Shelly Peiken, Featuring Betty Wright) 002. AFTER HOURS songwriters (Mozella) Dennis Bell, Julia Garrison, Kim 019. AND THE RAIN 033. BACK IN JUNE José Promis, songwriter (José Promis) Outerbridge & Victor Sanchez, Buck Aaron Thomas & Gary Wayne songwriters (Infinite Embrace Zaiontz, songwriters (Jokers Wild 034. BACK IN YOUR HEAD Featuring Casey Benjamin) Band) Sara Quin & Tegan Quin, songwriters (Tegan And Sara) 003. AFTER YOU 020. ANDUHYAUN Dick Wagner, songwriter (Wensday) Jimmy Lee Young, songwriter (Jimmy 035. BARTENDER Akon Thiam & T-Pain, songwriters 004. AGAIN & AGAIN Lee Young) (T-Pain Featuring Akon) Inara George & Greg Kurstin, 021. ANGEL songwriters (The Bird And The Bee) Chris Cartier, songwriter (Chris 036. BE GOOD OR BE GONE Fionn Regan, songwriter (Fionn 005. AIN'T NO TIME Cartier) Regan) Grace Potter, songwriter (Grace Potter 022. ANGEL & The Nocturnals) Chaka Khan & James Q. Wright, 037. BE GOOD TO ME Kara DioGuardi, Niclas Molinder & 006. -
Deformation at the Microscale
Deformation at the Microscale Deformation processes occur at the microscale and lead to changes in the internal structure, shape or volume of a rock. Brittle versus Plastic deformation mechanisms is a function of: • Pressure – increasing pressure favors plastic deformation • Temperature – increasing temperature favors plastic deformation • Rheology of the deforming minerals (for example quartz vs feldspar) • Availability of fluids – favors brittle deformation • Strain rate – lower strain rate favors plastic deformation Given the different rheology of different minerals, brittle and plastic deformation mechanisms can occur in the same sample under the same conditions. The controlling deformation mechanism determines whether the deformation belongs to the brittle or plastic regime. Brittle deformation mechanisms operative at shallow depths. Crystal-plastic Deformation Mechanisms Mechanical twining – mechanical bending or kinking of the crystal structure. Mechanical twins in calcite Deformation (glide) twins in a calcite crystal. Stress is ideally at 45o to the shear In the case of calcite, the 38o angle (glide plane). Dark lamellae turns the twin plane into a mirror have been sheared (simple plane. The amount of strain shear). associated with a single kink is fixed by this angle. Crystal Defects • Point defects – due to vacancies or impurities in the crystal structure. • Line defects (dislocations) – a mobile line defect that causes intracrystalline deformation via slip. The slip plane is usually the place in a crystal that has the highest density of atoms. • Plane defects – grain boundaries, subgrain boundaries, and twin planes. Migration of vacancies Types of defects – vacancy, through a crystal structure by substitution, interstitial diffusion. The movement of dislocations occurs in the plane or direction which requires the least energy. -
Actually Consists of 2 Cleavages
Types of foliations • Crenulation Cleavage- – Actually consists of 2 cleavages – The first may be a slaty cleavage or schistosity that becomes microfolded – Fold axial planes typically form at high angle to the σ1 of the second compressional phase 1 Progressive development (a → c) of a crenulation cleavage for both asymmetric (top) and symmetric (bottom) situations. From Spry (1969) Metamorphic Textures. Pergamon. Oxford. 2 Figure 23.24a. Symmetrical crenulation cleavages in amphibole-quartz-rich schist. Note concentration of quartz in hinge areas. From Borradaile et al. (1982) Atlas of Deformational and Metamorphic Rock Fabrics. Springer-Verlag. 3 Figure 23.24b. Asymmetric crenulation cleavages in mica-quartz-rich schist. Note horizontal compositional layering (relict bedding) and preferential dissolution of quartz from one limb of the folds. From Borradaile et al. (1982) Atlas of Deformational and Metamorphic Rock Fabrics. Springer-Verlag. 4 Figure 23.25. Stages in the development of crenulation cleavage as a function of temperature and intensity of the second deformation. From Passchier and Trouw (1996) Microtectonics. Springer-Verlag. Development of S2 micas depends upon T and the intensity of the second deformation 5 Types of lineations a. Preferred orientation of elongated mineral aggregates b. Preferred orientation of elongate minerals c. Lineation defined by platy minerals d. Fold axes (especially of crenulations) e. Intersecting planar elements. Figure 23.26. Types of fabric elements that define a lineation. From Turner and Weiss (1963) Structural 6 Analysis of Metamorphic Tectonites. McGraw Hill. Analysis of Deformed Rocks • If two or more geometric elements are present, we can add a numeric subscript to denote the chronological sequence in which they were developed and superimposed- • Deformational events: D1 D2 D3 … • Metamorphic events: M1 M2 M3 … • Foliations: So S1 S2 S3 … • Lineations: Lo L1 L2 L3 … • Plot on a metamorphism-deformation-time plot showing the crystallization of each mineral 7 Deformation vs. -
Stress and Fluid Control on De Collement Within Competent Limestone
Journal of Structural Geology 22 (2000) 349±371 www.elsevier.nl/locate/jstrugeo Stress and ¯uid control on de collement within competent limestone Antonio Teixell a,*, David W. Durney b, Maria-Luisa Arboleya a aDepartament de Geologia, Universitat AutoÁnoma de Barcelona, 08193 Bellaterra, Spain bDepartment of Earth and Planetary Sciences, Macquarie University, Sydney, NSW 2109, Australia Received 5 October 1998; accepted 23 September 1999 Abstract The Larra thrust of the Pyrenees is a bedding-parallel de collement located within a competent limestone unit. It forms the ¯oor of a thrust system of hectometric-scale imbrications developed beneath a synorogenic basin. The fault rock at the de collement is a dense stack of mainly bedding-parallel calcite veins with variable internal deformation by twinning and recrystallization. Veins developed as extension fractures parallel to a horizontal maximum compressive stress, cemented by cavity-type crystals. Conditions during vein formation are interpreted in terms of a compressional model where crack-arrays develop at applied stresses approaching the shear strength of the rock and at ¯uid pressures equal to or less than the overburden pressure. The cracks developed in response to high dierential stress, which was channelled in the strong limestone, and high ¯uid pressure in or below the thrust plane. Ductile deformation, although conspicuous, cannot account for the kilometric displacement of the thrust, which was mostly accommodated by slip on water sills constituted by open cracks. A model of cyclic dierential brittle contraction, stress reorientation, slip and ductile relaxation at a rheological step in the limestone is proposed as a mechanism for episodic de collement movement. -
Essentials for Getting Things Done in Complex Organizations Susan Z
MASTER THE MATRIX MASTER YOU’RE IN A MATRIX, WHETHER YOU REALIZE IT OR NOT. HERE’S THE TEST: Do you have multiple bosses (one may be referred to as “solid line” and others as “dotted line”)? Do you depend on a variety of resources through- out the organization to get your tasks done, and : do these resources report to other people, teams 7 or organizations? ESSENTIALS FOR GETTING THINGS DONE IN COMPLEX ORGANIZATIONS SUSAN Z. FINERTY FOR GETTING THINGS DONE IN COMPLEX ORGANIZATIONS ESSENTIALS IF YOU ANSWERED “YES” TO EITHER OF THESE, you work in a matrix role—whether your organization calls itself a matrix or not. You get results by navigating either a matrix above or surrounding you. MASTER Matrix roles are everywhere. The field customer contact person who has to work through a maze of resources to write contracts, negotiate delivery and troubleshoot product issues is in a matrix role. The product manager in Italy who is simul- taneously accountable for numbers in her country, region and business unit despite the fact that they are in conflict, is in a matrix role. And the HR person who reports to a globalized THE ABOUT THE AUTHOR HR function, with a dotted line to the head of the business 7ESSENTIALS he supports? Yes, again a matrix role. Susan Finerty has been working Master the Matrix: 7 Essentials for Getting Things in matrix roles and with matrix Done in Complex Organizations is based on the experiences organizations for more than FOR and ideas of over 100 matrix practioners. The frameworks, 20 years. -
Post-Seismic Deformation Mechanism of the July 2015 MW 6.5 Pishan
www.nature.com/scientificreports OPEN Post‑seismic deformation mechanism of the July 2015 MW 6.5 Pishan earthquake revealed by Sentinel‑1A InSAR observation Sijia Wang1*, Yongzhi Zhang1,2*, Yipeng Wang1, Jiashuang Jiao 1, Zongtong Ji1 & Ming Han1 On 3 July 2015, the Mw 6.5 Pishan earthquake occurred at the junction of the southwestern margin of the Tarim Basin and the northwestern margin of the Tibetan Plateau. To understand the seismogenic mechanism and the post‑seismic deformation behavior, we investigated the characteristics of the post‑seismic deformation felds in the seismic area, using 9 Sentinel‑1A TOPS synthetic aperture radar (SAR) images acquired from 18 July 2015 to 22 September 2016 with the Small Baseline Subset Interferometric SAR (SBAS‑InSAR) technique. Postseismic LOS deformation displayed logarithmic behavior, and the temporal evolution of the post‑seismic deformation is consistent with the aftershock sequence. The main driving mechanism of near‑feld post‑seismic displacement was most likely to be afterslip on the fault and the entire creep process consists of three creeping stages. Afterward, we used the steepest descent method to invert the afterslip evolution process and analyzed the relationship between post‑seismic afterslip and co‑seismic slip. The results witness that 447 days after the mainshock (22 September 2016), the afterslip was concentrated within one principal slip center. It was located 5–25 km along the fault strike, 0–10 km along with the fault dip, with a cumulative peak slip of 0.18 m. The 447 days afterslip seismic moment was approximately 2.65 × 1017 N m, accounting for approximately 4.1% of the co‑seismic geodetic moment. -
LIBRO GEOLOGIA 30.Qxd:Maquetaciûn 1
Trabajos de Geología, Universidad de Oviedo, 30 : 163-168 (2010) Peek inside the black box of calcite twinning paleostress analysis J. REZ1* AND R. MELICHAR1 1Department of Geological Sciences, Faculty of Science, Masaryk University, Kotlarska 2, 61137 Brno, Czech Republic. *e-mail: [email protected] Abstract: Calcite e-twinning has been used for stress inversion purposes since the fifties. The common- ly used technique is the Etchecopar method (e.g. Laurent et al., 1981), based on testing of 500-1000 randomly generated reduced stress tensors using a penalization function fL. A systematic search of all possible reduced stress tensors with a new penalization function fR double checked with a spatial dis- tribution plot is suggested. Keywords: stress inversion, paleostress analysis, calcite, mechanical twinning. Extensive research of the deformation mechanisms of sion is 10 MPa, which was experimentally determined τ calcite monocrystals and polycrystalline aggregates by Turner et al. (1954). The magnitude of c is inde- during the last century provided evidence of several pendent of normal stress σ, magnitude and tempera- glide and twinning systems present in calcite. Twelve ture (e.g. Turner et al., 1954; De Bresser and Spiers, different glide systems on five different crystallo- 1997; figure 1b). In order to cause twinning, the graphic planes and three different twinning systems stress tensor acting upon an e-plane must have appro- have been defined (Bestmann and Prior, 2003). Only priate principal direction orientation and sufficient twinning systems are suitable for stress inversion pur- differential component. The magnitude of the shear poses because they are easy to observe under an opti- stress is controlled by the Schmid criterion μ, which σ cal microscope, their orientation can be measured is a function of the orientation of the 1 vector σ using either a universal stage or EBSD and only one (Handin and Griggs, 1951; figure 1c). -
Physical Properties of Surface Outcrop Cataclastic Fault Rocks, Alpine Fault, New Zealand
Article Volume 13, Number 1 28 January 2012 Q01018, doi:10.1029/2011GC003872 ISSN: 1525-2027 Physical properties of surface outcrop cataclastic fault rocks, Alpine Fault, New Zealand C. Boulton Department of Geological Sciences, University of Canterbury, PB 4800, Christchurch 8042, New Zealand ([email protected]) B. M. Carpenter Department of Geosciences, Pennsylvania State University, 522 Deike Building, University Park, Pennsylvania 16802, USA V. Toy Department of Geology, University of Otago, P.O. Box 56, Dunedin 9054, New Zealand C. Marone Department of Geosciences, Pennsylvania State University, 522 Deike Building, University Park, Pennsylvania 16802, USA [1] We present a unified analysis of physical properties of cataclastic fault rocks collected from surface exposures of the central Alpine Fault at Gaunt Creek and Waikukupa River, New Zealand. Friction experi- ments on fault gouge and intact samples of cataclasite were conducted at 30–33 MPa effective normal stress (sn′) using a double-direct shear configuration and controlled pore fluid pressure in a true triaxial pressure vessel. Samples from a scarp outcrop on the southwest bank of Gaunt Creek display (1) an increase in fault normal permeability (k=7.45 Â 10À20 m2 to k = 1.15 Â 10À16 m2), (2) a transition from frictionally weak (m = 0.44) fault gouge to frictionally strong (m = 0.50–0.55) cataclasite, (3) a change in friction rate depen- dence (a-b) from solely velocity strengthening, to velocity strengthening and weakening, and (4) an increase in the rate of frictional healing with increasing distance from the footwall fluvioglacial gravels contact. At Gaunt Creek, alteration of the primary clay minerals chlorite and illite/muscovite to smectite, kaolinite, and goethite accompanies an increase in friction coefficient (m = 0.31 to m = 0.44) and fault- perpendicular permeability (k=3.10 Â 10À20 m2 to k = 7.45 Â 10À20 m2).