Fault Rocks and Fault Mechanisms

Total Page:16

File Type:pdf, Size:1020Kb

Fault Rocks and Fault Mechanisms Fault rocks and fault mechanisms R. H. SIBSON SUMMARY Physical factors likely to affect the genesis of the with the production of mylonite series rocks various fault rocks--frictional properties, tem- possessing strong tectonite fabrics. In some cases, perature, effective stress normal to the fault and fault rocks developed by transient seismic fault- differential stress--are examined in relation to ing can be distinguished from those generated the energy budget of fault zones, the main by slow aseismic shear. Random-fabric fault velocity modes of faulting and the type of fault- rocks may form as a result of seismic faulting ing, whether thrust, wrench, or normal. In a within the ductile shear zones from time to conceptual model of a major fault zone cutting time, but tend to be obliterated by continued crystalline quartzo-feldspathic crust, a zone of shearing. Resistance to shear within the fault elastico-frictional (EF) behaviour generating zone reaches a peak value (greatest for thrusts random-fabric fault rocks (gouge--breccia-- and least for normal faults) around the EF/OP cataclasite series--pseudotachylyte) overlies a transition level, which for normal geothermal region where quasi-plastic (QP) processes of gradients and an adequate supply of water, rock deformation operate in ductile shear zones occurs at depths of lO-15 km. SINCE LAPWORTH'$ (I885) description of the type mylonite from the Moine Thrust in NW Scotland, there have been many petrographic descriptions and classifications of the texturally distinctive rocks found associated with fault zones (e.g. Waters & Campbell 1935, Hsu 1955, Christie 196o , 1963, Reed 1964, Spry I969, Higgins 1971 ). These rocks provide a tangible source of information on the processes which operate in major fault zones, but little has been done to correlate the various types of fault rock with different deformation environments and modes of faulting. In this paper, I discuss the physical factors which may affect the genesis of fault rocks, and make some tentative correlations between their textures and deforma- tion environments. For the most part, the effects of faulting in crystalline quartzo- feldspathic crust are considered. I. Textures and occurrence of fault rocks In this paper fault rocks is used as a collective term for the distinctive rock types found in zones of shear dislocation at both high and low crustal levels, whose textures are thought to arise at least in part from the shearing process. It is not denied that similar textures may develop in association with other geological structures (e.g. protoclastic textures arising from igneous intrusion). The term cataclastic rocks, introduced by Waters & Campbell (1935) as a collective name for all rocks of the gouge--breccia--cataclasite--mylonite kindred, is not used because of the misleading implication that such rocks have developed solely by cataclasis. In the strict sense, cataclasis involves the brittle fragmentation of mineral grains with rotation of grain fragments accompanied by frictional grain boundary sliding dTl geol. Soc. Lond. vol. I33 , 1977, pp. 191-213, 8 figs., 3 plates, 3 tables. Printed in Great Britain. Downloaded from http://pubs.geoscienceworld.org/jgs/article-pdf/133/3/191/4885339/gsjgs.133.3.0191.pdf by guest on 01 October 2021 I92 R. H. Sibson and dilatancy, and it is now clear that these are not the dominant processes leading to the formation of mylonite series textures. In quartzo-feldspathic mylonites, quartz grains have been reduced in grain size by the dynamic recovery and recrystallization of highly strained grains which have undergone intense intra- crystalline plastic deformation (Bell & Etheridge I973, White I973). It is also apparent, as originally noted for the type mylonite (Lapworth I885, Teall I918), that extensive recrystallization and neomineralization occurs in the groundmass of most cohesive 'cataclastic' rocks. (A) TEXTURAL CLASSIFICATION Because changes in textural type tend to be gradational (P1. 3 a) and some fault rocks retain mixed textures resulting from polyphase deformation under different T A B L E I : Textural classification of fault rocks RANDOM - FABRIC FOLIATED FAULT BRECCIA (visible fragments >30% of rock mass) FAULT GOUGE (vlslble fragments 430% of rock mess) L w PSEUDOTACHYLYTE CR~SH BRECCIA (frasments • 0.5 cm) I FINE CRUSH BRECCIA (O.lcm • frasso < 0.Scm) CRUSH NICROBRECCIA (fragments < 0. I cm) O ! PROTOCATACLASITE PROTOHYLOKITE ..... N ¢.o '-t- O O ! CATACLASITE I~fLONITE ~O Z ULTRACATACLASITE ULT~ONITE BLASTONYLONITE Downloaded from http://pubs.geoscienceworld.org/jgs/article-pdf/133/3/191/4885339/gsjgs.133.3.0191.pdf by guest on 01 October 2021 Loch Eport SCOTLAND C~ Loch 0bisary % // I / ~EAVAL'. ",',', "," .''," • 347m ......... '.'o'.''.'','-',. |.. J.~ KEY Thrust r" Crush zone Phylbniti¢ shear belt ~. • . ° Crush • . melange. ". ° . ltl ;~ ...- , . ..:.,,. , ~ .I I . - ~,~ 0 b Mylonitic { 30-60° ' I foliatm ( 60_90o ..4" J increasing palaeotemperature , > IX~eudofachylyte- uitraca~¢lasite crush zone Fzo. I Map and schematic cross-section of the Outer Hebrides Thrust in Eaval block, N Uist. Downloaded from http://pubs.geoscienceworld.org/jgs/article-pdf/133/3/191/4885339/gsjgs.133.3.0191.pdf by guest on 01 October 2021 194 R. H. Sibson T A B L E 2 "Fault rocks and style of faulting in the Outer Hebrides Thrust zone StTle of Faulting Fault Rocks Brittle shearing of intact rock~ Pseudotachylyte Sliding on existing planes J Cataclastic crush zones Cataclaslte-Ultracataclasite (& some pseudotachylyte) Crush Melange Crush breccias, microbreccias & protocataclasite Quasi-plastlc shear zones Phyllonltic mylonites & ultramylonites Crush Melange with crude Protomylonites mylonitic foliation crustal conditions (PI. 2), (Christie I96O) attempts to classify the textures of fault rocks in a pigeon-hole manner that can never be entirely satisfactory. The scheme outlined in Table I serves as a simple reference system, adequate for the following discussion. It is based largely on that put forward by Spry (I969, p. 229), modified to avoid genetic connotations, with some additional elements from Higgins' (i 97 I) classification. The whole has been rearranged to emphasize a division which I consider to be of great mechanical significance; the separation of those fault rocks with an essentially random shape (and crystallographic) fabric from those that are foliated, usually with a strongly inosculafing L-S shape fabric (fluxion structure). Another main division is made on the presence or absence ofprirnary cohesion, the cohesive fault rocks then being further subdivided on the nature of their matrix. Cohesive rocks in which tectonic reduction in grain size has dominated processes of grain growth form the bulk of the commonly recognized fault rocks formed at other than near surface conditions (P1. I). The term phillonite is retained as a useful descriptive name for hydrated, mica-rich mylordtes and ultramylonites which have the silky appearance of phyllites. (B) DISTRIBUTION WITHIN FAULT ZONE'S Many major ancient fault zones are now exposed at erosion levels which corres- pond to considerable depths when the faults were active. They often consist of a mesh of shear zones enclosing lozenge-shaped areas of comparatively undeformed rock, the whole being perhaps a few kilometres or possibly tens of kilometres in width. Variations in both the style and the rock products of faulting occur across such zones when they have a large component of finite dip-slip. As an example we consider a section across the Outer Hebrides Thrust, a major dislocation of prob- able late Caledonian age which borders the eastern coastline of the Outer Isles in NW Scotland (Francis & Sibson 1973, Sibson 1975). This structure is especially suitable for discussion, because it disrupts crystalline Lewisian basement gneisses of fairly uniform bulk composition, and because fault rocks are generally best Downloaded from http://pubs.geoscienceworld.org/jgs/article-pdf/133/3/191/4885339/gsjgs.133.3.0191.pdf by guest on 01 October 2021 J1 geol. Soc. Lond. x33 , i977 SIBSON a • . ~ '~,q~ ~ e :: PLATE I Mylonite series (a--protomylonite, b--mylonite, c--ultramylonite) versus Catacla- site series (d--protocataclasite, e--cataclasite, f--ultracataclasite). All specimens from the Outer Hebrides Thrust zone (crossed polars except c & f, × 7)- 194 Downloaded from http://pubs.geoscienceworld.org/jgs/article-pdf/133/3/191/4885339/gsjgs.133.3.0191.pdf by guest on 01 October 2021 J1 geol. Soc. Lond. I33 , 1977 SIBSON (a) (b) PLATE 2 Polyphase texture from Seaforth Head, Lewis (NB 305 158). (a) Vein material forming breccia matrix and disrupting banded mylonite-ultramylonite, was probably random- fabric pseudotachylyte developed by seismic faulting within a ductile shear zone (plane polars, × 3.0). (b) Porphyroclasts within vein are now aligned in a strong shape fabric as a result of continued ductile deformation (plane polars, x 15 . 75)- Downloaded from http://pubs.geoscienceworld.org/jgs/article-pdf/133/3/191/4885339/gsjgs.133.3.0191.pdf by guest on 01 October 2021 J1 geol. Soc. Lond. i33 , i977 SIBSON (a) (b) PLAIE 3" (a) Gradational change in texture. Amphibolite -+ protomlyonite -~- mylonite --~ ultramylonite (Ness, Lewis NB 521664) (plane polars, × 14.o ). (b). Phyllonitic shear belt cutting crush m61ange, east coast ofN Uist (NF 922597). Note marginal curve-in of schistosity and asymmetric chevron folds developed within the belt. Downloaded from http://pubs.geoscienceworld.org/jgs/article-pdf/133/3/191/4885339/gsjgs.133.3.0191.pdf
Recommended publications
  • 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.
    [Show full text]
  • Download Article (PDF)
    Open Geosci. 2015; 7:53–64 Research Article Open Access László Molnár*, Balázs Vásárhelyi, Tivadar M. Tóth, and Félix Schubert Integrated petrographic – rock mechanic borecore study from the metamorphic basement of the Pannonian Basin, Hungary Abstract: The integrated evaluation of borecores from the 1 Introduction Mezősas-Furta fractured metamorphic hydrocarbon reser- voir suggests significantly distinct microstructural and Brittle fault zones of crystalline rock masses can serve as rock mechanical features within the analysed fault rock migration pathways or also as sealing surfaces for fluid samples. The statistical evaluation of the clast geometries flow in the Earth’s crust, so the understanding of their in- revealed the dominantly cataclastic nature of the sam- ternal structure is crucial for interpreting hydraulic sys- ples. Damage zone of the fault can be characterised by tems. Earlier studies [1, 2] on the architecture of fault an extremely brittle nature and low uniaxial compressive zones defined two main structural elements: first, a weakly strength, coupled with a predominately coarse fault brec- disaggregated, densely fractured “damage zone” and a cia composition. In contrast, the microstructural manner strongly deformed and fragmented “fault core”, where of the increasing deformation coupled with higher uni- the pre-existing rock fabrics were erased by fault devel- axial compressive strength, strain-hardening nature and opment. These elements can be characterised by the for- low brittleness indicate a transitional interval between mation of diverse tectonite types (fault breccias, catacla- the weakly fragmented damage zone and strongly grinded sites, fault gouges), which often also possess quite hetero- fault core. Moreover, these attributes suggest this unit is geneous rheological features.
    [Show full text]
  • Composition, Alteration, and Texture of Fault-Related Rocks from Safod Core and Surface Outcrop Analogs
    Pure Appl. Geophys. Ó 2014 Springer Basel DOI 10.1007/s00024-014-0896-6 Pure and Applied Geophysics Composition, Alteration, and Texture of Fault-Related Rocks from Safod Core and Surface Outcrop Analogs: Evidence for Deformation Processes and Fluid-Rock Interactions 1 1 1 1 1 KELLY K. BRADBURY, COLTER R. DAVIS, JOHN W. SHERVAIS, SUSANNE U. JANECKE, and JAMES P. EVANS Abstract—We examine the fine-scale variations in mineralogi- 1. Introduction cal composition, geochemical alteration, and texture of the fault- related rocks from the Phase 3 whole-rock core sampled between 3,187.4 and 3,301.4 m measured depth within the San Andreas Fault Well-constrained geological, geochemical, and Observatory at Depth (SAFOD) borehole near Parkfield, California. geophysical models of active fault zones are needed if This work provides insight into the physical and chemical properties, we are to understand fault zone behavior and earth- structural architecture, and fluid-rock interactions associated with the actively deforming traces of the San Andreas Fault zone at depth. quake deformation, constraining the factors that affect Exhumed outcrops within the SAF system comprised of serpentinite- the distribution of earthquakes, and the nature of slip bearing protolith are examined for comparison at San Simeon, Goat in the shallow crust by developing realistic models of Rock State Park, and Nelson Creek, California. In the Phase 3 SAFOD drillcore samples, the fault-related rocks consist of multiple subsurface fault zone structure and ground motion juxtaposed lenses of sheared, foliated siltstone and shale with block- predictions. Earthquakes nucleate in rocks at depth in-matrix fabric, black cataclasite to ultracataclasite, and sheared (e.g., FAGERENG and TOY 2011;SIBSON 1977; 2003), serpentinite-bearing, finely foliated fault gouge.
    [Show full text]
  • Rnic~Ess T~Ese
    GEOPHYSICAL RESEARCH LETTERS, VOL. 18, NO.5, PAGES 979-982, MAY 1991 HYDROGEOLOGY OF THRUST FAULTS AND CRYSTALLINE THRUST SHEETS: RESULTS OF COMBINED FIELD AND MODELING STUDIES Craig B. Forster Department of Geology & Geophysics, University of Utah James P. Evans Department of Geology, Utah State University Abstract. Field,. laboratory, and.modeling studies of faulted obtained for systems that span a wide range of spatial scales, rock yield insight 1Oto the hydraulic character of thrust faults. aid in establishing appropriate scales of observation. Although Late-stage fau lts comprise foliated and su?par~lel faults, ~ith our numerical models cannot provide a unique answer that clay-rich gouge and fracture zones, that YIeld mterpenetratmg applies directly to a given field situation, the numerical results layers of low-permeability gou~e and higher-permeab~l~ty do provide insight into this class of groundwater flow system. damage zones. Laboratory testmg suggests a permeabIlity contrast of two orders of magnitude between gouge and damage zones. Layers of differing permeability lead to overall Fault Zone Hydrogeology permeability anisotropy with maximum permeability within the plane of the fault and minimum permeability perpendicular to the fault plane. Numerical modeling of regional-scale fluid Precambrian granites and gneisses found in our field area flow and heat transport illustrates the impact of fault zone (northwest Wyoming) were thrusted over adjacent sedimentary hydrogeology on fluid flux, fluid pore pressure, and rocks along moderately-dipping thrust faults. About 150 m of temperature in the vicinity of a crystalline thrust sheet. exposed fault were examined through large-scale field mapping and detailed sampling both across and along strike.
    [Show full text]
  • Strength of Chrysotile-Serpentinite Gouge Under Hydrothermal Conditions: Can It Explain a Weak San Andreas Fault?
    Strength of chrysotile-serpentinite gouge under hydrothermal conditions: Can it explain a weak San Andreas fault? D. E. Moore D. A. Lockner U.S. Geological Survey, Menlo Park, California 94025 R. Summers Ma Shengli Institute of Geology, State Seismological Bureau, Beijing, China J. D. Byerlee U.S. Geological Survey, Menlo Park, California 94025 ABSTRACT more, it has been suggested that at higher temperatures (Reinen et Chrysotile-bearing serpentinite is a constituent of the San An- al., 1993) and/or lower strain rates (Reinen and Tullis, 1995) the dreas fault zone in central and northern California. At room tem- frictional strength of chrysotile may be reduced to ␮ Յ 0.1. As a test perature, chrysotile gouge has a very low coefficient of friction (␮ of this hypothesis, we report here on the strength of a pure chrysotile Ϸ 0.2), raising the possibility that under hydrothermal conditions gouge at elevated temperatures and a wide range of velocities, in- ␮ might be reduced sufficiently (to <0.1) to explain the apparent tended to more closely represent conditions at depth in the fault. weakness of the fault. To test this hypothesis, we measured the Our results suggest that chrysotile alone is not a likely explanation frictional strength of a pure chrysotile gouge at temperatures to for a weak San Andreas fault. ؇C and axial-shortening velocities as low as 0.001 ␮m/s. As 290 temperature increases to Ϸ100 ؇C, the strength of the chrysotile EXPERIMENTAL PROCEDURES gouge decreases slightly at low velocities, but at temperatures The chrysotile gouge used in this study was prepared from a ؇C, it is substantially stronger and essentially independent of soft, layered, light to medium grayish-green rock from the New Idria 200< velocity at the lowest velocities tested.
    [Show full text]
  • 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).
    [Show full text]
  • Generation of Sintered Fault Rock and Its Implications for Earthquake
    ARTICLE https://doi.org/10.1038/s43247-020-0004-z OPEN Generation of sintered fault rock and its implications for earthquake energetics and fault healing ✉ Tetsuro Hirono 1 , Shunya Kaneki 2, Tsuyoshi Ishikawa 3, Jun Kameda4, Naoya Tonoike1,7, Akihiro Ito5 & Yuji Miyazaki6 1234567890():,; After an earthquake, faults can recover strength through fault healing, but the mechanisms responsible are not well understood. Seismic slip may induce sintering, a bonding process between solid particles in contact under high temperatures without melting, which could produce a fault rock with elevated strength and chemical stability. Here we present results from electron microscope analyses that show a typical sintered structure in a black disk- shaped rock from the Chelungpu fault, Taiwan. This structure is experimentally reproducible in simulated fault material, prepared from the local host-rock, by heating at 800–900 °C. Through thermal and kinetic analyses of experimental materials, we show that sintering is an exothermic process which can generate energy to enhance post-slip thermochemical reac- tions in the fault. We propose that sintering substantially contributes to earthquake ener- getics and fault healing and that its occurrence can be a useful indicator of past seismic slip. 1 Department of Earth and Space Science, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan. 2 Disaster Prevention Research Institute, Kyoto University, Uji, Kyoto 611-0011, Japan. 3 Kochi Institute for Core Sample Research, Japan Agency for Marine-Science and Technology (JAMSTEC), Nankoku, Kochi 783-8502, Japan. 4 Department of Natural History Sciences, Graduate School of Science, Hokkaido University, Sapporo, Hokkaido 060-0810, Japan.
    [Show full text]
  • Scientific Drilling Into the San Andreas Fault Zone —An Overview of SAFOD’S First Five Years
    Science Reports Scientific Drilling Into the San Andreas Fault Zone —An Overview of SAFOD’s First Five Years by Mark Zoback, Stephen Hickman, William Ellsworth, and the SAFOD Science Team doi:10.2204/iodp.sd.11.02.2011 Abstract Detailed planning of a research experiment focused on drilling, sampling, and downhole measurements directly The San Andreas Fault Observatory at Depth (SAFOD) within the San Andreas Fault Zone began with an interna- was drilled to study the physical and chemical processes tional workshop held in Asilomar, California in December controlling faulting and earthquake generation along an 1992. This workshop highlighted the importance of active, plate-bounding fault at depth. SAFOD is located near deploying a permanent geophysical observatory within the Parkfield, California and penetrates a section of the fault that fault zone at seismogenic depth for near-field monitoring of is moving due to a combination of repeating microearth- earthquake nucleation. Hence, from the outset, the SAFOD quakes and fault creep. Geophysical logs define the San project has been designed to achieve two parallel suites of Andreas Fault Zone to be relatively broad (~200 m), contain- objectives. The first is to carry out a series of experiments in ing several discrete zones only 2–3 m wide that exhibit very and near the San Andreas Fault that address long-standing low P- and S-wave velocities and low resistivity. Two of these questions about the physical and chemical processes that zones have progressively deformed the cemented casing at control deformation and earthquake generation within active measured depths of 3192 m and 3302 m.
    [Show full text]
  • Hydrogeological Properties of Fault Zones in a Karstified Carbonate Aquifer (Northern Calcareous Alps, Austria)
    Hydrogeol J DOI 10.1007/s10040-016-1388-9 PAPER Hydrogeological properties of fault zones in a karstified carbonate aquifer (Northern Calcareous Alps, Austria) H. Bauer1 & T. C. Schröckenfuchs 1 & K. Decker1 Received: 17 July 2015 /Accepted: 14 February 2016 # The Author(s) 2016. This article is published with open access at Springerlink.com Abstract This study presents a comparative, field-based impermeable fault cores only very locally have the potential hydrogeological characterization of exhumed, inactive fault to create barriers. zones in low-porosity Triassic dolostones and limestones of the Hochschwab massif, a carbonate unit of high economic Keywords Fractured rocks . Carbonate rocks . Fault zones . importance supplying 60 % of the drinking water of Austria’s Hydrogeological properties . Austria capital, Vienna. Cataclastic rocks and sheared, strongly cemented breccias form low-permeability (<1 mD) domains along faults. Fractured rocks with fracture densities varying by Introduction a factor of 10 and fracture porosities varying by a factor of 3, and dilation breccias with average porosities >3 % and per- Fault zones in the upper crust produce permeability heteroge- meabilities >1,000 mD form high-permeability domains. With neities that have a large impact on subsurface fluid migration respect to fault-zone architecture and rock content, which is and storage patterns (e.g. Agosta et al. 2010, 2012; Caine et al. demonstrated to be different for dolostone and limestone, four 1996;Faulkneretal.2010;Jourdeetal.2002; Mitchell and types of faults are presented. Faults with single-stranded mi- Faulkner 2012; Shipton and Cowie 2003; Shipton et al. 2006; nor fault cores, faults with single-stranded permeable fault Wibberley and Shimamoto 2003; Wibberley et al.
    [Show full text]
  • Structure, Petrophysics, and Diagenesis of Shale Entrained Along a Normal Fault Shale and Sand from the Host Rock to the Fault
    Structure, petrophysics, AUTHORS Peter Eichhubl Department of Geologi- and diagenesis of shale cal and Environmental Sciences, Stanford University, Stanford, California 94305; present entrained along a normal address: Department of Physical and Life Sci- ences, Texas A&M University–Corpus Christi, fault at Black Diamond Mines, 6300 Ocean Drive, Corpus Christi, Texas 78412; [email protected] California— Implications Peter Eichhubl received his M.S. degree at the University of Vienna, Austria, and his Ph.D. at the University of California, Santa Barbara. for fault seal After research positions at Stanford University and Monterey Bay Aquarium Research In- Peter Eichhubl, Peter S. D’Onfro, Atilla Aydin, stitute, he joined the faculty at Texas A&M John Waters, and Douglas K. McCarty University–Corpus Christi. His research inter- ests include the interaction of chemical mass transfer and brittle deformation, diagenesis, and fault and fracture mechanics. ABSTRACT Peter S. D’Onfro ConocoPhillips, P.O. The structure, texture, composition, and capillary-pressure resis- Box 2197, Houston, Texas 77252-2197; tancewereassessedforshaledeformedalonganormalfaultwith [email protected] 9 m (29 ft) of dip separation. Shale is entrained from a 1.6-m (5-ft)- Peter D’Onfro earned his B.S. and M.S. degrees thick source layer into the fault zone and attenuated to about 5 cm from Boston College. After a research posi- (2 in.). A quantitative analysis of shale mineral composition indi- tion at Los Alamos National Laboratories, he cates that little material is contributed to the fault rock from the joined Conoco in 1979 and then ConocoPhillips sandstone units that over- and underlie the shale source layer.
    [Show full text]
  • Coseismic Fluid–Rock Interactions in the Beichuan-Yingxiu Surface Rupture Zone of the Mw 7.9 Wenchuan Earthquake and Its Impli
    https://doi.org/10.5194/se-2020-117 Preprint. Discussion started: 28 July 2020 c Author(s) 2020. CC BY 4.0 License. 1 Coseismic fluid–rock interactions in the Beichuan-Yingxiu surface rupture zone 2 of the Mw 7.9 Wenchuan earthquake and its implication for the fault zone 3 transformation 4 Yangyang Wang a*, Xiaoqi Gao a, Sijia Li b, Shiyuan Wang c, Deyang Shi a,d, Weibing Shen e** 5 a The Key Laboratory of Crustal Dynamics, Institute of Crustal Dynamics, China Earthquake Administration, Beijing, 6 100085, China 7 b. Geological Exploration and Development Research Institute, Chuanqing Drilling Engineering Co., Ltd., CNPC, 8 Chengdu, Sichuan, 610500, China. 9 c. Sichuan Earthquake Agency, Chengdu, 610041,China 10 d. Institute of Geophysics, China Earthquake Administration, Beijing, 100081, China 11 e. MLR Key Laboratory of Isotope Geology, Institute of Geology, Chinese Academy of Geological Sciences, Beijing 12 100037, China 13 * Corresponding Author 14 ** CO-corresponding Author 15 E-mail: [email protected] 16 Phone number: +8615117973405 17 Present address: Key Laboratory of Crustal Dynamics, Institute of Crustal Dynamics, China Earthquake 18 Administration, No. 1, Anningzhuang Road, Haidian District, Beijing, People’s Republic of China, 100085 1 https://doi.org/10.5194/se-2020-117 Preprint. Discussion started: 28 July 2020 c Author(s) 2020. CC BY 4.0 License. 19 Abstract 20 Mechanism of fluids in modifying mineralogy and geochemistry of the fault zone and the role of rock- 21 fluid interaction in the faulting weakening is still debatable. Through analyzing mineralogical 22 compositions, major elements as well as micro-structural characteristics of outcrop samples including 23 wall rocks, low damage zone, high damage zone and oriented fault gouge samples from principal slip 24 zone gouges, mineralogical and geochemical variations of the fault-rocks is observed from Shaba 25 outcrop of Beichuan-Yingxiu surface rupture zone of the Mw 7.9 Wenchuan earthquake, China.
    [Show full text]
  • Cataclasis and the Generation of Fault Gouge
    Cataclasis and the Generation of Fault Gouge JAMES T. ENGELDER* Center for Tectonophysics, Texas A&M University, College Station, Texas 77843 ABSTRACT ose sandstone. Natural textures and fabrics discovered in this study are used as a control in designing geologically reasonable Cataclasis, a friction-dependent mechanism of deformation in- sliding friction experiments with quartz gouge. In another paper, volving fracture and rigid-body rotation, occurs during faulting of the experimentally determined frictional characteristics of sand- sandstone in the upper crust. Two stages of cataclasis of a sand- stone sliding on quartz gouge are presented in detail (Engelder, stone are represented by (1) mildly deformed cataclastic sandstone 1974). that is shattered but contains many original grains that have not Quartz gouge and faults in sandstone were studied for several been fragmented and (2) gouge so severely deformed that the few reasons: the quartz gouge is easier to work with in the laboratory surviving grains are almost surrounded by a fine-grained matrix of compared to clay and shale; it is monomineralic; its optical proper- crushed grains. Gouge is restricted to shear fractures and larger slip ties simplify petrographic observations; it is a common type of planes within the natural fault zones, wnereas cataclastic sandstone gouge in nature; and stick-slip sliding, a possible mechanism for usually pervades the fault zone. Grain size and sorting of gouge de- shallow earthquakes, occurs on fractures in quartzose rocks (Brace crease as a function of increasing confining pressure and increasing and Byerlee, 1966; Logan and others, 1973). displacement along a shear fracture. In cataclastic sandstone as- sociated with gouge, microfractures are strongly oriented parallel CHARACTERISTICS OF to the maximum principal compressive stress.
    [Show full text]