Quasi-Flexural Folding of Pseudo-Bedding

Total Page:16

File Type:pdf, Size:1020Kb

Quasi-Flexural Folding of Pseudo-Bedding 30963 1st pages / 1 of 22 Quasi-fl exural folding of pseudo-bedding George H. Davis† Department of Geosciences, University of Arizona, Tucson, Arizona 85721, USA ABSTRACT These factors, plus the apparent ease with uncommon fold geometries and structural rela- which the limestone pseudo-beds deform by tionships in a limestone formation in the Pindos The disharmonic outcrop-scale folds and tectonically induced mass-transfer dissolu- fold-and-thrust belt in the Peloponnese, Greece. associated structures in a 300-m-thick Creta- tion creep, were responsible for the distinc- Particularly important is the infl uence on fold- ceous limestone formation in the Pindos Group tive structures observed in outcrop. These in- ing exerted by “pseudo-bedding” (Fig. 1), exposed on Mount Lykaion (Arcadia, Greece) clude indentation structures, where a part of which is created by pressure dissolution during can be understood only in the context of super- one fold limb indents into the other, or where diagenetic gravitational loading accompanying posed pre-tectonic and tectonic mass-transfer the hanging wall of a small thrust indents burial and primary compaction. This work calls dissolution creep. Though the structures de- into its footwall, or where the limbs of a com- particular attention to the kinematic limitations scribed may seem unusual, they are undoubt- mon anticline or syncline migrate toward one of pseudo-bedding stylolite surfaces in accom- edly abundant in strongly deformed pseudo- another by pressure dissolution removal of modating requisite fl exural slip on the limb of bedded limestone formations. In this example the axial-trace region. In terms of the overall a major anticline, and how fl exural-slip budget the Thick White Limestone Beds (TWLB) progressive deformation, tectonically driven defi cits are managed by tectonic pressure disso- formation displays pervasive “fl aggy” pseudo- layer-parallel shortening of pseudo-beds lution and certain uncommon mesoscopic-scale bedding, which is a diagenetic stylolitic layer- fi rst resulted in tectonic stylolites perpen- fold/fault mechanisms. Structural products that ing resulting from pressure dissolution. The dicular to pseudo-bedding, with teeth paral- result from this dissolution creep–dominated mass-transfer dissolution creep that produced lel to pseudo-bedding. This was superseded progressive deformation include quasi-fl exural the diagenetic stylolitic surfaces was achieved at the mesoscopic scale by a layer-parallel folding (Donath and Parker, 1964), an over- during gravitational loading accompanying shortening achieved by buckling of pseudo- looked category of folding which is likely com- burial, compaction, and lithifi cation, and was beds, with loci of buckling and incipient monplace in highly deformed pseudo-bedded driven by high stress concentrations at grain buckling geometries infl uenced primarily limestone formations in mountain belts of the contacts. The diagenetic stylolitic surfaces are by pseudo-bed thickness (and variations in world, such as within fold-and-thrust belts of the lined with insoluble residue and commonly same), wedge-outs of pseudo-beds, and the Appalachians, Arbuckles, Alps, Apennines, and are marked by interlocking stylolite teeth ori- mechanical properties of the pseudo-beds. the western Cordillera of North America. ented perpendicular to the pseudo-bedding. In some cases shortening and tightening of At the outcrop scale, individual pseudo-beds buckle folds involved fl exural-slip kinemat- MASS-TRANSFER DISSOLUTION display signifi cant thickness variability. More- ics, accommodated in part by slip or shear CREEP: AN OVERVIEW over, the individual pseudo-beds not uncom- along clayey insoluble residue at pseudo-bed monly wedge out and disappear laterally over contacts. Where diagenetic stylolite surfaces Stylolites very short distances. abruptly tipped out, or where friction along Along with all the Pindos Group strata, the them was excessively high, the slip defi cit Stylolites are surfaces of localized dissolution, TWLB formation was profoundly shortened (and thus shortening defi cit) was replaced by commonly displaying in cross-section a rough in the Late Cretaceous and early Tertiary as mass interpenetration of pseudo-beds, stylo- suture geometry lined with insoluble residue a result of inversion tectonics. The Pindos faulting, stylo-duplexing, and other forms of of clay, oxides, and/or organic matter (Fig. 2) Group limestone-dominated formations mass-transfer dissolution creep. Slip toward (Stockdale, 1922; Heald, 1955; Bayly, 1986; under lying and overlying TWLB readily ac- the tip lines of wedge-outs even may have Groshong, 1988; Aharonov and Katsman, 2009, commodated fl exural-slip folding, for these produced end loading that, in turn, generated p. 607). They occur at mesoscopic and micro- formations are marked by optimum mechan- adjacent localized buckle folds. The proper- scopic scales. Lengths of stylolite surfaces typi- ical stratigraphy, ubiquitous thin bedding, ties of the folds and associated structures in cally range from centimeters to many meters, and pervasive bedding-plane slip surfaces. the TWLB formation are introduced here as though trace lengths of individual stylolite sur- For the TWLB formation, however, strain a new category of quasi-fl exural folds in the faces of 1 km and more have been observed and accommodation by fl exural-slip kinematics Donath and Parker (1964) classifi cation. measured by Ben-Itzhak et al. (2012). Lengths was spotty and ineffi cient, primarily because of stylolite surfaces generally increase according individual diagenetic stylolite surfaces are by INTRODUCTION to the amount of contractional strain accommo- no means planar or smoothly curviplanar; dated by the stylolite (Benedicto and Schultz, they tip out over short distances; and their The purpose of this paper is to describe and 2010; Ben-Itzhak et al., 2012). interlocking stylolite teeth create elevated interpret the infl uence of mass-transfer dis- Stylolites that are sutured resemble brain frictional resistance to layer-parallel slip. solution creep, i.e., both pre-tectonic and tec- sutures and are distinguished by serrated sur- tonic, as a dominant deformation mechanism faces marked by abundant teeth (Geiser, 1974; †E-mail: [email protected]. that contributed to generating some apparently Geiser and Sansone, 1981; Ben-Itzhak et al., GSA Bulletin; Month/Month 2014; v. 1xx; no. X/X; p. 1–22; doi:10.1130/B30963.1; 30 fi gures. For permission to copy, contact [email protected] 1 © 2014 Geological Society of America 30963 1st pages / 2 of 22 Davis Diagenetic Stylolites Diagenetic stylolites tend to be parallel or subparallel to bedding. They form in the late stages of diagenesis (Groshong, 1988; Smith, 2000; Larbi, 2003) within rock, not unconsoli- dated sediments (Merino et al., 1983; Merino, 1992). Sutured diagenetic stylolites display teeth oriented perpendicular to layering (see Fig. 1), consistent with the horizontality of original bed- ding and the verticality of gravitational loading at the time of their genesis (Larbi, 2003). During sediment burial, compaction, and diagenesis, the ever-increasing gravitational loading raises the magnitudes of compres- sive tractions at grain contacts, which bear the load. Under these conditions of contractional strain calcite grains may rotate, break, and/or twin, and additionally they may dissolve and go into solution as a response to pressure dis- solution (Groshong, 1988; Aharonov and Kats- man, 2009). Merino et al. (1983) and Aharonov Figure 1. Pseudo-bedding in building blocks, Temple of Apollo Epicurius in Bassai, Greece. and Katsman (2009) have elaborated on the Note thickness variations of individual pseudo-beds. Middle block is ~80 cm long. Diagenetic kinematics and mechanics of such dissolu- stylolites are lined with insoluble clayey residue (black), now etched by weathering. Light tion in calcite limestones. This deformational gray steeply dipping fabric elements are calcite veins, products of pressure dissolution. mechanism is a mass-transfer creep involving material dissolution, diffusion, and reprecipita- tion (Guzzetta, 1984; Bayly, 1986; Karcz and 2012). Stylo lite teeth are commonly quite Scholz, 2003). Grains are brought into grain- evident in outcrop and thin section because to-grain contact, thus producing elevated stress they are lined with dark insoluble residue (see concentrations (Railsback, 1993; Aharonov and Fig. 2). Amplitudes of teeth vary in size, but Katsman, 2009). Dissolution creep takes place generally range from 1 µm to 1 cm (Sheppard, at the locations of high stress concentration, 2002; Aharo nov and Katsman, 2009), though high surface energy, and high chemical potential Merino et al. (1983) have reported stylolite teeth (Koehn, 2011). Calcium carbonate is removed amplitudes in the range of tens of centimeters. by diffusion to sites of lower stress concentra- Groshong (1975, p. 1367) defi ned “stylolite” in tion and chemical potential. Dissolution at grain a way that eliminated any requirement for the contacts eases strain energy (Aharonov and presence of suture geometry. He considered a Katsman, 2009). Insoluble residue accumulates stylolite to be “any zone of relatively insoluble at faceted contacts. Where such pressure dis- residue against which the original fabric ele- solution operates, there is a slow interpenetra- ments of the rock are truncated by removal tion of grains and rock elements (Merino et al., rather than offset.” This broader defi nition of 1983; Aharonov and
Recommended publications
  • GEO 2008 Conference Abstracts, Bahrain GEO 2008 Conference Abstracts
    GEO 2008 conference abstracts, Bahrain GEO 2008 Conference Abstracts he abstracts of the GEO 2008 Conference presentations (3-5 March 2008, Bahrain) are published in Talphabetical order based on the last name of the first author. Only those abstracts that were accepted by the GEO 2008 Program Committee are published here, and were subsequently edited by GeoArabia Editors and proof-read by the corresponding author. Several names of companies and institutions to which presenters are affiliated have been abbreviated (see page 262). For convenience, all subsidiary companies are listed as the parent company. (#117804) Sandstone-body geometry, facies existing data sets and improve exploration decision architecture and depositional model of making. The results of a recent 3-D seismic reprocessing Ordovician Barik Sandstone, Oman effort over approximately 1,800 square km of data from the Mediterranean Sea has brought renewed interest in Iftikhar A. Abbasi (Sultan Qaboos University, Oman) deep, pre-Messinian structures. Historically, the reservoir and Abdulrahman Al-Harthy (Sultan Qaboos targets in the southern Mediterranean Sea have been the University, Oman <[email protected]>) Pliocene-Pleistocene and Messinian/Pre-Messinian gas sands. These are readily identifiable as anomalousbright The Lower Paleozoic siliciclastics sediments of the amplitudes on the seismic data. The key to enhancing the Haima Supergroup in the Al-Haushi-Huqf area of cen- deeper structure is multiple and noise attenuation. The tral Oman are subdivided into a number of formations Miocene and older targets are overlain by a Messinian- and members based on lithological characteristics of aged, structurally complex anhydrite layer, the Rosetta various rock sequences.
    [Show full text]
  • 326-97 Lab Final S.D
    Geol 326-97 Name: KEY 5/6/97 Class Ave = 101 / 150 Geol 326-97 Lab Final s.d. = 24 This lab final exam is worth 150 points of your total grade. Each lettered question is worth 15 points. Read through it all first to find out what you need to do. List all of your answers on these pages and attach any constructions, tracing paper overlays, etc. Put your name on all pages. 1. One way to analyze brittle faults is to calculate and plot the infinitesimal shortening and extension directions on a lower hemisphere, stereographic projection. These principal axes lie in the “movement plane”, which contains the pole to the fault plane and the slickensides, and are at 45° to the pole. The following questions apply to a single fault described in part (a), below: (a) A fault has a strike and dip of 250, 57 N and the slickensides have a rake of 63°, measured from the given strike azimuth. Plot the orientations of the fault plane and the slickensides on an equal area projection. (b) Bedding in the vicinity of the fault is oriented 37, 42 E. Assuming that the fault formed when the bedding was horizontal, determine and plot the original geometry of the fault and the slickensides. (c) Determine the original (pre-rotation)orientation of the infinitesimal shortening and extension axes for fault. 2. All of the following questions apply to the map shown on the next page. In all of the rocks with cleavage, you may assume that both cleavage and bedding strike 024°.
    [Show full text]
  • 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.
    [Show full text]
  • Geologic Map of the Yellow Pine Quadrangle, Valley County, Idaho
    IDAHO GEOLOGICAL SURVEY IDAHOGEOLOGY.ORG DIGITAL WEB MAP 190 MOSCOW AND BOISE STEWART AND OTHERS present in exposures in the southern part of the map. Quartzite is feldspar The Johnson Creek shear zone is a major regional structure (Lund, 2004). To PIONEER GROUP (CH0776) poor. Thickness unknown because of complex internal folding and the the south of the quadrangle it can be traced as a series of faults (Fisher and 19DS16 GEOLOGIC MAP OF THE YELLOW PINE QUADRANGLE, VALLEY COUNTY, IDAHO The Pioneer group is a prospected area located northeast of the mouth of presence of a foliation that may or may not be transposed bedding. Likely others, 1992; Stewart and others, 2018), none of which appear to be as equivalent to the quartzite and schist unit in the Stibnite roof pendant silicified as in the Yellow Pine area. One splay likely connects to the Dead- Riordan Creek. One Defense Minerals Administration (DMA) application Cambrian y CORRELATION OF MAP UNITS and one Defense Minerals Exploration Administration (DMEA) loan appli- t i mapped by Stewart and others (2016). wood fault, which is locally mineralized at and southwest of the Deadwood l i lower cation were made in the 1950s for claims in this area, details of which are b Mine (Kiilsgaard and others, 2006). To the north, north of the Red Mountain a b Zmsm Marble of Moores Station Formation (Neoproterozoic)—Discontinuous lenses available in Frank (2016). Prospects at slightly lower elevation were termed o qtzite David E. Stewart, Reed S. Lewis, Eric D. Stewart, and Zachery M. Lifton stockwork, the fault zone is intruded by voluminous Eocene dikes (Lund, r p of buff to light-gray marble and lesser amounts of millimeter- to the Syringa Group (DMA Docket 1036).
    [Show full text]
  • Pacific Petroleum Eology
    Pacific Petroleum Geology NEWSLETTER Pacific Section • American Association of Petroleum Geologists September & October• 2010 School of Rock Ridge Basin CONTENTS 2010-2011 OFF I C E RS EV E RY ISSU E President Cynthia Huggins 661.665.5074 [email protected] 4 Message from the President • C. Huggins President-Elect John Minch 805.898.9200 6 Editor’s Corner • E. Washburn [email protected] Vice President Jeff Gartland 7 PS-AAPG News 661.869.8204 [email protected] 13 Publications Secretary Tony Reid 661.412.5467 17 Member Society News [email protected] Treasurer 2009-2011 Cheryl Blume TH I S ISSU E 661.864.4722 [email protected] 8 Sharktooth Hill Fossil Fund • K. Hancharick Treasurer 2010-2012 Jana McIntyre 661.869.8231 [email protected] 10 AAPG Young Professionals • J. Allen Past President Scott Hector 11 Serpentine: The Rest of the Story • Mel 707.974.6402 [email protected] Erskine Editor-in-Chief Ed Washburn 661.654.7182 [email protected] ST AFF Web Master Bob Countryman 661.589.8580 [email protected] Membership Chair Brian Church 661.654.7863 [email protected] Publications Chair Larry Knauer 661.392.2471 [email protected] [email protected] Advisory Council Representative Kurt Neher 661.412.5203 [email protected] Cover photo of Ridge Basin outcrop courtesy Jonathan Allen Page 3 Pacific Petroleum Geologist Newsletter September & October • 2010 MESSAGE FRO M THE PRESIDENT CYNTHIA HUGGINS Do you know what Marilyn Bachman, Mike Fillipow, Peggy Lubchenco, and Jane Justus Frazier have in common? They were all recipients of the Teacher of the Year Award from AAPG, and they all came from the Pacific Section! Of the 13 recipients of this award, four have been from PSAAPG.
    [Show full text]
  • Chapter 01.Pdf
    Mathematical Background in Aircraft Structural Mechanics CHAPTER 1. Linear Elasticity SangJoon Shin School of Mechanical and Aerospace Engineering Seoul National University Active Aeroelasticityand Rotorcraft Lab. Basic equation of Linear Elasticity Structural analysis … evaluation of deformations and stresses arising within a solid object under the action of applied loads - if time is not explicitly considered as an independent variable → the analysis is said to be static → otherwise, structural dynamic analysis or structural dynamics Small deformation Under the assumption of { Linearly elastic material behavior - Three dimensional formulation → a set of 15 linear 1st order PDE involving displacement field (3 components) { stress field (6 components) strain field (6 components) plane stress problem → simpler, 2-D formulations { plane strain problem For most situations, not possible to develop analytical solutions → analysis of structural components … bars, beams, plates, shells 1-2 Active Aeroelasticity and Rotorcraft Lab., Seoul National University 1.1 The concept of Stress 1.1.1 The state of stress at a point State of stress in a solid body… measure of intensity of forces acting within the solid - distribution of forces and moments appearing on the surface of the cut … equipollent force F , and couple M - Newton’s 3rd law → a force and couple of equal magnitudes and opposite directions acting on the two forces created by the cut Fig. 1.1 A solid body cut by a plane to isolate a free body 1-3 Active Aeroelasticity and Rotorcraft
    [Show full text]
  • Mechanical Stratigraphic Controls on Natural Fracture Spacing and Penetration
    Journal of Structural Geology 95 (2017) 160e170 Contents lists available at ScienceDirect Journal of Structural Geology journal homepage: www.elsevier.com/locate/jsg Mechanical stratigraphic controls on natural fracture spacing and penetration * Ronald N. McGinnis a, , David A. Ferrill a, Alan P. Morris a, Kevin J. Smart a, Daniel Lehrmann b a Department of Earth, Material, and Planetary Sciences, Southwest Research Institute, 6220 Culebra Road, San Antonio, TX 78238-5166, USA b Geoscience Department, Trinity University, One Trinity Place, San Antonio, TX 78212, USA article info abstract Article history: Fine-grained low permeability sedimentary rocks, such as shale and mudrock, have drawn attention as Received 20 July 2016 unconventional hydrocarbon reservoirs. Fracturing e both natural and induced e is extremely important Received in revised form for increasing permeability in otherwise low-permeability rock. We analyze natural extension fracture 21 December 2016 networks within a complete measured outcrop section of the Ernst Member of the Boquillas Formation Accepted 7 January 2017 in Big Bend National Park, west Texas. Results of bed-center, dip-parallel scanline surveys demonstrate Available online 8 January 2017 nearly identical fracture strikes and slight variation in dip between mudrock, chalk, and limestone beds. Fracture spacing tends to increase proportional to bed thickness in limestone and chalk beds; however, Keywords: Mechanical stratigraphy dramatic differences in fracture spacing are observed in mudrock. A direct relationship is observed be- Natural fractures tween fracture spacing/thickness ratio and rock competence. Vertical fracture penetrations measured Fracture spacing from the middle of chalk and limestone beds generally extend to and often beyond bed boundaries into Fracture penetration the vertically adjacent mudrock beds.
    [Show full text]
  • The Role of Pressure Solution Seam and Joint Assemblages In
    THE ROLE OF PRESSURE SOLUTION SEAM AND JOINT ASSEMBLAGES IN THE FORMATION OF STRIKE-SLIP AND THRUST FAULTS IN A COMPRESSIVE TECTONIC SETTING; THE VARISCAN OF SOUTHWESTERN IRELAND Filippo Nenna and Atilla Aydin Department of Geological and Environmental Sciences, Stanford University, Stanford, CA 94305 e-mail: [email protected] scale such as strike-slip faults and thrust-cored folds in Abstract various stages of their development. In this study we focus on the initiation and development of strike-slip The Ross Sandstone in County Clare, Ireland, was faults by shearing of the initial JVs and PSSs and deformed by an approximately north-south compression formation of thrust faults by exploiting weak shale during the end-Carboniferous Variscan orogeny. horizons and the strike-parallel PSSs in the adjacent Orthogonal sets of fundamental structures form the sandstone intervals. initial assemblage; mutually abutting arrays of 170˚ Development of faults from shearing of initial oriented set 1 joints/veins (JVs) and approximately 75˚ fundamental structural elements with either opening or pressure solution seams (PSSs) that formed under the closing modes in a wide range of structural settings has same stress conditions. Orientations of set 2 (splay) JVs been extensively reported. Segall and Pollard (1983), and PSSs suggest a clockwise remote stress rotation of Martel and Pollard (1989) and Martel (1990) have about 35˚ responsible for the contemporaneous described strike-slip faults formed by shearing of shearing of the set 1 arrays. Prominent strike-slip faults thermal fractures in granitic rocks. Myers and Aydin are sub-parallel to set 1 JVs and form by the linkage of (2004) and Flodin and Aydin (2004) reported strike-slip en-echelon segments with broad damage zones faulting formed by shearing of joints formed by an responsible for strike-slip offsets of hundreds of metres.
    [Show full text]
  • Sedimentary Stylolite Networks and Connectivity in Limestone
    Sedimentary stylolite networks and connectivity in Limestone: Large-scale field observations and implications for structure evolution Leehee Laronne Ben-Itzhak, Einat Aharonov, Ziv Karcz, Maor Kaduri, Renaud Toussaint To cite this version: Leehee Laronne Ben-Itzhak, Einat Aharonov, Ziv Karcz, Maor Kaduri, Renaud Toussaint. Sed- imentary stylolite networks and connectivity in Limestone: Large-scale field observations and implications for structure evolution. Journal of Structural Geology, Elsevier, 2014, pp.online first. <10.1016/j.jsg.2014.02.010>. <hal-00961075v2> HAL Id: hal-00961075 https://hal.archives-ouvertes.fr/hal-00961075v2 Submitted on 19 Mar 2014 HAL is a multi-disciplinary open access L'archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destin´eeau d´ep^otet `ala diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publi´esou non, lished or not. The documents may come from ´emanant des ´etablissements d'enseignement et de teaching and research institutions in France or recherche fran¸caisou ´etrangers,des laboratoires abroad, or from public or private research centers. publics ou priv´es. 1 2 Sedimentary stylolite networks and connectivity in 3 Limestone: Large-scale field observations and 4 implications for structure evolution 5 6 Laronne Ben-Itzhak L.1, Aharonov E.1, Karcz Z.2,*, 7 Kaduri M.1,** and Toussaint R.3,4 8 9 1 Institute of Earth Sciences, The Hebrew University, Jerusalem, 91904, Israel 10 2 ExxonMobil Upstream Research Company, Houston TX, 77027, U.S.A 11 3 Institut de Physique du Globe de Strasbourg, University of Strasbourg/EOST, CNRS, 5 rue 12 Descartes, F-67084 Strasbourg Cedex, France.
    [Show full text]
  • Along Strike Variability of Thrust-Fault Vergence
    Brigham Young University BYU ScholarsArchive Theses and Dissertations 2014-06-11 Along Strike Variability of Thrust-Fault Vergence Scott Royal Greenhalgh Brigham Young University - Provo Follow this and additional works at: https://scholarsarchive.byu.edu/etd Part of the Geology Commons BYU ScholarsArchive Citation Greenhalgh, Scott Royal, "Along Strike Variability of Thrust-Fault Vergence" (2014). Theses and Dissertations. 4095. https://scholarsarchive.byu.edu/etd/4095 This Thesis is brought to you for free and open access by BYU ScholarsArchive. It has been accepted for inclusion in Theses and Dissertations by an authorized administrator of BYU ScholarsArchive. For more information, please contact [email protected], [email protected]. Along Strike Variability of Thrust-Fault Vergence Scott R. Greenhalgh A thesis submitted to the faculty of Brigham Young University in partial fulfillment of the requirements for the degree of Master of Science John H. McBride, Chair Brooks B. Britt Bart J. Kowallis John M. Bartley Department of Geological Sciences Brigham Young University April 2014 Copyright © 2014 Scott R. Greenhalgh All Rights Reserved ABSTRACT Along Strike Variability of Thrust-Fault Vergence Scott R. Greenhalgh Department of Geological Sciences, BYU Master of Science The kinematic evolution and along-strike variation in contractional deformation in over- thrust belts are poorly understood, especially in three dimensions. The Sevier-age Cordilleran overthrust belt of southwestern Wyoming, with its abundance of subsurface data, provides an ideal laboratory to study how this deformation varies along the strike of the belt. We have per- formed a detailed structural interpretation of dual vergent thrusts based on a 3D seismic survey along the Wyoming salient of the Cordilleran overthrust belt (Big Piney-LaBarge field).
    [Show full text]
  • Folds and Folding
    Chapter ................................ 11 Folds and folding Folds are eye-catching and visually attractive structures that can form in practically any rock type, tectonic setting and depth. For these reasons they have been recognized, admired and explored since long before geology became a science (Leonardo da Vinci discussed them some 500 years ago, and Nicholas Steno in 1669). Our understanding of folds and folding has changed over time, and the fundament of what is today called modern fold theory was more or less consolidated in the 1950s and 1960s. Folds, whether observed on the micro-, meso- or macroscale, are clearly some of our most important windows into local and regional deformation histories of the past. Their geometry and expression carry important information about the type of deformation, kinematics and tectonics of an area. Besides, they can be of great economic importance, both as oil traps and in the search for and exploitation of ores and other mineral resources. In this chapter we will first look at the geometric aspects of folds and then pay attention to the processes and mechanisms at work during folding of rock layers. 220 Folds and folding 11.1 Geometric description (a) Kink band a a It is fascinating to watch folds form and develop in the laboratory, and we can learn much about folds and folding by performing controlled physical experiments and numerical simulations. However, modeling must always be rooted in observations of naturally folded Trace of Axial trace rocks, so geometric analysis of folds formed in different bisecting surface settings and rock types is fundamental. Geometric analy- (b) Chevron folds sis is important not only in order to understand how various types of folds form, but also when considering such things as hydrocarbon traps and folded ores in the subsurface.
    [Show full text]
  • Folds & Folding
    Folds and Folding Earth Structure (2nd Edition), 2004 W.W. Norton & Co, New York Slide show by Ben van der Pluijm © WW Norton; unless noted otherwise Folds Maryland Appalachians Swiss Alps 9/18/2010 © EarthStructure (2nd ed) 2 Fold Classification fold shape in profile interlimb angle similar/parallel symmetry/vergence fold size amplitude wavelength fold facing upward/downward fold orientation axis/hinge line axial surface fold in 3D cylindrical/non-cylindrical presence of secondary features foliation lineation DePaor, 2002 9/18/2010 © EarthStructure (2nd ed) 3 Fold terminology 9/18/2010 © EarthStructure (2nd ed) 4 Fold facing (a) upward facing antiform or anticline (b) upward facing synform or syncline (c) downward-facing antiform or antiformal syncline (d) downward-facing synform or synformal anticline (e) profile view; (f) map view 9/18/2010 © EarthStructure (2nd ed) 5 Fold Shape parallel fold similar fold ptygmatic folds 9/18/2010 © EarthStructure (2nd ed) 6 Fold shape a. Parallel fold b. Similar fold t is layer-perpendicular thickness; T is axial trace-parallel thickness 9/18/2010 © EarthStructure (2nd ed) 7 Dip isogons In Class 1A (a) the construction of a single dip isogon is shown, which connects the tangents to upper and lower boundary of folded layer with equal angle (α) relative to a reference frame; dip isogons at 10° intervals are shown for each class. Class 1 folds (a– c) have convergent dip isogon patterns; dip isogons in Class 2 folds (d) are parallel; Class 3 folds (e) have divergent dip isogon patterns. In this classification, parallel (b) and similar (d) folds are labeled as Class 1B and Class 2, respectively.
    [Show full text]