Formation of Melange in Afore/And Basin Overthrust Setting: Example from the Taconic Orogen
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Nd Isotope Mapping of the Grenvillian Allochthon Boundary Thrust in Algonquin Park, Ontario
Canadian Journal of Earth Sciences Nd isotope mapping of the Grenvillian Allochthon Boundary Thrust in Algonquin Park, Ontario Journal: Canadian Journal of Earth Sciences Manuscript ID cjes-2018-0142.R1 Manuscript Type: Article Date Submitted by the 26-Sep-2018 Author: Complete List of Authors: Dickin, Alan; School of Geography and Geology Strong, Jacob; School of Geography and Geology Keyword: Nd isotopes,Draft Model ages, Grenville Province Is the invited manuscript for consideration in a Special Not applicable (regular submission) Issue? : https://mc06.manuscriptcentral.com/cjes-pubs Page 1 of 34 Canadian Journal of Earth Sciences 1 Nd isotope mapping of the Grenvillian Allochthon Boundary Thrust in Algonquin Park, 2 Ontario 3 4 A.P. Dickin and J.W.D. Strong 5 School of Geography and Earth Sciences, McMaster University, Hamilton ON, Canada 6 7 Abstract 8 Over fifty new Nd isotope analyses are presented for high-grade orthogneisses from 9 Algonquin Park and surrounding region in order to map major Grenvillian thrust boundaries. Nd 10 model ages display a consistent geographical pattern that allows detailed mapping of the 11 boundary between the Algonquin and MuskokaDraft domains, here interpreted as the local trajectory 12 of the Ottawan-age Allochthon Boundary Thrust (ABT). The ABT is underlain by a domain with 13 Paleoproterozoic Nd model ages, interpreted as a tectonic duplex entrained onto the base of the 14 main allochthon. The boundaries determined using Nd isotope mapping are consistent with field 15 mapping and with remotely sensed aeromagnetic and digital elevation data. The precise location 16 of the ABT can be observed in a road-cut on Highway 60, on the north shore of the Lake of Two 17 Rivers in the centre of Algonquin Park. -
The Geology of the Enosburg Area, Vermont
THE GEOLOGY OF THE ENOSBURG AREA, VERMONT By JOlIN G. DENNIS VERMONT GEOLOGICAL SURVEY CHARLES G. DOLL, State Geologist Published by VERMONT DEVELOPMENT DEPARTMENT MONTPELIER, VERMONT BULLETIN No. 23 1964 TABLE OF CONTENTS PAGE ABSTRACT 7 INTRODUCTION ...................... 7 Location ........................ 7 Geologic Setting .................... 9 Previous Work ..................... 10 Method of Study .................... 10 Acknowledgments .................... 10 Physiography ...................... 11 STRATIGRAPHY ...................... 12 Introduction ...................... 12 Pinnacle Formation ................... 14 Name and Distribution ................ 14 Graywacke ...................... 14 Underhill Facics ................... 16 Tibbit Hill Volcanics ................. 16 Age......................... 19 Underhill Formation ................... 19 Name and Distribution ................ 19 Fairfield Pond Member ................ 20 White Brook Member ................. 21 West Sutton Slate ................... 22 Bonsecours Facies ................... 23 Greenstones ..................... 24 Stratigraphic Relations of the Greenstones ........ 25 Cheshire Formation ................... 26 Name and Distribution ................ 26 Lithology ...................... 26 Age......................... 27 Bridgeman Hill Formation ................ 28 Name and Distribution ................ 28 Dunham Dolomite .................. 28 Rice Hill Member ................... 29 Oak Hill Slate (Parker Slate) .............. 29 Rugg Brook Dolomite (Scottsmore -
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. -
Chapter 8 Large Strains
Chapter 8 Large Strains Introduction Most geological deformation, whether distorted fossils or fold and thrust belt shortening, accrues over a long period of time and can no longer be analyzed with the assumptions of infinitesimal strain. Fortunately, these large, or finite strains have the same starting point that infinitesimal strain does: the deformation and dis- placement gradient tensors. However, we must clearly distinguish between gradi- ents in position or displacement with respect to the initial (material) or to the final (spatial) state and several assumptions from the last Chapter — small angles, addi- tion of successive phases or steps in the deformation — no longer hold. Finite strain can get complicated very quickly with many different tensors to worry about. Most of our emphasis here will be on the practical measurement of finite strain rather than the details of the theory but we do have to review a few basic concepts first, so that we can appreciate the differences between finite and infinitesimal strain. Some of these differences have a profound impact on how we analyze de- formation. CHAPTER 8 FINITE STRAIN Comparison to Infinitesimal Strain A Plethora of Finite Strain Tensors There are lots of finite strain tensors and they come in pairs: one referenced to the initial state and the other referenced to the final state. The derivation of these tensors is usually based on Figure 7.3 and is tedious but straightforward; we will skip the derivation here but you can see it in Allmendinger et al. (2012) or any good continuum mechanics text. The first tensor is the Lagrangian strain tensor: 1 ⎡ ∂ui ∂u j ∂uk ∂uk ⎤ 1 " Lij = ⎢ + + ⎥ = ⎣⎡Eij + E ji + EkiEkj ⎦⎤ (8.1) 2 ⎣∂ X j ∂ Xi ∂ Xi ∂ X j ⎦ 2 where Eij is the displacement gradient tensor from the last Chapter. -
Tectonic Klippe Served the Needs of Cult Worship, Sanctuary of Zeus, Mount Lykaion, Peloponnese, Greece
Tectonic Klippe Served the Needs of Cult Worship, Sanctuary of Zeus, Mount Lykaion, Peloponnese, Greece George H. Davis, Dept. of Geosciences, The University of Arizona, Tucson, Arizona 85721, USA, [email protected] ABSTRACT Mount Lykaion is a rare, historical, cul- tural phenomenon, namely a Late Bronze Age through Hellenistic period (ca. 1500– 100 BC) mountaintop Zeus sanctuary, built upon an unusual tectonic feature, namely a thrust klippe. Recognition of this klippe and its physical character provides the framework for understanding the cou- pling between the archaeology and geology of the site. It appears that whenever there were new requirements in the physical/ cultural expansion of the sanctuary, the overall geologic characteristics of the thrust klippe proved to be perfectly adapt- able. The heart of this analysis consists of detailed geological mapping, detailed structural geologic analysis, and close cross-disciplinary engagement with archaeologists, classicists, and architects. INTRODUCTION Figure 1. Location of the Sanctuary of Zeus, Mount Lykaion, Peloponnese, Greece. In the second century AD, Pausanias authored an invaluable description of the residual worked blocks of built structures The critical geologic emphasis here is Sanctuary of Zeus, Mount Lykaion, and activity areas, including a hippodrome that Mount Lykaion is a thrust klippe. located at latitude 37° 23′ N, longitude and stadium used for athletic games in Thrusting was achieved during tectonic 22° 00′ E, in the Peloponnese (Fig. 1). ancient times (see Romano and Voyatzis, inversion of Jurassic to early Cenozoic Pausanias’ accounts were originally writ- 2014, 2015). Pindos Basin stratigraphy (Degnan and ten in Greek and are available in a number In 2004, I signed on as geologist for the Robertson, 2006; Doutsos et al., 1993; of translations and commentaries, includ- Mount Lykaion Excavation and Survey Skourlis and Doutsos, 2003). -
Gy403 Structural Geology Kinematic Analysis Kinematics
GY403 STRUCTURAL GEOLOGY KINEMATIC ANALYSIS KINEMATICS • Translation- described by a vector quantity • Rotation- described by: • Axis of rotation point • Magnitude of rotation (degrees) • Sense of rotation (reference frame; clockwise or anticlockwise) • Dilation- volume change • Loss of volume = negative dilation • Increase of volume = positive dilation • Distortion- change in original shape RIGID VS. NON-RIGID BODY DEFORMATION • Rigid Body Deformation • Translation: fault slip • Rotation: rotational fault • Non-rigid Body Deformation • Dilation: burial of sediment/rock • Distortion: ductile deformation (permanent shape change) TRANSLATION EXAMPLES • Slip along a planar fault • 360 meters left lateral slip • 50 meters normal dip slip • Classification: normal left-lateral slip fault 30 Net Slip Vector X(S) 40 70 N 50m dip slip X(N) 360m strike slip 30 40 0 100m ROTATIONAL FAULT • Fault slip is described by an axis of rotation • Rotation is anticlockwise as viewed from the south fault block • Amount of rotation is 50 degrees Axis W E 50 FAULT SEPARATION VS. SLIP • Fault separation: the apparent slip as viewed on a planar outcrop. • Fault slip: must be measured with net slip vector using a linear feature offset by the fault. 70 40 150m D U 40 STRAIN ELLIPSOID X • A three-dimensional ellipsoid that describes the magnitude of dilational and distortional strain. • Assume a perfect sphere before deformation. • Three mutually perpendicular axes X, Y, and Z. • X is maximum stretch (S ) and Z is minimum stretch (S ). X Z Y Z • There are unique directions -
Best Practices for Shale Core Handling: Transportation, Sampling and Storage for Conduction of Analyses
Journal of Marine Science and Engineering Review Best Practices for Shale Core Handling: Transportation, Sampling and Storage for Conduction of Analyses Sudeshna Basu 1,2,*, Adrian Jones 1 and Pedram Mahzari 1 1 Department of Earth Sciences, University College London, London WC1E 6BS, UK; [email protected] (A.J.); [email protected] (P.M.) 2 Department of Chemical Engineering, University College London, London WC1E 7JE, UK * Correspondence: [email protected] Received: 9 January 2020; Accepted: 12 February 2020; Published: 20 February 2020 Abstract: Drill core shale samples are critical for palaeoenvironmental studies and potential hydrocarbon reservoirs. They need to be preserved carefully to maximise their retention of reservoir condition properties. However, they are susceptible to alteration due to cooling and depressurisation during retrieval to the surface, resulting in volume expansion and formation of desiccation and micro fractures. This leads to inconsistent measurements of different critical attributes, such as porosity and permeability. Best practices for core handling start during retrieval while extracting from the barrel, followed by correct procedures for transportation and storage. Appropriate preservation measures should be adopted depending on the objectives of the scientific investigation and core coherency, with respect to consolidation and weathering. It is particularly desirable to maintain a constant temperature of 1 to 4 ◦C and a consistent relative humidity of >75% to minimise any micro fracturing and internal moisture movement in the core. While core re-sampling, it should be ensured that there is no further core compaction, especially while using a hand corer. Keywords: shale; drill core instability; micro fracture; clay minerals 1. -
Ductile Deformation - Concepts of Finite Strain
327 Ductile deformation - Concepts of finite strain Deformation includes any process that results in a change in shape, size or location of a body. A solid body subjected to external forces tends to move or change its displacement. These displacements can involve four distinct component patterns: - 1) A body is forced to change its position; it undergoes translation. - 2) A body is forced to change its orientation; it undergoes rotation. - 3) A body is forced to change size; it undergoes dilation. - 4) A body is forced to change shape; it undergoes distortion. These movement components are often described in terms of slip or flow. The distinction is scale- dependent, slip describing movement on a discrete plane, whereas flow is a penetrative movement that involves the whole of the rock. The four basic movements may be combined. - During rigid body deformation, rocks are translated and/or rotated but the original size and shape are preserved. - If instead of moving, the body absorbs some or all the forces, it becomes stressed. The forces then cause particle displacement within the body so that the body changes its shape and/or size; it becomes deformed. Deformation describes the complete transformation from the initial to the final geometry and location of a body. Deformation produces discontinuities in brittle rocks. In ductile rocks, deformation is macroscopically continuous, distributed within the mass of the rock. Instead, brittle deformation essentially involves relative movements between undeformed (but displaced) blocks. Finite strain jpb, 2019 328 Strain describes the non-rigid body deformation, i.e. the amount of movement caused by stresses between parts of a body. -
And Eastern Pennsylvania
GEOLOGY OF THE RIDGE AND VALLEY PROVINCE, NORTHWESTERN NEW JERSEY AND EASTERN PENNSYLVANIA JACK B. EPSTEIN U. S. Geological Survey, Reston, Va. 22092 INTRODUCTION The rocks seen in this segment of the field trip range A general transgressive-shelf sequence followed in age from Middle Ordovician to Middle Devonian and characterized mainly by tidal sediments and barrier bars constitute a.deep basin-continental-shallow shelf succes (Poxono Island, Bossardville, Decker, Rondout)~ suc sion. Within this succession, three lithotectonic units, or ceeded by generally subtidal and bar deposits (Helder sequences of rock that were deformed semi burg and Oriskany Groups), and then by deeper sub independently of each other, have somewhat different tidal deposits (Esopus, . Schoharie. and Buttermilk structural characteristics. Both the Alleghenian and Falls), finally giving way to another deep~water to Taconic orogenies have left their imprint on the rocks. shoaling sequence (Marcellus Shale through the Catskill Wind and water gaps are structurally controlled, thus Formation). Rocks of the Marcellus through Catskill placing doubt upon the hypothesis of regional super will not be seen on this trip. position. Wisconsinan deposits and erosion effects are common. We will examine these geologic features as This vertical stratigraphic sequence is complicated a well as some of the economic deposits in the area. bit because most Upper Silurian and Lower Devonian units are much thinner or are absent toward a paleo Figure 1 is an index map of the field-trip area, show positive area a few tens of miles southwest of the field ing the trip route and quadrangle coverage. Figure 2 is a trip area. -
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. -
The High Pressure Belt in the Grenville Province: 75 Architecture, Timing, and Exhumation1
100 867 100 95 95 75 The High Pressure belt in the Grenville Province: 75 architecture, timing, and exhumation1 25 25 Toby Rivers, John Ketchum, Aphrodite Indares, and Andrew Hynes 5 5 0 0 Abstract: We propose that the Grenvillian allochthonous terranes may be grouped into High Pressure (HP) and Low Pressure (LP) belts and examine the HP belt in detail in the western and central Grenville Province. The HP belt is developed in Paleo- and Mesoproterozoic rocks of the pre-Grenvillian Laurentian margin and characterized by Grenvillian eclogite and co-facial HP granulite in mafic rocks. Pressure–temperature (P–T) estimates for eclogite-facies conditions in well-preserved assemblages are about 1800 MPa and 850°C. In the central Grenville Province, HP rocks formed at -1060–1040 Ma and underwent a single stage of unroofing with transport into the upper crust by -1020 Ma, whereas farther west they underwent two stages of unroofing separated by penetrative mid-crustal recrystallization before transport to the upper crust at -1020 Ma. Unroofing processes were comparable in the two areas, involving both thrusting and extensional faulting in an orogen propagating into its foreland by understacking. In detail, thrusting episodes preceded extension in the western Grenville Province, whereas in the central Grenville Province, they were coeval, resulting in unroofing by tectonic extrusion. In the central Grenville Province, the footwall ramp is well preserved, but any former ramp in the western Grenville Province was obliterated by later lower crustal extensional flow. Continuation of the HP belt into the eastern Grenville Province is not established, but likely on geological grounds. -
Geometry and Kinematics of Bivergent Extension in the Southern Cycladic Archipelago: Constraining an Extensional Hinge Zone on S
RESEARCH ARTICLE Geometry and Kinematics of Bivergent Extension in 10.1029/2020TC006641 the Southern Cycladic Archipelago: Constraining an Key Points: Extensional Hinge Zone on Sikinos Island, Aegean Sea, • New and novel (re)interpretation of extension-related structures in Greece Cycladic Blueschist Unit • Extensional structures resulted from Uwe Ring1 and Johannes Glodny2 high degree of pure-shear flattening during general-shear deformation 1Department of Geological Sciences, Stockholm University, Stockholm, Sweden, 2GFZ German Research Centre for • Structures are interpreted to reflect Geosciences, Potsdam, Germany an extensional hinge zone in southern Cyclades Abstract We report the results of a field study on Sikinos Island in the Aegean extensional province Supporting Information: of Greece and propose a hinge zone controlling incipient bivergent extension in the southern Cyclades. Supporting Information may be found A first deformation event led to top-S thrusting of the Cycladic Blueschist Unit (CBU) onto the Cycladic in the online version of this article. basement in the Oligocene. The mean kinematic vorticity number (Wm) during this event is between 0.56 and 0.63 in the CBU, and 0.72 to 0.84 in the basement, indicating general-shear deformation with about Correspondence to: equal components of pure and simple shear. The strain geometry was close to plane strain. Subsequent U. Ring, [email protected] lower-greenschist-facies extensional shearing was also by general-shear deformation; however, the pure- shear component was distinctly greater (Wm = 0.3–0.41). The degree of subvertical pure-shear flattening Citation: increases structurally upward and explains alternating top-N and top-S shear senses over large parts of Ring, U., & Glodny, J.