Carbon Fluxes and Primary Magma CO2 Contents Along the Global Mid

Total Page:16

File Type:pdf, Size:1020Kb

Carbon Fluxes and Primary Magma CO2 Contents Along the Global Mid Geochemistry, Geophysics, Geosystems RESEARCH ARTICLE Carbon Fluxes and Primary Magma CO2 Contents Along 10.1029/2018GC007630 the Global Mid-Ocean Ridge System Special Section: Marion Le Voyer1,2, Erik H. Hauri1,3 , Elizabeth Cottrell2 , Katherine A. Kelley4 , Carbon degassing through Vincent J. M. Salters5 , Charles H. Langmuir6 , David R. Hilton7,8, Peter H. Barry9 , volcanoes and active tectonic 10 regions and Evelyn Füri 1Department of Terrestrial Magnetism, Carnegie Institution for Science, Washington, DC, USA, 2Smithsonian Institution, Key Points: National Museum of Natural History, Washington, DC, USA, 3Deceased 5 September 2018, 4Graduate School of Oceanography, • New analyses (753) and compiled University of Rhode Island, Narragansett, RI, USA, 5National High Magnetic Field Laboratory and Department of Earth, Ocean data (2,446) for volatiles CO ,HO, F, 2 2 and Atmospheric Sciences, Florida State University, Tallahassee, FL, USA, 6Department of Earth and Planetary Sciences, S, and Cl are reported in a global suite 7 of mid-ocean ridge basalts Harvard University, Cambridge, MA, USA, Scripps Institution of Oceanography, University of California San Diego, San Diego, 8 9 10 • Estimated primary MORB CO2 CA, USA, Deceased 7 January 2018, Department of Earth Sciences, University of Oxford, Oxford, UK, Centre de Recherches contents vary from 104 ppm to Pétrographiques et Géochimiques, UMR7358, CNRS - Université de Lorraine, Vandoeuvre-lès-Nancy, France 1.9 wt% and are the result of variations in mantle composition • fl High CO2 uxes at ridges correlate Abstract The concentration of carbon in primary mid-ocean ridge basalts (MORBs), and the associated with high primary CO2 contents and are due to the presence of fluxes of CO2 outgassed at ocean ridges, is examined through new data obtained by secondary ion mass subduction components in MORB spectrometry (SIMS) on 753 globally distributed MORB glasses. MORB glasses are typically 80–90% degassed sources of CO2. We thus use the limited range in CO2/Ba (81.3 ± 23) and CO2/Rb (991 ± 129), derived from undegassed MORB and MORB melt inclusions, to estimate primary CO2 concentrations for ridges that have Supporting Information: • Supporting Information S1 Ba and/or Rb data. When combined with quality-controlled volatile-element data from the literature • Data Set S1 (n = 2,446), these data constrain a range of primary CO2 abundances that vary from 104 ppm to 1.90 wt%. Segment-scale data reveal a range in MORB magma flux varying by a factor of 440 (from 6.8 × 105 to 3.0 × 108 3 3 m /year) and an integrated global MORB magma flux of 16.5 ± 1.6 km /year. When combined with CO2/Ba Correspondence to: and CO /Rb-derived primary magma CO abundances, the calculated segment-scale CO fluxes vary by K. A. Kelley, 2 2 2 7 10 [email protected] more than 3 orders of magnitude (3.3 × 10 to 4.0 × 10 mol/year) and sum to an integrated global MORB CO2 fl : þ0:77 12 fl ux of 1 320:85 ×10 mol/year. Variations in ridge CO2 uxes have a muted effect on global climate; however, because the vast majority of CO degassed at ridges is dissolved into seawater and enters the marine Citation: 2 Le Voyer, M., Hauri, E. H., Cottrell, E., bicarbonate cycle. MORB degassing would thus only contribute to long-term variations in climate via degassing Kelley, K. A., Salters, V. J. M., Langmuir, directly into the atmosphere in shallow-water areas or where the ridge system is exposed above sea level. C. H., et al. (2019). Carbon fluxes and primary magma CO2 contents along the Plain Language Summary Estimated CO2 contents of primary mid-ocean ridge basalts (MORB), global mid-ocean ridge system. calculated on a segment-by-segment basis, vary from 104 ppm to 1.9 wt%. CO -enriched MORB are Geochemistry, Geophysics, Geosystems, 2 20, 1387–1424. https://doi.org/10.1029/ present in all ocean basins, in particular, in the Atlantic Ocean basin, which is younger and more likely to 2018GC007630 contain admixed material from recent subduction compared to the much older Pacific Ocean basin. CO2 fluxes at individual ridge segments vary by 3 orders of magnitude due primarily to large variability in primary Received 18 APR 2018 CO content. This study provides the most detailed and accurate estimate to date of the integrated total flux Accepted 26 SEP 2018 2 : þ0:77 12 Accepted article online 23 NOV 2018 of CO2 from mid-ocean ridges of 1 320:85 ×10 mol/year. Published online 14 MAR 2019 1. Introduction The 56,000-km length of the global mid-ocean ridge system represents the dominant locus of magma production and heat loss on Earth. Decades of deep-water oceanographic research have revealed that new seafloor is produced over a limited range of crustal thicknesses (6 ± 1 km, Behn & Grove, 2015; Klein & Langmuir, 1987; Van Avendonk et al., 2017; White et al., 1992) and at variable spreading rates that are well-described globally (e.g., Gale et al., 2013). As a result, magma production rates at mid-ocean ridges are well understood and the fluxes of nonvolatile elements emerging from the mantle at ridges are well constrained. These same research cruises have retrieved tens of thousands of individual submarine mid-ocean ridge basalt (MORB) samples, and the study of these samples has revealed that chemical variations in MORB magmas are produced by polybaric melting of mantle sources at variable temperatures, ©2018. American Geophysical Union. whereas local deviations from global trends are primarily due to variations in mantle composition (Gale et al., All Rights Reserved. 2014; Kelley et al., 2013; Kinzler & Grove, 1992; Klein & Langmuir, 1987; Langmuir et al., 1992). LE VOYER ET AL. 1387 Geochemistry, Geophysics, Geosystems 10.1029/2018GC007630 Carbon is present in MORBs in trace amounts as CO2-rich vesicles and as carbonate ions dissolved in quenched seafloor glass (Cartigny et al., 2008; Dixon & Stolper, 1995; Javoy & Pineau, 1991; Marty & Tolstikhin, 1998; Michael, 1995). The solubility of CO2 in basaltic magma is low at hydrostatic pressures corre- sponding to seafloor water depths (e.g., Dixon et al., 1995; Jendrzejewski et al., 1997; Shishkina et al., 2010), and thus nearly all magmas erupted at mid-ocean ridges have degassed the majority of their carbon. This flux of CO2 into the oceans contributes to the global surface carbon cycle, and changes in basaltic magma pro- duction and associated degassing have been proposed as one of several important forcing mechanisms that have influenced past global climate variations (Burley & Katz, 2015; Robock, 2000; Shindell et al., 2003; Tolstoy, 2015; Zhong et al., 2010). At the same time, it is now widely recognized that most of the Earth’s carbon is pre- sent in the Earth’s deep interior, rather than at Earth’s surface (Marty et al., 2013; Marty & Tolstikhin, 1998). Importantly, basaltic magmatism and subduction of oceanic crust represent the two largest outgassing and ingassing fluxes at the interface between the surface and deep-Earth carbon cycles. These observations provide the motivation of the present study, in which we apply the rapid, precise, and accurate measurement of volatiles by secondary ion mass spectrometry (SIMS; Hauri et al., 2002) to characterize the extensive worldwide sample collection of MORBs to examine in detail the flux of CO2 from the global ridge system. In this study we report new SIMS data on 753 geographically distributed MORB samples, and combine these data with a quality-controlled database of published data from an additional 2,446 samples (Figure 1). This combined data set permits a description of CO2 fluxes, and estimated primary magma CO2 contents, for 381 of the 458 global ridge segments with major element data, in addition to examination of the variability of primary MORB CO2 contents, the role of carbon in the melting processes that produce MORB, and the role of the oceanic crust in the context of the Earth’s deep carbon cycle. 2. Methods Here we briefly describe the methods used in this study for sample preparation, SIMS analysis of volatile elements, major elements, and trace elements. 2.1. Sample Preparation The majority of the basalt glasses analyzed in this study were obtained from the Rock and Ore collection of the Smithsonian Institution’s National Museum of Natural History. The equatorial mid-Atlantic Ridge glasses were obtained from the Schilling Volcanic Glass collection at the University of Rhode Island (University of Rhode Island Graduate School of Oceanography Marine Geological Samples Laboratory, 2018). Additional glass samples were provided from the Pacific-Antarctic Ridge (PACANTARCTIC 1 and 2 cruises, Clog et al., 2013; Hamelin et al., 2010; Labidi et al., 2014; Moreira et al., 2008; Vlastelic et al., 1999, 2000), the Central Indian Ridge (GIMNAUT, CD127, and KNOX11RR cruises, Füri et al., 2011; Murton et al., 2005; Barry, 2012), the Southwest Indian Ridge (PROTEA-5, MD34, AG22, and AG53 cruises, Arevalo & McDonough, 2010; B. Hamelin & Allègre, 1985; Janney et al., 2005; Le Roex et al., 1989; Mahoney et al., 1992), and the East Pacific Rise (CHEPR and PANORAMA-1 cruises, Langmuir, 2014; Salters et al., 2011). The major element, trace ele- ment, and isotopic ratio data for the glasses measured in this study were compiled from the literature (Clog et al., 2013; Cottrell & Kelley, 2011; C. Hamelin et al., 2010; Jenner & O’Neill, 2012; Labidi et al., 2014; Le Voyer et al., 2015; Moreira et al., 2008; Vlastelic et al., 2000, 1999; Nauret et al., 2006). We selected 1- to 3-mm glass chips that did not show any sign of alteration, crystallization, or devitrification. The chips were pressed into indium mounts together with secondary standards (ALV519-4-1 and VG2), and polished using silicon carbide papers, diamond paste, and finally 0.3-μm alumina paste.
Recommended publications
  • Primordial Hydrogen-Helium Degassing, an Overlooked Major Energy Source for Internal Terrestrial Processes
    HAIT Journal of Science and Engineering B, Volume 2, Issues 1-2, pp. 125-167 Copyright C 2005 Holon Academic Institute of Technology ° Primordial hydrogen-helium degassing, an overlooked major energy source for internal terrestrial processes 1, 2 Arie Gilat ∗ and Alexander Vol 1Geological Survey of Israel (ret.), 8 Yehoash St., Jerusalem 93152, Israel 2Enlightment Ltd. 33 David Pinsky St., Haifa 34454, Israel ∗Corresponding author: [email protected] Received 20 July 2004, revised 3 February 2005, accepted 16 February 2005 Abstract The currently accepted theories concerning terrestrial processes are lacking in accounting for a source of internal energy which: (a) are quickly focused, e.g. earthquakes and volcanic eruptions; (b) are of very high density; (c) provide very high velocities of energy re- lease; (d) have very high density of the energy transport and relatively small losses during transportation over long distances; (e) are quasi- constantly released and practically limitless. This energy release is always accompanied by H- and He-degassing. Solid solutions of H and He, and compounds of He with H, O, Si and metals were discovered in laboratory experiments of ultra-high PT-conditions; He-S, He-Cl, He- C, He-N structures can be deduced from their atomic structure and compositions of natural He-reach gases. Ultra-high PT-conditions ex- ist in the Earth’s interior; hence it seems most likely that some “exotic” compounds are present in the Earth’s core and mantle. During Earth’s accretion, primordial hydrogen and helium were trapped and stored in the planet interior as H- and He- solutions and compounds, stable only under ultrahigh PT-conditions that were dis- covered in recent experiments.
    [Show full text]
  • Global Geochemical Variation of Mid-Ocean Ridge Basalts
    Master Thesis, Department of Geosciences Global geochemical variation of mid-ocean ridge basalts Hermann Drescher Global geochemical variation of mid-ocean ridge basalts Hermann Drescher Master Thesis in Geosciences Discipline: Geology Department of Geosciences and Centre for Earth Evolution and Dynamics Faculty of Mathematics and Natural Sciences University of Oslo August 2014 © Hermann Drescher, 2014 This work is published digitally through DUO – Digitale Utgivelser ved UiO http://www.duo.uio.no It is also catalogued in BIBSYS (http://www.bibsys.no/english) All rights reserved. No part of this publication may be reproduced or transmitted, in any form or by any means, without permission. Acknowledgements I would like to sincerely thank my supervisors Prof. Reidar G. Trønnes and Dr. Carmen Gaina for the opportunity to venture into new fields of study, for their continued support, great optimism, patience and helpful discussions and reviews. I would like to specially thank Grace Shephard and Johannes Jakob for their help with getting started with exploring Linux, bash scripting and GMT. Further I would like to thank everyone at CEED, my study room mates at the PGP floor and my fellow Master students for the friendly atmosphere and generally for a good time in Oslo. I would also like to thank my friends and family for their permanent support, understanding and great company. Finally I would like to thank Nikola Heroldová with all my heart for always and unconditionally supporting me, keeping me sane and standing by my side. II Abstract The asthenosphere beneath the global network of spreading ridges is continuously sampled by partial melting, generating mid-ocean ridge basalts (MORB).
    [Show full text]
  • Cenozoic Changes in Pacific Absolute Plate Motion A
    CENOZOIC CHANGES IN PACIFIC ABSOLUTE PLATE MOTION A THESIS SUBMITTED TO THE GRADUATE DIVISION OF THE UNIVERSITY OF HAWAI`I IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF MASTER OF SCIENCE IN GEOLOGY AND GEOPHYSICS DECEMBER 2003 By Nile Akel Kevis Sterling Thesis Committee: Paul Wessel, Chairperson Loren Kroenke Fred Duennebier We certify that we have read this thesis and that, in our opinion, it is satisfactory in scope and quality as a thesis for the degree of Master of Science in Geology and Geophysics. THESIS COMMITTEE Chairperson ii Abstract Using the polygonal finite rotation method (PFRM) in conjunction with the hotspot- ting technique, a model of Pacific absolute plate motion (APM) from 65 Ma to the present has been created. This model is based primarily on the Hawaiian-Emperor and Louisville hotspot trails but also incorporates the Cobb, Bowie, Kodiak, Foundation, Caroline, Mar- quesas and Pitcairn hotspot trails. Using this model, distinct changes in Pacific APM have been identified at 48, 27, 23, 18, 12 and 6 Ma. These changes are reflected as kinks in the linear trends of Pacific hotspot trails. The sense of motion and timing of a number of circum-Pacific tectonic events appear to be correlated with these changes in Pacific APM. With the model and discussion presented here it is suggested that Pacific hotpots are fixed with respect to one another and with respect to the mantle. If they are moving as some paleomagnetic results suggest, they must be moving coherently in response to large-scale mantle flow. iii List of Tables 4.1 Initial hotspot locations .
    [Show full text]
  • Origine De La Diversité Géochimique Des Magmas Équatoriens : De L’Arc Au Minéral
    N°d’Ordre : D.U. 926 UNIVERSITÉ CLERMONT AUVERGNE U.F.R. Sciences et Technologies Laboratoire Magmas et Volcans ÉCOLE DOCTORALE DES SCIENCES FONDAMENTALES N°178 THÈSE présentée pour obtenir le grade de DOCTEUR D’UNIVERSITÉ spécialité : Géochimie Par Marie-Anne ANCELLIN Titulaire du Master 2 Recherche Terre et Planètes Origine de la diversité géochimique des magmas équatoriens : de l’arc au minéral Thèse dirigée par Ivan VLASTÉLIC Soutenue publiquement le 17/11/2017 piouiMembres de la commission d’examen : Janne BLICHERT-TOFT Directrice de recherche à l’Ecole Normale Supérieure de Lyon Rapporteur Gaëlle PROUTEAU Maitre de Conférence HDR à l’Université d’Orléans Rapporteur Kevin BURTON Professeur à l’Université de Durham Examinateur Hervé MARTIN Professeur à l’Université Clermont Auvergne, Clermont-Ferrand Examinateur Silvana HIDALGO Professeur à l’Escuela Politécnica Nacional, Quito Invité François NAURET Maitre de Conférence à l’Université Clermont Auvergne, Clermont-Ferrand Invité Ivan VLASTÉLIC Chargé de recherce HDR à l’Université Clermont Auvergne, Clermont-Ferrand Directeur de thèse Pablo SAMANIEGO Chargé de recherche à l’IRD, Université Clermont Auvergne, Clermont-Ferrand Co-encadrant de thèse Laboratoire Magmas et Volcans Université Clermont Auvergne Campus Universitaire des Cézeaux 6 Avenue Blaise Pascal TSA 60026 – CS 60026 63178 AUBIERE Cedex ii RÉSUMÉ Origine de la diversité géochimique des magmas équatoriens : de l’arc au minéral Les laves d’arc ont une géochimie complexe du fait de l’hétérogénéité des magmas primitifs et de leur transformation dans la croûte. L’identification des magmas primitifs dans les arcs continentaux est difficile du fait de l’épaisseur de la croûte continentale, qui constitue un filtre mécanique et chimique à l’ascension des magmas.
    [Show full text]
  • Arxiv:1906.03473V2 [Physics.Geo-Ph] 30 Dec 2019 Double the Carbon Solubility in fluids Co-Existing with Sediments Subducted Along Cool Geotherms
    Devolatilization of Subducting Slabs, Part II: Volatile Fluxes and Storage Meng Tian,1, ∗ Richard F. Katz,1 David W. Rees Jones,1, 2, 3 and Dave A. May1 1Department of Earth Sciences, University of Oxford, South Parks Road, Oxford, OX1 3AN, UK. 2Department of Earth Sciences, Bullard Laboratories, University of Cambridge, Madingley Road, Cambridge, CB3 0EZ, UK. 3School of Mathematics and Statistics, University of St Andrews, North Haugh, St Andrews, KY16 9SS, UK Subduction is a crucial part of the long-term water and carbon cycling between Earth's exo- sphere and interior. However, there is broad disagreement over how much water and carbon is liberated from subducting slabs to the mantle wedge and transported to island-arc volcanoes. In the companion paper Part I, we parameterize the metamorphic reactions involving H2O and CO2 for representative subducting lithologies. On this basis, a two-dimensional reactive transport model is constructed in this Part II. We assess the various controlling factors of CO2 and H2O release from subducting slabs. Model results show that up-slab fluid flow directions produce a flux peak of CO2 and H2O at subarc depths. Moreover, infiltration of H2O-rich fluids sourced from hydrated slab mantle enhances decarbonation or carbonation at lithological interfaces, increases slab surface fluxes, and redistributes CO2 from basalt and gabbro layers to the overlying sedimentary layer. As a result, removal of the cap sediments (by diapirism or off-scraping) leads to elevated slab surface CO2 and H2O fluxes. The modelled subduction efficiency (the percentage of initially subducted volatiles retained until ∼200 km deep) of H2O and CO2 is increased by open-system effects due to fractionation within the interior of lithological layers.
    [Show full text]
  • Chemical Systematics of an Intermediate Spreading Ridge: the Pacific-Antarctic Ridge Between 56°S and 66°S
    JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 105, NO. B2, PAGES 2915-2936, FEBRUARY 10, 2000 Chemical systematics of an intermediate spreading ridge: The Pacific-Antarctic Ridge between 56°S and 66°S Ivan Vlastélic,I,2 Laure DOSSO,I Henri Bougault/ Daniel Aslanian,3 Louis Géli,3 Joël Etoubleau,3 Marcel Bohn,1 Jean-Louis Joron,4 and Claire Bollinger l Abstract. Axial bathymetry, major/trace elements, and isotopes suggest that the Pacific-Antarctic Ridge (PAR) between 56°S and 66°S is devoid of any hotspot influence. PAR (56-66°S) samples 144 have in average lower 87Sr/86Sr and 143 Nd/ Nd and higher 206 PbP04 Pb than northern Pacific l11id­ ocean ridge basalts (MORB), and also than MORB From the other oceans. The high variability of pb isotopic ratios (compared to Sr and Nd) can be due to either a general high ~l (I-IIMU) (high U/Pb) affïnity of the southern Pacific upper mantle or to a mantle event first recorded in time by Pb isotopes. Compiling the results ofthis study with those From the PAR between 53°S and 57°S gives a continuous vie~ of mantle characteristics fr~m sOl~th ,Pitman. Fracture Z?ne (FZ) to . Vacquier FZ, representll1g about 3000 km of spreadll1g aXIs. [he latitude ofUdmtsev FZ (56°S) IS a limit between, to the narth, a domain with large geochemical variations and, to the south, one with small variations. The spreading rate has intermediate values (54 mm/yr at 66°S to 74 mm/yr at 56°S) which increase along the PAR, while the axial morphology changes from valley to dome.
    [Show full text]
  • The Transition-Zone Water Filter Model for Global Material Circulation: Where Do We Stand?
    The Transition-Zone Water Filter Model for Global Material Circulation: Where Do We Stand? Shun-ichiro Karato, David Bercovici, Garrett Leahy, Guillaume Richard and Zhicheng Jing Yale University, Department of Geology and Geophysics, New Haven, CT 06520 Materials circulation in Earth’s mantle will be modified if partial melting occurs in the transition zone. Melting in the transition zone is plausible if a significant amount of incompatible components is present in Earth’s mantle. We review the experimental data on melting and melt density and conclude that melting is likely under a broad range of conditions, although conditions for dense melt are more limited. Current geochemical models of Earth suggest the presence of relatively dense incompatible components such as K2O and we conclude that a dense melt is likely formed when the fraction of water is small. Models have been developed to understand the structure of a melt layer and the circulation of melt and vola- tiles. The model suggests a relatively thin melt-rich layer that can be entrained by downwelling current to maintain “steady-state” structure. If deep mantle melting occurs with a small melt fraction, highly incompatible elements including hydro- gen, helium and argon are sequestered without much effect on more compatible elements. This provides a natural explanation for many paradoxes including (i) the apparent discrepancy between whole mantle convection suggested from geophysical observations and the presence of long-lived large reservoirs suggested by geochemical observations, (ii) the helium/heat flow paradox and (iii) the argon paradox. Geophysical observations are reviewed including electrical conductivity and anomalies in seismic wave velocities to test the model and some future direc- tions to refine the model are discussed.
    [Show full text]
  • End of Chapter Question Answers Chapter 4 Review Questions 1
    End of Chapter Question Answers Chapter 4 Review Questions 1. Describe the three processes that are responsible for the formation of magma. Answer: Magmas form from melting within the Earth. There are three types of melting: decompression melting, where magmas form when hot rock from deep in the mantle rises to shallower depths without undergoing cooling (the decrease in pressure facilitates the melting process); flux melting, where melting occurs due to the addition of volatiles such as CO2 and H2O; and heat transfer melting, where melting results from the transfer of heat from a hotter material to a cooler one. 2. Why are there so many different compositions of magma? Does partial melting produce magma with the same composition as the magma source from which it was derived? Answer: Magmas are formed from many different chemical constituents. Partial melting of rock yields magma that is more felsic (silicic) than the magma source because a higher proportion of chemicals needed to form felsic minerals diffuse into the melt at lower temperatures. Magma may incorporate chemicals dissolved from the solid rock through which it rises or from blocks of rock that fall into the magma. This process is called assimilation. Finally, fractional crystallization can modify magma composition as minerals crystallize out of a melt during the cooling process, causing the residual liquid to become progressively more felsic. 3. Why does magma rise from depth to the surface of the Earth? Answer: Magma rises toward the surface of the Earth because it is less dense than solid rock and buoyant relative to its surroundings.
    [Show full text]
  • 06EAS458-7 Melting
    Why the Earth Melts EAS 458 Volcanology Lecture 7 How to Melt a Rock? . Raise the temperature . Heat production: radioactive heating, friction, impact heating . Heat conduction or advection . May occur in the crust, particularly where high-T magma intrudes low solidus country rock, otherwise, conduction is not efficient . Decompression . If the adiabatic gradient and the solidus intersect, rising rock will melt. This is the most important melting mechanism. Therefore, in a certain sense, volcanoes are like clouds. Lower the melting point . Just as salt lowers the freezing point of water, addition of some substances ( a flux) to rock can lower its melting point. Water is the most effective and most likely flux . This is very likely important in subduction zones 1 . Volcanism occurs at: . Divergent plate boundaries . Convergent plate boundaries . More rarely in plate interiors Decompression Melting . Decompression of rising mantle accounts for most volcanism on Earth, in particular, volcanism at divergent plate boundaries and in intraplate settings. With the help of thermodynamics, we can readily understand why this melting occurs. 2 Fundamental Variables . T: temperature . always absolute temperature, or Kelvins, in thermodynamics . P: pressure . force per unit area; SI unit is the Pascal (P) = 1 Newton/m2 = 1 kg-m/s2; in geology, we use MPa (106 Pa) or GPa (109 Pa). 1 atm ≈ 1 bar = 0.1 MPa. In the mantle pressure increases at a rate of ~ 1 GPa for each 35 km depth. V: volume Fundamental Variables . U: Energy . SI unit is the Joule . Q: Heat: a form of energy . W: Work: a form of energy dW = -PdV .
    [Show full text]
  • Chapter 3 Intrusive Igneous Rocks
    Chapter 3 Intrusive Igneous Rocks Learning Objectives After carefully reading this chapter, completing the exercises within it, and answering the questions at the end, you should be able to: • Describe the rock cycle and the types of processes that lead to the formation of igneous, sedimentary, and metamorphic rocks, and explain why there is an active rock cycle on Earth. • Explain the concept of partial melting and describe the geological processes that lead to melting. • Describe, in general terms, the range of chemical compositions of magmas. • Discuss the processes that take place during the cooling and crystallization of magma, and the typical order of crystallization according to the Bowen reaction series. • Explain how magma composition can be changed by fractional crystallization and partial melting of the surrounding rocks. • Apply the criteria for igneous rock classification based on mineral proportions. • Describe the origins of phaneritic, porphyritic, and pegmatitic rock textures. • Identify plutons on the basis of their morphology and their relationships to the surrounding rocks. • Explain the origin of a chilled margin. 65 Physical Geology - 2nd Edition 66 Figure 3.0.1 A fine-grained mafic dyke (dark green) intruded into a felsic dyke (pink) and into coarse diorite (grey), Quadra Island, B.C. All of these rocks are composed of more than one type of mineral. The mineral components are clearly visible in the diorite, but not in the other two rock types. A rock is a consolidated mixture of minerals. By consolidated, we mean hard and strong; real rocks don’t fall apart in your hands! A mixture of minerals implies the presence of more than one mineral grain, but not necessarily more than one type of mineral (Figure 3.0.1).
    [Show full text]
  • University of California Santa Cruz Lower
    UNIVERSITY OF CALIFORNIA SANTA CRUZ LOWER CRUSTAL XENOLITHS OF THE SOUTHERN SIERRA NEVADA: A MAJOR ELEMENT AND GEOCHRONOLOGICAL INVESTIGATION A thesis submitted in partial satisfaction of the requirements for the degree of MASTER OF SCIENCE In EARTH SCIENCES by Adrienne Grant December 2016 The Thesis of Adrienne Grant is approved: Professor Terrence Blackburn, Chair Professor Jeremy Hourigan Professor Elise Knittle Tyrus Miller Vice Provost and Dean of Graduate Studies Table of Contents Table of Contents iii List of Figures iii Abstract iv Introduction 1 Geologic Background 5 Methods 7 Results 8 Discussion 15 Conclusion 23 Appendix 1 24 Appendix 2 25 Appendix 3 26 References 30 List of Figures Figure 1. Experimental results for melt compositions generated by partial melting of hydrous basalts at high pressure 3 Figure 2. Experimental results for melt compositions generated by fractional crystallization of hydrous basalt at high pressure 3 Figure 3. General map of the Sierra Nevada with expanded local map of study area 6 Figure 4. CL populations of 15-CP-01 10 Figure 5. Representative CL photomicrographs of tonalite samples 15-CPX-03 and 15-CPX-04 10 Figure 6. Compiled weighted mean plot of zircon dates from selected samples 12 Figure 7. Mg# versus wt% SiO2 13 Figure 8. Minimum and maximum sample age versus wt% SiO2 (pink) and Mg# (green) 14 Figure 9. CL images showing zircons with metamorphic rims and overgrowths 16 Figure 10. Cumulate textures in sample 116478-0027 16 List of Appendices Appendix 1. Major element chemistry data 23 Appendix 2. Thin Section description table 24 Appendix 3.
    [Show full text]
  • Young Tracks of Hotspots and Current Plate Velocities
    Geophys. J. Int. (2002) 150, 321–361 Young tracks of hotspots and current plate velocities Alice E. Gripp1,∗ and Richard G. Gordon2 1Department of Geological Sciences, University of Oregon, Eugene, OR 97401, USA 2Department of Earth Science MS-126, Rice University, Houston, TX 77005, USA. E-mail: [email protected] Accepted 2001 October 5. Received 2001 October 5; in original form 2000 December 20 SUMMARY Plate motions relative to the hotspots over the past 4 to 7 Myr are investigated with a goal of determining the shortest time interval over which reliable volcanic propagation rates and segment trends can be estimated. The rate and trend uncertainties are objectively determined from the dispersion of volcano age and of volcano location and are used to test the mutual consistency of the trends and rates. Ten hotspot data sets are constructed from overlapping time intervals with various durations and starting times. Our preferred hotspot data set, HS3, consists of two volcanic propagation rates and eleven segment trends from four plates. It averages plate motion over the past ≈5.8 Myr, which is almost twice the length of time (3.2 Myr) over which the NUVEL-1A global set of relative plate angular velocities is estimated. HS3-NUVEL1A, our preferred set of angular velocities of 15 plates relative to the hotspots, was constructed from the HS3 data set while constraining the relative plate angular velocities to consistency with NUVEL-1A. No hotspots are in significant relative motion, but the 95 per cent confidence limit on motion is typically ±20 to ±40 km Myr−1 and ranges up to ±145 km Myr−1.
    [Show full text]