Carbon Fluxes and Primary Magma CO2 Contents Along the Global Mid
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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. -
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). -
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 . -
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. -
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. -
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. -
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. -
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. -
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 . -
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). -
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. -
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.