DOCSLIB.ORG

The Lehmann Discontinuity Due to Dehydration of Subducted Sediment Shigeaki Ono*,1,2

Total Page：16

File Type：pdf, Size：1020Kb

Download full-text PDF Read full-text
The Lehmann Discontinuity Due to Dehydration of Subducted Sediment Shigeaki Ono*,1,2 The Open Mineralogy Journal, 2007, 1, 1-4 1 The Lehmann Discontinuity Due to Dehydration of Subducted Sediment Shigeaki Ono*,1,2 1Institute for Research on Earth Evolution, Japan Agency for Marine-Earth Science and Technology, 2-15 Natsushima-cho, Yokosuka-shi, Kanagawa 237-0061, Japan 2Department of Earth Sciences, University College London, Gower Street, London WC1E 6BT, UK Abstract: Recent high-pressure experiments have led to the conclusion that water release from subducted sediments lying under continents in subduction regions occurs at about 220 km depth. This dehydration reaction is in good agreement with the seismological signature of the discontinuity indicating that sediment dehydration causes the Lehmann discontinuity in the upper mantle. Keywords: Lehmann discontinuity, high pressure, water, dehydration, 220 km, sediment. 1. INTRODUCTION the upper mantle, whereas most observations are under con- tinents. It is therefore impossible to explain the local occur- The Lehmann discontinuity was first observed in Europe rence of the discontinuity using this concept. and North America from seismic refraction studies beneath continents [1, 2]. The discontinuity is characterized by the In the case of the silica phase transition, if the coesite- following features: (1) The depth of the seismic discontinuity stishovite transformation occurs at 220 km depth, the tem- is around 220 km depth. (2) A regionally varying negative perature of the upper mantle would be about 800 K; far too seismological Clapeyron slope (dP/dT) of the discontinuity low a typical temperature for this depth. Although both depth has been estimated [3]. (3) The discontinuity has not phase transitions have a positive Clapeyron slope, such a been detected everywhere at around 220 km depth [4]. It is negative seismological Clapeyron slope has been reported observed under continents more than twice as often as under [3]. It is, therefore, difficult to explain the origin of the dis- oceans [5], and the largest amplitudes of this discontinuity continuity simply by mineral transition. appear beneath the continents [6]. (4) An increase in the The relationship between the seismic discontinuity and compressional or shear wave velocity and in seismic reflec- chemical boundaries in the mantle has often been discussed tions from around 220 km depth has been reported [7, 8]. (5) [15]. Chemical change induces a different mineral assem- A seismic transition from anisotropic to a more isotropic blage. As the physical properties of rock are influenced by state occurs at depths corresponding to the Lehmann discon- each constituent mineral, the seismic discontinuities can be a tinuity [9, 10]. reflection of a chemical boundary. There is no clear evi- The phase transitions of (Mg,Fe)SiO3 pyroxene [11, 12] dence, however, that such a boundary exists at 220 km depth and silica (SiO2) [13, 14] were reported at high pressures in the upper mantle [16, 17]. corresponding to the depth of the Lehmann discontinuity. Karato [18] proposed that the change of deformation These transitions seemed to be candidates for the origin of mechanism from dislocation creep to diffusion creep caused the discontinuity. However, both models have serious flaws, the Lehmann discontinuity. The diffusion creep is due to and from the view point of the mineralogy, those characteris- transport of matter by self-diffusion through the grains of a tic features of this discontinuity could not be explained by polycrystal. In the case of the dislocation creep, dislocations previous models. are carriers of plastic deformation in solids. Olivine shows a The dP/dT slope of the mineralogical phase transition is pressure-induced change in its deformation mechanism. This one of the important features to understand the structure of seems to occur between 240 and 380 km depth. This varia- the mantle. This slope can be expressed using differences of tion is due to differing parameters of grain size, temperature, entropy and volume at the transition (dP/dT = dS/dV). The water fugacity, and strain rate. This model can explain a ve- seismological Clapeyron slope can be estimated using the locity jump at the depth of the deformation mechanism depth of the discontinuity and the relative seismic velocity change. However, if the mechanism change causes the seis- perturbation taken from a tomographic model [3]. mic discontinuity, this would be observed everywhere, be- cause olivine is a major mineral present in the upper mantle. (Mg,Fe)SiO pyroxene is one of the major minerals pre- 3 As most observations of the Lehmann discontinuity are lo- sent in the pyrolite mantle, which has a typical upper mantle cal, this hypothesis cannot be accepted. composition. If the phase transition of pyroxene causes the seismic discontinuity, this would be observed everywhere in In this paper, it is proposed that the Lehmann discontinu- ity is a consequence of the dehydration of subducted sedi- ment. The proposal is made on the basis of high-pressure *Address correspondence to this author at the Department of Earth Sci- experiments using a multianvil press. This new model can ences, University College London, Gower Street, London WC1E 6BT, UK; explain all the characteristic features of the discontinuity Tel: +44-(0)20-7679-3424; Fax: +44-(0)20-7679-4166; such as depth, seismological Clapeyron slope, locality of E-mail: [email protected] observation and the velocity jump. 1874-4567/07 2007 Bentham Science Publishers Ltd. 2 The Open Mineralogy Journal, 2007, Volume 1 Shigeaki Ono 2. EXPERIMENTAL WORKS OH. The volume of fluid released in low temperature loca- tions typified by the subduction zone is therefore less than in We conducted experiments with hydrous sediment. Sam- a normal mantle geothermal region. ples were contained in Au75Pd25 capsules and the tempera- ture was varied between 1073 and 1673 K, while a pressure of 6-15 GPa was applied using the multi-anvil press. A syn- Temperature (K) 800 1000 1200 1400 1600 1800 2000 thetic gel was used to produce a reactive and homogeneous 100 starting material. We confirmed that the gel starting material Oceanic 4 quickly achieved a nearly equilibrium state in the multi-anvil Continental experiments [19]. The typical pelite composition was used as 6 the sediment [20]. Sediment with 6 wt% H2O was produced 200 G+C+Co+P+f from synthetic dry gel and reagent-grade Al(OH)3 as the G+C+Co+f Pressure (GPa) maximum H2O content stored in the sediment composition 8 G+C+S+P+f was less than 6 wt%, our experiment was a water saturated condition. It is known that the natural subducted sediment 300 10 has a considerable variation of chemical composition. Com- G+C+S+H+F+T+f G+C+S+H+F+K+f positional changes of experimental starting material can Depth (km) 12 change the mineral proportions of hydrous minerals. The influence of compositional change in sediments was dis- 400 14 cussed in our previous study [21]. The average composition G+C+S+H+F+E+f G+C+S+H+F+f of continental crust is sufficiently close to the sediment composition so that the phase relationships of the sediment Geotherm 16 composition may be generally applicable to that of continen- 500 tal crust. Details of the experimental procedure and results are described elsewhere [21]. Fig. (1). Experimental constraints on the dehydration of subducted Garnet ((Ca,Fe,Mg)3(Al,Fe)2Si3O12), clinopyroxene ((Ca, sediment. Symbols represent observed phase assemblages. Thin Fe,Mg)2-x(NaAl)xSi2O6), and silica (SiO2) phases were pre- lines represent the inferred boundaries of phase relation of sediment sent in all of the experiments. Three hydrous phases were [21]. Abbreviations of phases are as follows: G, garnet; C, clinopy- observed at temperatures below 1573 K. The stable crystal- roxene; Co, coesite; S, stishovite; K, kyanite; H, K-hollandite; F, line hydrous minerals consisted of phengite ((K,Na)Al2(Si3 Fe-Ti oxide; P, phengite; T, topaz-OH; E, phase egg; f, fluid. The Al)O10(OH)2) below 8 GPa, topaz-OH (Al2SiO4(OH)2) from thick line represents the dehydration boundary of phengite. The 9-12 GPa, and phase egg (AlSiO3(OH)) above 12 GPa (Fig. dashed lines represent typical geotherms under oceanic and conti- 1). The breakdown boundaries of topaz-OH and phase egg nental crust. The geotherms intersect with the phengite dehydration show a positive Clapeyron slope. In contrast, the breakdown boundary at ~220 km depth. reaction of phengite gave a negative slope at about 7 GPa 3. ORIGIN OF LEHMANN DISCONTINUITY corresponding to 220 km depth. In the case of most high- pressure hydrous mineral, such as alphabet phases, the stabil- The physical properties of water in the upper mantle are ity limit in response to temperature is not high [22]. How- distinctly different to those of silicate minerals. It seems ever, the upper temperature limit for phengite is greater than nevertheless difficult to explain the origin of the Lehmann 1473 K. This phase is thus likely to be stable within average discontinuity by water alone. As the volume of the subducted adiabatic mantle conditions. sediment is likely to be very small and the volume of the released water from the sediment is also negligible, the in- Water-saturated experiments show that the maximum fluence of water itself on the discontinuity is not considered water content in subducted sediment is ~2 wt% H O, be- 2 important. One interesting feature of water is its percolation cause phengite, which includes ~4 wt% H O, constitutes ~50 2 into the surrounding rocks. When the dehydration occurs, wt% of the assemblage. In the case of the continental com- water can migrate upwards by permeable flow because of the position, the water content is estimated to be a half of the large density difference between the fluid and the surround- sediment composition [21].
Load more

Recommended publications
  • Chapter 3. the Crust and Upper Mantle
    Theory of the Earth Don L. Anderson Chapter 3. The Crust and Upper Mantle Boston: Blackwell Scientific Publications, c1989 Copyright transferred to the author September 2, 1998. You are granted permission for individual, educational, research and noncommercial reproduction, distribution, display and performance of this work in any format. Recommended citation: Anderson, Don L. Theory of the Earth. Boston: Blackwell Scientific Publications, 1989. http://resolver.caltech.edu/CaltechBOOK:1989.001 A scanned image of the entire book may be found at the following persistent URL: http://resolver.caltech.edu/CaltechBook:1989.001 Abstract: T he structure of the Earth's interior is fairly well known from seismology, and knowledge of the fine structure is improving continuously. Seismology not only provides the structure, it also provides information about the composition, crystal structure or mineralogy and physical state. In subsequent chapters I will discuss how to combine seismic with other kinds of data to constrain these properties. A recent seismological model of the Earth is shown in Figure 3-1. Earth is conventionally divided into crust, mantle and core, but each of these has subdivisions that are almost as fundamental (Table 3-1). The lower mantle is the largest subdivision, and therefore it dominates any attempt to perform major- element mass balance calculations. The crust is the smallest solid subdivision, but it has an importance far in excess of its relative size because we live on it and extract our resources from it, and, as we shall see, it contains a large fraction of the terrestrial inventory of many elements. In this and the next chapter I discuss each of the major subdivisions, starting with the crust and ending with the inner core.
    [Show full text]
  • The Deep Structure of Continents
    VOL. 84, NO. B I3 JOURNAL OF GEOPHYSICAL RESEARCH DECEMBER 10, 1979 The Deep Structure of Continents DON L. ANDERSON SeismologicalLaboratory, California Institute of Technology,Pasadena, California 91125 The Lehmann discontinuityat 220-km depth is an important global feature which occursunder both oceansand continents.It is a barrier to penetrationby younglithosphere and marks the baseof seismic- ity in regionsof continent-continentcollision. The stronglateral variationin uppermantle velocitiesoc- cursmainly abovethis depth. Continentalroots extend no deeperthan about 150-200 km. The basalt- eclogitetransformation and eclogite-harzburgiteseparation may be responsiblefor the geometryof inter- mediatedepth earthquakes.Oceanic and continentalgeotherms converge above about 200 km and be- comeless steep than the meltinggradient at greaterdepth. This impliesa low viscositychannel near 250 km. This would give a decouplingzone of maximumshear beneath continental shields. The Lehmann discontinuitymay be the interfacebetween two distinctgeochemical reservoirs. The velocityjump, and the inferreddensity jump, at 220 km are consistentwith an increasein garnetcontent. The mantle may be garnetlherzolite above and eclogiteimmediately below the Lehmanndiscontinuity. The transitionre- gion may be mainly eclogiteand be the sourceregion for oceanictholeiites. INTRODUCTION nental values[Jordan and Anderson,1974; Jordan, 1975].Hart et al. [1977] determined an attenuation corrected free oscilla- Continental lithosphereis much thicker than oceanic litho- sphere,but the question of how thick a sectionof continent tion averageearth model, QM2, which is comparedwith the translatescoherently during continental drift has not yet been continentalmodel SHR14 of Helmbergerand Engen[1974] in adequatelyaddressed. The bottom of the low-velocity zone is Figure 2. A more direct comparisonis the Pacific-easternU.S. usuallyconsidered to be the bottom of the asthenosphereand curve which is from Cara's [1979] surfacewave study.
    [Show full text]
  • Upper-Mantle Low-Velocity Zone Structure Beneath the Kaapvaal Craton from S-Wave Receiver Functions
    Geophys. J. Int. (2009) doi: 10.1111/j.1365-246X.2009.04178.x Upper-mantle low-velocity zone structure beneath the Kaapvaal craton from S-wave receiver functions Samantha E. Hansen,1 Andrew A. Nyblade,2 Jordi Julia,` 1 Paul H.G.M. Dirks3 and Raymond J. Durrheim3 1Department of Geosciences, 407 Deike Bldg., Pennsylvania State University, University Park, PA 16802, USA. E-mail: [email protected] 2Department of Geosciences, 447 Deike Bldg., Pennsylvania State University, University Park, PA 16802, USA 3School of Geosciences, University of the Witwatersrand, Private Bag X3, Wits 2050, South Africa Accepted 2009 March 10. Received 2009 February 9; in original form 2008 October 3 SUMMARY The southern African Plateau is marked by anomalously high elevations, reaching 1–2 km above sea level, and there is much debate as to whether this topography is compensated by a lower mantle source or by elevated temperatures in the upper mantle. In this study, we use S-wave receiver functions (SRFs) to estimate the lithospheric thickness and sublithospheric mantle velocity structure beneath the Kaapvaal craton, which forms the core of the Plateau. To fit the SRF data, a low-velocity zone (LVZ) is required below a ∼160-km-thick lithospheric lid, but the LVZ is no thicker than ∼90 km. Although the lid thickness obtained is thinner than that reported in previous SRF studies, neither the lid thickness nor the shear velocity decrease (∼4.5%) associated with the LVZ is anomalous compared to other cratonic environ- ments. Therefore, we conclude that elevated temperatures in the sublithospheric upper mantle contribute little support to the high elevations in this region of southern Africa.
    [Show full text]
  • MAPS CCP STACKS of P- & S-Wave RECEIVER
    LITHOSPHERIC STRUCTURE BENEATH FENNOSCANDIA BASED ON P- AND S-WAVE CONTACT ME: RECEIVER FUNCTIONS [email protected] Anna Makushkina 1, Benoit Tauzin 1,2, Meghan Miller 1, Hans Thybo 3,4,5, and Hrvoje Tkalčić 1 1 Australian National University; 2 University of Lyon, Laboratoire de Géologie de Lyon; 3 CEED, University of Oslo; 4 Eurasia Institute of Earth Sciences, Istanbul Technical University; 5 China University of Geosciences, Wuhan, China, INTRODUCTION Fennoscandia consists of geologically distinct domains of Archaean, RESULTS: MAPS Moho MLD HVZ early and late Proterozoic and Phanerozoic age at the surface. A little is known about the interrelation of these domains at depth. Moho depth obtained by picking (left) SRF CCP images (background color) and (right) PRF Map of the Mid-lithospheric discontinuity Depths of the high-velocity zone CCP images with Moho depth (background) measurements from EUNAseis [1] (diamonds) Controlled-source experiments show potential expression of suture zones extending down to 100 km depth. SRF PRF Regional studies show evidence for the mid-lithospheric (MLD), 8-degree discontinuity or the lithosphere– asthenosphere boundary (LAB), that are markers of continent formation and evolution. But each study samples a small portion of Sketch of the expected discontinuities. Fennoscandia and does not provide a Red color indicates discontinuity with increase of velocity with depth, blue – Topography map (m); white circles are stations used comprehensive model for the whole decrease. MLD – mid-lithospheric in this study system [e.g. 2,3,4]. discontinuity; HVZ – high velocity zone; Our goal is to image structural differences of the upper mantle in 3 geological domains LVZ – low velocity zone; LAB – create a unified model of Fennoscandia.
    [Show full text]
  • Inge Lehmann: Discoverer of the Earth's Inner Core 2/4/17, 524 PM
    Inge Lehmann: Discoverer of the Earth's Inner Core 2/4/17, 524 PM Log In | Register Select Language​▼ Search Keywords or Topics GO SHARE: (http://www.facebook.com/sharer.php?u=http://www.amnh.org/explore/resource-collections/earth-inside-and-out/inge-lehmann-discoverer-of- the-earth-s-inner-core) Explore(http://twitter.com/intent/tweet? Inge Lehmann: Discoverer of the Earth's Inner text=Inge%20Lehmann%3A%20Discoverer%20of%20the%20Earth%27s%20Inner%20Core&url=http://www.amnh.org/explore/resource- collections/earth-inside-and-out/inge-lehmann-discoverer-of-the-earth-s-inner-core)Science Topics Core Kids Guide to the How can we find out what’s happening deep inside the Earth? Collect Museum The temperatures are too hot, pressures too extreme, and distances too vast to be explored by conventional probes. So Resource Collections scientists rely on seismic waves—shock waves generated by earthquakes and explosions that travel through Earth and Biodiversity Crisis across its surface—to reveal the structure of the interior of the Cosmic Horizons planet. Thousands of earthquakes occur every year, and each Earth Inside and one provides a fleeting glimpse of the Earth’s interior. Seismic Out signals consist of several kinds of waves. Those important for understanding the Earth’s interior are P-waves, (primary, or A Conversation compressional waves), and S-waves (secondary, or shear with Jacques waves), which travel through solid and liquid material in Malavieille different ways. Forecasting Earthquakes Using Paleoseismology The seismograph, which detects and records the movement of Dr. Inge Lehmann (1888-1993), seismic waves, was invented in 1880.
    [Show full text]
  • Anisotropic Shear-Wave Velocity Structure of the Earth's Mantle
    JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 113, B06306, doi:10.1029/2007JB005169, 2008 Click Here for Full Article Anisotropic shear-wave velocity structure of the Earth’s mantle: A global model B. Kustowski,1,2 G. Ekstro¨m,3 and A. M. Dziewon´ski1 Received 12 May 2007; revised 8 February 2008; accepted 14 March 2008; published 25 June 2008. [1] We combine a new, large data set of surface wave phase anomalies, long-period waveforms, and body wave travel times to construct a three-dimensional model of the anisotropic shear wave velocity in the Earth’s mantle. Our modeling approach is improved and more comprehensive compared to our earlier studies and involves the development and implementation of a new spherically symmetric reference model, simultaneous inversion for velocity and anisotropy, as well as discontinuity topographies, and implementation of nonlinear crustal corrections for waveforms. A comparison of our new three-dimensional model, S362ANI, with two other models derived from comparable data sets but using different techniques reveals persistent features: (1) strong, 200-km-thick, high-velocity anomalies beneath cratons, likely representing the continental lithosphere, underlain by weaker, fast anomalies extending below 250 km, which may represent continental roots, (2) weak velocity heterogeneity between 250 and 400 km depths, (3) fast anomalies extending horizontally up to 2000–3000 km in the mantle transition zone beneath subduction zones, (4) lack of strong long-wavelength heterogeneity below 650 km suggesting inhibiting character of the upper mantle–lower mantle boundary, and (5) slow- velocity superplumes beneath the Pacific and Africa. The shear wave radial anisotropy is strongest at 120 km depth, in particular beneath the central Pacific.
    [Show full text]
  • Seismic and Electrical Signatures of the Lithosphere–Asthenosphere System of the Normal Oceanic Mantle
    EA45CH06-Kawakatsu ARI 14 August 2017 12:51 Annual Review of Earth and Planetary Sciences Seismic and Electrical Signatures of the Lithosphere–Asthenosphere System of the Normal Oceanic Mantle Hitoshi Kawakatsu and Hisashi Utada Earthquake Research Institute, The University of Tokyo, Tokyo 113-0032, Japan; email: [email protected] Annu. Rev. Earth Planet. Sci. 2017. 45:139–67 Keywords The Annual Review of Earth and Planetary Sciences is lithosphere, asthenosphere, Lid, low-velocity zone, G-discontinuity, plate online at earth.annualreviews.org tectonics, anisotropy, electrical conductivity https://doi.org/10.1146/annurev-earth-063016- 020319 Abstract Copyright c 2017 by Annual Reviews. Although plate tectonics started as a theory of the ocean basins nearly 50 years All rights reserved ago, the mechanical details of how it works are still poorly known. Our Annu. Rev. Earth Planet. Sci. 2017.45:139-167. Downloaded from www.annualreviews.org understanding of these details has been hampered partly by our inability to characterize the physical nature of the lithosphere–asthenosphere system ANNUAL (LAS) beneath the ocean. We review the existing observational constraints REVIEWS Further Click here to view this article's on the seismic and electrical properties of the LAS, particularly for normal Access provided by University of Tokyo - Library Earthquake Research Institute on 09/08/17. For personal use only. online features: oceanic regions away from mid-oceanic ridges, hot spots, and subduction • Download figures as PPT slides • Navigate linked references zones, where plate tectonics is expected to present its simplest form. Whereas • Download citations • Explore related articles a growing volume of seismic data on land has provided remarkable advances • Search keywords in large-scale pictures, seafloor observations have been shedding new light on essential details.
    [Show full text]
  • Earth's Internal Structure: a Seismologist's View
    Earth’s internal structure: a seismologist’s view Types of waves used by seismologists Organizing the information • Seismic travel times • Dispersion curves • Free oscillation frequencies Putting it all together Mantle 1-D seismic structure summary • Between 10-50 km have Mohorovicic discon;nuity – this marks the CRUST/ MANTLE boundary •At 50-200 km have a LOW VELOCITY ZONE – par;cularly under oceans and younger con;nents The crust Mohorovicic 1909 The lithosphere The asthenosphere Compositional interpretation of 1-D seismic profiles Seismic discontinuities and velocity gradients can arise from • A chemical change (e.g. the Moho) • A phase change (reorganisation of atoms into a different crystalline structure) The relative roles of phase changes and chemical changes provide a major challenge in interpreting seismology. Mantle 1-D seismic structure summary • Several seismological methods indicate a discon;nuity near 220 km depth. •Although present on PREM, it is now generally accepted not to be a global feature •Some;mes called the “Lehmann discon;nuity” aer Inge Lehmann NB: The 220-km Lehmann Discontinuity Not global in character! May reflect local anisotropy due to shearing of the asthenosphere i.e. a textural rather than chemical or phase change Mantle 1-D seismic structure summary • Between 410 and up to ~1000 km we are in the MANTLE TRANSITION ZONE • A number of sharp discon;nui;es separate regions of high velocity gradients •Main discon;nui;es are at 410 and 660 km. •660-discon;nuity widely taken as the UPPER MANTLE/LOWER MANTLE boundary The transition zone • Characterized by discontinuities in velocity and density models.
    [Show full text]
  • Mantle Flow and Melting Beneath Young Oceanic Lithosphere: Seismic
    MANTLE FLOW AND MELTING BENEATH YOUNG OCEANIC LITHOSPHERE: SEISMIC STUDIES OF THE GALÁPAGOS ARCHIPELAGO AND THE JUAN DE FUCA PLATE by JOSEPH STEPHEN BYRNES A DISSERTATION Presented to the Department of Earth Sciences and the Graduate School of the University of Oregon in partial fulfillment of the requirements for the degree of Doctor of Philosophy June 2017 DISSERTATION APPROVAL PAGE Student: Joseph Stephen Byrnes Title: Mantle Flow and Melting beneath Young Oceanic Lithosphere: Seismic Studies of the Galápagos Archipelago and the Juan de Fuca Plate This dissertation has been accepted and approved in partial fulfillment of the requirements for the Doctor of Philosophy degree in the Department of Earth Sciences by: Douglas Toomey Chairperson Emilie Hooft Core Member Eugene Humphreys Core Member Alan Rempel Core Member Allen Malony Institutional Representative and Scott L. Pratt Dean of the Graduate School Original approval signatures are on file with the University of Oregon Graduate School. Degree awarded June 2017 ii © 2017 Joseph Stephen Byrnes iii DISSERTATION ABSTRACT Joseph Stephen Byrnes Doctor of Philosophy Department of Earth Sciences June 2017 Title: Mantle Flow and Melting beneath Young Oceanic Lithosphere: Seismic Studies of the Galápagos Archipelago and the Juan de Fuca Plate In this dissertation, I use seismic imaging techniques to constrain the physical state of the upper mantle beneath regions of young oceanic lithosphere. Mantle convection is investigated beneath the Galápagos Archipelago and then beneath the Juan de Fuca (JdF) plate, with a focus on the JdF and Gorda Ridges before turning to the off-axis asthenosphere. In the Galápagos Archipelago, S-to-p receiver functions reveal a discontinuity in seismic velocity that is attributed to the dehydration of the upper mantle.
    [Show full text]
  • Kshamayaa Dharithri 1 (Oh Tolerant Mother Earth! Forgive Me)
    CHAPTER Kshamayaa Dharithri 1 (Oh Tolerant Mother Earth! Forgive Me) O’MY SILENT INNER VIBES (O’M S I V – 1) The mother Earth has greatest tolerance that she bears all our mistakes and misdeeds. She gives us everything such as minerals, food, shelter etc. But she can smash everything if we cross our limits. So,..... I bow to Mother Earth to save the mankind! I pray to mankind to save the mother Earth! Oh! Mother Earth... Forgive us and give us your blessings! Though ploughed through your belly, you fill our stomachs fully Though cared never gratefully, you fulfil our needs gracefully, I stand before Thee! Maa... with folded hands Forgive us and give us your blessings! Even when your body is split parts and parts, you never move apart Though made you victim of our party, But you never leave our party I kneel down! Maa... eyes filled with tears Forgive us and give us your blessings! Even if your heart’s ‘mine’ is broken, you give us gold and diamonds Even if garbage is thrown on you! You grab in your lap and garb us I lay down on thee! Maa... to prostrate with stretched hands Forgive us and give us your blessings! Despite being kicked always with our feet! Yet, you make us walk thousands and thousands of feet! Touching thy feet! Maa...I salute you with these words Forgive us and give us your blessings! Kshamayaa Dharithri! Rakshathu! Samrakshathu!! Parirakshathu!!! 1 2 Disaster Management: Hazard and Risk Awareness Namo Prithvee Matha! – Namo Prithvee Natha!! The God (Prithvee Nath) created PrithveePrithvee Matha, ‘The Earth’ as the most beautiful planet! No other planet has all the requisites for living-hood except the Earth.
    [Show full text]
  • Interior Parts of the Earth in Reference to Seismology
    INTERNAL STRUCTURE OF THE EARTH IN REFERENCE TO SEISMOLOGY SEISMILOGY • Disturbance within Earth's interior, which is in a constant state of movement, result in the release of energy in packets known as seismic waves. An area of geophysics known as seismology is the study of these waves and their effects, which often can be devastating when experienced in the form of earthquakes. The latter do not only take lives and destroy buildings, but they also produce secondary effects, most often in the form of a tsunami, or tidal wave. Using seismographs and seismometers, seismologists study earthquakes and other seismic phenomena, including volcanoes and even explosions resulting from nuclear testing. They measure earthquakes according to their magnitude or energy as well as their intensity or human impact. Seismology also is used to study Earth's interior, about which it has revealed a great deal. SEISMIC WAVES • When an earthquake occurs the seismic waves (P and S waves) spread out in all directions through the Earth's interior. Seismic stations located at increasing distances from the earthquake epicenter will record seismic waves that have traveled through increasing depths in the Earth. • Seismic velocities depend on the material properties such as composition, mineral phase and packing structure, temperature, and pressure of the media through which seismic waves pass. Seismic waves travel more quickly through denser materials and therefore generally travel more quickly with depth. Anomalously hot areas slow down seismic waves. Seismic waves move more slowly through a liquid than a solid. Molten areas within the Earth slow down P waves and stop S waves because their shearing motion cannot be transmitted through a liquid.
    [Show full text]
  • Oceanic Mantle Dynamics Implementation Plan: Report of a Community Workshop
    Oceanic Mantle Dynamics Implementation Plan: Report of a Community Workshop Snowbird, Utah September 18-20, 2002 Executive Summary and Workshop Recommendations The plate tectonics revolution in the earth sciences three decades ago provided a descriptive, or kinematic model for processes at the earth’s surface. The underlying mantle flow and dynamics behind this governing paradigm for the earth sciences have been far harder to elucidate. One of the greatest difficulties has been that seismic data, the primary imaging tool for the earth’s interior, have been collected primarily on the continents, while most of the earth’s interior lies beneath the sea floor. Recent advances in sea floor seismic instrumentation and geodynamic modeling, combined with constraints from other fields of geophysics and geochemistry, now provide unprecedented opportunities to understand the structure and circulation of the earth’s mantle. The advances require an integrated, interdisciplinary approach on a large scale, far beyond the planning and resources of individual investigators. Therefore a decade-long program in Oceanic Mantle Dynamics (OMD) is needed. This program will permit major advances in our understanding of every type of tectonic setting found in the ocean basins, will yield much higher resolution global imaging of the earth’s mantle, and in combination with continental USArray seismic data, will elucidate the great unanswered questions regarding the nature of the continent–ocean transition. A multidisciplinary approach centered around experiments made possible by a new generation of ocean-bottom seismometer (OBS) instrumentation could move beyond the kinematic revolution of plate tectonics towards testing and refining geodynamic models of mantle flow.
    [Show full text]