Introductory Oceanography (OCNG 251) Study Guide: Part 1

Total Page:16

File Type:pdf, Size:1020Kb

Introductory Oceanography (OCNG 251) Study Guide: Part 1 Introductory Oceanography (OCNG 251) Study Guide: Part 1 This half session dealt with the construction of all conditions responsible for the observed global circulation patterns in the World Ocean. In a sense, we started the course from the very end, trying to build an ocean and understanding its physical structure (the water part in this case). The objective of the entire session is to understand the concept behind Figure 1 below: Figure 1: General circulation pattern of the ocean. Surface currents are indicated in red while deep currents are presented in blue. In Figure 1, one can see that there is a link between surface circulation (red) and deep circulation (blue). Of course, to conserve mass, there must be a link between these wo circulation patterns. Areas of “deep water formation” will transfer water from the surface to the deep ocean whereas water returns to the surface via zones of upwelling. Transfer from the surface to the deep ocean will occur due to densification (increased density) of surface water (mostly through cooling but also through some increased salinity during ice formation and salt concentration in seawater). Upwelling will occur through physical transfer from current formation (Ekman circulation in eastern ocean basins) and as water is pushed up continental slope (like when the North Atlantic Deep Water is pushed up the slope of the Antarctic continent). These features are all shown in Figure 1 with areas of deep water formation as purple dots (North and South Atlantic), and areas of upwelling with blue‐to‐red arrows (eastern regions of ocean basins). Also note that surface currents are characterized by circular patterns, called gyres, in each oceanic basin for each hemisphere (Atlantic and Pacific each have 2 gyres, whereas the Indian has only 1). The entire purpose of the first session was thus to bring all the elements necessary to comprehend the processes responsible for the ocean circulation illustrated in Figure 1. These elements are: OCNG 251 (Dr. P. Louchouarn) – Study Guide #1 2 ‐ Systems and cycles. Specifically, how mass and energy cycle through different section of a system (from the micro‐ to macro‐scales). In this section we emphasized notions of reservoir, flux, source/sink, residence time, steady state, as well as positive and negative feedback mechanisms. ‐ Physical properties of water and, in particular, how temperature and salinity affect the density of seawater. We also focused on heat capacity to explain the temperature changes different media experience (i.e. atmosphere vs. ocean, continents, vs. oceans, etc) when subjected to a gain or loss of heat. ‐ Heat budget of the earth, particularly with respect to the unbalance in incoming short wave radiations and outgoing long wave radiations that is observed in inter‐tropical vs. high latitude zones. ‐ Atmospheric circulation, as it is driven by that same unbalance in the earth heat budget and affected by the earth’s rotation ( Coriolis). The interplay of these processes then leads to global as well as seasonal wind patterns (e.g. easterlies/westerlies and monsoons, respectively). ‐ Surface ocean circulation, driven itself by the wind drag of constant winds and affected by coriolis, vorticity, and geostrophic forces. Except for the effect of local winds, the general surface ocean circulation follows the atmospheric High/Low distribution pattern with circular motion (gyres) in each ocean basin. The circulation is clockwise in the north hemisphere, and counterclockwise in the south hemisphere. ‐ Deep ocean circulation, driven by density formation in high latitude zones. Surface water can undergo large increases in density due to an interplay of salinity and temperature changes. When warm water cools, its density increases markedly. Similarly, when water increases in salinity, its density increases as well. The cooling of surface seawater in northern latitudes (e.g. sub‐Arctic seas and around Antartica) leads to an increase in its density and thus vertical transfer of water towards the deep ocean. Similarly, during sea ice formation, the expulsion of salts from the forming ice results in brine formation (increase in salinity in sea waters) and thus an increase in the water density. These processes lead to deep water‐mass formation, each with specific density conditions that help or prevent their mixing in the deep ocean. ‐ Global ocean circulation. The surface and deep ocean circulations are tied at both “ends” where surface water cools (at high latitudes) to form deep waters, and where deep waters are upwelled towards to surface (mostly on eastern boundaries of oceans) to reintegrate the surface circulation loops and eventually reach the cooling sites for another cycle. On average, a full ocean circulation cycle takes several hundred years to complete (~500 yrs) but this “mixing speed” is variable and can accelerate or decelerate depending on the rate of deep water formation (cooling, salinity changes) and upwelling (wind strength, atmospheric pressure oscillation). ‐ Earth climate balance. The relationship between atmospheric and ocean circulation, help redistribute heat from zones of surplus radiation (inter‐tropical zones) to zones of deficit (high latitudes). In low latitudes, the majority of the heat transfer occurs through ocean circulation, whereas atmospheric circulation is responsible for most of the heat transfer in mid‐ to high latitudes. Event such as hurricanes are rapid and natural “pressure valve” processes that transfer large amounts of heat from the inter‐tropical zones to mid‐latitude regions. OCNG 251 (Dr. P. Louchouarn) – Study Guide #1 3 1) Systems and cycles Some Definitions Transport and transformation processes within definite reservoirs: Carbon, Rock, Water Cycles Reservoir: (box, compartment: M in mass units or moles) An amount of material defined by certain physical, chemical, or biological characteristics that can be considered homogeneous: O2 in the atmosphere; carbon in living organic matter in the Ocean; ocean water in surface water masses. Flux: (F) The amount of material transferred from one reservoir to another per unit time (per unit area): The rate of evaporation of water from the surface ocean; the rate of deposition of inorganic carbon (carbonates in marine sediments); the rate of contaminant input to a lake or a bay Source: (Q) A flux of material into a reservoir Sink: (S) A flux of material out of a reservoir Budget: A balance sheet of all sources and sinks of a reservoir. If sources and sinks balance each other and do not change with time, the reservoir is in steady‐state (M does not change with time). If steady‐state prevails, then a flux that is unknown can be estimated by its difference from the other fluxes Turnover time: The ratio of the content (M) of the reservoir to the sum of its sinks (S) or sources (Q). The time it will take to empty the reservoir if there aren’t any sources. It is also a measure of the average time an atom/molecule spends in the reservoir. Cycle: A system consisting of two or more connected reservoir, where a large part of the material is transferred through the system in a cyclic fashion Feedback: All closed and open systems respond to inputs and have outputs. A feedback is a specific output that serves as an input to the system. Negative Feedback (stabilizing): The system’s response is in the opposite direction as that of the output. An example given in class is the increased reflection of solar radiation (albedo) from upper level clouds. Increased heat evaporation clouds increased albedo lowered incoming radiation decreased overall heat. Positive Feedback (destabilizing): The system’s response is in the same direction as that of the output. An example given in class is the increased trapping of infrared radiation from lower level clouds. Increased heat evaporation clouds increased I.R. trapping increased overall heat. We also sent some time on the concept of residence time (a concept we will be using also in the second section of this course to explain the salt composition of seawater and biogeochemical cycles). Residence Time is a high probability that a certain fraction of a substance (atoms or molecules) forming the reservoir (M) will be of a certain age (mean age of the element when it leaves the reservoir). The residence time of water in the atmosphere is very short (~10‐20 days). The residence time of water in the Oceans is much longer (~4000 years). However, the residence time in different components of the atmosphere and oceans, and therefore the time of exchange between these different reservoirs, vary widely. OCNG 251 (Dr. P. Louchouarn) – Study Guide #1 4 Figure 2: Time exchange for exchange of air and water between the atmosphere and ocean. Advantages of Cycle Approach • Provides overview of fluxes, reservoir contents, and turnover time • Gives a basis for quantitative modeling • Helps to estimate the relative magnitudes of natural and anthropogenic fluxes • Stimulates questions such as: Where is the material coming from?, where is it going next? • Helps identify gaps in knowledge Disadvantages of Cycle Approach • Analysis, by necessity, superficial. Little or no insight into what goes inside the reservoir (“black box”) • Gives false impression of certainty. Often, at least one of the fluxes is derived from balance considerations (may be erroneous!) • Analysis based on average quantities that cannot always be easily measured because of spatial and temporal variations, as well as other factors. 2) Physical properties of water Water molecule: Dipole Uneven charge Hydrogen bonds! (DNA anyone?) Higher energy requirement for change of state (solid to liquid, liquid to gaseous) than similar molecules. Make sure you can explain the figure below: Figure 3: Melting and boiling temperatures for water and a series of molecules with similar chemical composition. OCNG 251 (Dr. P. Louchouarn) – Study Guide #1 5 The structure of the water molecule thus leads to very high energy requirements for changes of state (Latent Heat), in particular for changes between liquid to gaseous state.
Recommended publications
  • Preliminary Catalog of the Sedimentary Basins of the United States
    Preliminary Catalog of the Sedimentary Basins of the United States By James L. Coleman, Jr., and Steven M. Cahan Open-File Report 2012–1111 U.S. Department of the Interior U.S. Geological Survey U.S. Department of the Interior KEN SALAZAR, Secretary U.S. Geological Survey Marcia K. McNutt, Director U.S. Geological Survey, Reston, Virginia: 2012 For more information on the USGS—the Federal source for science about the Earth, its natural and living resources, natural hazards, and the environment, visit http://www.usgs.gov or call 1–888–ASK–USGS. For an overview of USGS information products, including maps, imagery, and publications, visit http://www.usgs.gov/pubprod To order this and other USGS information products, visit http://store.usgs.gov Any use of trade, firm, or product names is for descriptive purposes only and does not imply endorsement by the U.S. Government. Although this information product, for the most part, is in the public domain, it also may contain copyrighted materials as noted in the text. Permission to reproduce copyrighted items must be secured from the copyright owner. Suggested citation: Coleman, J.L., Jr., and Cahan, S.M., 2012, Preliminary catalog of the sedimentary basins of the United States: U.S. Geological Survey Open-File Report 2012–1111, 27 p. (plus 4 figures and 1 table available as separate files) Available online at http://pubs.usgs.gov/of/2012/1111/. iii Contents Abstract ...........................................................................................................................................................1
    [Show full text]
  • Bottom Water and Bottom Configuration of the Great Atlantic Deeps. (1) (2)
    bOTTOM WATER AND bOTTOM CONFIGURATION OF THE GREAT ATLANTIC DEEPS. (1) (2). (Extract from the Results of the German Atlantic Expedition) by G e o r g WUST. The problem of the origin and distribution of bottom water has been discussed from early times, and often. This results from the fact that more abundant materials of observation exist for the bottom than for the deep layers, because measurements of bottom temperature have been taken not only by exploring vessels, but also by hydro- graphic and cable-laying ships. The remarkably low temperatures of nearly o° C. on the bottom, which were confirmed on each occasion, also early served as the principal foun­ dation of the hypothesis of the polar origin of the bottom water. The polar bottom currents are consequently members of the deep oceanic circulation, the existence of which had been deduced from the distribution of the temperature before the Challenger expedi­ tion. If it had been thought before that time that the Arctic and Antarctic currents showed roughly the same development and met at the equator, it became clear, after the Challenger and Gazelle observations, that the principal mass of the bottom waters of the great oceans comes from the Antarctic Basin ; that in the Atlantic Ocean this bottom current chiefly leads into the western trough ; and that it can still be detected in the form of a cold stream as far as the equator (in its last ramifications it even passes the equator and reaches the North Atlantic). These expeditions have also shown the value of bottom temperatures for revealing the first magnitude shapes of the ocean bottom, a value which has been proved for the Atlantic Ocean by two examples which have become classic.
    [Show full text]
  • Kinematics and Extent of the Piemont-Liguria Basin
    https://doi.org/10.5194/se-2020-161 Preprint. Discussion started: 8 October 2020 c Author(s) 2020. CC BY 4.0 License. Kinematics and extent of the Piemont-Liguria Basin – implications for subduction processes in the Alps Eline Le Breton1, Sascha Brune2,3, Kamil Ustaszewski4, Sabin Zahirovic5, Maria Seton5, R. Dietmar Müller5 5 1Department of Earth Sciences, Freie Universität Berlin, Germany 2Geodynamic Modelling Section, German Research Centre for Geosciences, GFZ Potsdam, Germany 3Institute of Geosciences, University of Potsdam, Potsdam, Germany 4Institute for Geological Sciences, Friedrich-Schiller-Universität Jena, Germany 10 5EarthByte Group, School of Geosciences, The University of Sydney, NSW 2006, Australia Correspondence to: Eline Le Breton ([email protected]) Abstract. Assessing the size of a former ocean, of which only remnants are found in mountain belts, is challenging but crucial to understand subduction and exhumation processes. Here we present new constraints on the opening and width of the Piemont- Liguria (PL) Ocean, known as the Alpine Tethys together with the Valais Basin. We use a regional tectonic reconstruction of 15 the Western Mediterranean-Alpine area, implemented into a global plate motion model with lithospheric deformation, and 2D thermo-mechanical modelling of the rifting phase to test our kinematic reconstructions for geodynamic consistency. Our model fits well with independent datasets (i.e. ages of syn-rift sediments, rift-related fault activity and mafic rocks) and shows that the PL Basin opened in four stages: (1) Rifting of the proximal continental margin in Early Jurassic (200-180 Ma), (2) Hyper- extension of the distal margin in Early-Middle Jurassic (180-165 Ma), (3) Ocean-Continent Transition (OCT) formation with 20 mantle exhumation and MORB-type magmatism in Middle-Late Jurassic (165-154 Ma), (4) Break-up and “mature” oceanic spreading mostly in Late Jurassic (154-145 Ma).
    [Show full text]
  • UNIVERSITY of CALIFORNIA, SAN DIEGO Marine Geophysical Study
    UNIVERSITY OF CALIFORNIA, SAN DIEGO Marine Geophysical Study of Cyclic Sedimentation and Shallow Sill Intrusion in the Floor of the Central Gulf of California A dissertation submitted in partial satisfaction of the requirements for the degree Doctor of Philosophy in Oceanography by Jared W. Kluesner Committee in Charge: Professor Peter Lonsdale, Chair Professor Paterno Castillo Professor Graham Kent Professor Falko Kuester Professor Michael Tryon Professor Edward Winterer 2011 Copyright Jared Kluesner, 2011 All rights reserved. The Dissertation of Jared W. Kluesner is approved, and it is acceptable in quality and in form for publication on microfilm and electronically: Chair University of California, San Diego 2011 iii To my parents, Tony and Donna Kluesner and my grandfather James Kluesner iv "...Let us go, we said, into the Sea of Cortez, realizing that we become forever a part of it" The Log from the Sea of Cortez John Steinbeck v TABLE OF CONTENTS Signature Page ...................................................................................... iii Dedication.............................................................................................. iv Epigraph ................................................................................................ v Table of Contents .................................................................................. vi List of Figures ........................................................................................ ix Acknowledgments ................................................................................
    [Show full text]
  • The 18.6Year Lunar Nodal Cycle and Surface Temperature Variability In
    JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 112, C02002, doi:10.1029/2006JC003671, 2007 The 18.6-year lunar nodal cycle and surface temperature variability in the northeast Pacific Stewart M. McKinnell1 and William R. Crawford2 Received 27 April 2006; revised 24 August 2006; accepted 21 September 2006; published 2 February 2007. [1] The 18.6-year lunar nodal cycle (LNC) is a significant feature of winter (January) air and sea temperatures along the North American west coast over a 400-year period. Yet much of the recent temperature variation can also be explained by wind patterns associated with the PNA teleconnection. At Sitka, Alaska, (57°N) and nearby stations in northern British Columbia, the January PNA index accounts for over 70% of average January air temperatures in lengthy meteorological records. It appears that the LNC signal in January air temperatures in this region is not independent of the PNA, but is a component of it. The Sitka air temperature record, along with SSTs along the British Columbia coast and the PNA index have significant cross-correlations with the LNC that appear at a 2-year lag, LNC leading. The influence of the PNA pattern declines in winter with decreasing latitude but the LNC component does not. It appears as a significant feature of long-term SST variation at Scripps Pier and the California Current System. The LNC also appears over centennial-scales in proxy temperatures along western North America. The linkage of LNC-moderated surface temperatures to processes involving basin-scale teleconnections expands the possibility that the proximate mechanism may be located remotely from its expression in the northeast Pacific.
    [Show full text]
  • OCEAN SUBDUCTION Show That Hardly Any Commercial Enhancement Finney B, Gregory-Eaves I, Sweetman J, Douglas MSV Program Can Be Regarded As Clearly Successful
    1982 OCEAN SUBDUCTION show that hardly any commercial enhancement Finney B, Gregory-Eaves I, Sweetman J, Douglas MSV program can be regarded as clearly successful. and Smol JP (2000) Impacts of climatic change and Model simulations suggest, however, that stock- Rshing on PaciRc salmon over the past 300 years. enhancement may be possible if releases can be Science 290: 795}799. made that match closely the current ecological Giske J and Salvanes AGV (1999) A model for enhance- and environmental conditions. However, this ment potentials in open ecosystems. In: Howell BR, Moksness E and Svasand T (eds) Stock Enhancement requires improvements of assessment methods of and Sea Ranching. Blackwell Fishing, News Books. these factors beyond present knowledge. Marine Howell BR, Moksness E and Svasand T (1999) Stock systems tend to have strong nonlinear dynamics, Enhancement and Sea Ranching. Blackwell Fishing, and unless one is able to predict these dynamics News Books. over a relevant time horizon, release efforts are Kareiva P, Marvier M and McClure M (2000) Recovery not likely to increase the abundance of the target and management options for spring/summer chinnook population. salmon in the Columbia River basin. Science 290: 977}979. Mills D (1989) Ecology and Management of Atlantic See also Salmon. London: Chapman & Hall. Ricker WE (1981) Changes in the average size and Mariculture, Environmental, Economic and Social average age of PaciRc salmon. Canadian Journal of Impacts of. Salmonid Farming. Salmon Fisheries: Fisheries and Aquatic Science 38: 1636}1656. Atlantic; Paci\c. Salmonids. Salvanes AGV, Aksnes DL, FossaJH and Giske J (1995) Simulated carrying capacities of Rsh in Norwegian Further Reading fjords.
    [Show full text]
  • Glacial Isostatic Adjustment and Sea-Level Change – State of the Art Report Technical Report TR-09-11
    Glacial isostatic adjustment and sea-level change – State of the art report Glacial isostatic adjustment and sea-level change Technical Report TR-09-11 Glacial isostatic adjustment and sea-level change State of the art report Pippa Whitehouse, Durham University April 2009 Svensk Kärnbränslehantering AB Swedish Nuclear Fuel and Waste Management Co Box 250, SE-101 24 Stockholm Phone +46 8 459 84 00 TR-09-11 ISSN 1404-0344 CM Gruppen AB, Bromma, 2009 Tänd ett lager: P, R eller TR. Glacial isostatic adjustment and sea-level change State of the art report Pippa Whitehouse, Durham University April 2009 This report concerns a study which was conducted for SKB. The conclusions and viewpoints presented in the report are those of the author and do not necessarily coincide with those of the client. A pdf version of this document can be downloaded from www.skb.se. Preface This document contains information on the process of glacial isostatic adjustment (GIA) and how this affects sea-level and shore-line displacement, and the methods which are employed by researchers to study and understand these processes. The information will be used in e.g. the report “Climate and climate-related issues for the safety assessment SR-Site”. Stockholm, April 2009 Jens-Ove Näslund Person in charge of the SKB climate programme Contents 1 Introduction 7 1.1 Structure and purpose of this report 7 1.2 A brief introduction to GIA 7 1.2.1 Overview/general description 7 1.2.2 Governing factors 8 1.2.3 Observations of glacial isostatic adjustment 9 1.2.4 Time scales 9 2 Glacial
    [Show full text]
  • The Subduction Initiation Stage of the Wilson Cycle
    Downloaded from http://sp.lyellcollection.org/ by guest on February 20, 2018 The subduction initiation stage of the Wilson cycle ROBERT HALL SE Asia Research Group, Department of Earth Sciences, Royal Holloway University of London, Egham, Surrey, TW20 0EX, UK [email protected] R.H., 0000-0003-1693-6914 Abstract: In the Wilson cycle, there is a change from an opening to a closing ocean when subduction begins. Subduction initiation is commonly identified as a major problem in plate tectonics and is said to be nowhere observable, yet there are many young subduction zones at the west Pacific margins and in eastern Indonesia. Few studies have considered these examples. Banda subduction developed by the eastwards propagation of the Java trench into an oceanic embayment by tearing along a former ocean–continent boundary. The earlier subducted slab provided the driving force to drag down unsubducted oceanic lithosphere. Although this process may be common, it does not account for young subduction zones near Sulawesi at different stages of develop- ment. Subduction began there at the edges of ocean basins, not at former spreading centres or transforms. It initiated at a point where there were major differences in elevation between the ocean floor and the adjacent hot, weak and thickened arc/continental crust. The age of the ocean crust appears to be unimportant. A close relationship with extension is marked by the dramatic elevation of land, the exhumation of deep crust and the spectacular subsidence of basins, raising questions about the time required to move from no subduction to active subduction, and how initiation can be identified in the geological record.
    [Show full text]
  • Geosciences 528 Sedimentary Basin Analysis
    Geosciences 528 Sedimentary Basin Analysis Spring, 2011 G528 – Sedimentary Basins • Prof. M.S. Hendrix – Office SC359 – Office Phone: 243-5278 – Cell Phone: 544-0780 – [email protected] • Textbook = Principles of Sedimentary Basin Analysis - Andrew Miall • Lab 320 • Syllabus Introduction to sedimentary basin analysis What is a sedimentary basin? • thick accumulation (>2-3 km) of sediment • physical setting allowing for sed accumulation e.g. Mississippi Delta up to 18 km of sediment accumulated • significant element of vertical tectonics which cause formation of sed basins, uplift of sed source areas, and reorganization of sediment dispersal systems • Study of history of sedimentary basins and processes that influence nature of basin fill Vertical tectonics caused primarily by: • plate tectonic setting and proximity of basin to plate margin • type of nearest plate boundary(s • nature of basement rock • nature of sedimentary rock Requires working or expert knowledge on wide variety of geologic subdisciplines • sedimentology (basis of interpretation of depositional systems • depositional systems analysis • paleocurrent analysis • provenance analysis • floral/ faunal analysis • geochronology • crustal scale tectonic processes, geophysical methods • thermochronology (Ar/Ar, apatite F-T, etc.) • special techniques - organic geochemical analysis - paleosol analysis - tree ring analysis • involves both surface and subsurface data • involves large changes in scale and may involve long temporal histories Location/ exposure quality Stratigraphic measurements, sedimentology, paleoflow data Clast Composition Analysis Paleogeographic/ paleoenvironmental interpretation Regional tectonic picture Basin models: 1) a norm, for purposes of comparison 2) a framework and guide for future observation 3) a predictor 4) an integrated basis for interpretation of the class of basins it represents Francis Bacon: ‘Truth emerges more readily from error than from confusion.’ S.J.
    [Show full text]
  • Insights from the Permian–Triassic
    RESEARCH Can eustatic charts go beyond first order? Insights from the Permian–Triassic B. Guillaume1, S. Pochat2, J. Monteux2,3, L. Husson4, and G. Choblet2 1UMR CNRS 6118, GÉOSCIENCES RENNES, OBSERVATOIRE DES SCIENCES DE L’UNIVERS DE RENNES (OSUR), UNIVERSITÉ DE RENNES 1, 35042 RENNES CEDEX, FRANCE 2LABORATOIRE DE PLANÉTOLOGIE ET GÉODYNAMIQUE, UNIVERSITÉ DE NANTES–CENTRE NATIONAL DE LA RECHERCHE SCIENTIFIQUE (CNRS), UMR-6112, 2, RUE DE LA HOUSSINIÈRE, 44322 NANTES CEDEX 03, FRANCE 3LABORATOIRE MAGMAS ET VOLCANS, UMR 6524, 6 AVENUE BLAISE PASCAL, 63178 AUBIÈRE CEDEX, FRANCE 4ISTERRE, CENTRE NATIONAL DE LA RECHERCHE SCIENTIFIQUE (CNRS), UNIVERSITÉ GRENOBLE ALPES, 38000 GRENOBLE, FRANCE ABSTRACT First-order variations of eustatic charts (200–400 m.y.) are in agreement with our understanding of the geodynamic processes that control sea level. By extrapolation, second-order (10–100 m.y.) and third-order (1–10 m.y.) variations are also thought to follow the same rules. However, this assumption may be jeopardized by a closer examination of the Permian–Triassic example, for which climatic and tectonic eustasy fails to explain the variations of the eustatic charts. During this period, eustatic charts peak down to their lowermost Phanerozoic values and display second-order variations at rates of up to 3 m/m.y., which is inconsistent with the expected eustatic signal during the early fragmentation of the Pangean supercontinent and the late Paleozoic melting of ice sheets. Here, we review the possible mechanisms that could explain the apparent sea-level variations. Some of them do modify the eustatic sea level (ESL). In particular, dynamic deflections of Earth’s surface above subduction zones and their locations with respect to continents appear to have been the primary controls of absolute sea level as the Pangean supercontinent formed and broke up.
    [Show full text]
  • The Ocean Biosphere: from Microbes to Mammals
    Keywords: biosphere, bioaccumulate, biodiversity, food web, ecology, abiotic factors, and biotic factors. Lesson II: The Ocean Biosphere: From Microbes to Mammals Planet Earth is truly a water environments is called ecology. planet! We have a connection to all Living things such as plants and living things in the ocean, from the animals in the environment are called microscopic floating plants that biotic factors, or biota. Nonliving supply us with the oxygen we breathe, things in the environment, such as to the huge blue whale that fills its soil, water, temperature, light, belly with a ton of krill. This circle of salinity, chemical composition, and life is called a biosphere. The earth’s currents are abiotic factors. biosphere is composed of all living Together, these factors interact and things, from the deepest oceans to the function as an ecosystem. An upper atmosphere. It includes all the ecosystem is a community of different air, land and water where life exists. organisms interacting with the abiotic All living things depend upon and parts of its environment. Ecosystems interact with each other and with the may be as small as a beehive, or as non-living things in their large as the Atlantic Ocean. With the environment. aid of technology, we are discovering The study of interactions entire new ecosystems that survive in between organisms and their our biosphere. Our Ocean Biosphere Look at an atlas of the world animals. A few abiotic factors are and identify one of the major oceans temperature, salinity, pressure, found on planet earth. In short, the dissolved gases and depth.
    [Show full text]
  • Transition from Continental Rifting to Oceanic Spreading in the Northern Red Sea Area Sami El Khrepy1,2, Ivan Koulakov3,4,5*, Taras Gerya6, Nassir Al‑Arif1, Mamdouh S
    www.nature.com/scientificreports OPEN Transition from continental rifting to oceanic spreading in the northern Red Sea area Sami El Khrepy1,2, Ivan Koulakov3,4,5*, Taras Gerya6, Nassir Al‑Arif1, Mamdouh S. Alajmi7 & Ayman N. Qadrouh7 Lithosphere extension, which plays an essential role in plate tectonics, occurs both in continents (as rift systems) and oceans (spreading along mid‑oceanic ridges). The northern Red Sea area is a unique natural geodynamic laboratory, where the ongoing transition from continental rifting to oceanic spreading can be observed. Here, we analyze travel time data from a merged catalogue provided by the Egyptian and Saudi Arabian seismic networks to build a three‑dimensional model of seismic velocities in the crust and uppermost mantle beneath the northern Red Sea and surroundings. The derived structures clearly reveal a high‑velocity anomaly coinciding with the Red Sea basin and a narrow low‑velocity anomaly centered along the rift axis. We interpret these structures as a transition of lithospheric extension from continental rifting to oceanic spreading. The transitional lithosphere is manifested by a dominantly positive seismic anomaly indicating the presence of a 50–70‑km‑thick and 200–300‑km‑wide cold lithosphere. Along the forming oceanic ridge axis, an elongated low‑velocity anomaly marks a narrow localized nascent spreading zone that disrupts the transitional lithosphere. Along the eastern margins of the Red Sea, several low‑velocity anomalies may represent crustal zone of massive Cenozoic basaltic magmatism. Te transition from continental rifing to oceanic spreading is a crucial yet partly enigmatic stage that determines the birth and further evolution of an oceanic basin.
    [Show full text]