Variability of Western Indian Ocean Currents 83

Total Page:16

File Type:pdf, Size:1020Kb

Variability of Western Indian Ocean Currents 83 Western Indian Ocean J. Mar.VARIABILITY Sci. Vol. 1,OF No. WESTERN 1, pp. 81–90,INDIAN 2002 OCEAN CURRENTS 81 © 2002 WIOMSA VariabilityofWesternIndianOceanCurrents PeterN.Benny Department of Physical Oceanography, Cochin University of Science & Technology, Cochin, India –682016 E-mail: [email protected] Key words: western Indian Ocean, currents, circulation, Somali Current, dynamic topography, variability Abstract—In the study reported, an attempt was made to understand the intra-annual variability of the western Indian Ocean circulation by estimating the monthly dynamic topography with respect to 400db. The major currents in the western Indian Ocean are clearly depicted in the topography. Among the currents, the Somali Current exhibits strong annual variability. Eddy circulation is prominent in the northern part of the Somali Current during the southwest monsoon period. Seasonal variability is also noticed in the North Equatorial Current. Slight spatial and temporal changes are noticed in the South Equatorial Current and Equatorial Counter Current. The Equatorial Jet flow occurs in the monsoon transition periods of May and November between the equator and 3° South. INTRODUCTION Equatorial Current, which was directed towards the west during the northeast monsoon, reverses The western Indian Ocean receives special its directions towards the east. This combines with attention from oceanographers and meteorologists, the eastward-flowing Equatorial Counter Current as it exhibits more dramatic seasonal variation than and the whole eastward flow from 7 to 15 °N is the rest of the Indian Ocean and is an important called the monsoon current. One component of the region of air–sea interaction. Intense upwelling South Equatorial Current turns to north and occurs during the south-west monsoon season in supplies the Somali Current up the east coast of the Somali area (Bruce, 1974; Packard, 1985). As Africa. The Somali Current is notable for its high a result of this upwelling, cold surface water is speeds of up to 200 cm/s and has a transport of brought to the nearshore surface layers, which about 65 Sv, most of it in the upper 200 m (Pickard spreads over extensive areas of the Arabian Sea. and Emery, 1964). However, the current speed in Thus, the local climate and biological productivity western tropical Indian Ocean is of the order of 75 are much controlled by the oceanic processes. to 100 cm/s (Bahulayan et al., 1997). Tomczak and The existence of a strong surface current during Godfrey (1994) have given a detailed account of the southwest monsoon flow parallel to the African currents and circulation. Coast in the northwestern Indian Ocean, close Several authors (Bruce, 1966; 1968; 1974; inshore and towards the northeast has been long 1979; 1985; Leetmaa, 1972; 1982; Reverdin & known from the ship reports of Findlay (1866) and Fieux, 1987; Schott et al., 1990; Fischer et al., Hoffmann (1886). Based on collection of ship logs, 1996; Benny & Mizuno, 2000) have studied the Schott’s (1935) chart gives a clear picture of the western Indian Ocean currents. Modelling efforts Somali Current. were made by Cox (1970; 1979), Anderson et al. During the southwest monsoon, the North (1976), Luther & O’Brien (1985), Das et al. (1987), 82 P. N. BENNY Woodberry et al. (1989), Bhahulayen and Shaji possible to give an adequate description of annual (1996) and Shaji et al. (1997), to simulate the cycle of dynamic height. Hence, we tried to include western Indian Ocean circulation. Satellite the temperature/depth data also to estimate the observations of sea surface temperature, altimetery dynamic height employing the correlation between and scatterometer wind data have been used in heat content and dynamic height. studying the circulation and processes in the ∫z⌠ western Indian Ocean (Perigaud & Minister, 1988; The heat content (H)= 0 CpTdz Perigaud & Delecluse, 1989; 1992; 1993). where ⌠ is the density, Cp is the specific heat Considering the influence of the western Indian at constant pressure, T is the in situ temperature Ocean on the climate of the neighbouring region, and z is depth. efforts were made in the study reported here, to The correlation between the heat content and elucidate the intra-annual variability of the Ocean’s dynamic height with reference to 400 m was currents using available oceanographic information. determined using the hydrographic data. Significant correlation was obtained between DATASETSANDMETHODS dynamic height and heat content for the study region. The study was confined to the region between the The linear fit equation of correlation is eastern African coast and 60 °E, 20 °S and 15 °N. Historical data sets were used to produce the Y= – 0.251916 + 0.0751593 X dynamic topography with reference to 400db. The available hydrographic observations (BT, XBT, where Y is the dynamic height, X is the heat CTD and STD and Nansen casts) for the region content, correlation coefficient = 0.95 and standard from NODC (National Oceanographic Data deviation = 0.02. Centre, Washington, New York), INODC (Indian The temperature profiles aggregate to about National Oceanographic Data Centre, Goa) and 10,000 for the study region and only observations data collected by National Research Institute of extending to 400 m depths were considered for this Far Seas Fisheries, Japan were acquired and used study. Also, observations with no data for more for this analysis. than two consecutive standard depths (0, 10, 20, Ever since the existence of an intimate 30, 50, 75, 100, 125, 150, 200, 250, 300 and 400 relationship between the field of mass and field of m) were rejected. flow was established, dynamic topographies Thus, using the correlation dynamic height was (geopotential topographies) have been used to also estimated from the temperature/depth data and study the circulation of the oceans. the monthly dynamic topography maps were The anomaly of the dynamic depth (∆D) is prepared. Figure 1 shows the location of stations given by including temperature-salinity as well as the temperature profiles used for the estimation of ∆ =∫pδ dynamic height (steric height). DdP0 Where δ is the specific volume anomaly and P RESULTS is the pressure in decibars. The long-term mean monthly dynamic topography The first step involved is the use of in situ of the western Indian Ocean is presented in Figs temperature and salinity at observed depths to 2–13. compute the specific volume anomaly. For all integrations the depth in metres was taken to be January numerically equivalent to pressure in decibars. The temperature-salinity profiles number about The long term mean dynamic topography exhibits 3200 for the study region. Employing the strong gradient in steric height in the northern, temperature-salinity profiles alone, it is not southern and eastern parts of the study region VARIABILITY OF WESTERN INDIAN OCEAN CURRENTS 83 20 10 AFRICA 0 Latitude -10 -20 35 40 45 50 55 60 Longitude Fig. 1. Location of stations used for dynamic height estimation (Fig. 2). The equatorial zone shows dull circulation latitudes, up to 18 °S. The Equatorial Counter where the steric height is less than 1 dynamic Current is much stronger and is between 2 and 7 metre. Along the Somali Coast a weak southward °S. Thus, the dynamic topography depicts that the flow is noticed. The Equatorial Counter Current is whole western Indian Ocean is dynamically active weak and is around the equator. The northern part in this month. is marked with counter-rotating eddies between 10 and 15 °N. The strong flow of the South Equatorial March Current is between 5 and 15 °S. Part of the South Equatorial Current turns south at the Madagascar The steric height distribution in March (Fig. 4) Coast. An anticyclonic eddy circulation is evident shows slight increase in height, but the gradient is between Africa and Madagascar. weakened in the northern Indian Ocean compared to February. An offshore current displaces the February southward flow along the Somali Coast. The conspicuous feature noticed in this month is the Slight changes in dynamic height distribution are presence of the North Equatorial Current in visible in this month (Fig. 3). The steric height is between 0 and 5 °N. Counter-rotating eddies are increased at the equatorial zone, 5 °N – 5 °S. The present in the northern part. To the south, the South flow along the Somali Coast is towards south itself. Equatorial Current and the Equatorial Counter The eddy circulation is weaker at the northern part Current keeps the same structure as in February. than it is in January. To the south, the South Strong anticyclonic circulation is present between Equatorial Current is more extended into the higher Africa and Madagascar. 84 P. N. BENNY 15 15 0.75 0.90 0.95 1.00 0.90 1.00 10 10 1.00 0.95 5 5 1.00 0.95 1.20 1.00 0 0 0.95 1.20 Latitude Latitude 0.95 -5 -5 0.95 1.00 0.90 -10 -10 0.95 1.20 -15 1.20 -15 1.20 1.20 1.10 1.20 -20 -20 40 45 50 55 60 40 45 50 55 60 Longitude Longitude Fig. 2. Dynamic topography (January) Fig. 3. Dynamic topography (February) 15 15 0.95 0.90 1.00 0.95 1.00 1.05 1.00 10 10 1.00 1.05 1.05 5 5 1.10 1.05 1.05 0 1.00 0 1.00 1.05 Latitude -5 Latitude -5 0.95 0.95 0.90 0.90 1.00 0.90 -10 -10 1.10 1.15 1.10 1.15 -15 -15 1.10 1.20 1.10 1.00 0.90 1.20 -20 -20 40 45 50 55 60 40 45 50 55 60 Longitude Longitude Fig. 4. Dynamic topography (March) Fig.
Recommended publications
  • Fronts in the World Ocean's Large Marine Ecosystems. ICES CM 2007
    - 1 - This paper can be freely cited without prior reference to the authors International Council ICES CM 2007/D:21 for the Exploration Theme Session D: Comparative Marine Ecosystem of the Sea (ICES) Structure and Function: Descriptors and Characteristics Fronts in the World Ocean’s Large Marine Ecosystems Igor M. Belkin and Peter C. Cornillon Abstract. Oceanic fronts shape marine ecosystems; therefore front mapping and characterization is one of the most important aspects of physical oceanography. Here we report on the first effort to map and describe all major fronts in the World Ocean’s Large Marine Ecosystems (LMEs). Apart from a geographical review, these fronts are classified according to their origin and physical mechanisms that maintain them. This first-ever zero-order pattern of the LME fronts is based on a unique global frontal data base assembled at the University of Rhode Island. Thermal fronts were automatically derived from 12 years (1985-1996) of twice-daily satellite 9-km resolution global AVHRR SST fields with the Cayula-Cornillon front detection algorithm. These frontal maps serve as guidance in using hydrographic data to explore subsurface thermohaline fronts, whose surface thermal signatures have been mapped from space. Our most recent study of chlorophyll fronts in the Northwest Atlantic from high-resolution 1-km data (Belkin and O’Reilly, 2007) revealed a close spatial association between chlorophyll fronts and SST fronts, suggesting causative links between these two types of fronts. Keywords: Fronts; Large Marine Ecosystems; World Ocean; sea surface temperature. Igor M. Belkin: Graduate School of Oceanography, University of Rhode Island, 215 South Ferry Road, Narragansett, Rhode Island 02882, USA [tel.: +1 401 874 6533, fax: +1 874 6728, email: [email protected]].
    [Show full text]
  • Observations of the North Equatorial Current, Mindanao Current, and Kuroshio Current System During the 2006/ 07 El Niño and 2007/08 La Niña
    Journal of Oceanography, Vol. 65, pp. 325 to 333, 2009 Observations of the North Equatorial Current, Mindanao Current, and Kuroshio Current System during the 2006/ 07 El Niño and 2007/08 La Niña 1 2 3 4 YUJI KASHINO *, NORIEVILL ESPAÑA , FADLI SYAMSUDIN , KELVIN J. RICHARDS , 4† 5 1 TOMMY JENSEN , PIERRE DUTRIEUX and AKIO ISHIDA 1Institute of Observational Research for Global Change, Japan Agency for Marine Earth Science and Technology, Natsushima, Yokosuka 237-0061, Japan 2The Marine Science Institute, University of the Philippines, Quezon 1101, Philippines 3Badan Pengkajian Dan Penerapan Teknologi, Jakarta 10340, Indonesia 4International Pacific Research Center, University of Hawaii, Honolulu, HI 96822, U.S.A. 5Department of Oceanography, University of Hawaii, Honolulu, HI 96822, U.S.A. (Received 19 September 2008; in revised form 17 December 2008; accepted 17 December 2008) Two onboard observation campaigns were carried out in the western boundary re- Keywords: gion of the Philippine Sea in December 2006 and January 2008 during the 2006/07 El ⋅ North Equatorial Niño and the 2007/08 La Niña to observe the North Equatorial Current (NEC), Current, ⋅ Mindanao Current (MC), and Kuroshio current system. The NEC and MC measured Mindanao Current, ⋅ in late 2006 under El Niño conditions were stronger than those measured during early Kuroshio, ⋅ 2006/07 El Niño, 2008 under La Niña conditions. The opposite was true for the current speed of the ⋅ 2007/08 La Niña. Kuroshio, which was stronger in early 2008 than in late 2006. The increase in dy- namic height around 8°N, 130°E from December 2006 to January 2008 resulted in a weakening of the NEC and MC.
    [Show full text]
  • Somali Fisheries
    www.securefisheries.org SECURING SOMALI FISHERIES Sarah M. Glaser Paige M. Roberts Robert H. Mazurek Kaija J. Hurlburt Liza Kane-Hartnett Securing Somali Fisheries | i SECURING SOMALI FISHERIES Sarah M. Glaser Paige M. Roberts Robert H. Mazurek Kaija J. Hurlburt Liza Kane-Hartnett Contributors: Ashley Wilson, Timothy Davies, and Robert Arthur (MRAG, London) Graphics: Timothy Schommer and Andrea Jovanovic Please send comments and questions to: Sarah M. Glaser, PhD Research Associate, Secure Fisheries One Earth Future Foundation +1 720 214 4425 [email protected] Please cite this document as: Glaser SM, Roberts PM, Mazurek RH, Hurlburt KJ, and Kane-Hartnett L (2015) Securing Somali Fisheries. Denver, CO: One Earth Future Foundation. DOI: 10.18289/OEF.2015.001 Secure Fisheries is a program of the One Earth Future Foundation Cover Photo: Shakila Sadik Hashim at Alla Aamin fishing company in Berbera, Jean-Pierre Larroque. ii | Securing Somali Fisheries TABLE OF CONTENTS LIST OF FIGURES, TABLES, BOXES ............................................................................................. iii FOUNDER’S LETTER .................................................................................................................... v ACKNOWLEDGEMENTS ............................................................................................................. vi DEDICATION ............................................................................................................................ vii EXECUTIVE SUMMARY (Somali) ............................................................................................
    [Show full text]
  • The Equatorial Current System
    The Equatorial Current System C. Chen General Physical Oceanography MAR 555 School for Marine Sciences and Technology Umass-Dartmouth 1 Two subtropic gyres: Anticyclonic gyre in the northern subtropic region; Cyclonic gyre in the southern subtropic region Continuous components of these two gyres: • The North Equatorial Current (NEC) flowing westward around 20o N; • The South Equatorial Current (SEC) flowing westward around 0o to 5o S • Between these two equatorial currents is the Equatorial Counter Current (ECC) flowing eastward around 10o N. 2 Westerly wind zone 30o convergence o 20 N Equatorial Current EN Trade 10o divergence Equatorial Counter Current convergence o -10 S. Equatorial Current ES Trade divergence -20o convergence -30o Westerly wind zone 3 N.E.C N.E.C.C S.E.C 0 50 Mixed layer 100 150 Thermoclines 200 25oN 20o 15o 10o 5o 0 5o 10o 15o 20o 25oS 4 Equatorial Undercurrent Sea level East West Wind stress Rest sea level Mixed layer lines Thermoc • At equator, f =0, the current follows the wind direction, and the wind drives the water to move westward; • The water accumulates against the western boundary and cause the sea level rises over there; • The surface pressure gradient pushes the water eastward and cancels the wind-driven westward currents in the mixed layer. 5 Wind-induced Current Pressure-driven Current Equatorial Undercurrent Mixed layer Thermoclines 6 Observational Evidence 7 Urbano et al. (2008), JGR-Ocean, 113, C04041, doi: 10.1029/2007/JC004215 8 Observed Seasonal Variability of the EUC (Urbano et al. 2008) 9 Equatorial Undercurrent in the Pacific Ocean Isotherms in an equatorial plane in the Pacific Ocean (from Philander, 1980) In the Pacific Ocean, it is called “the Cormwell Current}; In the Atlantic Ocean, it is called “the Lomonosov Current” 10 Kessler, W, Progress in Oceanography, 69 (2006) 11 In the equatorial Pacific, when the South-East Trade relaxes or turns to the east, the sea surface slope will “collapse”, causing a flat mixed layer and thermocline.
    [Show full text]
  • EBSA Template 1 Costa Rica Dome-En
    Appendix Template for Submission of Scientific Information to Describe Ecologically or Biologically Significant Marine Areas Note: Please DO NOT embed tables, graphs, figures, photos, or other artwork within the text manuscript, but please send these as separate files. Captions for figures should be included at the end of the text file, however . Title/Name of the area: Costa Rica Dome Presented by (names, affiliations, title, contact details) Abstract (in less than 150 words) The Costa Rica Dome is an area of high primary productivity in the northeastern tropical Pacific, which supports marine predators such as tuna, dolphins, and cetaceans. The endangered leatherback turtle (Dermochelys coriacea ), which nests on the beaches of Costa Rica, migrates through the area. The Costa Rica Dome provides year-round habitat that is important for the survival and recovery of the endangered blue whale (Balaenoptera musculus ). The area is of special importance to the life history of a population of the blue whales, which migrate south from Baja California during the winter for breeding, calving, raising calves and feeding. Introduction (To include: feature type(s) presented, geographic description, depth range, oceanography, general information data reported, availability of models) Biological hot spots in the ocean are often created by physical processes and have distinct oceanographic signatures. Marine predators, including large pelagic fish, marine mammals, seabirds, and fishing vessels, recognize that prey organisms congregate at ocean fronts, eddies, and other physical features (Palacios et al, 2006). One such hot spot occurs in the northeastern tropical Pacific at the Costa Rica Dome. The Costa Rica Dome was first observed in 1948 (Wyrtki, 1964) and first described by Cromwell (1958).
    [Show full text]
  • Structure and Transport of the East African Coastal Current
    See discussions, stats, and author profiles for this publication at: https://www.researchgate.net/publication/248793481 Structure and transport of the East African Coastal Current Article in Journal of Geophysical Research Atmospheres · January 1991 DOI: 10.1029/91JC01942 CITATIONS READS 48 209 3 authors, including: Michele Fieux Pierre and Marie Curie University - Paris 6 56 PUBLICATIONS 1,894 CITATIONS SEE PROFILE Some of the authors of this publication are also working on these related projects: It is in a book: " L'océan à découvert " , 321 p. , sept 2017, CNRS Editions View project All content following this page was uploaded by Michele Fieux on 09 June 2018. The user has requested enhancement of the downloaded file. JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 96, NO. C12, PAGES 22,245-22,257, DECEMBER 15, 1991 Structure and Transport of the East African Coastal Current JOHN C. SWALLOW Drakewalls, Gunnislake, Cornwall, England FRIEDRICH SCHOTT lnstitut fiir Meereskunde an der Universitiit Kiel, Kiel, Germany MICH•,LE FIEUX Laboratoire d'Oc•anographie Dynamique et de Climatologie, Universit• Paris VI, Paris The East African Coastal Current (EACC) runs northward throughout the year between latitudes 11øSand 3øS, with surfacespeeds exceeding 1 m s-1 in northernsummer. Mean transport from five sectionsnear 4ø-5øS is 19.9Sv (1 Sv -- 106 m3 s-1) northwardin theupper 500 dbar, out to 120km offshore. Below that, between 500 and 1000 dbar, there appears to be a weak variable transport of the order of 1 Sv. Comparing transports in the EACC with those in the boundary current north of Madagascar, it seems that most of the water in the upper 300 dbar of the northern branch of the South Equatorial Current goes into the EACC.
    [Show full text]
  • Poleward Shift of the Pacific North Equatorial Current Bifurcation
    RESEARCH ARTICLE Poleward Shift of the Pacific North Equatorial 10.1029/2019JC015019 Current Bifurcation Key Points: Haihong Guo1,2 , Zhaohui Chen1,2 , and Haiyuan Yang1,2 • In the North Pacific, the North Equatorial Current bifurcation in 1Physical Oceanography Laboratory/Institute for Advanced Ocean Study, Ocean University of China, Qingdao, China, the upper ocean shifts poleward 2 with increasing depth Pilot National Laboratory for Marine Science and Technology (Qingdao), Qingdao, China • The poleward shift of the bifurcation is associated with the asymmetric wind stress curl input to Abstract The dynamics of the poleward shift of the Pacific North Equatorial Current bifurcation latitude tropical/subtropical gyre ‐ • (NBL) is studied using a 5.5 layer reduced gravity model. It is found that the poleward shift of the NBL is The equatorial currents bifurcations fi in other basins share the same associated with the asymmetric intensity of the wind stress curl input to the Paci c tropical and subtropical vertical structure gyres. Stronger wind stress curl in the subtropical gyre leads to equatorward transport in the interior upper ocean across the boundary between the two gyres, causing a poleward transport compensation at the western boundary. In the lower layer ocean, in turn, there is poleward (equatorward) transport at the Correspondence to: interior (western boundary) due to Sverdrup balance which requires zero transport at the gyre boundary Z. Chen, where zonally integrated wind stress curl is zero. Therefore, the NBL exhibits a titling feature, with its [email protected] position being more equatorward in the upper layer and more poleward in the lower layer.
    [Show full text]
  • Future Changes to the Upper Ocean Western Boundary Currents Across Two Generations of Climate Models Alex Sen Gupta1,2,3*, Annette Stellema1,2,3, Gabriel M
    www.nature.com/scientificreports OPEN Future changes to the upper ocean Western Boundary Currents across two generations of climate models Alex Sen Gupta1,2,3*, Annette Stellema1,2,3, Gabriel M. Pontes4, Andréa S. Taschetto1,2, Adriana Vergés3,5 & Vincent Rossi6 Western Boundary Currents (WBCs) are important for the oceanic transport of heat, dissolved gases and nutrients. They can afect regional climate and strongly infuence the dispersion and distribution of marine species. Using state-of-the-art climate models from the latest and previous Climate Model Intercomparison Projects, we evaluate upper ocean circulation and examine future projections, focusing on subtropical and low-latitude WBCs. Despite their coarse resolution, climate models successfully reproduce most large-scale circulation features with ensemble mean transports typically within the range of observational uncertainty, although there is often a large spread across the models and some currents are systematically too strong or weak. Despite considerable diferences in model structure, resolution and parameterisations, many currents show highly consistent projected changes across the models. For example, the East Australian Current, Brazil Current and Agulhas Current extensions are projected to intensify, while the Gulf Stream, Indonesian Throughfow and Agulhas Current are projected to weaken. Intermodel diferences in most future circulation changes can be explained in part by projected changes in the large-scale surface winds. In moving to the latest model generation, despite structural model advancements, we fnd little systematic improvement in the simulation of ocean transports nor major diferences in the projected changes. Anthropogenic climate change manifests as increases in surface temperature and sea level, rainfall distribution changes and increasing frequency and intensity of certain extreme events1.
    [Show full text]
  • Physical Oceanography - UNAM, Mexico Lecture 3: the Wind-Driven Oceanic Circulation
    Physical Oceanography - UNAM, Mexico Lecture 3: The Wind-Driven Oceanic Circulation Robin Waldman October 17th 2018 A first taste... Many large-scale circulation features are wind-forced ! Outline The Ekman currents and Sverdrup balance The western intensification of gyres The Southern Ocean circulation The Tropical circulation Outline The Ekman currents and Sverdrup balance The western intensification of gyres The Southern Ocean circulation The Tropical circulation Ekman currents Introduction : I First quantitative theory relating the winds and ocean circulation. I Can be deduced by applying a dimensional analysis to the horizontal momentum equations within the surface layer. The resulting balance is geostrophic plus Ekman : I geostrophic : Coriolis and pressure force I Ekman : Coriolis and vertical turbulent momentum fluxes modelled as diffusivities. Ekman currents Ekman’s hypotheses : I The ocean is infinitely large and wide, so that interactions with topography can be neglected ; ¶uh I It has reached a steady state, so that the Eulerian derivative ¶t = 0 ; I It is homogeneous horizontally, so that (uh:r)uh = 0, ¶uh rh:(khurh)uh = 0 and by continuity w = 0 hence w ¶z = 0 ; I Its density is constant, which has the same consequence as the Boussinesq hypotheses for the horizontal momentum equations ; I The vertical eddy diffusivity kzu is constant. ¶ 2u f k × u = k E E zu ¶z2 that is : k ¶ 2v u = zu E E f ¶z2 k ¶ 2u v = − zu E E f ¶z2 Ekman currents Ekman balance : k ¶ 2v u = zu E E f ¶z2 k ¶ 2u v = − zu E E f ¶z2 Ekman currents Ekman balance : ¶ 2u f k × u = k E E zu ¶z2 that is : Ekman currents Ekman balance : ¶ 2u f k × u = k E E zu ¶z2 that is : k ¶ 2v u = zu E E f ¶z2 k ¶ 2u v = − zu E E f ¶z2 ¶uh τ = r0kzu ¶z 0 with τ the surface wind stress.
    [Show full text]
  • Lecture 4: OCEANS (Outline)
    LectureLecture 44 :: OCEANSOCEANS (Outline)(Outline) Basic Structures and Dynamics Ekman transport Geostrophic currents Surface Ocean Circulation Subtropicl gyre Boundary current Deep Ocean Circulation Thermohaline conveyor belt ESS200A Prof. Jin -Yi Yu BasicBasic OceanOcean StructuresStructures Warm up by sunlight! Upper Ocean (~100 m) Shallow, warm upper layer where light is abundant and where most marine life can be found. Deep Ocean Cold, dark, deep ocean where plenty supplies of nutrients and carbon exist. ESS200A No sunlight! Prof. Jin -Yi Yu BasicBasic OceanOcean CurrentCurrent SystemsSystems Upper Ocean surface circulation Deep Ocean deep ocean circulation ESS200A (from “Is The Temperature Rising?”) Prof. Jin -Yi Yu TheThe StateState ofof OceansOceans Temperature warm on the upper ocean, cold in the deeper ocean. Salinity variations determined by evaporation, precipitation, sea-ice formation and melt, and river runoff. Density small in the upper ocean, large in the deeper ocean. ESS200A Prof. Jin -Yi Yu PotentialPotential TemperatureTemperature Potential temperature is very close to temperature in the ocean. The average temperature of the world ocean is about 3.6°C. ESS200A (from Global Physical Climatology ) Prof. Jin -Yi Yu SalinitySalinity E < P Sea-ice formation and melting E > P Salinity is the mass of dissolved salts in a kilogram of seawater. Unit: ‰ (part per thousand; per mil). The average salinity of the world ocean is 34.7‰. Four major factors that affect salinity: evaporation, precipitation, inflow of river water, and sea-ice formation and melting. (from Global Physical Climatology ) ESS200A Prof. Jin -Yi Yu Low density due to absorption of solar energy near the surface. DensityDensity Seawater is almost incompressible, so the density of seawater is always very close to 1000 kg/m 3.
    [Show full text]
  • Global Ocean Surface Velocities from Drifters: Mean, Variance, El Nino–Southern~ Oscillation Response, and Seasonal Cycle Rick Lumpkin1 and Gregory C
    JOURNAL OF GEOPHYSICAL RESEARCH: OCEANS, VOL. 118, 2992–3006, doi:10.1002/jgrc.20210, 2013 Global ocean surface velocities from drifters: Mean, variance, El Nino–Southern~ Oscillation response, and seasonal cycle Rick Lumpkin1 and Gregory C. Johnson2 Received 24 September 2012; revised 18 April 2013; accepted 19 April 2013; published 14 June 2013. [1] Global near-surface currents are calculated from satellite-tracked drogued drifter velocities on a 0.5 Â 0.5 latitude-longitude grid using a new methodology. Data used at each grid point lie within a centered bin of set area with a shape defined by the variance ellipse of current fluctuations within that bin. The time-mean current, its annual harmonic, semiannual harmonic, correlation with the Southern Oscillation Index (SOI), spatial gradients, and residuals are estimated along with formal error bars for each component. The time-mean field resolves the major surface current systems of the world. The magnitude of the variance reveals enhanced eddy kinetic energy in the western boundary current systems, in equatorial regions, and along the Antarctic Circumpolar Current, as well as three large ‘‘eddy deserts,’’ two in the Pacific and one in the Atlantic. The SOI component is largest in the western and central tropical Pacific, but can also be seen in the Indian Ocean. Seasonal variations reveal details such as the gyre-scale shifts in the convergence centers of the subtropical gyres, and the seasonal evolution of tropical currents and eddies in the western tropical Pacific Ocean. The results of this study are available as a monthly climatology. Citation: Lumpkin, R., and G.
    [Show full text]
  • Atlantic Ocean Equatorial Currents
    188 ATLANTIC OCEAN EQUATORIAL CURRENTS ATLANTIC OCEAN EQUATORIAL CURRENTS S. G. Philander, Princeton University, Princeton, Centered on the equator, and below the westward NJ, USA surface Sow, is an intense eastward jet known as the Equatorial Undercurrent which amounts to a Copyright ^ 2001 Academic Press narrow ribbon that precisely marks the location of doi:10.1006/rwos.2001.0361 the equator. The undercurrent attains speeds on the order of 1 m s\1 has a half-width of approximately Introduction 100 km; its core, in the thermocline, is at a depth of approximately 100 m in the west, and shoals to- The circulations of the tropical Atlantic and PaciRc wards the east. The current exists because the west- Oceans have much in common because similar trade ward trade winds, in addition to driving divergent winds, with similar seasonal Suctuations, prevail westward surface Sow (upwelling is most intense at over both oceans. The salient features of these circu- the equator), also maintain an eastward pressure lations are alternating bands of eastward- and west- force by piling up the warm surface waters in the ward-Sowing currents in the surface layers (see western side of the ocean basin. That pressure force Figure 1). Fluctuations of the currents in the two is associated with equatorward Sow in the thermo- oceans have similarities not only on seasonal but cline because of the Coriolis force. At the equator, even on interannual timescales; the Atlantic has where the Coriolis force vanishes, the pressure force a phenomenon that is the counterpart of El Ninoin is the source of momentum for the eastward Equa- the PaciRc.
    [Show full text]