Ocean Circulation
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Chapter 10. Thermohaline Circulation
Chapter 10. Thermohaline Circulation Main References: Schloesser, F., R. Furue, J. P. McCreary, and A. Timmermann, 2012: Dynamics of the Atlantic meridional overturning circulation. Part 1: Buoyancy-forced response. Progress in Oceanography, 101, 33-62. F. Schloesser, R. Furue, J. P. McCreary, A. Timmermann, 2014: Dynamics of the Atlantic meridional overturning circulation. Part 2: forcing by winds and buoyancy. Progress in Oceanography, 120, 154-176. Other references: Bryan, F., 1987. On the parameter sensitivity of primitive equation ocean general circulation models. Journal of Physical Oceanography 17, 970–985. Kawase, M., 1987. Establishment of deep ocean circulation driven by deep water production. Journal of Physical Oceanography 17, 2294–2317. Stommel, H., Arons, A.B., 1960. On the abyssal circulation of the world ocean—I Stationary planetary flow pattern on a sphere. Deep-Sea Research 6, 140–154. Toggweiler, J.R., Samuels, B., 1995. Effect of Drake Passage on the global thermohaline circulation. Deep-Sea Research 42, 477–500. Vallis, G.K., 2000. Large-scale circulation and production of stratification: effects of wind, geometry and diffusion. Journal of Physical Oceanography 30, 933–954. 10.1 The Thermohaline Circulation (THC): Concept, Structure and Climatic Effect 10.1.1 Concept and structure The Thermohaline Circulation (THC) is a global-scale ocean circulation driven by the equator-to-pole surface density differences of seawater. The equator-to-pole density contrast, in turn, is controlled by temperature (thermal) and salinity (haline) variations. In the Atlantic Ocean where North Atlantic Deep Water (NADW) forms, the THC is often referred to as the Atlantic Meridional Overturning Circulation (AMOC). -
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. -
Lesson 8: Currents
Standards Addressed National Science Lesson 8: Currents Education Standards, Grades 9-12 Unifying concepts and Overview processes Physical science Lesson 8 presents the mechanisms that drive surface and deep ocean currents. The process of global ocean Ocean Literacy circulation is presented, emphasizing the importance of Principles this process for climate regulation. In the activity, students The Earth has one big play a game focused on the primary surface current names ocean with many and locations. features Lesson Objectives DCPS, High School Earth Science Students will: ES.4.8. Explain special 1. Define currents and thermohaline circulation properties of water (e.g., high specific and latent heats) and the influence of large bodies 2. Explain what factors drive deep ocean and surface of water and the water cycle currents on heat transport and therefore weather and 3. Identify the primary ocean currents climate ES.1.4. Recognize the use and limitations of models and Lesson Contents theories as scientific representations of reality ES.6.8 Explain the dynamics 1. Teaching Lesson 8 of oceanic currents, including a. Introduction upwelling, density, and deep b. Lecture Notes water currents, the local c. Additional Resources Labrador Current and the Gulf Stream, and their relationship to global 2. Extra Activity Questions circulation within the marine environment and climate 3. Student Handout 4. Mock Bowl Quiz 1 | P a g e Teaching Lesson 8 Lesson 8 Lesson Outline1 I. Introduction Ask students to describe how they think ocean currents work. They might define ocean currents or discuss the drivers of currents (wind and density gradients). Then, ask them to list all the reasons they can think of that currents might be important to humans and organisms that live in the ocean. -
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. -
Ocean Circulation and Climate: an Overview
ocean-climate.org Bertrand Delorme Ocean Circulation and Yassir Eddebbar and Climate: an Overview Ocean circulation plays a central role in regulating climate and supporting marine life by transporting heat, carbon, oxygen, and nutrients throughout the world’s ocean. As human-emitted greenhouse gases continue to accumulate in the atmosphere, the Meridional Overturning Circulation (MOC) plays an increasingly important role in sequestering anthropogenic heat and carbon into the deep ocean, thus modulating the course of climate change. Anthropogenic warming, in turn, can influence global ocean circulation through enhancing ocean stratification by warming and freshening the high latitude upper oceans, rendering it an integral part in understanding and predicting climate over the 21st century. The interactions between the MOC and climate are poorly understood and underscore the need for enhanced observations, improved process understanding, and proper model representation of ocean circulation on several spatial and temporal scales. The ocean is in perpetual motion. Through its DRIVING MECHANISMS transport of heat, carbon, plankton, nutrients, and oxygen around the world, ocean circulation regulates Global ocean circulation can be divided into global climate and maintains primary productivity and two major components: i) the fast, wind-driven, marine ecosystems, with widespread implications upper ocean circulation, and ii) the slow, deep for global fisheries, tourism, and the shipping ocean circulation. These two components act industry. Surface and subsurface currents, upwelling, simultaneously to drive the MOC, the movement of downwelling, surface and internal waves, mixing, seawater across basins and depths. eddies, convection, and several other forms of motion act jointly to shape the observed circulation As the name suggests, the wind-driven circulation is of the world’s ocean. -
What Is the Thermohaline Circulation?
S CIENCE’ S C OMPASS PERSPECTIVES 65 flow thus appear to be driven by thermal 64 PERSPECTIVES: OCEANOGRAPHY and evaporative forcing from the atmo- 63 sphere. The ocean seems to act like a heat 62 engine, in analogy to the atmosphere. 61 What Is the Some authors apparently think of this 60 convective mode of motion as the thermo- 59 haline circulation. But results of the past 58 Thermohaline Circulation? few years suggest that such a convectively 57 Carl Wunsch driven mass flux is impossible. There are 56 several lines of argument. The first goes 55 he discussion of today’s climate and mass affect the movements of all other back to Sandström (4), who pointed out that 54 its past and potential future changes properties, such as heat, salt, oxygen, car- when a fluid is heated and cooled at the 53 Tis often framed in the context of the bon, and so forth (1, 2), all of which differ same pressure (or heated at a lower pres- 52 ocean’s thermohaline circulation. Wide- from each other. For example, the North sure), no significant work can be extracted 51 spread consequences are ascribed to its Atlantic imports heat, but exports oxygen. from the flow, with the region below the 50 shutdown and acceleration—a deus ex It seems most sensible to regard the ther- cold source becoming homogeneous. 49 machina for climate change. mohaline circulation –8 –2 The ocean is both 48 But what is meant by this term? In in- as the circulation of 0 heated and cooled ef- 500 47 terdisciplinary fields such as climate temperature and salt. -
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). -
The Role of Thermohaline Circulation in Global Climate Change
The Role of Thermohaline Circulation in Global Climate Change • by Arnold Gordon ©&prinlfrom lAmonl-Doherl] Ceologicoi Observatory 1990 & /99/ &PorI Lamont-Doherty Geological Observatory of Columbia University Palisades, NY 10964 (914)359-2900 The Role of • The world ocean consists of 1.3 billion cu km of salty water, and covers 70.8% of the Earth's suiface. This enormous body of Thermohaline water exerts a poweiful influence on Earth's climate; indeed, it is an integral part of the global climate system. Therefore, under Circulation in standing the climate system requires a knowledge of how the ocean and the atmosphere exchange heat, water and greenhouse gases. If Global Climate we are to be able to gain a capability for predicting our changing climate we must learn, for example, how pools of warm salty Change water move about the ocean, what governs the growth and decay of sea ice, and how rapidly the deep ocean's interior responds to the changes in the atmosphere. The ocean plays a considerable features for the most part only role in the rate of greenhouse move heat and water on horizon warming. It does this in two tal planes. It is the slower ther ways: it absorbs excess green mohaline circulation, driven by house gases from the atmos buoyancy forcing at the sea sur phere, such as carbon dioxide, face (i.e., exchanges of heat and methane and chlorofluoro fresh water between ocean and methane, and it also absorbs atmosphere change the density • some of the greenhouse-induced or buoyancy of the surface water; by Arnold L. -
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. -
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. -
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. -
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.