Atlantic Climate Variability and Predictability: a CLIVAR Perspective
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
The Mean Flow Field of the Tropical Atlantic Ocean
Deep-Sea Research II 46 (1999) 279—303 The mean flow field of the tropical Atlantic Ocean Lothar Stramma*, Friedrich Schott Institut fu( r Meereskunde, an der Universita( t Kiel, Du( sternbrooker Weg 20, 24105 Kiel, Germany Received 26 August 1997; received in revised form 31 July 1998 Abstract The mean horizontal flow field of the tropical Atlantic Ocean is described between 20°N and 20°S from observations and literature results for three layers of the upper ocean, Tropical Surface Water, Central Water, and Antarctic Intermediate Water. Compared to the subtropical gyres the tropical circulation shows several zonal current and countercurrent bands of smaller meridional and vertical extent. The wind-driven Ekman layer in the upper tens of meters of the ocean masks at some places the flow structure of the Tropical Surface Water layer as is the case for the Angola Gyre in the eastern tropical South Atlantic. Although there are regions with a strong seasonal cycle of the Tropical Surface Water circulation, such as the North Equatorial Countercurrent, large regions of the tropics do not show a significant seasonal cycle. In the Central Water layer below, the eastward North and South Equatorial undercurrents appear imbedded in the westward-flowing South Equatorial Current. The Antarcic Intermediate Water layer contains several zonal current bands south of 3°N, but only weak flow exists north of 3°N. The sparse available data suggest that the Equatorial Intermediate Current as well as the Southern and Northern Intermediate Countercurrents extend zonally across the entire equatorial basin. Due to the convergence of northern and southern water masses, the western tropical Atlantic north of the equator is an important site for the mixture of water masses, but more work is needed to better understand the role of the various zonal under- and countercur- rents in cross-equatorial water mass transfer. -
Spontaneous Abrupt Climate Change Due to an Atmospheric Blocking–Sea-Ice–Ocean Feedback in an Unforced Climate Model Simulation
Spontaneous abrupt climate change due to an atmospheric blocking–sea-ice–ocean feedback in an unforced climate model simulation Sybren Drijfhouta,b,1, Emily Gleesonc, Henk A. Dijkstrad, and Valerie Livinae aDepartment of Climate Research, Royal Netherlands Meteorological Institute, 3730AE, De Bilt, The Netherlands; bSchool of Ocean and Earth Sciences, National Oceanography Centre, Southampton SO14 3TB, United Kingdom; cResearch, Environment and Applications Division, Met Éireann, Dublin 9, Ireland; dInstitute for Marine and Atmospheric Research Utrecht, Utrecht University, 3584 CC Utrecht, The Netherlands; and eNational Physical Laboratory, Teddington TW11 0LW, United Kingdom Edited by Mark H. Thiemens, University of California at San Diego, La Jolla, CA, and approved October 18, 2013 (received for review March 15, 2013) Abrupt climate change is abundant in geological records, but the warm, salty layer is inaccessible to the atmosphere when the climate models rarely have been able to simulate such events in surface halocline is present. As a result, subsurface warming response to realistic forcing. Here we report on a spontaneous takes place below the surface halocline, which eventually desta- abrupt cooling event, lasting for more than a century, with bilizes the water column and erodes the surface halocline. a temperature anomaly similar to that of the Little Ice Age. The The link between multiple sea-ice states and AMOC was also event was simulated in the preindustrial control run of a high- investigated within an idealized coupled climate model (9). The resolution climate model, without imposing external perturba- sea-ice switch featured abrupt transitions between a weak and tions. Initial cooling started with a period of enhanced atmo- strong AMOC, essentially showing that these two mechanisms spheric blocking over the eastern subpolar gyre. -
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]]. -
The Evolution and Demise of North Brazil Current Rings*
VOLUME 36 JOURNAL OF PHYSICAL OCEANOGRAPHY JULY 2006 The Evolution and Demise of North Brazil Current Rings* DAVID M. FRATANTONI Department of Physical Oceanography, Woods Hole Oceanographic Institution, Woods Hole, Massachusetts PHILIP L. RICHARDSON Department of Physical Oceanography, Woods Hole Oceeanographic Institution, and Associated Scientists at Woods Hole, Woods Hole, Massachusetts (Manuscript received 27 May 2004, in final form 26 October 2005) ABSTRACT Subsurface float and surface drifter observations illustrate the structure, evolution, and eventual demise of 10 North Brazil Current (NBC) rings as they approached and collided with the Lesser Antilles in the western tropical Atlantic Ocean. Upon encountering the shoaling topography east of the Lesser Antilles, most of the rings were deflected abruptly northward and several were observed to completely engulf the island of Barbados. The near-surface and subthermocline layers of two rings were observed to cleave or separate upon encountering shoaling bathymetry between Tobago and Barbados, with the resulting por- tions each retaining an independent and coherent ringlike vortical circulation. Surface drifters and shallow (250 m) subsurface floats that looped within NBC rings were more likely to enter the Caribbean through the passages of the Lesser Antilles than were deeper (500 or 900 m) floats, indicating that the regional bathymetry preferentially inhibits transport of intermediate-depth ring components. No evidence was found for the wholesale passage of rings through the island chain. 1. Introduction ration from the NBC, anticyclonic rings with azimuthal speeds approaching 100 cm sϪ1 move northwestward a. Background toward the Caribbean Sea on a course parallel to the The North Brazil Current (NBC) is an intense west- South American coastline (Johns et al. -
Annual Cycle and Variability of the North Brazil Current
JANUARY 1998 JOHNS ET AL. 103 Annual Cycle and Variability of the North Brazil Current W. E. J OHNS AND T. N . L EE Rosenstiel School of Marine and Atmospheric Science, University of Miami, Miami, Florida R. C. BEARDSLEY,J.CANDELA, AND R. LIMEBURNER Woods Hole Oceanographic Institution, Woods Hole, Massachusetts B. CASTRO Instituto Oceanogra®co Universidade SaÄo Paulo, SaÄo Paulo, Brazil (Manuscript received 18 October 1996, in ®nal form 5 June 1997) ABSTRACT Current meter observations from an array of three subsurface moorings located on the Brazil continental slope near 48N are used to describe the annual cycle and low-frequency variability of the North Brazil Current (NBC). The moored array was deployed from September 1989 to January 1991, with further extension of the shallowest mooring, located over the 500-m isobath near the axis of the NBC, through September 1991. Moored current measurements were also obtained over the adjacent shelf for a limited time between February and May 1990. The NBC has a large annual cycle at this latitude, ranging from a maximum transport of 36 Sv (Sv [ 106 m3 s21) in July±August to a minimum of 13 Sv in April±May, with an annual mean transport of approximately 26 Sv. The mean transport is dominated by ¯ow in the upper 150 m, and the seasonal cycle is contained almost entirely in the top 300 m. Transport over the continental shelf is 3±5 Sv and appears to be fairly constant throughout the year, based on the available current meter records and shipboard ADCP surveys. The NBC transport cycle is in good agreement with linear wind-driven models and appears to be in near-equilibrium with remote wind stress curl forcing across the tropical Atlantic for much of the year. -
Ocean Circulation and Climate: a 21St Century Perspective
Chapter 13 Western Boundary Currents Shiro Imawaki*, Amy S. Bower{, Lisa Beal{ and Bo Qiu} *Japan Agency for Marine–Earth Science and Technology, Yokohama, Japan {Woods Hole Oceanographic Institution, Woods Hole, Massachusetts, USA {Rosenstiel School of Marine and Atmospheric Science, University of Miami, Miami, Florida, USA }School of Ocean and Earth Science and Technology, University of Hawaii, Honolulu, Hawaii, USA Chapter Outline 1. General Features 305 4.1.3. Velocity and Transport 317 1.1. Introduction 305 4.1.4. Separation from the Western Boundary 317 1.2. Wind-Driven and Thermohaline Circulations 306 4.1.5. WBC Extension 319 1.3. Transport 306 4.1.6. Air–Sea Interaction and Implications 1.4. Variability 306 for Climate 319 1.5. Structure of WBCs 306 4.2. Agulhas Current 320 1.6. Air–Sea Fluxes 308 4.2.1. Introduction 320 1.7. Observations 309 4.2.2. Origins and Source Waters 320 1.8. WBCs of Individual Ocean Basins 309 4.2.3. Velocity and Vorticity Structure 320 2. North Atlantic 309 4.2.4. Separation, Retroflection, and Leakage 322 2.1. Introduction 309 4.2.5. WBC Extension 322 2.2. Florida Current 310 4.2.6. Air–Sea Interaction 323 2.3. Gulf Stream Separation 311 4.2.7. Implications for Climate 323 2.4. Gulf Stream Extension 311 5. North Pacific 323 2.5. Air–Sea Interaction 313 5.1. Upstream Kuroshio 323 2.6. North Atlantic Current 314 5.2. Kuroshio South of Japan 325 3. South Atlantic 315 5.3. Kuroshio Extension 325 3.1. -
Sea Changes Ashore: the Ocean and Iceland's Herring Capital
University of New Hampshire University of New Hampshire Scholars' Repository Sociology Scholarship Sociology 12-2004 Sea changes ashore: The ocean and iceland's herring capital. Lawrence C. Hamilton University of New Hampshire, [email protected] Steingrimur Jonsson University of Akureyri Helga Ogmundardottir University of Uppsala Igor M. Belkin University of Rhode Island Follow this and additional works at: https://scholars.unh.edu/soc_facpub Part of the Sociology Commons Recommended Citation Hamilton, L.C., Jónsson, S., Ögmundardóttir, H., Belkin, I.M. Sea changes ashore: The ocean and iceland's herring capital. (2004) Arctic, 57 (4), pp. 325-335. This Article is brought to you for free and open access by the Sociology at University of New Hampshire Scholars' Repository. It has been accepted for inclusion in Sociology Scholarship by an authorized administrator of University of New Hampshire Scholars' Repository. For more information, please contact [email protected]. ARCTIC VOL. 57, NO. 4 (DECEMBER 2004) P. 325– 335 Sea Changes Ashore: The Ocean and Iceland’s Herring Capital LAWRENCE C. HAMILTON,1 STEINGRÍMUR JÓNSSON,2 HELGA ÖGMUNDARDÓTTIR3 and IGOR M. BELKIN4 (Received 16 May 2003; accepted in revised form 6 February 2004) ABSTRACT. The story of Siglufjör›ur (Siglufjordur), a north Iceland village that became the “Herring Capital of the World,” provides a case study of complex interactions between physical, biological, and social systems. Siglufjör›ur’s natural capital— a good harbor and proximity to prime herring grounds—contributed to its development as a major fishing center during the first half of the 20th century. This herring fishery was initiated by Norwegians, but subsequently expanded by Icelanders to such an extent that the fishery, and Siglufjör›ur in particular, became engines helping to pull the whole Icelandic economy. -
Formation and Propagation of Great Salinity Anomalies H
GEOPHYSICAL RESEARCH LETTERS, VOL. 30, NO. 9, 1473, doi:10.1029/2003GL017065, 2003 Formation and propagation of great salinity anomalies H. Haak,1 J. Jungclaus,1 U. Mikolajewicz,1 and M. Latif 2 Received 5 February 2003; accepted 3 April 2003; published 8 May 2003. [1] North Atlantic/Arctic ocean and sea ice variability for LS is presented self-consistently within the framework of a the period 1948–2001 is studied using a global Ocean global ocean/sea ice model. General Circulation Model coupled to a dynamic/ thermodynamic sea ice model forced by daily NCEP/ NCAR reanalysis data [Kalnay et al., 1996]. Variability of 2. Numerical Experiments Arctic sea ice properties is analysed, in particular the [3] The Max-Planck-Institute ocean model (MPI-OM) is formation and propagation of sea ice thickness anomalies a primitive equation model (z-level, free surface), with the that are communicated via Fram Strait into the North hydrostatic and Boussinesq assumptions made. MPI-OM Atlantic. These export events led to the Great Salinity includes an embedded dynamic/thermodynamic sea ice Anomalies (GSA) of the 1970s, 1980s and 1990s in the model with viscous-plastic rheology following Hibler Labrador Sea (LS). All GSAs were found to be remotely [1979]. For details, see Marsland et al. [2003]. The excited in the Arctic, rather than by local atmospheric particular model configuration has 40 vertical levels, with forcing over the LS. Sea ice and fresh water exports through 20 of them in the upper 600 m. The horizontal resolution the Canadian Archipelago (CAA) are found to be only of gradually varies between a minimum of 20 km in the Arctic minor importance, except for the 1990s GSA. -
The Sargassum Invasion of the Eastern Caribbean and Dynamics of the Equatorial North Atlantic
The Sargassum Invasion of the Eastern Caribbean and Dynamics of the Equatorial North Atlantic Invasión de Sargazo en el Caribe Oriental y la Dinámica en la Zona Ecuatorial del Atlántico Norte L'Invasion de Sargasse dans les Caraïbes Orientales et leur Dynamique dans la Partie Nord de l'Atlantique Ėquatorial DONALD R. JOHNSON1*, DONG S. KO2, JAMES S. FRANKS1, PAULA MORENO1, and GUILLERMO SANCHEZ-RUBIO1 1Center for Fisheries Research and Development, Gulf Coast Research Laboratory, University of Southern Mississippi, Ocean Springs, Mississippi 39564 USA. *[email protected]. [email protected]. [email protected]. [email protected]. 2Ocean Dynamics and Prediction Branch, Naval Research Laboratory, Stennis Space Center, Mississippi 39529 USA. [email protected]. EXTENDED ABSTRACT In the spring and summer of 2011, unprecedented quantities of pelagic sargassum came ashore on many islands of the eastern Caribbean (Figure 1), seriously affecting fishery and tourism industries. Concurrently, pelagic sargassum also washed ashore in massive amounts along the coasts of western Africa (Sierra Leone and Benin) and was spotted in large mats by aircraft off northern Brazil (Széchy et al. 2012). Two species were identified in the invasion: Sargassum natans and Sargassum fluitans, both of which coexist throughout the North Atlantic with large mats and long lines commonly found in the Sargasso Sea (Winge 1923) and in the northern Gulf of Mexico (Comyns et al. 2002). Using satellite tracked mixed- layer drifters during 2010 and 2011 we were unable to connect the Caribbean invasion to the central North Atlantic and the Sargasso Sea. However, from archived results of a numerical circulation model (HYCOM), back-tracking from where landfalls were reported suggested that the sargassum may have bloomed in the north equatorial recirculation region (NERR) where conditions in the spring/summer of 2010 were conducive to growth and consolidation. -
Atmospheric Forcing During Active Convection in the Labrador Sea
PUBLICATIONS Journal of Geophysical Research: Oceans RESEARCH ARTICLE Atmospheric forcing during active convection in the Labrador 10.1002/2015JC011607 Sea and its impact on mixed-layer depth Key Points: Lena M. Schulze1, Robert S. Pickart2, and G. W. K. Moore3 Well-defined storm tracks toward Greenland result in the largest heat 1Florida State University, Tallahassee, Florida, USA, 2Department of Physical Oceanography, Woods Hole Oceanographic fluxes in the Labrador Sea 3 The canonical low-pressure system Institute, Woods Hole, Massachusetts, USA, Department of Physics, University of Toronto, Toronto, Ontario, Canada that drives convection is located east of the southern tip of Greenland Deeper mixing in the western basin is Abstract Hydrographic data from the Labrador Sea collected in February–March 1997, together with due to higher heat fluxes rather than oceanic preconditioning atmospheric reanalysis fields, are used to explore relationships between the air-sea fluxes and the observed mixed-layer depths. The strongest winds and highest heat fluxes occurred in February, due to the nature Correspondence to: and tracks of the storms. While greater numbers of storms occurred earlier and later in the winter, the L. M. Schulze, storms in February followed a more organized track extending from the Gulf Stream region to the Irminger [email protected] Sea where they slowed and deepened. The canonical low-pressure system that drives convection is located east of the southern tip of Greenland, with strong westerly winds advecting cold air off the ice edge over Citation: the warm ocean. The deepest mixed layers were observed in the western interior basin, although the vari- Schulze, L. -
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. -
Brazil Shelf LME (Sea Around Us 2006)
Sustainable Management of the Shared Living Marine Resources of the Caribbean Sea Large Marine Ecosystem (CLME) and Adjacent Regions Caribbean Large Marine Ecosystem Regional Transboundary Diagnostic Analysis - DRAFT - May 2011 Table of contents 1. EXECUTIVE SUMMARY ...................................................................................................... 8 2. INTRODUCTION .................................................................................................................. 16 2.1. BACKGROUND TO THE CLME REGION ............................................................................ 16 2.1.1. Global and regional significance of the CLME .............................................................. 16 2.1.2. Purpose of the Transboundary Diagnostic Analysis ...................................................... 18 2.2. STRUCTURE OF REGIONAL TDA ...................................................................................... 19 3. METHODOLOGY ................................................................................................................. 20 3.1. INTRODUCTION ................................................................................................................ 20 3.2. SUMMARY OF THE PRELIMINARY TDA (2007) ................................................................ 20 3.3. APPROACH ADOPTED FOR THE CLME TDA .................................................................... 21 3.3.1. Background ....................................................................................................................