The Brazil current as represented by the Mariano Global Surface Velocity Analysis (MGSVA). The Brazil current is the western boundary current of the South Atlantic subtropical gyre. It transports warm water polewards. Near 22 S, the Brazil current splits; one component flows eastward and the other component hugs the coast and flows toward the southwest and interacts with the colder Malvinas Current. Click here for example plots of seasonal averages.
Columbus had sailed into the Caribbean for Spain in 1492, first landing on what is now San Salvador in the Bahamas. There, he met the Lucayans, a docile, pleasant group of natives who told him of lands to the south (Richardson, 1998). He set sail days later and landed along the north coast of what is now Hispaniola. At first he thought that he had found some islands off the coast of India, and quickly claimed the lands for Spain. In order to prove that he did not simply find an additional coast or island of Africa, already claimed by Portugal, Columbus returned to Europe with several Tainos, the native inhabitants of the Greater Antilles who resembled indigenous tribes of South America. Spain was on the brink of becoming a world power as a result of Columbus' voyage, which did not sit well with the Portuguese, the predominant maritime power at the time. Pope Alexander VI would settle the matter in 1494 with the Treaty of Tordesillas which established a "Bull of Demarkation" at 46°W. Everything west of this meridian belonged to Spain and everything east would stay under the control of Portugal. Like Columbus, the Portuguese had hoped they would find a western seaway to Asia without having to round the treacherous Horn of Africa. The Ottomans and Arabs had full control of the trade routes on land while Indian and Arab traders dominated the Indian Ocean, making it difficult for the Portuguese who had established some trade with Japan. The Portuguese soon began to explore the westward reaches of the Atlantic bestowed on them by the Pope, and hoped to find an easier seaway to east Asia. Instead, they found what is now known as Brazil and thus were the first Europeans to sail the waters of the Brazil Current (Steinberg, 2001).

The Brazil Current is a weak western boundary current carrying warm subtropical water, which runs south along the coast of Brazil from about 9°S to about 38°S and is generally confined to the upper 600m of the water column. Its origin begins where the westward flowing trans-Atlantic South Equatorial Current (SEC) bifurcates (or splits) as it approaches the continental shelf off of Cabo de Sao Roque, Brazil (Stramma et al., 1990; Podesta et al., 1991). SEC water flowing north becomes the North Brazil Current, and the branch flowing south becomes the Brazil Current (BC). Although Isaaci Vossius is given credit as the first to recognize and describe the Brazil Current in 1663 in "A Treatise Concerning the Motion of the Seas & Winds," it was James Rennell in 1832 who worked out details of the actual flow, and dubbed the current the Brazil Current. He had been a member of the British Royal Navy and later joined the East India Company, making several trips across the Atlantic under the supervision of John Purdy. In addition to his detailed descriptions of these currents, it was Rennell who first determined that the BC was weaker than the North Brazil Current and was among the first to map out the surface currents along the New World continents (Peterson et al., 1996).

The Brazil Current begins at about 10°S, separating slightly from the coast near 12°S where the continental shelf becomes wider (Peterson & Stramma, 1991; Stramma et al., 1990). Satellite images taken over three years (1984-1987) show that the actual point at which the BC separates from the continental shelf varies anywhere between 33°S-38°S, with the average being about 36°S (Olson et al., 1988; Podesta et al., 1991). The BC continues to flow south off the Brazilian coast until it reaches about 33-38°S, when it collides with the north-flowing Malvinas (Falkland) Current. The BC is then, in part, deflected to the east offshore of Rio de la Plata, a region known as the Brazil-Malvinas Confluence Zone (BMC), one of the most energetic regions in all the oceans (Sarceno et al.,2004). Gordon and Greengrove (1986) were the first to label this region the Confluence. The latitude of confluence, which determines where the BC will separate from the continent, is farther north during austral winter and spring. This seasonality is presumed to be related to the general seasonal shift of wind systems and seasonal meridional shift of the subtropical gyre (Peterson & Stramma, 1991).

The transport of the Brazil Current is considered small when compared to that of the Gulf Stream, its counterpart in the Northern Atlantic. The problem when estimating transport of the BC is that in its northern region, it is shallow and closely confined to the continental shelf. Transport values between 5 Sv and 6.5 Sv have been observed near surface waters (upper 500m) of the BC around 20°S (Peterson and Stramma, 1990; Stramma et al., 1990). At about 20.5°S, the current encounters the Vitoria-Trindade Ridge, a zonal seamount chain where it has been observed to flow through the inshore passage rather than the passages farther east. In this region, a cyclonic gyre seaward of the Brazil Current, centered at about 17°S and 34°W has been observed and attributed to the southernmost meanders of the South Equatorial Current that are reflected northward by this same seamount chain (Memery et al., 2000; Stramma et al., 1990). At about 20.5°S, near the seamount chain, the current flows at about 50-60 cm s-1 as estimated by Evans and others (1983).

As the Brazil Current flows south of 24°S, its flow intensifies by about 5% per 100km, which is similar to the growth rate in the Gulf Stream, although transport values in the BC are considerably less (Peterson and Stramma, 1991). Thus, at about 33°S the total transport (which includes a recirculation cell in the upper 1400m) is about 18Sv, and reaches values from 19-22 Sv at about 38°S, where it encounters the Malvinas (Falkland) Current (Olson et al., 1988; Peterson and Stramma, 1991). The mean latitude of the BC's separation from the shelf break is about 35.8°S ± 1.1° and for the Malvinas Current, the mean latitude of separation is 38.9°S ± 0.9°. The coastal ranges of the separation positions are at 950km and 850km respectively (Olson et al., 1988).

The combined flow of the two currents causes a strong thermohaline frontal region, called the Brazil-Malvinas Confluence (BMC) in which the BC breaks off into two branches, one turning to the north forming a recirculation cell, while the other continues southward and veers northeast at about 45°S, becoming the South Atlantic Current (Boebel et al., 1999; Saraceno et al., 2004). The mean transport in this region has been measured to be about 11Sv (Garzoli and Bianchi, 1987). Maximum velocities at the confluence (at about 38°S) reach 55 cm s-1 with the average value of 35 cm s-1 with transports of 18 and 11 Sv respectively. Flow can increase up to 23 Sv at the Brazil-Malvinas Confluence (Garzoli, 1993) Mean conditions of circulation vary significantly, and more recent evidence shows that it is likely related to meteorological anomalies (Assireu et al., 2003). Some short term variability in the southward extent of the BC has also been observed. Occasionally, when a BC meander that has extended unusually far south retreats, it can shed a series of warm core eddies that migrate into the Antarctic Circumpolar Current (Partos and Piccolo, 1988). Values also vary according to measurement method and depth. A comprehensive overview of literature on BC transport estimates prior to 1991 can be found in Table 2 of Peterson and Stramma (1991).

The range of the Confluence oscillate between about 54°W and 45°W, a total distance of about 770 km (at 38°S). The meanders appear to occur on a twelve month cycle and are likely correlate to changes in the separation latitude of the Brazil Current (Boebel et al., 1999; Garzoli and Bianchi, 1987; Goni & Wainer, 2001; Maamaatuaiahutapu et al., 1999; Zavialov et al., 1999). The mean speed of the front is estimated to be about 14 cm s-1. The front oscillates around its mean seasonal position (farther north and east during austral winter and farther south and west during austral summer) within a period of about one month and an amplitude that varies from 10-50 km per day. The mean velocity of the displacement of the front reaches values up to 10 km/day (Garzoli and Bianchi, 1987). This area is also rich in eddies, more often called Brazil Current Rings, averaging to about 7-9 rings per year. These elliptical rings can vary in size from about 56 to 225 km along the semi-major axis, and 23 to 108 km for the semi-minor axis. These anticyclones have a mean lifetime of about 35 days and translational speeds of anywhere between 4-27 km per day (Lentini et al., 2002).

On average, the temperature in the Brazil Current is about 18°C-28°C, with essentially three meridional zones that experience several degrees of distinctly different annual temperature fluctuations, which corresponds to their proximity to shore. The first zone is located over the shelf and experiences temperature variability of 7-10 degrees, which is controlled by both winter invasions of subantarctic water from the Malvinas Current and discharges from Rio de la Plata and Patos-Mirim. The second or central portion, closer to the eastern margin of the continental shelf, experiences a 5-7 degree variance. The third, on the seaward-most zone, shows little fluctuation until the Confluence (Memery, et al., 2000; Zavialov et al., 1999). Temperatures in the southern section of the current, near the Confluence, can change by 5-13 degrees, with the cooler temperatures occurring around August-September and the warmer values observed in February (Boebel et al., 1999; Podesta, et al., 1991). Almost yearly temperature anomalies of warm and cold fronts occur that seem to be related to the El Nino-Southern Oscillation (ENSO) events. Anomalous cold water extensions to the north occur on the shelf generally one year after every warm ENSO event, and anomalous warm water extensions occur generally one year after every cold ENSO (Lentini et al., 2001). Surface salinities indicative of Brazil Current waters range from 35.1 to 36.2, with the maximum commonly found at around 20°S, where it can reach a salinity of 37.3 (Memery et al., 2000; Wilson & Rees, 2000).

References

Assireu, A.T., M.R. Stevenson, J.L. Stech, 2003: Surface circulation and kinetic energy in the SW Atlantic obtained by drifters. Continental Shelf Research, 23, 145-157.

Boebel, O., C. Schmid, G. Podesta and W. Zenk, 1999: Intermediate water in the Brazil-Malvinas Confluence Zone: A Lagrangian view. Journal of Geophysical Research, 104 (C9), 21,063-21,082.

Evans, D.L, S.S. Signorini and L.B. Miranda, 1983: A note on the transport of the Brazil Current. Journal of Physical Oceanography, 13, 1732-1738.

Garzoli S.L. and A. Bianchi, 1987: Time-Space Variability of the Local Dynamics of the Malvinas-Brazil Confluence as Revealed by Inverted Echo Sounders. Journal of Geophysical Research, 92, 1914-1922.

Goni, G. and I. Wainer, 2001: Investigation of the Brazil Current front variability from altimeter data. Journal of Geophysical Research, 106 (C12), 31,117-31,128.

Gordon, A.L. and C.L. Greengrove, 1986: Geostrophic circulation of the Brazil-Falkland Confluence. Deep-Sea Research, 33, 573-585.

Lentini, C.A.D., G.G. Podesta, E.J.D. Campos, and D.B. Olson, 2001: Sea surface temperature anomalies on the Western South Atlantic from 1982-1994. Continental Shelf Research, 21, 89-112.

Maamaatuaiahutapu, K., C. Provost, C. Andrie, and X. Vigan, 1999: Origin and ages of mode waters in the Brazil-Malvinas Confluence region during austral winter 1994. Journal of Geophysical Research, 104 (C9), 21,051-21,061.

Memery, L., M. Arhan, X.A. Alvarez-Salgado, M-J. Messias, H. Mercier, C.G. Castro, A.F. Rios, 2000: The water masses along the western boundary of the south and equatorial Atlantic. Progress in Oceanography, 47, 69-98.

Olson, DB, G.P. Podesta, R.H. Evans and O.B. Brown, 1988: Temporal variations in the separation of Brazil and Malvinas currents. Deep-Sea Research, 35 (12), 1971-1990.

Partos, P. and M.C. Piccolo, 1988: Hydrography of the Argentine continental shelf between 38°S and 42°S. Continental Shelf Research, 8, 1043-1056.

Peterson, R.G., L. Stramma, and G. Kortum, 1996: Early concepts in charts and circulation. Progress in Oceanography, 37, 1-115.

Peterson, R.G. and L. Stramma, 1990: Upper-level circulation in the South Atlantic Ocean. Progress in Oceanography, 26, 1-73.

Podesta, G.P., O.B. Brown, and R.H. Evans, 1991: The Annual Cycle of Satellite-derived Sea Surface Temperature in the Southwestern Atlantic Ocean. Journal of Climate, 4 (4), 457-467.

Richardson, B., 1998: The Caribbean in the Wider World 1492-1992: A Regional Geography. Cambridge University Press: Cambridge. 235p.

Saraceno, M., C. Provost, A.R. Piola, J. Bava, and A. Gagliardini, 2004: Brazil Malvinas Frontal System as seen from 9 years of advanced very high resolution radiometer data. Journal of Geophysical Research, 109 (C5),

Steinberg, P.E., 2001: The Social Construction of the Ocean. Cambridge Studies in International Relations, Cambridge University Press: Cambridge, UK. 239p.

Stramma, L., Y. Ikeda, R.G. Peterson, 1990: Geostrophic transport in the Brazil Current region north of 20°S. Deep-Sea Research, 37 (12), 1875-1886.

Zavilov, P.O., I. Wainer, J.M. Absy, 1999: Sea surface temperature variability off southern Brazil and Uruguay as revealed from historical data since 1854. Journal of Geophysical Research, 105 (C9), 21,021-21,032.

Wilson, H.R. and N.W. Rees, 2000: Classification of mesoscale features in the Brazil-Falkland Current confluence zone. Progress in Oceanography, 45, 415-426.