In the ocean, all the water masses have different physical properties, defining their density. The most important factors impacting the water density are the salinity and the temperature. The lower the salinity and the temperature, the denser the water mass. These density difference makes the water masses move and create currents (figure).
In the tropical areas, the water masses are warmer. Furthermore, the sea surface evaporation is important, and consequently, the surface water masses are saltier. When these masses arrive to the poles, their temperature decrease and the melting ice caps are adding fresh water, making these water masses even denser. At high latitude, the densest bodies of water are plunging beneath the least dense and these denser bodies of water circulate at depth, beneath the less dense bodies of water, which remain on the surface. The thermohaline circulation is of much of importance for the climate system, as it has an influence on the heat transport and repartition at the Earth surface.
Figure: Schematic representation of the thermohaline circulation, with the warm and salted water in red and the cold and fresher water in blue, displayed on a world map (modified after Rahmstorf, 2002, ocean data view, Schlitzer, 2018).
These water masses, with different properties (e.g. salinity, temperature, nutrient content or ion concentrations) also have a strong influence on the marine life and marine productivity. For example, in some places, the cold and rich in nutrients bottom water is brought to the sea surface due to the wind configuration. This is called an upwelling and this important nutrient supply from the depths generally leads to an important biodiversity development.
The continental configuration at the Earth surface has an influence on the currents dynamics. For example, from Neogene to present, the main tectonic change that has affected the Atlantic Ocean is the closure of the Panama Isthmus, between 13 Ma and 2.6 Ma (Bartoli et al., 2005; Lunt et al., 2008; O’Dea et al., 2016). This affected the oceanic circulation, currents position and exchange between the Pacific and the Atlantic as well as ocean atmosphere feedback mechanisms, and so, climate in general since the late Miocene-early Pliocene (Haug and Tiedemann, 1998; Lear et al., 2003; Maier-Reimer and Mikolajewicz, 1990; Billups et al., 1999; Haug et al., 2001). For these reasons, the closure of the Panama Isthmus is also at the origin of the intensification of the Northern hemisphere glaciation (NHG) (appearance of perennial ice caps in the North hemisphere) (Bartoli et al., 2005; Lunt et al., 2008a). These currents are also under the influence of the glacial-Interglacial cycles and orbital cycles during the Cenozoic (Kleiven et al., 2003; Rühlemann et al., 2004, 1999).
Bibliography
Bartoli, G., Sarnthein, M., Weinelt, M., Erlenkeuser, H., Garbe-Schönberg, D., and Lea, D. W.: Final closure of Panama and the onset of northern hemisphere glaciation, Earth and Planetary Science Letters, 237, 33–44, https://doi.org/10.1016/j.epsl.2005.06.020, 2005.
Billups, K., Ravelo, A. C., Zachos, J. C., and Norris, R. D.: Link between oceanic heat transport, thermohaline circulation, and the Intertropical Convergence Zone in the early Pliocene Atlantic, Geology, 27, 319–322, https://doi.org/10.1130/0091-7613(1999)027<0319:LBOHTT>2.3.CO;2, 1999.
Haug, G. H. and Tiedemann, R.: Effect of the formation of the Isthmus of Panama on Atlantic Ocean thermohaline circulation, Nature, 393, 673–676, https://doi.org/10.1038/31447, 1998.
Haug, G. H., Tiedemann, R., Zahn, R., and Ravelo, A. C.: Role of Panama uplift on oceanic freshwater balance, Geology, 29, 207–210, 2001.
Kleiven, H. F., Jansen, E., Curry, W. B., Hodell, D. A., and Venz, K.: Atlantic Ocean thermohaline circulation changes on orbital to suborbital timescales during the mid-Pleistocene, Paleoceanography, 18, 13, https://doi.org/10.1029/2001PA000629, 2003.
Lear, C. H., Rosenthal, Y., and Wright, J. D.: The closing of a seaway: ocean water masses and global climate change, Earth and Planetary Science Letters, 210, 425–436, https://doi.org/10.1016/S0012-821X(03)00164-X, 2003.
Lunt, D. J., Foster, G. L., Haywood, A. M., and Stone, E. J.: Late Pliocene Greenland glaciation controlled by a decline in atmospheric CO2 levels, Nature, 454, 1102–1105, https://doi.org/10.1038/nature07223, 2008.
Maier-Reimer, E. and Mikolajewicz, U.: Ocean general circulation model sensitivity experiment with an open central American Isthmus, Paleoceanography, 5, 349–366, 1990.
O’Dea, A., Lessios, H. A., Coates, A. G., Eytan, R. I., Restrepo-Moreno, S. A., Cione, A. L., Collins, L. S., de Queiroz, A., Farris, D. W., Norris, R. D., Stallard, R. F., Woodburne, M. O., Aguilera, O., Aubry, M.-P., Berggren, W. A., Budd, A. F., Cozzuol, M. A., Coppard, S. E., Duque-Caro, H., Finnegan, S., Gasparini, G. M., Grossman, E. L., Johnson, K. G., Keigwin, L. D., Knowlton, N., Leigh, E. G., Leonard-Pingel, J. S., Marko, P. B., Pyenson, N. D., Rachello-Dolmen, P. G., Soibelzon, E., Soibelzon, L., Todd, J. A., Vermeij, G. J., and Jackson, J. B. C.: Formation of the Isthmus of Panama, Sci. Adv., 2, 11, https://doi.org/10.1126/sciadv.1600883, 2016.
Rahmstorf, S.: Ocean circulation and climate during the past 120,000 years, Nature, 419, 207–214, https://doi.org/10.1038/nature01090, 2002.
Rühlemann, C., Mulitza, S., Müller, P. J., Wefer, G., and Zahn, R.: Warming of the tropical Atlantic Ocean and slowdown of thermohaline circulation during the last deglaciation, Nature, 402, 511–514, https://doi.org/10.1038/990069, 1999.
Rühlemann, C., Mulitza, S., Lohmann, G., Paul, A., Prange, M., and Wefer, G.: Intermediate depth warming in the tropical Atlantic related to weakened thermohaline circulation: Combining paleoclimate data and modeling results for the last deglaciation, Paleoceanography, 19, PA1025, https://doi.org/10.1029/2003PA000948, 2004.
Schlitzer, R.: Ocean Data View, 2018.
January 2025