Books on the topic 'Coastral upwelling'

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1

Barth, John A. Stability of a coastal upwelling front over topography. Woods Hole, Mass: Woods Hole Oceanographic Institution, 1987.

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2

Park, M. M. Coastal transition zone pilot - 1987: Rapid sampling vertical profiler observations. Corvallis, Or: College of Oceanography, Oregon State University, 1987.

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3

Fasciano, William Culp. Meandering of the coastal upwelling jet near Cape Mendocino, California: A comparison between laboratory simulations and oceanic observations. Monterey, Calif: Naval Postgraduate School, 1989.

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4

Howe, John T. Biogeochemical cycling in the ocean. Moffett Field, Calif: National Aeronautics and Space Administration, Ames Research Center, 1986.

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5

Collard, Sneed B. Coastal upwelling and mass mortalities of fishes and invertebrates in the northeastern Gulf of Mexico during spring and summer 1998: Final report. New Orleans, La: U.S. Dept. of the Interior, Minerals Management Service, Gulf of Mexico OCS Region, 1999.

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6

Suess, Erwin, and Jörn Thiede. Coastal Upwelling Its Sediment Record : Part A: Responses of the Sedimentary Regime to Present Coastal Upwelling. Springer, 2012.

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7

Suess, Erwin, and Jörn Thiede. Coastal Upwelling Its Sediment Record : Part A: Responses of the Sedimentary Regime to Present Coastal Upwelling. Springer, 2013.

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8

Dickson, Mary-Lynn. Nitrogen dynamics in a coastal upwelling regime. 1994.

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9

McCaffrey, Mark A. Sedimentary lipids as indicators of depositional conditions in the coastal Peruvian upwelling regime. 1990.

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10

Coastal upwelling indices, west coast of North America, 1946-1995. [La Jolla, Calif.]: U.S. Dept. of Commerce, National Oceanic and Atmospheric Administration, National Marine Fisheries Service, Southwest Fisheries Science Center, 1996.

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11

Sanford, Eric. Oceanographic influences on rocky intertidal communities: Coastal upwelling, invertebrate growth rates, and keystone predation. 1999.

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12

Evolution of upwelling fronts off the coast of Portugal: Final technical report. [Palisades, N.Y.?]: Lamont-Doherty Earth Observatory of Columbia University, 1994.

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13

Polar Research Program (U.S.), ed. Sea ice on the Southern Ocean: Final technical report, grant # NAGW-3362. [Washington, DC?]: Polar Research Program, Office of Mission to Planet Earth, National Aeronautics and Space Administration, 1998.

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14

Polar Research Program (U.S.), ed. Sea ice on the Southern Ocean: Final technical report, grant # NAGW-3362. [Washington, DC?]: Polar Research Program, Office of Mission to Planet Earth, National Aeronautics and Space Administration, 1998.

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15

Hameed, Saji N. The Indian Ocean Dipole. Oxford University Press, 2018. http://dx.doi.org/10.1093/acrefore/9780190228620.013.619.

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Discovered at the very end of the 20th century, the Indian Ocean Dipole (IOD) is a mode of natural climate variability that arises out of coupled ocean–atmosphere interaction in the Indian Ocean. It is associated with some of the largest changes of ocean–atmosphere state over the equatorial Indian Ocean on interannual time scales. IOD variability is prominent during the boreal summer and fall seasons, with its maximum intensity developing at the end of the boreal-fall season. Between the peaks of its negative and positive phases, IOD manifests a markedly zonal see-saw in anomalous sea surface temperature (SST) and rainfall—leading, in its positive phase, to a pronounced cooling of the eastern equatorial Indian Ocean, and a moderate warming of the western and central equatorial Indian Ocean; this is accompanied by deficit rainfall over the eastern Indian Ocean and surplus rainfall over the western Indian Ocean. Changes in midtropospheric heating accompanying the rainfall anomalies drive wind anomalies that anomalously lift the thermocline in the equatorial eastern Indian Ocean and anomalously deepen them in the central Indian Ocean. The thermocline anomalies further modulate coastal and open-ocean upwelling, thereby influencing biological productivity and fish catches across the Indian Ocean. The hydrometeorological anomalies that accompany IOD exacerbate forest fires in Indonesia and Australia and bring floods and infectious diseases to equatorial East Africa. The coupled ocean–atmosphere instability that is responsible for generating and sustaining IOD develops on a mean state that is strongly modulated by the seasonal cycle of the Austral-Asian monsoon; this setting gives the IOD its unique character and dynamics, including a strong phase-lock to the seasonal cycle. While IOD operates independently of the El Niño and Southern Oscillation (ENSO), the proximity between the Indian and Pacific Oceans, and the existence of oceanic and atmospheric pathways, facilitate mutual interactions between these tropical climate modes.
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16

Behera, Swadhin, and Toshio Yamagata. Climate Dynamics of ENSO Modoki Phenomena. Oxford University Press, 2018. http://dx.doi.org/10.1093/acrefore/9780190228620.013.612.

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The El Niño Modoki/La Niña Modoki (ENSO Modoki) is a newly acknowledged face of ocean-atmosphere coupled variability in the tropical Pacific Ocean. The oceanic and atmospheric conditions associated with the El Niño Modoki are different from that of canonical El Niño, which is extensively studied for its dynamics and worldwide impacts. A typical El Niño event is marked by a warm anomaly of sea surface temperature (SST) in the equatorial eastern Pacific. Because of the associated changes in the surface winds and the weakening of coastal upwelling, the coasts of South America suffer from widespread fish mortality during the event. Quite opposite of this characteristic change in the ocean condition, cold SST anomalies prevail in the eastern equatorial Pacific during the El Niño Modoki events, but with the warm anomalies intensified in the central Pacific. The boreal winter condition of 2004 is a typical example of such an event, when a tripole pattern is noticed in the SST anomalies; warm central Pacific flanked by cold eastern and western regions. The SST anomalies are coupled to a double cell in anomalous Walker circulation with rising motion in the central parts and sinking motion on both sides of the basin. This is again a different feature compared to the well-known single-cell anomalous Walker circulation during El Niños. La Niña Modoki is the opposite phase of the El Niño Modoki, when a cold central Pacific is flanked by warm anomalies on both sides.The Modoki events are seen to peak in both boreal summer and winter and hence are not seasonally phase-locked to a single seasonal cycle like El Niño/La Niña events. Because of this distinction in the seasonality, the teleconnection arising from these events will vary between the seasons as teleconnection path will vary depending on the prevailing seasonal mean conditions in the atmosphere. Moreover, the Modoki El Niño/La Niña impacts over regions such as the western coast of the United States, the Far East including Japan, Australia, and southern Africa, etc., are opposite to those of the canonical El Niño/La Niña. For example, the western coasts of the United States suffer from severe droughts during El Niño Modoki, whereas those regions are quite wet during El Niño. The influences of Modoki events are also seen in tropical cyclogenesis, stratosphere warming of the Southern Hemisphere, ocean primary productivity, river discharges, sea level variations, etc. A remarkable feature associated with Modoki events is the decadal flattening of the equatorial thermocline and weakening of zonal thermal gradient. The associated ocean-atmosphere conditions have caused frequent and persistent developments of Modoki events in recent decades.
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