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=== North Atlantic Ocean === While in the stratosphere (post-test period), the tritium interacted with and oxidized to water molecules and was present in much of the rapidly produced rainfall, making tritium a prognostic tool for studying the evolution and structure of the [[water cycle]] as well as the ventilation and formation of water masses in the North Atlantic.<ref name="Oceanus"/> Bomb-tritium data were used from the Transient Tracers in the Ocean (TTO) program in order to quantify the replenishment and overturning rates for deep water located in the North Atlantic.<ref name="Bomb Tritium"> {{cite journal |last=Doney |first=Scott C. |year=1992 |title=Bomb tritium in the deep north Atlantic |journal=Oceanography |volume=5 |issue=3 |pages=169β170 |doi=10.5670/oceanog.1992.11 |doi-access=free }} </ref> Bomb-tritium also enters the deep ocean around the Antarctic.<ref name="Bomb Tritium Antarctic"> {{cite journal |last1=Michel |first1=Robert |first2=Peter M. |last2=Williams |date=1973 |title=Bomb-produced tritium in the Antarctic Ocean |journal=Earth and Planetary Science Letters |volume=20 |issue=3 |pages=381β384 |doi=10.1016/0012-821X(73)90013-7 |bibcode=1973E&PSL..20..381M }} </ref> Most of the bomb tritiated water (H{{sup|3}}HO) throughout the atmosphere can enter the ocean through the following processes: * precipitation * vapor exchange * river runoff These processes make H{{sup|3}}HO a great tracer for time scales of up to a few decades.<ref name="Bomb Tritium"/> Using the data from these processes for 1981, the 1-TU isosurface lies between 500 and 1,000 meters deep in the [[subtropical]] regions and then extends to 1,500β2,000 meters south of the [[Gulf Stream]] due to recirculation and ventilation in the upper portion of the Atlantic Ocean.<ref name="Oceanus"/> To the north, the isosurface deepens and reaches the floor of the [[abyssal plain]] which is directly related to the ventilation of the ocean floor over 10β20 year time-scales.<ref name="Oceanus"/> Also evident in the Atlantic Ocean is the tritium profile near [[Bermuda]] between the late 1960s and late 1980s. There is a downward propagation of the tritium maximum from the surface (1960s) to 400 meters (1980s), which corresponds to a deepening rate of about 18 meters per year.<ref name="Oceanus" /> There are also tritium increases at 1,500 m depth in the late 1970s and 2,500 m in the middle of the 1980s, both of which correspond to cooling events in the deep water and associated deep water ventilation.<ref name="Oceanus"/> From a study in 1991, the tritium profile was used as a tool for studying the mixing and spreading of newly formed [[North Atlantic Deep Water]] (NADW), corresponding to tritium increases to 4 TU.<ref name="Bomb Tritium" /> This NADW tends to spill over sills that divide the [[Norwegian Sea]] from the North Atlantic Ocean and then flows to the west and equatorward in deep boundary currents. This process was explained via the large-scale tritium distribution in the deep North Atlantic between 1981 and 1983.<ref name="Bomb Tritium" /> The sub-polar gyre tends to be freshened (ventilated) by the NADW and is directly related to the high tritium values (>1.5 TU). Also evident was the decrease in tritium in the deep western boundary current by a factor of 10 from the [[Labrador Sea]] to the [[Tropics]], which is indicative of loss to ocean interior due to turbulent mixing and recirculation.<ref name="Bomb Tritium" />
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