Ocean Circulation: Thermohaline Circulation, Slides of Fluid Dynamics

The thermohaline circulation, for the most part, is an 'overturning' circulation in which warm water flows poleward near the surface and is subsequently ...

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The circulation of the ocean is usually divided
into two parts, a wind-driven circulation that
dominates in the upper few hundred meters,
and a density-driven circulation that dominates
below. The latter is called the ‘thermohaline’
circulation because of the role of heating, cool-
ing, freshening, and salinification in producing
regional density differences within the ocean.
The thermohaline circulation, for the most
part, is an ‘overturning’ circulation in which
warm water flows poleward near the surface
and is subsequently converted into cold water
that sinks and flows equatorward in the in-
terior. Radiocarbon measurements show that
the thermohaline circulation turns over all the
deep water in the ocean every 600 years or so.
The most spectacular features of the ther-
mohaline circulation are seen in the sinking
phase, in the formation of new deep water in
the North Atlantic and the Southern Ocean.
Large volumes of cold polar water can be
readily observed spilling over sills, mixing
violently with warmer ambient water, and
otherwise descending to abyssal depths. The
main features of the upwelling phase are less
obvious. Most of the gaps in our knowledge
about the thermohaline circulation are due to
uncertainty about where the upwelling occurs
and how upwelled deep water returns to the
areas of deep-water formation. The main new
development in studies of the thermohaline
circulation is the role of Drake Passage and the
Antarctic Circumpolar Current (ACC) in the
upwelling phase.
The thermohaline circulation is an impor-
tant factor in the earth’s climate because it
transports roughly 1015 W of heat poleward
into high latitudes, about one fourth of the total
heat transport of the ocean/atmosphere circu-
lation system. The upwelling branch of the
thermohaline circulation is important for the
ocean’s biota as it brings nutrient-rich deep
water up to the surface. The thermohaline
circulation is thought to be vulnerable to the
warming and freshening of the earth’s polar
regions associated with global warming.
The Cooling Phase - Deep-Water
Formation
The most vigorous thermohaline circulation in
the ocean today is in the Atlantic Ocean where
the overturning is often likened to a giant con-
veyor belt. The upper part of the conveyor
carries warm, upper ocean water through the
tropics and subtropics toward the north while
the deep part carries cold dense polar water
southward through the Atlantic, around the tip
of Africa, and into the ocean beyond. The
Atlantic conveyor converts roughly 15x106
m3s-1 of upper ocean water into deep water.
(Oceanographers designate a flow rate of
1x106m3s-1 to be one Sverdrup, or Sv. All the
world’s rivers combined deliver about one Sv
of fresh water to the ocean.) Most of the 15-Sv
flow of the upper part of the conveyor passes
through the Florida Straits and up the east
coast of North America as part of the Gulf-
stream. The path of the conveyor cuts east-
ward across the Atlantic and continues
northward along the coast of Europe. As the
conveyor moves out across the Atlantic and
northward off Europe it gives up roughly 50 W
of heat per square meter of ocean surface to the
atmosphere. This heat flux is comparable to
Ocean Circulation: Thermohaline Circulation
J. R. Toggweiler, Geophysical Fluid Dynamics Laboratory, NOAA, Princeton, NJ 08542
Robert M. Key, Atmospheric and Oceanic Sciences Program, Department of Geosciences,
Princeton University, Princeton, NJ 08540
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The circulation of the ocean is usually divided into two parts, a wind-driven circulation that dominates in the upper few hundred meters, and a density-driven circulation that dominates below. The latter is called the ‘thermohaline’ circulation because of the role of heating, cool- ing, freshening, and salinification in producing regional density differences within the ocean. The thermohaline circulation, for the most part, is an ‘overturning’ circulation in which warm water flows poleward near the surface and is subsequently converted into cold water that sinks and flows equatorward in the in- terior. Radiocarbon measurements show that the thermohaline circulation turns over all the deep water in the ocean every 600 years or so.

The most spectacular features of the ther- mohaline circulation are seen in the sinking phase, in the formation of new deep water in the North Atlantic and the Southern Ocean. Large volumes of cold polar water can be readily observed spilling over sills, mixing violently with warmer ambient water, and otherwise descending to abyssal depths. The main features of the upwelling phase are less obvious. Most of the gaps in our knowledge about the thermohaline circulation are due to uncertainty about where the upwelling occurs and how upwelled deep water returns to the areas of deep-water formation. The main new development in studies of the thermohaline circulation is the role of Drake Passage and the Antarctic Circumpolar Current (ACC) in the upwelling phase.

The thermohaline circulation is an impor- tant factor in the earth’s climate because it transports roughly 10^15 W of heat poleward

into high latitudes, about one fourth of the total heat transport of the ocean/atmosphere circu- lation system. The upwelling branch of the thermohaline circulation is important for the ocean’s biota as it brings nutrient-rich deep water up to the surface. The thermohaline circulation is thought to be vulnerable to the warming and freshening of the earth’s polar regions associated with global warming.

The Cooling Phase - Deep-Water

Formation

The most vigorous thermohaline circulation in the ocean today is in the Atlantic Ocean where the overturning is often likened to a giant con- veyor belt. The upper part of the conveyor carries warm, upper ocean water through the tropics and subtropics toward the north while the deep part carries cold dense polar water southward through the Atlantic, around the tip of Africa, and into the ocean beyond. The Atlantic conveyor converts roughly 15x10 6 m 3 s-1^ of upper ocean water into deep water. (Oceanographers designate a flow rate of 1x10^6 m^3 s-1^ to be one Sverdrup, or Sv. All the world’s rivers combined deliver about one Sv of fresh water to the ocean.) Most of the 15-Sv flow of the upper part of the conveyor passes through the Florida Straits and up the east coast of North America as part of the Gulf- stream. The path of the conveyor cuts east- ward across the Atlantic and continues northward along the coast of Europe. As the conveyor moves out across the Atlantic and northward off Europe it gives up roughly 50 W of heat per square meter of ocean surface to the atmosphere. This heat flux is comparable to

Ocean Circulation: Thermohaline Circulation

J. R. Toggweiler , Geophysical Fluid Dynamics Laboratory, NOAA, Princeton, NJ 08542

Robert M. Key , Atmospheric and Oceanic Sciences Program, Department of Geosciences,

Princeton University, Princeton, NJ 08540

the solar energy reaching the lowest layers of the atmosphere during the winter months and is a significant factor in the climate of North- ern Europe.

As the upper part of the conveyor moves northward through the tropical and subtropical North Atlantic it spans a depth range from the surface down to ~800 m and has a mean tem- perature of some 15-20°C. During its transit through the tropics and subtropics the flow becomes saltier due to the excess of evapora- tion over precipitation in this region. It also becomes warmer and saltier by mixing with the salty outflow from the Mediterranean Sea. By the time the flow has crossed the 50°N parallel into the subpolar North Atlantic it has cooled to an average temperature of 11.5°C. Roughly half of the water carried northward by the conveyor flows into the Norwegian Sea between Iceland and Norway. Part of the con- veyor flow extends into the Arctic Ocean.

The final stages of the cooling process make the salty North Atlantic water dense enough to sink. Sinking is known to occur in three main places. The densest sinking water in the North Atlantic is formed in the Barents Sea north of Norway where salty water from the Norwegian Current is exposed to the atmo- sphere on the shallow ice-free Barents shelf. Roughly 2 Sv of water from the Norwegian Current crosses the shelf and sinks into the Arctic basin after being cooled down to 0°C. This water eventually flows out of the Arctic along the coast of Greenland at a depth of 600 to 1000 m. The volume of this flow is in- creased by additional sinking and open-ocean convection in the Greenland Sea north of Ice- land. A mixture of these two water masses flows into the North Atlantic over the sill be- tween Iceland and Greenland (Denmark Strait) at 600 m.

As 0°C water from the Arctic and Green- land Seas passes through Denmark Strait it mixes with 6°C Atlantic water beyond the sill and descends the Greenland continental slope down to a depth of 3000 m. It flows southward

around the southern tip of Greenland into the Labrador Sea as part of a deep boundary cur- rent that follows the perimeter of the subpolar North Atlantic. A slightly warmer water mass is formed by open-ocean convection within the Labrador Sea. The deep-water formed in the Labrador Sea increases the volume flow of the boundary current that exits the subpolar North Atlantic beyond the eastern tip of Newfound- land. Newly formed water masses are easy to track by their distinct temperature and salinity signatures, high oxygen, and anthropogenic tracer concentrations. The southward flow of North Atlantic Deep Water (NADW) is a prime example. NADW is identified as a water mass with a narrow spread of temperatures and salinities between 2.0 and 3.5°C and 34.9 and 35.0 psu. NADW quickly ventilates the Atlantic Ocean. Figure 1 shows an oceano- graphic section between the southern tip of Greenland and the coast of Labrador showing recent ventilation by chloroflorocarbon 11 (CFC 11, or Freon 11). High CFC water with concentrations in excess of 3.0 units tags the overflow water from Denmark Strait that flows around the tip of Greenland along the sloping bottom on the right into the Labrador Sea. Deep water with a slightly lower CFC concen- tration flows out of the Labrador Sea at the same depth on the left. High CFC water in the center of the basin (3.5 - 4.0 units) tags Labra- dor Sea Water that has been ventilated by win- ter convection down to 2000 m. There is presently no water in the North Atlantic north of 30°N that is uncomtaminated with CFCs. NADW flows southward along the coasts of North and South America until it reaches the circumpolar region south of the tip of Africa. Figure 2 shows the distribution of salinity in the western Atlantic along the path of the flow. Newly formed NADW (S>34.9) is easily distinguished from the relatively fresh intermediate water above (S<34.6) and the Antarctic water below (S<34.7). NADW exits the Atlantic south of Africa between 35° and

the south. The deep water formed around Ant- arctica does not readily ventilate the Southern Ocean. It is diluted many times by mixing with the weakly ventilated water offshore. Figure 3 shows CFC 11 concentrations along a transect at 140°E that begins on the Antarctic continental shelf on the left. This section was occupied at roughly the same time as the North Atlantic section in figure 1. In contrast to figure 1, water with more than 3.0 units of CFC 11 is limited to near-surface waters and the continental shelf. A small amount of recently ventilated water (>1.0 units) is seen descending to the bottom along the continental slope. The mass of old CFC-free water that fills the interior is known as Circumpolar Deep Water (CDW). The mixture of Antarctic shelf water and CDW descending the slope is Ant- arctic Bottom Water (AABW). AABW occu- pies the deepest parts of the ocean and is observed penetrating northward into the Atlan-

tic, Indian, and Pacific Oceans through deep passages in the mid-ocean ridge system. Small quantities of deep water are also observed to form in evaporative seas like the Mediterranean and Red Seas. These water masses are dense owing to their high salinities. They tend to form intermediate-depth water masses in relation to the colder deep and bottom waters from the North Atlantic and Antarctica.

The Warming Phase - Upwelling and the Return Flow

The upwelling of deep water back to the ocean’s surface was thought at one time to be widely distributed over the whole ocean. This variety of upwelling was linked to turbulent mixing processes that were hypothesized to be active throughout the interior. Mixing was

Figure 2: North-south section of salinity down the western Atlantic from Iceland to Drake Passage. The salinity distribution has been contoured every 0.1 psu between 34.0 and 35.0 psu to highlight North Atlantic Deep Water (34.9-35.0).

Latitude

Depth (m)

60S 40 20 Eq 20 40 60N

37.0 36.

34.7 34.

34.7 (^) 34.

thought to be slowly heating the deep ocean, making the old deep water in the interior pro- gressively less dense so that it could be dis- placed upward by the colder and saltier deep waters forming near the poles. Since the main areas of deep water formation are located at either end of the Atlantic, and since most of the ocean’s area is found in the Indian and Pacific Oceans, it stood to reason that the warming of the return flow should be widely distributed across the Indian and Pacific. Schematic diagrams often depict the closure of the conveyor circulation as a flow of warm upper-ocean water that passes from the North Pacific through Indonesia, across the Indian Ocean, and then around the tip of Africa into the Atlantic.

Observations made over the last 30 years have failed to support the idea of a broad, dif- fuse upwelling. Attempts to directly measure turbulent mixing rates in the interior have shown that the actual mixing rates are gener- ally only about 10 or 20% of the amount re- quired. There is no indication that any deep water is actually upwelling to the surface in the warm parts of the Indian and Pacific Oceans. Mixing does seem to be effective in warming the deepest part of the ocean, however. Modern circulation reconstructions show Ant- arctic Bottom Water flowing northward into the Indian, Pacific, and Atlantic basins at 0°C, upwelling across 3500 m, and exiting back to the south at less than 2°C between 2000 and 3500 m. This indicates that the circulation and heat transport associated with mixing in the

Figure 3: Section of CFC 11 extending northward from the coast of Antarctica along 140°E (WOCE section SR3) illustrating the penetration of CFCs into the Southern Ocean. Measurements courtesy of J. Bullister of NOAA-PMEL, collected during Aurora Australis cruise AU9404 12/94 - 1/95.

Latitude

Depth (m)

66S 64 62 60 58 56 54S

3.0 2.

4.0 5.0 4.

6.0 7.0 6.

is a reflection of the Antarctic Circumpolar Current which flows to the east across the sec- tion (out of the page), i.e. the north-south den- sity gradient between 40 and 60°S is in ther- mal wind balance with an eastward flow that increases toward the surface. The relatively deep and flat position of the isopycnals at the base of the thermocline reflect, to a large ex- tent, the mechanical work done by the winds that drive the ACC. The convergent surface flow generated by the winds pushes down rela- tively light water north of the ACC in relation to the cold, dense water being lifted up by the winds south of the ACC.

The position of the 36.0 and 36.4 g kg- isopycnals at depths near 1000 m is important because it signals the presence of relatively warm water adjacent to the sills in the north

where new NADW spills into the deep North Atlantic. It is the contrast between the cold water behind the sills and relatively warm water beyond the sills that provides the density gradient that drives the flow of dense water into the deep Atlantic. Numerical experiments carried out in ocean GCMs suggest that all the warm isopycnals in the lower thermocline would be squeezed up into the main thermo- cline if Drake Passage were to be closed up and the ACC eliminated. Gnanadesikan has described a general theory for the thermohaline circulation which relates the thickness of the thermocline, as illustrated in figure 4, with the intensity of the Atlantic conveyor. When deep-water formation occurs in the North Atlantic it converts rela- tively light low-density water within the ther-

Figure 4: Density structure of the Atlantic thermocline. Seawater density is referenced to a depth of 2000 m and has been zonally averaged across the Atlantic basin (units g kg-1). Contours have been chosen to highlight the lower part of the thermocline. The zonally averaged topography in figure 4 fails to capture the height of the sills in the Greenland-Scotland Ridge (65°N) which are closer to 600 m.

Latitude

Depth (m)

60S 40 20 Eq 20 40 60 80N

35.0 35.

36.0 35.

36.0 36.

37.0 (^) 37.

mocline into new deep water. It thereby removes mass from the thermocline, allowing it to be squeezed upward. When water is up- welled from the deep ocean and pumped into the thermocline in the south it adds mass to the thermocline, causing it to thicken downward. In this way the thermocline thickness reflects a balance between the addition of mass to the thermocline via winds in the south, the addi- tion of mass via upwelling from below (pre- sumably minor), and the loss of mass by deep water formation in the north. Gnanadesikan also includes the potentially important effect of eddies in the ACC which tend to drain mass from the thermocline in opposition to the wind effect. The strength of the conveyor in Gnan- adesikan’s scheme is reduced to a simple func- tion of the thermocline thickness and the density difference between thermocline water and deep water.

Instability of the Thermohaline

Circulation

Cooling of the ocean in high latitudes makes polar surface waters denser in relation to warmer waters at lower latitudes. Thus cool- ing contributes to a stronger thermohaline cir- culation. The salinity section through the Atlantic Ocean in figure 1 gives one a superfi- cial impression that haline forces also make a positive contribution to the thermohaline circu- lation. This is actually not true. The cycling of fresh water between the ocean and atmo- sphere (the hydrological cycle) results in a net addition of fresh water to high latitudes which reduces the density of polar surface waters. Thus, the haline contribution to the thermoha- line circulation is nearly always in opposition to the thermal forcing. The earth’s hydrologi- cal cycle is expected to become more vigorous in the future with global warming. This is ex- pected to weaken the thermohaline circulation in a way which could be fairly abrupt and un- predictable.

North Atlantic Deep Water is salty because the water in the upper part of the con- veyor flows through zones of intense evapo- ration in the tropics and subtropics. If the rate at which new deep water is forming is rela- tively high, as it seems to be at the present time, the sinking water removes much of the fresh water added in high latitudes and carries it into the interior. The added fresh water in this case dilutes the salty water being carried into the deep-water formation areas but does not erase the effect of evaporation in low lati- tudes. Thus, NADW remains fairly salty and is able to export fresh water from the Atlantic basin. (The key factor here is that NADW at depth is actually a bit fresher than the water flowing northward). If the rate of deep-water formation is rela- tively low, however, or the hydrological cycle is fairly strong, the export of fresh water via NADW is reduced and the fresh water added in high latitudes tends to accumulate. There seems to be a critical threshold of fresh water input for maintaining the Atlantic conveyor. If the fresh water input is close to the threshold, the overturning becomes unstable and may oscillate over time. If the fresh water input exceeds the threshold, the haline effect over- whelms the thermal effect and the thermo- ha- line circulation stops dead. Manabe and Stouffer have projected that a four-fold increase in atmospheric CO 2 would increase the hydrological cycle sufficiently that the Atlantic conveyor might collapse. This would lead to a substantially deeper thermo- cline and a shift in the heat exchange between the hemispheres. It would also lead to a dras- tic reduction in the rate at which nutrients are supplied to the upper ocean biota and a reduc- tion in the oxygen content of deep water.

Further Reading

Broecker, W. S., The Great Ocean Conveyor, Oceanography, 4, 79-89, 1991.