- •Preface
- •1 A Voyage of Discovery
- •1.2 Goals
- •1.3 Organization
- •1.4 The Big Picture
- •1.5 Further Reading
- •2 The Historical Setting
- •2.2 Eras of Oceanographic Exploration
- •2.3 Milestones in the Understanding of the Ocean
- •2.4 Evolution of some Theoretical Ideas
- •2.5 The Role of Observations in Oceanography
- •2.6 Important Concepts
- •3 The Physical Setting
- •3.1 Ocean and Seas
- •3.2 Dimensions of the ocean
- •3.3 Sea-Floor Features
- •3.4 Measuring the Depth of the Ocean
- •3.5 Sea Floor Charts and Data Sets
- •3.6 Sound in the Ocean
- •3.7 Important Concepts
- •4.1 The Earth in Space
- •4.2 Atmospheric Wind Systems
- •4.3 The Planetary Boundary Layer
- •4.4 Measurement of Wind
- •4.5 Calculations of Wind
- •4.6 Wind Stress
- •4.7 Important Concepts
- •5 The Oceanic Heat Budget
- •5.1 The Oceanic Heat Budget
- •5.2 Heat-Budget Terms
- •5.3 Direct Calculation of Fluxes
- •5.4 Indirect Calculation of Fluxes: Bulk Formulas
- •5.5 Global Data Sets for Fluxes
- •5.6 Geographic Distribution of Terms
- •5.7 Meridional Heat Transport
- •5.8 Variations in Solar Constant
- •5.9 Important Concepts
- •6.2 Definition of Temperature
- •6.4 The Oceanic Mixed Layer and Thermocline
- •6.5 Density
- •6.6 Measurement of Temperature
- •6.7 Measurement of Conductivity or Salinity
- •6.8 Measurement of Pressure
- •6.10 Light in the Ocean and Absorption of Light
- •6.11 Important Concepts
- •7.1 Dominant Forces for Ocean Dynamics
- •7.2 Coordinate System
- •7.3 Types of Flow in the ocean
- •7.4 Conservation of Mass and Salt
- •7.5 The Total Derivative (D/Dt)
- •7.6 Momentum Equation
- •7.7 Conservation of Mass: The Continuity Equation
- •7.8 Solutions to the Equations of Motion
- •7.9 Important Concepts
- •8.2 Turbulence
- •8.3 Calculation of Reynolds Stress:
- •8.4 Mixing in the Ocean
- •8.5 Stability
- •8.6 Important Concepts
- •9 Response of the Upper Ocean to Winds
- •9.1 Inertial Motion
- •9.2 Ekman Layer at the Sea Surface
- •9.3 Ekman Mass Transport
- •9.4 Application of Ekman Theory
- •9.5 Langmuir Circulation
- •9.6 Important Concepts
- •10 Geostrophic Currents
- •10.1 Hydrostatic Equilibrium
- •10.2 Geostrophic Equations
- •10.3 Surface Geostrophic Currents From Altimetry
- •10.4 Geostrophic Currents From Hydrography
- •10.5 An Example Using Hydrographic Data
- •10.6 Comments on Geostrophic Currents
- •10.7 Currents From Hydrographic Sections
- •10.8 Lagrangian Measurements of Currents
- •10.9 Eulerian Measurements
- •10.10 Important Concepts
- •11.2 Western Boundary Currents
- •11.4 Observed Surface Circulation in the Atlantic
- •11.5 Important Concepts
- •12 Vorticity in the Ocean
- •12.2 Conservation of Vorticity
- •12.4 Vorticity and Ekman Pumping
- •12.5 Important Concepts
- •13.2 Importance of the Deep Circulation
- •13.3 Theory for the Deep Circulation
- •13.4 Observations of the Deep Circulation
- •13.5 Antarctic Circumpolar Current
- •13.6 Important Concepts
- •14 Equatorial Processes
- •14.1 Equatorial Processes
- •14.6 Important Concepts
- •15 Numerical Models
- •15.2 Numerical Models in Oceanography
- •15.3 Global Ocean Models
- •15.4 Coastal Models
- •15.5 Assimilation Models
- •15.6 Coupled Ocean and Atmosphere Models
- •15.7 Important Concepts
- •16 Ocean Waves
- •16.1 Linear Theory of Ocean Surface Waves
- •16.2 Nonlinear waves
- •16.3 Waves and the Concept of a Wave Spectrum
- •16.5 Wave Forecasting
- •16.6 Measurement of Waves
- •16.7 Important Concepts
- •17 Coastal Processes and Tides
- •17.1 Shoaling Waves and Coastal Processes
- •17.2 Tsunamis
- •17.3 Storm Surges
- •17.4 Theory of Ocean Tides
- •17.5 Tidal Prediction
- •17.6 Important Concepts
- •References
13.5. ANTARCTIC CIRCUMPOLAR CURRENT |
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7.Fluorocarbons (Freon used in air conditioning) have been recently injected into atmosphere. They can be measured with very great sensitivity, and they are being used for tracing the sources of deep water.
8.Sulphur hexafluoride SF6 can be injected into sea water, and the concentration can be measured with great sensitivity for many months.
Each tracer has its usefulness, and each provides additional information about the flow.
North Atlantic Meridional Overturning Circulation The great importance of the meridional overturning circulation for European climate has led to programs to monitor the circulation. The Rapid Climate Change/Meridional Overturning Circulation and Heat Flux Array rapid/mocha deployed an array of instruments that measured bottom pressure plus temperature and salinity throughout the water column at 15 locations along 24◦N near the western and eastern boundaries and on either side of the mid-Atlantic ridge beginning in 2004 (Church, 2007). At the same time, flow of the Gulf Stream was measured through the Strait of Florida, and wind stress, which gives the Ekman transports, was measured along 24◦N by satellite instruments. The measurements show that transport across 24◦N was zero, within the accuracy of the measurements, as expected. The one-year average of the Meridional Overturning Circulation was 18.7 ± 5.6 Sv, with variability ranging from 4.4 to 35.3 Sv. Accuracy of the measurement was ± 1.5 Sv.
13.5Antarctic Circumpolar Current
The Antarctic Circumpolar Current is an important feature of the ocean’s deep circulation because it transports deep and intermediate water between the Atlantic, Indian, and Pacific Ocean, and because Ekman pumping driven by westerly winds is a major driver of the deep circulation. Because it is so important for understanding the deep circulation in all ocean, let’s look at what is known about this current.
A plot of density across a line of constant longitude in the Drake Passage (figure 13.12) shows three fronts. They are, from north to south: 1) the Subantarctic Front, 2) the Polar Front, and 3) the Southern acc Front. Each front is continuous around Antarctica (figure 13.13). The plot also shows that the constant-density surfaces slope at all depths, which indicates that the currents extend to the bottom.
Typical current speeds are around 10 cm/s with speeds of up to 50 cm/s near some fronts. Although the currents are slow, they transport much more water than western boundary currents because the flow is deep and wide. Whitworth and Peterson (1985) calculated transport through the Drake Passage using several years of data from an array of 91 current meters on 24 moorings spaced approximately 50 km apart along a line spanning the passage. They also used measurements of bottom pressure measured by gauges on either side of the passage. They found that the average transport through the Drake Passage was 125 ±11 Sv, and that the transport varied from 95 Sv to 158 Sv. The maximum transport tended to occur in late winter and early spring (figure 13.14).
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CHAPTER 13. DEEP CIRCULATION IN THE OCEAN |
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Figure 13.12 Cross section of neutral density across the Antarctic Circumpolar Current in the Drake Passage from the World Ocean Circulation Experiment section A21 in 1990. The current has three streams associated with the three fronts (dark shading): sf = Southern acc Front, pf = Polar Front, and saf = Subantarctic Front. Hydrographic station numbers are given at the top, and transports are relative to 3,000 dbar. Circumpolar deep water is indicated by light shading. Data from Alex Orsi, Texas A&M University.
Because the antarctic currents reach the bottom, they are influenced by topographic steering. As the current crosses ridges such as the Kerguelen Plateau, the Pacific-Antarctic Ridge, and the Drake Passage, it is deflected by the ridges.
The core of the current is composed of Circumpolar Deep Water, a mixture of deep water from all ocean. The upper branch of the current contains oxygen-poor water from all ocean. The lower (deeper) branch contains a core of high-salinity water from the Atlantic, including contributions from the north Atlantic deep water mixed with salty Mediterranean Sea water. As the di erent water masses circulate around Antarctica they mix with other water masses with similar density. In a sense, the current is a giant ‘mix-master’ taking deep water from each ocean, mixing it with deep water from other ocean, and then redistributing it back to each ocean (Garabato et al, 2007).
13.5. ANTARCTIC CIRCUMPOLAR CURRENT |
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Figure 13.13 Distribution Subantarctic Front; PF: Shaded areas are shallower
of fronts around Antarctica: STF: Subtrobical Front; SAF: Polar Front; SACC: Southern Antarctic Circumpolar Front. than 3 km. From Orsi (1995).
Transport (10 6 m 3 s - 1 )
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Figure 13.14 Variability of the transport in the Antarctic Circumpolar Current as measured by an array of current meters deployed across the Drake Passage. The heavier line is smoothed, time-averaged transport. From Whitworth (1988).
232 |
CHAPTER 13. DEEP CIRCULATION IN THE OCEAN |
The coldest, saltiest water in the ocean is produced on the continental shelf around Antarctica in winter, mostly from the shallow Weddell and Ross seas. The cold salty water drains from the shelves, entrains some deep water, and spreads out along the sea floor. Eventually, 8–10 Sv of bottom water are formed (Orsi, Johnson, and Bullister, 1999). This dense water then seeps into all the ocean basins. By definition, this water is too dense to cross through the Drake Passage, so it is not circumpolar water.
The Antarctic currents are wind driven. Strong west winds with maximum speed near 50◦S drive the currents (see figure 4.2), and the north-south gradient of wind speed produces convergence and divergence of Ekman transports. Divergence south of the zone of maximum wind speed, south of 50◦S leads to upwelling of the Circumpolar Deep Water. Convergence north of the zone of maximum winds leads to downwelling of the Antarctic intermediate water. The surface water is relatively fresh but cold, and when they sink they define characteristics of the Antarctic intermediate water.
The position of the circumpolar current relative to the maximum of the westerly winds influences the meridional overturning circulation and climate. North of the maximum, Ekman transports converge, pushing water downward into the Antarctic Intermediate Water north of the Polar Front. South of the maximum winds, Ekman transports diverge, pulling Circumpolar Atlantic Deep Water to the surface south of the Polar Front, which helps drive the deep circulation (figure 13.10). When the maximum winds are further from the pole, less deep water is pulled upward, and the deep circulation is weak, as it was during the last ice age. As the earth warmed after the ice age, the maximum winds shifted south. The winds were more aligned with the Circumpolar Current, and they pulled more deep water to the surface. Since 1960, the winds have strengthened and shifted southward, further strengthening Circumpolar Current and the deep circulation Toggweiler and Russell, 2008).
Because wind constantly transfers momentum to the Antarctic Circumpolar Current, causing it to accelerate, the acceleration must be balanced by drag, and we are led to ask: What keeps the flow from accelerating to very high speeds? Munk and Palmen (1951), suggest form drag dominates. Form drag is due to the current crossing sub-sea ridges, especially at the Drake Passage. Form drag is also the drag of the wind on a fast moving car. In both cases, the flow is diverted, by the ridge or by your car, creating a low pressure zone downstream of the ridge or down wind of the car. The low pressure zone transfers momentum into the solid earth, slowing down the current.
13.6Important Concepts
1.The deep circulation of the ocean is very important because it determines the vertical stratification of the ocean and because it modulates climate.
2.The ocean absorbs CO2 from the atmosphere reducing atmospheric CO2 concentrations. The deep circulation carries the CO2 deep into the ocean temporarily keeping it from returning to the atmosphere. Eventually, however, most of the CO2 must be released back to the atmosphere. But, some
13.6. IMPORTANT CONCEPTS |
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remains in the ocean. Phytoplankton convert CO2 into organic carbon, some of which sinks to the sea floor and is buried in sediments. Some CO2 is used to make sea shells, and it too remains in the ocean.
3.The production of deep bottom waters in the north Atlantic draws a petawatt of heat into the northern hemisphere which helps warm Europe.
4.Variability of deep water formation in the north Atlantic has been tied to large fluctuations of northern hemisphere temperature during the last ice ages.
5.Deep convection which produces bottom water occurs only in the far north Atlantic and at a few locations around Antarctica.
6.The deep circulation is driven by vertical mixing, which is largest above mid-ocean ridges, near seamounts, and in strong boundary currents.
7.The deep circulation is too weak to measure directly. It is inferred from observations of water masses defined by their temperature and salinity and from observation of tracers.
8.The Antarctic Circumpolar Current mixes deep water from the Atlantic, Pacific, and Indian Ocean and redistributes it back to each ocean. The current is deep and slow with a transport of 125 Sv.
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CHAPTER 13. DEEP CIRCULATION IN THE OCEAN |