globalchange  > 气候变化事实与影响
DOI: doi:10.1038/nclimate2132
论文题名:
Cessation of deep convection in the open Southern Ocean under anthropogenic climate change
作者: Casimir de Lavergne
刊名: Nature Climate Change
ISSN: 1758-1387X
EISSN: 1758-7507
出版年: 2014-03-02
卷: Volume:4, 页码:Pages:278;282 (2014)
语种: 英语
英文关键词: Physical oceanography
英文摘要:

In 1974, newly available satellite observations unveiled the presence of a giant ice-free area, or polynya, within the Antarctic ice pack of the Weddell Sea, which persisted during the two following winters1. Subsequent research showed that deep convective overturning had opened a conduit between the surface and the abyssal ocean, and had maintained the polynya through the massive release of heat from the deep sea2, 3. Although the polynya has aroused continued interest1, 2, 3, 4, 5, 6, 7, 8, 9, the presence of a fresh surface layer has prevented the recurrence of deep convection there since 19768, and it is now largely viewed as a naturally rare event10. Here, we present a new analysis of historical observations and model simulations that suggest deep convection in the Weddell Sea was more active in the past, and has been weakened by anthropogenic forcing. The observations show that surface freshening of the southern polar ocean since the 1950s has considerably enhanced the salinity stratification. Meanwhile, among the present generation of global climate models, deep convection is common in the Southern Ocean under pre-industrial conditions, but weakens and ceases under a climate change scenario owing to surface freshening. A decline of open-ocean convection would reduce the production rate of Antarctic Bottom Waters, with important implications for ocean heat and carbon storage, and may have played a role in recent Antarctic climate change.

Antarctic Bottom Water (AABW) is the coldest, densest and most voluminous11 water mass of the world ocean and its shrinking in recent decades12, 13 has been linked to deep ocean heat uptake12, 14. Produced at present on Antarctic continental shelves, AABW is exported northwards to fill the deepest layers of the three oceanic basins and feed the deep branch of the meridional overturning circulation11, 15. In 1928, on the basis of early hydrographic observations, it was suggested16 that open-ocean convection also contributes to the production of AABW, as it does to North Atlantic Deep Water in the Labrador Sea. It was argued that deep convection occurred within the Weddell Gyre, but because of difficulty monitoring the Weddell Sea during austral winter, this contention went unverified until the mid-1970s6.

Microwave observing satellites were first launched in December 1972, providing global observations of sea ice, and soon thereafter revealed the presence of a 250,000-km2 ice-free area within the seasonally ice-covered Weddell Sea1 (Fig. 1a). The huge polynya, located near Maud Rise (65° S, 0°), reappeared during the winters of 1974 to 1976, slowly drifting westward with the background flow1. The polynya was maintained by vigorous convective mixing, whereby the upward flux of relatively warm deep waters supplied enough heat to prevent sea ice formation1, 2, 3. Heat loss at the surface drove cooling to depths of about 3,000 m, producing new deep waters3 that could have fed the observed surge in Southern Ocean AABW volume during the following decade13. Together with the inference from hydrographic data of a Weddell convective event circa 19603, these observations confirm that deep convection in the open Weddell Sea has been a significant mode of AABW ventilation5, 6. However, following 1976, no similar polynya has been observed. The continuing quiescence over the past 37 of 41 available years of satellite observation makes it tempting to assume that deep convection in the open Southern Ocean occurs rarely, with little global consequence. Here we propose, instead, that deep convection was more common in the pre-industrial state, but that the hydrological changes associated with global warming17, 18, 19 are now suppressing this convective activity.

Figure 1: Spatial pattern of Southern Ocean deep convection in observations and models.
Spatial pattern of Southern Ocean deep convection in observations and models.

a, Observed 1974–1976 mean September sea ice concentration (%) from Nimbus-5 ESMR Polar Gridded Sea Ice Concentrations30 delineating the Weddell Polynya extent. b, September mixed layer depth (shading) and 25%, 50% and 75% September sea ice concentration contours (grey lines) in the MPI-ESM-LR model, averaged over pre-industrial control years during which the convection area exceeds half of its overall maximum. c, The same as in b, but for the HadGEM2-ES model. Deep mixed layers, coinciding with anomalously low sea ice concentrations, are found over an area of comparable size to the Weddell Polynya and in a similar location. The spatial pattern of deep convection in all convective models is presented in Supplementary Fig. 1.

Observational record.

All profiles were taken from the latest version of the BLUELink Ocean Archive28. We also used salinity and temperature monthly climatologies from the CSIRO (Commonwealth Scientific and Industrial Research Organisation) Atlas of Regional Seas28 (CARS 2009), which is built from the same database. We first selected profiles with sufficient depth coverage for which the 0–1,500 m dynamic height is less than the CARS monthly minimum within Drake Passage (5.1–5.7 dyn dm). This dynamic height criterion allows a focus on profiles south of the Antarctic Circumpolar Current. To optimize the use of the relatively sparse data, an equivalent 0–500 m dynamic height threshold (2.2–2.6 dyn dm) was determined using the strong relationship between 0–1,500 m and 0–500 m dynamic heights, as obtained from a simple linear regression. This enabled us to include additional profiles covering only the 0–500 m depth range.

Salinity, in situ temperature and surface-referenced potential density were averaged over 0–100 m and 100–200 m for every profile. The derivatives of potential density with respect to salinity and temperature are also calculated and averaged over 0–200 m to obtain the individual contributions of salinity and temperature to the vertical density gradient. To avoid the aliasing of spatial and seasonal variability, we subtract the appropriate monthly gridded (0.5° × 0.5°) CARS atlas values from the 0–100 m and 100–200 m profile means. Yearly anomalies are then constructed as area-weighted averages over the sampled monthly, 0.5° × 0.5° bins. We finally add the CARS climatological annual mean to the yearly anomalies to obtain the annual mean time series of Fig. 2. Standard errors are obtained from the standard deviation across sampled bins within each year (July to June), scaled by the square root of their number. Note that years with less than 20 sampled bins were discarded, resulting in quasi-continuous coverage from 1956 onwards.

CMIP5 archive.

We analysed all CMIP5 models for which ‘piControl’, ‘historical’ and ‘rcp85’ experiments with potential temperature, salinity and sea ice concentration monthly fields were available. Model outputs were downloaded from the Program for Climate Model Diagnosis and Intercomparison data portal24 at http://pcmdi9.llnl.gov/esgf-web-fe/. A list of all analysed models along with details on their numerical treatment of oceanic convection is given in Supplementary Table 3.

Pre-industrial control runs use fixed boundary conditions, held at the 1860 level. Historical experiments include the full range of natural and anthropogenic forcings, consistent with observations. RCP8.5 corresponds to a high-emissions scenario that includes time-varying greenhouse gas, stratospheric ozone, anthropogenic aerosols, and solar forcings. Under RCP8.5, the radiative forcing relative to pre-industrial conditions rises continuously to reach about 8.5 W m−2 in 2100, and increases for another 150 years in the 22–23 century extension before stabilizing at approximately 12 W m−2.

Only one run (r1i1p1) per model and per experiment was considered. Available pre-industrial control simulations had lengths ranging between 240 and 1,000 years. Historical (1860–2005) and RCP8.5 (2006–2100 or 2006–2300) outputs were concatenated to obtain the climate change time series. Nine models had extended RCP8.5 integrations (2006–2300).

CMIP5 model output analysis.

From monthly salinity and temperature fields, we determined mixed layer depths as the depth z at which σθ(z) − σθ(10m) = 0.03kgm−3, where σθ is the potential density referenced to the surface29. This criterion was found to provide a robust diagnostic of modelled mixed layers in the southern polar regions as deep mixed layers were observed to coincide closely with positive sea surface temperature and sea surface salinity anomalies, as well as low sea ice concentration anomalies, signalling the strong vertical flux of heat and salt. Convection area is defined as the total surface area south of 55° S with a September mixed layer depth exceeding 2,000 m. This depth criterion ensures that only deep convection in the open ocean is taken into account. Convection areas are relatively insensitive to the chosen depth threshold because deep convective overturning was generally observed to extend over most of the water column. September was chosen because maximum convection depths and areas are commonly found at the end of austral winter.

Convective years are defined as years during which the convection area is larger than 100,000 km2 (about a third of the observed 1970s Weddell Polynya area). The 11 models featuring no significant open ocean convection are those that do not simulate any convection area above this threshold (with the exception of MIROC-ESM, which convects during the last 100 years of its 630-year-long control run as a result of drifting deep Southern Ocean densities, but exhibits no convective activity during the historical period; see Supplementary Table 2).

  1. Carsey, F. D. Microwave observation of the Weddell Polynya. Mon. Weath. Rev. 108, 20322044 (1980).
  2. Martinson, D. G., Killworth, P. D. & Gordon, A. L. A convective model for the Weddell Polynya. J. Phys. Oceanogr. 11, 466488 (1981).
  3. Gordon, A. L. Weddell deep water variability. J. Mar. Res. 40, 199217 (1982).
  4. Parkinson, C. L. On the development and cause of the Weddell Polynya in a sea ice simulation. J. Phys. Oceanogr. 13, 501511 (1983).
  5. Killworth, P. D. Deep convection in the world ocean. Rev. Geophys. 21, 126 (1983).
  6. Martinson, D. G. in Deep Convection and Deep Water Formation in the Oceans (eds Chu, P. C. & Gascard, J. C.) 3752 (Elsevier Oceanography Series, 1991).
  7. Holland, D. M. Explaining the Weddell Polynya—a large ocean eddy shed at Maud Rise. Science 292, 16971700 (2001).
  8. Gordon, A. L., Visbeck, M. & Comiso, J. C. A possible link between the Weddell Polynya and the Southern Annular Mode. J. Clim. 20, 25582571 (2007).
  9. Hirabara, M., Tsujino, H., Nakano, H. & Yamanaka, G. Formation mechanism of the Weddell Sea Polynya and the impact on the global abyssal ocean. J. Oceanogr. 68, 771796 (2012).
  10. Heuzé, C., Heywood, K. J., Stevens, D. P. & Ridley, J. K. Southern Ocean bottom water characteristics in CMIP5 models. Geophys. Res. Lett. 40, 14091414 (2013).
URL: http://www.nature.com/nclimate/journal/v4/n4/full/nclimate2132.html
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资源类型: 期刊论文
标识符: http://119.78.100.158/handle/2HF3EXSE/5208
Appears in Collections:气候变化事实与影响
科学计划与规划
气候变化与战略

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Casimir de Lavergne. Cessation of deep convection in the open Southern Ocean under anthropogenic climate change[J]. Nature Climate Change,2014-03-02,Volume:4:Pages:278;282 (2014).
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