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An ice-core proxy for Antarctic circumpolar zonal wind intensity

Published online by Cambridge University Press:  14 September 2017

Yuping Yan
Affiliation:
Climate Change Institute, University of Maine, 303 Bryand Global Sciences Center, Orono, ME 04469-5790, USAE-mail: [email protected] National Climate Center, China Meteorological Administration, 46 Zhongguancun Nandajie, Haidian District, Beijing 10081, China
Paul A. Mayewski
Affiliation:
Climate Change Institute, University of Maine, 303 Bryand Global Sciences Center, Orono, ME 04469-5790, USAE-mail: [email protected] Department of Earth Sciences, 5790 Bryand Global Sciences Center, University of Maine, Orono, ME 04469-5790, USA
Shichang Kang
Affiliation:
Climate Change Institute, University of Maine, 303 Bryand Global Sciences Center, Orono, ME 04469-5790, USAE-mail: [email protected] Institute of Tibetan Plateau Research, Chinese Academy of Sciences, 18 Shuangqing Road, Haidian District, Beijing 100085, China
Eric Meyerson
Affiliation:
Climate Change Institute, University of Maine, 303 Bryand Global Sciences Center, Orono, ME 04469-5790, USAE-mail: [email protected] Department of Earth Sciences, 5790 Bryand Global Sciences Center, University of Maine, Orono, ME 04469-5790, USA
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Abstract

Using US National Centers for Environmental Prediction/US National Center for Atmospheric Research re-analysis data, we investigate the relationships between crustal ion (nssCa2+) concentrations from three West Antarctic ice cores, namely, Siple Dome (SD), ITASE00-1 (IT001) and ITASE01-5 (IT015), and primary components of the climate system, namely, air pressure/geopotential height, zonal (u) and meridional (v) wind strength. Linear correlation analyses between nssCa2+ concentrations and both air-pressure and wind fields for the period of overlap between records indicate that the SD nssCa2+ variation is positively correlated with spring circumpolar zonal wind, while IT001 nssCa2+ has a positive correlation with circumpolar zonal wind throughout the year (r > 0.3, p < 0.01). Intensified Southern Westerlies circulation is conducive to transport of more crustal aerosols to both sites. Further correlation analyses between nssCa2+ concentrations from SD and IT001 and atmospheric circulation suggest that the high inland plateau (represented by core IT001) is largely influenced by transport from the upper troposphere. IT015 nssCa2+ is negatively correlated with westerly wind in October and November, suggesting that stronger westerly circulation may weaken the transport of crustal species to IT015. Correlations of nssCa2+ from the three ice cores with the Antarctic Oscillation index are consistent with results developed from the wind-field investigation. In addition, calibration between nssCa2+ concentration and the multivariate El Niño–Southern Oscillation (ENSO) index shows that crustal species transport to IT001 is enhanced during strong ENSO events.

Type
Research Article
Copyright
Copyright © The Author(s) [year] 2005

1. Introduction

Ice-core records provide proxy information on local climate (accumulation and temperature via isotopes of water), regional climate (atmospheric circulation via wind-blown dust and sea salt), climate over hemispheric to global scales (trapped-gas records of carbon dioxide, methane, nitrous oxide and other gases), and conditions beyond the Earth (concentrations of extraterrestrial dust and cosmogenic isotopes). The chemical composition of polar snow and ice reflects the characteristics of the atmospheric pathway transporting the chemistry (e.g. Reference MayewskiMayewski and others, 1997), changes in source emission strength, and post-depositional effects for reversible species (not utilized in this study; e.g. Reference Legrand and MayewskiLegrand and Mayewski, 1997; Reference Wolff, Rankin and RöthlisbergerWolff and others, 2003).

Instrumental climate records are relatively sparse over the Southern Hemisphere and extend back typically <50 years. Glaciochemical proxy data can extend the paleoclimate record back hundreds to thousands of years and also provide a unique resource for examining changes in the sources, pathways and distribution of chemical species in the atmosphere through time (Reference MayewskiMayewski and others, 1993).

The sources of chemical species deposited in polar snow and ice have been summarized in numerous papers (e.g. Reference HerronHerron, 1982; Reference Lyons, Mayewski, Altshuller and LinthurstLyons and Mayewski, 1984; Reference SteffensenSteffensen, 1988; Reference Delmas, Legrand, Oeschger and LangwayDelmas and Legrand, 1989; Reference Shaw, Oeschger and LangwayShaw, 1989; Reference Davidson, Jaffrezo, Mayewski and W.T.Davidson and others, 1992; Reference Mayewski, Spencer, Lyons, Moore and DavidMayewski and others, 1992; Reference Whitlow, Mayewski and HoldsworthWhitlow and others, 1994, Reference Legrand and MayewskiLegrand and Mayewski, 1997; Reference RöthlisbergerRöthlisberger and others, 2002). Calcium in polar snow has two major sources: sea-salt (ss) and crustally derived non-sea-salt (nss) aerosols (Reference MayewskiMayewski, and others, 1997). Increases in crustal source species indicate enhanced atmospheric turbidity, increased aridity in the source area and/or increased exposure of ice-free areas (Reference Mayewski and LyonsMayewski and Lyons, 1982; Reference Mumford and PeelMumford and Peel, 1982). Previous studies suggest that aerosol transport is highly correlated with sea-level pressure (SLP) in Antarctica, Greenland and Asia (Reference Kreutz, Mayewski, Meeker, Twickler, Whitlow and PittalwalaKreutz and others, 1997, Reference Kreutz, Mayewski, Pittalwala, Meeker, Twickler and Whitlow2000; Reference MayewskiMayewski and others, 1997; Reference FischerFischer, 2001; Reference KangKang and others; 2002, Reference Kang, Mayewski, Yan and Qin2003; Reference Meeker and MayewskiMeeker and Mayewski, 2002; Reference Souney, Mayewski, Goodwin, Morgan and van OmmenSouney and others, 2002). This paper focuses on the non sea-salt calcium (nssCa2+ = Ca2+ – (0.038×Na+)) time series from the three ice cores from West Antarctica and investigates the relationships between nssCa2+ and atmospheric circulation using US National Centers for Environmental Prediction (NCEP)/US National Center for Atmospheric Research (NCAR) re-analysis meteorological data.

2. Data

Ice cores recovered from West Antarctica by the United States component of the International Trans-Antarctic Scientific Expedition (US ITASE) and during the Siple Dome project (ITASE 00-1 (IT001), ITASE 01-5 (IT015) and Siple Dome (SD)) were selected for this study (Fig. 1; Table 1). The SD core glaciochemistry was previously reported (Reference Mayewski, Twickler and WhitlowMayewski and others, 1995; Reference Kreutz, Mayewski, Twickler and WhitlowKreutz and others, 1996, Reference Kreutz and Mayewski1999, Reference Kreutz, Mayewski, Pittalwala, Meeker, Twickler and Whitlow2000) and annually dated by Reference KreutzKreutz and others (1999). The other two cores were drilled during the US ITASE West Antarctic traverses of 1999–2001 and analyzed at sub-annual, continuous resolution (Reference KaspariKaspari and others, 2004; Reference DixonDixon and others, 2005). The ITASE cores were processed at an average resolution of ~50 samples m–1. Samples were examined for their major soluble ions (Na+, K+, Mg2+, Ca2+, Cl, NO3 , SO4 2–) using a DX-500 ion chromatograph (IC) coupled to a Gilson ® autosampler. Major cations (Na+, Ca2+, Mg2+ and K+) were determined using a CS-12a column with 25Mm methanesulfonate (MSA) eluent. Antarctic samples may contain dissolved ions at very low concentrations. Detection limits, analytical variability and blank measurements are important for establishing confidence in reporting low values. Based on several tests of multiple runs, the IC detection limits for Na+ and Ca2+ are 0.1 ppb, with analytical variability of 0.17 ppb for Na+ and 0.22 ppb for Ca2+. Blank concentrations are 0 ppb. Also crucial to achieving low detection limits are ice-handling techniques. During collection, core sections are minimally handled, and personnel wear plastic gloves and face masks. Core processing is performed using a continuous melting system which minimizes exposure of the samples to contamination. Further, IC analysis does not require the addition of reagents or dilution with water.

Fig. 1. Location map for the three core sites in West Antarctica.

Table 1. Ice cores in West Antarctica

Cores are annually dated by matching seasonal peaks from each of the ion time series (Reference DixonDixon and others, 2005). A ‘core-chemistry’ year is defined by a winter–spring peak in Na+, K+, Mg2+, Ca2+ and Cl combined with spring–summer peaks in both NO3 and xsSO4 2– in accord with the seasonal timing identified by previous research (e.g. Reference Whitlow, Mayewski and HoldsworthWhitlow and others, 1994; Reference Wagenbach, Wolff and BalesWagenbach, 1996; Reference Legrand and MayewskiLegrand and Mayewski, 1997; Reference Kreutz and MayewskiKreutz and Mayewski, 1999; Reference SommerSommer and others, 2000).

Mean concentrations of major ions in the three ice cores are shown in Table 2. Na+ and Cl concentrations are an order of magnitude higher than K+, Mg2+ and Ca2+ values, indicating the strong marine impacts on the region. Iterative testing of potential conservative sea-salt species following techniques described by Reference O’Brien, Mayewski, Meeker, Meese, Twickler and WhitlowO’Brien and others (1995) shows that Na+ is a conservative indicator of sea salt and that, as a consequence, most of the Ca2+ in IT001 and IT015 (87% and 83.3%, respectively) is of crustal origin.

Table 2. Summary of ion chemistry: average concentrations (ppb) for the overlap period. Values in parentheses are % of non-sea-salt calcium relative to total calcium

Numerical analyses involving European Centre for Medium-Range Weather Forecasts (ECMWF) datasets have played an important role in a variety of atmospheric studies in the high southern latitudes (e.g. Tremberth and Solomon, 1994; Reference Bromwich, Robasky, Cullather and van WoertBromwich and others, 1995, Reference Bromwich, Rogers, Kållberg, Cullather, White and Kreutz2000; Reference Budd, Reid and MintyBudd and others, 1995; Reference Cullather, Bromwich and van WoertCullather and others, 1996; Reference Reijmer, van den Broeke and ScheeleReijmer and others, 2002). ECMWF analyses are generally found to offer a reasonable depiction of broad-ranging atmospheric circulation, pressure-level fields and surface winds when compared to Antarctic automatic weather station (AWS) and ship observations (Reference Cullather, Bromwich and GrumbineCullather and others, 1997). However, a major obstacle to using operationally analyzed data for climate studies is the effect of alterations in the data assimilation system on the climatic ensemble of analyses (Reference TrenberthTrenberth, 1992). An alternative is to use NCEP/NCAR re-analysis data (Reference TrenberthTrenberth, 1995; Reference KalnayKalnay and others, 1996; Reference Simmonds and KeaySimmonds and Keay, 2000). The NCEP/NCAR analyses were obtained by assimilating past data into a frozen state-of-the-art analysis/ forecast model system. The database was enhanced with many sources of observations that were not available in real-time operations, and the product is regarded as one of the most complete, physically consistent meteorological datasets (Reference Simmonds and KeaySimmonds and Keay, 2000). The NCEP/NCAR re-analysis archive is provided by the National Oceanic and Atmospheric Administration–Cooperative Institute for Research in Atmospheric Sciences (NOAA–CIRES) Climate Diagnostics Center, Boulder, CO, USA (http://www.cdc.noaa.gov). It contains monthly averaged analyses (reported every 6 hours from 0000 UTC) on a 2.5˚ latitude–longitude grid, at 17 standard pressure levels, as well as surface- and boundary-level variables for the period 1948–2002.

The Antarctic Oscillation (AAO) is the dominant pattern of non-seasonal tropospheric circulation variations south of 20˚ S, and is characterized by pressure anomalies of one sign centered in the Antarctic, and of the opposite sign centered close to 40–50˚ S. The AAO is also referred to as the Southern Annular Mode. It is defined as the leading principal component of the 850 hPa geopotential height anomalies south of 20˚ S (Reference Thompson and WallaceThompson and Wallace, 2000).

To investigate potential associations between crustal species concentrations and atmospheric circulation, we use the available NCEP/NCAR instrumented/modeled meteorological data, namely, zonal (u) and meridional (v) wind, and geopotential height, as well as AAO to compare with nssCa2+ from three ice cores.

3. Results and Discussion

3.1. Relationships between SD nssCa2+ and atmospheric circulation, 1948–95

The input timing of marine aerosols (ssNa+) to SD is from September to November (SON; Reference Kreutz, Mayewski, Pittalwala, Meeker, Twickler and WhitlowKreutz and others, 2000). Comparison of nssCa2+ with ssNa+ concentrations at SD over the last 1000 years indicates the same inputting time for the two species. Seasonal variations of the two species over the last 20 years are shown in Figure 2, and indicate similar trends. The long-term (1948–95) seasonal mean of the 850 hPa zonal wind field is characterized by circumpolar westerly circulation (Fig. 3a). Stronger zonal winds (>12ms–1) occur over the southeast and southwest sectors of the Indian Ocean. The positive correlation between seasonal (SON) mean 850 hPa zonal wind and SD nssCa2+ concentration (Fig. 3b) is significant (at the 95% confidence level) in the belt of westerly circulation, suggesting that strong westerly winds are conducive to transport of crustal aerosols to SD. Correlation analyses at higher levels in the atmosphere (500 hPa) reveal a similar region of westerly wind influence (Fig. 3c). Significantly correlated regions reduce in size or disappear at this level, even though wind speeds increase by 6–10ms–1 (Fig. 3c and d), indicating that the transport of crustal aerosols to SD is mostly influenced by the lower-tropospheric circulation. Reference CarletonCarleton (1989) notes that the belt of westerlies in the high-latitude Southern Hemisphere includes traveling wave cyclones, which originate in the lower middle latitudes, move poleward and intensify and stagnate along the coast of Antarctica in four general locations (Amundsen Sea, Weddell Sea, southeast and southwest Indian Ocean). These wave cyclones could carry not only heat and moisture poleward (Reference RogersRogers, 1983), but also crustal dust at the same time.

Fig. 2. A recent 20 year section of seasonal variations of sea-salt aerosol (ssNa+) and nssCa2+ concentrations at SD.

Fig. 3. Seasonal mean 850 hPa zonal wind (a) and its spatial correlation patterns with SD nssCa2+ (b), for the period 1948–95, plotted as correlation coefficients. (c, d) Same as (a) and (b) respectively, but for 500 hPa zonal wind.

The zonal anomalies of seasonal mean geopotential height at 500 hPa in SON (Fig. 4a) are characterized by a sharp gradient (60–150m geopotential height) in the South Pacific and the southeast and southwest of the Indian Ocean in the 45–65˚ S region (gradients are smaller at lower levels). The western ridge of increased geopotential height creates a west-to-east pressure gradient that intensifies winds over the southwest and southern sectors of the Indian Ocean (Fig. 4b). These winds could deliver crustal aerosols from South America and South Africa to the West Antarctic atmosphere as demonstrated by difference fields for the seasonal u component in SON at 500 hPa (Fig. 4b). Westerly flow decreases (by 4–6ms–1) in the South Pacific 45–60˚ S region and increases (by 4–6ms–1) at the same latitude in the south Indian Ocean, as well as in the Ross Sea region (zonal wind velocity differences at lower levels are smaller). Crustal aerosols are spiraled into West Antarctica by these strong westerly winds. Comparison of the differences in zonal wind patterns with the correlation patterns (Fig. 3b and d) verifies the similarity.

Fig. 4. Zonal anomalies (minus zonal mean) of seasonal mean geopotential height (a) and 500 hPa zonal wind (b) in the Southern Hemisphere during SON.

There is also a large region of low geopotential height around the Ross Sea (Fig. 4a), consistent with the strong westerly winds in this area (Fig. 4b). The Ross Sea area is the average center of the circumpolar vortex. Crustal aerosol is transported from the coast to the vicinity of SD under the influence of cyclonic storms in the Ross Sea.

The foregoing suggests that lower-tropospheric transport is more important than that at higher levels and the region of maximum zonal wind is around 608 S. Reference Simmonds and KeaySimmonds and Keay (2000) noted that the axis of maximum Southern Hemisphere (SH) cyclogenesis lies at, or to the south of, 60˚ S. The lower-level (850 hPa) seasonal zonal mean wind at 60˚ S during SON is significantly correlated with nssCa2+ concentration at SD (r = 0.38, p < 0.005; r = 0.33, p < 0.01 for the period since 1968; Fig. 5a). From 1958 to 1967, however, the 850 hPa seasonal zonal mean wind at 60˚ S has a weakly negative correlation with SD nssCa2+ concentration, a correlation that does not occur at 500 hPa atmosphere. The reason for this needs further work. It may be that the atmospheric boundary layer is easily affected by local climate when the circumpolar vortex is weak. In- and out-of-phase relationships between climate variables have been identified in previous Antarctic climate studies (e.g. Reference Cullather, Bromwich and van WoertCullather and others, 1996).

Fig. 5. Variation of SD nssCa2+ concentration and 850 hPa zonal mean wind at 60˚ S (a), and July AAO (b), for the period 1948–2002. r is the correlation coefficient.

SON seasonal mean meridional wind velocities are much smaller than zonal wind velocities and there is no apparent correlation between nssCa2+ and meridional wind. Also the correlation pattern is irregular. Therefore, the correlation between meridional circulation and nssCa2+ at SD is not significant.

Further analysis shows that nssCa2+ from SD is also correlated with monthly AAO (June–October; average r = 0.34, p < 0.01 for the period 1948–95), with the most significant correlations occurring in July (r = 0.43, p < 0.005) (Fig. 5b). This result is consistent with Reference HarrisHarris’ (1992) work, which indicates that the most vigorous long-range transport to the South Pole occurs from July through October.

3.2. Relationships between IT001 nssCa2+ and atmospheric circulation, 1948–2002

Generally the IT001 is little affected by the marine boundary atmosphere due to its high elevation (Tables 1 and 2). Most of the IT001 Ca2+ originates from continental source dust (about 87%; Table 2). There is no obvious seasonal variation for nssCa2+ concentration at IT001. It is positively correlated with zonal wind in circumpolar areas throughout the year, especially at higher atmospheric levels (e.g. mid- and upper troposphere), suggesting that the nssCa2+ in IT001 is transported through the mid- and upper troposphere (r > 0.3, p < 0.01). The influence of westerly circulation on the circumpolar areas is apparent throughout the year (only July is shown in Fig. 6). IT001 nssCa2+ has the highest mean concentration (6.0 ppb) of the three ice cores. The elevation of IT001 is ~1171m higher than that of SD, and the nssCa2+ is probably transported over long distances by westerly circulation in the mid- to upper troposphere throughout the year.

Fig. 6. Spatial correlation pattern of IT001 nssCa2+ concentration with 500 hPa zonal mean wind (only July is shown) for the period 1948–2002, plotted as correlation coefficients.

Since upper-tropospheric westerly circulation is significantly correlated with the nssCa2+ at IT001, we compare the annually averaged 500 hPa zonal mean wind at 60˚ S with nssCa2+ concentrations. In general, variations in nssCa2+ are consistent with zonal mean wind at 60˚ S (r = 0.44, p < 0.001; Fig. 7a). Investigation of the relationship between nssCa2+ concentration and AAO indicates a significant positive correlation between the two time series for most of the year, except January when westerly flow is weakest and wind speed is lowest. The average correlation coefficient for 11 months is 0.36 (p < 0.005). The correlation in July and August is the most significant, with an r value of 0.48 and 0.49, respectively (p < 0.001) (only July is shown in Fig. 7b). This agrees well with the correlation between zonal wind and nssCa2+.

Fig. 7. Variation of IT001 nssCa2+ concentration and 500 hPa zonal mean wind at 60˚ S (a), and AAO (only July is shown) (b), for the period 1948–2002. r is the correlation coefficient.

Investigation of the influence of meridional wind on nssCa2+ concentration at IT001 shows no distinct correlation.

3.3. Relationships between IT015 nssCa2+ and atmospheric circulation, 1948–2001

NssCa2+ concentration in IT015 is close to that from IT001 and higher than that from SD (Table 2). The negative correlation between IT015 nssCa2+ concentration and zonal wind is significant (p < 0.05) at higher levels (700–300 hPa) in October and November. The best-correlated regions are the South Pacific and South America, and the southwest Indian Ocean (only November is shown in Fig. 8). Correlation investigations at different pressure levels indicate a more significant relationship when the atmospheric layer is higher. A negative correlation is also found between the nssCa2+ and AAO, and the most significantly correlated period is June–October (average r = –0.27, p < 0.025), especially October (r = –0.38, p < 0.005) when winds are strongest (Fig. 9). This negative correlation indicates that stronger westerly circulation does not favor transport of dust aerosols to IT015.

Fig. 8. Spatial correlation pattern of IT015 nssCa2+ concentration with 500 hPa zonal mean wind (only November is shown) for the period 1948–2001, plotted as correlation coefficients.

Fig. 9. Variation of IT015 nssCa2+ concentration and October AAO for the period 1948–2002. r is the correlation coefficient.

The reason for the negative correlation is unclear but may be related to high-latitude blocking on seasonal scales. This may impact IT015 differently from IT001 and SD because IT015 is significantly eastward of SD and IT001. Persistent, slow-moving anticyclones can interrupt regional weather sequences by ‘blocking’ the normal passage of cyclonic disturbances (Reference RexRex, 1950a, Reference Rexb; Reference Trenberth and MoTrenberth and Mo, 1985). Studies by Reference Van LoonVan Loon (1956) and Reference LejenäLejenä s (1984) suggest that the highest frequency of SH blocking is in the New Zealand– southwest Pacific region, with secondary maxima east of South America and in the southwest Indian Ocean. Reference SinclairSinclair (1996) points out that anticyclones poleward of 50˚ S are related to an anomalous breakdown of the westerlies in regions southeast of Australia, New Zealand, South America and Africa that are especially prone to rapid anticyclone genesis. More persistent and intense blocking is largely confined to two regions in the South Pacific: southeast of New Zealand and west of South America (Reference SinclairSinclair, 1996). Regions of significant negative correlation between IT015 nssCa2+ and atmospheric circulation are included in the blocking areas suggested by Reference Van LoonVan Loon (1956), Reference LejenäLejenäs (1984) and Reference SinclairSinclair (1996).

3.4. Connections between ENSO and nssCa2+

Several studies have demonstrated a link between El Niño– Southern Oscillation (ENSO) and high-southern-latitude meteorology. Reference Newell, Chiu, Ebisuzaki, Navato and SelkirkNewell and others (1981) speculated that possible high-latitude forcing of the Southern Oscillation could be achieved by atmospheric forcing of the Antarctic circumpolar current. More recent research has focused on the role of South Pacific atmospheric double jet variability in the southward propagation of the ENSO signal (Reference Smith and BromwichSmith and Bromwich, 1994; Reference Smith, Bromwich and ChenSmith and others, 1995; Reference Chen, Smith and BromwichChen and others, 1996). On the basis of its observed periodicity, Reference White and PetersonWhite and Peterson (1996) speculate that initiation of the Antarctic Circumpolar Wave (ACW) is associated with ENSO activity in the equatorial Pacific, possibly through an atmospheric teleconnection with higher southern latitudes. Evidence of links to lower latitudes has been discovered through correlations between ENSO and moisture convergence in a sector (75–90˚ S, 120–180˚ W) of West Antarctica (Reference Cullather, Bromwich and van WoertCullather and others 1996). The nature of this teleconnection to tropical latitudes is unclear and its existence is still debated (Reference Genthon and KrinnerGenthon and Krinner, 1998; Reference Bromwich, Rogers, Kållberg, Cullather, White and KreutzBromwich and others 2000). It may relate to changes in position and intensity of the Amundsen Sea low, as well as other changes in atmospheric circulation over the Antarctic Plateau as demonstrated by previous ice-core studies (Reference Meyerson, Mayewski, Kreutz, Meeker, Whitlow and TwicklerMeyerson and others, 2002).

To find out if there are teleconnections between ENSO signals and crustal species concentrations in Antarctic snow, associations between the multivariate ENSO index (MEI; Reference Wolter and TimlinWolter and Timlin, 1993, Reference Wolter and Timlin1998) and nssCa2+ from the three ice cores were investigated. MEI integrates more information than other indices, reflecting the nature of the coupled ocean–atmosphere system better than either component, and is less vulnerable to occasional data glitches in the monthly update cycles (Reference Wolter and TimlinWolter and Timlin, 1993, Reference Wolter and Timlin1998).

The investigations show no correlation between MEI and nssCa2+ in SD and IT015. However, MEI is significantly correlated with nssCa2+ concentration in IT001 from January to March (average correlation coefficient is 0.32 (p < 0.01)). The most significantly correlated period is January–February (correlation coefficient 0.35, p < 0.01 (p < 0.05 also appears in April and May)). The MEI value for each month represents the average of 2 months (e.g. values in January represent the average over January and February). This suggests that crustal aerosols in IT001 are correlated with ENSO during the Southern Hemisphere summer. This possible link to the ENSO signal at the highest-elevation site (IT001) is consistent with our previous finding that crustal aerosols in the ice core come from the mid- to upper troposphere through vertical atmospheric movement. Figure 10 shows the correlation of nssCa2+ concentration in IT001 and MEI in January–February. During the strong ENSO period 1972–73 (Reference Quinn, Neal and Antunez de MayoloQuinn and others, 1987; Reference Legrand and Feniet-SaigneLegrand and Feniet-Saigne, 1991), nssCa2+ concentration increased by ~3 ppb, and the increase continued until 1979. The average nssCa2+ concentration during this period is about 8.7 ppb, 2.7 ppb higher than the 50 year mean value (Table 2). During the strongest ENSO event, in 1982–83, nssCa2+ concentration is the highest in the last 50 years. High concentrations continue until 1988 at ~14 ppb, 2.3 times the 50 year mean (the nssCa2+ concentration during this period is the highest in the last 350 years (not shown)). The concentrations stay high for several years and could be related to the propagating period of 4–5 years that ENSO may impart to the ACW (Reference White and PetersonWhite and Peterson, 1996). Exceptionally, the strong ENSO event of 1957–58 is not recorded in IT001 nssCa2+ concentration.

Fig. 10. Variation of IT001 nssCa2+ concentration and January–February MEI, 1948–2002. r is the correlation coefficient.

One of the effects of El Niño events on global climate is that drought occurs in the western Pacific (southeastern Africa, India and the northeastern region of South America), an area normally rich in rainfall. During the most severe El Niño of the century, in 1982 and 1983, dust storms and brush fires ravaged eastern Australia as a result of decreased rainfall. Drought caused by the ENSO events in South Africa, Australia and South America resulted in land surface desertification and more dust aerosols in the atmosphere, especially in arid regions of those areas. The air mass containing these dust aerosols may have been transported to the high inland region of West Antarctica.

4. Conclusions

The relationships between atmospheric circulation and nssCa2+ concentrations from the three ice cores in West Antarctica are investigated using NCAR/NCEP data covering the period 1948–2002. By performing spatial correlation analyses between the monthly NCAR/NCEP field and the nssCa2+ concentrations in the ice cores, we found that nssCa2+ concentration in SD is positively correlated with circumpolar zonal wind in SON. West-to-east pressure gradients intensified winds over the southeastern and southwestern Indian Ocean. Stronger westerly winds are conducive to the transport of crustal aerosols to SD. This is mostly connected to lower-layer circumpolar atmospheric circulation, such as the cyclonic systems around Antarctica that often move southward over the ice sheet. There is also a significant correlation between SD nssCa2+ concentrations and AAO from June to October over the last 50 years.

IT001 is mostly influenced by westerly circulation, resulting in higher nssCa2+ concentrations here than at the other two sites. The positive correlation between IT001 nssCa2+ concentration and the circumpolar higher-layer westerly wind exists throughout the year, indicating that IT001 is mainly influenced by the mid- to upper troposphere as expected due to its high elevation (Reference DixonDixon and others, 2005). The regions most highly correlated to the zonal wind areas are South Africa, Australia and the southwestern Indian Ocean. IT001 nssCa2+ concentration is also correlated with AAO except in January, when westerly circulation is weakest and the wind is lightest.

The relationship of IT015 nssCa2+ concentration to atmospheric circulation is different to that of SD and IT001 nssCa2+. The correlation of nssCa2+ with higher-layer zonal wind is significantly negative in October and November. The best-correlated regions are the South Pacific and South America, and the southwestern Indian Ocean. A negative correlation exists between IT015 nssCa2+ concentration and AAO, and the most correlated period of the AAO is October, when westerly winds are strongest. The negative correlation indicates that the stronger westerly circulation does not favor dust aerosol transport to IT015. The reason for the negative correlation is unclear but is probably related to high-latitude blocking on seasonal scales.

Correlations between meridional circulation and nssCa2+ concentrations from the three ice cores are not obvious, suggesting that the contribution of meridional circulation to crustal dust in SD, IT001 and IT015 is not significant. However, calibration between nssCa2+ concentration and MEI shows that more crustal species are transported to IT001 during the stronger ENSO event.

Acknowledgements

This research was supported by the US National Science Foundation Office of Polar Programs, the National Natural Science Foundation of China (40401054) and the ‘Talent Project’ of the Chinese Academy of Sciences. We greatly appreciate suggestions for the improvement of our paper from the referees and Scientific Editor, C Genthon.

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Figure 0

Fig. 1. Location map for the three core sites in West Antarctica.

Figure 1

Table 1. Ice cores in West Antarctica

Figure 2

Table 2. Summary of ion chemistry: average concentrations (ppb) for the overlap period. Values in parentheses are % of non-sea-salt calcium relative to total calcium

Figure 3

Fig. 2. A recent 20 year section of seasonal variations of sea-salt aerosol (ssNa+) and nssCa2+ concentrations at SD.

Figure 4

Fig. 3. Seasonal mean 850 hPa zonal wind (a) and its spatial correlation patterns with SD nssCa2+ (b), for the period 1948–95, plotted as correlation coefficients. (c, d) Same as (a) and (b) respectively, but for 500 hPa zonal wind.

Figure 5

Fig. 4. Zonal anomalies (minus zonal mean) of seasonal mean geopotential height (a) and 500 hPa zonal wind (b) in the Southern Hemisphere during SON.

Figure 6

Fig. 5. Variation of SD nssCa2+ concentration and 850 hPa zonal mean wind at 60˚ S (a), and July AAO (b), for the period 1948–2002. r is the correlation coefficient.

Figure 7

Fig. 6. Spatial correlation pattern of IT001 nssCa2+ concentration with 500 hPa zonal mean wind (only July is shown) for the period 1948–2002, plotted as correlation coefficients.

Figure 8

Fig. 7. Variation of IT001 nssCa2+ concentration and 500 hPa zonal mean wind at 60˚ S (a), and AAO (only July is shown) (b), for the period 1948–2002. r is the correlation coefficient.

Figure 9

Fig. 8. Spatial correlation pattern of IT015 nssCa2+ concentration with 500 hPa zonal mean wind (only November is shown) for the period 1948–2001, plotted as correlation coefficients.

Figure 10

Fig. 9. Variation of IT015 nssCa2+ concentration and October AAO for the period 1948–2002. r is the correlation coefficient.

Figure 11

Fig. 10. Variation of IT001 nssCa2+ concentration and January–February MEI, 1948–2002. r is the correlation coefficient.