Introduction
Polar ice-core records have proven to be valuable tools for palaeoclimate reconstruction, recording both anthropogenic and natural global climate change (e.g. Reference Benoist, Jouzel, Lorius, Merlivat and PourchetBenoist and others, 1982; Reference Dansgaard, Oeschger, Oeschger and LangwayDansgaard and Oeschger, 1989; Reference MayewskiMayewski and others, 1994). Information about past climate conditions is preserved as particles and air bubbles entrapped in the ice matrix, absorbed gases, dissolved trace-ion species and in the isotopic composition of the ice. However, our ability to interpret these ice-core signals is limited by difficulties in understanding the relative importance of changes in the source, transport and deposition processes that influence a precipitating air mass. Current research is directed towards this issue by comparing high-resolution, recently deposited glaciochemical records with contemporaneous meteorological observations (Reference Hardy, Vuille, Braun, Keimig and BradleyHardy and others, 1998; Reference Vuille, Hardy, Braun, Keimig and BradleyVuille and others, 1998 ;Reference McMorrow, Curran, van Ommen, Morgan, Pook and AllisonMcMorrow and others, 2001).
The research described in this paper extends the preliminary analysis technique reported in Reference McMorrow, Curran, van Ommen, Morgan, Pook and AllisonMcMorrow and others, 2001 where shallow firn-core records from Law Dome, East Antarctica, were directly compared with local, regional and synoptic meteorological observations. the climatology of the Dome Summit South (DSS) drilling site on Law Dome (Fig.1; Reference CurranCurran and others, 2002) indicates it is an ideal site for high-resolution studies of the snowpack. the high annual accumulation (0.7ma–1 ice equivalent), low mean summer temperatures (–12.6˚C) and absence of frequent high wind gusts leads to the deposition of thick annual layers and ensures limited disturbance of the chemical archive (Reference Morgan, Wookey, Jun, T. D., Skinner and Fitzpatrick.Morgan and others, 1997; Reference McMorrow, Curran, van Ommen, Morgan, Pook and AllisonMcMorrow and others, 2001).
Moreover, seasonal characteristics of the synoptic-scale meteorology influencing the region allow a comprehensive examination of the impact of meteorological conditions on glaciochemical signals. for example, it is well documented that the Law Dome region is influenced by generally intensified cyclonic activity during the austral winter months (June–August) and a semi-annual variation in atmospheric pressure, with minima in the austral spring (September–November) and autumn (March–May) (Reference SchwerdtfegerSchwerdtfeger, 1984; Reference Allison, Wendler and RadokAllison and others, 1993; Reference Jones and SimmondsJones and Simmonds, 1993; Reference King and TurnerKing and Turner,1997).
This paper presents preliminary results from techniques by which trace chemical and oxygen isotope ratio (δ18O) records in snow pits and firn cores, collected between 20 February and 6 March 2000, are directly compared with observed meteorological conditions. Glaciochemical records are examined on spatial scales ranging from 30 cm up to 7.7 km in order to identify regional accumulation events. High-resolution snow-accumulation data measured by a co-located automatic weather station (AWS) are used to identify the meteorological events that comprise the snow-pit records. the top 0.5 m of the snow-pit records is then compared with meteorological conditions during the most recent summer period (summer 1999/2000).
Methods and Sample Collection
The results presented here draw on material from a 2 mdeep snow pit (Rama) and four shallow (6 m) firn cores located up to 7.7 km a part from near the DSS drilling site on Law Dome (Fig.1; Reference CurranCurran and others, 2002). the snow pit and firn cores are located on the accumulation isopleth that crosses DSS (approximately 640 kg m–2 a–1) in order to minimize accumulation scaling differences between drilling sites.
The snow pit was sampled using clean techniques to allow the extraction of trace-ion samples free from contamination. All instruments used in the digging and sampling of the snow pits were washed with deionized Milli-Q water (resistivity >18MΩ-cm) prior to transportation to the field. Snow-pit personnel wore clean suits, at least two sets of plastic gloves and dust masks to minimize contamination from human interference. Initial digging of the snow pit to approximately 1m depth was done using cleaned stainless-steel shovels. A further 20 cm of the wall was removed with a number of scrapers to ensure an uncontaminated sampling wall. Just before sampling, a further 2 cm was scraped away using a clean microtome blade. A cleaned metal template was then fastened to the wall using steel pins, and two samples for each depth interval were extracted using steel square tube probes. Sample resolution was 2.5 cm, and the template ensured millimetre depth accuracy. Samples were collected for δ18O and trace-ion chemical species (magnesium, sodium, potassium, calcium, nitrate, sulphate, methanesulphonic acid (MSA) and chloride). Thediggingandsampling process was then repeated for the 1–2m depth interval. Seven lines of samples (approximately 30 cm apart) were collected from the snow pit: three lines from 0 to 2m and four lines covering a depth range 0.25–1.25m.
Several shallow firn cores (6m) were collected within approximately 0.5 mof the snow-pitwall, and at regular intervals along the north/south accumulation isopleth that crosses DSS. All cores were collected with a hand auger, with special care taken to preserve the top 0.3 msection of friable material. Firn cores and snow-pit samples were transported frozen back to Australia for decontamination, sampling and analysis of δ18O, trace-ion chemical species and hydrogen peroxide at 2.5 cm resolution using established techniques (Reference Curran and Palmer.Curran and Palmer, 2001; Reference McMorrow, Curran, van Ommen, Morgan, Pook and AllisonMcMorrow and others, 2001).
Spatial Reproducibility of Glaciochemical Signals
Snow-pit and firn-core comparisons are made at various scales across Law Dome to assess the spatial reproducibility of signals and to identify regional accumulation events preserved in the snowpack. Regional accumulation events are recorded at different depths in snow-pit or firn-core records due to accumulation differences between sites, different sampling/drilling dates, loss of surface snow at the time of sampling/drilling, surface snow redistribution by wind, surface irregularity, and local firn-density variations. Despite these effects, there is excellent agreement in multiple trace-ion and δ18O records at both the intra-pit scale (Fig.1) and the inter-core scale (Fig. 2). the seven-line intra-pit comparison highlights the minimal impact that surface irregularities (sastrugi and dunes) over spatial scales from 30 cm to approximately 2m has on the snow-pit records (Fig. 1). Major features in the trace-ion and δ18O records are represented in all or most of the sample lines, indicating regional accumulation events that can be used in the meteorology comparison. the δ18O and MSA records show very good agreement at this spatial scale; in contrast, sodium shows greater spatial variability when concentrations are high. These results are consistent with results reported by Reference Steffensen, Clausen, Christensen, Wolff and BalesSteffensen andothers (1996). However, in contrast to Reference Steffensen, Clausen, Christensen, Wolff and BalesSteffensen and others (1996), nitrate profiles presented here show considerable variability when concentrations are low, but good agreement when concentrations are higher.
At Law Dome, δ18O, MSA and nitrate concentrations peak in the summer period, and sea salts (indicated by sodium) generally peak in winter (Reference Curran, van Ommen and MorganCurran and others, 1998a). A clear seasonal signal can be seen for δ18O, MSA, nitrate and sodium in the snow pit over two annual cycles, with summer species peaking around 0.5 and 1.3m and winter species peaking around 0.9 and 1.7m(Fig.1). It is interesting to note that all species show high concentrations at the very surface of the snow pit, corresponding to late February 2000. This event is discussed in detail later in the paper. In addition to seasonal cycles, the 2.5 cm sample resolution at this high-accumulation site has captured many sub-seasonal phenomena (e.g.multiple δ18O peaks during summer deposition, non-summer elevated levels of MSA, and double peaks in winter sodium levels (Fig.1)).
Comparisons between δ18O records over spatial scales of up to 7.7 km also show excellent agreement (Fig. 2). These inter-core comparisons are used to identify regional events in the firn-core records and to assess the spatial reproducibility of signals preserved at different drilling sites on Law Dome. the depth of accumulation events in the core record is influenced by different drilling dates of the cores, accumulation differences between drilling sites, surface irregularity caused by sastrugi and the rapid density changes in the top layers of the snowpack. Accumulation differences between sites were minimized by drilling along the same accumulation isopleth, and drilling-date differences were minimized by drilling within a 16 day window. Figure 2 shows that seasonal and major sub-seasonal signals are preserved in all cores, allowing the identification of regional events for further analysis and comparison with meteorological conditions.
Identification of Meteorological Events
Meteorological events that make up the snow-pit and firn-core records are identified using snow accumulation recorded by the AWS, located 50 m west of the Rama snow pit. the AWS measured snow height using an ultrasonic sounding at hourly intervals. Net accumulation is calculated as the difference between snow-accumulation and snow-removal events, as recorded by the AWS (Fig. 3). the most notable feature of Figure 3 is the difference in seasonal net accumulation during 1998 (Julian days (1998) 0–365) compared to 1999 (Julian days 366–730). the seasonal distribution of net accumulation during 1998 is relatively even, with each calendar season receiving approximately equal amounts of net snowfall (average 0.42 m per season). However, from summer 1998/99 through to early spring 1999 (Julian days 360–655) the AWS recorded limited net snow accumulation (summer 1998/99, 0.11m; autumn 1999, 0.15 m; winter 1999, 0.08 m). Snow accumulation began to increase during spring 1999 (0.38m) and into summer 1999/ 2000 (0.53m) (Julian days 655–780). These results highlight interannual accumulation variability and have clear implications for interpreting longer ice-core records.
Difficulties arise in registering the AWS accumulation depth scale (Fig.3) with the snow-pit records due to densification effects. the accumulation sensor is mounted on a mast supported by a fixed baseplate that is buried approximately 0.6 mbelowthe surface at the start of the observation periods (when the AWS was installed or re-installed). Gradual densification of this material between sensor and baseplate at the start of the accumulation period acts to lower the surface height registered by the sensor. This leads to an underestimate of accumulated material and an apparent ``shortening’’ of the firn column height as reported by the AWS over the observation period. Similarly, material deposited during the observation period is compressed, distorting the time– depth relationship inferred from the AWS scale (Fig. 3).
The degree of record-shortening by compaction during the observation period has been estimated here assuming Sorge’s law (a steady-state density profile) and experimenting with different empirical density profiles. the baseplate depth changes from 0.6m to 1.84m during the most recent observation period (December 1998–February 2000). Compression of the 0.6 m layer over this depth range varies from 4 to 6 cm depending upon the assumed density profile. the low estimate arises from a density model which fits the overall DSS profile extremely well (Reference Van Ommen, Morgan, Jacka, Woon and ElcheikhVan Ommen and others, 1999), but which may not capture changes in the upper few tens of centimetres of firn. the higher estimate arises if the previous model is altered to include a rapid (exponential) densification in the upper 0.5 m from a nominal surface density of 350 kg m–3.
For the purposes of this paper, densification effects are not treated any further, and detailed temporal registration is confined to the uppermost portion of the records where the effects can largely be neglected. Development of this work, comparing measured densities and using observed ties between AWS data and snow-pit signals, should provide data that can be used to develop a refined model of densification in the future.
Examination of Recent Accumulation Periods
The AWS net accumulation record indicates three main periods of net accumulation in the Rama snow pit for summer 1999/2000 (P1–P3) (Fig. 3). the corresponding glaciochemical signals are represented in Figure 4. Densification effects, as noted above, may lead to small shifts in the period boundaries represented in Figure 4. for this reason, the following analysis is restricted to the major changes in this recent portion of the record.
All three of the net accumulation periods preserved similar amounts of accumulated material (0.16–0.19m) (Fig. 3; Table 1) yet quite different glaciochemical signals (Fig.4;Table1). the snow-pit signals associated with P1 (late summer) include elevated levels of MSA, δ18O, sodium and nitrate concentrations. the deposition of MSA with δ18O and sea salts outside the mid-summer MSA peak is also observed in deeper records at DSS (Reference CurranCurran and others, 2002). the snow-pit signals preserved during P2 show levels of MSA, nitrate, δ18O and sodium comparable to average summer concentrations at DSS with no distinct peaks. In contrast, P3 has preserved a very narrow and pronounced peak in MSA and δ18O, with MSA concentrations peaking at 1.7 μeq L–1, which is higher than average summer levels from deeper records at DSS (0.07–0.25 μeq L–1).
Local meteorological conditions recorded by the AWS during summer 1999/2000 are illustrated in Figure 5. the accumulation periods are all marked by a sharp decline in atmospheric pressure and pronounced peaks in wind speed (Fig.5). There is also evidence of elevated temperatures during net accumulation periods, especially for P3. In addition, these conditions are reflected in the meteorology at Casey station (located 110 km from DSS), indicating the influence of large-scale atmospheric systems. Precipitation events at Law Dome are usually caused by the passage of cloud bands associated with cyclonic systems over the ocean to the north, and resulting in strong easterly winds, falling atmospheric pressure and elevated temperatures (Reference SchwerdtfegerSchwerdtfeger, 1984; Reference Callaghan and BettsCallaghan and Betts, 1987; Bromwich, 1998). the conditions recorded by the AWS and Casey station during the net accumulation periods are consistent with these findings.
There is also a period (Julian days 738–743) in the summer record where the AWS measured conditions similar to the net accumulation periods (Fig. 5), yet only 0.02m of accumulation was retained in the record (Fig.3). Significant snowfalls are recorded during this period, but the majority of material was lost through wind scouring (Fig. 3). This is consistent with the sustained high levels of wind speeds recorded by the AWS, in contrast to the other net accumulation periods which are characterized by sharp spikes in wind speed (Fig. 5).
Advanced Very High Resolution Radiometer (AVHRR) infrared imagery illustrates differences in source and transport mechanisms influencing each of the accumulation periods (Fig. 6, Table 1). All periods were characterized by cyclonic systems passing over Law Dome, yet the intensity, travel path and speed of travel of the cyclones varied between periods. P1 is characterized by a large cyclonic system that began to develop on 20 February 2000 (Julian day 781) around 45˚ S, 90˚E (Fig. 6a) and then intensified and moved due south onto Law Dome early on 22 February 2000 (Julian day 783) (Fig. 6b). This system continued to influence Law Dome until around 27 February 2000 ( Julian day 788). P2 is characterized by weak and disorganized cyclonic systems that decayed quickly while passing over Law Dome throughout the period. An example of one of these systems is given in Figure 6c and d. In contrast, AVHRR imagery for P3 shows two large cyclonic systems passing over Law Dome in quick succession. System 1 is sourced from the Heard/McDonald Island region (55˚ S, 70˚E) around 20 December 1999, and travelled southeast and onto Law Dome on 22 December 1999 (Julian day 721) (Fig. 6e and f). System 2 followed a similar path, and passed over Law Dome on 27 December 1999 (Julian day 726), although cloud cover indicates a less intense system (not shown).
The late-summer deposition of MSA, δ18O and sea salts preserved during P1can be explained by the rapid poleward transport of a strong cyclonic system from mid-latitudes (Table 1). Rapid advection of warm marine air from mid-latitudes, where there is an expected source of DMS from marine biota at this time of year (Reference Curran and JonesCurran and Jones, 2000), provides an explanation for the enhanced MSA concentrations in the snow-pit record. Limited fractionation of δ18O due to the short time available for precipitation and increased uptake of sea salts during rapid transport of warm air masses explains the high levels of δ18O and sodium in the snow-pit record. the average summer levels of MSA, δ18O, nitrate and sodium preserved during P2 are the result of weak cyclonic systems passing in close succession during this period. These systems all developed in close proximity to Law Dome (Table1), with systems passing over the sea ice before reaching Law Dome. the sea-ice zone is an important source of MSA for summer deposition at Law Dome (Reference Curran and JonesCurran and Jones, 2000), and the low sodium concentrations can be explained by limited sea-salt aerosol production associated with these weak systems. In contrast, the enhanced mid-summer levels of MSA preserved during P3 may be sourced from the Heard/McDonald Island region where DMS productivity from marine biota is extremely high (Table 1) (Reference Curran, Jones and BurtonCurran and others, 1998b).
Concluding Remarks
This paper presents preliminary results from ongoing research aimed at increasing our understanding of the link between ice-core signals and climate conditions. the comparison of net accumulation between two successive years, where 1998 recorded relatively uniform accumulation throughout the year, and 1999 recorded varied amounts of net accumulation throughout the year, highlights interannual accumulation variability and has implications for interpreting the deep ice-core record (e.g. ice-core dating, seasonality studies). Particular examination of the accumulation periods that comprise summer 1999/2000 reveals variable meteorological conditions for specific snow-pit signals. Late-summer deposition of MSA, δ18O and sea salts is associated with rapid advection of air from low latitudes where DMS production is high at this time of year. This allows identification of a potential source region for non-summer elevated levels of MSA (see Reference CurranCurran and others, 2002) observed in deeper ice-core records at DSS. In addition, a pronounced mid-summer MSA peak, higher than concentrations observed in deeper records at DSS, is associated with strong cyclonic systems sourced from a known area of high DMS production. In contrast, average summer levels of MSA, δ18O and sodium are associated with weak cyclonic development close to the Law Dome region. These results highlight the effects of circulation patterns on the snow-pit record. Deep ice-core records from coastal Antarctic sites influenced mainly by the procession of cyclonic systems are likely to be sensitive to changes in circulation patterns through the palaeoclimate record. This three-period comparison provides some insight into source and transport paths influencing summer snow-pit signals, and enhances our understanding of similar signals preserved in deeper ice-core records at Law Dome.
Acknowledgements
The authors would like to thank the Trans-Antarctic Association for providing financial assistance to attend the International Symposium on Ice Cores and Climate. Thanks also to the 1999/2000 Law Dome field party for assistance in sample collection.