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Recent Deposition of 210Pb on the Greenland Ice Sheet: Variations in Space and Time

Published online by Cambridge University Press:  20 January 2017

Jack E. Dibb*
Affiliation:
Glacier Research Group, University of New Hampshire Institute for the Study of Earth, Oceans and Space, Science and Engineering Research Building, Durham, NH 03824, U.S.A.
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Abstract

Detailed 210Pb profiles were determined for four “Chernobyl dated” snowpits sampled during a wide-ranging survey of the Greenland ice sheet during the 1988 season. The profiles from widely separated pits show little or no coherence; even for two pits only 40 km apart the profiles differ in detail. There does not appear to have been any seasonality in the deposition of 210Pb onto the ice sheet in the two years since the Chernobyl accident. The total deposition of 210Pb during this period (10-20 bq m-2) was about 20 times less than has been observed at mid-latitude sites in the eastern United States. The three pits west of the ice-sheet divide recorded very similar depositional fluxes, while the one eastern pit had only two-thirds the average of the others, suggesting a west-to-east gradient in the deposition of 210Pb, and perhaps other continentally-derived submicron aerosols, onto the Greenland ice sheet.

Type
Research Article
Copyright
Copyright © International Glaciological Society 1990

Introduction

Glacial ice from around the world is increasingly regarded as representing perhaps the most important archive of information on past climate and atmospheric conditions. Because of this interest, the number, diversity and quality of records recovered from glacial snow and ice is rapidly-increasing. However, in order to decipher the information contained in the depth profiles of the various parameters measured in ice, two key points must be addressed: the conversion of depth in the glacier to a temporal framework, and the relation between the concentrations measured in ice and those in the atmosphere at the time the snow fell. Atmospheric radionuclides can contribute greatly in both of these areas.

A substantial body of research has clearly established the utility of natural (mainly 210Pb) and anthropogenic (derived from bomb testing) atmospheric radionuclides for dating glacial snow and ice (Reference GoldbergGoldberg, 1963; Reference Crozaz, Picciotto and de BreuckCrozaz and others, 1964; Reference Picciotto, Crozaz and de BreuckPicciotto and others, 1964, Reference Picciotto, Crozaz, Ambach and Eisner1967; Reference Crozaz and FabriCrozaz and Langway, 1966; Reference Jouzel, Merlivat, Pourchet and LoriusJouzel and others, 1979; Gunten and others, 1982; GäReference Gäggeler, von Gunten, Rössler, Oeschger and Schottererggeler and others, 1983). The relatively high accumulation rates on the Greenland ice sheet limit the application of these dating techniques to studies where samples are taken from depths (10s to 100s of m) much greater than those to which snowpits can routinely be dug. The nuclear reactor accident at Chernobyl in April 1986 injected enough radioactive material into the atmosphere to provide a valuable new time horizon in the upper layers of the snow on the Greenland ice sheet (Reference DibbDibb, 1989).

Atmospheric 210Pb results from the decay of the gaseous, 238U decay series radionuclide, mRn emitted from continents (Reference Turekian, Y and BenningenTurekian and others, 1977). Very shortly after production the 210Pb associates with submicron aerosols (Reference Bondietti, Papastefanou and RangarajanBondietti and others, 1987, Reference Bondietti, Brantley and Rangarajan1988) and thereafter shares the same fate as the aerosol. As a result, atmospheric 210Pb serves as a tracer of continentally-derived submicron aerosols in the atmosphere.

In Antarctica several long-term studies have monitored aerosol concentrations of 210Pb to help clarify the atmospheric transport processes bringing aerosols and their associated chemical species to the ice sheet (Reference Lockhart, Patterson and SaundersLockhart and others, 1966; Reference Maenhaut, Zoller and ColesMaenhaut and others, 1979; Reference Wagenbach, Görlach, Moser and MünnichWagenbach and others, 1988). Although not conclusive, the results have suggested the importance of stratospheric transport in bringing continentally-derived aerosols to high southern latitudes. In the Arctic, Rahn and McCaffrey (1980) and Daisy and others (1981) observed a pronounced seasonality in Pb aerosol concentrations at Barrow (winter maximum with concentrations 15 times higher than in summer) that was corroborated by Graustein and Barrie (personal communication from W. Graustein) during a study at Mold Bay. The seasonal pattern of 210Pb in the aerosol at these high-latitude, low-altitude sites was very similar to the seasonality of the pollution phenomenon known as Arctic Haze; in particular, Rahn and others (1980) reported very high correlations between the concentrations of 210Pb and SO4 2−. They proposed that the annual migration of the Polar Front from its high-latitude summer position to a more southern winter position brought large, mid-latitude, continental areas effectively into the polar air mass, so that Pb and pollutants emitted from these areas in the winter are readily transported to high latitudes.

The present study describes detailed 210Pb profiles from the top 3 m of four “Chernobyl dated” snowpits on the Greenland ice sheet. The primary goals of the investigation were to ascertain whether 210Pb might provide a strong seasonal signal to assist in the interpretation of detailed chemical records recovered from these and future shallow pits in Greenland, and to examine spatial and short-term temporal variability in the deposition of 210Pb on the Greenland ice sheet.

Methods and Materials

Large volume (approximately 1 litre when melted) snow samples for radionuclide analyses were collected in a series of snowpits in Greenland as part of a regional snow chemistry survey conducted in 1987 and 1988 (Fig. 1). In relation to the overall survey, the primary purpose of the radionuclide sampling was to determine the distribution of fallout on the Greenland ice sheet from the Chernobyl reactor accident. To achieve this goal 2 m sections of seven snowpits, centered on what the field party estimated was the level of the 1986 summer surface, were sampled at 6 cm intervals. In four of the pits dug in 1988 the entire depth was sampled in order to examine in detail the recent history of 210Pb deposition. All of the samples were immediately double-bagged in polyethylene and returned to New Hampshire frozen, where they were stored at −20°C until preparation for analysis.

Upon removal from the freezer the outside 0.5 cm of the originally vertical sides of each block were carefully scraPed off, then concentrated HCl (0.333 ml kg×1 sample) and 208Po tracer (for the samples destined for 210Pb analysis) were added to the samples. The radionuclides were concentrated from the melted samples onto cation exchange filters (Delmas and Pourchet, 1977). Each sample was filtered three times, the filters dried and then placed in polyethylene vials for gamma spectrometric determination of 134Cs and 137Cs. After gamma counting the filters were placed in a porcelain funnel and leached with 5 ml of concentrated HCl. The leachate was collected in acid-washed teflon beakers, to which 20 ml of Milli-Q deionized H2O and 5 ml of Na-citrate was added. Polonium was then spontaneously plated onto polished silver planchets, for four hours at 70°C with frequent gentle swirling and then overnight at room temperature. 2l0Pb activities were determined from the ratio of the alpha activities of the daughter 210Po and the tracer 208Po (Crozaz and Fabri, 1966; Reference FlynnFlynn, 1968).

Fig. 1. Location of pits where large-volume samples were collected for radionuclide analyses. The Summit (S) pit was sampled in the 1987 season and the rest were sampled during the 1988 season.

Results and Discussion

Fallout from Chernobyl was found in all of the pits. The distribution of this radioactive debris on the Greenland ice sheet is discussed more fully elsewhere (Reference DibbDibb, 1989). However, the presence of a layer of snow labeled with Chernobyl fallout in each of the pits does provide a very well constrained temporal framework in which to consider the 210Pb results.

The depth profiles of 210Pb concentrations in the top 3 m of the four pits are noisy (Figs 2 and 3). Perhaps the most striking aspect of these profiles is the lack of any obvious seasonality in the concentration of 210Pb in recent Greenland snow, considering the previously mentioned 15-fold increase in 210Pb concentration observed in the aerosol at Barrow during the winter (Reference Rahn and McCaffreyRahn and McCaffrey, 1980; Reference Daisey, McCaffrey and GallagherDaisey and others, 1981) and the 21-fold increase observed by Graustein and Barrie at Mold Bay (personal communication from W. Graustein). Davidson and others (Reference Davidson, Santhanam, Fortmann and Olson1985, Reference Davidson, Harrington, Stephenson, Boscoe and Gandley1989) have suggested that the seasonal pattern of SO2− 4 deposition in snow at Dye 3 follows the annual cycle observed for aerosol concentrations at a number of stations around the Arctic (winter maximum and summer minimum), but that the signal is greatly dampened in the snow due to the prevalence of rimed snow (with much higher scavenging efficiency) occurring during the summer. Such a mechanism might explain the apparent lack of a winter peak in Pb concentration in the snow falling on the Greenland ice sheet in recent years. Alternatively, it may be that the presence of the Greenland ice sheet has enough of an influence on the atmospheric dynamics around and above it that the climatology of 210Pb (and perhaps other continentally derived submicron aerosol-associated species) over the ice sheet has little or no relation to what has been described for other regions of the Arctic. (A 12-month aerosol sampling campaign at Dye 3 did not reveal any pronounced increase in the concentration of 210Pb during the winter of 1988-89 (Dibb, in preparation).)

The details of the 210Pb profiles show little coherence between the three widely separated pits (Fig. 2). Pits 1 and 2, separated by 40 km, have 210Pb profiles that are more similar but still differ in detail (Fig. 3). This is not surprising, considering the importance of wet deposition processes in carrying aerosol-associated species to the surface of the ice sheet (Reference JungeJunge, 1977; Reference DavidsonDavidson, 1989) and the extreme heterogeneity of these processes in space and time. However, if longer intervals of time are examined, some interesting trends appear.

Fig. 2. Detailed profiles of 210Pb activity versus depth in the firn for pits 1, 6 and 7. Pits were sampled at continuous 0.06 m intervals. The horizontal bars represent one sigma counting uncertainty. The depth of the winter layers was derived from δ18O profiles (not shown). The Chernobyl layer is from Dibb (1989).

Over the two years since the deposition of the Chernobyl debris layer, the average concentration of 210Pb in snow has been 23.3, 21.8, 20.2 and 14.8mbqkg−1 at the locations of pits 1, 2, 6 and 7 respectively. Given the depth to the Chernobyl layer (2.04, 2.28, 2.34 and 2.28 respectively), and assuming an average density in the range of 300-400 kg m×3, the total amount of 210Pb deposited during that two-year period has been calculated for each of the pits (Fig. 4). Even the highest estimate of 210Pb deposition onto the Greenland ice sheet (20 bq m×2 in two years) is almost 20 times lower than those observed at continental sites. Olsen and others (1985) measured fluxes of 152 and 173bq m−2y−1 at sites in Virginia and Tennessee that were very similar to the 5-year average of 177bqm×2y−1 reported by Turekian (1983) for a coastal Connecticut site. The lower 210Pb flux to the surface of the Greenland ice sheet reflects both loss of submicron aerosols during the long transport from the continental source areas and the limited amount of precipitation onto the ice sheet.

Fig. 3. Detailed profiles of 210Pb activity versus depth in the firn for pits 1 and 2. Pits were sampled at continuous 0.06 m intervals. The horizontal bars represent one sigma counting uncertainty. The depth of the winter layers was derived from δ18O profiles (not shown). The Chernobyl layer is from Dibb (1989).

Fig. 4. 210 Pb deposition at the four sites during the two-year interval between the Chernobyl accident in late April, 1986, and sampling in May, 1988. The range in estimated deposition reflects the uncertainty in the density of the firn over the depth sampled. The low estimate for each pit assumes an average density of 300 kg m×3 and the high estimate assumes 400 kg m×3.

The very close agreement in the 210Pb fluxes recorded in pits 1, 2 and 6 is striking, given the aforementioned lack of correspondence between the detailed profiles (Figs 2-4). The flux at pit 7 is only about two-thirds that at the other pits. It is interesting that pit 7 is the only one of the four that is east of the ice-sheet divide. Pit 7 is also further south and closer to the divide than the other pits, but the suggestion of a significant difference in 210Pb deposition on either side of the divide is intriguing. The proximity of North America, particularly Arctic Canada, to the west coast of Greenland and the long transport pathways over water from potential Eurasian source areas suggest North America as perhaps the dominant source of 210Pb Greenland snow. The apparent west-to-east gradient in 210Pb deposition might then reflect progressive removal of 210Pb (and, by implication, other continentally derived submicron aerosols) as air masses cross Greenland from the west. Obviously, four pits constitute a very sparse data set and the dynamic interactions between transport and deposition processes in the atmosphere are complex; however, it is interesting to note that Heidam (1984) observed higher concentrations of crustally derived species during 1979-80 at a station on the west coast of Greenland (GOVN) than at two stations on the east coast (NORD and KATO).

Conclusions

The natural atmospheric radionuclide 210Pb, as it is preserved in snow and firn deposits, has great potential as a tracer of atmospheric transport and deposition processes in addition to its well established role as a dating tool. The lack of seasonality in 210Pb deposition on the Greenland ice sheet suggests that the air masses over Greenland are decoupled to some extent from the general high Arctic atmosphere. On very short time scales, 210Pb indicates the spatial heterogeneity of the deposition (and subsequent preservation) of submicron aerosols on the Greenland ice sheet. For periods on the order of two years (perhaps as short as one year) 2l0Pb deposition appears to be nearly uniform over large regions of the ice sheet. The very limited data set described here suggests significantly more 210Pb deposition west compared to east of the ice-sheet divide, which agrees with previous work showing higher concentrations of crustally-derived species in the aerosol on the west than the east coast of Greenland. Similar studies, particularly to verify the gradient in deposition hinted at by the present results, should further our understanding of the linkages between snow and ice chemistry records and the atmospheric processes that are responsible for these records.

Acknowledgements

I gratefully acknowledge the financial support of the W.M. Keck Foundation during the analytical portion of this research. Thanks are due to the UNH field team of P. Mayewski (leader), M. Twickler, C. Wake, M. Hussey and S. Drummey for collecting the samples and K. Swanson of PICO for providing them with logistical support. The field program was supported by National Science Foundation grant #DPP 8619158.

References

Bondietti, E.A, Papastefanou, C and Rangarajan, C 1987. Aerodynamic size associations of natural radioactivity with ambient aerosols. In Hopke, P.K., ed. Radon and it’s decay products: occurrence, properties, and health effects. Washington, DC, American Chemical Society, 377-397. (ACS Symposium Ser. 331.)CrossRefGoogle Scholar
Bondietti, E.A, Brantley, J.Nand Rangarajan, C 1988. Size distribution and growth of natural and Chernobyl-derived submicron aerosols in Tennessee. J. Environ. Radioactivity, 6, 99-120.CrossRefGoogle Scholar
Crozaz, G and Fabri, P 1966. Mesure du polonium a�l’échelle de 10×13 Curie tracage par le 208Po et application à� la chronologie des glaces. Earth Planet. Sci. Lett., 1(6) 446-448.CrossRefGoogle Scholar
Crozaz, G and Langway, C.C jr. 1966. Dating Greenland firn-ice cores with Pb-210. Earth Planet Sci Lett., 1, 194-196.CrossRefGoogle Scholar
Crozaz, G, Picciotto, E, and de Breuck, W 1964. Antarctic snow chronology with Pb210. J. Geophys. Res., 69(12), 2597-2604.CrossRefGoogle Scholar
Daisey, J.M, McCaffrey, R.J and Gallagher, R.A 1981. Polycyclic aromatic hydrocarbons and total extractable particulate organic matter in the Arctic aerosol. Atmos Environ., 15, 1353-1363.CrossRefGoogle Scholar
Davidson, C.I 1989. Mechanism of wet and dry deposition of atmospheric contaminants to snow surfaces. In Oeschger, H. and C.C. Langway, jr, eds. The environmental record in glaciers and ice sheets. New York, Wiley and Sons, 29-51.Google Scholar
Davidson, C.I, Santhanam, S, Fortmann, R.C, and Olson, M.P 1985. Atmospheric transport and deposition of trace elements onto the Greenland ice sheet. Atmos. Environ 19(12), 2065-2081.CrossRefGoogle Scholar
Davidson, C.I, Harrington, J.R, Stephenson, M.J, Boscoe, F.P and Gandley, R.E 1989. Seasonal variations in Sulfate, nitrate, and chloride in the Greenland ice sheet: relation to atmospheric concentrations. Almos. Environ., 23(11), 2483-2494.Google Scholar
Delmas, R and Pourchet, M 1977. Utilisation de filtres échangeurs d’ions pour l’étude de l’activite β globale d’un carrotage glaciologique. International Association of Hydrological Sciences Publication 118 (Symposium at Grenoble 1975 — Isotopes and Impurities in Snow and Ice). 159-163.Google Scholar
Dibb, J.E 1989. The Chernobyl reference horizon (?) on the Greenland ice sheet. Geophys. Res. Lett., 16(9), 987-990.CrossRefGoogle Scholar
Flynn, W.W 1968. The determination of low levels of polonium-210 in environmental materials. Anal. Chim. Acta, 43, 221-227.CrossRefGoogle ScholarPubMed
Gäggeler, H, von Gunten, H.R, Rössler, E, Oeschger, H and Schotterer, U 1983. 210Pb-dating of cold Alpine firn/ice cores from Colle Gnifetti, Switzerland. J. Glaciol., 29(101), 165-177.CrossRefGoogle Scholar
Goldberg, E.D 1963. Geochronology with 210 Pb. In Symposium on Radioactive Dating. Proceedings. Vienna, International Atomic Energy Agency, 121-131.Google Scholar
Gunten von, H.R, Rössler, E and Gäggeler, M 1983. Dating of ice cores from Vernagtferner (Austria) with fission products and lead-210. Z. Gletscherkd. Glazialgeol., 18(1), 1982, 37-45.Google Scholar
Heidam, N.Z 1984. The components of the Arctic aerosol. Atmos. Environ., 18, 329-343.CrossRefGoogle Scholar
Jouzel, J, Merlivat, L, Pourchet, M and Lorius, C 1979. A continuous record of artificial tritium fallout at the South Pole (1954-1978). Earth Planet. Sci. Lett., 45(1), 188-200.CrossRefGoogle Scholar
Junge, CE 1977. Processes responsible for the trace content in precipitation. International Association of Hydrological Sciences Publication 118 (Symposium at Grenoble 1975 — Isotopes and Impurities in Snow and Ice), 63-77.Google Scholar
Lockhart, L.B jr, Patterson, R.L jr, and Saunders, A.W jr. 1966. Airborne radioactivity in Antarctica. J. Geophys. Res., 71(8), 1985-1991.Google Scholar
Maenhaut, W, Zoller, W.H and Coles, D.G 1979. Radionuclides in the South Pole atmosphere. J. Geophys. Res., 84(C6), 3131-3138.CrossRefGoogle Scholar
Olsen, C.R and 6 others. 1985. Atmospheric fluxes and marsh-soil inventories of 7Be and 210Pb. J. Geophys. Res., 90(D6), 10,487-10,495. CrossRefGoogle Scholar
Picciotto, E, Crozaz, G and de Breuck, W 1964. Rate of accumulation of snow at the South Pole as determined by radioactive measurements. Nature, 203(4943), 393-394.CrossRefGoogle Scholar
Picciotto, E, Crozaz, G, Ambach, W and Eisner, H 1967. Lead-210 and strontium-90 in an Alpine glacier. Earth Planet. Sci. Lett., 3, 237-242.CrossRefGoogle Scholar
Rahn, K.A and McCaffrey, R.J 1980. On the origin and transport of the winter Arctic aerosol. Ann. N.Y. Acad. Sci., 338, 486-503.CrossRefGoogle Scholar
Turekian, K.K., Y, Nozaki and Benningen, L.K 1977. Geochemistry of atmospheric radon and radon products. Annu. Rev. Earth Planet. Sci., 5, 227-255.Google Scholar
Turekian, K.K, Benninger, L.K and Dion, E.P 1983. Be and 210Pb total deposition fluxes at New Haven, Connecticut and at Bermuda. J. Geophys. Res., 88(C9), 5411-5415.CrossRefGoogle Scholar
Wagenbach, D, Görlach, U, Moser, K and Münnich, K 1988. Coastal Antarctic aerosol: the seasonal pattern of its chemical composition and radionuclide content. Tellus, 40B, 426-433.CrossRefGoogle Scholar
Figure 0

Fig. 1. Location of pits where large-volume samples were collected for radionuclide analyses. The Summit (S) pit was sampled in the 1987 season and the rest were sampled during the 1988 season.

Figure 1

Fig. 2. Detailed profiles of 210Pb activity versus depth in the firn for pits 1, 6 and 7. Pits were sampled at continuous 0.06 m intervals. The horizontal bars represent one sigma counting uncertainty. The depth of the winter layers was derived from δ18O profiles (not shown). The Chernobyl layer is from Dibb (1989).

Figure 2

Fig. 3. Detailed profiles of 210Pb activity versus depth in the firn for pits 1 and 2. Pits were sampled at continuous 0.06 m intervals. The horizontal bars represent one sigma counting uncertainty. The depth of the winter layers was derived from δ18O profiles (not shown). The Chernobyl layer is from Dibb (1989).

Figure 3

Fig. 4. 210 Pb deposition at the four sites during the two-year interval between the Chernobyl accident in late April, 1986, and sampling in May, 1988. The range in estimated deposition reflects the uncertainty in the density of the firn over the depth sampled. The low estimate for each pit assumes an average density of 300 kg m×3 and the high estimate assumes 400 kg m×3.