RESIDENCE TIMES OF ARCTIC HAZE AEROSOLS USING SHORT-LIVED RADIONUCLIDES

M. Baskaran1 and G. E. Shaw2

1: Department of Geology, Wayne State University, Detroit, MI 48202 (E-Mail: Baskaran@chem.wayne.edu)

2: Geophysical Research Institute, University of Alaska, Fairbanks, AK 99775

 

ABSTRACT:

Pollutants from mid latitudes (mainly from Eurasia) reach the polar regions through long-range atmospheric transport during winter. Due to very low precipitation in the arctic region, the pollutant-laden aerosols in the stable, and dark polar atmosphere are believed to have relatively longer residence times. The disequilibrium between the daughter products of radon-222, in conjunction with the concentrations of 7Be in arctic aerosols can be utilized to obtain information on the residence times and sources of the arctic haze.

                We have analyzed 8 aerosol samples from two stations, Poker Flat and Eagle, Alaska for the concentrations and activity ratios of 7Be, 210Po, and 210Pb. The activity ratios of 210Po/210Pb varied between 0 and 0.18. The corresponding residence time obtained using the disequilibrium between the 210Po and 210Pb, varied between 0 and 39 days.    It appears that there is no extraneous source of 210Po to the arctic and most of the 210Po is derived from the decay of 210Pb locally. This is the first time an estimate on the residence time of aerosols from the arctic haze is determined. The 7Be/210Pb activity ratios varied between 0.6 and 14.0, possibly suggesting varying inputs of 7Be to the arctic atmosphere. Since long-range atmospheric transport is one of the major pathways of arctic pollution, this study has potential significance on the fate and transport of inorganic and organic atmospheric pollutants in the arctic region.

 

INTRODUCTION:

                Two classes of radionuclides have been used for the determination of the residence time of aerosols as well as other atmospheric processes.  They include: (i) radioactive decay products of radon which emanates from continental surfaces into the atmosphere, and (ii) radionuclides in the atmosphere produced by cosmic-ray interactions.  Of these two classes, beryllium-7 (half-life = 53.3 d) and lead-210 (half-life = 22.1 y) are two radionuclides, which have been widely used as tracers in atmospheric systems [e.g., Martell and Moore, 1974; Poet et al., 1972; Turekian et al., 1977; Baskaran, 1995].  Even though the sources of these two nuclides to the atmosphere are distinctly different, both are highly particle-reactive and thus get attached to aerosols in the atmosphere. 

                The Arctic haze is believed to be derived largely from long-range transport of midlatitude pollution products (Rahn, 1982).  Earlier studies indicated that the concentrations of 210Pb in Arctic aerosols are the highest so far documented in the world, suggesting that most of the 210Pb are likely continent-derived.  Information obtained from the satellite measurements and weather records from ships and islands have revealed that the amount of precipitation in the oceans adjoining the Arctic regions, such as North Atlantic and North Pacific, are considerably higher during winter than those in the continents.  This will result in efficient removal of aerosols in the oceans.  Thus, the continental pathway is a much more efficient transporter of aerosol to the Arctic than the Atlantic or Pacific marine pathway (Rao et al., 1976; Rahn, 1982). The marine air should be highly scavenged, while that of the stagnant Arctic air (polar air mass) should be relatively old (10-100 days, Shaw, 1991). 

During the long-range atmospheric transport of air masses from sub-polar regions, if all the particle-reactive radionuclides produced from the decay of 222Rn during long-range atmospheric transport are scavenged from the atmosphere before reaching the arctic area, then, almost all of 210Pb and its daughter products (210Bi, half-life =5.01 days and 210Po, half-life = 138 days) in the arctic aerosols would be produced from the decay of 222Rn.  In such a case, the disequilibrium between 210Pb and 210Po can be utilized to obtain the residence time of aerosols under the assumption that these nuclides are instantaneously removed on to aerosols after their production.  It is pertinent to point out that the time span of the existence of arctic haze is only 4-5 months and is comparable to the mean-life of 210Po and hence the 210Po/210Pb ratios can be utilized to obtain information on the residence time of aerosols from the arctic haze.  This is the first attempt to determine the residence time of aerosols collected from the arctic haze.

 

MATERIALS AND METHODS:

                Large volume air samples from Poker Flat (65.1 N; 147.5 W) and Eagle (65.9 N; 141.2 W) were filtered through an air filtration assembly at a typical flow rate of 1 m3/minute.  Whatman 41 cellulose fiber filter was utilized for the collection of aerosols.  All the samples analyzed in this study were collected between January and March 1996.  The time of collection varied between 2 and 8 days (Table 1).  One half-section of the filter was digested (with 12 ml 6M HCl + 2ml Conc. HNO3 + 0.8 ml conc. HF) in a microwave for 2 hours.  After the digestion was complete, the solution was dried and taken in dilute HCl and then transferred into a gamma counting vial.  After gamma counting the vial for 7Be and 210Pb, the solution was further processed for polonium plating after adding 209Po spike.  Polonium was electroplated onto a silver planchet and then the planchet was counted in an alpha spectrometer.  The activities of 210Po, 210Pb and 7Be were corrected for decay and ingrowth from the mid-time of collection to the time of counting.  The errors reported are propagated errors arising from the one sigma counting uncertainty due to detector calibration and background correction.

 

RESULTS AND DISCUSSION:

                The concentrations of 7Be, 210Pb and 210Po on the 10 samples are given in Table 1.  The concentrations of 7Be varied between 99 to 339 dpm m-3, with a mean value of 158 dpm m-3.  Concentrations of 210Pb and 210Po varied between 13.4 and 155 dpm m-3 (mean value = 42.7 dpm m-3) and below detection limit and 9.11 dpm m-3 (mean value = 2.51 dpm m-3), respectively.  The activity ratios of 210Po/210Pb and 7Be/210Pb varied between 0 to 0.177 (mean value = 0.085) and 0.55 and 14.0 (mean value = 5.8), respectively.

                The residence time of aerosols based on the disequilibrium between 210Po-210Pb is given in Table 1.  This residence time is based on the following assumptions:

i)                     The initial concentration of 210Po is zero at the time when the aerosols reach the arctic (210Pb concentration need not be zero for the determination of residence time using 210Po/210Pb disequilibrium); and

ii)                    The entire Po is derived from the decay of 210Pb and there is no extraneous source(s) of 210Po to the aerosols collected for this study. 

Earlier studies based on 210Bi/210Pb activity ratios on the residence times of aerosols for the continental United States yielded a few days while that of 210Po/210Pb resulted in a month or more (summarized in Moore et al., 1976 and Robbins, 1978).  This discrepancy of residence times between 210Bi/210Pb and 210Po/210Pb was attributed to the additional sources of 210Po to the atmosphere, including dust storms, coal-burning power plants, forest fires, and plant exudates (Moore et al., 1976).  Unlike the earlier studies in the continental United States and other places (e.g., Moore et al., 1976), additional sources of 210Po to the study area are likely insignificant.  From an evaluation of various sources of 210Po to the atmosphere in the continental United States, Moore et al. (1976) estimated that the suspended soil particles could account for 53% of the additional sources of 210Po, 37% due to release from plant exudates, 3.2 % from stratospheric injection, 0.8% from forest fires, and the remaining 5.8% from anthropogenic sources (including phosphate fertilizer dispersion, by-product gypsum, lead production, cement and other metal production, and fossil fuel burning).  The relative importance of each of these sources to the winter arctic air is unknown; however, certain input terms during winter such as anthropogenic (in the form of phosphate fertilizer, fossil fuel burning, etc.), suspended soil particles, release from plant exudates (ability of leaf surfaces to collect and retain 210Pb and 210Po aerosols were reported by Moore et al., 1976) are likely negligible.  During the long-range transport of aerosols from Europe and Asia through the upper atmosphere, it is likely that most of the daughter products of 222Rn  (210Po, 210Bi, and 210Pb) are removed and only 222Rn reaches the arctic air.  Recent study by Kim et al. (2000) on the atmospheric fallout of 7Be, 210Pb and stable Pb in the Chesapeake Bay area indicates that stable Pb is mainly transported from remote areas through the upper atmosphere while 210Pb transport is primarily through lower atmosphere.  In addition, information obtained from the satellite measurements and weather records from ships and islands have indicated that the amount of precipitation in the oceans adjoining the Arctic regions, such as North Atlantic and North Pacific, are considerably higher during winter than those in the continents.  This will result in efficient removal of aerosols in the oceans (Rao et al., 1976).  However, the pollutants that reach the arctic are likely transported from remote areas through the upper troposphere without much removal.  When 222Rn alone are transported to the arctic and there is no additional source of 210Po other than from the decay of 210Pb, the residence time calculated using the 210Po/210Pb ratio will be a realistic value of the residence time of aerosols.

The residence times varied between 0 to 39±3 days (Table 1).  As we discussed before, earlier studies using 210Po-210Pb disequilibrium for the continental United States resulted in residence times of >1 month and our values of ~ 0 days on two samples (Eagle -1 and 2) likely indicate that there are no additional sources of 210Po to the arctic air.  The arctic haze typically lasts for about 3-4 months during winter and if the aerosols in the haze stay for that long, then, the residence time of individual aerosol particles could vary from few days to 3-4 months.  In this context, the range obtained for the residence time seems quite reasonable.  It must be pointed out the reliability of this residence time critically depends on the initial concentration of 210Po in the incoming aerosols to the arctic region.  If there is some amount of 210Pb (but negligible amount of 210Po) present when the aerosols reach the arctic region, then, that would not affect the values of the residence time.  Since we do not have any other radionuclide data on the incoming aerosols prior to coming into the arctic region, we cannot rigorously address this issue.

 

Table 1: Sample location, concentrations of 7Be and 210Pb and activity ratios of 210Po/210Pb and7Be/210Pb of the aerosols from Arctic and non-Arctic haze.

 

Station

Date of Collection

(Days collected)

7Be

dpm/ 103 m3

210Po

dpm/ 103 m3

210Pb

dpm/ 103 m3

210Po/210Pb

Activity Ratio

7Be/210Pb

Activity Ratio

Residence

Time (days)

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

Poker Flat - 1

8 Jan. 1996

(8.0 d)

339.3

9.11±1.00

61.3±0.9

0.149±0.025

5.50

32±5

 

 

 

 

 

 

 

 

Poker Flat - 2

26 Feb. 1996

(2.0 d)

182.4

2.87±0.49

49.3±1.7

0.058±0.012

3.69

12 ±2

 

 

 

 

 

 

 

 

Eagle - 3

4 March 1996

(1.6 d)

109.5

1.05±0.49

16.5±2.0

0.063±0.037

6.60

13±7

 

 

 

 

 

 

 

 

Eagle -4

6 March 1996

(2.0 d)

253.9

3.20±0.23

18.1±0.6

0.177±0.016

14.0

39±3

 

 

 

 

 

 

 

 

Eagle- 5

8 March 1996

(3.5 d)

159.1

3.55±0.36

26.7±1.4

 

0.133±0.017

5.95

29±4

 

 

 

 

 

 

 

 

Eagle - 6

11 March 1996

(1.5 d)

126.8

1.55±0.45

33.2±2.2

0.047±0.016

3.81

10±3

 

 

 

 

 

 

 

 

Eagle - 7

13 March 1996

(2.3 d)

98.8

1.90±0.27

22.1±1.5

0.086±0.015

4.45

18±3

 

 

 

 

 

 

 

 

Eagle - 8

15 March 1996

(3.0 d)

152.3

1.90±0.23

13.4±1.5

0.141±0.025

11.3

30±5

 

 

 

 

 

 

 

 

 

Similar studies in the continental United States by Marenco and Fontan (1972) and Nevissi et al. (1974) showed that the 210Po/210Pb ratio in rain samples were high as compared to the aerosols indicating longer tropospheric aerosol residence times which also could be due to stratospheric air intrusions into the stratosphere during the passage of frontal systems (Moore et al., 1976). 

 

CONCENTRATIONS OF 7Be AND USE OF 7Be/210Pb ACTIVITY RATIOS AS ATMOSPHERIC TRACER:

                The 7Be concentration in 6 aerosol samples from Eagle station collected between a period of two weeks varied between 99 and 254 dpm m-3, with a mean value of 150 dpm m-3.  The concentrations of 7Be in aerosols are primarily controlled by three factors: (1) variations in the amount of precipitation which causes the change in the deposition fluxes as well as air concentrations of 7Be; (2) changes in the stratosphere-troposphere exchange during late winter and early spring seasons; and (3) variations in the amount of 7Be brought by long-range transport.  Since the production source functions of 210Pb and 7Be are distinctly different, a relatively high correlation between the concentrations of 7Be and 210Pb will provide information on the atmospheric removal behavior of these nuclides as well as information whether these two radionuclides can be used as independent atmospheric tracers (Todd et al., 1989; Baskaran et al., 1993; Baskaran, 1995).  The 7Be/210Pb activity ratios varied over a factor of 25 in the arctic aerosol samples while a factor of 15 has been reported in the precipitation samples from Galveston (Baskaran et al., 1993).

                The concentrations of 7Be plotted against 210Pb in the aerosol filter samples (Figure 2) indicate that there is a positive correlation between the two (r = 0.63, P < 0.1).  A strong positive correlation between the depositional fluxes of 7Be and 210Pb (in rainfall) was observed for several places suggesting that the atmospheric removal behavior of 7Be and 210Pb are relatively similar and that these two nuclides cannot be used as two independent atmospheric tracers (Todd et al., 1989; Baskaran et al., 1993).  From a synthesis of all the earlier published data on the depositional fluxes of 7Be and 210Pb, Baskaran et al. (1993) concluded that in most of the continental and coastal stations, 7Be and 210Pb cannot be used as two independent atmospheric tracers and only in oceanic and a few coastal stations, do 7Be and 210Pb fluxes seem to vary independently and in such places these nuclides can be used as independent air mass tracers.  Our data is limited and hence we are unable to address this issue from our pilot data set if these tracers can be used independent atmospheric tracers. More extensive database from several stations in the Arctic will enable us to address the issues on the sources and transport of arctic aerosols.

 

Conclusions:

From a limited number of samples, we can draw the following conclusions:

i) The activity ratios of 210Po/210Pb in arctic aerosol samples varied between 0 and 0.177 corresponding to a range of residence times between ~ 0 and 39 days.  This range of values is in contrast with earlier studies for the continental US where additional sources of 210Po were attributed to the longer residence time.  Thus it appears that there may not be any additional sources of 210Po to the arctic and most of the 210Po to the study area is derived from the decay of 210Pb present in the arctic air. 

ii) There appears to be correlation between 7Be and 210Pb, possibly suggesting that these tracers cannot be used as independent atmospheric tracers. 

More extensive study from the beginning till the disappearance of the arctic haze will enable us to determine the usefulness of 210Po/210Pb and 210Bi/210Pb disequilibria for the residence times of arctic haze.  In addition, such studies will also help to elucidate various sources of air to the arctic region.

 

ACKNOWLEDGEMENTS:

This work was supported in part by NSF grant (OCE-9732536).

 

BIBLIOGRAPHY

Baskaran M, Coleman CH and Santschi PH (1993) J. Geophys. Res., 98: 20,555-20,571.

Baskaran, M (1995) J. Geophys. Res., 100:2833-2840.

Kim G, Hussain N, Scudlark JR, Church TM (2000) J. Atmos. Chem. 36: 65-79.

Kuroda PK, Hodges HL, Fry LM, Moore HE (1962) Science 137: 15-17.

Marenco A, Fontan J (1972) Tellus 24: 38-46.

Martell AE, Moore HE (1974) J. Rech. Atmos. 8: 903-920.

Moore HE, Poet SE, Martell EA (1973) J. Geophys. Res. 78: 7065-7075.

Moore HE, Martell EA, Poet SE (1976) Environm. Sci. Technol. 10: 586-591.

Nevissi A, Beck JN, Kuroda PK (1974) Health Phys. 27: 181-188. 

Poet SE, Moore HE, Martell EA (1972) J. Geophys. Res. 77: 6515-6527.

Rahn KA (1982) On the causes, characteristics and potential environmental effects of aerosols in the Arctic atmosphere. In: The Arctic Ocean, (ed.: L. Rey), John Wiley, pp. 163-195.

Rao MS, Abbott VWV, Theon JS (1976) NASA SP-410, NASA, Washington, DC.

Robbins JA (1978) In: The Biogeochemistry of Radioactive Lead in the Environment. Ed.: J. O. Nriagu, pp. 285-393, Elsevier, New York.

Shaw GE (1991) J. Geophys. Res., 96, 22,357-22,368.

Todd JF, Wong GTF, Olsen CR, Larsen IL (1989) J. Geophys. Res. 94: 11,106-11,116.

Turekian KK, Nozaki Y, Benninger LK (1977) Ann. Rev. Earth Planet. Sci. 5: 227-255.