Radioisotope composition of atmospheric fallouts (snow water)
Based on the obtained analytical data on the content of 210Pbatm, 7Be and 137Cs in the studied snow samples, the specific activities and densities of radioisotope fallout at the sampling points on the Sherstobitovsky and Ubinsky burnt raised bogs were calculated. The results obtained correspond to the total atmospheric input of radioisotopes during the 4-month winter period of the stable snow accumulation. All data are linked to the date of snow sampling on March 11, 2018 (Table 1).
Тable 1 Specific activities of suspended matter of snow melt water and the fallout density of radioisotopes at the snow sampling points on the Sherstobitovsky and Ubinsky burnt raised bogs
Sample
|
Фракция
|
Fallout density, Bq/m2
|
Specific activity, mBq/l*
|
7Be/210Pbatm
|
Sherstobitovsky raised bog
|
210Pbatm
|
7Be
|
137Cs
|
210Pbatm
|
7Be
|
137Cs
|
1
|
9.7
|
6.8
|
0.11
|
90
|
64
|
1.1
|
0.71
|
2
|
18.7
|
13.8
|
0.16
|
175
|
129
|
1.5
|
0.74
|
3
|
3.6
|
2.7
|
0.07
|
34
|
25
|
0.67
|
0.74
|
4
|
4.9
|
30.6
|
0.27
|
46
|
287
|
2.5
|
6.2
|
Sum
|
|
36.9
|
53.9
|
0.61
|
345
|
505
|
5.77
|
1.5
|
Ubinsky burnt raised bog
|
1
|
16.1
|
11.5
|
0.08
|
157
|
112
|
0.76
|
0.71
|
2
|
14.8
|
12.5
|
< 0.01
|
144
|
122
|
0.04
|
0.85
|
3
|
4.5
|
3.0
|
0.03
|
44
|
29
|
0.30
|
0.66
|
4
|
3.9
|
23
|
0.10
|
38
|
221
|
0.98
|
5.8
|
Sum
|
|
39.3
|
5.0
|
0.21
|
383
|
484
|
2.08
|
1.3
|
1 — coarse-grained fraction (matter particles > 3 microns retained after decantation); 2 — fraction consisted of particles > 3 microns in size (the matter settled during filtration of snow melt water on a “blue-ribbon” filter); 3 — highly dispersed fraction consisted of particles 0.45–3 microns (the matter settled during successive filtration trough membrane filte; 4 — highly-dispersed fraction consisted of particles < 0.45microns (colloidal and dissolved components); * — snowmelt water.
Specific activities of 210Pbatm, 7Be and 137Cs in snow water with respect to the contribution of all granulometric fractions of suspended matter for snow samples taken at Sherstobitovsky raised bog are as follows: 345, 505 and 5.77 mBq/l, and at Ubinsky burnt raised bog 383, 484 and 2.08 mBq/l, respectively. The calculated values of 210Pbatm precipitation densities on the Sherstobitovsky (36.9 Bq/m2) and on the Ubinsky burnt (39.3 Bq/m2) raised bogs, as well as 7Be on the Sherstobitovsky (53.9 Bq/m2) and the Ubinsky burnt (50.0 Bq/m2) raised bogs were similar in values despite the farness distance of these raised bogs from each other by 110 km. This suggests that the input of these radionuclides in the composition of snowfalls was fairly uniform in the area. With respect to the short half-life period of 7Be, the real density of its precipitation during winter period will be significantly higher than the values given in table 1. As it may be supposed conditionally that the input of 7Be was uniform in time, then the density of its precipitation for entire period of snow accumulation with reference to radioactive decay, it can be estimated according to the technique (Aba et al., 2016) at the level of 112 Bq/m2 for the Sherstobitovsky raised bog and 104 Bq/m2 for the Ubinsky raised bog. It should be noted low specific activities of 137Cs in the suspended matter of snow water of the Sherstobitovsky and Ubinsky burnt raised bogs such as 5.77 and 2.08 mBq/l respectively as compared with specific activities of 210Pbatm and 7Be. This indicates insignificant contemporary intake of this manmade radionuclide from the atmosphere to the Earth’s surface. It should be noted that specific activities of 137Cs in the studied samples are close to the detection limit of the used analytical method. Consequently, the error of their determination often exceeds the value of 20–30%, which makes it impossible to perform statistical interpretation of the data for 137Cs in conjunction with 210Pbatm and 7Be.
The share contribution of granulometric fractions of suspended matter of snow water into the common specific activity of 210Pbatm and 7Be has being studied (Table 2).
Table 2
Share of granulometric fractions % of suspended matter of snow samples in the common activity of studied radioisotopes
Sherstobitovsky raised bog
|
Fraction
|
210Pbatm
|
7Be
|
137Cs
|
1–2
|
77
|
38
|
44
|
3
|
10
|
5
|
12
|
4
|
13
|
57
|
44
|
Ubinsky burnt raised bog
|
1–2
|
79
|
48
|
37
|
3
|
11
|
6
|
15
|
4
|
10
|
46
|
48
|
1–2 is sum of fractions, where 1 is the matter composed of particles with sizes > 3µm remained after decantation and 2 is the matter settled during filtration of snow water on a filter “blue ribbon”; 3 is fine fraction of particles with sizes 0.45–3 3µm (matter settled during sequential filtration through membrane filter); 4 — fine fraction with particles < 0.45 3µm (colloidal and dissolved components). |
The comparative analysis of contributions of granulometric fractions showed that:
1) Most of 7Be (46–57%) is associated with a fine fraction of suspended matter consisted of particles with sizes of less than 0.45 3µm. In this fraction, the specific activity of 7Be is 5.8–6.2 times higher than that of 210Pbatm (Table 1). The share of the coarse-grained fraction of a suspended matter in the total activity of 7Be is 38% for Sherstobitovsky raised bog and that is 48% for the Ubinsky burnt raised bog.
2) The share of the fraction of suspended matter consisted of particles with sizes from 0.45µm to 3 3µm is so small just as for 210Pbatm, and so 7Be in all studied samples of snow water and it is no more than 11%.
3) The main share of 210 Pbatm (77–79%) in the studied samples of suspended matter in snow water is in the composition of a coarse-grained fraction mainly represented by dusty particles of various sizes.
Thus, the main concentrator of the 7Be radioisotope is a fine fraction consisted of colloids and a dissolved component (fraction particles < 0.45 µm), and 210Pbatm is concentrated mainly in a coarse-grained fraction of suspended matter consisted of dust particles (> 3 3µm).
The important value characterizing the source of radioisotope intake on the Earth's surface is the 7Be/210Pbatm ratio (Melgunov et al., 2019a). The data presented in Table 1 demonstrate that very close values of 7Be/210Pbatm ratios: from 0.71 to 0.74 with an average of 0.73 for the Sherstobitovsky raised bog and 0.66–0.85 (average of 0.74) for the Ubinsky burnt raised bog. Such proximity of the 7Be/210Pb ratios indicates the same source of dust particles settled out at sampling points. This dust, most likely, is represented by soil particles raised from a surface as a result of soil aeolation and transported with continental air masses from the arid regions of Central Eurasia. In this coarse-grained fraction, significantly lower values of 210Be/Pbatm ratios are observed as compared to the fraction with particles < 0.45 µm (6.2 and 5.8). With respect to the short half-life of 7Be, it should be assumed that such particles succeed to the initial values of 7Be/210Pbatm ratios, which are inherent to them initially when they are located in the upper horizons of the soil cover.
Based on the data given in Tables 1 and 2, it can be stated that the separation according to granulometric fractions of the suspended matter in snow water shows that the studied radioisotopes are present in all isolated fractions (from the largest particle sizes > 3 µm to the smallest ones < 0.45 µm associated with nanoscale aerosol particles, colloidal and dissolved component). Specific activities of 137Cs in suspended matter of snow water of both the Sherstobitovsky and Ubinsky burnt raised bogs (5.77 and 2.08 mBq/l respectively) are significantly less as compared to those 210Pbatm and 7Be.This indicates the resent insignificant contents of this radionuclide in the atmosphere.
The distribution of radioisotopes in the vertical profile of the Sherstobitovsky burnt bog
For the first time, the data on distribution of natural (238U, 210Pb, 226Ra, and 40K) and manmade (137Cs) radioisotopes in the section of the Sherstobitovsky peat bog have been obtained (Table 3). Its peat core is composed of highmoor peat. The upper layer is formed mainly by remains of sphagnum mosses (S. magellanicum and S. angustifoliun) to the depth of 25 cm, the layer 25–35 cm is formed by pine-sphagnum peat (pine remains make up 30%), and the layer 35–40 cm is represented by pine peat.
Table 3
Contents of radioactive elements in the vertical profile of peat deposit of the Sherstobitovsky raised bog
Interval,
cm
|
U-238
|
U
|
Ra-226
|
Pb-210
|
K-40
|
K
|
Cs-137
|
Ra/U
|
Bq/kg
|
g/t
|
Bq/rg
|
Bq/rg
|
Bq/kg
|
%
|
Bq/rg
|
0–2
|
14
|
1.1
|
18
|
593
|
42
|
0.14
|
54
|
1.3
|
2–4
|
2.6
|
0.2
|
17
|
585
|
< 25
|
< 0.08
|
54
|
6.5
|
4–6
|
2.8
|
0.2
|
16
|
619
|
71
|
0.23
|
99
|
5.7
|
6–8
|
6.7
|
0.5
|
25
|
478
|
114
|
0.38
|
169
|
3.7
|
8–10
|
6.5
|
0.5
|
25
|
333
|
42
|
0.14
|
35
|
3.8
|
10–12
|
11
|
0.9
|
15
|
224
|
35
|
0.12
|
17
|
1.4
|
12–14
|
< 2.5
|
< 0.2
|
17
|
176
|
< 25
|
< 0.08
|
15
|
> 6.8
|
14–16
|
< 2.5
|
< 0.2
|
19
|
112
|
27
|
0.11
|
15
|
> 7.6
|
16–18
|
< 2.5
|
< 0.2
|
20
|
110
|
< 25
|
< 0.08
|
12
|
> 8.0
|
18–20
|
< 2.5
|
< 0.2
|
28
|
108
|
< 25
|
< 0.08
|
12
|
> 11.2
|
20–22
|
< 2.5
|
< 0.2
|
18
|
120
|
< 25
|
< 0.08
|
18
|
> 7.2
|
22–25
|
< 2.5
|
< 0.2
|
18
|
111
|
49
|
0.16
|
33
|
> 7.2
|
25–30
|
10
|
0.8
|
21
|
121
|
30
|
0.12
|
31
|
2.1
|
30–35
|
16
|
1.3
|
24
|
38
|
< 25
|
< 0.08
|
9
|
1.5
|
35–40
|
< 2.5
|
< 0.2
|
21
|
22
|
< 25
|
< 0.08
|
6
|
> 8.4
|
Mass contents of U and K were calculated in terms of specific activities of 238U and 40K judging from the following ratios: activity 1 mg U corresponds to 12.432 Bq of U238; 1% K corresponds to 303.1 Bq of 40K. |
The shape of the 210Pb distribution curve through the depth of the studied peat core of the Sherstobitovsky raised bog makes it possible to date the upper horizons up to the depth of 35 cm. Nonequilibrium 210Pb (Pbex) gradually settled on the Earth’s surface from the atmosphere is often used for dating the upper, near-surface layers of ombrotrophic peat bog up to the age of 150–200 years (Appleby et al., 1997; Bao et al., 2010; Bobrov et al., 2019; Clymo et al., 1990; El-Daoushy et al., 1982; Gavshin et al., 2004; Holynska et al., 1998; Oldfield et al., 1979). 210Pb (half-life T1/2=22.3 years) is a natural radioactive element included into the 238U radioactive series. The source of Pbex in the atmosphere is 222Rn. Radon (222Rn), being a decay product of 226Ra and gas, emits from the Earth's surface. Having a half-life (T1/2) of 3.82 days, 222Rn decays into 210Pb over a short time period through a series of short-lived isotopes. At the moment of formation, radon atoms and their decay products are electrically charged. This leads to their rapid sorption by aerosol and dust particles in the atmosphere. In the composition of these particles, Pbex gradually is settled on the Earth's surface. This process is continuous. Settled on the surface of stratified formations such as lake sediments or peat deposits, Pbex is gradually superposed by younger formations. In the absence of processes leading to vertical migration, the further behavior of buried Pbex is governed by the law of its radioactive decay. This provides the basis of methods for dating stratified formations by nonequilibrium 210Pb. As a rule, the model of permanent stream of Pbex (CRS is Constant Rate of Supply) is used for dating the upper horizons of ombrotrophic peat bog deposits (Appleby, 2002; Appleby and Oldfield, 1978). The CRS model, as applied to the dating of peat deposits, is assumed the presence of two main initial conditions, namely: 1) The rate of Pbex precipitation from the atmosphere is the constant magnitude throughout the entire period of material accumulation; 2) There is no significant vertical redistribution of Pbex after its burial. The model takes into account the possibility of changing the rate of biomass growth over the entire dating period.
According to the CRS model, the age of the lower surface of the horizon being dated is calculated by the formula (Appleby, 2002; Sanchez-Cabeza and Ruiz-Fernández, 2012):
t(i) = λ−1 ln(A(0)/A(i)) (1),
where i is the number of the dated horizon, λ is the decay constant of 210Pb (year− 1), А(0) is a cumulative supply of Pbex in the dated section of peat (Bq m2), A(i) is a cumulative supply of Pbex in the dated section of peat bog (Bq m− 2), and A(i) is the cumulative supply of Pbex in the dated (Bq m− 2). The cumulative supply of Pbex below the dated horizon (Bqm− 2). The cumulative supply is calculated through specific activities of 210Pb defined for each horizon of the dated section by applied analytical method with reference to the data on the density of dry matter in the studied peat bog material. The activity of a nonequilibrium (atmospheric) Pbex is equal to the difference between the total activity of 210Pb in the sample and the activity of 210Pb being in balance with the parent 226Ra. Complementary to dating the upper horizons of a peat deposit, the CRS model provides an estimate of dry material accumulation rates, which can be determined using the formula:
r(i) = λ A(i)/C(i)) (2),
where C(i) is the specific activity of Pbex on the surface separating i and i + 1 dated layers.
The results of calculation of age-related characteristics for the upper part of the Sherstobitovsky peat bog are given in Table 4 and in Fig. 2.
Table 4
Age-related characteristic of the upper part of Sherstobitovsky raised bog
Interval
|
Р
|
Сi
|
i
|
Аi
|
А(i)
|
t(i)
|
Year of forrmation
|
r(i)
|
cm
|
g cm− 3
|
Bq/kg− 1
|
cm
|
Bq
m− 2
|
Bq
m− 2
|
years
|
g cm− 2 year− 1
|
|
|
|
0
|
0
|
2762
|
0
|
2013
|
|
0–2
|
0.0353
|
575
|
2
|
406
|
2356
|
5
|
2008
|
129
|
2–4
|
0.0353
|
568
|
4
|
401
|
1955
|
11
|
2002
|
104
|
4–6
|
0.0364
|
603
|
6
|
439
|
1516
|
19
|
1994
|
90
|
6–8
|
0.0375
|
453
|
8
|
340
|
1176
|
27
|
1986
|
96
|
8–10
|
0.0375
|
308
|
10
|
231
|
945
|
34
|
1979
|
114
|
10–12
|
0.0411
|
209
|
12
|
172
|
773
|
41
|
1972
|
131
|
12–14
|
0.0411
|
159
|
14
|
131
|
642
|
47
|
1966
|
159
|
14–16
|
0.0394
|
93
|
16
|
73
|
569
|
51
|
1962
|
194
|
16–18
|
0.0376
|
90
|
18
|
68
|
502
|
55
|
1958
|
184
|
18–20
|
0.0376
|
80
|
20
|
60
|
441
|
59
|
1954
|
151
|
20–22
|
0.0422
|
102
|
22
|
86
|
355
|
66
|
1947
|
114
|
22–25
|
0.0422
|
93
|
25
|
118
|
238
|
79
|
1934
|
77
|
25–30
|
0.0404
|
100
|
30
|
202
|
36
|
140
|
1873
|
19
|
30–35
|
0.0470
|
14
|
35
|
33
|
3
|
223
|
1790
|
11
|
35–40
|
0.0524
|
1
|
40
|
|
|
|
|
|
Р is density of dry matter of peat within interval; Ci is specific activity of Pbex within interval; i — dated horizon; Ai is supply of Pbex in interval; A(i) is cumulative supply of Pbex below dated horizon; r(i) is rate of dry peat accumulation. |
Using the CRS model allowed us to perform reliable dating to the horizon of 30 cm, the age of which was estimated at 140 years. Verification of correctness of the applied approach can be performed by the distribution nature of manmade 137Cs, whose intake to the peat deposit is associated with local and global fallouts due to involvement of this isotope into atmospheric migration as a result of open nuclear test operations at the Semipalatinsk nuclear and other testing grounds during the period from 1949 to 1963, accidents at the Chernobyl (1986), and Fukushima (2011) nuclear power plants (NPP). In the graph of the vertical distribution of 137Cs shown in Fig. 2, there is observed a peak of activity in the lower part of the section, the upper limit and maximum of which is quite likely corresponds to the age-related verge.
Some blurring of the peak is probably associated with redistribution mechanisms of 137Cs in connection with significant fluctuations in the groundwater level (GWL) of both seasonal and annual ones, which are specific for a zone of the unstable heat and water supply as described in (Bogs of Western Siberia…, 1976) According to data from the Barabinsk weather station, the increase in water cut of a bog under conditions of the directed decrease in temperature and the increase in precipitation during the period from 1967 to 1986 years could contribute to the displacement of this peak, that is, the diffusion of 137Cs into the underlying layers of the peat deposit (All-Russian Research…, 2020). Under conditions of cooler and wetter climate, the duration of finding the upper horizons in a wet state increases, which should contribute to diffusion of 137Cs into the lower layers of the peat. The diffusion of 137Cs occurred in the layer of sphagnum peat, sharply decreasing, judging by its activity, in the layers of pine-sphagnum and pine peats.
In the upper part of the 137Cs distribution graph, there is observed a pronounced peak of its content on the time scale corresponding to the mid 80–90 years of the twentieth century, and the time of the maximum formation corresponds to the interval of 1986–1990 years. This increase in the specific activity of 137Cs could be partly attributed to the fallouts associated with emergency in the Chernobyl NPP (nuclear power plant). But such significant increase cannot be explained by only this occasion. It is most likely that here the influence of other sources of the 137Cs intake were superimposed on the insignificant contribution of the Chernobyl component. Usually, the maximum of its content in peat deposits in different regions of the Holarctic is peculiar to the peat layer deposited during the period of mass nuclear tests (Clymo, 1984). In the southern taiga subzone of Western Siberia, under conditions of a more humid climate compared to the forest-steppe, this peak of 137Cs (accepted as in 1963 year) is located at different depths of peat deposits. In this case, the tendency for dependence of its depth occurrence on the degree of stability of the water regime and activity of peat accumulation is identified. On native actively growing bogs, 137Cs is found at depths of 31–43 cm on naturally and anthropogenically drained ones at 16–21 cm, and on highly dehydrated ones at 9–12 cm (Preis et al., 2010), which is similar to the upper peak of 137Cs in peat deposits of the Sherstobitovsky raised bog. This similarity is explained by the fact that the core of this raised bog was sampled: 1) on the peripheral part of the bog, the water regime of which was also somewhat disturbed by the building a bypass channel of the reclamation system, 2) in the depression between sphagnum hummocks, where the peat growth was usually very low. However, the difference of this core from those of the south taiga is the presence of two 137Cs peaks, which does not allow us to date the upper peak at 8 cm to 1963.
It is known (Efremova et al., 2020) that the effect of fluctuations of groundwater levels is the main reason governing the boundary of vertical migration of 137Cs in peatlands. According to the data from the Barabinsk weather station (All-Russian Research…, 2020) during the period from 1987 to 2009 years, air temperatures were increased and the amount of liquid precipitation, just as average annual and so summer ones was decreased. Under conditions of climate aridization, fluctuations in the groundwater level (GWL) were intensified and this level was sharply decreased during warm seasons of the year. In contrast to the cooler and wetter period in 1967–86 years, when transpiration by helophytes (evaporation of water through leaf stomata) was less active, the sharp increase in transpiration under hot and dry conditions causes active suction of peat water and biophilic transfer of trace elements by plant roots from the lower peat horizons. It is common knowledge that 137Cs replaces biophilic 40K element in biochemical cycles of plant organic matter production (Kabata-Pendias and Pendias, 1989). This replacement process is especially active in the raised bogs, which are characterized by potassium deficiency. Therefore, it is likely that the peak of 137Cs at the depth of 8 cm is largely due to the transfer of the main amount of 137Cs deposited in 1949–1963 to the overlying horizons. This also explains the low activity of the lower 137Cs peak. This replacement process is especially active in the high-moor peats for which the potassium deficiency is intrinsic. Therefore, it is likely that the peak of 137Cs at a depth of 8 cm is largely due to the transfer of the main amount of 137Cs deposited in 1949–1963 years into the overlying horizons. This explains the low activity of the lower peak of 137Cs. According to this assumption, the different nature of 137Cs redistribution in the peat deposits of the Barabinsk forest-steppe during various time periods is largely due to the difference of their climatic parameters.
The assumption of a significant impact of fluctuations of a peat water level on the 137Cs migration is supported by two more facts.
Firstly, according to the data obtained with the help of the Automatic UPV Recorder (AKR4-logers), significant seasonal fluctuations of the groundwater level (GWL) of the Sherstobitovsky raised bog from September 2017 to September 2018 were revealed. During the snowmelt period, the GWL was raised from 80 cm (March 2018) to 35 cm (April) and it continued to rise to 10 cm from the surface (May). In summer, the GWL was reduced with specific sharp rises after precipitation and gradually decreased due to evaporation and runoff up to 30 cm. The highest values of GWL standing in the Sherstobitovsky raised bog up to 10 cm from the surface were recorded during the spring period at the peat core sampling point, which corresponds to the upper peak of 137Cs.
Secondly, the nature of the vertical distribution of the 40K isotope (Table 1 and Fig. 2) is a geochemical analog of Cs, which almost completely coincides with the distribution of 137Cs. Here, also, at the general low level of potassium contents (< 25 Bq/kg of 40K, with conversion to K < 0.08%) in horizons 4–12 cm and 22–30 cm, increased 40K activities reaching in the peak 114 Bq/kg and 49 Bq/kg, respectively, are observed. During summer period, when increasing transpiration (evaporation) of water through stomata of plant leaves takes place, the suction of peat water and its active transport by plant roots occurs along with biophilic 40K and 137Cs from the lower peat horizons.
Thus, significant GWL fluctuations stipulate just as blurring, so displacement of the 137Cs activity peaks, that should be taken into account when they are used for dating peat deposits.
In addition, frequent fires should be contribute to the increase of the specific 137Cs activity under conditions of climate aridization. It is known that almost all the raised bogs of the Barabinsk forest-steppe were subjected to multiple fires. Increasing ash-contents of the upper 15-cm peat layer in the Sherstobitovsky raised bog from 4.3 to 6.0–9.6%, in the absence of embers as traces of fires on the site of the raised bog, indicates the contamination of the Baraba atmosphere. This cannot be explained only by global anthropogenic pollution of the atmosphere as since 1985 it began to be purified as well as over Western Siberia (Preis et al., 2010). The significant burning of peat in the bogs of the Barabinsk forest-steppe, in particular in the Ubinsky burnt raised bog (Leonova et al., 2018), is indicated by an increase in the ash content in the surface layers of burnt peat in 0–22 cm from 3.7 to 14.5%, on average, to 6.4%, respectively. This is also evidenced by the occurrence of peat layers with the maximum activity of 137Cs (158–196 Bq/kg) directly on the surface (0–6 cm) in the burnt area of the Ubinsky burnt raised bog. Therefore, an additional contribution to the high activity of the 137Cs in the upper peak in a core from the Sherstobitovsky raised bog is quite likely due to secondary fallout of this radioisotope from the atmosphere as a result of fires.
The nature of the vertical distribution of 238U and 226Ra included in the natural radioactive uranium series is interesting. The 226Ra activity varies over the section in the narrow interval from 15 to 25 Bq/kg, at the average of 20 Bq/kg. The activity of 238U is significantly lower, which indicates the significant disequilibrium of the radioactive balance between uranium and radium in favor of the latter. Thus, the Ra /U ratio varies in the very wide range reaching minimum values of 1.3, 1.4, 1.5, and 2.1 in the horizons 0–2, 10–12, 30–35, and 25–30 cm. The maximum values of the Ra/U ratios correspond to the horizons 2–6, 12–25, and 35–40 cm reaching the maximum of 11.2 in the horizon 18–20 cm. Such radioactive disequilibrium between 238U and 226Ra is not unusual. 226Ra is intensely absorbed by plants. Its biological absorption coefficients (BAC) calculated as ratios of specific radionuclide activities in an ash of vegetation and soil, are usually, as a rule, greater than 1 (Aleksakhin et al., 1990; Markose et al., 1993). Moreover, it was previously shown (Noskova and Shuktomova, 2010) that the highest BAC values are observed in woody species: mountain ash (Sorbus aucuparia) and pubescent birch (Betula pubescents), the concentrations of radionuclide in which can exceed its concentration in the soil up to 1575 and 399 times, respectively. For herbaceous species, the BAС are lower, but they can reach values significantly greater than 1. For example, for fireweed (Chamaenerium angustifolium), BAС can reach up to 14.8 and for wild angelica (Angelica silvestris) up to 1.98. Thus, vegetation, especially some of the woody species, can be attributed to concentrators of 226Ra. For 238U, BAС > 1 are not typical. The BAC of 226Ra exceed that of 238U by 1–2 orders of magnitude for herbaceous vegetation species and by 2–4 orders of magnitude for woody species. From all of the above, it follows that under natural conditions, vegetation will accumulate 226Ra much more intensively than 238U. Table 5 shows the results of determining the contents of radioactive elements in the biogeocoenosis components from the Ubinsky burnt raised bog sampled on the background (unburned) site. The data given in Table 5 show that radioactive disequilibrium in favor of 226Ra in the coupe U-Ra is observed for all studied samples. In the forest floor and in the upper sod horizon of soils, 226Ra is 1.59 times greater than its equilibrium contents. Still greater excess of 226Ra is observed in green moss Polytrichum commune Hedw. (1.7) and in sphagnum moss Sphagnum magellanicum (2.13). As it was expected, the highest values of Ra/U ratios are found in terrestrial vegetation: this ratio in birch leaves is obviously greater than 10, and that in red bilberry leaves is 14.7. Thus, in all components of the phytocoenosis, the remains of which form a peat deposit, the significant excess of 226Ra is observed relative its equilibrium contents. Having regard to the long half-life period of 226Ra constituting ~ 1500 years, such state can be kept in the course of very extended time period (5–6 half-life periods of radium), provided that there are no processes leading to significant migration of uranium and radium. It is seen from the data given in Table 1 that the contents of 226Ra in the horizon of 35–40 cm are close to mean values throughout a section and they amount to 21 Bq/kg. Here the contents of 238U are low and do not exceed 2.5 Bq /kg. At the same time, the activity of 210Pb, amount to 22 Bq /kg, is close to values being in balance with 226Ra values. This suggests that superfluous atmospheric 210Pbex has already decayed. The entire amount of 210Pb situated in this horizon is extremely related to the radioactive decay of 226Ra. The assemblage of these facts shows that during the last 250 years at least, there were no processes leading to significant removal or input of radioactive elements within the region under study. It should be noted that for both 226Ra and 238U in the nature of their vertical distribution, the same regularity is traced as it is for 137Cs and 40K. In the horizons 6–12 cm, as well as in the lower part of the section (25–35 cm), the increase of activities of these radionuclides is observed. This indicates that the curvatures of the vertical distribution of these radioactive elements in the Sherstobitovsky peat bog were formed at the expense of the same processes.
Table 5
Radioactive elements in components of biogeocoenosis on the background site of the Ubinsky burnt raised bog
|
U-238
|
U-238
|
Pb-210
|
Ra-226
|
Cs-137
|
К
|
K-40
|
U/Ra
|
g/t
|
Bq/kg
|
Bq/kg
|
Bq/kg
|
Bq/kg
|
%
|
Bq/kg
|
|
Drained peat soil
|
0.65
0.47–0.69
|
8.1
5.8–8.6
|
596
643–753
|
12.9
7.2–15.1
|
203
174–279
|
0.39
0.22–0.47
|
117
68–141
|
1.59
|
Litter
|
0.26
0.16–0.32
|
3.2
2.0–4.0
|
721
603–856
|
5.1
4.9–5.2
|
113
83–150
|
0.21
0.20–0.21
|
63
60–65
|
1.59
|
Polytrichum commune
|
0.16
0.11–0.23
|
2.0
1.4–2.9
|
419
307–547
|
3.4
3.0–3.9
|
65
61–74
|
0.31
0.26–0.41
|
95
79–123
|
1.70
|
Sphagnum magellanicum
|
0.14
0.13–0.14
|
1.7
1.6–1.8
|
397
374–419
|
3.3
3.1–3.4
|
64
61–67
|
0.43
0.41–0.45
|
130
123–136
|
1.94
|
Birch leave
|
< 0.01
|
< 0.15
|
65
59–75
|
1.5
1.2–1.8
|
18
18–19
|
0.44
0.38–0.51
|
133
116–154
|
> 10.0
|
Cowberry leave
|
0.02
002–0.03
|
0.29
0.20–0.36
|
60
55–70
|
4.4
3.8–4.7
|
18
16–20
|
0.26
0.22–0.29
|
79
68–88
|
14.7
|