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Article

Radioactivity of Natural Nuclides (40K, 238U, 232Th, 226Ra) in Coals from Eastern Yunnan, China

1
School of Environment Science and Spatial Informatics, China University of Mining and Technology, Xuzhou 221000, China
2
Chinese Academy of Sciences Key Laboratory of Crust-Mantle Materials and the Environments, School of Earth and Space Sciences, University of Science and Technology of China, Hefei 230026, China
3
College of Life Sciences, Huai Bei Normal University, Huaibei 235000, China
*
Author to whom correspondence should be addressed.
Minerals 2015, 5(4), 637-646; https://doi.org/10.3390/min5040513
Submission received: 29 June 2015 / Revised: 11 September 2015 / Accepted: 18 September 2015 / Published: 30 September 2015
(This article belongs to the Special Issue Minerals in Coal)

Abstract

:
The naturally occurring primordial radionuclides in coals might exhibit high radioactivity, and can be exported to the surrounding environment during coal combustion. In this study, nine coal samples were collected from eastern Yunnan coal deposits, China, aiming at characterizing the overall radioactivity of some typical nuclides (i.e., 40K, 238U, 232Th, 226Ra) and assessing their ecological impact. The mean activity concentrations of 238U, 232Th, 40K and 226Ra are 63.86 (17.70–92.30 Bq·kg−1), 23.76 (11.10–37.10 Bq·kg−1), 96.84 (30.60–229.30 Bq·kg−1) and 28.09 Bq·kg−1 (3.10–61.80 Bq·kg−1), respectively. Both 238U and 232Th have high correlations with ash yield of coals, suggesting their inorganic origins. The overall environmental effect of natural radionuclides in studied coals is considered to be negligible, as assessed by related indexes (i.e., radium equivalent activity, air-adsorbed dose rate, annual effective dose, and external hazard index). However, the absorbed dose rates values are higher than the average value of global primordial radiation and the Chinese natural gamma radiation dose rate.

1. Introduction

Combustion of coals that are enriched in radioactive nuclides, particularly those of U series, possibly magnifies the background levels of radioactive nuclides in the surrounding environment and increases human exposure risks [1,2,3,4]. High concentrations of radioactive nuclides in coals have been reported worldwide. For example, Barber and Giorgio (1977) [5] found that the radioactive level of 226Ra in a coal sample from Illinois, USA, could reach up to 1500 Bq·kg−1. Measurement of 226Ra on the lignite originated from Kotili of Xanthi Prefecture, Northern Greece, showed a radioactivity as high as 2600 Bq·kg−1, which is more than one order of magnitude higher than that (110–260 Bq·kg−1) of lignite commonly used in coal-fired power plants [6,7]. High levels of radioactive nuclides in Chinese coals are rarely reported. Jiang et al. (1989) [8] reported that the weighted means of 226Ra, 232Th and 40K in Chinese coals are 36 (2–2300 Bq·kg−1), 30 (4–110 Bq·kg−1) and 104 Bq·kg−1 (5–750 Bq·kg−1), respectively. Liu et al. (2007) [9] calculated a weighted mean of 79.5 ± 45, 73.9 ± 53, 40.3 ± 34 and 152.4 ± 21 Bq·kg−1 for 238U, 226Ra, 232Th and 40K, respectively, from ~1000 samples collected from several Chinese coal mines. However, Dai et al. found that high concentration of U occurs in some coals from southwestern China, e.g., Linchang and Yanshan in Yunnan province [10,11] and Guiding in Guizhou province [12].
The coal deposits in eastern Yunnan province, China, have been identified to enrich high levels of natural radionuclides [13,14,15,16,17]. However, their spatial variation, modes of occurrences, and controlling factors are rarely illustrated. In this study, the radioactive nuclides in coal deposits of this area are reassessed, in an effort to generalize a basic knowledge on their potential environmental impacts.

2. Geological Setting

Eastern Yunnan province is located at the southern part of the Yangzi Craton. This region is composed of intermediate massif and suture zones, and has a complicated geological setting due to extensive development of faulting and folding systems [18,19,20,21]. In addition to coal deposits, this area is also abundant in metal resources, such as gold, antimony, germanium, gallium, arsenic, mercury, and thallium. The coal-forming periods in eastern Yunnan include the Early Carboniferous, Late Permian, Late Triassic and Neogene [18,19]. The main coal-bearing strata are the Upper Carboniferous Wanshoushan Formation, the Lower Permian Longtan Formation and the Miocene Xiaolongtan Formation. Different ranks of coal, from gas coal (subbituminous coal) to anthracite, have been developed. The frequent eruptions of volcanoes during coal-forming periods and the alternated marine and terrestrial facies have been suggested to be the main reasons causing the geochemical and mineralogical anomalies of regional coals [22,23].

3. Sampling and Analysis

Nine coal samples from eight active coalmines (Maoergou, Kelang, Changsheng, Xujiayuan, Shizhuang, Xingying, Tuobai and Gongqing) in eastern Yunnan were sampled (Figure 1 and Table 1) according to the Chinese Standard Method GB/T 482-2008 [24]. The samples include anthracite from Zhaotong (coalmines of Maoergou, Changsheng, Xujiayuan and Shizhuang), lignite from Kunming (Kelang coalmine) and coking (bituminous) coals from Qujing (coal mines of Xingying and Gongqing) and Honghezhou (Tuobai coal mine) (Table 1), on basis of GB5751-86 [25]. Each sample was taken by cutting 10-cm wide and 10-cm deep into the coalface to represent the full height or a section of the coal. Upon collection, all samples were stored in polyethylene bags to preclude contamination and weathering.
Figure 1. Sampling locations (filled triangle) of the coalmines in eastern Yunnan, China (HH: Honghezhou; KM: Kunming; QJ: Qujing; ZT: Zhaotong).
Figure 1. Sampling locations (filled triangle) of the coalmines in eastern Yunnan, China (HH: Honghezhou; KM: Kunming; QJ: Qujing; ZT: Zhaotong).
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Table 1. Proximate analysis (%), sulfur (%), radioactive elements (μg/g) of the eastern Yunnan coal.
Table 1. Proximate analysis (%), sulfur (%), radioactive elements (μg/g) of the eastern Yunnan coal.
Sample IDCoal MineCoal RankProximate AnalysisSt,dUThRa
MadAdVdaf
ZT-1MaoergouAnthracite1.2029.2412.664.005.509.651.87
KMKelangLignite9.9715.4656.341.957.322.712.49
ZT-3ChangshengAnthracite0.614.715.670.830.361.060.12
ZT-4XujiayuanAnthracite0.479.477.001.680.541.930.18
ZT-5ShizhuangAnthracite0.8232.1212.423.223.727.591.26
QJ-3XingyingCoking coal0.6214.0419.960.461.543.460.52
HH-1TuobaiCoking coal0.5522.8117.994.154.768.411.62
QJ-6GongqingCoking coal0.6910.8522.641.741.647.471.52
QJ-7Coking coal0.7519.8120.480.931.743.780.59
M, moisture; A, ash yield; V, volatile matter; St, total sulfur; ad, air-dry basis; d, dry basis; daf, dry and ash-free basis.
Coal samples were air-dried, pulverized using a jaw crusher and passed through a 100-mesh sieve before analysis. Proximate analysis (ash yield, volatile matter, moisture) and total sulfur were determined according to ASTM standards [26,27,28,29]. Powdered samples were digested using mixed acids (HNO3:HClO4:HF = 3:1:1) before U and Th measurement by inductively coupled-plasma mass spectrometry (ICP-MS). The method detection limit is 0.002 ng/mL for U and 0.003 ng/mL for Th. The uncertainty of elemental concentration is within ± 10% as evaluated by soil standard GBW 07114 [30] (GBW: national standard substance). The standard deviation for replicate sample digests is less than 10%.
Before radioactive measurement, powdered samples were dried in a temperature controlled furnace at 70 ± 1 °C for 24 h to remove moisture. After cooling down to room temperature, ~500 g of samples were sealed in gas-light, Rn impermeable cylindrical polyethylene containers (Inner Diameter = 40 mm). The samples were sealed and stored for 40 days in order to reach a radioactive equilibrium between 226Ra and its daughters. A GEM60P4-83 high-purity Ge gamma ray spectrometer (ORTEC, Oak Ridge, TN, USA) shielded from background radiation using Pb bricks was employed to measure the most prominent γ-ray energies of the radionuclides in equilibrium with 238U, 226Ra, 40K and 232Th. The gamma spectrometry measurements were made with an energy resolution of 1.95 keV at the 1.332 Mev of 60Co and the relative efficiency of 60%. The activity concentrations of 238U was determined through its daughter product 234Th, 226Ra by its daughter products 214Bi and 214Pb and 232Th by its daughter products 228Ac and 208Tl [31]. The activity concentration of 40K was obtained from its single gamma ray lines of 1460.83 keV. The detector output was connected to a spectroscopy amplifier. The counting time for each sample and background was 10,000 s. The energy and absolute efficiency calibrations of the spectrometers were carried out using calibration sources with energy range covering the studied nuclides. The activity concentrations (As) for the natural radionuclides is calculated as:
A S = N ε P r M t
where N is the net counting rate for a specific gamma line corrected for background, ε is the detector efficiency of a specific gamma ray, Pr is the absolute transition probability of gamma decay, M is the mass of the sample (kg), and t is counting time (s). The national standard reference materials (GBW04127 [32], GBW04325 [33] and GBW04326 [34]) were used for quality assurance, and the typically obtained values are within 5% of certified values. The statistic uncertainties of activity concentrations for radionuclides are estimated less then 2%.

4. Results and Discussion

4.1. Coal Basic Parameters

The studied coals have ash yields ranging from 4.71% to 32.12% (mean = 17.61%), and total sulfur ranging from 0.46% to 4.15% (mean = 2.11%), classifying as low ash, medium-high sulfur coals. The volatile matter values are generally low for most coal samples, varying from 5.67% to 23.28%, with the exception of one sample (KM) of up to 56.34%. According to the proximate analysis and on the basis of the Chinese Standard GB5751-86 [25], the studied coal samples are classified into different ranks: lignite, coking coal (bituminous coal) and anthracite (Table 1).

4.2. Concentrations of U and Th in Coals

The highest U concentration is observed in Kelang mine (KM) of 7.32 μg/g, whereas the lowest U concentration in Changsheng mine (ZT-3) of 0.36 μg/g (Figure 1). The average U concentration in studied coals is 3.01 μg/g, which is slightly higher than that in Chinese coals (2.71 μg/g) [35] and world coals (2.40 μg/g) [36], but is significantly lower than that in coals from Yunnan, China (7.08 μg/g) reported by Li et al. [37]. For Th in coals, the highest concentration is 9.65 μg/g in Maoergou mine (ZT-1), and the lowest concentration is 1.06 μg/g in Changsheng mine (ZT-3). The average Th concentration in studied coals is 5.12 μg/g, which is slightly higher than that in Chinese coals (4.93 μg/g) [35] and world coals (3.3 μg/g) [36], but is still lower than that in coals from Yunnan, China (5.83 μg/g) reported by Li et al. [37].

4.3. Levels of Radioactivity in Coals

The radioactivity of these radionuclides in studied coals is summarized in Table 2. The mean radioactivity of 238U, 226Ra, 232Th and 40K are 63.86, 28.09, 23.76 and 96.84 Bq·kg−1, respectively. The largest contributor to the total radioactivity is 40K for these coal samples.
Table 2. Comparison of radioactivity (Bq·kg−1) of nuclides in coals of eastern Yunnan, China with previous publications.
Table 2. Comparison of radioactivity (Bq·kg−1) of nuclides in coals of eastern Yunnan, China with previous publications.
Sample ID238U232Th226Ra40K
ZT-184.9036.0046.40165.00
KM68.8017.0061.80229.30
ZT-317.7010.303.1030.60
ZT-429.8015.804.5078.70
ZT-592.3037.1031.30134.20
QJ-365.1032.3013.0046.10
HH-178.2033.7040.2065.00
QJ-659.3011.1037.8054.90
QJ-778.6020.5014.6067.80
mean63.86 ± 2523.76 ± 1128.09 ± 2096.84 ± 66
Yunnan a36.60 ± 3116.50 ± 1539.20 ± 436.10 ± 35
China a64.90 ± 3237.50 ± 1849.40 ± 31106.00 ± 27
Poland b23.5014.3018.10129.90
Australia c25.0024.0021.0075.00
a Liu et al. (2007) [12]; b Bemet et al. (2002) [38]; c Fardyet et al. (1989) [39].
For comparison, the radioactivity of these radionuclides in coals from Yunnan province, China, and other countries are shown in Table 2. The average radioactivity of 238U and 40K in studied coals are 63.86 ± 25 and 96.84 ± 66 Bq·kg−1, respectively. Both values are comparable to those in Chinese coals, but are elevated by a factor of 1.7–2.7 as compared to those previously measured in Yunnan coals [11], Radioactivity of 232Th and 226Ra in both previously measured Yunnan coals and this study are slightly lower than those in Chinese coals [12]. It is noted that radionuclides in specific coals can reach to rather high levels such as 238U (84.90 Bq·kg−1), 232Th (36.00 Bq·kg−1) and 40K (165.00 Bq·kg−1) in Maoergou Mine (ZT-1), and 238U (68.80 Bq·kg−1), 226Ra (61.80 Bq·kg−1) and 40K (229.30 Bq·kg−1) in Kelang Mine (KM) (Table 2). Australia coals generally have low levels of radioactivity of nuclides, while Poland coals have relatively high radioactivity of 40K [38,39].

4.4. Factors Influencing Radioactivity of Nuclides

Coles et al. (1978) [40] identified radionuclides associated with organic matter and sulfides are more easily volatilized than those with affinity to alumino-silicate minerals. The correlation analysis of these radionuclides with coal ash yield is used to determine their preliminary modes of occurrence (Figure 2). As shown in Figure 2, the 238U has a positive correlation with ash yield (R2 = 0.81), indicating a dominant inorganic affinity. However, the correlation between U and ash yield is insignificant albeit positive (R2 = 0.24). Uranium can reside in coal matrix in a highly disperse, organic state, or as discrete minerals such as brannerite, uraninite and coffinite, depending on the coal-forming environment [10,40,41]. Seredin and Finkelman (2008) [41] and Dai et al. (2014) [10] showed that U in U-bearing coal deposits worldwide is mainly associated with the organic matter, and that only a small proportion of the U occurs in U-bearing minerals. The inferred modes of occurrence for 238U and U by statistic correction method are not consistent in present study, which need further confirmation.
Figure 2. Correlations of 238U (A) and U (B) with ash yield.
Figure 2. Correlations of 238U (A) and U (B) with ash yield.
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Thorium, Ra and K are commonly considered as refractory elements and associated with alumino-silicate ash of coal [40]. Thorium is generally associated with zircon (ZrSiO4) [42], a highly chemical-resistant mineral. Zircons in coals can have both volcanic and authigenic origins [43,44]. Besides, Th can be adsorbed by clay minerals in coals [45]. The positive correlations (Figure 3) of 232Th radioactivity (R2 = 0.73) and Th (R2 = 0.58) with ash yield demonstrate a dominant inorganic affinity of Th. It has been shown that the radioactivity of 226Ra in Indian coal slag is two times higher than that in feed coal [35,36], implying a dominant inorganic Ra state. A highly positive correlation of Ra with ash yield has been observed in our study (R2 = 0.50). However, the correlative of 226Ra with ash yield is weak (Figure 4).
Figure 3. Correlations of 232Th (A) and Th (B) with ash yield.
Figure 3. Correlations of 232Th (A) and Th (B) with ash yield.
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Figure 4. Correlations of 226Ra (A) and Ra (B) with ash yield.
Figure 4. Correlations of 226Ra (A) and Ra (B) with ash yield.
Minerals 05 00513 g004

4.5. Radioactive Impacts of Nuclides

The assessment of the radioactive impacts of nuclides in coals has an important environmental significance, since coal is abundantly used in power generation. Emissions from coal-fired power plants in gaseous and particulate forms containing nuclides probably discharge and accumulate in the surrounding environment, thus causing radiation exposures to the local population [46,47]. Inhalation of fly ash emitted from the stacks and the ingestion of foodstuffs receiving atmospheric deposition are the main pathways to increase human radiation exposure [48].
It has been hypothesized that 370 Bq·kg−1 of 226Ra or 259 Bq·kg−1 of 232Th or 4810 Bq·kg−1 of 40K could produce the same gamma dose rate [31,49]. The Ra equivalent radioactivity, the internal exposure index (IRa) and the external hazard index (Ir) can be calculated according to Beretka and Mathew (1985) [50] and GB6566-2010 [51] as:
R a e q = C R a + 1.43 C T h + 0.077 C K
I R a = C R a 200 1
I r = C R a 370 + C T h 259 + C K 4810 1
where CRa, CTh and CK, are the radioactivity of 226Ra, 232Th and 40K, respectively. The maximum value of Raeq in construction materials is set to 370 Bq·kg−1 for safe use [52], the maximum values of IRa and Ir must be lower than 1.0 according to GB6566-2010 [48]. The calculated values of Raeq for studied coals vary from 19.97 to 109.43 Bq·kg−1 (Table 3), with an average of 68.84 Bq·kg−1, which is lower than the recommended limit. The calculated values of Ir and IRa are generally below than 0.3 significantly lower than unity.
Table 3. Radium equivalent activity (Raeq), external hazard index (Ir), internal exposure index (IRa), air absorbed dose rates (D (nGy/h)) and annual effective dose (AED) of radionuclides in coals from eastern Yunnan, China.
Table 3. Radium equivalent activity (Raeq), external hazard index (Ir), internal exposure index (IRa), air absorbed dose rates (D (nGy/h)) and annual effective dose (AED) of radionuclides in coals from eastern Yunnan, China.
Sample IDRaeqIrIRaD (nGy/h)AED
ZT-1110.590.300.2350.0661.40
KM103.770.280.3148.3859.33
ZT-320.190.050.028.9310.95
ZT-433.150.090.0214.9018.28
ZT-594.690.260.1642.4752.08
QJ-362.740.170.0727.4433.65
HH-193.400.250.2041.6451.06
QJ-657.900.160.1926.4632.45
QJ-749.140.130.0721.9526.92
mean69.510.190.1431.3638.46
The total outdoor air absorbed dose rate (nGy/h) due to terrestrial gamma rays at 1 m above the ground is calculated from 226Ra, 232Th and 40K. The conversion factors used to calculate the absorbed dose rates are given as follows [53]:
D ( n G y / h ) = 0.462 C R a + 0.604 C T h + 0.0417 C K
The calculated absorbed dose rates range from 8.93 to 50.06 nGy/h with a mean value of 31.36 nGy/h (Table 3), which is lower than the average value of global primordial radiation of 59 nGy/h [53] and the Chinese natural gamma radiation dose rate of 63.0 nGy/h [53].
To estimate the annual effective dose rates, the conversion coefficient from the absorbed dose in air to the effective dose (0.7 nGy/h) and the outdoor occupancy factor (20%) recommended by UNSCEAR (2000) [53] are used. The annual effective dose rate is calculated by the following formula [52]:
Effective   dose   rate   ( μ Sv / year )   =   D   ( nGy / h )   ×   8760   ( h / year )   ×   0.7   ×   10 6 μ Sv / 10 9 nGy   × 0.2
The calculated effective dose rates vary from 10.95 to 61.40 μSv/year with an average value of 38.46 μSv/year.

5. Conclusions

This study provides an initial assessment on the natural radionuclides in coals from eastern Yunnan, China. The mean specific activity concentrations of radionuclides 238U, 226Ra, 232Th and 40K are 63.86, 28.09, 23.76 and 96.84 Bq·kg−1 in coals, respectively. Radioactivity of 238U and 40K in studied coal are elevated by a factor of 1.7–2.7 as compared to previously measured Yunnan coals. Radioactivity of 238U and 40K in all Yunnan coals is slightly lower than Chinese coals. Radioactivity of 238U and 232Th is closely correlated with coal ash, suggesting their inorganic origins. The environmental effect of natural radionuclides is considered to be negligible as evaluated by indexes of Raeq, IR and Ir. The absorbed dose rates D (nGy/h) values are lower than the average value of global primordial radiation and the Chinese natural gamma radiation dose rate.

Acknowledgments

This work was supported by the National Basic Research Program of China (973 Program, 2014CB238903), the National Natural Science Foundation of China (No. 41173032 and 41373110). We acknowledge editors and reviewers for polishing the language of the paper and for in-depth discussion.

Author Contributions

Guijian Liu and Qiyan Feng contributed to the conception of the study. Guijian Liu, Qiyan Feng, Ruoyu Sun and Xin Wang contributed significantly to analysis and manuscript preparation; Xin Wang performed the data analyses and wrote the manuscript; Ruoyu Sun helped perform the analysis with constructive discussions. All authors read and approved the manuscript.

Conflicts of Interest

The authors declare no conflict of interest.

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MDPI and ACS Style

Wang, X.; Feng, Q.; Sun, R.; Liu, G. Radioactivity of Natural Nuclides (40K, 238U, 232Th, 226Ra) in Coals from Eastern Yunnan, China. Minerals 2015, 5, 637-646. https://doi.org/10.3390/min5040513

AMA Style

Wang X, Feng Q, Sun R, Liu G. Radioactivity of Natural Nuclides (40K, 238U, 232Th, 226Ra) in Coals from Eastern Yunnan, China. Minerals. 2015; 5(4):637-646. https://doi.org/10.3390/min5040513

Chicago/Turabian Style

Wang, Xin, Qiyan Feng, Ruoyu Sun, and Guijian Liu. 2015. "Radioactivity of Natural Nuclides (40K, 238U, 232Th, 226Ra) in Coals from Eastern Yunnan, China" Minerals 5, no. 4: 637-646. https://doi.org/10.3390/min5040513

APA Style

Wang, X., Feng, Q., Sun, R., & Liu, G. (2015). Radioactivity of Natural Nuclides (40K, 238U, 232Th, 226Ra) in Coals from Eastern Yunnan, China. Minerals, 5(4), 637-646. https://doi.org/10.3390/min5040513

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