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Journal of Radiation Research logoLink to Journal of Radiation Research
. 2015 Oct 31;56(Suppl 1):i48–i55. doi: 10.1093/jrr/rrv056

Mapping of the cumulative β-ray dose on the ground surface surrounding the Fukushima area

Satoru Endo 1,*, Tsuyoshi Kajimoto 1, Kenichi Tanaka 1, Thanh T Nguyen 1, Gohei Hayashi 2, Tetsuji Imanaka 3
PMCID: PMC4732530  PMID: 26519736

Abstract

A large amount of the fission products released by the Fukushima Daiichi Nuclear Power Plant (FDNPP) accident on 11 March 2011 was deposited in a wide area from Tohoku to northern Kanto. A map of the estimated cumulative β-ray dose (70 μm dose equivalent) on the soil surface for one year after the FDNPP accident has been prepared using previously reported calculation methods and the 2-km mesh survey data by MEXT. From this map of estimated dose, areas with a high cumulative β-ray dose on the soil surface for one year after the FDNPP accident were found to be located in the Akogi-Teshichiro to Akogi-Kunugidaira region in Namie Town, and in the southern Futaba Town to the northern Tomioka Town region. The highest estimated cumulative β-ray dose was 710 mSv for one year at Akogi-Teshichiro, Namie Town.

Keywords: Fukushima Daiichi Nuclear Power Plant accident, β-ray dose, radiotellurium, radioiodine, radiocesium

INTRODUCTION

The nuclear accident at the Fukushima Daiichi Nuclear Power Plant (FDNPP) occurred after the enormous earthquake and associated tsunami on 11 March 2011. A large amount of fission products was released and deposited over a wide area from the Tohoku region to the northern Kanto region [14]. The deposited radionuclides were mainly 129mTe, 129Te, 131I, 132Te, 132I, 134Cs, 136Cs and 137Cs. These radionuclides emit both γ rays and β rays. Because β rays do not contribute to the effective dose, dose evaluations have been focused on γ rays. However, β rays contribute to the skin dose for humans, the whole-body dose for small insects, and the total dose for plant leaves.

In our previous publication, the time variation in the β-ray dose rate and the cumulative β-ray dose as 70 μm dose equivalent were estimated for the conditions of an initial 137Cs deposition of 1000 kBq/m2, using a Monte Carlo calculation [5]. In the current study, the deposition ratios of 129mTe, 129Te, 131I, 132Te, 132I and 134Cs to 137Cs were taken into account, values for which ratios were mainly taken from the Iitate Village contamination study [5]. For example, the 131I/137Cs ratio was assumed to be 9.2 at the time of deposition [4]. However, the 131I/137Cs ratio has a range of values for the various areas between the northwestern region and the southern region of the FDNPP [1, 2].

In addition, the Ministry of Education, Culture, Sports, Science and Technology (MEXT) conducted a 2-km mesh contamination study from June to August 2011 [6]. This study started three months after the main deposition occurred on 15 March 2011. Therefore, the short-half-life radionuclides, such as 132I and 132Te (half-life: 3.204 days), had already decayed out. 131I was also decayed by a factor of 2000 due to its short half-life (8.021 days). In the MEXT study, 131I radioactivity was detected in only 19% of 2181 soil sampling locations. Consequently, the 131I/137Cs ratio is available for only 415 locations in the Fukushima prefecture.

The purpose of this paper was to evaluate the cumulative β-ray dose (70 μm dose equivalent) for one year after the FDNPP accident on the ground surface and to create a β-ray dose map of contaminated areas in the Fukushima prefecture, using our previous β-ray calculation method [5] coupled with the MEXT 2-km mesh soil data [6].

MATERIALS AND METHODS

Calculation technique for the cumulative soil surface β-ray dose for one year

A previously published β-ray dose calculation technique [5, 7, 8] was used in this study. The transport of β-rays was simulated with Monte Carlo N-Particle transport code version 4C (MCNP-4C) [9]. Beta-ray sources were uniformly distributed in a surface soil layer of 5-mm thickness. Beta-ray energy spectra were used for the radionuclides: 129mTe, 129Te, 131I, 132Te, 132I, 134Cs and 137Cs [5]. Energy deposition in the air cell is accumulated as a function of height from the soil surface. The initial β-ray dose rate for each of seven radionuclides was calculated. Then, seven values of β-ray dose rates for the radionuclide i at the time of deposition (D˙i0) were combined according to the deposition ratio with that of 137Cs: fi, where fi is the radionuclide ratio: 129mTe/137Cs, 129Te/137Cs, 131I/137Cs, 132Te/137Cs, 132I/137Cs, 134Cs/137Cs and 137Cs/137Cs. In order to estimate the time variation, each β-ray dose rate component was reduced by the time after deposition according to each half-life time. The cumulative β-ray dose for one year was calculated by integration of the time after deposition. In the previous publication, the fi was assumed to be 1: 0.7: 9.2: 8.3: 8.3: 1: 1, where i means 129mTe, 129Te, 131I, 132Te, 132I, 134Cs and 137Cs [5]. In our study, in the calculation process for the cumulative β-ray dose, radionuclide ratios of 131I/137Cs and 129mI/137Cs were treated as two parameters of: rI and rT, respectively. Also, 129Te/137Cs and 132I/137Cs ratios were scaled to the 129mTe/137Cs ratio by factors of 0.7 and 8.3, respectively. Therefore, a relation of 129Te/137Cs = 0.7 x 129mTe/137Cs and 132I/137Cs = 8.3 x 129mTe/137Cs were used here, respectively. Consequently, the deposition ratio of fi was set to rT: (0.7·rT): rI : (8.3·rT): (8.3·rT): 1: 1. The β-ray dose rate (D˙i0) and the cumulative β-ray dose on the ground surface for one year (DA) are under conditions of an initial deposition density of 137Cs. The cumulative dose of D(rI , rT) for one year at unit deposition of 137Cs (kBq/m2) can be written as follows:

D˙(rI,rT,t)=ifiD˙i012tTi, Eq. 1
D(rI,rT)=01yearD˙(rI,rT,t)dt, Eq. 2

where Ti is the half-life of radionuclide i, and rI and rT are 131I/137Cs and 131I/137Cs ratios, respectively. After this calculation, the relationships between the cumulative soil surface β-ray dose for one year and conditions of deposition density of 137Cs were determined. The cumulative soil surface β-ray dose for one year (DA) was calculated by:

DA=D(rI,rT)A137Cs, Eq. 3

where A137Cs is the 137Cs deposition density (kBq/m2) taken from the MEXT 2-km mesh soil contamination data [6]. The dose conversion factor from Gy to Sv for β-rays was assumed to be 1 in this analysis.

129mTe/137Cs ratio interpolation

The 129mTe/137Cs ratio was obtained from the MEXT data (which includes 2181 sampling locations) at 797 locations. However, both ratios of 129mTe/137Cs and 131I/137Cs were obtained at only 175 locations. At the locations without 129mTe/137Cs data, 129mTe/137Cs data were interpolated with geographic information techniques (GIS): a multilevel B spline interpolation by SAGA-GIS [10]. The resultant 129mTe/137Cs map is shown in Fig. 1.

Fig. 1.

Fig. 1.

Map of 129mTe/137Cs ratio of the MEXT data [6] interpolated with a multilevel B spline interpolation by SAGA-GIS [10].

RESULTS AND DISCUSSION

The time dependence of the β-ray dose (70-μm dose equivalent) rate on the ground surface is shown in Fig. 2a for a fixed value of rT = 1.0, with parameter values of rI = 5, 9.2, 20, 40, 100 and 200. The 131I contribution diminishes about 80 days after deposition due to the decay from Fig. 2a. Figure 2b shows the time dependence of the β-ray dose rate for a fixed rI of 9.2 with various rT of 0.1, 0.5, 1, 5, 10 and 50. In case of rT being >5, small increases in the β-ray dose appear from 20 days. This increase is caused by the contribution of β-rays from 129,129mTe nuclides, which have a half-life of 33.6 days. For detailed calculation methods, please refer to the previous publication [5].

Fig. 2.

Fig. 2.

Beta-ray dose rate, μSv h-1, on soil surface as a function of time after deposition for variable 131I/137Cs and 129mTe/137Cs. (a) 129mTe/137Cs = 1 with 131I/137Cs = 5, 9.2, 20, 40, 100 and 200. (b) 131I/137Cs = 9.2 with 129mTe/137Cs = 0.1, 0.5, 1, 5, 10 and 50.

The cumulative β-ray dose on the ground surface can be obtained by integrating the time-dependent dose rate as Eq. 2. Results of cumulative β-ray dose calculation for various sets of rI and rT values are plotted in Fig. 3, respectively. The cumulative dose per 137Cs deposition of 1000 kBq/m2 is increasing with the 131I/137Cs ratio. The least square fitted function was determined to be D(rI, rT) = 1.1165 rI + b, as shown in Fig. 3. The fitted parameter values of b for several values of rT are listed in Table 1. The fitted parameter: b was re-fitted by linear function and determined to be b(rT) = 31.032 rT + 50.009. The fitted result is shown in Fig. 4. Finally, the cumulative β-ray dose on the ground surface per initial137Cs deposition for one year, D(rI, rT), can be expressed as a function of rI and rT as:

D(rI,rT)=1.1165rI+31.032rT+50.009. Eq. 4

The cumulative soil surface β-ray dose for one year was calculated for 415 MEXT sampling locations using Eq. 4. The representative 72 locations selected from 415 locations are listed in Table 2. The calculated results show that higher cumulative β-ray doses appear around the Akogi region in Namie Town and from Futaba Town to northern Tomioka Town. The values for cumulative soil surface β-ray dose were estimated to be 710 mSv at Namie-Akogi-Teshichiro, 477 mSv at Namie-Akogi-Kunugidaira, 246 mSv at Futaba-Ishiguma and 620 mSv at Tomioka-Osuge. Also, the southern Iitate Village had a relatively high cumulative β-ray dose of 100–150 mSv. In Fukushima City, the cumulative soil surface β-ray dose around the eastern region was estimated to be 20–60 mSv higher than that around the western region (4–10 mSv). On the other hand, areas with a high 131I/137Cs ratio of 69 ± 39 (maximum: 285) around Iwaki City showed a relatively low deposition density of 137Cs of 20–50 kBq/m2; thus, the cumulative β-ray dose showed slightly lower values: ∼1–24 mSv.

Fig. 3.

Fig. 3.

Cumulative β-ray dose per 137Cs deposition of 1000 kBq/m2 for the first year as a function of 131I/137Cs and 129mTe/137Cs ratio.

Table 1.

Fitted parameter b for 132I/137Cs of 0.1, 0.5, 1, 5, 10 and 50

132I/137Cs Parameter b
0.1 53.064
0.5 65.478
1 81.142
5 205.13
10 360.3
50 1601.6

Fig. 4.

Fig. 4.

Fitted parameter b as a function of 132I/137Cs ratio.

Table 2.

Cumulative soil surface β-ray dose for one year at representative 72 locations selected from the calculated results of 415 locations using the 2-km mesh soil deposition density (kBq/m2) by MEXT [6]

Location Longitude Latitude 131I 137Cs 129mTe 131I/137Cs 129mTe/137Cs D(rI,rT) (mSv) DA (mSv)
Iwaki City, Hisanohama 37.17292 140.9993 0.6 59 26.5 3.8 199 11.7
Iwaki City, Yamada 36.92822 140.7411 0.86 44 88 50.9 11.5 465 20.4
Iwaki City, Yotsukura 37.10747 140.9664 0.76 35 8.8 56.5 2.3 187 6.6
Iwaki City, Taira 37.03022 140.9233 0.82 26 6.9 82.1 1.7 199 5.2
Otama Village 37.54375 140.332 0.41 130 16 8.2 1.1 92.5 12.0
Kuwaori Town, Yachi 37.86128 140.5363 0.32 83 18 10.0 1.3 103 8.5
Kuwaori Town, Kamikori 37.84794 140.5284 1 200 36 13.0 1.3 105 20.9
Kunimi Town, Okido 37.89039 140.5723 0.69 110 18 16.3 1.1 103 11.3
Kawamata Town, Yamakiya 37.583 140.7186 3.6 870 190 10.8 1.3 104 90.0
Kawamata Town, Akiyama 37.69419 140.5603 0.25 51 11 12.8 1.3 105 5.4
Kawamata Town, Kotsunagai 37.63153 140.6581 0.46 81 22 14.8 1.4 111 9.0
Date City, Ryozan 37.784 140.6704 0.15 49 8.0 1.5 105 5.1
Date City, Yanagawa 37.85194 140.5667 0.84 180 35 12.1 1.2 101 18.2
Date City, Miyoda 37.74461 140.6127 1.7 320 52 13.8 1.2 104 33.2
Aizuwakamatsu City, Oto 37.37189 139.9251 0.49 4.5 283 1.3 421 1.9
Kagamiishi Town 37.25781 140.3391 0.25 76 8.6 1.6 110 8.3
Tenei Village 37.22039 140.2581 0.35 140 21 6.5 1.0 89.8 12.6
Koriyama City, Hiwada 37.45531 140.3889 0.12 170 5.3 1.8 0.7 75.3 12.8
Koriyama City, Narukami 37.39411 140.3381 0.49 230 5.5 1.0 87.2 20.1
Sukagawa City, Moriya 37.33333 140.2456 0.089 200 1.2 1.4 94.2 18.8
Sukagawa City, HokotsukiFurudate 37.26972 140.2694 0.6 130 20 12.0 1.0 95.3 12.4
Saigo Village 37.17011 140.2939 0.45 44 7.7 26.6 1.2 118 5.2
Kodono Town 37.07803 140.5705 0.04 33 0.82 3.2 0.4 66.5 2.2
Hirata Village 37.23067 140.5666 0.35 8.1 112 1.5 228 1.8
Katsurao Village, Ochiai-Karogawa 37.48575 140.8077 0.68 160 11.1 1.2 100 16.0
Katsurao Village, Katsurao 37.53778 140.7802 7.3 1600 11.9 1.2 102 163
Hirono Town, Oriki 37.19908 141.0019 2.1 250 21.9 4.5 215 53.7
Hirono Town, Yusuji 37.18967 140.9977 1.3 55 42 61.5 4.4 257 14.1
Kawauchi Village, Shimokawauchi 37.27697 140.8097 0.7 480 64 3.8 0.9 81.2 39.0
Kawauchi Village, Kamikawauchi 37.30375 140.7622 0.15 52 1.8 7.5 0.3 69.5 3.6
Futaba Town, Ishikuma 37.43553 140.954 31 1700 320 47.4 1.3 145 246
Okuma Town, Kumakawa 37.39225 141.0124 32 1700 250 49.0 1.1 141 240
Naraha Town, Yamadaoka 37.24358 140.9665 3.2 130 64.0 3.0 217 28.1
Naraha Town, Shimokobana 37.25817 140.9692 5.7 130 47 114 2.5 261 33.9
Tomioka Town, Osuge 37.37439 141.0081 55 5000 1100 28.6 1.3 124 620
Tomioka Town, Motooka 37.34036 140.9807 26 530 93 128 1.5 245 130
Namie Town, Minamitsushima 37.55683 140.7897 4.4 2100 5.5 1.1 90.4 190
Namie Town, Akogi-Teshichiro 37.59606 140.7541 17 7900 920 5.6 1.1 89.9 710
Namie Town, Akogi-Hirusone 37.54186 140.8622 2.8 1300 220 5.6 1.1 91.5 119
Namie Town, Akogi-Kunugidaira 37.56053 140.8238 19 5700 450 8.7 0.8 83.6 477
Namie Town, Akougi-Shiobite 37.56683 140.8021 10 2500 10.4 1.0 91.8 230
Shinchi Town 37.85694 140.8808 0.65 45 9.2 37.6 1.2 130 5.9
Iitate Village, Komiya 37.62881 140.7731 3.2 1300 190 6.4 1.1 92.4 120
Iitate Village, Warabidaira 37.62539 140.8105 3.7 1400 6.9 1.5 103 144.4
Iitate Village, Okura 37.72678 140.8348 0.49 140 29 9.1 1.3 102 14.2
Iitate Village, Notegami 37.63806 140.7982 5.3 1500 9.2 1.3 103 154
Iitate Village, Matsuzuka 37.68981 140.7201 3.6 1000 9.4 1.1 94.5 94.5
Iitate Village, Kusano 37.71753 140.7633 1.2 300 10.4 1.4 106 31.6
Iitate Village, Iitoi 37.66136 140.6972 1.5 280 13.9 1.0 97.6 27.3
Soma City, Nokikitahara 37.84108 140.8961 0.064 52 8.8 3.2 1.1 87.8 4.6
Soma City, Otsubo-Maenosawa 37.82283 140.8953 0.2 55 11 9.5 1.1 95.3 5.2
Soma City, Hatsuno-Nishihara 37.82603 140.8707 0.23 27 3.3 22.2 0.9 104 2.8
Miharu Town, Nanakusagi 37.475 140.4906 0.56 100 22 14.6 0.9 94.1 9.4
Miharu Town, Omachi 37.44297 140.4891 0.48 64 12 19.5 1.1 106 6.8
Ono Town 37.30439 140.6186 0.11 23 3.5 12.4 0.7 87.4 2.0
Tanura City, Miyakoji 37.45814 140.7183 0.24 160 16 3.9 0.8 79.8 12.8
Tanura City, Funehiki 37.51436 140.6562 0.68 88 20.1 1.2 109 9.6
Samekawa Village 37.07261 140.4606 0.14 19 2.7 19.2 0.9 99.6 1.9
Tanakura Town 37.01122 140.3368 0.22 76 2.8 7.5 0.8 82.8 6.3
Minami-Soma City, Takanokura 37.62867 140.8983 0.77 250 8.0 2.4 133 33.3
Minami-Soma City, Haramachi 37.62383 140.9612 0.42 100 25 10.9 1.4 105 10.5
Minami-Soma City, Karasuzaki 37.68547 141.0106 0.15 6.8 57.4 1.4 160 1.1
Nihonmatsu City, Kawasaki 37.61136 140.4875 0.63 270 6.1 1.0 88.3 23.8
Nihonmatsu City, Hatsumori 37.52533 140.5335 0.7 180 32 10.1 1.1 96.2 17.3
Nihonmatsu City, Babadaira 37.57969 140.3518 0.26 56 12.1 1.4 107 6.0
Nihonmatsu City, Dake-Onsen 37.60419 140.3556 0.28 29 8.7 25.1 1.7 131 3.8
Fukushima City, Arai 37.71081 140.3873 0.18 39 12.0 1.2 100 3.9
Fukushima City, Watari 37.72 140.4994 1.7 400 11.1 1.4 106 42.5
Fukushima City, Onami 37.757083 140.55381 2.9 570 110 13.2 1.4 108 61.3
Fukushima City, Matsukawacho 37.68006 140.3562 0.41 67 15.9 1.2 105 7.0
Motomiya City, Motomiya 37.52286 140.4116 0.12 92 6.5 3.4 0.8 78.3 7.2
Motomiya City, Arai 37.48628 140.3833 0.33 24 6.6 35.8 1.3 131 3.2

The ratios decay-corrected to 15 March 2011. The 129mTe/137Cs ratios interpolated with a multilevel B spline by SAGA-GIS [10] are listed.

The map of the estimated cumulative soil surface β-ray dose is shown in Fig. 5, edited by interpolating the results with the multilevel B spline interpolation using SAGA-GIS [10]. Three higher cumulative β-ray dose regions can be clearly seen in the Akogi-Teshichiro and Akogi-Kunugidaira regions in Namie Town, and also from Futaba Town to northern Tomioka Town. Compared with the cumulative γ-ray dose map produced by MEXT [11], the β-ray dose is slightly larger than the γ-ray dose around Iwaki City. This is due to the 129m,129Te contributions, which have longer half-lives (33.6 days) than 131I (8.021 days) and higher β-ray emission rates of ∼90% compared with the γ-ray emission rates (<10%).

Fig. 5.

Fig. 5.

Map of the cumulative β-ray dose (mSv) on ground surface in the first year after deposition.

As already stated in the Introduction, our estimation used the 70-μm dose equivalent as the skin dose for humans. These estimates are based on the assumption that people stay outside houses or buildings continuously for a year. Therefore, this skin dose is not strictly accurate for humans; however, the doses are fairly accurate for organisms living in the outside environment, such as small insects, plant leaves, etc.

CONCLUSION

The cumulative soil surface β-ray dose was calculated using the 2-km mesh soil contamination data by MEXT and our previously published β-ray dose calculation technique. From that, an estimated cumulative soil surface β-ray dose map was produced. As a result of this map, areas estimated to have a higher cumulative β-ray dose on the soil surface for the first year after the FDNPP accident were found to be located in the Akogi-Teshichiro to Akogi-Kunugidaira region in Namie Town and from Futaba Town to northern Tomioka Town. The highest estimated cumulative β-ray dose was 710 mSv for one year at Akogi-Teshichiro, Namie Town.

FUNDING

This study was supported by Grant-in-Aid for Challenging Exploratory Research No. 26550031 from the Japan Society for the Promotion of Science (JSPS). Funding to pay the Open Access publication charges for this special issue was provided by the Grant-in-Aid from the Japan Society for the Promotion of Science (JSPS) [KAKENHI Grant No. 26253022].

Acknowledgements

The authors are grateful to Prof. Shizuma, Hiroshima University, for discussions about the data analysis.

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