Distribution of oceanic 137Cs from the Fukushima Dai-ichi Nuclear Power Plant simulated numerically by a regional ocean model

https://doi.org/10.1016/j.jenvrad.2011.10.007Get rights and content

Abstract

Radioactive materials were released to the environment from the Fukushima Dai-ichi Nuclear Power Plant as a result of the reactor accident after the Tohoku earthquake and tsunami of 11 March 2011. The measured 137Cs concentration in a seawater sample near the Fukushima Dai-ichi Nuclear Power Plant site reached 68 kBq L−1 (6.8 × 104 Bq L−1) on 6 April. The two major likely pathways from the accident site to the ocean existed: direct release of high radioactive liquid wastes to the ocean and the deposition of airborne radioactivity to the ocean surface. By analysis of the 131I/137Cs activity ratio, we determined that direct release from the site contributed more to the measured 137Cs concentration than atmospheric deposition did.
We then used a regional ocean model to simulate the 137Cs concentrations resulting from the direct release to the ocean off Fukushima and found that from March 26 to the end of May the total amount of 137Cs directly released was 3.5 ± 0.7 PBq ((3.5 ± 0.7) × 1015 Bq). The simulated temporal change in 137Cs concentrations near the Fukushima Daini Nuclear Power Plant site agreed well with observations. Our simulation results showed that (1) the released 137Cs advected southward along the coast during the simulation period; (2) the eastward-flowing Kuroshio and its extension transported 137C during May 2011; and (3) 137Cs concentrations decreased to less than 10 Bq L−1 by the end of May 2011 in the whole simulation domain as a result of oceanic advection and diffusion.
We compared the total amount and concentration of 137Cs released from the Fukushima Dai-ichi reactors to the ocean with the 137Cs released to the ocean by global fallout. Even though the measured 137Cs concentration from the Fukushima accident was the highest recorded, the total released amount of 137Cs was not very large. Therefore, the effect of 137Cs released from the Fukushima Dai-ichi reactors on concentration in the whole North Pacific was smaller than that of past release events such as global fallout, and the amount of 137Cs expected to reach other oceanic basins is negligible comparing with the past radioactive input.

Introduction

Radioactive materials were released to the environment from the Fukushima Dai-ichi Nuclear Power Plant (1F NPP), operated by the Tokyo Electric Power Company (TEPCO), as a result of the reactor accident after the Tohoku earthquake and tsunami on 11 March 2011. The total estimated release amounts of 131I and 137Cs from the 1F NPP reactors (No. 1, No. 2 and No. 3) to the atmosphere were 160 PBq (1.6 × 1017 Bq) and 15 PBq (1.5 × 1016 Bq), respectively (Nuclear Emergency Response Headquarters, Government of Japan, NERH, 2011). There are several potential pathways by which these materials might reach the ocean (Table 1). Some of the radioactive materials released to the atmosphere were introduced into the ocean by wet and dry atmospheric deposition. The total estimated amount of 131I, 134Cs, and 137Cs released directly to the ocean during 1–6 April, observed near the water intake of the 1F NPP No. 2 reactor, was 4.7 PBq (4.7 × 1015 Bq), with 137Cs accounting for 0.94 PBq (9.4 × 1014 Bq) (NERH, 2011). In addition, an estimated 20 TBq (2.0 × 1013 Bq) of radioactive materials were released near the water intake of No. 3 reactor from 2:00 on 10 May to 19:00 on 11 May. The radioactivity in a planned release of low-level waste water was 42 GBq (4.2 × 1010 Bq). Thus, the direct release from 1F NPP No.2 reactor was the largest among these three direct release pathways from the 1F NPP reactors to the ocean. The estimates of the release rate from the 1F NPP No. 2 reactor to the ocean, however, have considerable uncertainty because they are not taken measured concentrations of radioactive materials in the ocean into account.
To distinguish the contributions of atmospheric deposition and direct release to the oceanic radioactive contamination, we examined 131I/137Cs observed data. Although freshwater runoff (including both groundwater discharge and river runoff) of radioactive materials deposited at the 1F NPP site and subsequently washed out to sea by precipitation and drainage is another possible release pathway to the ocean, we ignored it in this study under the assumption that its contribution was small. In fact, 137Cs deposited on land surface is difficult to be leached out by river runoff (Hirose et al., 1990). More detailed estimates may need to consider other potential release routes. We also ignored the planned release of low-level radioactive waste water in this study because the amount of radioactivity was far smaller than the estimated direct release from the 1F NPP No. 2 reactor.
Because it is more difficult to make observations from ships than to make similar observations on land, the available observations of the released radioactive materials in the ocean are too few to characterize the behavior of those materials in the ocean. Oceanic model simulations can interpolate and extrapolate sparse observations and thus can help us understand the oceanic behavior of radioactive materials (i.e., Tsumune et al., 2003a, Tsumune et al., 2003b, Tsumune et al., 2011). In addition, ocean circulation model simulations can provide useful information that allows efficient planning of future observations. Several institutions and agencies have performed simulations of the behavior of radioactive materials in the ocean, including the Japan Agency for Marine-Earth Science and Technology (JAMSTEC, 2011) and the Japan Atomic Energy Agency (JAEA, 2011) , and Toulouse University, France (Toulouse University, 2011). Intercomparison between simulation results obtained by multiple models will be useful to have better understanding of the behavior of oceanic tracer and improve ocean modeling. Moreover, by comparing observed concentrations of a radioactive tracer material with simulated results it is possible to assess the skill of an ocean circulation model. An accurate estimation of the release rate of 137Cs from the 1F NPP reactors will be useful for intercomparison of models used for simulating the behavior of radioactive materials in the ocean.
In this paper, we describe the observation data and the regional ocean model in Section 2. In Section 3 (Results and Discussion), we analyze the observed data for 131I and 137Cs to determine the amounts released directly and by atmospheric deposition. We also estimate the amount of 137Cs released directly from the 1F NPP No. 2 reactor by comparing the observed data with simulated results. In addition, we simulate the behavior of 137Cs released from the 1F NPP No. 2 reactor off Fukushima to understand the distribution of oceanic contamination. We verify the simulated result by comparison with the observed data. Finally, we compare the amount of oceanic contamination with 137Cs between the Fukushima accident and past radioactive contamination events due to atmospheric weapons tests since 1945, the Chernobyl accident in 1986, and releases from the British Nuclear Fuels, Ltd (BNFL) reprocessing site at Sellafield, UK since 1952.

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Section snippets

Observed data

TEPCO has observed radioactivity in seawater near shore at several sites, the discharge canal for 5 and 6 reactors (5–6 discharge canal) at the north of 1F NPP site and the discharge canal for 1, 2, 3 and 4 reactors (south discharge canal) at the south of the 1F NPP site, the north discharge canal at the Fukushima Daini Nuclear Power Plant (2F NPP) site (10 km south of the 1F NPP site), and off Iwasawa (16 km south of the 1F NPP site), since 21 March 2011 (TEPCO, 2011a). MEXT has observed the

Temporal changes in 137Cs concentrations

We estimated the behavior of 137Cs in the ocean by examining temporal changes in 137Cs concentrations in the 5–6 and south discharge canals at the 1F NPP site (Fig. 2), although the direct release did not occur at these discharge canals. The 137Cs concentrations in the discharge canals increased to more than 10 kBq L−1 (1.0 × 104 Bq L−1) from 21 to 31 March 2011. The 137Cs concentration peaks occurred on 30 March (47 kBq L−1) and 6 April (68 kBqoL−1). Then, The 137Cs concentrations decreased from 6

Conclusion

We differentiated two major release pathways by analyzing observed 131I/137Cs activity ratios, direct release and atmospheric deposition. The direct release of radioactivity-contaminated water started from the 1F NPP reactor from 26 March 2011. The large direct release of 137Cs continued until 6 April and then decreased, but the direct release did not stop altogether until the end of May. The contribution of direct release to the observed 137Cs concentrations was larger than that of atmospheric

Acknowledgments

We thank Motoyoshi Ikeda, Mitso Uematsu and members of the Earthquake Disaster Response Working Group of the Oceanographic Society of Japan for their helpful discussion. We also thank Hiromaru Hirakuchi and Atsushi Hashimoto for providing the NuWFAS results. We also thank Fukiko Taguchi and Ryosuke Niwa for technical support.

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