日本地球惑星科学連合2019年大会

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[J] Eveningポスター発表

セッション記号 M (領域外・複数領域) » M-AG 応用地球科学

[M-AG41] 福島原発事故により放出された放射性核種の環境動態

2019年5月26日(日) 17:15 〜 18:30 ポスター会場 (幕張メッセ国際展示場 8ホール)

コンビーナ:高橋 嘉夫(東京大学大学院理学系研究科地球惑星科学専攻)、北 和之(茨城大学理学部)、恩田 裕一(筑波大学アイソトープ環境動態研究センター)、津旨 大輔(一般財団法人 電力中央研究所)

[MAG41-P10] Estimating impacts of direct release and riverine discharge on oceanic 137Cs derived from the Fukushima Dai-ichi Nuclear Power Plant accident by an regional ocean model

★Invited Papers

*津旨 大輔1坪野 考樹1三角 和弘1立田 穣1恩田 裕一2青山 道夫3 (1.一般財団法人 電力中央研究所、2.筑波大学・アイソトープ環境動態研究センター、3.福島大学・環境放射能研究所)

キーワード:福島第一原子力発電所事故、セシウム137、領域海洋モデル、直接漏洩、河川供給

A series of accidents at the Fukushima Dai-ichi Nuclear Power Plant (1F NPP) following the Great East Japan Earthquake and tsunami of 11 March 2011 resulted in the release of radioactive materials to the ocean. Measured 137Cs activities in the coastal zone adjacent to the 1F NPP are still higher than the one before the accident because sources to the ocean are still existing. The Regional Ocean Model System (ROMS) was employed for regional-scale simulation of 137Cs activity in the ocean offshore of Fukushima, the sources of radioactivity being direct release, atmospheric deposition, the inflow of 137Cs deposited into the ocean by atmospheric deposition outside the domain of the model, and river discharges. Direct release of 137Cs was estimated for 7 years after the accident by comparing simulated results and measured activities adjacent to the accident site. In addition, riverine discharge rates 137Cs were also estimated by multiplication between river flow simulation rate and measured 137Cs activities. Simulated atmospheric deposition to the ocean was employed by atmospheric transport model. Inflow of 137Cs from boundary sections was set by the results of the North Pacific scale ocean model. Sensitivity experiments were carried out to investigate the contributions of each source to measured 137Cs activities in the ocean. We focused on the term from 2013 to 2016 because there were few data in the river before 2012, and also focused on dissolved 137Cs because most of 137Cs is dissolved form in the ocean.

Simulated 137Cs activity attributable to direct release were in good agreement with measured data in the coast zone adjacent to the 1F NPP, because the effect of direct release was dominant from 2013 to 2016. On the other hands, simulated results attributable to inflow from boundary sections were slightly underestimated to the measured data offshore area. This suggests that recirculation of subducted 137Cs to the surface layer was underestimated in the North Pacific model. Apparent half-life of direct released and river discharged 137Cs activity were estimated to be about 1 year and 2 years, respectively. And apparent half-life of inflow of 137Cs activity was much longer due to time scale of dilution process in the North Pacific. Apparent half-life of each source should be similar to the measured one attributable to each source. Apparent half-life of measured 137Cs activity adjacent to the 1F NPP was about 1 year, on the other hand, the ones increased with increasing distance from the 1F NPP. Apparent half-life of measured data was about 2 years in front of the Uda river mouth where is far from the 1F NPP. Although 137Cs activity in this area was mainly affected by the river input, simulated 137Cs activities with river input were one fifth of observations. There is a brackish lagoon, Matsukawa-ura in front of Uda river mouth. The observed 137Cs activities in the Matsukawa-ura were 3-5 times larger than the one in the Uda river. This suggests the removal process from particle 137Cs to dissolved form in the brackish lagoon may be important.