Activation properties of NbSn, NbTi and GFRP irradiated with D-T neutrons
D-T中性子照射によるNbSn, NbTi及びGFRP材料の放射化特性
落合 謙太郎; 西村 新*; 西谷 健夫; 西嶋 茂宏*
Ochiai, Kentaro; Nishimura, Arata*; Nishitani, Takeo; Nishijima, Shigehiro*
核融合炉用超伝導コイル候補材であるNbSn, NbTi及びGFRP材料のDT中性子照射実験を行い、それらの放射化特性を調べた。照射サンプルはNbSnとNbTiのマルチフィラメント線材及び商業用GFRP(G10CR)を用いた。原子力機構の核融合中性子源施設FNSを用いて410n/mまで照射し、照射後サンプルの線量率と誘導線エネルギースペクトルを測定した。測定の結果、主要な放射性核種はNb-92m, Sn-117m, Sn-113とCo-60であった。また、Na-24, Na-22, Sc-47, Co-57, As-74, Rb-83, Mn-54と若干の未知の放射性核種がGFRPから検知され、GFRP中の付加化合物の放射化によるものであることがわかった。NbSn, NbTiとGFRPサンプルの照射直後の線量率は160Sv/h, 120Sv/hと20Sv/hであった。照射から5ヵ月後の線量率はいずれも約3Sv/hまで減衰した。また線エネルギースペクトル測定の結果からNbSnとNbTi線材及びGFRPの最終的な線量率はCo-60(5.27y)及びNa-22(2.60y)によって支配されることを明らかにした。
NbSn, NbTi wires and glass fiber reinforced plastics (GFRP) are prospective candidate materials of the superconducting coil assembly for fusion reactors. These materials are activated by D-T neutrons penetrating through the reactor core. From the radioactive waste point of view, it is important to investigate the activation properties for these candidate materials. However, no experiment has been done to investigate the activation properties for these materials. Therefore, we have carried out the experimental investigation of the activation properties of NbSn, NbTi wires and GFRP materials. The neutron irradiation experiment has been done by the FNS D-T neutron source of JAEA. We used complex multi-filaments wires of NbSn and NbTi produced by FURUKAWA-electric Ltd. and a commercial GFRP (G10CR) plate. These samples were irradiated up to the neutron fluence of 410n/m corresponding to about one twentieth neutron fluence expected for ITER life time. After the cooling time, the dose rates and the emitted -ray spectra were measured with a survey meter and a Ge detector, respectively. Induced major radioactive nuclides are Nb-92m, Sn-117m, Sn-113 and Co-60 for NbSn, and Nb-92m, Sc-46 and Co-60 for NbTi. Also Na-24, Na-22, Sc-47, Co-57, As-74, Rb-83, Mn-54 and some unknown radioactive nuclides were observed from the irradiated GFRP. It is considered that those radioactive elements are due to the activation of the additive compounds in GFRP. The initial dose rates of the irradiated NbSn, NbTi and GFRP samples were 160Sv/h, 120Sv/h and 20Sv/h, respectively. After 5 months from the irradiation, these dose rates were reduced to 2-4Sv/h. Also, from the measured -ray spectra, it was found that the final dose rates of NbSn and NbTi wires were dominated by Co-60 (5.27y) and the that of GFRP was dominated by Na-22 (2.60y).