@article{oai:repo.qst.go.jp:00079113,
 author = {Miyoshi, Yuuya and Hiwatari, Ryoji and Someya, Yoji and Asakura, Nobuyuki and Tokunaga, Shinsuke and Homma, Yuuki and Sakamoto, Yoshiteru and Yuuya, Miyoshi and Ryoji, Hiwatari and Yoji, Someya and Nobuyuki, Asakura and Shinsuke, Tokunaga and Yuuki, Homma and Yoshiteru, Sakamoto},
 journal = {Fusion Engineering and Design},
 month = {Jul},
 note = {The blanket modules in DEMO are made of reduced-activation ferritic martensitic (RAFM) steel F82H. This material is ferromagnetic and it drags the magnetic field lines into the first wall (FW). Because of this, the heat load by the plasma heat flux, which goes along the magnetic field line will become higher. In this research, the first analysis of such effect has been done. The extra magnetic field Bm made by RAFM wall becomes higher at inner midplane, and the heat load at the module front surface becomes 1.3 MW/m2 to 5 MW/m2. Additionally, near the toroidal gaps, BM becomes high. Thus, at the top of the FW, magnetic field lines are dragged into the toroidal gaps directly because, the magnetic flux surface is not closed. This makes high (about 10MW/m2) heat load concentration at the moduel edge. The effect of the NBI port is also analyzed. Also near the port, Bm becomes high and the orbit of the magnetic field lines are changed. The effect of this doesn't occur near the port, but far region such as inner midplane or top of the FW. The heat load becomes 6 MW/m2 at inner midplane. These results indicate that the effect of RAFM steel on the FW heat load is not negligible, and more detailed analysis is necessary.},
 title = {Effect of dragged magnetic field lines into RAFM steel blanket modules on first wall heat load},
 volume = {156},
 year = {2020}
}