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Kajita, Shin*; Hatae, Takaki; Sakuma, Takeshi; Takamura, Shuichi*; Ono, Noriyasu*; Itami, Kiyoshi
Plasma and Fusion Research (Internet), 7(Sp.1), p.2405121_1 - 2405121_4, 2012/09
Ide, Shunsuke; Hayashi, Nobuhiko; Honda, Mitsuru; Urano, Hajime; Suzuki, Takahiro; Miyata, Yoshiaki; Aiba, Nobuyuki; Shiraishi, Junya; Kurita, Genichi; Fujita, Takaaki
Plasma and Fusion Research (Internet), 7(Sp.1), p.2403131_1 - 2403131_4, 2012/09
no abstracts in English
Uto, Hiroyasu; Tobita, Kenji; Someya, Yoji; Nakamura, Makoto
Plasma and Fusion Research (Internet), 7(Sp.1), p.2405109_1 - 2405109_4, 2012/07
For optimization of coolant conditions in DEMO blanket design, a two-dimensional (2-D) nuclear-thermal-coupled analysis code, DOHEAT, has been modified. The striking feature of DOHEAT is to have a user-friendly interface that enables users to create an appropriate analysis model for different blanket concepts without much difficulty. However, in the previous version of DOHEAT, the coolant temperature is given as an input data. Actually, a temperature change of the coolant along the cooling tube needs to be determined implicitly when the inlet temperature, pressure and flow speed are given. In modified DOHEAT, the coolant condition calculation module was added into the 2-D thermal analysis module, and the temperature profile in the blanket was provided based on the nuclear heating rate profile and coolant temperature. A validation calculation indicates that DOHEAT provides reasonable results on the temperature profile in the blanket.
Someya, Yoji; Tobita, Kenji
Plasma and Fusion Research (Internet), 7(Sp.1), p.2405066_1 - 2405066_4, 2012/07
Decay heat of activated materials is important in safety of fusion DEMO reactor. Effects of decay heat for main components of the SlimCS DEMO reactor are studied. The main reactor components consist of the inboard (IB) and outboard (OB) blanket modules, and divertor. The decay heats of IB blanket, OB blanket and divertor are calculated by a design code for radioactive, ACT-4. The dominant radioactive nuclide determining the decay heat is short-lived nuclide at the immediately after the shutdown of operation. Therefore, the decay heat depends in a large part on neutron flux after the shout down. On the other hand, the dominant reaction determining the decay heat is (n, ) reaction. When thermal neutron is decreased, the decay heat is decreased in the blanket and divertor. Methods of reducing the decay heat are (1) decreased thermal neutron and (2) decreased the fusion power. Finally, a detailed estimation of between (1) and (2) is discussed from view point of fusion DEMO reactor.
Bierwage, A.; Aiba, Nobuyuki; Todo, Yasushi*; Deng, W.*; Ishikawa, Masao; Matsunaga, Go; Shinohara, Koji; Yagi, Masatoshi
Plasma and Fusion Research (Internet), 7(Sp.1), p.2403081_1 - 2403081_4, 2012/07
Hada, Kazuyoshi*; Nagasaki, Kazunobu*; Masuda, Kai*; Kinjo, Ryota*; Ide, Shunsuke; Isayama, Akihiko
Plasma and Fusion Research (Internet), 7(Sp.1), p.2403104_1 - 2403104_5, 2012/07
no abstracts in English
Narita, Emi*; Takizuka, Tomonori*; Hayashi, Nobuhiko; Fujita, Takaaki; Ide, Shunsuke; Honda, Mitsuru; Isayama, Akihiko; Itami, Kiyoshi; Kamada, Yutaka; Tanaka, Yasuyuki*; et al.
Plasma and Fusion Research (Internet), 7(Sp.1), p.2403102_1 - 2403102_5, 2012/07
Isayama, Akihiko; Kobayashi, Takayuki; Yokokura, Kenji; Shimono, Mitsugu; Sawahata, Masayuki; Suzuki, Sadaaki; Terakado, Masayuki; Hiranai, Shinichi; Wada, Kenji; Hinata, Jun; et al.
Plasma and Fusion Research (Internet), 7(Sp.1), p.2405029_1 - 2405029_5, 2012/05
no abstracts in English
Seto, Keita*; Nagatomo, Hideo*; Koga, J. K.; Mima, Kunioki*
Plasma and Fusion Research (Internet), 7(Sp.1), p.2404010_1 - 2404010_4, 2012/02
Hemmi, Tsutomu; Harjo, S.; Nunoya, Yoshihiko; Kajitani, Hideki; Koizumi, Norikiyo; Nakajima, Hideo; Aizawa, Kazuya; Machiya, Shutaro*; Osamura, Kozo*
no journal, ,
Internal strain in Cable-In-Conduit Conductors (CICC) is caused by differences in the coefficients of thermal expansion between NbSn strands and the stainless steel jacket over a temperature range of 5 - 923 K. In addition, transverse electromagnetic loading is generated by a current of 68 kA and a magnetic field of 11.8 T in the case of ITER TF coils. The performances of Nb
Sn strands change significantly, depending on the presence of strain. The presence of internal strain in Nb
Sn cables is important to evaluate the superconducting performance. However, the strain of strands in the conductor has not been measured so far because of the cabling configuration and their location in a jacket. Internal strain can be determined by neutron diffraction measurement using Takumi of J-PARC. Test results of the neutron diffraction and the role of the neutron diffraction measurement for the investigation of Tcs degradation of short conductor sample will be presented and discussed.
Harjo, S.; Aizawa, Kazuya; Ito, Takayoshi*; Abe, Jun; Osamura, Kozo*; Hemmi, Tsutomu; Jin, X.*; Nakamoto, Tatsushi*; Awaji, Satoshi*; Takahashi, Koki*
no journal, ,
Saigusa, Mikio*; Sugawara, Shuhei*; Atsumi, Kohei*; Oda, Yasuhisa; Yamaguchi, Tomoki*; Sakamoto, Keishi
no journal, ,
Tojo, Hiroshi; Ejiri, Akira*; Hiratsuka, Junichi*; Yamaguchi, Takashi*; Takase, Yuichi*; Itami, Kiyoshi
no journal, ,