Experimental studies of ITER demonstration discharges

Sips, ACC; Casper, TA; Doyle, EJ; Giruzzi, G; Gribov, Y; Hobirk, J; Hogeweij, GMD; Horton, LD; Hubbard, AE; Hutchinson, I; Ide, S; Isayama, A; Imbeaux, F; Jackson, GL; Kamada, Y; Kessel, C; Kochl, F; Lomas, P; Litaudon, X; Luce, TC; Marmar, E; Mattei, M; Nunes, I; Oyama, N; Parail, V; Portone, A; Saibene, G; Sartori, R; Stober, JK; Suzuki, T; Wolfe, SM; Anda, G; Dunai, D; Gál, K; Kálvin, S; Kocsis, G; Petravich, G; Szepesi, T; Zoletnik, S [Zoletnik, Sándor (Plazmafizika), author] Department of Plasma Physics (KFKI RMKI); Mayer, M; Andrzejczuk, M; Dux, R; Fortuna-Zalesna, E; Hakola, A; Koivuranta, S; Krieger, K; Kurzydlowski, KJ; Likonen, J; Matern, G; Neu, R; Ramos, G; Rasinski, M; Rohde, V; Sugiyama, K; Wiltner, A; Zielinski, W; Kallenbach, A; Adamek, J; Aho-Mantila, L; Äkäslompolo, S; Angioni, C; Atanasiu, C V; Balden, M; Behler, K; Belonohy, E; Bergmann, A; Bernert, M; Bilato, R; Bobkov, V; Boom, J; Bottino, A; Braun, F; Brüdgam, M; Buhler, A; Burckhart, A; Chankin, A; Classen, I G J; Conway, G D; Coster, D P; de Marné, P; D'Inca, R; Drube, R; Dux, R; Eich, T; Endstrasser, N; Engelhardt, K; Esposito, B; Fable, E; Fahrbach, H -U; Fattorini, L; Fischer, R; Flaws, A; Fünfgelder, H; Fuchs, J C; Gál, K; García, Muñoz M; Geiger, B; Gemisic, Adamov M; Giannone, L; Giroud, C; Görler, T; da Graca, S; Greuner, H; Gruber, O; Gude, A; Günter, S; Haas, G; Hakola, A H; Hangan, D; Happel, T; Hauff, T; Heinemann, B; Herrmann, A; Hicks, N; Hobirk, J; Höhnle, H; Hölzl, M; Hopf, C; Horton, L; Huart, M; Igochine, V; Ionita, C; Janzer, A; Jenko, F; Käsemann, C -P; Kálvin, S; Kardaun, O; Kaufmann, M; Kirk, A; Klingshirn, H -J; Kocan, M; Kocsis, G; Kollotzek, H; Konz, C; Koslowski, R; Krieger, K; Kurki-Suonio, T; Kurzan, B; Lackner, K; Lang, P T; Lauber, P; Laux, M; Leipold, Frank; Leuterer, F; Lohs, A; Luhmann, N C Jr; Lunt, T; Lyssoivan, A; Maier, H; Maggi, C; Mank, K; Manso, M -E; Maraschek, M; Martin, P; Mayer, M; McCarthy, P J; McDermott, R; Meister, H; Menchero, L; Meo, Fernando; Merkel, P; Merkel, R; Mertens, V; Merz, F; Mlynek, A; Monaco, F; Müller, H W; Münich, M; Murmann, H; Neu, G; Neu, R; Nold, B; Noterdaeme, J -M; Park, H K; Pautasso, G; Pereverzev, G; Podoba, Y; Pompon, F; Poli, E; Polochiy, K; Potzel, S; Prechtl, M; Püschel, M J; Pütterich, T; Rathgeber, S K; Raupp, G; Reich, M; Reiter, B; Ribeiro, T; Riedl, R; Rohde, V; Roth, J; Rott, M; Ryter, F; Sandmann, W; Santos, J; Sassenberg, K; Sauter, P; Scarabosio, A; Schall, G; Schmid, K; Schneider, P A; Schneider, W; Schramm, G; Schrittwieser, R; Schweinzer, J; Scott, B; Sempf, M; Serra, F; Sertoli, M; Siccinio, M; Sigalov, A; Silva, A; Sips, A C C; Sommer, F; Stäbler, A; Stober, J; Streibl, B; Strumberger, E; Sugiyama, K; Suttrop, W; Szepesi, T; Tardini, G; Tichmann, C; Told, D; Treutterer, W; Urso, L; Varela, P; Vincente, J; Vianello, N; Vierle, T; Viezzer, E; Vorpahl, C; Wagner, D; Weller, A; Wenninger, R; Wieland, B; Wigger, C; Willensdorfer, M; Wischmeier, M; Wolfrum, E; Würsching, E; Yadikin, D; Yu, Q; Zammuto, I; Zasche, D; Zehetbauer, T; Zhang, Y; Zilker, M; Zohm, H

English Scientific Study Group (Journal Article)
Published: NUCLEAR FUSION 0029-5515 1741-4326 49 (8) Paper: 085015 2009
  • SJR Scopus - Condensed Matter Physics: D1
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    Key parts of the ITER scenarios are determined by the capability of the proposed poloidal field (PF) coil set. They include the plasma breakdown at low loop voltage, the current rise phase, the performance during the flat top (FT) phase and a ramp down of the plasma. The ITER discharge evolution has been verified in dedicated experiments. New data are obtained from C-Mod, ASDEX Upgrade, DIII-D, JT-60U and JET. Results show that breakdown for E-axis < 0.23-0.33 V m(-1) is possible unassisted (ohmic) for large devices like JET and attainable in devices with a capability of using ECRH assist. For the current ramp up, good control of the plasma inductance is obtained using a full bore plasma shape with early X-point formation. This allows optimization of the flux usage from the PF set. Additional heating keeps l(i)(3) < 0.85 during the ramp up to q(95) = 3. A rise phase with an H-mode transition is capable of achieving l(i)(3) < 0.7 at the start of the FT. Operation of the H-mode reference scenario at q(95) similar to 3 and the hybrid scenario at q(95) = 4-4.5 during the FT phase is documented, providing data for the l(i) (3) evolution after the H-mode transition and the li (3) evolution after a back-transition to L-mode. During the ITER ramp down it is important to remain diverted and to reduce the elongation. The inductance could be kept <= 1.2 during the first half of the current decay, using a slow I-p ramp down, but still consuming flux from the transformer. Alternatively, the discharges can be kept in H-mode during most of the ramp down, requiring significant amounts of additional heating.
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    2021-04-21 21:29