Overview of ASDEX Upgrade results

Zohm, H; Adamek, J; Angioni, C; Antar, G; Atanasiu, CV; Balden, M; Becker, W; Behler, K; Behringer, K; Bergmann, A; Bertoncelli, T; Bilato, R; Bobkov, V; Boom, J; Bottino, A; Brambilla, M; Braun, F; Brudgam, M; Buhler, A; Chankin, A; Classen, I; Conway, GD; Coster, DP; de Marne, P; D, Inca R; Drube, R; Dux, R; Eich, T; Engelhardt, K; Esposito, B; Fahrbach, HU; Fattorini, L; Fink, J; Fischer, R; Flaws, A; Foley, M; Forest, C; Fuchs, JC; Gal, K [Gál-Hobirk, Kinga Izabella (Plazmafizika), szerző] Plazmafizikai Főosztály (KFKI RMKI); Munoz, MG; Adamov, MG; Giannone, L; Gorler, T; Gori, S; da Graca, S; Granucci, G; Greuner, H; Gruber, O; Gude, A; Gunter, S; Haas, G; Hahn, D; Harhausen, J; Hauff, T; Heinemann, B; Herrmann, A; Hicks, N; Hobirk, J; Holzl, M; Holtum, D; Hopf, C; Horton, L; Huart, M; Igochine, V; Janzer, M; Jenko, F; Kallenbach, A; Kalvin, S [Kálvin, Sándor Csaba, szerző] Plazmafizikai Főosztály (KFKI RMKI); Kardaun, O; Kaufmann, M; Kick, M; Kirk, A; Klingshirn, HJ; Koscis, G; Kollotzek, H; Konz, C; Krieger, K; Kurki-Suonio, T; Kurzan, B; Lackner, K; Lang, PT; Langer, B; Lauber, P; Laux, M; Leuterer, F; Likonen, J; Liu, L; Lohs, A; Lunt, T; Lyssoivan, A; Maggi, CF; Manini, A; Mank, K; Manso, ME; Mantsinen, M; Maraschek, M; Martin, P; Mayer, M; McCarthy, P; McCormick, K; Meister, H; Meo, F; Merkel, P; Merkel, R; Mertens, V; Merz, F; Meyer, H; Mlynek, A; Monaco, F; Muller, HW; Munich, M; Murmann, H; Neu, G; Neu, R; Neuhauser, J; Nold, B; Noterdaeme, JM; Pautasso, G; Pereverzev, G; Poli, E; Potzel, S; Puschel, M; Putterich, T; Pugno, R; 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; Schilling, HB; Schirmer, J; Schmid, A; Schmid, K; Schneider, W; Schramm, G; Schrittwieser, R; Schustereder, W; Schweinzer, J; Schweizer, S; Scott, B; Seidel, U; Sempf, M; Serra, F; Sertoli, M; Siccinio, M; Sigalov, A; Silva, A; Sips, CC; Speth, E; Stabler, A; Stadler, R; Steuer, KH; Stober, J; Streibl, B; Strumberger, E; Suttrop, W; Tardini, G; Tichmann, C; Treutterer, W; Troster, C; Urso, L; Vainonen-Ahlgren, E; Varela, P; Vermare, L; Volpe, F; Wagner, D; Wigger, C; Wischmeier, M; Wolfrum, E; Wursching, E; Yadikin, D; Yu, Q; Zasche, D; Zehetbauer, T; Zilker, M

Angol nyelvű Tudományos Sokszerzős vagy csoportos szerzőségű szakcikk (Folyóiratcikk)
Megjelent: NUCLEAR FUSION 0029-5515 1741-4326 49 (10) Paper: 104009 2009
  • SJR Scopus - Condensed Matter Physics: D1
Azonosítók
Szakterületek:
    ASDEX Upgrade was operated with a fully W-covered wall in 2007 and 2008. Stationary H-modes at the ITER target values and improved H-modes with H up to 1.2 were run without any boronization. The boundary conditions set by the full W wall (high enough ELM frequency, high enough central heating and low enough power density arriving at the target plates) require significant scenario development, but will apply to ITER as well. D retention has been reduced and stationary operation with saturated wall conditions has been found. Concerning confinement, impurity ion transport across the pedestal is neoclassical, explaining the strong inward pinch of high-Z impurities in between ELMs. In improved H-mode, the width of the temperature pedestal increases with heating power, consistent with a beta(1/2)(pol,ped) scaling. In the area of MHD instabilities, disruption mitigation experiments using massive Ne injection reach volume averaged values of the total electron density close to those required for runaway suppression in ITER. ECRH at the q = 2 surface was successfully applied to delay density limit disruptions. The characterization of fast particle losses due to MHD has shown the importance of different loss mechanisms for NTMs, TAEs and also beta-induced Alfven eigenmodes (BAEs). Specific studies addressing the first ITER operational phase show that O1 ECRH at the HFS assists reliable low-voltage breakdown. During ramp-up, additional heating can be used to vary l(i) to fit within the ITER range. Confinement and power threshold in He are more favourable than in H, suggesting that He operation could allow us to assess H-mode operation in the non-nuclear phase of ITER operation.
    Hivatkozás stílusok: IEEEACMAPAChicagoHarvardCSLMásolásNyomtatás
    2021-05-09 22:39