A power-balance model, with radiation losses from impurities and neutrals, gives a unified description of the density limit (DL) of the stellarator, the L-mode tokamak, and the reversed field pinch (RFP). The model predicts a Sudo-like scaling for the stellarator, a Greenwald- like scaling, alpha I-p(8/9), for the RFP and the ohmic tokamak, a mixed scaling, alpha (PIp4/9)-I-4/9, for the additionally heated L-mode tokamak. In a previous paper (Zanca et al 2017 Nucl. Fusion 57 056010) the model was compared with ohmic tokamak, RFP and stellarator experiments. Here, we address the issue of the DL dependence on heating power in the L-mode tokamak. Experimental data from high-density disrupted L-mode discharges performed at JET, as well as in other machines, arc taken as a term of comparison. The model fits the observed maximum densities better than the pure Greenwald limit.
A power-balance model of the density limit in fusion plasmas: application to the L-mode tokamak
Zanca, P; Sattin, F; Escande, DF; Abduallev, S; Abhangi, M; Abreu, P; Afzal, M; Aggarwal, KM; Ahlgren, T; Ahn, JH; Aho-Mantila, L; Aiba, N; Airila, M; Albanese, R; Aldred, V; Alegre, D; Alessi, E; Aleynikov, P; Alfier, A; Alkseev, A; Allinson, M; Alper, B; Alves, E; Ambrosino, G; Ambrosino, R; Amicucci, L; Amosov, V; Sunden, EA; Angelone, M; Anghel, M; Angioni, C; Appel, L; Appelbee, C; Arena, P; Ariola, M; Arnichand, H; Arshad, S; Ash, A; Ashikawa, N; Aslanyan, V; Asunta, O; Auriemma, F; Austin, Y; Avotina, L; Axton, MD; Ayres, C; Bacharis, M; Baciero, A; Baiao, D; Bailey, S; Baker, A; Balboa, I; Balden, M; Balshaw, N; Bament, R; Banks, JW; Baranov, YF; Barnard, MA; Barnes, D; Barnes, M; Barnsley, R; Wiechec, AB; Orte, LB; Baruzzo, M; Basiuk, V; Bassan, M; Bastow, R; Batista, A; Batistoni, P; Baughan, R; Bauvir, B; Baylor, L; Bazylev, B; Beal, J; Beaumont, PS; Beckers, M; Beckett, B; Becoulet, A; Bekris, N; Beldishevski, M; Bell, K; Belli, F; Bellinger, M; Belonohy, E; Ben Ayed, N; Benterman, NA; 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2019-01-01
Abstract
A power-balance model, with radiation losses from impurities and neutrals, gives a unified description of the density limit (DL) of the stellarator, the L-mode tokamak, and the reversed field pinch (RFP). The model predicts a Sudo-like scaling for the stellarator, a Greenwald- like scaling, alpha I-p(8/9), for the RFP and the ohmic tokamak, a mixed scaling, alpha (PIp4/9)-I-4/9, for the additionally heated L-mode tokamak. In a previous paper (Zanca et al 2017 Nucl. Fusion 57 056010) the model was compared with ohmic tokamak, RFP and stellarator experiments. Here, we address the issue of the DL dependence on heating power in the L-mode tokamak. Experimental data from high-density disrupted L-mode discharges performed at JET, as well as in other machines, arc taken as a term of comparison. The model fits the observed maximum densities better than the pure Greenwald limit.
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Il report seguente simula gli indicatori relativi alla propria produzione scientifica in relazione alle soglie ASN 2023-2025 del proprio SC/SSD. Si ricorda che il superamento dei valori soglia (almeno 2 su 3) è requisito necessario ma non sufficiente al conseguimento dell'abilitazione. La simulazione si basa sui dati IRIS e sugli indicatori bibliometrici alla data indicata e non tiene conto di eventuali periodi di congedo obbligatorio, che in sede di domanda ASN danno diritto a incrementi percentuali dei valori. La simulazione può differire dall'esito di un’eventuale domanda ASN sia per errori di catalogazione e/o dati mancanti in IRIS, sia per la variabilità dei dati bibliometrici nel tempo. Si consideri che Anvur calcola i valori degli indicatori all'ultima data utile per la presentazione delle domande. La presente simulazione è stata realizzata sulla base delle specifiche raccolte sul tavolo ER del Focus Group IRIS coordinato dall’Università di Modena e Reggio Emilia e delle regole riportate nel DM 589/2018 e allegata Tabella A. Cineca, l’Università di Modena e Reggio Emilia e il Focus Group IRIS non si assumono alcuna responsabilità in merito all’uso che il diretto interessato o terzi faranno della simulazione. Si specifica inoltre che la simulazione contiene calcoli effettuati con dati e algoritmi di pubblico dominio e deve quindi essere considerata come un mero ausilio al calcolo svolgibile manualmente o con strumenti equivalenti.