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dc.creatorSips, A. C. C.es
dc.creatorSchweinzer, J.es
dc.creatorLuce, T. C.es
dc.creatorWolfe, S.es
dc.creatorUrano, H.es
dc.creatorJet Contributorses
dc.creatorGarcía Muñoz, Manueles
dc.date.accessioned2020-08-31T16:16:06Z
dc.date.available2020-08-31T16:16:06Z
dc.date.issued2018-12
dc.identifier.citationSips, A.C.C., Schweinzer, J., Luce, T.C., Wolfe, S., Urano, H., Jet Contributors, y García Muñoz, M. (2018). Assessment of the baseline scenario at q(95) similar to 3 for ITER. Nuclear Fusion, 58 (12), 26010. https://doi.org/10.1088/1741-4326/aade57.
dc.identifier.issn1741-4326es
dc.identifier.urihttps://hdl.handle.net/11441/100582
dc.description.abstractThe International Tokamak Physics Activity topical group on integrated operational scenarios has compiled a database of stationary H-mode discharges at q95 ~ 3 from AUG, C-Mod, DIII-D, JET and JT-60U, for both carbon wall and high-Z metal wall experiments with ~3300 entries. The analyses focus on discharges that are stationary for ⩾5 thermal energy confinement times to evaluate the baseline scenario proposed for ITER at 15 MA for achieving its goals of Q = 10, fusion power of 500 MW at normalised pressure, βN = 1.8 and normalised confinement as predicted by the standard H-mode scaling, H98y2 = 1. With the data restricted to stationary H-modes at q95 ~ 3, the database shows significant variation of thermal energy confinement compared to the standard H-mode scaling (IPB98(y,2)) in dimensionless form. The data show similar scaling with normalised gyro-radius, but more favourable scaling towards lower collision frequency and more favourable scaling with plasma beta. Using all the engineering variables employed in IPB98(y,2), results in an overfit due to correlations among the data. Moreover, there are significant residual trends in the confinement for plasma current, device size, loss power, and in particular for the plasma density. Significant differences between results obtained for devices with a carbon wall and high-Z metal wall are observed in the data, with data from carbon wall devices providing a larger operating space, encompassing ITER parameters or even exceeding them. H-modes in high-Z metal wall devices have, so-far, not accessed conditions at low collision frequencies, have lower normalised confinement (H98y2 ~ 0.8–0.9) at low input power or beta, achieving H98y2 ~ 1.0 only at input powers two times the L- to H-mode transition scaling predictions and at βN ~ 2.0. Hence, only the best H-modes with high-Z metal walls reach ITER baseline performance requirements. The data show that operating at high plasma density, with line-averaged density at 85% of Greenwald density is achievable for H98y2 > 0.95 for a range of plasma configurations, and that operation at low plasma inductance with li(3) ~ 0.7–0.75 is feasible. Scenario simulations employed for projecting the plasma performance in ITER should incorporate a lower thermal confinement at low plasma beta for the entry to burn and provide projections using higher levels of plasma core radiation by plasma impurities. Moreover, ITER projections should not subtract the core radiation in the evaluation of the thermal confinement time and H98y2, to allow a fair comparison with experimental data currently available. From the data presented here, it is likely that in ITER the energy confinement time will not increase with plasma density and will have no degradation with plasma beta. The analyses indicate that the data at q95 ~ 3 are consistent with achievement of the ITER mission goals at 15 MA.es
dc.description.sponsorshipEURATOM 633053es
dc.description.sponsorshipU.S. Department of Energy DE-FC02-99ER54512es
dc.formatapplication/pdfes
dc.format.extent24 p.es
dc.language.isoenges
dc.publisherIOP Publishinges
dc.relation.ispartofNuclear Fusion, 58 (12), 26010.
dc.rightsAttribution-NonCommercial-NoDerivatives 4.0 Internacional*
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/4.0/*
dc.subjectITERes
dc.subjectScenarioes
dc.subjectITPAes
dc.subjectConfinementes
dc.subjectPerfomancees
dc.subjectDatabasees
dc.titleAssessment of the baseline scenario at q(95) similar to 3 for ITERes
dc.typeinfo:eu-repo/semantics/articlees
dcterms.identifierhttps://ror.org/03yxnpp24
dc.type.versioninfo:eu-repo/semantics/publishedVersiones
dc.rights.accessRightsinfo:eu-repo/semantics/openAccesses
dc.contributor.affiliationUniversidad de Sevilla. Departamento de Física Atómica, Molecular y Nucleares
dc.relation.projectID633053es
dc.relation.projectIDDE-FC02-99ER54512es
dc.relation.publisherversionhttps://doi.org/10.1088/1741-4326/aade57es
dc.identifier.doi10.1088/1741-4326/aade57es
dc.contributor.groupUniversidad de Sevilla. RNM138: Física Nuclear Aplicadaes
dc.journaltitleNuclear Fusiones
dc.publication.volumen58es
dc.publication.issue12es
dc.publication.initialPage26010es

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