Please use this identifier to cite or link to this item: https://hdl.handle.net/10216/143451
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dc.creatorM. F. F. Nave
dc.creatorE. Delabie
dc.creatorJ. Ferreira
dc.creatorJ. Garcia
dc.creatorD. King
dc.creatorM. Lennholm
dc.creatorB. Lomanowski
dc.creatorF. Parra
dc.creatorP. Rodriguez- Fernandez
dc.creatorJ. Bernardo
dc.creatorM. Baruzzo
dc.creatorM. Barnes
dc.creatorF. Casson
dc.creatorJ.C. Hillesheim
dc.creatorA. Hubber
dc.creatorE. Joffrin
dc.creatorA. Kappatou
dc.creatorC. F. Maggi
dc.creatorA. Mauriya
dc.creatorL. Meneses
dc.creatorM. Romanelli
dc.creatorF. Salzedas
dc.creatorJET Contributors
dc.date.accessioned2022-09-07T12:16:02Z-
dc.date.available2022-09-07T12:16:02Z-
dc.date.issued2022-06-30
dc.identifier.othersigarra:574202
dc.identifier.urihttps://hdl.handle.net/10216/143451-
dc.description.abstractJET is the largest tokamak in operation and the main link between smaller machines, where intrinsic rotation has been mostly studied, and ITER the next step in fusion research. While the main ion in present tokamak plasmas is a single hydrogen isotope, mainly Deuterium (D) in JET, future nuclear fusion machines, such as ITER, will operate with a mixture of D and Tritium (T). Recent experimental campaigns at JET performed a series of experiments with different hydrogen isotopes, designed to clarify the impact that isotope mass has on physics questions, and in particular transport and confinement questions, relevant for reliable predictions for ITER. This talk will report on experiments that studied for the first time the isotope effect on intrinsic rotation in a tokamak plasma, by comparing rotation measurements in Hydrogen (H), D and T in Ohmic plasmas. One of the objects of the JET intrinsic rotation experiments was to study rotation reversals, a puzzling phenomenon commonly observed in small and medium size tokamaks, where a transition from monotonic to non-monotonic rotation profiles is observed at a critical density, in some cases leading to plasmas with central and outer regions flowing in opposite directions. At JET, as the density increased, two consecutive core rotation reversals were observed. The first, shows a change from peaked co- current rotation to hollow profiles with the core in some cases counter-current rotating, similarly to observations in smaller tokamaks. Further increasing the density leads to restoration of monotonic profiles. The magnitude of the core rotation was found to depend on isotope type, stronger co-current rotation observed in H. Core counter-rotation was observed with D and T but not with H. Gyrokinetic calculations, show that the low-density rotation reversal, for all three isotopes, occurs close to the density of transition from dominant TEM to ITG instabilities. The type of instability cannot be associated to different directions of core rotation since for all three isotopes, co-rotation is observed with dominant TEM for the low- densities and ITG for high-densities. Non-linear modeling of rotation profiles with the low- flow model show changes of sign in rotation gradient, qualitatively consistent with the observation of peaked to hollow to peaked profiles as the density increased .These results have strong implications for ITER, as rotation extrapolations from present day experiments, mostly based on D plasmas, might not recover in full the physics mechanisms playing a role in momentum transport.
dc.language.isoeng
dc.relation.ispartof48th EPS Plasma Physics Conference
dc.rightsopenAccess
dc.subjectFísica, Engenharia nuclear, Física
dc.subjectPhysics, Nuclear engineering, Physical sciences
dc.titleIsotope Effects on Intrinsic Toroidal Rotation and Rotation Reversals
dc.typeArtigo em Livro de Atas de Conferência Internacional
dc.contributor.uportoFaculdade de Engenharia
dc.subject.fosCiências exactas e naturais::Física
dc.subject.fosNatural sciences::Physical sciences
Appears in Collections:FEUP - Artigo em Livro de Atas de Conferência Internacional

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