2022
DOI: 10.1088/1741-4326/ac5667
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Role of NBI fuelling in contributing to density peaking between the ICRH and NBI identity plasmas on JET

Abstract: Density peaking has been studied between an ICRH and NBI identity plasma in JET. The comparison shows that 8MW of NBI heating/fueling increases the density peaking by a factor of two, being R/Ln=0.45 for the ICRH pulse and R/Ln=0.93 for the NBI one averaged radially over ρtor=0.4‒0.8. The dimensionless profiles of q, ρ*, υ*, βn and Ti/Te≈1 were matched within 5% difference except in the central part of the plasma (ρtor<0.3). The difference in the curvature pinch (same q-profile) and thermo-pinch (Ti=Te) bet… Show more

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Cited by 4 publications
(3 citation statements)
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“…The normalised n e gradient length R/L n averaged over ρ TOR = 0.4-0.8 is R/L n = 0.93 and R/L n = 0.45 for the NBI and ICRH case, respectively. The increase in the density peaking by a factor of 2 can be explained solely by NBI fuelling, since, according to GENE and TGLF simulations, the background transport is the same between the ICRH and NBI discharges [58]. This result is consistent with that from a dimensionless collisionality scan in JET H-mode plasma [59], showing the NBI contributing to ∼50% of the fuelling.…”
Section: Core and Pedestal Transport And Confinementsupporting
confidence: 80%
“…The normalised n e gradient length R/L n averaged over ρ TOR = 0.4-0.8 is R/L n = 0.93 and R/L n = 0.45 for the NBI and ICRH case, respectively. The increase in the density peaking by a factor of 2 can be explained solely by NBI fuelling, since, according to GENE and TGLF simulations, the background transport is the same between the ICRH and NBI discharges [58]. This result is consistent with that from a dimensionless collisionality scan in JET H-mode plasma [59], showing the NBI contributing to ∼50% of the fuelling.…”
Section: Core and Pedestal Transport And Confinementsupporting
confidence: 80%
“…the R/L n radial profiles corresponding to simulations that locally give as output Γ profiles that are smaller and larger, respectively, than the experimental particle source Γ exp. (an example of local flux-tube GK analysis of density peaking, comparing cases from the JET tokamak with or without NBI can be found in [25]). The ZPFD approach, on the contrary, can not be so trivially generalized to a case with finite Γ exp.…”
Section: Global Zpfd Simulationsmentioning
confidence: 99%
“…Gas puff modulation technique will be exploited here as the extra tool to quantify the core isotope scaling in the electron particle transport channel between the Deuterium and Tritium plasmas. There is a lot of previous experience at JET in using the gas puff modulation technique to analyse electron particle transport and obtain electron particle transport coefficients [22,23]. Recently, the methodology has been further refined and optimised also to be appropriately used in this isotope mass scaling experiment [24].…”
Section: Introductionmentioning
confidence: 99%