Ripple-induced neoclassical toroidal viscous torque in Augmented-First Plasma operation phase in ITER

Abstract A systematic calculation is performed on the ripple-induced neoclassical toroidal viscous (NTV) torque for new ITER scenarios designed for the Augmented-First Plasma (A-FP) operation phase with the full tungsten wall, where the plasma-wall gap is varied in view of mitigating the impact of tungsten wall-plasma interactions. The torque calculation includes drift kinetic response of the plasma thermal and energetic particles to the n = 18 ( n is the toroidal harmonic number) ripple field. For the plasma scenario with ~45 cm plasma-wall gap at the outboard mid-plane and considering the corrected ripple level of 0.17% by the ferritic steel inserts, the computed net NTV torque acting on the plasma column is in the sub-Nm level. However, with decreasing the plasma-wall gap, the computed net NTV torque can reach a level comparable to that produced by the neutral-beam momentum injection in ITER. Ripple correction by ferritic inserts reduces the net torque by a factor of 3.3 for all the three A-FP scenarios considered. The <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mi>n</mml:mi> <mml:msub> <mml:mi>ω</mml:mi> <mml:mi>d</mml:mi> </mml:msub> <mml:mo>=</mml:mo> <mml:mi>l</mml:mi> <mml:msub> <mml:mi>ω</mml:mi> <mml:mi>b</mml:mi> </mml:msub> </mml:mrow> </mml:math> (with ω d and ω b being the toroidal precession and bounce frequencies of trapped particles, respectively, and l an integer number) type of resonance-enhancement of the NTV torque, due to thermal particles, is found to be weak in ITER despite high- n of 18. The same also holds for the ITER 10 MA steady state scenario from the D-T operation phase, where the aforementioned resonance associated with fusion-born alphas is also included. The ripple-induced NTV torque is well below that produced by the resonant magnetic perturbation applied for controlling the type-I edge-localized mode in ITER.

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Publication Details

Journal
Nuclear Fusion
Published
2024-08-19
DOI
https://doi.org/10.1088/1741-4326/ad70cb
Citations
1
Primary Topic
Magnetic confinement fusion research
Type
article
Field-Weighted Citation Impact
0.66

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article

Ripple-induced neoclassical toroidal viscous torque in Augmented-First Plasma operation phase in ITER

S. D. Pinches, Yueqiang Liu, L. Schmitz, F. Koechl et al.
1 citations
Nuclear Fusion
Magnetic confinement fusion research
0.66
article

Ripple-induced neoclassical toroidal viscous torque in Augmented-First Plasma operation phase in ITER

S. D. Pinches, Yueqiang Liu, L. Schmitz, F. Koechl, Xue Bai, Y. Gribov, A. Loarte
article en
1 citations

Abstract

Abstract A systematic calculation is performed on the ripple-induced neoclassical toroidal viscous (NTV) torque for new ITER scenarios designed for the Augmented-First Plasma (A-FP) operation phase with the full tungsten wall, where the plasma-wall gap is varied in view of mitigating the impact of tungsten wall-plasma interactions. The torque calculation includes drift kinetic response of the plasma thermal and energetic particles to the n = 18 ( n is the toroidal harmonic number) ripple field. For the plasma scenario with ~45 cm plasma-wall gap at the outboard mid-plane and considering the corrected ripple level of 0.17% by the ferritic steel inserts, the computed net NTV torque acting on the plasma column is in the sub-Nm level. However, with decreasing the plasma-wall gap, the computed net NTV torque can reach a level comparable to that produced by the neutral-beam momentum injection in ITER. Ripple correction by ferritic inserts reduces the net torque by a factor of 3.3 for all the three A-FP scenarios considered. The <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mi>n</mml:mi> <mml:msub> <mml:mi>ω</mml:mi> <mml:mi>d</mml:mi> </mml:msub> <mml:mo>=</mml:mo> <mml:mi>l</mml:mi> <mml:msub> <mml:mi>ω</mml:mi> <mml:mi>b</mml:mi> </mml:msub> </mml:mrow> </mml:math> (with ω d and ω b being the toroidal precession and bounce frequencies of trapped particles, respectively, and l an integer number) type of resonance-enhancement of the NTV torque, due to thermal particles, is found to be weak in ITER despite high- n of 18. The same also holds for the ITER 10 MA steady state scenario from the D-T operation phase, where the aforementioned resonance associated with fusion-born alphas is also included. The ripple-induced NTV torque is well below that produced by the resonant magnetic perturbation applied for controlling the type-I edge-localized mode in ITER.

Nuclear FusionVol. 64(10)
ITER (FR), University of California, Los Angeles (US), General Atomics (United States) (US)
Basic Energy Sciences
Openalex Percentile: Top 15%
Magnetic confinement fusion research
0.66
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