Bulletin of the American Physical Society
66th Annual Meeting of the APS Division of Plasma Physics
Monday–Friday, October 7–11, 2024; Atlanta, Georgia
Session TP12: Poster Session VII:
Turbulence and transport in fusion plasmas
ITER
MFE Heating and Energetic Particles
Self-organized configuration FRC, RFP, Spheromak
9:30 AM - 12:30 PM
Thursday, October 10, 2024
Hyatt Regency
Room: Grand Hall West
Abstract: TP12.00053 : Quasi-Linear Simulation of Energetic Ion Relaxation in ITER Mediated by Alfvén Instabilities*
Presenter:
Nikolai N Gorelenkov
(Princeton Plasma Physics Laboratory)
Authors:
Nikolai N Gorelenkov
(Princeton Plasma Physics Laboratory)
Vinicius N Duarte
(Princeton Plasma Physics Laboratory)
Marina Gorelenkova
(Princeton Plasma Physics Laboratory)
Zhihong Lin
(University of California, Irvine)
Simon D Pinches
(ITER Organization)
products or auxiliary heating fast ions will be confined sufficiently
long to compensate for thermal plasma energy losses is addressed.
This issue is mediated by the instability of low, sub-cyclotron frequency Alfven
eigenmodes (AEs) in ITER steady-state scenario. Using a recently
revisited quasi-linear treatment of EP relaxation dynamics in the
presence of AEs we apply it to ITER steady state conditions. We have
found that although the resulting fast ion transport remains modest if
classical particle slowing down is assumed. We report on AE dynamics
utilizing several tools: the comprehensive linear stability study of
the sub-cyclotron Alfvenic spectrum computed by the ideal MHD
NOVA simulations, drift kinetic NOVA-C
calculations for wave-particle interaction and AE growth/damping
rates, and eventually the predictive quasi-linear modeling code RBQ to
assess the EP relaxation on the equilibrium time scale [N.Gorelenkov
et al., PLA'21]. The applications of RBQ in its 2D version have shown
that the AE amplitudes remain relatively low, deltaB/B < 0.003, for
all 42 analyzed unstable TAE modes. We have identified a potentially
important effect of AEs on EP confinement in ITER which is due to EP
depletion near the plasma center. This effect is connected with the
beam ion and fusion alpha particle current drives which is expected to
be also depleted near the center.
*This work was supported by the US DoE under contract DE-AC02-09CH11466.
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