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Validity limits of the passive treatment of impurities in gyrokinetic tokamak simulations

Authors :
Chabha Djerroud
J. Médina
Maxime Lesur
Thomas Drouot
Xavier Garbet
Etienne Gravier
Thierry Reveille
T. Cartier-Michaud
Malik Idouakass
Kyungtak Lim
Jérôme Moritz
Institut Jean Lamour (IJL)
Université de Lorraine (UL)-Institut de Chimie du CNRS (INC)-Centre National de la Recherche Scientifique (CNRS)
National Institute for Fusion Science (NIFS)
Laboratoire de Mécanique, Modélisation et Procédés Propres (M2P2)
Centre National de la Recherche Scientifique (CNRS)-École Centrale de Marseille (ECM)-Aix Marseille Université (AMU)
Institut de Recherche sur la Fusion par confinement Magnétique (IRFM)
Commissariat à l'énergie atomique et aux énergies alternatives (CEA)
Institut de Chimie du CNRS (INC)-Université de Lorraine (UL)-Centre National de la Recherche Scientifique (CNRS)
Aix Marseille Université (AMU)-École Centrale de Marseille (ECM)-Centre National de la Recherche Scientifique (CNRS)
Source :
Nuclear Fusion, Nuclear Fusion, IOP Publishing, 2020, 60 (3), pp.036016. ⟨10.1088/1741-4326/ab6e48⟩, Nuclear Fusion, 2020, 60 (3), pp.036016. ⟨10.1088/1741-4326/ab6e48⟩
Publication Year :
2020
Publisher :
IOP Publishing, 2020.

Abstract

In gyrokinetic simulations of turbulent impurity transport, trace impurity species are often treated as passive species, in the sense that they are not included in Maxwell equations. This is consistent with the assumption that impurities with low enough concentrations are impacted by turbulence generated by electrons and main ions, but do not impact it significantly in return. In this work, we relax this assumption, and investigate the active impacts of impurity on impurity transport as a function of its concentration, in the presence of trapped-particle-driven turbulence. We focus on $W^{40+}$ tungsten, which is relevant for modern tokamaks, and adopt a reduced gyrokinetic bounce-averaged model for trapped particles in a simplified tokamak geometry. The impacts depend on the relationship between equilibrium density gradient and temperature gradient. When these gradients are equal, we observe that tungsten can be treated as a passive species for concentrations below $2\times 10^{-4}$. Above this concentration, the impurity significantly impacts both density and heat transport, essentially quenching them for concentrations above $10^{-3}$. This quenching occurs as electric potential fluctuations become in phase with impurity density fluctuations.

Details

ISSN :
17414326, 00295515, 07413335, and 17426596
Volume :
60
Database :
OpenAIRE
Journal :
Nuclear Fusion
Accession number :
edsair.doi.dedup.....9ae17fb55c2e79001f05aed34f849ada
Full Text :
https://doi.org/10.1088/1741-4326/ab6e48