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2–5 Oct 2023
Caffè Pedrocchi
Europe/Rome timezone

Simulation of neoclassical heavy impurity transport in AUG with applied 3D magnetic fields with the nonlinear MHD code JOREK

O.9
3 Oct 2023, 14:40
25m
Sala Rossini (Caffè Pedrocchi)

Sala Rossini

Caffè Pedrocchi

Piazzetta Cappellato Pedrocchi, 17, Padova GPS: 45.4076321 N, 11.8772911 E

Speaker

Sven Korving (Eindhoven University of Technology)

Description

An accumulation of heavy impurities in the tokamak core is detrimental for its performance and can lead to disruption of the plasma. In smaller to medium size tokamaks the effective neoclassical transport in the pedestal is radially inwards [3]. In larger tokamaks---e.g. ITER--- where the temperature gradient is higher, the neoclassical transport is predicted to be outwards. The models are derived for axisymmetric quasi-steady-state plasmas. Applied 3D magnetic fields---i.e. Resonant Magnetic Perturbation (RMPs)--- can be used to suppress Edge Localized Modes (ELMs). Experimentally it has been observed in AUG, the use of RMPs enhances the outflow of heavy impurities in the pedestal. There is no model which can predict neoclassical heavy impurity transport in these ergodized 3D magnetic fields self-consistently.

In this contribution we present our tungsten transport simulation for an ASDEX Upgrade plasma with applied RMPs. Our model utilizes a full-orbit pusher, ionization, recombination, effective line and continuum radiation and neoclassical collisions with the background plasma. The effective collisional radiative rates are from the OpenADAS database, the neoclassical collision operator uses the framework of Homma [4].
We have compared the average radial transport between axisymmetric and 3D RMP scenarios in the pedestal region. RMPs clearly cause enhanced transport. However, it is not just enhanced axisymmetric diffusion, but perpendicular transport has a equivalently strong component in the n=2 toroidal harmonic. Additionally to the enhanced transport we found that part of the W gets trapped in 3D potential wells in the Scrape-off layer as shown in Fig.1. With the newly developed neutral model [5], we can combine the interaction in the divertor with the 3D RMPs to model the tungsten transport from the divertor towards the core of the plasma.

Author

Sven Korving (Eindhoven University of Technology)

Co-authors

Dr Alberto Loarte (ITER Organization) Guido Huijsmans (CEA, TU Eindhoven) Matthias Hoelzl (Max Planck Institute for Plasma Physics) The ASDEX Upgrade team The JOREK Team Ms Verena Mitterauer (Max Planck Institute for Plasma Physics)

Presentation materials