Electric field and turbulence in global Braginskii simulations across the ASDEX Upgrade edge and scrape-off layer. (12th February 2021)

• Record Type: Journal Article
• Authors: Zholobenko, W; Body, T; Manz, P; Stegmeir, A; Zhu, B; Griener, M; Conway, G D; Coster, D; Jenko, F
• Other Names: collab.
• Is Part Of: Plasma physics and controlled fusion. Volume 63:Number 3(2021)
• Publication Date: 2021-02-12
• Subjects: turbulence simulations -- electric field -- zonal flows -- Braginskii -- ASDEX Upgrade -- edge and scrape-off layer; Plasma (Ionized gases) -- Periodicals; Controlled fusion -- Periodicals; 530.44
• DOI: 10.1088/1361-6587/abd97e
• Languages: English
• ISSNs: 0741-3335

Abstract

Abstract: Turbulence simulations in diverted geometry across the edge and scrape-off layer (SOL) of ASDEX Upgrade are performed with the GRILLIX code (Stegmeir et al 2019 Phys. Plasmas 26 052517). The underlying global (full- f ) drift-reduced Braginskii model allows to concurrently study the self-consistent dynamics of the turbulence and the background as well as the evolution of toroidal and zonal flows. Different contributions to the radial electric field are identified. The dominant contribution on closed flux surfaces comes from the ion pressure gradient, due to the diamagnetic drift in the curved magnetic field. Large deviations can be induced, in particular, by the polarization particle flux, leading to zonal flows. The latter are driven by small-scale eddies, but do not exhibit much impact on the overall transport which is driven by ballooning modes at larger scales. Ion viscosity is found to be important in damping poloidal rotation through adjusting of the parallel velocity profile, but not via direct vorticity damping. The zonal flow drive peaks at the separatrix, where a strong shear layer forms due to the sheath-induced counter-propagating SOL flow, allowing for the formation of a transport barrier. The temperature profile across the separatrix is determined by the competition between cross-field transport and outflow in the SOL, the latter being largely controlled by the parallel heat conductivity.