2013/09/11 by F. Ryter, S.K. Rathgeber, S. K. Rathgeber +15 · 145 citations
Chemistry · Engineering · Materials Science · Physics and Astronomy · #ASDEX Upgrade #Atomic physics #Chemistry #Computer science #Engineering #Fusion materials and technologies #Ionosphere and magnetosphere dynamics #Magnetic confinement fusion research #Mode (computer interface) #Nuclear engineering #Nuclear physics #Physics #Plasma #Power (physics) #Quantum mechanics #Tokamak #Transition (genetics) #Upgrade
paper · open access · doi:10.1088/0029-5515/53/11/113003
published in Nuclear Fusion 53(11), 113003 (IOP Publishing)
openalex publication_date 2013/09/11 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/22
An overview of the H-mode threshold power in ASDEX Upgrade which addresses the impact of the tungsten versus graphite wall, the dependences upon plasma current and density, as well as the influence of the plasma ion mass is given.Results on the H-L back transition are also presented.Dedicated L-H transition studies with electron heating at low density, which enable a complete separation of the electron and ion channels, reveal that the ion heat flux is a key parameter in the L-H transition physics mechanism through the main ion pressure gradient which is itself the main contribution to the radial electric field and the induced flow shearing at the edge.The electron channel does not play any role.The 3D magnetic field perturbations used to mitigate the ELMs are found to also influence the L-H transition and to increase the power threshold.This effect is caused by a flattening of the edge pressure gradient in the presence of the 3D fields such that the L-H transitions with and without perturbations occur at the same value of the radial electric field well, but at different heating powers.