Dependence of the L–H power threshold on the alignment of external non-axisymmetric magnetic perturbations in ASDEX Upgrade

Author:

Willensdorfer M.1ORCID,Plank U.1,Brida D.1ORCID,Cavedon M.2ORCID,Conway G. D.1,Ryan D. A.3,Suttrop W.1ORCID,Buchholz R.4,Dunne M.1,Fischer R.1,Griener M.1ORCID,Hobirk J.1ORCID,Kasilov S.4,Kirk A.3ORCID,McDermott R. M.1ORCID,Pütterich T.1,Tardini G.1,Yu Q.1ORCID, ,

Affiliation:

1. Max Planck Institute for Plasma Physics, 85748 Garching, Germany

2. Dipartimento di Fisica “G. Occhialini,” Universit di Milano-Bicocca, 20126 Milano, Italy

3. CCFE, Culham Science Centre, Abingdon OX14 3DB, United Kingdom

4. Fusion@ÖAW, Institut für Theoretische Physik-Computational Physics, TU Graz, 8010 Graz, Austria

Abstract

Experiments at ASDEX Upgrade have been conducted to study the impact of the alignment of external magnetic perturbations (MPs) with n = 2 toroidal mode symmetry on the power threshold of the transition from L- to H-mode ([Formula: see text]). This is interesting for ITER, since its operation will rely on an MP field configuration that securely suppresses edge localized modes (ELMs) while avoiding an increase in the L–H power threshold. [Formula: see text] can increase up to [Formula: see text] when the external MP field is aligned to maximize the associated plasma response at the edge. This alignment deviates from the equilibrium field pitch and is similar to the one that is required to suppress ELMs by MPs in H-mode. The relative radial magnetic field perturbation [Formula: see text] has to exceed a critical value, roughly [Formula: see text] (at the q = 5 surface), to cause an increase in [Formula: see text]. This value is above the one that is required to sustain ELM suppression at ASDEX Upgrade. Combining plasma response calculations with a critical value of [Formula: see text] captures well the measured dependencies of [Formula: see text] on the alignment of the applied MP field. The increase in [Formula: see text] is accompanied by a change in the [Formula: see text] flow velocity ([Formula: see text]) profile. The application of MPs in L-mode flattens and reverses the edge [Formula: see text] profile when at least [Formula: see text] is applied. This is the same value above which [Formula: see text] increases. More heating power is needed to roughly achieve the same shear in the [Formula: see text] profile at the transition to H-mode as without MPs but with an [Formula: see text] profile that is shifted into the ion diamagnetic direction.

Funder

Euratom Research and Training Programme

Publisher

AIP Publishing

Subject

Condensed Matter Physics

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