APS Logo

Dependence of the L-H power threshold on the alignment of externally applied non-axisymmetric MPs

ORAL

Abstract

A series of experiments at ASDEX Upgrade (AUG) has 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-mode to H-mode (L-H transition). This is interesting for ITER, since its operation will rely on an MP-field configuration that is expected to solidly suppress edge localised modes (ELMs) while avoiding an increase in the L-H power threshold (PLH).

Experiments at AUG show that PLH increases by up to ≈ 80% when the external n = 2 MP field is aligned to maximise the associated plasma response at the edge. This alignment differs from the equilibrium field pitch and is the same needed in H-mode to suppress ELMs by MPs. The relative perturbation amplitude δBr/B has to surpass a critical value, roughly 2×10−4, to cause an increase in PLH. This is above the value needed to sustain ELM suppression at AUG and is favourable for ITER. State-of-the-art diagnostics probing the edge E × B velocity measure a reversal and flattening during the application of MPs. More heating power is needed to get roughly the same shear in the edge ExB velocity profile as without MPs, but with an ExB velocity profile elevated in the ion diamagnetic direction.

Presenters

  • Matthias Willensdorfer

    Max Planck Institute for Plasma Physics, Max-Planck-Institut für Plasmaphysik

Authors

  • Matthias Willensdorfer

    Max Planck Institute for Plasma Physics, Max-Planck-Institut für Plasmaphysik

  • Ulrike Plank

    Max Planck Insitute for Plasma Physics, Garching, Germany, Max Planck Institute for Plasma Physics

  • Marco Cavedon

    Max Planck Institute for Plasma Physics, Dipartimento di Fisica "G. Occhialini", Università di Milano-Bicocca, Milano, Italy

  • Garrard D Conway

    Max-Planck-Institut für Plasmaphysik, Garching, Germany, Max Planck Institute for Plasma Physics, Garching, Germany, Max Planck Institute for Plasma Physics

  • David Ryan

    CCFE, Culham Science Centre, CCFE, CCFE, Culham Science Centre, Abingdon, Oxon, OX14 3DB, UK, UKAEA

  • Wolfgang Suttrop

    Max-Planck-Institut für Plasmaphysik, 85748 Garching, Germany, Max Planck Institute for Plasma Physics

  • Rico Buchholz

    Fusion@ÖAW, Institut für Theoretische Physik-Computational Physics, TU Graz

  • Mike Dunne

    Max Planck Institute for Plasma Physics

  • Michael Griener

    Max Planck Institute for Plasma Physics

  • Jörg Hobrik

    Max Planck Institute for Plasma Physics

  • Andrew Kirk

    CCFE Culham Science Centre, CCFE, Culham Science Centre, Culham Centre for Fusion Energy, CCFE, CCFE, Culham Science Centre, Abingdon, Oxon, OX14 3DB, UK, MAST

  • Rachael M McDermott

    Max-Planck-Institut für Plasmaphysik, Garching, Germany, Max Planck Institute for Plasma Physics, Garching, Germany, Max Planck Institute for Plasma Physics

  • Thomas Pütterich

    Max Planck Institute for Plasma Physics

  • Giovanni Tardini

    Max Planck Institute for Plasma Physics

  • Rainer Fischer

    Max Planck Institute for Plasma Physics

  • Qingquan Yu

    Max Planck Institute for Plasma Physics, Max-Plank-Institut fur Plasmaphysik

  • Dominik Brida

    Max Planck Insitute for Plasma Physics, Garching, Germany, Max Planck Institute for Plasma Physics

  • Sergei Kasilov

    Fusion@ÖAW, Institut für Theoretische Physik-Computational Physics