Electron cyclotron heating scenarios for long pulse and high performance operation at the stellarator Wendelstein 7‑X

ORAL

Abstract

Electron cyclotron resonance heating (ECRH) with an absorbed power of 7.5 MW provided by 10 gyrotrons is the dominating heating system at the stellarator Wendelstein 7-X. As a very versatile technique, ECRH provides plasma start-up, wall conditioning, heating & electron cyclotron current drive (ECCD). Even though a stellarator is operated without a toroidally driven current, the magnetic island divertor requires “fine tuning” of the edge rotational transform by ECCD at least during transitional phases. A not vanishing bootstrap current can be compensated or mimicked during plasma ramp-up to prohibit an unwanted sweep over the divertor. In preparation for long pulse and high performance operation with an actively cooled divertor beyond 2020, the necessary ECRH scenarios were already demonstrated in the operational phase 1.2 with an uncooled divertor & an energy limit of about 80 MJ per pulse. Up to densities of 1020m-3 a standard X2-heating scenario is used which has to be optimized with regard to finite beta & Shafranov-shift. For densities close and beyond the X2-cutoff density, an advanced O2-heating scenario was developed which makes use of holographic reflection tiles to allow 3 beam paths. Central densities of 1.4∙1020 m-3 were achieved at a central temperature of 3 keV.

Presenters

  • Torsten Stange

    Max-Planck-Institute for Plasma Physics, D-17491 Greifswald, Germany, Max Planck Institute for Plasma Physics (IPP), 17491 Greifswald, Germany

Authors

  • Torsten Stange

    Max-Planck-Institute for Plasma Physics, D-17491 Greifswald, Germany, Max Planck Institute for Plasma Physics (IPP), 17491 Greifswald, Germany

  • Heinrich Peter Laqua

    Max Planck Institute for Plasma Physics (IPP), 17491 Greifswald, Germany

  • Sergey Bozhenkov

    Max-Planck-Institute for Plasma Physics, D-17491 Greifswald, Germany, Max-Planck Institut für Plasmaphysik, Max Planck Institute for Plasma Physics (IPP), 17491 Greifswald, Germany, Max-Planck-Institute for Plasma Physics, Greifswald, Germany

  • Kai Jakob Brunner

    Max Planck Institute for Plasma Physics (IPP), 17491 Greifswald, Germany

  • Golo Fuchert

    Max-Planck-Institute for Plasma Physics, D-17491 Greifswald, Germany, Max Planck Institute for Plasma Physics (IPP), 17491 Greifswald, Germany

  • Udo Hoefel

    Max-Planck-Institute for Plasma Physics, D-17491 Greifswald, Germany, Max Planck Institute for Plasma Physics (IPP), 17491 Greifswald, Germany

  • Walter Kasparek

    Institute of Interfacial Process Engineering & Plasma Technology (IGVP), University Stuttgart, Germany

  • Yevgen Kazakov

    ERM-KMS, Laboratory for Plasma Physics, LPP-ERM/KMS, Brussels, Belgium, LPP/ERM-KMS, Brussels

  • Stefan Marsen

    Max Planck Institute for Plasma Physics (IPP), 17491 Greifswald, Germany

  • Dmitry Moseev

    Max-Planck Institut für Plasmaphysik, Max Planck Institute for Plasma Physics (IPP), 17491 Greifswald, Germany

  • Burkhard Plaum

    Institute of Interfacial Process Engineering & Plasma Technology (IGVP), University Stuttgart, Germany

  • Robert C Wolf

    Max-Planck Institut für Plasmaphysik, Max Planck Institute for Plasma Physics (IPP), 17491 Greifswald, Germany, Max-Planck-Institute for Plasma Physics, Max-Planck-Institute for Plasma Physics, Greifswald, Germany

  • Marco Zanini

    Max Planck Institute for Plasma Physics (IPP), 17491 Greifswald, Germany

  • W7-X Team

    Max Planck Institute for Plasma Physics (IPP), 17491 Greifswald, Germany