Overview of shattered pellet injection studies at ASDEX Upgrade

ORAL  · Invited

Abstract

Shattered Pellet Injection (SPI) has been selected for ITER as the primary Disruption Mitigation System (DMS). To support the ITER DMS development, a flexible SPI system [1, 2] was installed at ASDEX Upgrade (AUG) to investigate the impact of different fragment size and velocity distributions on the disruption dynamics. In collaboration with the ITER Organization and EUROfusion, we carried out a large experimental campaign with the goal of optimising material assimilation and heat load mitigation. The experiments are also accompanied by modelling with the DREAM, INDEX and JOREK codes, showing good agreement with the experimental observations. With a major update to the radiation measurements of AUG, the investigation of toroidal asymmetries between five toroidal locations is enabled. Of the three shatter head geometries used in AUG plasmas in the 2022 experimental campaign, the 12.5° rectangular shatter head produces relatively large and fast fragments [3], which in turn lead to the highest material assimilation [4] and radiated energy fraction. Simulations suggest that a minor neon doping (<1%) of the otherwise pure deuterium pellets increased the material assimilation via plasmoid drift suppression. We observed the highest impact of the fragment size and velocity distributions on the radiation characteristics in both experiment and simulation for these doped pellets. Otherwise, the radiated energy fraction and (toroidal) radiation asymmetry is a strong function of neon content inside the pellet and only shows a minor dependence on the shatter geometry [5]. The AUG results support the current ITER SPI design [6] with a 15° shatter angle.

[1] M. Dibon et al., Review of Scientific Instruments, 94 (4):043504 (2023).

[2] P. Heinrich et al., accepted manuscript in Fusion Engineering and Design (2024).

[3] T. Peherstorfer, MSc Thesis, TU Wien, 2022.

[4] S. Jachmich et al., 49th EPS Conference on Plasma Physics, Bordeaux, France (2023).

[5] P. Heinrich et al., 49th EPS Conference on Plasma Physics, Bordeaux, France (2023).

[6] M. Lehnen et al., 29th IAEA FEC, TECH/1-1, London, UK (2023).

*The views and opinions expressed herein do not necessarily reflect those of the European Commission or the ITER Organization.

Publication: "Recipes for pellet generation and launching in the ASDEX Upgrade SPI" accepted manuscript in Fusion Engineering and Design;
"Radiated energy fraction of SPI induced disruptions at ASDEX Upgrade" submitted to Nuclear Fusion;
PhD thesis submission and paper on radiation asymmetries planned.

Presenters

  • Paul Heinrich

    • Max Planck Institute for plasma physics
    • Max Planck Institute for Plasma Physics, Garching, Germany; Technical University of Munich (TUM), Garching, Germany

Authors

  • Paul Heinrich

    • Max Planck Institute for plasma physics
    • Max Planck Institute for Plasma Physics, Garching, Germany; Technical University of Munich (TUM), Garching, Germany
  • Gergely Papp

    • Max Planck Institute for Plasma Physics, Garching, Germany
  • Javier Artola

    • ITER Organization, St. Paul-lez-Durance, France
  • Matthias Bernert

    • Max Planck Institute for Plasma Physics
    • Max Planck Institute for Plasma Physics, Garching, Germany
  • Alexander Bock

    • Max Planck Institute for Plasma Physics, Garching, Germany
  • Pierre David

    • Max-Planck-Institut für Plasmaphysik, Boltzmannstr. 2, 85748 Garching, Germany
    • Max Planck Institute for Plasma Physics, Garching, Germany
  • Pascal de Marné

    • Max Planck Institute for Plasma Physics, Garching, Germany
  • Mathias Dibon

    • ITER Organization, St.~Paul-lez-Durance, France
  • Ralph Dux

    • Max Planck Institute for Plasma Physics
    • Max Planck Institute for Plasma Physics, Garching, Germany
  • Thomas Eberl

    • Max Planck Institute for Plasma Physics, Garching, Germany
  • Rainer Fischer

    • Max Planck Institute for Plasma Physics
    • Max Planck Institute for Plasma Physics, Garching, Germany
  • Peter E Halldestam

    • Max Planck Institute for Plasma Physics, Garching, Germany;Technical University of Munich (TUM), Garching, Germany
  • Matthias Hoelzl

    • Max Planck Institute for Plasma Physics, Garching, Germany
  • Joerg Hobirk

    • Max-Planck-Institut für Plasmaphysik, Boltzmannstr. 2, 85748 Garching, Germany
    • Max Planck Institute for Plasma Physics, Garching, Germany
  • Mathias Hoppe

    • Department of Electrical Engineering, KTH Royal Institute of Technology, Stockholm, Sweden
    • KTH Royal Institute of Technology
  • Johannes Illerhaus

    • Max Planck Institute for Plasma Physics, Garching, Germany; Technical University of Munich (TUM), Garching, Germany
  • Stefan Jachmich

    • ITER Organization, Route de Vinon-sur-Verdon - CS 90 046, 13067 St Paul Lez Durance Cedex, France
    • ITER Organization, St. Paul-lez-Durance, France
  • Michael Lehnen

    • ITER Organization, Route de Vinon-sur-Verdon - CS 90 046, 13067 St Paul Lez Durance Cedex, France
    • ITER Organization, St. Paul-lez-Durance, France
  • Tilmann Lunt

    • Max Planck Institute for Plasma Physics, Garching, Germany
  • Akinobu Matsuyama

    • Graduate School of Energy Science, Kyoto University
    • Graduate School of Energy Science, Kyoto University, Uji, Japan
  • Marc Maraschek

    • Max Planck Institute for Plasma Physics, Garching, Germany
  • Mohammad Miah

    • Max Planck Institute for Plasma Physics, Garching, Germany
  • Ansh Patel

    • Max Planck Institute for Plasma Physics, Garching, Germany; Ludwig-Maximilians-University Munich (LMU), Munich, Germany,
  • Tobias Peherstorfer

    • Institute for Applied Physics, Wien, Austria
  • Volker Rohde

    • Max Planck Institute for Plasma Physics, Garching, Germany
  • Nina Schwarz

    • Max Planck Institute for Plasma Physics, Garching, Germany
  • Umar Sheikh

    • EPFL, Swiss Plasma Center (SPC), CH – 1015 Lausanne, Switzerland
    • Swiss Plasma Center (SPC), École Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland,
  • Bernhard Sieglin

    • Max Planck Institute for Plasma Physics, Garching, Germany
  • Jakub Svoboda

    • Institute of Plasma Physics of the CAS, Prague, Czech Republic
  • Weikang Tang

    • Max Planck Institute for Plasma Physics, Garching, Germany
  • Oskar Vallhagen

    • Department of Physics, Chalmers University of Technology, Gothenburg, Sweden