Plasma profile development with pellet injection on Wendelstein 7-X

ORAL

Abstract

The ability of a magnetically-confined fusion plasma to confine energy and reach ignition conditions depends substantially on the shapes of the plasma profiles. This dependence arises from the influence of spatial gradients in temperature and density on energy and particle loss mechanisms such as turbulent transport. Hence, the ability to develop and sustain plasma scenarios with profiles favorable to good confinement is likely to be essentially to the success of tokamaks and stellarators alike. Wendelstein 7-X (W7-X), for example, is known to achieve substantially better confinement and triple products when its density profiles are peaked. One key way to achieve such profiles is from core fueling via pellet injection. In this talk, we present the results of experiments on W7-X that utilized its new Continuous Pellet Fueling System to obtain plasma profiles amenable to high performance. One especially promising method for scenario development entails initializing a pellet train in a low-power ECRH heated discharge and steadily increasing the heating power during the first few pellets. We also briefly discuss preparations of real-time diagnostics to enable control and sustainment of the profiles in future experiment campaigns.

*This work was supported by the U.S. Department of Energy under Contract No. DE-AC02-09CH11466 and by the European Union via the Euratom Research and Training Programme under Grant Agreement No 101052200 - EUROfusion.

Presenters

  • Kenneth C Hammond

    • Princeton Plasma Physics Laboratory (PPPL), Princeton, NJ, USA
    • Princeton Plasma Physics Laboratory (PPPL)

Authors

  • Kenneth C Hammond

    • Princeton Plasma Physics Laboratory (PPPL), Princeton, NJ, USA
    • Princeton Plasma Physics Laboratory (PPPL)
  • Juergen Baldzuhn

    • Max Planck Institute for Plasma Physics, Greifswald, Germany
    • Max Planck Institute for Plasma Physics
    • Max Planck Institute for Plasma Physics, 17491 Greifswald
  • Larry Robert Baylor

    • Oak Ridge National Laboratory
  • Torsten Bluhm

    • Max Planck Institute for Plasma Physics
  • Sergey Bozhenkov

    • Max Planck Institute for Plasma Physics, Greifswald, Germany
    • Max Planck Institute for Plasma Physics, Greifswald
  • Kai Jakob Brunner

    • Max Planck Institute for Plasma Physics, Greifswald, Germany
    • Max Planck Institute for Plasma Physics, Greifswald
  • Mark de Haas

    • Princeton Plasma Physics Laboratory (PPPL)
    • Princeton Plasma Physics Laboratory
  • Andreas Dinklage

    • Max Planck Institute for Plasma Physics, Greifswald, Germany
    • Max Planck Institute for Plasma Physics
  • Golo Fuchert

    • Max Planck Institute for Plasma Physics, Greifswald, Germany
    • Max Planck Institute for Plasma Physics, Greifswald
  • Jens Knauer

    • Max Planck Institute for Plasma Physics, Greifswald, Germany
    • Max Planck Institute for Plasma Physics, Greifswald
  • Ameer Insaf Mohammed

    • Princeton Plasma Physics Laboratory (PPPL)
  • Novimir A Pablant

    • Princeton Plasma Physics Laboratory (PPPL)
  • Timo Schröder

    • Max Planck Institute for Plasma Physics, Greifswald
  • Gregory L Schmidt

    • Princeton University
  • Torsten Stange

    • Max Planck Institute for Plasma Physics, Greifswald, Germany
    • Max Planck Institute for Plasma Physics, 17491 Greifswald
  • Naoki Tamura

    • Max-Planck Institute for Plasma Physics
  • Sherwin Trieu

    • Princeton Plasma Physics Laboratory (PPPL)
  • Gavin M Weir

    • Max Planck Institute for Plasma Physics