Nuclear Materials and Energy (Dec 2024)

Wall conditions in WEST during operations with a new ITER grade, actively cooled divertor

  • A. Gallo,
  • Ph. Moreau,
  • D. Douai,
  • T. Alarcon,
  • K. Afonin,
  • V. Anzallo,
  • R. Bisson,
  • J. Bucalossi,
  • E. Caprin,
  • Y. Corre,
  • M. De Combarieu,
  • C. Desgranges,
  • P. Devynck,
  • A. Ekedahl,
  • N. Fedorczak,
  • J. Gaspar,
  • A. Grosjean,
  • C. Guillemaut,
  • R. Guirlet,
  • J.P. Gunn,
  • J. Hillairet,
  • T. Loarer,
  • P. Maget,
  • P. Manas,
  • J. Morales,
  • F.P. Pellissier,
  • E. Tsitrone,
  • K. Krieger,
  • A. Hakola,
  • A. Widdowson

Journal volume & issue
Vol. 41
p. 101741

Abstract

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Future fusion reactors like ITER and DEMO will have all-tungsten (W) walls and long pulses. These features will make wall conditioning more difficult than in most of the existing devices. The W Environment Steady-state Tokamak (WEST) is one of the few long pulse (364 s) fusion devices with actively cooled W plasma-facing components in the world. WEST is a unique test bed to study impurity migration and plasma density control via reactor relevant wall conditioning techniques. The phase II of WEST operations began in 2022, after the installation of a new lower divertor, now entirely equipped with actively cooled, ITER grade, W monoblocks. After pump down, we baked WEST between 90 °C and 170 °C for ∼2 weeks. After 82.5 h at 90 °C and 33 h at 170 °C, vacuum conditions were stable with a vessel pressure of 6x10-5 Pa and mass spectra dominated by H2 molecules. While at 170 °C, we performed ∼40 h of D2 glow discharge cleaning (GDC) and ∼5 h of glow discharge boronization (GDB), using a 15 %-85 % B2D6-He mix and a total boron mass of ∼12 g. This was the very first GDB at such high temperature for WEST. The whole wall conditioning sequence led to a ∼10 times reduction of the H2O signal as well as to a ∼3 times reduction of the O2 signal, according to mass spectra. Once back to 70 °C, the vessel pressure was 5.5x10-6 Pa and plasma restart was seamless with ∼30 s cumulated over the very first 5 pulses and an Ohmic radiated power fraction Frad = 0.6, showing successful conditioning of the new ITER grade divertor. The effect of the first, ‘hot’ GDB faded with a characteristic cumulative injected energy of 2.45 GJ and saturation towards Frad ∼0.8. After 1.4 h and 7.5 GJ of cumulative plasma time and injected energy, we carried out a second GDB, this time at 70 °C. This ‘cold’ GDB initially led to a much lower Ohmic Frad = 0.3–0.4 but the effect lasted ∼7 times less, with a characteristic cumulative injected energy of 0.37 GJ. At the end of the campaign, we cumulated ∼3h and ∼30 GJ through repetitive, minute long pulses without any boronization. Throughout this 4-weeks-long experiment, Frad in the 4 MW heating phase evolved only marginally (from 0.5 to 0.55). This increase is mostly due to the build-up of re/co-deposited layers on both lower divertor targets.