Interplay of Ion Impact Angle and Plasma Parameters in Predicting ELM-resolved Carbon Deposition and Tungsten Erosion in DIII-D

ORAL

Abstract

Using a near surface mixed material model, a shift of the average ion impact angle (θ) by several degrees towards the surface normal of the DIII-D Small Angle Slot V-shaped W (SAS-VW) divertor is predicted to increase the fractional carbon (C) coverage (σC) of the W divertor by tens of percent. Particularly, reflection coefficients (R) and sputtering yields (Y) of C are highly sensitive to θ at background plasma-thermalized ion impact energies (Ei). Without assessment of σC, our models vastly overpredict gross W erosion (ΓW), especially during an Edge Localized Mode (ELM).

We predict higher σC for plasma discharges with higher C plasma impurity concentrations (%) and lower electron temperature (Te) at the divertor. In an experiment, we injected varying rates of D2 at the outboard midplane and assessed the impact on SAS-VW divertor σC and ΓW. Binary collision code RustBCA computes R and Y of C and D ions on C and W materials. Variation in θ and Ei have a large effect on Y and R to influence σC and ΓW.

With different ion sheath models, we provide novel estimations of C and D θ and consequent σC on a smooth W divertor surface with respect to varying key plasma parameters. WYKO profilometry obtained topographical data of the SAS-VW tiles to correct θ predictions for rough surfaces.

*Work supported by US DOE under DE-SC0023378, DE-FC02-04ER54698, DE-AC05-00OR22725.

Presenters

  • Alec Cacheris

    • University of Tennessee

Authors

  • Alec Cacheris

    • University of Tennessee
  • Tyler W Abrams

    • General Atomics
  • Luca Cappelli

    • General Atomics
    • ORAU
  • Daisuke Shiraki

    • Oak Ridge National Laboratory
  • Jeffery Herfindal

    • Oak Ridge National Laboratory
  • Robert S Wilcox

    • Oak Ridge National Laboratory
  • Davis C Easley

    • Oak Ridge Associated Universities ; Oak Ridge National Laboratory
    • University of Tennessee
  • Shota Abe

    • Princeton Plasma Physics Laboratory
  • David C Donovan

    • University of Tennessee