Bulletin of the American Physical Society
66th Annual Meeting of the APS Division of Plasma Physics
Monday–Friday, October 7–11, 2024; Atlanta, Georgia
Session UO06: MFE:Research in Support of ITER
2:00 PM–5:12 PM,
Thursday, October 10, 2024
Hyatt Regency
Room: Regency V
Chair: Charles Greenfield, Oak Ridge National Laboratory
Abstract: UO06.00011 : Integrated modeling of solid boron injection for real-time coating of tokamak plasmas-facing components*
4:00 PM–4:12 PM
Presenter:
Florian Effenberg
(Princeton Plasma Physics Laboratory)
Authors:
Florian Effenberg
(Princeton Plasma Physics Laboratory)
Klaus Schmid
(Max Planck Institute for Plasma Physics)
Federico Nespoli
(Princeton Plasma Physics Laboratory)
Alessandro Bortolon
(Princeton Plasma Physics Laboratory)
Yuhe Feng
(Max Planck Institute for Plasma Physics)
Jeremy Lore
(Oak Ridge National Laboratory)
Tyler W Abrams
(General Atomics - San Diego)
Brian A Grierson
(General Atomics)
Rajesh Maingi
(Princeton Plasma Physics Laboratory)
Dmitry L Rudakov
(UCSD)
The Dust Injection Simulator (DIS) was combined with EMC3-EIRENE to model the B powder particle transport and ablation, revealing B flux distribution asymmetries similar to single-point injection modeling [1]. However, these models do not account for erosion and re-deposition, failing to replicate the observed B deposition on the outer divertor target.
Therefore, erosion, migration, and re-deposition of B were modeled by integrating EMC3-EIRENE and DIS with WallDYN3D [2]. This approach, including the mixed-material dynamics at the surface, more realistically replicates real-time wall coating with B powders, achieving B surface concentrations of 0.4 close to those observed in experimental B-C layers.
This integrated modeling approach provides a basis for analyzing real-time coatings and conditioning techniques in advanced tokamak scenarios and predictive studies for solid boron injection in ITER.
[1] F. Effenberg et al 2021 Nucl. Mater. and Energy 26 100900
[2] K. Schmid et al 2020 Nucl. Mater. Energy 25 100821
*This work was supported by the United States Department of Energy (DoE) under Grants No. DE-AC02-09CH11466, DE-FC02-04ER54698, and DE-AC05-00OR22725.
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