Bulletin of the American Physical Society
60th Annual Meeting of the APS Division of Plasma Physics
Volume 63, Number 11
Monday–Friday, November 5–9, 2018; Portland, Oregon
Session YP11: Poster Session IX: The crossover between high-energy-density plasmas and ultracold neutral plasmas ; Supplemental; Post-Deadline Abstracts (9:30am-12:30pm)
Friday, November 9, 2018
OCC
Room: Exhibit Hall A1&A
Abstract ID: BAPS.2018.DPP.YP11.2
Abstract: YP11.00002 : Modeling of sources and transport of impurity ions and their interaction with material surfaces in powder-dropping experiments*
Presenter:
M. V. Umansky
(Lawrence Livermore Natl Lab)
Authors:
M. V. Umansky
(Lawrence Livermore Natl Lab)
A. Bortolon
(Princeton Plasma Physics Lab)
D. Curreli
(Univ of Illinois - Urbana)
J. T. Drobny
(Univ of Illinois - Urbana)
R. Maingi
(Princeton Plasma Phys Lab)
T. D. Rognlien
(Lawrence Livermore Natl Lab)
R. D. Smirnov
(Univ of California - San Diego)
In powder-dropping experiments, a stream of dust particles containing boron nitride, pure boron, or other materials is continuously injected into tokamak edge plasma [1]. This is potentially a powerful tool for real-time wall conditioning and edge plasma radiation control. We are undertaking modeling of impurity particles dynamics and their interaction with plasma facing material surfaces in powder-dropping experiments as a sequence of several processes. First, to capture dynamics of injected dust particles, the DUSTT code is used, which allows modeling of physical processes for individual dust grains, including ablation. As dust particles are ablated, they produce a localized impurity ion source; impurity ion transport is modeled with the UEDGE code solving fluid equations for impurity ions and the background plasma. Interaction of plasma and impurity ions with material surfaces is modeled with the F-TRIDYN code which follows evolution of surface morphology. For boron powder injection, of particular interest is the thickness of the steady state layer of boron atoms on the surface, which is the result of dynamic balancing between deposition and sputtering. [1] Bortolon et al., to be submitted to Nucl. Mater. & Energy.
*Prepared for US DOE by LLNL under Contract DE-AC52-07NA27344
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2018.DPP.YP11.2
Follow Us |
Engage
Become an APS Member |
My APS
Renew Membership |
Information for |
About APSThe American Physical Society (APS) is a non-profit membership organization working to advance the knowledge of physics. |
© 2024 American Physical Society
| All rights reserved | Terms of Use
| Contact Us
Headquarters
1 Physics Ellipse, College Park, MD 20740-3844
(301) 209-3200
Editorial Office
100 Motor Pkwy, Suite 110, Hauppauge, NY 11788
(631) 591-4000
Office of Public Affairs
529 14th St NW, Suite 1050, Washington, D.C. 20045-2001
(202) 662-8700