Bulletin of the American Physical Society
63rd Annual Meeting of the APS Division of Plasma Physics
Volume 66, Number 13
Monday–Friday, November 8–12, 2021; Pittsburgh, PA
Session GP11: Poster Session III:
MFE - MHD and Stability; C-2W and Other FRC
9:30 AM - 12:30 PM
Tuesday, November 9, 2021
Room: Hall A
Abstract: GP11.00027 : Benchmarking NIMROD Continuum Kinetic Formulations through the Steady-State Poloidal Flow*
Presenter:
Joseph R Jepson
(University of Wisconsin - Madison)
Authors:
Joseph R Jepson
(University of Wisconsin - Madison)
Chris C Hegna
(University of Wisconsin - Madison)
Eric D Held
(Utah State Univ)
Joseph A Spencer
(Utah State University)
Brendan C Lyons
(General Atomics - San Diego)
In this work, continuum kinetic formulations are employed as a mechanism to include closure physics in an extended magnetohydrodynamics (MHD) model. Two continuum kinetic approaches have been implemented in the plasma fluid code NIMROD including a Chapman-Enskog-like (CEL) [1] formulation, and a more conventional $\delta f$ approach. Herein, predictions for steady-state values of poloidal flow profiles in tokamak geometry are provided, using both the $\delta f$ formulation, and two different solution methods for CEL. These results are benchmarked against analytic theory as well as results from the drift kinetic code DK4D [2]. The kinetic formulations employed here show agreement with both the analytic theory and DK4D results, and offer a novel velocity space representation involving higher-order finite elements in pitch angle. Preliminary results involving the full fluid-kinetic coupling of the CEL method are also presented. [1] J. J. Ramos, “Fluid and drift-kinetic description of a magnetized plasma with low collisionality and slow dynamics orderings. i. electron theory,” Physics of Plasmas \textbf{17}, 082502 (2010). [2] B. C. Lyons, “Steady-state benchmarks of DK4D: A time-dependent, axisymmetric drift-kinetic equation solver,” Physics of Plasmas \textbf{22}, 056103 (2015).
*This research is supported by the U. S. Department of Energy (DOE) Office of Science, Office of Fusion Energy Science under grant numbers DE-FG02-86ER53218, DE-SC0018146, and DE-SC0018109, and DE-AC02-05CH11231. This research used resources of the National Energy Research Scientific Computing Center (NERSC), a U.S. Department of Energy Office of Science User Facility located at Lawrence Berkeley National Laboratory.
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