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UID:UW-Physics-Event-8641
DTSTART:20240325T180000Z
DURATION:PT1H0M0S
DTSTAMP:20260413T205402Z
LAST-MODIFIED:20240226T152155Z
LOCATION:B343 Sterling
SUMMARY:A CHAPMAN-ENSKOG-LIKE (CEL) CONTINUUM KINETIC CLOSURE APPROACH
  IN NIMROD\, Thesis Defense\, Joseph Jepson\, Physics Graduate Student
DESCRIPTION:Herein\, a numerical method for solving a Chapman-Enskog-l
 ike (CEL) continuum kinetic model for plasmas is formulated\, analyzed
 \, and applied in the plasma fluid code NIMROD. The CEL approach is a 
 $\\delta f$ drift kinetic approach that allows rigorous closure of the
  plasma fluid equations in all collisionality regimes. Importantly\, i
 n this approach\, the zeroth-order in $\\delta$ ($\\delta\\equiv\\rho_
 i/L$\, with $\\rho_i$ the ion gyroradius and $L$ a macroscopic length 
 scale) distribution function is a time-evolving Maxwellian. This diffe
 rence leads to an $O(\\delta)$ kinetic equation that analytically enfo
 rces that the first-order kinetic distortion $f_1$ have no number dens
 ity ($n$)\, flow ($\\mathbf{u}$)\, and temperature ($T$) moments. The 
 fluid variables in this method are allowed to deviate far from an init
 ial equilibrium. The fluid equations are closed by incorporating appro
 priate velocity space moments of the first-order kinetic distortion.<b
 r>\n<br>\nAn axisymmetric poloidal flow damping calculation is perform
 ed to benchmark the implementation. It is first shown that the kinetic
  aspects of the implementation give results for the steady-state poloi
 dal flow that agree both with other codes\, analytics\, and a fixed-ba
 ckground (i.e. $f_0$ a stationary Maxwellian) $\\delta f$ implementati
 on in NIMROD. It is then shown that the flow dynamics in the full CEL 
 approach agree well both with analytics\, and with results from the fi
 xed-background $\\delta f$ implementation.<br>\n<br>\nA von Neumann li
 near stability analysis of the full fluid-kinetic system is also perfo
 rmed to help elucidate methods to make the time advance of the full sy
 stem numerically stable. It is shown that numerical stability is impos
 sible to achieve without explicitly enforcing key tenets of the CEL cl
 osure approach\, in particular\, that the $n$\, $\\mathbf{u}$\, and $T
 $ moments of the kinetic distortion remain small in time. In addition\
 , it is shown that centering the heat flux at the beginning of the tim
 e step and the ion temperature at the end of the time step in the kine
 tic equation allows for a numerically-stable time advance of the coupl
 ed fluid-kinetic system. Furthermore\, these linear stability results 
 are seen to remain applicable when running NIMROD fully nonlinearly.<b
 r>\n<br>\nThe methodology of applying the CEL approach to non-axisymme
 tric problems is also discussed. Future work will include applying thi
 s closure approach to the problem of forced magnetic reconnection in t
 oroidal geometry\, as well as to accurate simulation of neoclassical t
 earing modes (NTMs) in tokamaks.
URL:https://www.physics.wisc.edu/events/?id=8641
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