2023
DOI: 10.1063/5.0134966
|View full text |Cite
|
Sign up to set email alerts
|

An alternative justification for the stationary assumption made by many reduced models for nonlocal electron heat flow in plasmas

Abstract: Nonlocal models are widely used for approximating kinetic effects on electron heat flow in fusion-relevant plasmas. Almost universally, such models have no explicit time dependence and are designed to make heat flow predictions based directly on instantaneous profiles of macroscopic plasma parameters. While this is usually justified by the claim that transient effects fade before temperature profiles evolve appreciably, a more rigorous justification of the stationarity assumption in terms of kinetic theory is … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
1
0

Year Published

2024
2024
2024
2024

Publication Types

Select...
1

Relationship

0
1

Authors

Journals

citations
Cited by 1 publication
(1 citation statement)
references
References 28 publications
0
1
0
Order By: Relevance
“…The deviation from Maxwellian δf α and therefore transport fluxes are established on much faster, kinetic timescales than the characteristic timescales on which hydrodynamic quantities vary. The RKM then solves for δf α from only the instantaneous hydrodynamic profiles [34] by relaxing the kinetic equation (4) to the stationary state where ∂ t δf α = 0. This relaxed solution corresponds to the physical state for δf α for the input hydrodynamic profiles, even though the transient states that the DF evolves through in the RKM on the way to this relaxed state are not necessarily physical.…”
Section: Reduced Kinetic Methodsmentioning
confidence: 99%
“…The deviation from Maxwellian δf α and therefore transport fluxes are established on much faster, kinetic timescales than the characteristic timescales on which hydrodynamic quantities vary. The RKM then solves for δf α from only the instantaneous hydrodynamic profiles [34] by relaxing the kinetic equation (4) to the stationary state where ∂ t δf α = 0. This relaxed solution corresponds to the physical state for δf α for the input hydrodynamic profiles, even though the transient states that the DF evolves through in the RKM on the way to this relaxed state are not necessarily physical.…”
Section: Reduced Kinetic Methodsmentioning
confidence: 99%