Kinetic simulations of electron heat flux in the scrape-off layer

Parallel electron heat flux qe|| on open field lines is studied with the 1D2V kinetic Vlasov-Fokker-Planck (VFP) code KIPP [15–17]. In order to assess the importance of kinetic effects on the scrape-off layer heat transport in a systematic way, a series of self-similar KIPP cases with the stagnation...

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Main Authors: M. Zhao, A.V. Chankin, D.P. Coster
Format: Article
Language:English
Published: Elsevier 2017-08-01
Series:Nuclear Materials and Energy
Online Access:http://www.sciencedirect.com/science/article/pii/S2352179116300576
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spelling doaj-53ca551d2a1e481d8b7100472f92f7232020-11-25T00:31:56ZengElsevierNuclear Materials and Energy2352-17912017-08-0112819824Kinetic simulations of electron heat flux in the scrape-off layerM. Zhao0A.V. Chankin1D.P. Coster2Max-Planck-Institut für Plasmaphysik, Garching bei München, Boltzmannstr. 2, 85748, Germany; Technische Universität München, 80333 München, Germany; Corresponding author.Max-Planck-Institut für Plasmaphysik, Garching bei München, Boltzmannstr. 2, 85748, GermanyMax-Planck-Institut für Plasmaphysik, Garching bei München, Boltzmannstr. 2, 85748, GermanyParallel electron heat flux qe|| on open field lines is studied with the 1D2V kinetic Vlasov-Fokker-Planck (VFP) code KIPP [15–17]. In order to assess the importance of kinetic effects on the scrape-off layer heat transport in a systematic way, a series of self-similar KIPP cases with the stagnation point and one target, logical sheath condition, parabolic ion velocity profiles reaching ion sound speed at the target were run. The variable parameter was upstream electron collisionality v* (collisionality scan cases) and for each collisionality two different numerical schemes of particle source were implemented for comparison. It shows no significant difference between the results with two different schemes of particle source for any scanned collisionality. In high collisionality cases, heat flux converges to Braginskii formula as expected, while in comparatively low collisionality cases transport coefficients deviate far away from classical value due to target cut-off effect implicating that fluid model is not applicable near the target.Enhanced radiation near the target, forcing Te drop by factor 10 for low upstream v* comparable to that expected at the separatrix in the ITER baseline H-mode scenario, was required in KIPP runs. Pairs of such cases with two different ways of radiation power sink, by modeling sink (a) evenly from all velocity space, and (b) only from high energy electrons, were compared. The simulation results show almost no difference between the two cases in the steady-state, despite the presence of a strong heat flux limiting upstream and enhancement downstream.http://www.sciencedirect.com/science/article/pii/S2352179116300576
collection DOAJ
language English
format Article
sources DOAJ
author M. Zhao
A.V. Chankin
D.P. Coster
spellingShingle M. Zhao
A.V. Chankin
D.P. Coster
Kinetic simulations of electron heat flux in the scrape-off layer
Nuclear Materials and Energy
author_facet M. Zhao
A.V. Chankin
D.P. Coster
author_sort M. Zhao
title Kinetic simulations of electron heat flux in the scrape-off layer
title_short Kinetic simulations of electron heat flux in the scrape-off layer
title_full Kinetic simulations of electron heat flux in the scrape-off layer
title_fullStr Kinetic simulations of electron heat flux in the scrape-off layer
title_full_unstemmed Kinetic simulations of electron heat flux in the scrape-off layer
title_sort kinetic simulations of electron heat flux in the scrape-off layer
publisher Elsevier
series Nuclear Materials and Energy
issn 2352-1791
publishDate 2017-08-01
description Parallel electron heat flux qe|| on open field lines is studied with the 1D2V kinetic Vlasov-Fokker-Planck (VFP) code KIPP [15–17]. In order to assess the importance of kinetic effects on the scrape-off layer heat transport in a systematic way, a series of self-similar KIPP cases with the stagnation point and one target, logical sheath condition, parabolic ion velocity profiles reaching ion sound speed at the target were run. The variable parameter was upstream electron collisionality v* (collisionality scan cases) and for each collisionality two different numerical schemes of particle source were implemented for comparison. It shows no significant difference between the results with two different schemes of particle source for any scanned collisionality. In high collisionality cases, heat flux converges to Braginskii formula as expected, while in comparatively low collisionality cases transport coefficients deviate far away from classical value due to target cut-off effect implicating that fluid model is not applicable near the target.Enhanced radiation near the target, forcing Te drop by factor 10 for low upstream v* comparable to that expected at the separatrix in the ITER baseline H-mode scenario, was required in KIPP runs. Pairs of such cases with two different ways of radiation power sink, by modeling sink (a) evenly from all velocity space, and (b) only from high energy electrons, were compared. The simulation results show almost no difference between the two cases in the steady-state, despite the presence of a strong heat flux limiting upstream and enhancement downstream.
url http://www.sciencedirect.com/science/article/pii/S2352179116300576
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AT avchankin kineticsimulationsofelectronheatfluxinthescrapeofflayer
AT dpcoster kineticsimulationsofelectronheatfluxinthescrapeofflayer
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