Impact of ion temperature anisotropy on 2D edge-plasma transport
A model of ion temperature anisotropy for 2D plasma transport in the scrape-off layer (SOL) of tokamaks is described and implemented in the UEDGE fluid transport code. Two ion energy equations are used to describe the evolution of the separate parallel and perpendicular ion temperatures. The tempera...
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doaj-fc0d1d4b0f6f4a1db5112293c0c944952021-03-13T04:24:04ZengElsevierNuclear Materials and Energy2352-17912021-03-0126100881Impact of ion temperature anisotropy on 2D edge-plasma transportM. Zhao0A.E. Jaervinen1I. Joseph2T.D. Rognlien3Correspondence to: Lawrence Livermore National Lab, Livermore, P.O. Box 808 L-440, Livermore CA 94551, USA.; Lawrence Livermore National Laboratory, Livermore, CA 94551, USALawrence Livermore National Laboratory, Livermore, CA 94551, USALawrence Livermore National Laboratory, Livermore, CA 94551, USALawrence Livermore National Laboratory, Livermore, CA 94551, USAA model of ion temperature anisotropy for 2D plasma transport in the scrape-off layer (SOL) of tokamaks is described and implemented in the UEDGE fluid transport code. Two ion energy equations are used to describe the evolution of the separate parallel and perpendicular ion temperatures. The temperature anisotropy generates viscous forces in both parallel and perpendicular directions that modify the parallel force balance equation and add an additional cross-magnetic-field drift velocity. Using the full set of UEDGE plasma and neutral equations (particle continuity, momentum, and energy), simulations are performed for both a 1D poloidal case and a 2D (radial and poloidal) single-null tokamak geometry case to highlight the 2D effects. The results show that ion parallel flows near the magnetic X-point in a comparatively low collisionality regime can be overestimated by the standard isotropic Braginskii model. The 2D ion temperature anisotropy varies substantially near the X-point and also near the divertor target plates, due to ionization sources. Moving radially outwards at the outer midplane, the anisotropy decreases between the core boundary and the magnetic separatrix and then it increases while moving across the SOL to the chamber wall.http://www.sciencedirect.com/science/article/pii/S2352179120301459Scrape-off layerIon temperature anisotropyUEDGE |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
M. Zhao A.E. Jaervinen I. Joseph T.D. Rognlien |
spellingShingle |
M. Zhao A.E. Jaervinen I. Joseph T.D. Rognlien Impact of ion temperature anisotropy on 2D edge-plasma transport Nuclear Materials and Energy Scrape-off layer Ion temperature anisotropy UEDGE |
author_facet |
M. Zhao A.E. Jaervinen I. Joseph T.D. Rognlien |
author_sort |
M. Zhao |
title |
Impact of ion temperature anisotropy on 2D edge-plasma transport |
title_short |
Impact of ion temperature anisotropy on 2D edge-plasma transport |
title_full |
Impact of ion temperature anisotropy on 2D edge-plasma transport |
title_fullStr |
Impact of ion temperature anisotropy on 2D edge-plasma transport |
title_full_unstemmed |
Impact of ion temperature anisotropy on 2D edge-plasma transport |
title_sort |
impact of ion temperature anisotropy on 2d edge-plasma transport |
publisher |
Elsevier |
series |
Nuclear Materials and Energy |
issn |
2352-1791 |
publishDate |
2021-03-01 |
description |
A model of ion temperature anisotropy for 2D plasma transport in the scrape-off layer (SOL) of tokamaks is described and implemented in the UEDGE fluid transport code. Two ion energy equations are used to describe the evolution of the separate parallel and perpendicular ion temperatures. The temperature anisotropy generates viscous forces in both parallel and perpendicular directions that modify the parallel force balance equation and add an additional cross-magnetic-field drift velocity. Using the full set of UEDGE plasma and neutral equations (particle continuity, momentum, and energy), simulations are performed for both a 1D poloidal case and a 2D (radial and poloidal) single-null tokamak geometry case to highlight the 2D effects. The results show that ion parallel flows near the magnetic X-point in a comparatively low collisionality regime can be overestimated by the standard isotropic Braginskii model. The 2D ion temperature anisotropy varies substantially near the X-point and also near the divertor target plates, due to ionization sources. Moving radially outwards at the outer midplane, the anisotropy decreases between the core boundary and the magnetic separatrix and then it increases while moving across the SOL to the chamber wall. |
topic |
Scrape-off layer Ion temperature anisotropy UEDGE |
url |
http://www.sciencedirect.com/science/article/pii/S2352179120301459 |
work_keys_str_mv |
AT mzhao impactofiontemperatureanisotropyon2dedgeplasmatransport AT aejaervinen impactofiontemperatureanisotropyon2dedgeplasmatransport AT ijoseph impactofiontemperatureanisotropyon2dedgeplasmatransport AT tdrognlien impactofiontemperatureanisotropyon2dedgeplasmatransport |
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1724222113387118592 |