Numerical simulation of the multiple core localized low shear toroidal Alfvenic eigenmodes

In modern tokamak experiments, scenarios with weak central magnetic shear has been proposed. It is necessary to study the Alfvenic mode activities in such scenarios. Theoretical researches have predicted the multiplicity of core-localized toroidally induced Alfvenic eigenmodes for ε/s > 1, where...

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Main Authors: Wenjia Wang, Deng Zhou, Youjun Hu, Yue Ming
Format: Article
Language:English
Published: AIP Publishing LLC 2018-03-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/1.5010407
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spelling doaj-6da87416e21b4a599fd084d1d68ef4432020-11-25T02:25:40ZengAIP Publishing LLCAIP Advances2158-32262018-03-0183035104035104-1010.1063/1.5010407090802ADVNumerical simulation of the multiple core localized low shear toroidal Alfvenic eigenmodesWenjia Wang0Deng Zhou1Youjun Hu2Yue Ming3Institute of Plasma Physics, Chinese Academy of Sciences, Hefei 230031, P. R. ChinaInstitute of Plasma Physics, Chinese Academy of Sciences, Hefei 230031, P. R. ChinaInstitute of Plasma Physics, Chinese Academy of Sciences, Hefei 230031, P. R. ChinaInstitute of Plasma Physics, Chinese Academy of Sciences, Hefei 230031, P. R. ChinaIn modern tokamak experiments, scenarios with weak central magnetic shear has been proposed. It is necessary to study the Alfvenic mode activities in such scenarios. Theoretical researches have predicted the multiplicity of core-localized toroidally induced Alfvenic eigenmodes for ε/s > 1, where ε is the inverse aspect ratio and s is magnetic shear. We numerically investigate the existence of multiplicity of core-localized TAEs and mode characteristics using NOVA code in the present work. We firstly verify the existence of the multiplicity for zero beta plasma and the even mode at the forbidden zone. For finite beta plasma, the mode parities become more distinguishable, and the frequencies of odd modes are close to the upper tip of the continuum, while the frequencies of even modes are close to the lower tip of the continuum. Their frequencies are well separated by the forbidden zone. With the increasing value of ε/s, more modes with multiple radial nodes will appear, which is in agreement with theoretical prediction. The discrepancy between theoretical prediction and our numerical simulation is also discussed in the main text.http://dx.doi.org/10.1063/1.5010407
collection DOAJ
language English
format Article
sources DOAJ
author Wenjia Wang
Deng Zhou
Youjun Hu
Yue Ming
spellingShingle Wenjia Wang
Deng Zhou
Youjun Hu
Yue Ming
Numerical simulation of the multiple core localized low shear toroidal Alfvenic eigenmodes
AIP Advances
author_facet Wenjia Wang
Deng Zhou
Youjun Hu
Yue Ming
author_sort Wenjia Wang
title Numerical simulation of the multiple core localized low shear toroidal Alfvenic eigenmodes
title_short Numerical simulation of the multiple core localized low shear toroidal Alfvenic eigenmodes
title_full Numerical simulation of the multiple core localized low shear toroidal Alfvenic eigenmodes
title_fullStr Numerical simulation of the multiple core localized low shear toroidal Alfvenic eigenmodes
title_full_unstemmed Numerical simulation of the multiple core localized low shear toroidal Alfvenic eigenmodes
title_sort numerical simulation of the multiple core localized low shear toroidal alfvenic eigenmodes
publisher AIP Publishing LLC
series AIP Advances
issn 2158-3226
publishDate 2018-03-01
description In modern tokamak experiments, scenarios with weak central magnetic shear has been proposed. It is necessary to study the Alfvenic mode activities in such scenarios. Theoretical researches have predicted the multiplicity of core-localized toroidally induced Alfvenic eigenmodes for ε/s > 1, where ε is the inverse aspect ratio and s is magnetic shear. We numerically investigate the existence of multiplicity of core-localized TAEs and mode characteristics using NOVA code in the present work. We firstly verify the existence of the multiplicity for zero beta plasma and the even mode at the forbidden zone. For finite beta plasma, the mode parities become more distinguishable, and the frequencies of odd modes are close to the upper tip of the continuum, while the frequencies of even modes are close to the lower tip of the continuum. Their frequencies are well separated by the forbidden zone. With the increasing value of ε/s, more modes with multiple radial nodes will appear, which is in agreement with theoretical prediction. The discrepancy between theoretical prediction and our numerical simulation is also discussed in the main text.
url http://dx.doi.org/10.1063/1.5010407
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AT dengzhou numericalsimulationofthemultiplecorelocalizedlowsheartoroidalalfveniceigenmodes
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AT yueming numericalsimulationofthemultiplecorelocalizedlowsheartoroidalalfveniceigenmodes
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