Effect of plasma beta on the nonlinear evolution of m/n = 2/1 double tearing mode in high Lundquist number regime

The existing results indicate that in the large Lundquist number regime, plasmoids play an important role in the growth and saturation of the double tearing mode (DTM). In this paper, the effect of plasma beta on the nonlinear evolution of the m / n = 2/1 DTM in large Lundquist number regime is nume...

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Main Authors: Dingzong Zhang, Zhaoqing Wu, Jun Ma, Wenfeng Guo, Yanqing Huang, Hongbo Liu
Format: Article
Language:English
Published: IOP Publishing 2025-01-01
Series:Nuclear Fusion
Subjects:
Online Access:https://doi.org/10.1088/1741-4326/ada628
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author Dingzong Zhang
Zhaoqing Wu
Jun Ma
Wenfeng Guo
Yanqing Huang
Hongbo Liu
author_facet Dingzong Zhang
Zhaoqing Wu
Jun Ma
Wenfeng Guo
Yanqing Huang
Hongbo Liu
author_sort Dingzong Zhang
collection DOAJ
description The existing results indicate that in the large Lundquist number regime, plasmoids play an important role in the growth and saturation of the double tearing mode (DTM). In this paper, the effect of plasma beta on the nonlinear evolution of the m / n = 2/1 DTM in large Lundquist number regime is numerically investigated in a cylinder geometry. The results demonstrate that the impact of plasma beta on plasmoid dynamics varies significantly with the separation distance between rational surfaces. In the small separation regime ( $\Delta r = 0.1$ ), no plasmoids are observed, regardless of plasma beta and resistivity. However, when the separation is relatively large ( $\Delta r = 0.2$ or $\Delta r = 0.3$ ), plasmoids exhibit highly complex behavior under different plasma beta and resistivity conditions. For the medium separation $\Delta r = 0.2$ , the resistivity threshold for the emergence of plasmoids is approximately $2.5 \times {10^{ - 6}}$ and is not affected by plasma beta. Conversely, when the separation increases to $\Delta r = 0.3$ , the resistivity threshold is significantly influenced by plasma beta. Under certain conditions, this threshold can reach as high as $1.0 \times {10^{ - 5}}$ , which is much higher than the typical value of around ${10^{ - 7}}$ . Furthermore, a preliminary case study shows that the tokamak plasma rotation shear has a significant impact on plasmoid dynamic.
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institution Kabale University
issn 0029-5515
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publishDate 2025-01-01
publisher IOP Publishing
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series Nuclear Fusion
spelling doaj-art-3d8b72dd7e384756b9d9a577206291972025-01-20T10:19:41ZengIOP PublishingNuclear Fusion0029-55152025-01-0165202604310.1088/1741-4326/ada628Effect of plasma beta on the nonlinear evolution of m/n = 2/1 double tearing mode in high Lundquist number regimeDingzong Zhang0Zhaoqing Wu1Jun Ma2https://orcid.org/0000-0002-8114-7340Wenfeng Guo3https://orcid.org/0000-0002-0799-9342Yanqing Huang4Hongbo Liu5https://orcid.org/0000-0001-7798-2661College of Physics and Electronic Engineering, Hengyang Normal University , Hengyang 421008, China; Institute of Plasma Physics, Chinese Academy of Sciences , Hefei 230031, ChinaCollege of Physics and Electronic Engineering, Hengyang Normal University , Hengyang 421008, China; Institute of Plasma Physics, Chinese Academy of Sciences , Hefei 230031, ChinaInstitute of Plasma Physics, Chinese Academy of Sciences , Hefei 230031, ChinaInstitute of Plasma Physics, Chinese Academy of Sciences , Hefei 230031, ChinaCollege of Physics and Electronic Engineering, Hengyang Normal University , Hengyang 421008, ChinaCollege of Physics and Electronic Engineering, Hengyang Normal University , Hengyang 421008, ChinaThe existing results indicate that in the large Lundquist number regime, plasmoids play an important role in the growth and saturation of the double tearing mode (DTM). In this paper, the effect of plasma beta on the nonlinear evolution of the m / n = 2/1 DTM in large Lundquist number regime is numerically investigated in a cylinder geometry. The results demonstrate that the impact of plasma beta on plasmoid dynamics varies significantly with the separation distance between rational surfaces. In the small separation regime ( $\Delta r = 0.1$ ), no plasmoids are observed, regardless of plasma beta and resistivity. However, when the separation is relatively large ( $\Delta r = 0.2$ or $\Delta r = 0.3$ ), plasmoids exhibit highly complex behavior under different plasma beta and resistivity conditions. For the medium separation $\Delta r = 0.2$ , the resistivity threshold for the emergence of plasmoids is approximately $2.5 \times {10^{ - 6}}$ and is not affected by plasma beta. Conversely, when the separation increases to $\Delta r = 0.3$ , the resistivity threshold is significantly influenced by plasma beta. Under certain conditions, this threshold can reach as high as $1.0 \times {10^{ - 5}}$ , which is much higher than the typical value of around ${10^{ - 7}}$ . Furthermore, a preliminary case study shows that the tokamak plasma rotation shear has a significant impact on plasmoid dynamic.https://doi.org/10.1088/1741-4326/ada628plasmoidDTMhigh Lundquist number regime
spellingShingle Dingzong Zhang
Zhaoqing Wu
Jun Ma
Wenfeng Guo
Yanqing Huang
Hongbo Liu
Effect of plasma beta on the nonlinear evolution of m/n = 2/1 double tearing mode in high Lundquist number regime
Nuclear Fusion
plasmoid
DTM
high Lundquist number regime
title Effect of plasma beta on the nonlinear evolution of m/n = 2/1 double tearing mode in high Lundquist number regime
title_full Effect of plasma beta on the nonlinear evolution of m/n = 2/1 double tearing mode in high Lundquist number regime
title_fullStr Effect of plasma beta on the nonlinear evolution of m/n = 2/1 double tearing mode in high Lundquist number regime
title_full_unstemmed Effect of plasma beta on the nonlinear evolution of m/n = 2/1 double tearing mode in high Lundquist number regime
title_short Effect of plasma beta on the nonlinear evolution of m/n = 2/1 double tearing mode in high Lundquist number regime
title_sort effect of plasma beta on the nonlinear evolution of m n 2 1 double tearing mode in high lundquist number regime
topic plasmoid
DTM
high Lundquist number regime
url https://doi.org/10.1088/1741-4326/ada628
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