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Title: Global kinetic ballooning mode simulations in BOUT++

Abstract

We report on simulation results of a 3+1 gyro-Landau-fluid (GLF) model in BOUT++ framework, which contributes to increasing the physics understanding of the edge turbulence. We find that there is no second stability region of kinetic ballooning modes (KBM) in the concentric circular geometry. The first unstable β of KBM decreases below the ideal ballooning mode threshold with increasing $${{\eta}_{i}}$$. In order to study the KBM in the real tokamak equilibrium, we find that the approximation of shifted circular geometry ($$\beta \ll {{\varepsilon}^{2}}$$ ) is not valid for a high β global equilibrium near the second stability region of KBM. Thus we generate a series of real equilibria from a global equilibrium solver CORSICA, including both Shafranov shift and elongation effects, but not including bootstrap current. In these real equilibria, the second stability region of KBM are observed in our global linear simulations. The most unstable mode for different β are the same while the mode number spectrum near the second stability region is wider than the case near the first stability region. Here, the nonlinear simulations show that the energy loss of an ELM keeps increasing with β, because the linear drive of the turbulence remains strong for the case near the second stability region during profile evolution.

Authors:
 [1];  [2]
  1. Peking Univ., Beijing (People's Republic of China); Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States)
  2. Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States)
Publication Date:
Research Org.:
Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)
Sponsoring Org.:
USDOE National Nuclear Security Administration (NNSA)
OSTI Identifier:
1566004
Report Number(s):
LLNL-JRNL-736516
Journal ID: ISSN 0029-5515; 889351; TRN: US2000952
Grant/Contract Number:  
AC52-07NA27344
Resource Type:
Accepted Manuscript
Journal Name:
Nuclear Fusion
Additional Journal Information:
Journal Volume: 57; Journal Issue: 1; Journal ID: ISSN 0029-5515
Publisher:
IOP Science
Country of Publication:
United States
Language:
English
Subject:
70 PLASMA PHYSICS AND FUSION TECHNOLOGY; KBM; ELMs; turbulence

Citation Formats

Ma, C. H., and Xu, X. Q. Global kinetic ballooning mode simulations in BOUT++. United States: N. p., 2016. Web. doi:10.1088/0029-5515/57/1/016002.
Ma, C. H., & Xu, X. Q. Global kinetic ballooning mode simulations in BOUT++. United States. https://doi.org/10.1088/0029-5515/57/1/016002
Ma, C. H., and Xu, X. Q. Wed . "Global kinetic ballooning mode simulations in BOUT++". United States. https://doi.org/10.1088/0029-5515/57/1/016002. https://www.osti.gov/servlets/purl/1566004.
@article{osti_1566004,
title = {Global kinetic ballooning mode simulations in BOUT++},
author = {Ma, C. H. and Xu, X. Q.},
abstractNote = {We report on simulation results of a 3+1 gyro-Landau-fluid (GLF) model in BOUT++ framework, which contributes to increasing the physics understanding of the edge turbulence. We find that there is no second stability region of kinetic ballooning modes (KBM) in the concentric circular geometry. The first unstable β of KBM decreases below the ideal ballooning mode threshold with increasing ${{\eta}_{i}}$. In order to study the KBM in the real tokamak equilibrium, we find that the approximation of shifted circular geometry ($\beta \ll {{\varepsilon}^{2}}$ ) is not valid for a high β global equilibrium near the second stability region of KBM. Thus we generate a series of real equilibria from a global equilibrium solver CORSICA, including both Shafranov shift and elongation effects, but not including bootstrap current. In these real equilibria, the second stability region of KBM are observed in our global linear simulations. The most unstable mode for different β are the same while the mode number spectrum near the second stability region is wider than the case near the first stability region. Here, the nonlinear simulations show that the energy loss of an ELM keeps increasing with β, because the linear drive of the turbulence remains strong for the case near the second stability region during profile evolution.},
doi = {10.1088/0029-5515/57/1/016002},
journal = {Nuclear Fusion},
number = 1,
volume = 57,
place = {United States},
year = {Wed Sep 28 00:00:00 EDT 2016},
month = {Wed Sep 28 00:00:00 EDT 2016}
}

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Works referencing / citing this record:

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Quasi-coherent mode simulation during inter-ELM period in HL-2A
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A Landau-fluid closure for arbitrary frequency response
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Nonlinear saturation of kinetic ballooning modes by zonal fields in toroidal plasmas
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