Global gyrokinetic simulations of kinetic ballooning mode in NSTX-U plasmas

Abstract Understanding the kinetic ballooning mode (KBM) is crucial for optimizing plasma performance in high- β spherical tokamaks. Global gyrokinetic simulations of KBMs in a projected NSTX-U shot are presented using realistic magnetic geometry and plasma profiles. Linear simulations across varying plasma β values show that the KBM is unstable in NSTX-U at significantly higher plasma β than conventional tokamaks due to the plasma shaping effects. Isotope effects on KBM are more pronounced at higher plasma β but remain relatively weak near the KBM stability threshold. Without flow shear, KBMs are unstable in both the core and pedestal regions. In the core, the investigated toroidal mode numbers in the range <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mi>n</mml:mi> <mml:mo>=</mml:mo> <mml:mo stretchy="false">[</mml:mo> <mml:mn>15</mml:mn> <mml:mo>,</mml:mo> <mml:mo>…</mml:mo> <mml:mo>,</mml:mo> <mml:mn>31</mml:mn> <mml:mo stretchy="false">]</mml:mo> </mml:mrow> </mml:math> are observed to be unstable. In the pedestal, on the other hand, the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mi>n</mml:mi> <mml:mstyle scriptlevel="0"/> <mml:mo>=</mml:mo> <mml:mn>15</mml:mn> </mml:mrow> </mml:math> mode is the most unstable mode due to local β values lower than those in the core. Parameter scans of plasma profile gradients and plasma β demonstrate that the linear KBM in the core exhibits a high sensitivity to β , whereas KBM in the pedestal shows a lower sensitivity. A reduction of β by approximately 15% from the projected value stabilizes KBMs in the core. Nonlinear simulations reveal that self-generated zonal flows play a crucial role in regulating KBM-driven turbulence, reducing the size of turbulent eddies, shortening the radial correlation length by nearly threefold, and decreasing turbulent transport by approximately 35%. These findings provide valuable insights into KBM stability and turbulent transport, offering guidance for optimizing operational scenarios in future experiments.

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Publication Details

Journal
Nuclear Fusion
Published
2025-09-17
DOI
https://doi.org/10.1088/1741-4326/ae0801
Citations
3
Primary Topic
Magnetic confinement fusion research
Type
article
Field-Weighted Citation Impact
5.61

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article

Global gyrokinetic simulations of kinetic ballooning mode in NSTX-U plasmas

Animesh Kuley, Tajinder Singh, T. Rafiq, Eugenio Schuster et al.
3 citations
Nuclear Fusion
Magnetic confinement fusion research
5.61
article

Global gyrokinetic simulations of kinetic ballooning mode in NSTX-U plasmas

Animesh Kuley, Tajinder Singh, T. Rafiq, Eugenio Schuster, Zhihong Lin
article en
3 citations

Abstract

Abstract Understanding the kinetic ballooning mode (KBM) is crucial for optimizing plasma performance in high- β spherical tokamaks. Global gyrokinetic simulations of KBMs in a projected NSTX-U shot are presented using realistic magnetic geometry and plasma profiles. Linear simulations across varying plasma β values show that the KBM is unstable in NSTX-U at significantly higher plasma β than conventional tokamaks due to the plasma shaping effects. Isotope effects on KBM are more pronounced at higher plasma β but remain relatively weak near the KBM stability threshold. Without flow shear, KBMs are unstable in both the core and pedestal regions. In the core, the investigated toroidal mode numbers in the range <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mi>n</mml:mi> <mml:mo>=</mml:mo> <mml:mo stretchy="false">[</mml:mo> <mml:mn>15</mml:mn> <mml:mo>,</mml:mo> <mml:mo>…</mml:mo> <mml:mo>,</mml:mo> <mml:mn>31</mml:mn> <mml:mo stretchy="false">]</mml:mo> </mml:mrow> </mml:math> are observed to be unstable. In the pedestal, on the other hand, the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mi>n</mml:mi> <mml:mstyle scriptlevel="0"/> <mml:mo>=</mml:mo> <mml:mn>15</mml:mn> </mml:mrow> </mml:math> mode is the most unstable mode due to local β values lower than those in the core. Parameter scans of plasma profile gradients and plasma β demonstrate that the linear KBM in the core exhibits a high sensitivity to β , whereas KBM in the pedestal shows a lower sensitivity. A reduction of β by approximately 15% from the projected value stabilizes KBMs in the core. Nonlinear simulations reveal that self-generated zonal flows play a crucial role in regulating KBM-driven turbulence, reducing the size of turbulent eddies, shortening the radial correlation length by nearly threefold, and decreasing turbulent transport by approximately 35%. These findings provide valuable insights into KBM stability and turbulent transport, offering guidance for optimizing operational scenarios in future experiments.

Nuclear FusionVol. 65(10)
Lehigh University (US), University of California, Irvine (US), Indian Institute of Science Bangalore (IN)
U.S. Department of Energy, National Energy Research Scientific Computing Center, Department of Science and Technology, Ministry of Science and Technology, India, Office of Science, Science and Engineering Research Board, Board of Research in Nuclear Sciences
Openalex Percentile: Top 5%
Magnetic confinement fusion research
5.61
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