L–H power threshold for neutral beam heated plasmas with deuterium, hydrogen, helium and mixed ion species in TCV

Abstract A systematic study of the power threshold for L–H transition has been conducted in TCV. Only results from NB heated plasmas are reported. The dependencies of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi mathvariant="italic">P</mml:mi> </mml:mrow> <mml:mrow> <mml:mi>LH</mml:mi> </mml:mrow> </mml:msub> </mml:mrow> </mml:mrow> </mml:math> on plasma current, plasma density and main ion species have been investigated. For deuterium plasmas and at low <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi mathvariant="italic">q</mml:mi> </mml:mrow> <mml:mrow> <mml:mn>95</mml:mn> </mml:mrow> </mml:msub> </mml:mrow> </mml:mrow> </mml:math> , the L–H power threshold dependence on density is well described by the International Tokamak Physics Activities scaling law. Nevertheless at larger <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi mathvariant="italic">q</mml:mi> </mml:mrow> <mml:mrow> <mml:mn>95</mml:mn> </mml:mrow> </mml:msub> </mml:mrow> </mml:mrow> </mml:math> values (reduced plasma current at constant toroidal magnetic field), the threshold deviates significantly from the scaling law and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi mathvariant="italic">P</mml:mi> </mml:mrow> <mml:mrow> <mml:mi>LH</mml:mi> </mml:mrow> </mml:msub> </mml:mrow> </mml:mrow> </mml:math> increases with <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi mathvariant="italic">q</mml:mi> </mml:mrow> <mml:mrow> <mml:mn>95</mml:mn> </mml:mrow> </mml:msub> </mml:mrow> </mml:mrow> </mml:math> . As a consequence, a strong correlation of power threshold with transport is reported suggesting that L–H transition is more favorable for L-mode plasmas with already good confinement.

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Journal
Plasma Physics and Controlled Fusion
Published
2025-04-03
DOI
https://doi.org/10.1088/1361-6587/adc8ce
Citations
1
Primary Topic
Plasma Diagnostics and Applications
Type
article
Field-Weighted Citation Impact
0.73

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article

L–H power threshold for neutral beam heated plasmas with deuterium, hydrogen, helium and mixed ion species in TCV

A. Pau, O. Sauter, B. Labit, A. Karpushov et al.
1 citations
Plasma Physics and Controlled Fusion
Plasma Diagnostics and Applications
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article

L–H power threshold for neutral beam heated plasmas with deuterium, hydrogen, helium and mixed ion species in TCV

A. Pau, O. Sauter, B. Labit, A. Karpushov, M. Vallar, D. Mykytchuk, B.P. Duval, A. Perek, Yves Martin, B. Linehan, F. Bagnato
article en
1 citations

Abstract

Abstract A systematic study of the power threshold for L–H transition has been conducted in TCV. Only results from NB heated plasmas are reported. The dependencies of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi mathvariant="italic">P</mml:mi> </mml:mrow> <mml:mrow> <mml:mi>LH</mml:mi> </mml:mrow> </mml:msub> </mml:mrow> </mml:mrow> </mml:math> on plasma current, plasma density and main ion species have been investigated. For deuterium plasmas and at low <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi mathvariant="italic">q</mml:mi> </mml:mrow> <mml:mrow> <mml:mn>95</mml:mn> </mml:mrow> </mml:msub> </mml:mrow> </mml:mrow> </mml:math> , the L–H power threshold dependence on density is well described by the International Tokamak Physics Activities scaling law. Nevertheless at larger <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi mathvariant="italic">q</mml:mi> </mml:mrow> <mml:mrow> <mml:mn>95</mml:mn> </mml:mrow> </mml:msub> </mml:mrow> </mml:mrow> </mml:math> values (reduced plasma current at constant toroidal magnetic field), the threshold deviates significantly from the scaling law and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi mathvariant="italic">P</mml:mi> </mml:mrow> <mml:mrow> <mml:mi>LH</mml:mi> </mml:mrow> </mml:msub> </mml:mrow> </mml:mrow> </mml:math> increases with <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi mathvariant="italic">q</mml:mi> </mml:mrow> <mml:mrow> <mml:mn>95</mml:mn> </mml:mrow> </mml:msub> </mml:mrow> </mml:mrow> </mml:math> . As a consequence, a strong correlation of power threshold with transport is reported suggesting that L–H transition is more favorable for L-mode plasmas with already good confinement.

Plasma Physics and Controlled FusionVol. 67(5)
École Polytechnique Fédérale de Lausanne (CH), Massachusetts Institute of Technology (US)
Schweizerischer Nationalfonds zur Förderung der Wissenschaftlichen Forschung
Openalex Percentile: Top 30%
Plasma Diagnostics and Applications
0.73
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