Control of resistive wall modes in the spherical tokamak
In this work, the MARS-F/K codes (Liu et al 2000 Phys. Plasmas 7 3681; Liu et al 2008 Phys. Plasmas 15 112503) are utilized to model the passive and active control of the n = 1 ( n is the toroidal mode number) resistive wall mode (RWM) in a spherical tokamak (aspect ratio A = 1.66). It is found that...
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Veröffentlicht in: | Nuclear fusion 2023-02, Vol.63 (2), p.26021 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | In this work, the MARS-F/K codes (Liu
et al
2000
Phys. Plasmas
7
3681; Liu
et al
2008
Phys. Plasmas
15
112503) are utilized to model the passive and active control of the
n
= 1 (
n
is the toroidal mode number) resistive wall mode (RWM) in a spherical tokamak (aspect ratio
A
= 1.66). It is found that passive stabilization of the RWM gives a relatively small increase in normalized beta above the no-wall limit, relying on toroidal plasma flow and drift kinetic resonance damping from both thermal and energetic particles. Results of active control show that with the flux-to-voltage control scheme, which is the basic choice, a proportional controller alone does not yield complete stabilization of the mode. Adding a modest derivative action, and assuming an ideal situation without any noise in the closed-loop, the RWM can be fully stabilized with the axial plasma flow at 5% of the Alfvén speed. In the presence of sensor signal noise, success rates exceeding 90% are achieved, and generally increase with the proportional feedback gain. On the other hand, the required control coil voltage also increases with feedback gain and with the sensor signal noise. |
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ISSN: | 0029-5515 1741-4326 |
DOI: | 10.1088/1741-4326/acadf0 |