Requirements for active resistive wall mode (RWM) feedback control

被引:15
|
作者
In, Y. [1 ]
Chu, M. S. [2 ]
Jackson, G. L. [2 ]
Kim, J. S. [1 ]
La Haye, R. J. [2 ]
Liu, Y. Q. [3 ]
Marrelli, L. [4 ]
Okabayashi, M. [5 ]
Reimerdes, H. [6 ]
Strait, E. J. [2 ]
机构
[1] FAR TECH Inc, San Diego, CA USA
[2] Gen Atom Co, San Diego, CA 92186 USA
[3] Euratom CCFE Fus Assoc, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England
[4] Consorzio RFX, I-35127 Padua, Italy
[5] Princeton Plasma Phys Lab, Princeton, NJ 08543 USA
[6] Columbia Univ, Dept Appl Phys & Appl Math, New York, NY 10027 USA
基金
英国工程与自然科学研究理事会;
关键词
DIII-D; EXTERNAL-MODES; STABILIZATION; TOKAMAKS; COILS; STABILITY; ROTATION; PLASMAS;
D O I
10.1088/0741-3335/52/10/104004
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
The requirements for active resistive wall mode (RWM) feedback control have been systematically investigated and established using highly reproducible current-driven RWMs in ohmic discharges in DIII-D. The unambiguous evaluation of active RWM feedback control was not possible in previous RWM studies primarily due to the variability of the onset of the pressure-driven RWMs; the stability of the pressure-driven RWM is thought to be sensitive to various passive stabilization mechanisms. Both feedback control specifications and physics requirements for RWM stabilization have been clarified using the current-driven RWMs in ohmic discharges, when little or no passive stabilization effects are present. The use of derivative gain on top of proportional gain is found to be advantageous. An effective feedback control system should be equipped with a power supply with bandwidth greater than the RWM growth rate. It is beneficial to apply a feedback field that is toroidally phase-shifted from the measured RWM phase in the same direction as the plasma current. The efficacy of the RWM feedback control will ultimately be determined by the plasma fluctuations on internal diagnostics, as well as on external magnetics. The proximity of the feedback coils to the plasma appears to be an important factor in determining the effectiveness of the RWM feedback coils. It is desirable that an RWM feedback control system simultaneously handles error field correction at a low frequency, along with direct RWM feedback at a high frequency. There is an indication of the influence of a second least stable RWM, which had been theoretically predicted but never identified in experiments. A preliminary investigation based on active MHD spectroscopic measurement showed a strong plasma response around 400 Hz where the typical plasma response associated with the first least stable RWM was expected to be negligible. Present active feedback control requirements are based on a single mode assumption, so the investigation of the second least stable RWM is of high interest.
引用
收藏
页数:16
相关论文
共 50 条
  • [31] Active control system for stabilization of resistive wall mode in the low-aspect-ratio RFP RELAX
    Nagano T.
    Masamune S.
    Sanpei A.
    IEEJ Transactions on Fundamentals and Materials, 2020, 140 (06) : 340 - 341
  • [32] Progress in physics and control of the resistive wall mode in advanced tokamaks
    Liu, Yueqiang
    Chapman, I. T.
    Chu, M. S.
    Reimerdes, H.
    Villone, F.
    Albanese, R.
    Ambrosino, G.
    Garofalo, A. M.
    Gimblett, C. G.
    Hastie, R. J.
    Hender, T. C.
    Jackson, G. L.
    La Haye, R. J.
    Okabayashi, M.
    Pironti, A.
    Portone, A.
    Rubinacci, G.
    Strait, E. J.
    PHYSICS OF PLASMAS, 2009, 16 (05)
  • [33] Models of resistive wall tearing mode disruptions
    Strauss, H. R.
    PHYSICS OF PLASMAS, 2023, 30 (11)
  • [34] Theory based recommendations to the resistive wall mode stability studies in tokamaks
    Pustovitov, V. D.
    PHYSICS OF PLASMAS, 2024, 31 (02)
  • [35] Physical understanding of the instability spectrum and the feedback control of resistive wall modes in reversed field pinch
    Wang, Z. R.
    Guo, S. C.
    NUCLEAR FUSION, 2011, 51 (05)
  • [36] Influence of wall thickness on the stability of the resistive wall mode in tokamak plasmas
    Fitzpatrick, Richard
    PHYSICS OF PLASMAS, 2013, 20 (01)
  • [37] Toroidal modeling of anisotropic thermal transport and energetic particle effects on stability of resistive plasma resistive wall mode
    Bai, Xue
    Liu, Yueqiang
    Gao, Zhe
    Hao, Guangzhou
    PHYSICS OF PLASMAS, 2020, 27 (07)
  • [38] Control of linear modes in cylindrical resistive magnetohydrodynamics with a resistive wall, plasma rotation, and complex gain
    Brennan, D. P.
    Finn, J. M.
    PHYSICS OF PLASMAS, 2014, 21 (10)
  • [39] Effect of Trapped Energetic Particles on the Resistive Wall Mode
    Hao, G. Z.
    Wang, A. K.
    Liu, Y. Q.
    Qiu, X. M.
    PHYSICAL REVIEW LETTERS, 2011, 107 (01)
  • [40] Resistive Wall Mode Instability at Intermediate Plasma Rotation
    Berkery, J. W.
    Sabbagh, S. A.
    Betti, R.
    Hu, B.
    Bell, R. E.
    Gerhardt, S. P.
    Manickam, J.
    Tritz, K.
    PHYSICAL REVIEW LETTERS, 2010, 104 (03)