Effect of a static external magnetic perturbation on resistive mode stability in tokamaks
Phys. Plasmas 1, 3337 (1994); doi:10.1063/1.870918
Issue Date: October 1994
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The influence of a general static external magnetic perturbation on the stability of resistive modes in a tokamak plasma is examined. There are three main parts to this investigation. First, the vacuum perturbation is expanded as a set of well-behaved toroidal ring functions, and is, thereafter, specified by the coefficients of this expansion. Second, a dispersion relation is derived for resistive plasma instabilities in the presence of a general external perturbation, and finally, this dispersion relation is solved for the amplitudes of the tearing and twisting modes driven in the plasma by a specific perturbation. It is found that the amplitudes of driven tearing and twisting modes are negligible until a certain critical perturbation strength is exceeded. Only tearing modes are driven in low-
plasmas with 
p
1. However, twisting modes may also be driven if 
p
1. For error-field perturbations made up of a large number of different poloidal and toroidal harmonics the critical strength to drive locked modes has a ``staircase'' variation with edge-q, characterized by strong discontinuities as coupled rational surfaces enter or leave the plasma. For single harmonic perturbations, the variation with edge-q is far smoother. Both types of behavior have been observed experimentally. The critical perturbation strength is found to decrease strongly close to an ideal external kink stability boundary. This is also in agreement with experimental observations.
Physics of Plasmas is copyrighted by The American Institute of Physics.
plasmas with 
p
1. However, twisting modes may also be driven if 
p
1. For error-field perturbations made up of a large number of different poloidal and toroidal harmonics the critical strength to drive locked modes has a ``staircase'' variation with edge-q, characterized by strong discontinuities as coupled rational surfaces enter or leave the plasma. For single harmonic perturbations, the variation with edge-q is far smoother. Both types of behavior have been observed experimentally. The critical perturbation strength is found to decrease strongly close to an ideal external kink stability boundary. This is also in agreement with experimental observations.
Physics of Plasmas is copyrighted by The American Institute of Physics.
| History: | Received 1 April 1994; accepted 17 June 1994 |
| Permalink: |
http://link.aip.org/link/?PHPAEN/1/3337/1 |
KEYWORDS and PACS
TOKAMAK DEVICES,
MAGNETIC FIELDS,
PLASMA MACROINSTABILITIES,
DISPERSION RELATIONS,
TEARING INSTABILITY,
PERTURBATION THEORY,
ROTATING PLASMA,
LOW&minus,
BETA PLASMA
- 52.35.Py
The physics of plasmas and electric discharges Waves, oscillations, and instabilities in plasma Plasma macroinstabilities (hydromagnetic, e.g., kink, fire-hose, mirror, ballooning, tearing, trapped-particle, flute, Rayleigh
Taylor)
- 52.55.Fa
The physics of plasmas and electric discharges Plasma equilibrium and confinement Tokamaks - 52.40.Hf
The physics of plasmas and electric discharges Plasma interactions Solid
plasma interactions; wall effects; probes; sheaths
- 52.30.Jb
The physics of plasmas and electric discharges Plasma flow; magnetohydrodynamics Resistive MHD effects - YEAR: 1994
RELATED DATABASES
PUBLICATION DATA
1070-664X (print)
1089-7674 (online)
REFERENCES (24)
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- J. T. Scoville, R. J. La Haye, A. G. Kellman, T. H. Osborne, R. D. Stambaugh, E. J. Strait, and T. S. Taylor,
Nucl. Fusion 31, 875 (1991 ). - R. Fitzpatrick and T. C. Hender, Phys. Fluids B 3, 644 (1991).
- A. W. Morris, P. G. Carolan, R. Fitzpatrick, T. C. Hender, and T. N. Todd, Phys. Fluids B 4, 413 (1992).
- T. C. Hender, R. Fitzpatrick, A. W. Morris, P. G. Carolan, R. D. Durst, T. Edlington, J. Ferreira, S. J. Fielding, P. S. Haynes, J. Hugill, I. J. Jenkins, R. J. La Haye, B. J. Parham, D. C. Robinson, T. N. Todd, M. Valovič, and G. Vayakis, Nucl. Fusion 32, 2091 (1992).
- R. J. La Haye, A. W. Hyatt, and J. T. Scoville, Nucl. Fusion 2, 2119 (1992).
- R. Fitzpatrick, in Theory of Fusion Plasmas, Proceedings of the Joint Varenna-Lausanne International Workshop, Varenna 1992 (Società Italiana di Fisica, Bologna, 1992), p. 147.
- R. J. La Haye, R. Fitzpatrick, T. C. Hender, A. W. Morris, J. T. Scoville, and T. N. Todd, Phys. Fluids B 4, 2098 (1992).
- T. H. Jensen, A. W. Leonard, and A. W. Hyatt, Phys. Fluids B 5, 1239 (1993).
- R. Fitzpatrick, Nucl. Fusion 33, 1049 (1993).
- G. M. Fishpool and P. S. Haynes,
Nucl. Fusion 34, 109 (1994 ). - R. Toschi, in Plasma Physics and Controlled Nuclear Fusion Research 1990, Proceedings of the 13th International Conference, Washington (International Atomic Energy Agency, Vienna, 1991), Vol. 3, p. 225.
- R. Fitzpatrick, Phys. Plasmas 1, 3308 (1994).
- R. Fitzpatrick, R. J. Hastie, T. J. Martin, and C. M. Roach,
Nucl. Fusion 33, 1533 (1993 ). - H. P. Furth, J. Killeen, and M. N. Rosenbluth, Phys. Fluids 6, 459 (1963).
- W. A. Newcomb,
Ann. Phys. 10, 232 (1960 ). - T. C. Hender and S. C. Cowley, Phys. Fluids B 1, 2194 (1989).
- M. N. Bussac, D. Edery, R. Pellat, and J. L. Soulé, in Plasma Physics and Controlled Nuclear Fusion Research 1976, Proceedings of the 6th International Conference, Berchtesgaden (International Atomic Energy Agency, Vienna, 1977), Vol. 1, p. 607.
- S. C. Cowley and R. J. Hastie, Phys. Fluids 31, 426 (1988).
- R. Fitzpatrick, in Ref. 6, p. 147.
- P. H. Rutherford, Phys. Fluids 16, 1903 (1973).
- A. W. Morris, P. G. Carolan, R. Fitzpatrick, T. C. Hender, R. O'Connell, T. N. Todd, and M. Valovič, in Controlled Fusion and Plasma Physics, Proceedings of the 20th European Conference, Lisbon, 1993 (European Physical Society, Petit-Lancy, 1993), Vol. 1, p. 227.
- P. H. Rebut, D. V. Bartlett, G. Bäumel, K. Behringer, R. Behrisch, E. Bertolini, C. Best, R. J. Bickerton, F. Bombi, J. L. Bonnerue, A. Boschi, G. Bracco, M. L. Browne, M. Brusati, A. Bulliard, D. J. Campbell, P. G. Carolan, J. Christiansen, P. Chuilon, J. G. Cordey, S. Corti, A. E. Costley, G. Decker, K. J. Dietz, D. F. Düchs, G. Duesing, R. K. F. Emery, W. W. Englehardt, T. Eriksson, J. Fessey, M. J. Forrest, C. Froger, K. Fullard, M. Gadeberg, A. Gibson, R. Gill, A. Gondhalekar, C. Gowers, B. J. Green, G. Grosso, N. C. Hawkes, J. Hemmerich, M. Huart, A. Hubbard, C. A. Hugenholtz, M. Huguet, O. N. Jarvis, B. E. Jensen, E. M. Jones, G. E. Källne, J. C. Källne, L. de Kock, H. Krause, P. Kupschus, J. R. Last, E. Lazzaro, P. Lomas, G. M. McCracken, G. Magyar, F. K. Mast, M. Mead, P. L. Mondino, P. Morgan, A. W. Morris, L. Nickesson, H. Niedermeyer, P. Nielsen, P. Noll, J. Paillére, N. J. Peacock, M. Pick, J. P. Poffe, R. Prentice, C. Raymond, D. C. Robinson, R. Ross, G. Sadler, J. Saffert, V. Schmidt, F. C. Schüller, K. Sonnenberg, M. F. Stamp, C. A. Steed, A. Stella, P. E. Stott, D. Summers, A. Tanga, P. R. Thomas, G. Tonetti, E. Usselmann, P. Van Belle, H. Van Der Beken, J. E. Van Montfoort, M. L. Watkins, J. A. Wesson, T. Winkel, V. Zanza, and J. Zwart, in Plasma Physics and Controlled Nuclear Fusion Research 1984, Proceedings of the 10th International Conference, London (International Atomic Energy Agency, Vienna, 1985), Vol. 1, p. 11.
- M. N. Bussac, R. Pellat, D. Edery, and J. L. Soulé, Phys. Rev. Lett. 35, 1638 (1975).
- C. Mercier,
Nucl. Fusion 1, 47 (1960 ).







