Stability of the resistive wall mode in HBT-EP plasmas
Phys. Plasmas 13, 072512 (2006); doi:10.1063/1.2245542
Published 31 July 2006
You are not logged in to this journal. Log in
A relatively simple model of the resistive wall mode (RWM) is derived for a large aspect ratio, low
, circular cross section, tokamak plasma, surrounded by a concentric, thin, uniform resistive wall. The model employs uniform toroidal plasma rotation, and includes the following realistic edge dissipation mechanisms: dissipation due to charge-exchange with cold neutrals, and dissipation due to neoclassical flow damping. The model is applied to the HBT-EP tokamak [T. Ivers, E. Eisner, A. Garofalo et al., Phys. Plasmas 3, 1926 (1996)], with the wall parameters determined by fitting to output from the VALEN code [J. Bialek, A. H. Boozer, M. E. Mauel, and G. A. Navratil, Phys. Plasmas 8, 2170 (2001)]. Dissipation due to charge-exchange with cold neutrals is found to be not quite large enough to account for the observed rotational stabilization of the RWM in HBT-EP plasmas. On the other hand, dissipation due to neoclassical flow damping is sufficiently large to explain the observations.
©2006 American Institute of Physics
, circular cross section, tokamak plasma, surrounded by a concentric, thin, uniform resistive wall. The model employs uniform toroidal plasma rotation, and includes the following realistic edge dissipation mechanisms: dissipation due to charge-exchange with cold neutrals, and dissipation due to neoclassical flow damping. The model is applied to the HBT-EP tokamak [T. Ivers, E. Eisner, A. Garofalo et al., Phys. Plasmas 3, 1926 (1996)], with the wall parameters determined by fitting to output from the VALEN code [J. Bialek, A. H. Boozer, M. E. Mauel, and G. A. Navratil, Phys. Plasmas 8, 2170 (2001)]. Dissipation due to charge-exchange with cold neutrals is found to be not quite large enough to account for the observed rotational stabilization of the RWM in HBT-EP plasmas. On the other hand, dissipation due to neoclassical flow damping is sufficiently large to explain the observations.
©2006 American Institute of Physics
| History: | Received 25 April 2006; accepted 10 July 2006; published 31 July 2006 |
| Permalink: |
http://link.aip.org/link/?PHPAEN/13/072512/1 |
KEYWORDS and PACS
plasma instability,
plasma-wall interactions,
Tokamak devices,
plasma toroidal confinement,
plasma flow,
plasma boundary layers,
plasma transport processes,
charge exchange
- 52.35.Py
Plasma macroinstabilities (hydromagnetic) e.g., kink, fire-hose, mirror, ballooning, tearing, trapped-particle, flute, Rayleigh-Taylor instabilities, etc - 52.40.Hf
Plasmamaterial interactions; boundary layer effects - 52.55.Fa
Tokamaks - 52.55.Tn
Ideal and resistive plasma MHD modes; kinetic modes - 52.30.-q
Plasma dynamics and flow - 52.25.Fi
Plasma transport properties - YEAR: 2006
RELATED DATABASES
PUBLICATION DATA
1070-664X (print)
1089-7674 (online)
REFERENCES (30)
For access to fully linked references, you need to log in.
For access to fully linked references, you need to Log in.
- F. Troyon, R. Gruber, H. Saurenmann, S. Semenzato, and S. Succi,
Plasma Phys. Controlled Fusion 26, 209 (1984) . - C. Kessel, J. Manickam, G. Rewoldt, and W. M. Tang, Phys. Rev. Lett. 72, 1212 (1994).
- E. A. Lazarus, G. A. Navratil, C. M. Greenfield et al., Phys. Rev. Lett. 77, 2714 (1996).
- J. P. Goedbloed, D. Pfirsch, and H. Tasso,
Nucl. Fusion 12, 649 (1972) . - M. Okabayashi, N. Pomphrey, J. Manikam et al.,
Nucl. Fusion 36, 1167 (1996) . - A. M. Garofalo, E. Eisner, T. H. Ivers et al.,
Nucl. Fusion 38, 1029 (1998) . - S. A. Sabbagh, J. M. Bialek, R. E. Bell et al.,
Nucl. Fusion 44, 560 (2004) . - M. Shilov, C. Cates, R. James et al., Phys. Plasmas 11, 2573 (2004).
- A. Bondeson, and D. J. Ward, Phys. Rev. Lett. 72, 2709 (1994).
- R. Betti, and J. P. Freidberg, Phys. Rev. Lett. 74, 2949 (1995).
- R. Fitzpatrick, Phys. Plasmas 9, 3459 (2002).
- W. L. Rowan, A. G. Meigs, E. R. Solano, P. M. Valanju, M. D. Calvin, and R. D. Hazeltine, Phys. Fluids B 5, 2485 (1993).
- E. D. Taylor, C. Cates, M. E. Mauel, D. A. Maurer, D. Nadle, G. A. Navratril, and M. Shilov, Phys. Plasmas 9, 3938 (2002).
- T. H. Stix, Phys. Fluids 16, 1260 (1973).
- K. C. Shaing, Phys. Plasmas 11, 5525 (2004).
- J. A. Wesson, Tokamaks, 3rd ed. (Oxford University Press, Oxford, 2004).
- T. Ivers, E. Eisner, A. Garofalo et al., Phys. Plasmas 3, 1926 (1996).
- J. P. Freidberg, Ideal Magnetohydrodynamics (Springer, New York, 1987).
- S. I. Braginskii, "Transport processes in a plasma," in Reviews of Plasma Physics (Consultants Bureau, New York, 1965), Vol. 1, p. 205.
- R. D. Hazeltine and J. D. Meiss, Plasma Confinement (Dover, New York, 2003).
- J. D. Callen, W. X. Qu, K. D. Siebert et al., in Plasma Physics and Controlled Nuclear Fusion Research 1986 Proceedings of the 11th Conference, Kyoto (International Atomic Energy Agency, Vienna, 1987), Vol. 2, p. 157.
- A. I. Smolyakov and E. Lazzaro, Phys. Plasmas 11, 4353 (2004).
- A. H. Boozer, Phys. Plasmas 5, 3350 (1998).
- W. A. Newcomb,
Ann. Phys. (N.Y.) 10, 232 (1960) . - D. Maurer and M. E. Mauel (private communication, 2006).
- J. A. Wesson,
Nucl. Fusion 18, 87 (1978) . - M. E. Mauel, J. Bialek, A. H. Boozer, et al.,
Nucl. Fusion 45, 285 (2005) . - R. Fitzpatrick, Phys. Plasmas 1, 2931 (1994).
- J. Bialek, A. H. Boozer, M. E. Mauel, and G. A. Navratil, Phys. Plasmas 8, 2170 (2001).
- A. C. Riviere,
Nucl. Fusion 11, 363 (1971) .







