Transport, energy balance, and stability of a large field‐reversed configuration

Experiments have been conducted on the Large s Experiment (LSX) [Phys. Rev. Lett. 69, 2212 (1992)] field‐reversed theta pinch, where plasmas confined in a field‐reversed configuration (FRC) have exhibited record energy, particle, and configuration lifetimes. By careful control of the formation process, it was possible to form symmetric, quiescent FRCs with s values (the number of ion gyroradii from the field null to the separatrix of the FRC) as large as 5. LSX particle confinement showed a strong scaling with s. The inferred particle diffusivity, Ds, at large s approached ∼2 m2/s, which, along with previous experimental results, indicate a favorable Ds∼s−1/2 scaling. At large s, both electron and ion cross‐field thermal conduction losses become negligible compared to convective losses, with the inferred χ⊥e∼4 m2/s, which was near classical values. Data from several diagnostics employed on the LSX device were analyzed to seek correlation between distortions in the plasma shape and the confinement properti...

[1]  M. Tuszewski,et al.  Field reversed configurations , 1988 .

[2]  A. Ishida,et al.  Ideal stability of a toroidal confinement system without a toroidal magnetic field , 1994 .

[3]  E. Crawford,et al.  Wideband ``silicon bolometers'' on the LSX field reversed configuration experiment , 1992 .

[4]  J. Slough,et al.  Formation studies of field‐reversed configurations in a slow field‐reversed theta pinch , 1989 .

[5]  J. Slough,et al.  Field reversed configuration lifetime scaling based on measurements from the Large s Experiment , 1993 .

[6]  Yasuji Kohzaki,et al.  Conceptual design of the D-3He reactor artemis , 1992 .

[7]  J. Slough,et al.  Flux and particle life-time measurements in field-reversed configurations , 1984 .

[8]  Daniel C. Barnes,et al.  Kinetic tilting stability of field‐reversed configurations , 1986 .

[9]  L. Steinhauer Electrostatic confinement in the edge layer of field‐reversed configurations , 1986 .

[10]  M. Tuszewski,et al.  Axial dynamics in field‐reversed theta pinches. II: Stability , 1991 .

[11]  A. Ishida,et al.  Profile consistency in equilibria of field‐reversed configurations , 1992 .

[12]  D. Barnes,et al.  Stabilization of the field‐reversed configuration (FRC) tilt instability with energetic ion beams , 1991 .

[13]  J. Slough,et al.  Stability of field-reversed configurations in the large s experiment (LSX) , 1993 .

[14]  W. Armstrong,et al.  Particle Confinement Scaling in Field-Reversed Configurations , 1983 .

[15]  Hoffman,et al.  Confinement and stability of plasmas in a field-reversed configuration. , 1992, Physical review letters.

[16]  M. Rosenbluth,et al.  MHD stability of Spheromak , 1979 .

[17]  M. Tuszewski,et al.  A zero-dimensional transport model for field-reversed configurations , 1984 .

[18]  M. Tuszewski,et al.  Electron energy confinement in field reversed configuration plasmas , 1990 .