Confinement heating and stability in the ELMO bumpy torus (EBT)

High power ECH (utilizing a 28-GHz gyrotron at power levels up to 200 kW, cw) and fast-wave ICH (in the frequency range 15-30 MHz at power levels up to 20 kW, cw) experiments on EBT-Scale (EBT-S) have yielded Te approximately 1.1 keV, n approximately 1-2*1018 m-3, and tau E approximately 6 ms. The ring and core loss rates scale as predicted by the neoclassical theory, and the plasma parameters have the predicted values for the densities, temperatures, and confinement times reachable in this small plasma radius (10 cm) device at low field (1.0 T). In addition, the following observations were made: (1) the stable operating window is larger at high power levels, (2) a substantial increase in energetic ion tails (Ti>100 eV) and a doubling of the ring electron stored energy (beta) were seen at the highest ICH power levels, and (3) a significant increase in core density and stabilization of hot electron modes was possible with gas puffing.

[1]  F. W. Baity,et al.  Plasma properties in the ELMO bumpy torus , 1983 .

[2]  J. S. Tolliver,et al.  Resonant ion transport in EBT , 1983 .

[3]  M. Rosenbluth,et al.  EBT stability theory , 1983 .

[4]  F. W. Baity,et al.  Heating experiments in the ion cyclotron range of frequencies on EBT-S , 1983 .

[5]  N. Uckan,et al.  Synchrotron emission from the relativistic ring electrons in the ELMO Bumpy Torus , 1982 .

[6]  L. Berry,et al.  Electron-confinement studies on EBT-S using soft-x-ray techniques , 1982 .

[7]  R. Richards,et al.  Confinement scaling of core plasma electrons in the ELMO Bumpy Torus experiment , 1982 .

[8]  N. Uckan Hot-electron-ring physics , 1982 .

[9]  N. Uckan Temperature limit in ECH hot electron plasmas , 1982 .

[10]  D. Batchelor A simple power deposition model for microwave heating in EBT-I , 1981 .

[11]  Nermin A. Uckan,et al.  EBT reactor magnetics and particle confinement , 1981 .

[12]  J. Glowienka ELMO Bumpy Torus: An alternate concept to tokamaks and mirrors , 1981 .

[13]  J. Cobble,et al.  Electron heating and confinement measurements in the EBT-S toroidal core plasma with Thomson scattering , 1981 .

[14]  F. Bieniosek Study of plasma confinement in ELMO Bumpy Torus with a heavy-ion beam probe , 1981 .

[15]  N. Uckan EBT Ring Physics , 1981 .

[16]  C. Hedrick,et al.  Variational corrections to ELMO Bumpy Torus neoclassical ion plateau transport , 1980 .

[17]  D. B. Nelson Effects of hot electrons on magnetohydrodynamic modes in ELMO Bumpy Torus , 1980 .

[18]  R. Hazeltine,et al.  Bumpy torus transport in the low collision frequency limit , 1981 .

[19]  Nermin A. Uckan,et al.  A simple annulus power balance in EBT experiments , 1980 .

[20]  S. Kuo,et al.  Elmo Bumpy Torus heavy ion probe , 1980 .

[21]  C. Hedrick,et al.  Radial transport in the Elmo Bumpy Torus in collisionless electron regimes , 1979 .

[22]  C. Hedrick,et al.  Radial transport in ELMO bumpy torus with constant edge neutral flux , 1979 .

[23]  H. Moos,et al.  Spatial distribution of impurities and H neutrals in ELMO Bumpy Torus (EBT) , 1979 .

[24]  C. Hedrick,et al.  Radial transport in the ELMO Bumpy Torus in collisional regimes , 1979 .

[25]  P. Colestock,et al.  Influence of globalmagnetic perturbations on plasma behavior in Elmo Bumpy Torus , 1979 .

[26]  F. W. Baity,et al.  Summary of EBT-I experimental results , 1978 .

[27]  H. Berk,et al.  Stability of interchange modes in a hot electron plasma , 1978 .

[28]  R. Cohen,et al.  Nonadiabaticity in mirror machines , 1978 .

[29]  C. Hedrick,et al.  Macroscopic stability and beta limit in the ELMO Bumpy Torus , 1977 .

[30]  R. A. Dory,et al.  ELMO Bumpy Torus , 1977 .

[31]  N. Hoernqvist Plasma physics and controlled nuclear fusion research 1971: Fourth Conference Proceedings, Madison 17–23 June 1971 (IAEA, Vienna, 1971) vols. II + III: pp. 755 + 673, US $20.00 + 20.00. , 1972 .