R. Granetz1, T. H. Osborne2, R. L. Boivin1, M. Greenwald1,
R. J. Groebner2, A. Hubbard1, J. Irby1, L. L. Lao2,
A. W. Leonard2, Y. Lin1, R. L. Miller2, T. Sunn Pedersen1,
G. D. Porter3, Alcator C-MOD Team and DIII-D Team
1 MIT Plasma Science and Fusion Center, Cambridge, MA, USA
2 General Atomics, PO Box 85608, San Diego, CA, USA
3 Lawrence Livermore National Laboratory, Livermore, CA, USA
Abstract. Since the H-mode edge pedestal effectively sets the
boundary conditions for energy transport throughout the core, a better
understanding of the pedestal region is necessary in order to fully predict
H-mode performance. Pedestal characteristics in the DIII-D and Alcator C-Mod
tokamaks are described, and scalings of the pedestal width with various plasma
parameters are shown. The pedestal width in both tokamaks varies in an inverse
sense with plasma current, and is independent of toroidal field. Other
similarities, as well as differences, are discussed. It is also found that the
pedestal widths of the various physical quantities involved
(
Te, Ti, ne, ni) may be different.
IAEA 2001