Pedestal Studies in DIII-D
Journal Article
·
· Fusion Science and Technology
OSTI ID:20854278
- General Atomics (United States)
- Lawrence Livermore National Laboratory (United States)
- University of California (United States)
- Oak Ridge National Laboratory (United States)
- University of Toronto (Canada)
Studies of the H-mode pedestal in the DIII-D tokamak are presented. The global energy confinement increases as the plasma pressure on top of the pedestal increases. The best empirical description for a pedestal width parameter is {delta}{sub pe} [proportional to] ({beta}{sub pol}{sup PED}){sup 0.4}, where {delta}{sub pe} is the width of the electron pressure pedestal and {beta}{sub pol}{sup PED} is the poloidal beta at the top of the pedestal. The edge profiles of electron density n{sub e}, electron temperature T{sub e}, and ion temperature T{sub i} can all have different shapes. Thus, a simple width scaling for the edge might not exist, and studies of the physics of individual profiles have been initiated. A model for the n{sub e} profile, based on self-consistent treatment of edge particle sources and edge particle transport, agrees with several experimental observations. The steep gradient region for the T{sub e} profile often extends farther into the plasma than the n{sub e} pedestal step. Magnetohydrodynamic stability provides the ultimate limits to the evolution of the pedestal and usually leads to edge instabilities called edge-localized modes (ELMs). However, the absence of ELMs in a regime called the Quiescent H-mode shows that large pedestals can be produced without ELMs.
- OSTI ID:
- 20854278
- Journal Information:
- Fusion Science and Technology, Journal Name: Fusion Science and Technology Journal Issue: 2 Vol. 48; ISSN 1536-1055
- Country of Publication:
- United States
- Language:
- English
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