Limiter H-mode experiments on TFTR
Limiter H-modes with centrally peaked density profiles have been obtained in TFTR using a highly conditioned graphite limiter. The transition to these centrally peaked H-modes takes place from the supershot to the H-mode rather than the usual L- to H-mode transition observed on other tokamaks. Bidirectional beam heating is required to induce the transition. Density peaking factors, n{sub e}(0)/, greater than 2.3 are obtained and at the same time the H-mode characteristics are similar to those of limiter H-modes on other tokamaks, while the global confinement, {tau}{sub E}, can be >2.5 times L-mode scaling. The transport analysis of the data shows that transport in these H-modes is similar to that of supershots within the inner 0.6 m core of the plasma, but the stored electron energy (calculated using measured values of T{sub e} and n{sub e}) is higher for the H-mode at the plasma edge. Microwave scattering data for the edge plasma shows broad spectra at k = 5.5 cm{sup {minus}1} which begin at the drop in D{sub {alpha}} radiation and are strongly shifted in the electron diamagnetic drift direction. At the same time, beam emission spectroscopy (BES) shows a coherent mode near the boundary which propagates in the ion direction with m = 15--20 at 20--30 kHz. During the ELM event these apparent rotations cease and Mirnov fluctuations in the frequency range of 50--500 kHz increase in intensity. 16 refs., 8 figs.
- Research Organization:
- Princeton Plasma Physics Lab. (PPPL), Princeton, NJ (United States)
- Sponsoring Organization:
- USDOE; USDOE, Washington, DC (USA)
- DOE Contract Number:
- AC02-76CH03073
- OSTI ID:
- 5838587
- Report Number(s):
- PPPL-2743; ON: DE91012309
- Country of Publication:
- United States
- Language:
- English
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Characteristics of the TFTR limiter H-mode: The transition, ELMs, transport and confinement
Characteristics of the TFTR limiter H-mode: The transition, ELMs, transport and confinement
Related Subjects
TFTR TOKAMAK
H-MODE PLASMA CONFINEMENT
BEAM INJECTION HEATING
CONFINEMENT TIME
FLUCTUATIONS
GRAPHITE
LIMITERS
MAGNETIC FIELDS
CARBON
CONFINEMENT
ELEMENTAL MINERALS
ELEMENTS
HEATING
MINERALS
NONMETALS
PLASMA CONFINEMENT
PLASMA HEATING
THERMONUCLEAR REACTORS
TOKAMAK TYPE REACTORS
VARIATIONS
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