Skip to main content
U.S. Department of Energy
Office of Scientific and Technical Information

Stability of negative central magnetic shear discharges in the DIII-D tokamak

Journal Article · · Physics of Plasmas
DOI:https://doi.org/10.1063/1.872366· OSTI ID:560620
Discharges with negative central magnetic shear (NCS) hold the promise of enhanced fusion performance in advanced tokamaks. However, stability to long wavelength magnetohydrodynamic modes is needed to take advantage of the improved confinement found in NCS discharges. The stability limits seen in DIII-D [J. L. Luxon and L. G. Davis, Fusion Technol. {bold 8}, 441 (1985)] experiments depend on the pressure and current density profiles and are in good agreement with stability calculations. Discharges with a strongly peaked pressure profile reach a disruptive limit at low beta, {beta}{sub N}={beta}(I/aB){sup {minus}1}{le}2.5 ({percent}m T/MA), caused by an n=1 ideal internal kink mode or a global resistive instability close to the ideal stability limit. Discharges with a broad pressure profile reach a soft beta limit at significantly higher beta, {beta}{sub N}=4 to 5, usually caused by instabilities with n{gt}1 and usually driven near the edge of the plasma. With broad pressure profiles, the experimental stability limit is independent of the magnitude of negative shear but improves with the internal inductance, corresponding to lower current density near the edge of the plasma. Understanding of the stability limits in NCS discharges has led to record DIII-D fusion performance in discharges with a broad pressure profile and low edge current density. {copyright} {ital 1997 American Institute of Physics.}
Research Organization:
General Atomics
DOE Contract Number:
AC03-89ER51114
OSTI ID:
560620
Report Number(s):
CONF-961102--
Journal Information:
Physics of Plasmas, Journal Name: Physics of Plasmas Journal Issue: 5 Vol. 4; ISSN PHPAEN; ISSN 1070-664X
Country of Publication:
United States
Language:
English