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Journal Articles

Stabilization and prevention of the 2/1 neoclassical tearing mode for improved performance in DIII-D

Prater, R.*; La Haye, R. J.*; Luce, T. C.*; Petty, C. C.*; Strait, E. J.*; Ferron, J. R.*; Humphreys, D. A.*; Isayama, Akihiko; Lohr, J.*; Nagasaki, Kazunobu*; et al.

Nuclear Fusion, 47(5), p.371 - 377, 2007/05

 Times Cited Count:58 Percentile:87.07(Physics, Fluids & Plasmas)

The $$m=2$$ /$$n=1$$ neoclassical tearing mode (NTM) has been observed to strongly degrade confinement and frequently lead to a disruption in high $$beta$$ discharges in DIII-D if allowed to grow to large size. Stabilization of grown NTMs by application of highly localized electron cyclotron current drive (ECCD) at the island location has led to operation at increased plasma pressure, up to the no-wall kink limit. After the NTM is stabilized by the ECCD, the correct location for the current drive is maintained using information from real-time equilibrium reconstructions which include measurements from the motional Stark effect diagnostic. This same process is used alternatively to prevent the mode from ever growing, leading to performance at the pressure limit in high performance hybrid discharges with $$beta$$ above 4%. Modeling using the modified Rutherford equation shows that the required power is in close agreement with the experimental threshold for prevention of the 2/1 NTM.

Journal Articles

Prevention of the 2/1 neoclassical tearing mode in DIII-D

Prater, R.*; La Haye, R. J.*; Luce, T. C.*; Petty, C. C.*; Strait, E. J.*; Ferron, J. R.*; Humphreys, D. A.*; Isayama, Akihiko; Lohr, J.*; Nagasaki, Kazunobu*; et al.

Proceedings of 21st IAEA Fusion Energy Conference (FEC 2006) (CD-ROM), 8 Pages, 2007/03

Onset of the m/n=2/1 neoclassical tearing mode (NTM) has been prevented in high-performance DIII-D discharges using localized electron cyclotron current drive (ECCD). Active tracking of the $$q$$=2 surface location, using real-time equilibrium reconstructions with motional Stark effect data, allows the current drive to be maintained at the rational surface even in the absence of a detectable mode. With the application of this technique in DIII-D hybrid discharges, the 2/1 mode is avoided and good energy confinement is maintained for more than 1 second with $$beta$$ at the estimated n=1 no-wall stability limit for ideal kink modes ($$beta$$$$_{rm T}$$ approximately equals 3.9 % and normalized beta $$beta$$$$_{rm N}$$ approximately equals 3.2). The results can be understood through modeling using the modified Rutherford equation.

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