Tokamak Operation with Safety Factor q95 | Zendy

P. Piovesan | Zendy; J.M. Hanson | Zendy; P. Martin | Zendy; G.A. Navratil | Zendy; F. Turco | Zendy; J. Bialek | Zendy; N.M. Ferraro | Zendy; R.J. La Haye | Zendy; M.J. Lanctot | Zendy; M. Okabayashi | Zendy; C. Paz-Soldan | Zendy; E. J. Strait | Zendy; A. D. Turnbull | Zendy; P. Zanca | Zendy; M. Baruzzo | Zendy; T. Bolzonella | Zendy; A. W. Hyatt | Zendy; G.L. Jackson | Zendy; L. Marrelli | Zendy; L. Piron | Zendy; D. Shiraki | Zendy

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Tokamak Operation with Safety Factor q95<2 via Control of MHD Stability

Author(s) -

P. Piovesan,

J.M. Hanson,

P. Martin,

G.A. Navratil,

F. Turco,

J. Bialek,

N.M. Ferraro,

R.J. La Haye,

M.J. Lanctot,

M. Okabayashi,

C. Paz-Soldan,

E. J. Strait,

A. D. Turnbull,

P. Zanca,

M. Baruzzo,

T. Bolzonella,

A. W. Hyatt,

G.L. Jackson,

L. Marrelli,

L. Piron,

D. Shiraki

Publication year - 2014

Publication title -

physical review letters

Language(s) - English

Resource type - Journals

SCImago Journal Rank - 3.688

H-Index - 673

eISSN - 1079-7114

pISSN - 0031-9007

DOI - 10.1103/physrevlett.113.045003

Subject(s) - divertor , tokamak , safety factor , physics , magnetohydrodynamic drive , limit (mathematics) , resistive touchscreen , toroid , fusion power , magnetohydrodynamics , bootstrap current , plasma , algorithm , nuclear engineering , computational physics , computer science , nuclear physics , mathematical analysis , mathematics , computer vision , engineering

Magnetic feedback control of the resistive-wall mode has enabled the DIII-D tokamak to access stable operation at safety factor q95=1.9 in divertor plasmas for 150 instability growth times. Magnetohydrodynamic stability sets a hard, disruptive limit on the minimum edge safety factor achievable in a tokamak, or on the maximum plasma current at a given toroidal magnetic field. In tokamaks with a divertor, the limit occurs at q95=2, as confirmed in DIII-D. Since the energy confinement time scales linearly with current, this also bounds the performance of a fusion reactor. DIII-D has overcome this limit, opening a whole new high-current regime not accessible before. This result brings significant possible benefits in terms of fusion performance, but it also extends resistive-wall mode physics and its control to conditions never explored before. In present experiments, the q95<2 operation is eventually halted by voltage limits reached in the feedback power supplies, not by intrinsic physics issues. Improvements to power supplies and to control algorithms have the potential to further extend this regime

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