2012
DOI: 10.1063/1.3699364
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High non-inductive fraction H-mode discharges generated by high-harmonic fast wave heating and current drive in the National Spherical Torus Experiment

Abstract: A deuterium H-mode discharge with a plasma current of 300 kA, an axial toroidal magnetic field of 0.55 T, and a calculated non-inductive plasma current fraction of 0.7-1 has been generated in the National Spherical Torus Experiment by 1.4 MW of 30 MHz high-harmonic fast wave (HHFW) heating and current drive. Seventy-five percent of the non-inductive current was generated inside an internal transport barrier that formed at a normalized minor radius $0.4. Three quarters of the non-inductive current was bootstrap… Show more

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Cited by 24 publications
(11 citation statements)
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“…Further, edge losses in the scrape-off-layer to the divertor [84][85][86][87] can degrade HHFW core coupling efficiency, and parasitic absorption by NBI fast-ions [88][89][90] can compete with thermal electron heating and current drive. For these reasons, HHFW appears most applicable to heating and driving current in low-current high-bootstrap-fraction plasmas [91] serving as targets for subsequent non-inductive current rampup through other means. Electron Bernstein waves (EBW) are another potentially very attractive wave for heating and driving current in over-dense plasma conditions [92][93][94], but the necessity for precise tailoring of the edge density gradient [95] to maximize the double-mode-conversion efficiency combined with other loss mechanisms in the plasma edge [96,97] have thus far made efficiently coupling to the EBW operationally challenging.…”
Section: Energy Confinementmentioning
confidence: 99%
“…Further, edge losses in the scrape-off-layer to the divertor [84][85][86][87] can degrade HHFW core coupling efficiency, and parasitic absorption by NBI fast-ions [88][89][90] can compete with thermal electron heating and current drive. For these reasons, HHFW appears most applicable to heating and driving current in low-current high-bootstrap-fraction plasmas [91] serving as targets for subsequent non-inductive current rampup through other means. Electron Bernstein waves (EBW) are another potentially very attractive wave for heating and driving current in over-dense plasma conditions [92][93][94], but the necessity for precise tailoring of the edge density gradient [95] to maximize the double-mode-conversion efficiency combined with other loss mechanisms in the plasma edge [96,97] have thus far made efficiently coupling to the EBW operationally challenging.…”
Section: Energy Confinementmentioning
confidence: 99%
“…Present NSTX research is pursuing noninductive formation of plasma current using CHI [140] to form a closed-flux plasma of 0.2-0.3 MA to be heated and sustained by high-harmonic fast-waves in a high bootstrapcurrent-fraction H-mode plasma. Promising HHFW heating and current drive results have recently been obtained [141] in low-current (I P = 300 kA) ohmic target plasmas being developed as plasma current ramp-up targets for NBI. In these plasmas, an HHFW-induced H-mode with a central electron temperature of up to 3 keV was achieved with 65% noninductive current drive (f BS = 43%, f RFCD = 22%) with 1.4 MW of injected HHFW power.…”
Section: Overview Of Non-inductive Current Formation and Ramp-upmentioning
confidence: 99%
“…The computed bootstrap current varies from 100 to 230 kA. The current generated directly by HHFW power was generated inside a normalized minor radius ∼0.2, and 75% of the non-inductive current was generated inside a normalized minor radius ∼0.4 [135]. Over the entire range of NBI heated plasmas, up to 65% NICF was experimentally reached (computed by TRANSP), peaking at plasma current value of I p = 0.7 MA (figure 31).…”
Section: Non-inductive Current By Nbi and Rfmentioning
confidence: 99%