Hot spots of the main limiter induced by fast ions in experimental advanced superconducting tokamak (EAST)

Abstract

The main limiter in EAST was observed to endure a high heat load and was cracked near the midplane at the right side during the plasma operation. To explore the heat load carried by fast ion loss toward the main limiter, the neutral beam injection (NBI) and radio frequency power proportion experiment was conducted in EAST where the plasma stored energy and line integrated density were kept almost constant. The hot spot at the right side of the main limiter was observed to be enhanced by co-current perpendicular (co-perp) NBI. An NBI ion loss simulation was performed in the presence of the toroidal field ripple and the Coulomb collision by using the orbit code GYCAVA and the NBI code TGCO. The result indicates that the NBI ion loss by ripple and collision mainly causes a bright area below the midplane of the right side of the main limiter as observed in the EAST experiment. The peak heat load of lost fast ions generated by co-perp NBI is ∼0.5 MW/m2 as obtained by 1 MW of NBI deposited power and comparable with the heat load carried by fast electrons induced by lower hybrid current drive. In addition, increasing the gap between the separatrix and the first-wall limiters in the simulation is found to reduce this heat load.

Active generation and control of radial electric field by local neutral beamlets injection in tokamaks

“…The toroidal distribution of wall heat load resulting from local beamlet injection is provided in appendix B. The highest thermal load on the wall caused by the counter-current local beamlet is 0.23 MW m −2 , which is still a relatively small thermal load on the first wall [31]. Figure 12 illustrates the slowing-down density distribution of beam electrons and ions resulting from a beamlet injected at different radii.…”