Steady-state plasma heating was successfully performed and sustained for more than 30 min in the LHD. By using ICRF heating and additional EC and NBI heating, a total input energy of 1.3 GJ was achieved. The average input power was 680 kW and the plasma duration was 31 min 45 sec. The hardware of the ICRF and divertor plates was much improved and the position of the ICRF antenna was optimized. The heat load to the divertor plates was effectively dispersed by the magnetic axis swing technique, which caused large changes in the heat load distribution along the divertor leg traces.
Keywords:Large Helical Device, Steady state operation, ICRF heating, Divertor, 1.3 GJ In December 2004, steady-state plasma sustainment was successfully performed for more than 30 min in the Large Helical Device (LHD) [1]. The average input power was 680 kW (ICRF [2-4] 520 kW, ECH 100 kW and NBI 60 kW) and the plasma duration was 31 min 45 sec. Before the 2003 campaign, the plasma sustainment time of the ICRF longpulse experiment was limited by local temperature rises of the divertor carbon plates near the ICRF antenna section, and gradual increase of out-gassing from the wall finally terminated the plasma operation [5]. After that experiment, a new mechanical structure and new carbon material sheets were used to suppress the temperature rise and the out-gassing rate. The hardware of ICRF heating was also much improved.The steady-state operation was performed using the standard experimental configuration of the LHD. The magnetic axis radius was around 3.67 to 3.7 m, the magnetic strength was 2.75 T at 3.6 m, and the pitch parameter of the helical winding was 1.254. The helical coil current was fixed and the vertical coil currents were controlled. Three ICRF antennas were used and the frequency was 38.47 MHz. In author's e-mail: mutoh@nifs.ac.jp this condition, the cyclotron resonance region of minority ions is located near the saddle point on the mod-B contour plane in the cross-section of the plasma. In this mode, the ICRF wave power heated minority ions and did not heat electrons directly. The LHD vacuum chamber was conditioned by boronization, which seemed to be effective in suppressing the impurity influx to low levels during steady-state operations.The plasma parameters are shown in Fig. 1. The ICRF and ECH were continuously injected, and NBI was repetitively injected by the 25 sec pulse operations. The plasma was mainly sustained by ICRF and partially supported by ECH [6] and NBI [7]. The ECH and NBI helped to control some disturbances, for example, occasional dust particles from the upper vacuum vessel. During the operation time of 31 min, helium gas was fed by a puffing system to form the majority ion species for the ICRF heating. The repetitive NBI pulses worked to heat the plasma and also to keep the hydrogen concentration ratio within a suitable range for the minority-heating mode of ICRF. Without the NBI pulses, the ratio of Hα to Helium I lines gradually decreased by a factor