The AC Loss Measurement of the KSTAR PF1 Coils During the First Commissioning

Abstract

The AC loss in a large superconducting magnet coil shows a tendency to be changed after assembly [1]. For the ac loss measurement of the Korea Superconducting Tokamak Advanced Research (KSTAR) superconducting coils after assembly, several current scenarios, trapezoidal pulses and a DC offset sinusoidal pulses, were applied to the PF1 Upper (U) and Lower (L) coils during the commissioning. The measurement was done once before and once after the plasma discharge experiments. All coil data were obtained by the tokamak monitoring system and helium distribution system which were designed to measure temperature, pressure, and mass-flow at both inlets and outlets of the coils. The PF1 coils of the cable-in-conduit conductor type were made of Nb 3 Sn superconducting strands, whose winding scheme is 20 layers with each layer having 9 turns. Each has 10 cooling channels for the heat removal by the supercritical helium at 4.5 K. For the trapezoidal pulse tests, the current was increased up to 4 kA with several different ramp rates and a 2 kA DC offset and 0.5 kA sine waves with different frequencies from 0.1 Hz to 0.3 Hz were applied to the coil. According to the analyses, the AC loss was slightly decreased for the same condition after 700 plasma shots. It was believe that such a result was due to reduced inter-strand resistances which changed the transverse resistance between the inter-strands. The coupling time constant was estimated to be 32 ms in the trapezoidal tests and 13.6 ms for the DC offset sinusoidal pulses. The former is larger than the latter because of the effect of the jacket eddy current loss due to Incoloy 908 which is a ferromagnetic material. Considering the jacket eddy current losses, the coupling time constant was recalculated and the value estimated to be about 13 ms for all current wave forms during first commissioning.Index Terms-CICC AC loss, DC offset sinusoidal pulse, KSTAR, Nb 3 SN, trapezoidal pulse.

Superconductor Application to the Magnetic Fusion Devices for the Steady-State Plasma Confinement Achievement

“…The applied current was dc biased 2 kA and sinusoidal ac current with amplitude of 0.5 kA for 600 s according to changing the frequency from 0.1 to 0.2 Hz. The figure shows that thermal parameters reached a steady-state condition after 350 s. The coupling loss of PF1 showed different results according to the waveforms (Lee, H.J. et al, 2010;Oh, D.K.…”