Development of a new error field correction coil (C-coil) for DIII-D

The C-coil recently installed on the DIII-D tokamak was developed to reduce the error fields created by imperfections in the location and geometry of the existing coils used to confine, heat, and shape the plasma. First results from C-coil experiments include stable operation in a 1.6 MA plasma with a density less than 1.0/spl times/10/sup 13/ cm/sup -3/, nearly a factor of three lower density than that achievable without the C-coil. The C-coil has also been used in magnetic braking of the plasma rotation and high energy particle confinement experiments. The C-coil system consists of six individual saddle coils, each 60/spl deg/ wide toroidally, spanning the midplane of the vessel with a vertical height of 1.6 m. The coils are located at a major radius of 3.2 m, just outside of the toroidal field coils. The actual shape and geometry of each coil section varied somewhat from the nominal dimensions due to the large number of obstructions to the desired coil path around the already crowded tokamak. Each coil section consists of four turns of 750 MCM insulated copper cable banded with stainless steel straps within the web of a 3 in. /spl times/3 in. stainless steel angle frame. The C-coil structure was designed to resist peak transient radial forces (up to 1800 Nm) exerted on the coil by the toroidal and poloidal fields. The coil frames were supported from existing poloidal field coil case brackets, coil studs, and various other structures on the tokamak.