CORC® ACCELERATOR MAGNET CABLES AND WIRES

CORC® accelerator magnet cables and wires form our solution for developing the next generation of accelerator magnets operating at fields above 20 T, or at temperatures above 4.2 K.

CORC® accelerator cables and wires are being developed with support of the U.S. Department of Energy and in collaboration with Lawrence Berkeley National Laboratory, CERN, Brookhaven National Laboratory, the University of Twente and the National High Magnetic Field Laboratory.

 

 

 

 

 

 

CORC® magnet cables and wires:
– Are the only isotropic REBCO-based HTS cables
– Have demonstrated high-field performance without degradation
– Have demonstrated high current density at 20 T of 530 A/mm2
– Will soon have current densities in excess of 600 A/mm2 at 20 T
– Allow bending to less than 20 mm radius
– Have demonstrated the ability to sustain over 7 % axial tensile strain, far exceeding that of any other practical superconductor

Best CORC® wire performance to date, measured at 4.2 K a different applied magnetic fields
Current and current density as a function of magnetic field at 4.2 K of a CORC® wire
CORC® wire performance as a function of applied axial tensile strain compared to other practical superconductors
Performance of CORC® wires during fatigue cycling at different axial tensile loads

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

CORC® magnet cablesCORC® magnet wires
Diameter5 to 10 mm2.5 to 4.5 mm
Temperature, Field4.2 K, 20 T4.2 K, 20 T
Currentup to 35,000 Aup to 10,000 A
Current Densityup to 500 A/mm2up to 530 A/mm2
Bending Radius40 - 100 mm20 mm

 

 

CORC® accelerator magnet cables and wires are currently being incorporated into:
– Canted-Cosine-Theta and Uni-layer accelerator magnets at Lawrence Berkeley National Laboratory
– COM dipole magnets at Fermi National Laboratory
– Common Coil dipole magnets at Brookhaven National Laboratory

Outer layer of a CORC® CCT magnet developed by Lawrence Berkeley National Laboratory
Voltage measured across each coil of a 6-layer, 40-turn/layer CCT magnet wound from CORC® wires as a function of current at 4.2 K
Dipole field as a function of current for the CCT magnet developed at LBNL. A peak dipole field of 6 T was reached.