Abstract

The levitated dipole experiment (LDX) explores the physics of high-temperature plasmas confined by a dipole magnetic field. Stable high-beta plasma has been created and confined by the magnetic field of a superconducting coil. Discharges containing trapped electrons form when microwaves cause strong perpendicular heating at cyclotron resonance. To eliminate the losses to the supports, the magnetic dipole (a superconducting solenoid) will be magnetically levitated for several hours. The dipole magnetic field is generated by a Nb 3 Sn floating coil (F-coil), a maximum field of 5.3 T, operating for up to 2 h. A NbTi charging coil (C-coil) surrounds a portion of the vacuum chamber and induces the current in the floating coil. After the F-coil is lifted to the center of the chamber, the levitation coil (L-coil), made from high-temperature superconductor, magnetically supports it. In the first year of operation, the device has been operated in a supported mode of operation while experience has been gained in the cryogenic performance of the F-coil and the integration of the F-coil and C-coil. Current work focuses on the integration of the F and L coils in preparation for first levitation tests.

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