Abstract
Magnetisation is one of the main barriers to practical use of bulk superconductors as high field magnets. Recently several authors have reported a flux jump effect that allows penetration of magnetic flux into a bulk superconductor during pulsed field magnetisation (PFM) at lower fields than that would be predicted on the basis of the Bean model. We have systematically investigated macroscopic flux jumps in single grain GdBa2Cu3O7−δ–Ag (GdBCO–Ag) bulk superconductors with diameters of up to 30 mm when subjected to pulsed magnetic fields. Flux jumps were observed at temperatures between 30 and 77 K and in applied magnetic fields of up to 7 T. The applied pulsed field required to trigger the instability or flux jump field, Bj, was determined experimentally and found to increase with decreasing temperature. An extended instability criterion based on a 2D axisymmetric model was used to predict Bj at various temperatures and the results are in good agreement with experiments. A significant temperature rise has been measured experimentally during the magnetisation process which indicates that local heat generation due to the sharp rise of the applied field in the PFM process is the primary cause of the flux jumps. The experimental results suggest further that the critical current density reduces to almost zero in the warm part of the sample during the short period of non-equilibrium. A peak trapped field of 4.1 T at the surface and 5.3 T between a stack of two GdBCO–Ag bulk superconductors was achieved at 30 K by means of an optimised two-step pulse sequence with the assistance of the flux jumps, which is extremely promising for potential applications of these technologically important materials.
Highlights
Flux was pushed further towards the centre when magnetic fields higher than 4.2 T were applied, which enhanced the peak flux density, but reduced the trapped field towards the edge of the sample as indicated by the dashed arrows in figure 4
We report flux jumps in bulk high temperature superconducting (HTS) observed during a pulsed field magnetisation (PFM) process with a pulsed magnetic field of up to 7 T and a fixed rise time of 35 ms
Flux jumps in a single grain GdBCO–Ag bulk superconductor of diameter up to 30 mm have been observed during the PFM process
Summary
Flux was pushed further towards the centre when magnetic fields higher than 4.2 T were applied, which enhanced the peak flux density, but reduced the trapped field towards the edge of the sample as indicated by the dashed arrows in figure 4. The magnetic field distribution follows the critical state model, with the gradient of the flux density being directly proportional to Jc of the sample, until a flux jump occurs at 31 ms.
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