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Transport Current Measurement of - and - for a Bulk REBCO Superconductor | IEEE Journals & Magazine | IEEE Xplore

Transport Current Measurement of I_{c}(T, B,\theta) and n(T, B,\theta) for a Bulk REBCO Superconductor


Abstract:

Bulk rare-earth barium cuprate (REBCO) high-temperature superconductors are attractive for many electromagnetic applications due to their ability to support large current...Show More

Abstract:

Bulk rare-earth barium cuprate (REBCO) high-temperature superconductors are attractive for many electromagnetic applications due to their ability to support large current densities and trap large magnetic fields. At present, magnetisation techniques are the predominant method of measuring the critical current density, J_\text {c}, for bulk superconductors, due to the abundance of measurement devices and ease of sample preparation and measurement. However, this approach does not provide direct access to measurements of magneto-angular anisotropy of J_\text {c} nor n-value. By contrast, transport current techniques allow direct measurement of the full thermo-magneto-angular dependence of both I_\text {c} and n, but limited data is available for REBCO bulks, due to the difficulties of sample preparation and measurement. This work introduces a reproducible method to prepare a single-grain bulk GdBCO-Ag superconductor for transport current characterisation, and presents measured data for both I_\text {c} and n that has been obtained over a broad parameter-space. The measured n-values are lower than is commonly assumed, with typical n-values at 77 K being in the range of 10 to 14. An accurate value of n is required when computationally modelling transient effects.
Published in: IEEE Transactions on Applied Superconductivity ( Volume: 33, Issue: 5, August 2023)
Article Sequence Number: 6800106
Date of Publication: 23 January 2023

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Funding Agency:

Paihau-Robinson Research Institute, Victoria University of Wellington, Lower Hutt, New Zealand
MacDiarmid Institute for Advanced Materials and Nanotechnology, Victoria University of Wellington, Wellington, New Zealand
Paihau-Robinson Research Institute, Victoria University of Wellington, Lower Hutt, New Zealand
CAN SUPERCONDUCTORS s.r.o., Kamenice, Czechia
CAN SUPERCONDUCTORS s.r.o., Kamenice, Czechia
Paihau-Robinson Research Institute, Victoria University of Wellington, Lower Hutt, New Zealand
Department of Engineering, King's College London, London, U.K.
Paihau-Robinson Research Institute, Victoria University of Wellington, Lower Hutt, New Zealand
MacDiarmid Institute for Advanced Materials and Nanotechnology, Victoria University of Wellington, Wellington, New Zealand

Paihau-Robinson Research Institute, Victoria University of Wellington, Lower Hutt, New Zealand
MacDiarmid Institute for Advanced Materials and Nanotechnology, Victoria University of Wellington, Wellington, New Zealand
Paihau-Robinson Research Institute, Victoria University of Wellington, Lower Hutt, New Zealand
CAN SUPERCONDUCTORS s.r.o., Kamenice, Czechia
CAN SUPERCONDUCTORS s.r.o., Kamenice, Czechia
Paihau-Robinson Research Institute, Victoria University of Wellington, Lower Hutt, New Zealand
Department of Engineering, King's College London, London, U.K.
Paihau-Robinson Research Institute, Victoria University of Wellington, Lower Hutt, New Zealand
MacDiarmid Institute for Advanced Materials and Nanotechnology, Victoria University of Wellington, Wellington, New Zealand

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