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Evaluation of residual stress and texture in isotope based Mg(11)B(2) superconductor using neutron diffraction

Magnesium diboride (MgB(2)) superconducting wires have demonstrated commercial potential to replace niobium–titanium (NbTi) in terms of comparable critical current density. Its higher critical temperature makes MgB(2) wire suitable for liquid-helium-free operation. We recently reported boron-11 isot...

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Detalles Bibliográficos
Autores principales: Jie, Hyunseock, Qiu, Wenbin, Gajda, Daniel, Kim, Jeonghun, Anvar, Valiyaparambil Abdulsalam, Nijhuis, Arend, Bando, Yoshio, Yamauchi, Yusuke, Luzin, Vladimir, Shahriar A. Hossain, Md.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2018
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9090752/
https://www.ncbi.nlm.nih.gov/pubmed/35558062
http://dx.doi.org/10.1039/c8ra05906c
Descripción
Sumario:Magnesium diboride (MgB(2)) superconducting wires have demonstrated commercial potential to replace niobium–titanium (NbTi) in terms of comparable critical current density. Its higher critical temperature makes MgB(2) wire suitable for liquid-helium-free operation. We recently reported boron-11 isotope-based low-activation Mg(11)B(2) superconducting wire with decent critical current density appropriate for low-cost superconducting fusion magnets. In this study, we have mainly focused on the neutron diffraction technique to measure the residual stress in Mg(11)B(2) superconducting wire for the first time. The residual stress state was given qualitative and quantitative interpretation in terms of micro- and macrostress generation mechanisms based on the isotropic model confirmed by neutron texture measurements. The relationship between the stress/strain state in the wire and the transport critical current density is also discussed. This investigation could pave the way to further enhancement of the critical current density of low-activation Mg(11)B(2) superconducting wires suitable for next-generation fusion grade magnets.