Realisation of Hybrid Trapped Field Magnetic Lens (HTFML) consisting of REBCO bulk lens and REBCO bulk cylinder at 77 K
dc.contributor.author | Namba, S | |
dc.contributor.author | Fujishiro, H | |
dc.contributor.author | Naito, T | |
dc.contributor.author | Ainslie, MD | |
dc.contributor.author | Zhou, D | |
dc.date.accessioned | 2022-02-04T00:36:38Z | |
dc.date.available | 2022-02-04T00:36:38Z | |
dc.date.issued | 2020 | |
dc.identifier.issn | 1742-6588 | |
dc.identifier.other | jpcs_1559_1_012079 | |
dc.identifier.other | j15591079 | |
dc.identifier.uri | https://www.repository.cam.ac.uk/handle/1810/333632 | |
dc.description.abstract | <jats:title>Abstract</jats:title> <jats:p>A hybrid trapped field magnet lens (HTFML) can reliably generate a concentrated magnetic field, <jats:italic>B</jats:italic> <jats:sub>c</jats:sub>, in the centre of the magnetic lens higher than the trapped field of the trapped field magnet (TFM) and the applied magnetic field, <jats:italic>B</jats:italic> <jats:sub>app</jats:sub>, even after the external magnetizing field decreased to zero. In this paper, the performance of HTFMLs consisting of EuBaCuO bulk TFM with various heights and a GdBaCuO bulk magnetic lens was investigated at 77 K using liquid nitrogen. A concentrated magnetic field of <jats:italic>B</jats:italic> <jats:sub>c</jats:sub> = 0.80 T was achieved at the centre of the HTFML for the tallest TFM after removing an applied magnetic field of <jats:italic>B</jats:italic> <jats:sub>app</jats:sub> = 0.50 T. The influence of the height of the outer TFM cylinder on the final concentrated field was studied experimentally and discussed using numerical simulation.</jats:p> | |
dc.description.sponsorship | - Adaptable and Seamless Technology transfer Program through Target-driven R&D (A-STEP) from Japan Science and Technology Agency (JST), Grant No. VP30218088419 - JSPS KAKENHI Grant No. 19K05240 | |
dc.language | en | |
dc.publisher | IOP Publishing | |
dc.subject | Paper | |
dc.title | Realisation of Hybrid Trapped Field Magnetic Lens (HTFML) consisting of REBCO bulk lens and REBCO bulk cylinder at 77 K | |
dc.type | Article | |
dc.date.updated | 2022-02-04T00:36:38Z | |
prism.issueIdentifier | 1 | |
prism.publicationName | Journal of Physics: Conference Series | |
prism.volume | 1559 | |
dc.identifier.doi | 10.17863/CAM.81048 | |
dcterms.dateAccepted | 2020-02-03 | |
rioxxterms.versionofrecord | 10.1088/1742-6596/1559/1/012079 | |
rioxxterms.version | VoR | |
rioxxterms.licenseref.uri | http://creativecommons.org/licenses/by/3.0/ | |
dc.contributor.orcid | Ainslie, Mark [0000-0003-0466-3680] | |
dc.identifier.eissn | 1742-6596 | |
pubs.funder-project-id | Engineering and Physical Sciences Research Council (EP/P020313/1) | |
pubs.conference-name | 14th European Conference on Applied Superconductivity | |
pubs.conference-start-date | 2019-09-01 | |
pubs.conference-finish-date | 2019-09-05 |
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