Comparison of Superconducting Properties of Bulk MgB2 Samples with Pyrene Additive Produced by B Powder and C encapsulated B Powder
dc.contributor.author | Erdem, Ozge | |
dc.date.accessioned | 2024-10-04T18:49:24Z | |
dc.date.available | 2024-10-04T18:49:24Z | |
dc.date.issued | 2024 | |
dc.department | Bayburt Üniversitesi | en_US |
dc.description.abstract | In this paper, the advantages and disadvantages of using B powder and C encapsulated B powder as a precursor during the production process of MgB2 with the addition of pyrene (C16H10) were investigated. Two MgB2 bulk samples with the addition of 10 wt % C16H10 of 1 g MgB2 were produced by the in-situ method using B powder and C encapsulated B powder. The C encapsulated B powder as a precursor was prepared by adding 10% C16H10 as a C source. From XRD and SEM analysis, a greater increase in MgO phase and a greater decrease in a-lattice parameter were observed for the sample produced with B, compared to the sample produced with C encapsulated B. The curves of critical current density (J(c)) at 5 K showed a similar character for both samples. The J(c) values at 5 K in self field were respectively obtained as 1.52 x 10(5) A/cm(2) and 1.90 x 10(5) A/cm(2) for the samples produced by B and C encapsulated B. The decrement ratio of in-field J(c) at 20 K was less affected by increasing magnetic field for the sample produced using C encapsulated B due to the relatively higher increase in the irreversibility field (H-irr) and the upper critical magnetic field (H-c2) values. The J(c) values at 20 K and 3 T were respectively determined as 1.49 x 10(4) A/cm(2) and 1.93 x 10(4) A/cm(2) for the samples produced with B and C encapsulated B. | en_US |
dc.identifier.doi | 10.1007/s10909-023-03016-7 | |
dc.identifier.endpage | 67 | en_US |
dc.identifier.issn | 0022-2291 | |
dc.identifier.issn | 1573-7357 | |
dc.identifier.issue | 1-2 | en_US |
dc.identifier.scopus | 2-s2.0-85178484341 | en_US |
dc.identifier.scopusquality | Q2 | en_US |
dc.identifier.startpage | 53 | en_US |
dc.identifier.uri | https://doi.org/10.1007/s10909-023-03016-7 | |
dc.identifier.uri | http://hdl.handle.net/20.500.12403/3108 | |
dc.identifier.volume | 214 | en_US |
dc.identifier.wos | WOS:001112439000001 | en_US |
dc.identifier.wosquality | Q4 | en_US |
dc.indekslendigikaynak | Web of Science | en_US |
dc.indekslendigikaynak | Scopus | en_US |
dc.language.iso | en | en_US |
dc.publisher | Springer/Plenum Publishers | en_US |
dc.relation.ispartof | Journal of Low Temperature Physics | en_US |
dc.relation.publicationcategory | Makale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı | en_US |
dc.rights | info:eu-repo/semantics/closedAccess | en_US |
dc.subject | MgB2 | en_US |
dc.subject | Pyrene | en_US |
dc.subject | Superconductivity | en_US |
dc.subject | Critical current density | en_US |
dc.subject | C encapsulated B | en_US |
dc.title | Comparison of Superconducting Properties of Bulk MgB2 Samples with Pyrene Additive Produced by B Powder and C encapsulated B Powder | en_US |
dc.type | Article | en_US |