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Reproducibility of small Ge(2)C(6)H(10)O(7)-added MgB(2) bulks fabricated by ex situ Spark Plasma Sintering used in compound bulk magnets with a trapped magnetic field above 5 T
Bulk discs (20 mm diameter and 4.3 mm thickness) of MgB(2) added with Ge(2)C(6)H(10)O(7) were obtained by Spark Plasma Sintering. Six samples with composition MgB(2)(Ge(2)C(6)H(10)O(7))(0.0014) and one undoped sample were fabricated under similar conditions and were magnetically characterized in ord...
Autores principales: | , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2020
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7324367/ https://www.ncbi.nlm.nih.gov/pubmed/32601322 http://dx.doi.org/10.1038/s41598-020-67463-y |
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author | Badica, P. Aldica, G. Grigoroscuta, M. A. Burdusel, M. Pasuk, I. Batalu, D. Berger, K. Koblischka-Veneva, A. Koblischka, M. R. |
author_facet | Badica, P. Aldica, G. Grigoroscuta, M. A. Burdusel, M. Pasuk, I. Batalu, D. Berger, K. Koblischka-Veneva, A. Koblischka, M. R. |
author_sort | Badica, P. |
collection | PubMed |
description | Bulk discs (20 mm diameter and 4.3 mm thickness) of MgB(2) added with Ge(2)C(6)H(10)O(7) were obtained by Spark Plasma Sintering. Six samples with composition MgB(2)(Ge(2)C(6)H(10)O(7))(0.0014) and one undoped sample were fabricated under similar conditions and were magnetically characterized in order to determine the scattering of properties and reproducibility. The main source of the scattering of the properties is the decomposition of the additive due to elimination of the organic part in gas form, which occurs stepwise with intensive vacuum drops at around ~ 560 and ~ 740 °C. A third drop, which is sometimes not well resolved being part of the second peak at 740 °C, occurs at ~ 820 °C. The critical temperature at the midpoint of the transition, T(c), shows only a relatively small variation between 37.4 and 38 K, and the irreversibility field at a low temperature of 5 K takes values between 8 and 10 T. The pinning force and pinning force related parameters do not correlate with the carbon substituting for boron in MgB(2) and suggest a synergetic influence of the microstructural details and carbon. Overall, despite the superconducting properties scattering, the samples are of high quality. Stacked into a column of six samples, they can trap at the center and on the surface of the column a magnetic field of 6.78 and 5.19 T at 12 K, 5.20 and 3.98 T at 20 K and 2.39, and 1.96 T at 30 K. These promising values, combined with facile fabrication of the samples with relatively high quality and reproducibility, show the feasibility of their use in building complex and large compound arrangements for bulk magnets and other applications. |
format | Online Article Text |
id | pubmed-7324367 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2020 |
publisher | Nature Publishing Group UK |
record_format | MEDLINE/PubMed |
spelling | pubmed-73243672020-06-30 Reproducibility of small Ge(2)C(6)H(10)O(7)-added MgB(2) bulks fabricated by ex situ Spark Plasma Sintering used in compound bulk magnets with a trapped magnetic field above 5 T Badica, P. Aldica, G. Grigoroscuta, M. A. Burdusel, M. Pasuk, I. Batalu, D. Berger, K. Koblischka-Veneva, A. Koblischka, M. R. Sci Rep Article Bulk discs (20 mm diameter and 4.3 mm thickness) of MgB(2) added with Ge(2)C(6)H(10)O(7) were obtained by Spark Plasma Sintering. Six samples with composition MgB(2)(Ge(2)C(6)H(10)O(7))(0.0014) and one undoped sample were fabricated under similar conditions and were magnetically characterized in order to determine the scattering of properties and reproducibility. The main source of the scattering of the properties is the decomposition of the additive due to elimination of the organic part in gas form, which occurs stepwise with intensive vacuum drops at around ~ 560 and ~ 740 °C. A third drop, which is sometimes not well resolved being part of the second peak at 740 °C, occurs at ~ 820 °C. The critical temperature at the midpoint of the transition, T(c), shows only a relatively small variation between 37.4 and 38 K, and the irreversibility field at a low temperature of 5 K takes values between 8 and 10 T. The pinning force and pinning force related parameters do not correlate with the carbon substituting for boron in MgB(2) and suggest a synergetic influence of the microstructural details and carbon. Overall, despite the superconducting properties scattering, the samples are of high quality. Stacked into a column of six samples, they can trap at the center and on the surface of the column a magnetic field of 6.78 and 5.19 T at 12 K, 5.20 and 3.98 T at 20 K and 2.39, and 1.96 T at 30 K. These promising values, combined with facile fabrication of the samples with relatively high quality and reproducibility, show the feasibility of their use in building complex and large compound arrangements for bulk magnets and other applications. Nature Publishing Group UK 2020-06-29 /pmc/articles/PMC7324367/ /pubmed/32601322 http://dx.doi.org/10.1038/s41598-020-67463-y Text en © The Author(s) 2020 Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/. |
spellingShingle | Article Badica, P. Aldica, G. Grigoroscuta, M. A. Burdusel, M. Pasuk, I. Batalu, D. Berger, K. Koblischka-Veneva, A. Koblischka, M. R. Reproducibility of small Ge(2)C(6)H(10)O(7)-added MgB(2) bulks fabricated by ex situ Spark Plasma Sintering used in compound bulk magnets with a trapped magnetic field above 5 T |
title | Reproducibility of small Ge(2)C(6)H(10)O(7)-added MgB(2) bulks fabricated by ex situ Spark Plasma Sintering used in compound bulk magnets with a trapped magnetic field above 5 T |
title_full | Reproducibility of small Ge(2)C(6)H(10)O(7)-added MgB(2) bulks fabricated by ex situ Spark Plasma Sintering used in compound bulk magnets with a trapped magnetic field above 5 T |
title_fullStr | Reproducibility of small Ge(2)C(6)H(10)O(7)-added MgB(2) bulks fabricated by ex situ Spark Plasma Sintering used in compound bulk magnets with a trapped magnetic field above 5 T |
title_full_unstemmed | Reproducibility of small Ge(2)C(6)H(10)O(7)-added MgB(2) bulks fabricated by ex situ Spark Plasma Sintering used in compound bulk magnets with a trapped magnetic field above 5 T |
title_short | Reproducibility of small Ge(2)C(6)H(10)O(7)-added MgB(2) bulks fabricated by ex situ Spark Plasma Sintering used in compound bulk magnets with a trapped magnetic field above 5 T |
title_sort | reproducibility of small ge(2)c(6)h(10)o(7)-added mgb(2) bulks fabricated by ex situ spark plasma sintering used in compound bulk magnets with a trapped magnetic field above 5 t |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7324367/ https://www.ncbi.nlm.nih.gov/pubmed/32601322 http://dx.doi.org/10.1038/s41598-020-67463-y |
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