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Modeling of High-T(c) Superconducting Bulk using Different J(c)–T Relationships over Dynamic Permanent Magnet Guideway
The linear temperature dependence of critical current density J(c)∝((T(c)-T)/(T(c)-T(0))) and the nonlinear functions of J(c)∝(1-(T/T(c))(2))(α) with the exponent α equal to 1, 3/2, and 2 are used to calculate the dynamic levitation force, the temperature distribution, and the current density distri...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2019
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6766180/ https://www.ncbi.nlm.nih.gov/pubmed/31505813 http://dx.doi.org/10.3390/ma12182915 |
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author | Hong, Ye Zheng, Jun Liao, Hengpei |
author_facet | Hong, Ye Zheng, Jun Liao, Hengpei |
author_sort | Hong, Ye |
collection | PubMed |
description | The linear temperature dependence of critical current density J(c)∝((T(c)-T)/(T(c)-T(0))) and the nonlinear functions of J(c)∝(1-(T/T(c))(2))(α) with the exponent α equal to 1, 3/2, and 2 are used to calculate the dynamic levitation force, the temperature distribution, and the current density distribution of the high-temperature superconducting (HTS) YBaCuO bulk over a permanent magnetic guideway (PMG). The calculations were based on the H-formulation and E–J power law. The model of the HTS bulk and the PMG has been built as a geometric entity by finite element software. To simulate the magnetic field fluctuation caused by the PMG arrangement irregularity, a small amplitude vibration in the vertical direction is applied to the PMG during the calculations. Both the low vibration frequency of 2 Hz and the high vibration frequency of 60 Hz are analyzed as the representative converted linear speeds of 34 km/h and 1018 km/h for magnetic levitation (Maglev) application. We compared the electromagnetic-thermo-force modeling with the experiments and the previous model without considering the thermal effect. The levitation force computed by the J(c)–T relationship, in which J(c) is proportional to (1-(T/T(c))(2))(2), is found to be in best agreement with the experimental data under quasi-static conditions. This work can provide a reference for the HTS electromagnetic-thermal-force coupling reproduction method of HTS Maglev at high speed. |
format | Online Article Text |
id | pubmed-6766180 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2019 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-67661802019-09-30 Modeling of High-T(c) Superconducting Bulk using Different J(c)–T Relationships over Dynamic Permanent Magnet Guideway Hong, Ye Zheng, Jun Liao, Hengpei Materials (Basel) Article The linear temperature dependence of critical current density J(c)∝((T(c)-T)/(T(c)-T(0))) and the nonlinear functions of J(c)∝(1-(T/T(c))(2))(α) with the exponent α equal to 1, 3/2, and 2 are used to calculate the dynamic levitation force, the temperature distribution, and the current density distribution of the high-temperature superconducting (HTS) YBaCuO bulk over a permanent magnetic guideway (PMG). The calculations were based on the H-formulation and E–J power law. The model of the HTS bulk and the PMG has been built as a geometric entity by finite element software. To simulate the magnetic field fluctuation caused by the PMG arrangement irregularity, a small amplitude vibration in the vertical direction is applied to the PMG during the calculations. Both the low vibration frequency of 2 Hz and the high vibration frequency of 60 Hz are analyzed as the representative converted linear speeds of 34 km/h and 1018 km/h for magnetic levitation (Maglev) application. We compared the electromagnetic-thermo-force modeling with the experiments and the previous model without considering the thermal effect. The levitation force computed by the J(c)–T relationship, in which J(c) is proportional to (1-(T/T(c))(2))(2), is found to be in best agreement with the experimental data under quasi-static conditions. This work can provide a reference for the HTS electromagnetic-thermal-force coupling reproduction method of HTS Maglev at high speed. MDPI 2019-09-09 /pmc/articles/PMC6766180/ /pubmed/31505813 http://dx.doi.org/10.3390/ma12182915 Text en © 2019 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Article Hong, Ye Zheng, Jun Liao, Hengpei Modeling of High-T(c) Superconducting Bulk using Different J(c)–T Relationships over Dynamic Permanent Magnet Guideway |
title | Modeling of High-T(c) Superconducting Bulk using Different J(c)–T Relationships over Dynamic Permanent Magnet Guideway |
title_full | Modeling of High-T(c) Superconducting Bulk using Different J(c)–T Relationships over Dynamic Permanent Magnet Guideway |
title_fullStr | Modeling of High-T(c) Superconducting Bulk using Different J(c)–T Relationships over Dynamic Permanent Magnet Guideway |
title_full_unstemmed | Modeling of High-T(c) Superconducting Bulk using Different J(c)–T Relationships over Dynamic Permanent Magnet Guideway |
title_short | Modeling of High-T(c) Superconducting Bulk using Different J(c)–T Relationships over Dynamic Permanent Magnet Guideway |
title_sort | modeling of high-t(c) superconducting bulk using different j(c)–t relationships over dynamic permanent magnet guideway |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6766180/ https://www.ncbi.nlm.nih.gov/pubmed/31505813 http://dx.doi.org/10.3390/ma12182915 |
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