2020
DOI: 10.1016/j.physc.2019.1353582
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Levitation forces and relaxation properties of a high-T superconductor in varying external magnetic fields

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Cited by 5 publications
(2 citation statements)
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“…Superconducting magnets have the great advantage of offering higher magnetic field intensity compared with traditional PMs; utilizing a superconducting magnet as magnetic field source can obtain much greater levitation force than PMs. Under a high background magnetic field, some new properties are obtained which could not be observed in PMs' magnetic fields [10][11][12]. To promote more profound understanding of the interaction mechanisms between HTSs and high external magnetic fields, a levitation force measurement system composed of a 6T NbTi conduction-cooled superconducting magnet has been built in our laboratory.…”
Section: Introductionmentioning
confidence: 99%
“…Superconducting magnets have the great advantage of offering higher magnetic field intensity compared with traditional PMs; utilizing a superconducting magnet as magnetic field source can obtain much greater levitation force than PMs. Under a high background magnetic field, some new properties are obtained which could not be observed in PMs' magnetic fields [10][11][12]. To promote more profound understanding of the interaction mechanisms between HTSs and high external magnetic fields, a levitation force measurement system composed of a 6T NbTi conduction-cooled superconducting magnet has been built in our laboratory.…”
Section: Introductionmentioning
confidence: 99%
“…Различные эффекты, такие как рост критического тока с увеличением магнитного поля, что проявляется в уширении петли перемагничивания образца [2], практически полностью определяются структурой и динамикой вихревой решетки. Сверхпроводящие образцы, а также кабели и ленты на основе ВТСП используются в сверхпроводящих магнитах [3], ограничителях тока [4,5] и в левитационной технологии [6][7][8]. В последнем случае используется магнитолевитационная система сверхпроводник -постоянный магнит, в которой сверхпроводник находится в градиентном поле постоянного магнита.…”
Section: Introductionunclassified