Numéro |
J. Phys. IV France
Volume 08, Numéro PR1, May 1998
CCAS1Actes du premier colloque sur les composites actifs supraconducteurs / Proceedings of the first conference on the active superconducting composites |
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Page(s) | Pr1-35 - Pr1-44 | |
DOI | https://doi.org/10.1051/jp4:1998106 |
Actes du premier colloque sur les composites actifs supraconducteurs / Proceedings of the first conference on the active superconducting composites
J. Phys. IV France 08 (1998) Pr1-35-Pr1-44
DOI: 10.1051/jp4:1998106
Magnetic field expulsion in superconducting granular ceramics and in polymer/superconductor composites
A. Benlhachemi1, 2, M.A. Fremy1, C. Breandon1, H. Tatarenko1, J.R. Gavarri1 and H. Benyaich21 Laboratoire des Matériaux Multiphasés et Interfaces, Faculté des Sciences et Techniques, Université de Toulon et du Var, BP. 132, 83957 La Garde, France
2 Laboratoire de Chimie des Solides, Faculté des Sciences, Université Ibnou Zohr, Agadir, Maroc
Abstract
The magnetic interaction between a permanent magnet and superconducting ceramics
such as YBa2Cu3O7-δ and Bi1,6Pb0,4Sr2Ca2Cu3O10+δ depend on the superconducting state of each
phase and on the junctions between grains. In the case of polymer/superconductor composites,
screening effects depend on the volume fraction of superconductor. Measurements of the
evolution of the levitation force (F=A/dγ) as a function of the interaction distance d are used to
characterize the effective response of the ceramics or composites to the magnetic flux penetration.
Some of the abnormal variations of the exponent ε and of the term "A" ( in F=A/dγ) could be reinterpreted
in terms of a change in superconducting regime. Other observed variations of γ should
be due to the variation of the effective field from the cylindrical magnet.
© EDP Sciences 1998