In the present work, the harmonic magnetic susceptibilities of the high-T c superconductors are examined and corresponding harmonic susceptibilities are calculated employing a model by Kim and coworkers. According to Kim's model, the critical-current density, J c is a function of the internal magnetic fieldwhere k and H o are constants. In the model calculations, full penetrations field, H p , is taken to beAs a result of the comparison of model calculations with experiments, we conclude that the harmonic susceptibilities for lower p values (p <10) correspond to the similar characteristic magnetic behaviour of granular superconductors, while the harmonic susceptibilities for higher p values correspond to the behaviour of homogeneous superconductors such as single crystal or samples with contiguous oriented grains.
We have carried out low-field ac measurements of harmonic susceptibilities and ac magnetization of a single-phase partially melt-textured Bi 2 Sr 2 CaCu 2 O 8 high-temperature superconductor over a wide range of temperatures, field amplitudes and measuring frequencies. Both the fundamental and third-harmonic susceptibility versus temperature and ac magnetization at fixed temperatures close to T c exhibit strong ac field amplitude and small frequency dependences. In the third-harmonic susceptibility, we observed a double-peak feature in the vicinity of T c as a function of the applied ac field. This strong field dependence is associated with depinning of vortices at some B and T in different superconducting matrices, which involves different ac loss mechanisms. Experimental results are compared with predictions of some existing theoretical models.
The interaction forces between a permanent disk and a superconductor disk are calculated for a cylindrical system by using the Anderson-Kim model. Model calculations show that both the vertical force and the stability exhibit a peak-like behavior in the repulsive branch. These peaks in the calculations are dependent on the model parameter and the ratio between the penetration and the applied fields, H p /H m . The features of hysteretic force and magnetic stiffness are discussed.
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