We have experimentally studied the magnetic shielding properties of a cylindrical shell of BiPbSrCaCuO subjected to low frequency AC axial magnetic fields. The magnetic response has been investigated as a function of the dimensions of the tube, the magnitude of the applied field and the frequency. These results are explained quantitatively by employing the method of Brandt ( 1998 Phys. Rev. B 58 6506) with a Jc( B) law appropriate for a polycrystalline material. Specifically, we observe that the applied field can sweep into the central region either through the thickness of the shield or through the opening ends, the latter mechanism being suppressed for long tubes. For the first time, we systematically detail the spatial variation of the shielding factor ( the ratio of the applied field over the internal magnetic field) along the axis of a high-temperature superconducting tube. The shielding factor is shown to be constant in a region around the centre of the tube, and to decrease as an exponential in the vicinity of the ends. This spatial dependence comes from the competition between two mechanisms of field penetration. The frequency dependence of the shielding factor is also discussed and shown to follow a power law arising from the finite creep exponent n.
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机译:我们已经通过实验研究了BiPbSrCaCuO圆柱壳在低频交流轴向磁场下的磁屏蔽性能。已经根据管的尺寸,所施加的场的大小和频率对磁响应进行了研究。这些结果通过采用Brandt(1998 Phys。Rev. B 58 6506)方法和适用于多晶材料的Jc(B)定律定量解释。具体而言,我们观察到,施加的电场可以通过屏蔽层的厚度或通过开口端扫入中心区域,对于长管,后者的机制受到抑制。我们第一次系统地详细说明了屏蔽系数(高温磁场与磁场的比例)沿高温超导管轴的空间变化。屏蔽系数在管的中心附近区域是恒定的,并且在端部附近呈指数下降。这种空间依赖性来自两种场穿透机制之间的竞争。还讨论了屏蔽因数的频率相关性,并表明它遵循由有限蠕变指数n引起的幂定律。
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