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Shielding efficiency and E(J) characteristics measured on large melt cast Bi-2212 hollow cylinders in axial magnetic fields

机译:在轴向磁场下在大型熔铸Bi-2212空心圆柱体上测得的屏蔽效率和E(J)特性

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摘要

We show that tubes of melt cast Bi-2212 used as current leads for LTS magnets canalso act as efficient magnetic shields. The magnetic screening properties under an axialDC magnetic field are characterized at several temperatures below the liquid nitrogentemperature (77 K). Two main shielding properties are studied and compared withthose of Bi-2223, a material that has been considered in the past for bulk magneticshields. The first property is related to the maximum magnetic flux density that canbe screened, Blim; it is defined as the applied magnetic flux density below which thefield attenuation measured at the centre of the shield exceeds 1000. For a cylinder ofBi-2212 with a wall thickness of 5 mm and a large ratio of length over radius, Blim isevaluated to 1 T at T = 10 K. This value largely exceeds the Blim value measured atthe same temperature on similar tubes of Bi-2223. The second shielding property thatis characterized is the dependence of Blim with respect to variations of the sweep rate ofthe applied field, dBapp/dt. This dependence is interpreted in terms of the power lawE = Ec(J/Jc)^n and allows us to determine the exponent n of this E(J) characteristicsfor Bi-2212. The characterization of the magnetic field relaxation involves very smallvalues of the electric field. This gives us the opportunity to experimentally determinethe E(J) law in an unexplored region of small electric fields. Combining these resultswith transport and AC shielding measurements, we construct a piecewise E(J) lawthat spans over 8 orders of magnitude of the electric field.
机译:我们证明了用作LTS磁体电流引线的Bi-2212熔铸管也可以用作有效的磁屏蔽。在低于液氮温度(77 K)的几个温度下表征了轴向DC磁场下的磁屏蔽性能。研究了两种主要的屏蔽性能,并将其与Bi-2223的屏蔽性能进行了比较,Bi-2223是过去用于体磁屏蔽的材料。第一个特性与可以筛选的最大磁通密度Blim有关;它被定义为所施加的磁通密度,在此密度以下,在屏蔽层中心测得的场衰减超过1000。对于壁厚5 mm,长度与半径之比大的Bi-2212圆柱,Blim评估为1 T在T = 10 K时。该值大大超过了在相同温度下在Bi-2223的类似管上测得的Blim值。表征的第二屏蔽特性是Blim与施加场的扫频速率dBapp / dt的关系。这种依赖关系根据幂定律E = Ec(J / Jc)^ n进行解释,并允许我们确定Bi-2212的此E(J)特性的指数n。磁场弛豫的表征涉及非常小的电场值。这使我们有机会在小电场的未探索区域中通过实验确定E(J)定律。将这些结果与传输和交流屏蔽测量相结合,我们构建了跨越8个数量级电场的分段E(J)定律。

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