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The measurement of current distribution in superconducting tape. Comparison of destructive and non-destructive methods

机译:超导带中电流分布的测量。破坏性方法与非破坏性方法的比较

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The question whether the current in superconducting tapes flows homogeneously or is distributed in some way across the width, between its edges, can be answered in several ways. If we are interested in the critical current distribution only, the destructive method can be applied. The tape can be cut longitudinally into several sub-tapes and the critical current can be measured in each sub-tape. The principle of the method is trivial and straightforward. Other modifications of destructive method exist, e.g. gradual brushing of the tape from one side and looking for a change in the overall critical current in the rest of the tape. The disadvantage of both methods is rough mechanical interaction with the tape, which can-modify its transport properties and inability to repeat measurements on the same piece of initial sample after changing some of the external parameters. The magnetic knife method is an example of a nondestructive approach. Still it is from principle limited to the critical current distribution only. Current distribution in general, without limitation to the critical one, can be achieved by measuring the self-magnetic-field of the tape and solving the inverse problem for corresponding current distribution. An improved, unique procedure of calculation is described here in detail. The results for special case of current equal to the critical current, i.e. the critical current distribution across the tape width, are compared with the results of the destructive method applied on the same tape. The possibility to check the method by making comparison is the only reason for limitation to (zero field) critical current. Any current distribution, at any phase of the tape transport current during AC cycle, can be determined by the non-destructive method. As an example, frozen currents distribution, after ramping transport current up to I. and afterwards down to zero current, are shown. (C) 2002 Elsevier Science'B.V. All rights reserved. [References: 12]
机译:超导带中的电流是均匀流动还是以某种方式在其边缘之间的宽度上分布,这一问题可以通过几种方式回答。如果仅对临界电流分布感兴趣,则可以应用破坏性方法。可以将胶带纵向切成几个子胶带,并可以在每个子胶带中测量临界电流。该方法的原理是简单而直接的。存在破坏性方法的其他修改,例如从一侧逐渐刷带,并寻找其余部分的总体临界电流的变化。两种方法的缺点是与磁带的机械相互作用较粗糙,这会改变其传输性能,并且在更改某些外部参数后无法在同一块初始样品上重复测量。电磁刀法是非破坏性方法的一个示例。从原理上讲,它仍然仅限于临界电流分布。通常,可以通过测量磁带的自磁场并解决对应电流分布的反问题来获得电流分布,而并不局限于临界电流。这里详细描述了一种改进的独特计算过程。将电流等于临界电流的特殊情况下的结果,即磁带宽度上的临界电流分布,与应用于同一磁带的破坏性方法的结果进行比较。通过比较来检查该方法的可能性是限制(零场)临界电流的唯一原因。可以通过非破坏性方法确定在AC循环期间磁带传输电流的任何相位上的任何电流分布。作为示例,示出了在使传输电流上升至I.然后下降至零电流之后的冻结电流分布。 (C)2002 Elsevier Science'B.V。版权所有。 [参考:12]

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