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Kiloampere, Variable-Temperature, Critical-Current Measurements of High-Field Superconductors

机译:高场超导体的千安培,可变温度,临界电流测量

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We review variable-temperature, transport critical-current (I_c) measurements made on commercial superconductors over a range of critical currents from less than 0.1 A to about 1 kA. We have developed and used a number of systems to make these measurements over the last 15 years. Two exemplary variable-temperature systems with coil sample geometries will be described: a probe that is only variable-temperature and a probe that is variable-temperature and variable-strain. The most significant challenge for these measurements is temperature stability, since large amounts of heat can be generated by the flow of high current through the resistive sample fixture. Therefore, a significant portion of this review is focused on the reduction of temperature errors to less than ±0.05 K in such measurements. A key feature of our system is a pre-regulator that converts a flow of liquid helium to gas and heats the gas to a temperature close to the target sample temperature. The pre-regulator is not in close proximity to the sample and it is controlled independently of the sample temperature. This allows us to independently control the total cooling power, and thereby fine tune the sample cooling power at any sample temperature. The same general temperature-control philosophy is used in all of our variable-temperature systems, but the addition of another variable, such as strain, forces compromises in design and results in some differences in operation and protocol. These aspects are analyzed to assess the extent to which the protocols for our systems might be generalized to other systems at other laboratories. Our approach to variable-temperature measurements is also placed in the general context of measurement-system design, and the perceived advantages and disadvantages of design choices are presented. To verify the accuracy of the variable-temperature measurements, we compared critical-current values obtained on a specimen immersed in liquid helium ("liquid" or I_(c liq)) at 5 K to those measured on the same specimen in flowing helium gas ("gas" or I_(c gas)) at the same temperature. These comparisons indicate the temperature control is effective over the superconducting wire length between the voltage taps, and this condition is valid for all types of sample investigated, including Nb-Ti, Nb_3Sn, and MgB_2 wires. The liquid/gas comparisons are used to study the variable-temperature measurement protocol that was necessary to obtain the "correct" critical current, which was assumed to be the I_(c liq). We also calibrated the magnetoresistance effect of resistive thermometers for temperatures from 4 K to 35 K and magnetic fields from 0 T to 16 T. This calibration reduces systematic errors in the variable-temperature data, but it does not affect the liquid/gas comparison since the same thermometers are used in both cases.
机译:我们回顾了在小于0.1 A至大约1 kA的临界电流范围内在商用超导体上进行的可变温度,传输临界电流(I_c)测量。在过去的15年中,我们已经开发并使用了许多系统来进行这些测量。将描述具有线圈样品几何形状的两个示例性可变温度系统:仅可变温度的探针和可变温度和可变应变的探针。这些测量面临的最大挑战是温度稳定性,因为流过电阻式样品夹具的高电流会产生大量热量。因此,本次审查的主要内容集中在将此类测量的温度误差降低到±0.05 K以下。我们系统的关键特征是预调节器,它可以将液氦流转化为气体,并将气体加热到接近目标样品温度的温度。预调节器并不紧邻样品,并且不受样品温度的影响。这使我们能够独立控制总冷却功率,从而在任何样品温度下微调样品冷却功率。我们所有的可变温度系统都使用相同的通用温度控制原理,但是增加了另一个变量(例如应变),会影响设计,并导致操作和协议上的某些差异。对这些方面进行了分析,以评估我们系统的协议在多大程度上可以推广到其他实验室的其他系统。我们在可变温度测量中的方法也被放置在测量系统设计的一般环境中,并提出了设计选择的优缺点。为了验证可变温度测量的准确性,我们比较了在5 K下浸入液氦(“液体”或I_(c liq))中的样品所获得的临界电流值与在流动氦气中在同一样品上所获得的临界电流值(“气体”或I_(c气体))在相同温度下。这些比较表明,温度控制在电压抽头之间的超导线长上是有效的,并且该条件对于所有类型的研究样本均有效,包括Nb-Ti,Nb_3Sn和MgB_2导线。液/气比较用于研究可变温度测量协议,该协议是获得“正确”临界电流所必需的,假定该临界电流为I_(c liq)。我们还校准了温度从4 K到35 K以及磁场从0 T到16 T的电阻温度计的磁阻效应。这种校准减少了可变温度数据中的系统误差,但是由于它不影响液/气比较,因此两种情况下使用相同的温度计。

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