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Simulations of the effects of tin composition gradients on the superconducting properties of Nb3Sn conductors

机译:锡组成梯度对Nb3Sn导体超导性能影响的模拟

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In powder-in-tube Nb3Sn composites, the A15 phase forms between a central tin-rich core and a coaxial Nb tube, thus causing the tin content and superconducting properties to vary with radius across the A15 layer. Since this geometry is also ideal for magnetic characterization of the superconducting properties with the field parallel to the tube axis, a system of concentric shells with varying tin content was used to simulate the superconducting properties, the overall severity of the Sn composition gradient being defined by an index N. Using well-known scaling relationships and property trends developed in an earlier experimental study, the critical current density for each shell was calculated, and from this the magnetic moment of each shell was found. By summing these moments, experimentally measured properties such as pinning-force curves and Kramer plots could be simulated. We found that different tin profiles have only a minor effect on the shape of Kramer plots, but a pronounced effect on the irreversibility fields defined by the extrapolation of Kramer plots. In fact, these extrapolated values H-K are very close to a weighted average of the superconducting properties across the layer for all N. The difference between H-K and the upper critical field commonly seen in experiments is a direct consequence of the different ways measurements probe the simulated Sn gradients. Sn gradients were found to be significantly deleterious to the critical current density J(c), since reductions to both the elementary pinning force and the flux pinning scaling field H-K compound the reduction in J(c). The simulations show that significant gains in J(c) of Nb3Sn strands might be realized by circumventing strong compositional gradients of tin. (C) 2004 American Institute of Physics.
机译:在管中粉末Nb3Sn复合材料中,中心富锡核心与同轴Nb管之间形成A15相,从而导致锡含量和超导性能随整个A15层的半径而变化。由于这种几何形状也是磁场平行于管轴的超导特性的磁性表征的理想选择,因此使用具有不同锡含量的同心壳系统来模拟超导特性,Sn组成梯度的总体严重性由下式定义:使用早期实验研究中开发的众所周知的比例关系和特性趋势,计算出每个壳体的临界电流密度,并由此得出每个壳体的磁矩。通过将这些力矩相加,可以模拟实验测量的特性,例如钉扎力曲线和Kramer图。我们发现,不同的锡分布对Kramer图的形状影响不大,但对通过Kramer图外推法定义的不可逆性场具有显着影响。实际上,这些外推值HK非常接近所有N层中超导特性的加权平均值。实验中常见的HK和上临界场之间的差异是测量方法探测模拟的不同方式的直接结果。锡梯度。由于基本钉扎力和磁通钉扎定标场H-K的减小都增加了J(c)的减小,因此Sn梯度对临界电流密度J(c)明显有害。模拟表明,可以通过规避锡的强成分梯度来实现Nb3Sn链J(c)的显着增加。 (C)2004美国物理研究所。

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