IEC 61788-3-2000
超导体 第3部分:临界电流测量 银-外膜铋-2212和铋-2223氧化物超导体的临界直流电流

Superconductivity - Part 3: Critical current measurement; DC critical current of Ag-sheathed Bi-2212 and Bi-2223 oxide superconductors


IEC 61788-3-2000 发布历史

This part of IEC 61788 covers a test method for the determination of the d.c. critical current of short and straight Ag- or Ag alloy-sheathed Bi-2212 and Bi-2223 oxide superconductors that have a monolithic structure and a shape of round wire or flat or square tape containing mono-or multicores of oxides. This method is intended for use with superconductors that have critical currents less than 500 A and n-values larger than 5. The test is carried out with and without applying external magnetic fields. In the test of the tape specimen in magnetic fields, the magnetic fields are parallel or perpendicular to the tape surface. The test specimen is immersed either in a liquid helium bath or a liquid nitrogen bath during testing. Deviations from this test method that are allowed for routine tests and other specific restrictions are given in this standard. Substantial parts of the test method covered in this standard are in common with, or similar to, those for Nb3Sn composite superconductors (IEC 61788-2). Special features newly found for oxide superconductors may be classified into two groups. The first group is specific to oxide composite superconductors, including mechanical fragility originating from the presence of weak links, cryogen gas bubble formation, aging degradation, magnetic flux flow and creep, large anisotropy, hysteresis in critical current with magnetic field sweep, etc. The second group is due to the short length of the specimen used in the standard. A critical current measurement on such a specimen may easily pick up different voltage signals due to thermal electromotive force, inductive voltage, thermal noise, current redistribution, specimen motion relative to the holder, etc. Current transfer voltages may be present due to the short distance from a current contact to a voltage tap. Short specimen length may reduce mechanical tolerance against the Lorentz force, for example, by promoting the formation of cryogen gas bubbles within the composite.

IEC 61788-3-2000由国际电工委员会 IX-IEC 发布于 2000-12。

IEC 61788-3-2000 在中国标准分类中归属于: L47 其他。

IEC 61788-3-2000的历代版本如下:

  • 2000年12月 IEC 61788-3-2000 超导体 第3部分:临界电流测量 银-外膜铋-2212和铋-2223氧化物超导体的临界直流电流
  • 2006年04月 IEC 61788-3-2006 超导性.第3部分:临界电流测量.银和/或银合金铠装的铋-2212和铋-2223氧化物超导体的临界直流电流

 

 

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标准号
IEC 61788-3-2000
发布日期
2000年12月
实施日期
废止日期
中国标准分类号
L47
发布单位
IX-IEC
代替标准
IEC 61788-3-2006
适用范围
This part of IEC 61788 covers a test method for the determination of the d.c. critical current of short and straight Ag- or Ag alloy-sheathed Bi-2212 and Bi-2223 oxide superconductors that have a monolithic structure and a shape of round wire or flat or square tape containing mono-or multicores of oxides. This method is intended for use with superconductors that have critical currents less than 500 A and n-values larger than 5. The test is carried out with and without applying external magnetic fields. In the test of the tape specimen in magnetic fields, the magnetic fields are parallel or perpendicular to the tape surface. The test specimen is immersed either in a liquid helium bath or a liquid nitrogen bath during testing. Deviations from this test method that are allowed for routine tests and other specific restrictions are given in this standard. Substantial parts of the test method covered in this standard are in common with, or similar to, those for Nb3Sn composite superconductors (IEC 61788-2). Special features newly found for oxide superconductors may be classified into two groups. The first group is specific to oxide composite superconductors, including mechanical fragility originating from the presence of weak links, cryogen gas bubble formation, aging degradation, magnetic flux flow and creep, large anisotropy, hysteresis in critical current with magnetic field sweep, etc. The second group is due to the short length of the specimen used in the standard. A critical current measurement on such a specimen may easily pick up different voltage signals due to thermal electromotive force, inductive voltage, thermal noise, current redistribution, specimen motion relative to the holder, etc. Current transfer voltages may be present due to the short distance from a current contact to a voltage tap. Short specimen length may reduce mechanical tolerance against the Lorentz force, for example, by promoting the formation of cryogen gas bubbles within the composite.

IEC 61788-3-2000系列标准

IEC 61788-1-2006 超导性.第1部分:临界电流测量.铌-钛复合超导体的临界直流电流 IEC 61788-10-2006 超导性.第10部分:临界温度测量.用电阻法对复合超导体的临界温度的测量 IEC 61788-11-2011 超导性.第11部分:剩余电阻率的测量.Nb3Sn复合超导体的剩余电阻率 IEC 61788-12-2013 超导性. 第12部分: 超导体基体的体积比测量. Nb3Sn复合超导导线的铜与非铜的体积比 IEC 61788-13-2012 超导性.第13部分:交流电损耗测量.多芯复合超导体磁滞损耗的磁强计法 IEC 61788-14-2010 超导性.第14部分:超导功率元件.设计用于超导功率元件的电流导线特性试验的一般要求 IEC 61788-15-2011 超导性.第15部分:电子特性测量.微波频率下超导薄膜的固有表面阻抗 IEC 61788-16-2013 超导性.第16部分:电气特性测量值.微波频率下超导体的功率依赖表面电阻 IEC 61788-17-2021 超导性. 第17部分: 电气特性测量值. 大面积超导薄膜的局部临界电流密度及其分布\r\n IEC 61788-18-2013 超导性.第18部分:机械特性测量.银和/或银合金护套的铋-2223和铋-2212复合超导体的室温拉伸试验 IEC 61788-19-2013 超导性.第19部分:机械性能的测量.起反应的Nb3Sn复合超导体的室温拉伸试验 IEC 61788-2-2006 超导性.第2部分:临界电流测量.Nb3Sn复合超导体的直流临界电流 IEC 61788-21-2015 超导性 - 第21部分:超导电线 - 实用超导电线的测试方法 - 一般特性和指导 IEC 61788-22-1-2017 超导电性 - 第22-1部分:超导电子器件 - 传感器和检测器的总规范 IEC 61788-22-2-2021 IEC 61788-23-2021 超导性.第23部分:剩余电阻比测量.腔级Nb超导体的剩余电阻比 IEC 61788-24-2018 超导性.第24部分:临界电流测量.银护套Bi-2223超导电线室温双弯后的保留临界电流 IEC 61788-25-2018 超导电性 - 第25部分:机械性能测量 - REBCO电线的室温拉伸试验 IEC 61788-26-2020 超导性第26部分:临界电流测量RE-Ba-Cu-O复合超导体的直流临界电流 IEC 61788-4-2020 超导性 - 第4部分:残余电阻率测量 - Nb-Ti和Nb3sn复合超导体的残余电阻比 IEC 61788-5-2013 超导体.第5部分:超导体体积比测量矩阵.铜对铜/铌-钛复合超导体的超导体体积比 IEC 61788-6-2011 超导体.第6部分:机械性能测量.铜/铌-钛复合超导体的室温拉伸试验 IEC 61788-7-2020 超导性.第7部分:电子特性测量.微波频率下高温超导体的表面电阻 IEC 61788-8-2010 超导性.第8部分:交流电损耗测量.用拾波线圈法在液氮温度下测量暴露于横向交流磁场中循环超导导线的交流电总损耗量 IEC 61788-9-2005 超导性.第9部分:成批高温超导体的测量.大粒氧化物超导体的陷波流量密度

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