首页> 外文期刊>IEEE Transactions on Applied Superconductivity >Critical-Current Measurements on an ITER Nb$_{3}$Sn Strand: Effect of Axial Tensile Strain
【24h】

Critical-Current Measurements on an ITER Nb$_{3}$Sn Strand: Effect of Axial Tensile Strain

机译:ITER Nb $ _ {3} $ Sn链上的临界电流测量:轴向拉伸应变的影响

获取原文
获取原文并翻译 | 示例
           

摘要

The dependence of transport critical current $(I_{rm c})$ on axial tensile strain $varepsilon$ was measured for a developmental ${rm Nb}_{3}{rm Sn}$ multifilamentary strand as a function of magnetic field $B$ between 12 T and 16 T, at the temperature of 4 K. This conductor was from the first stage of strand pre-production for the central solenoid of the International Thermonuclear Experimental Reactor (ITER) project. Straight samples were measured with a stress-free-cooling strain apparatus. The compressive pre-strain $varepsilon_{max}$ and the irreversible strain limit $varepsilon_{rm irr}$ were 0.19% and 0.8%, respectively; and the ultimate strain where the wire physically broke was about 0.95%. The pinning force $F_{rm p}(=I_{rm c} times B)$ was proportional to $(B_{{rm c}2}^{ast})^{rm s}b^{p}(1-b)^{q}$, where $b=B/B_{{rm c}2}^{ast}$ is the reduced magnetic field, and the scaling constants had values $p=0.58$, $q=1.86$, and $s=0.7$. The strain dependence of the effective upper critical field $B_{{rm c}2}^{ast}$ (the field at which $F_{rm p}$ extrapolates to zero) was well described within the measured strain range by $B_{{rm c}2max}^{ast}[1-avertvarepsilon-varepsilon_{max}vert^{u}]$ , where $B_{{rm c}2}^{ast}max$ is the maximum value of $B_{{rm c}2}^{ast}$ as a function of strain, $u=1.7$, and $a$ was about 1230 for the compressive strains and 1670 for the tensile strains. Ekin''s strain scaling law was applied to calculate the strain sensitivity of $I_{c}$ at various intrinsic strains between $-$0.5% and 0.5%, and magnetic fields from 12 T to 16 T.
机译:测量了发育的$ {rm Nb} _ {3} {rm Sn} $复丝股线的传输临界电流$(I_ {rm c})$对轴向拉伸应变$ varepsilon $的依赖性与磁场$的关系B $介于12 T和16 T之间,温度为4K。该导体来自国际热核实验堆(ITER)项目中央螺线管预生产的第一阶段。用无应力冷却应变仪测量直样品。压缩预应变$ varepsilon_ {max} $和不可逆应变极限$ varepsilon_ {rm irr} $分别为0.19%和0.8%;导线物理断裂的极限应变约为0.95%。钉扎力$ F_ {rm p}(= I_ {rm c}乘以B)$与$(B _ {{rm c} 2} ^ {ast})^ {rm s} b ^ {p}(1 -b)^ {q} $,其中$ b = B / B _ {{rm c} 2} ^ {ast} $是减小的磁场,并且缩放常数的值是$ p = 0.58 $,$ q = 1.86 $,而$ s = 0.7 $。有效上临界场$ B _ {{rm c} 2} ^ {ast} $($ F_ {rm p} $外推至零的场)的应变依赖性在测量的应变范围内由$ B_很好地描述了{{rm c} 2max} ^ {ast} [1-avertvarepsilon-varepsilon_ {max} vert ^ {u}] $,其中$ B _ {{rm c} 2} ^ {ast} max $是$的最大值B _ {{rm c} 2} ^ {ast} $作为应变的函数,$ u = 1.7 $,对于压缩应变,$ a $大约为1230,对于拉伸应变为$ 1670。应用Ekin的应变缩放定律,计算在$-$ 0.5%和0.5%之间的各种固有应变以及12 T至16 T的磁场下$ I_ {c} $的应变敏感性。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号