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Properties of Long GdBCO Coated Conductor by IBAD-PLD Method—The First GdBCO Coil Test

机译:IBAD-PLD方法对长GdBCO涂层导体的性能进行的首次GdBCO线圈测试

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We have developed the first ${rm GdBa}_{2}{rm Cu}_{3}{rm O}_{7-{rm x}}$ (GdBCO) coil using a 53.5 m long GdBCO coated conductor with a high end-to-end critical current $(I_{rm c})$ of 183 A. The coil was a 4 turns—84.5 layers (4 $times$ 84.5) solenoid type coil with the dimensions of 28 mm in bore diameter, 30 mm in inner diameter, 70.9 mm in outer diameter, and 44.3 mm in height. The obtained central magnetic fields $(B_{0})$ were 1.19 T and 0.48 T when the operating coil currents $(I_{rm op})$ were 184.8 A and 74.2 A at 64 K and 77 K, respectively. The measured $B_{0}$ were in good agreement with the calculated $B_{0}$. The $I_{rm op}$ corresponded to the $I_{rm c}$ of the conductor at the edge of the coil in the middle layer, where the magnetic field direction was around 45 degrees to the c-axis of the GdBCO layer. This is due to the fact that the GdBCO coated conductor exhibits a minimum of $I_{rm c}$ for these magnetic field directions. Therefore, the magnetic field of the coil was determined by the intersection of the coil load line for this part to the magnetic field dependence of critical current $(I_{rm c}-B)$ curve for the conductor in this direction. Since GdBCO coated conductor exhibits superior magnetic field dependence of critical current density $(J_{rm c}-B)$ property to that of ${-rm YBa}_{2}{rm Cu}_{3}{rm O}_{7-{rm x}}$ (YBCO) coated conductor, the GdBCO coil can generate a high magnetic field compared with the coil made from the YBCO coated conductor. If the above GdBCO coated conductor in the coil is substituted by a YBCO coated conductor, the length of the conductor would be about 1.6 times longer than the present GdBCO coated conductor. For practical application, the GdBCO coated conductor is more promising than the conventional YBCO coated conductor.
机译:我们开发了第一个$ {rm GdBa} _ {2} {rm Cu} _ {3} {rm O} _ {7- {rm x}} $(GdBCO)线圈,使用的是53.5 m长的GdBCO涂层导体,带有一个端到端的最高临界电流$(I_ {rm c})$为183A。线圈为4匝-84.5层(4乘以$ 84.5)螺线管型线圈,内径尺寸为28 mm,内径为30毫米,外径为70.9毫米,高度为44.3毫米。当工作线圈电流$(I_ {rm op})$在64 K和77 K时分别为184.8 A和74.2 A时,获得的中心磁场$(B_ {0})$为1.19 T和0.48T。测得的$ B_ {0} $与计算出的$ B_ {0} $非常一致。 $ I_ {rm op} $对应于中间层线圈边缘处导体的$ I_ {rm c} $,磁场方向与GdBCO层的c轴成45度角。这是由于以下事实:对于这些磁场方向,GdBCO涂层的导体表现出的最小值为$ I_ {rm c} $。因此,线圈的磁场由该部分的线圈负载线与导体在该方向上的临界电流$(I_ {rm c} -B)$曲线的磁场依赖性决定。由于涂覆GdBCO的导体对临界电流密度$(J_ {rm c} -B)$的性能表现出优于$ {-rm YBa} _ {2} {rm Cu} _ {3} {rm O}的磁场依赖性。 _ {7- {rm x}} $(YBCO)涂层导体,与由YBCO涂层导体制成的线圈相比,GdBCO线圈可以产生高磁场。如果线圈中的上述GdBCO涂层导体被YBCO涂层导体代替,则导体的长度将比当前的GdBCO涂层导体长约1.6倍。对于实际应用,GdBCO涂层导体比传统的YBCO涂层导体更有前景。

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