High Power Laser and Particle Beams, Volume. 36, Issue 1, 013013(2024)

Development of conduction-cold high temperature superconductingmagnet for high power microwave devices

Ce Xu1, Hui Liu1, Jianhua Liu1, Yinming Dai1, Shunzhong Chen1, Junsheng Cheng1, Qiuliang Wang1, Shaofei Huo2, Yanchao Shi2, and Huijie Huang2
Author Affiliations
  • 1Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences, Beijing 100190, China
  • 2Key Laboratory of Advanced High Power Microwave Technology, Northwest Institute of Nuclear Technology, Xi’an 710024, China
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    Figures & Tables(14)
    Composition and position of the HTS magnet modules
    Magnetic field distribution of the 4 T superconducting magnet
    Outer skeleton and tooling skeleton
    Configuration of the 4 T superconducting magnet system
    Configuration of tapered structure
    Stress cloud of superconducting magnet
    Cooling curves of the various parts of the magnet structure
    Voltage of the coil pancakes during the excitation process
    Voltage of the coil pancakes during the excitation stabilized process at operating temperature 48.9 K
    Field strength and current changes during excitation and demagnetization
    • Table 1. The Ic-B-θ-T characteristics curve of REBCO strip at 40 K and 50 K in vertical fields

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      Table 1. The Ic-B-θ-T characteristics curve of REBCO strip at 40 K and 50 K in vertical fields

      temperature/KIc/A
      00.5 T1.0 T1.5 T2.0 T2.5 T3.0 T3.5 T4.0 T4.5 T5.0 T5.5 T6.0 T6.5 T7.0 T
      40399.0241.8190.2170.1153.6140.4129.3122.1112.5105.999.093.087.683.478.6
      50296.7168.6135.9120.0106.296.088.881.975.669.664.560.056.151.648.6
    • Table 2. Thermal load of the cryostat

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      Table 2. Thermal load of the cryostat

      temperature/Kheat leakage of supports/Wheat leakage of current leads/Wradiation/Wradial resistance/Wjoint resistance/Wsum/W
      402.00.30.10.02510.03482.46
      775.28.015.0\\28.00
    • Table 3. Material property of each component of magnet

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      Table 3. Material property of each component of magnet

      No.materialtemperature/Kdensity/(g/cm3)Young’s modulus@300 K/GPaPoisson’s ratiocoefficient of linear expansion/(10−5 K−1)
      1PAI40~3001.66.40.431.0
      2AISI 30440/3007.9200.00.301.3
      31100 AL802.770.00.301.5
      4T2 Cu408.970.00.301.0
    • Table 4. Influence of random vibration of highway spectrum in three directions on the axis of magnet

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      Table 4. Influence of random vibration of highway spectrum in three directions on the axis of magnet

      axialityUx/mmUy/mmUz/mmUsum/mm
      y random vibrationp-axis deviation4.64E-042.09E-022.08E-042.08E-02
      s-axis deviation1.29E-032.02E-022.02E-042.03E-02
      z random vibrationp-axis deviation4.80E-05−1.52E-042.53E-022.53E-02
      s-axis deviation3.44E-041.80E-032.51E-022.52E-02
      x random vibrationp-axis deviation6.32E-032.34E-041.03E-056.32E-03
      s-axis deviation6.39E-032.73E-049.90E-066.40E-03
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    Ce Xu, Hui Liu, Jianhua Liu, Yinming Dai, Shunzhong Chen, Junsheng Cheng, Qiuliang Wang, Shaofei Huo, Yanchao Shi, Huijie Huang. Development of conduction-cold high temperature superconductingmagnet for high power microwave devices[J]. High Power Laser and Particle Beams, 2024, 36(1): 013013

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    Paper Information

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    Received: Jun. 15, 2023

    Accepted: Dec. 24, 2023

    Published Online: Mar. 21, 2024

    The Author Email:

    DOI:10.11884/HPLPB202436.230334

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