TY - JOUR
T1 - Comparison of Magnetizing Characteristics of Superconducting Bulk Magnet Cooled by Stirling and GM Refrigerators During Pulsed Field Magnetization
AU - Yokoyama, Kazuya
AU - Katsuki, Atsushi
AU - Miura, Atsuro
AU - Oka, Tetsuo
N1 - Funding Information:
Manuscript received September 17, 2017; accepted December 20, 2017. Date of publication January 11, 2018; date of current version January 26, 2018. This work was supported by the JSPS KAKENHI under Grant JP15K05951. (Corresponding author: Kazuya Yokoyama.) K. Yokoyama is with the Division of Electrical and Electronic Engineering, Ashikaga Institute of Technology, Ashikaga 326-8558, Japan (e-mail: k-yokoyama@ashitech.ac.jp).
Publisher Copyright:
© 2018 IEEE.
PY - 2018/6
Y1 - 2018/6
N2 - We developed several type superconducting bulk magnets with the goal of their industrial application, and study to improve a magnetic field by pulsed field magnetization. It is important to select a suitable refrigerator to cool a bulk superconductor. This paper investigates magnetizing characteristics when using different refrigerators. One is a Stirling refrigerator, in which an ultimate temperature was up to 50 K and cooling capacity was 11 W at 77 K. Another is a dual-stage GM refrigerator with an air-cooled compressor, in which an ultimate temperature was 13 K and cooling capacity was 5 W at 20 K. The other is a dual-stage GM refrigerator with a water-cooled compressor, in which an ultimate temperature was 12 K and cooling capacity was 12 W at 20 K. When a GdBCO bulk with dimensions of 60 mm in diameter and 20 mm thick was cooled by the Stirling refrigerator, the lowest temperature was approximately 55 K. Then, in the other refrigerators, the temperature was adjusted to the same value by a temperature regulator. The bulk was cooled by each refrigerator and a single pulsed field was applied while varying the amplitude of 3.1 to 7.0 T. During magnetization, time variations of magnetic flux density on the bulk surface were monitored. After magnetization, the trapped field distributions were measured on the magnetic pole surface. These data show that even the bulk magnet using the Stirling refrigerator with relatively low cooling ability could trap a high magnetic field. Consequently, the bulk magnet with high cooling capacity could not necessarily generate a high magnetic field.
AB - We developed several type superconducting bulk magnets with the goal of their industrial application, and study to improve a magnetic field by pulsed field magnetization. It is important to select a suitable refrigerator to cool a bulk superconductor. This paper investigates magnetizing characteristics when using different refrigerators. One is a Stirling refrigerator, in which an ultimate temperature was up to 50 K and cooling capacity was 11 W at 77 K. Another is a dual-stage GM refrigerator with an air-cooled compressor, in which an ultimate temperature was 13 K and cooling capacity was 5 W at 20 K. The other is a dual-stage GM refrigerator with a water-cooled compressor, in which an ultimate temperature was 12 K and cooling capacity was 12 W at 20 K. When a GdBCO bulk with dimensions of 60 mm in diameter and 20 mm thick was cooled by the Stirling refrigerator, the lowest temperature was approximately 55 K. Then, in the other refrigerators, the temperature was adjusted to the same value by a temperature regulator. The bulk was cooled by each refrigerator and a single pulsed field was applied while varying the amplitude of 3.1 to 7.0 T. During magnetization, time variations of magnetic flux density on the bulk surface were monitored. After magnetization, the trapped field distributions were measured on the magnetic pole surface. These data show that even the bulk magnet using the Stirling refrigerator with relatively low cooling ability could trap a high magnetic field. Consequently, the bulk magnet with high cooling capacity could not necessarily generate a high magnetic field.
KW - Superconducting bulk magnet
KW - cooling capacity
KW - magnetic flux density
KW - pulsed field magnetization
KW - refrigerator
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U2 - 10.1109/TASC.2018.2791993
DO - 10.1109/TASC.2018.2791993
M3 - Article
AN - SCOPUS:85041281696
SN - 1051-8223
VL - 28
JO - IEEE Transactions on Applied Superconductivity
JF - IEEE Transactions on Applied Superconductivity
IS - 4
M1 - 8253890
ER -