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Transport AC loss measurements in single- and two-layer parallel coated conductor arrays with low turn numbers. IEEE Trans Appl Supercond 2012; 22(6):8200306."}]}],"tabList":[{"magId":"2ecab0a8-a606-44c0-8365-b2c2172e6f33","titleEn":"Table 1. Modelling parameters for a single phase in the 1 MVA transformer.","labelEn":"Table 1.","id":"T1","table":"
LV HV
Inner diameter of winding (mm) 310 345
Width of the conductor (mm) 12.1 4
Thickness of the conductor (mm) 0.8 0.22
Turn number in x direction 20 48
Turn number in z direction 1 19
Total turn number 20 912
Number of Roebel strand 15 −
Width of Roebel strand (mm) 5 −
Gap between Roebel stacks (mm) 2.1 −
Axial gap between turns, dts (mm) 2.1 2.13
Constant critical current, Ic (A) 2226 118.7
Amplitude of the rated current (A) 1964 42.9
","captionEn":"

Modelling parameters for a single phase in the 1 MVA transformer.

"},{"magId":"c10218fc-8df4-47b5-8d6e-20235717d15b","titleEn":"Table 2. Magnetic field dependence parameters and n values for the transformer windings.","labelEn":"Table 2.","id":"T2","table":"
Parameters LV HV
Jc0 (A/m2) 3.55 × 1010 2.12 × 1010
B0 (mT) 149 149
α 0.6 0.6
n 19 17
","captionEn":"

Magnetic field dependence parameters and n values for the transformer windings.

"},{"magId":"37459889-0488-48c6-a73f-49a3b9b714b8","titleEn":"Table 3. Design parameters of the three-limb iron core.","labelEn":"Table 3.","id":"T3","table":"
Iron core
Type Three-phase three-limbs
Diameter (mm) 225
Window height (mm) 910
Center distance between limbs (mm) 590
Effective sectional area (cm2) 350.6
Material Grain-oriented silicon steel
Flux density (T) 1.54
","captionEn":"

Design parameters of the three-limb iron core.

"},{"magId":"10a883e6-b312-4ee5-837d-541edce37436","titleEn":"Table 4. FD parameters used in different combinations for the 1 MVA transformer.","labelEn":"Table 4.","id":"T4","table":"
Parameter Combination 1 (FDs_C1) Combination 2 (FDs_C2)
WHV (mm) 8.18 8.18
HHV (mm) 8.18 8.18
We, HV (mm) 2 2
gHV (mm) 2 2
WLV (mm) 4.8 12.8
HLV (mm) 4.8 4.8
We, LV (mm) 2 6
gLV (mm) 2 2
","captionEn":"

FD parameters used in different combinations for the 1 MVA transformer.

"},{"magId":"1942834c-d13a-4cee-a7d7-5d7c3b76fbbd","titleEn":"Table 5. FD parameters used for the stand-alone LV winding.","labelEn":"Table 5.","id":"T5","table":"
Parameter FDs_1 FDs_2
WLV (mm) 4.8 12.8
HLV (mm) 4.8 4.8
We, LV (mm) 2 6
gLV (mm) 2 2
","captionEn":"

FD parameters used for the stand-alone LV winding.

"},{"magId":"2f12e9e0-80b7-4af1-93ef-2949c8680199","titleEn":"Table 6. Loss values of the stand-alone LV winding with the iron core and different FDs at Irated.","labelEn":"Table 6.","id":"T6","table":"
Stand-alone LV winding
Cases WIC WIC_FDs_1 WIC_FDs_2
Values (W) 354.1 296.5 234.5
","captionEn":"

Loss values of the stand-alone LV winding with the iron core and different FDs at Irated.

"},{"magId":"f811255e-cc7a-4acf-bd5c-7ab572bbc9b2","titleEn":"Table 7. Loss values of phase B with the iron core and different FDs at Irated.","labelEn":"Table 7.","id":"T7","table":"
Phase B
Cases WIC WIC_FDs_C1 WIC_FDs_C2
Values (W) 85.9 69 61.7
","captionEn":"

Loss values of phase B with the iron core and different FDs at Irated.

"}],"journal":{"issn":"2772-8307","qiKanWangZhi":"//www.sghhindu.com/www.qk/supercon","qiKanMingCheng_CN":"Superconductivity","id":27,"qiKanMingCheng_EN":"Superconductivity"},"authorList":[{"deceased":false,"xref":"a, b","name_cn":"Yue Wu","xref_en":"a, b","name_en":"Yue Wu"},{"deceased":false,"xref":"b","name_cn":"Shuangrong You","xref_en":"b","name_en":"Shuangrong You"},{"deceased":false,"xref":"a, *","name_cn":"Jin Fang","email":"jfang@bjtu.edu.cn","xref_en":"a, *","name_en":"Jin Fang"},{"deceased":false,"xref":"b","name_cn":"Rodney A. Badcock","xref_en":"b","name_en":"Rodney A. Badcock"},{"deceased":false,"xref":"b","name_cn":"Nicholas J. Long","xref_en":"b","name_en":"Nicholas J. Long"},{"deceased":false,"xref":"b, *","name_cn":"Zhenan Jiang","email":"zhenan.jiang@vuw.ac.nz","xref_en":"b, *","name_en":"Zhenan Jiang"}],"affList_en":["aSchool of Electrical Engineering, Beijing Jiaotong University, Beijing, China","bPaihau-Robinson Research Institute, Victoria University of Wellington, Wellington, New Zealand"],"authorNotes_en":["* E-mail addresses: jfang@bjtu.edu.cn (J. Fang),","zhenan.jiang@vuw.ac.nz (Z. Jiang)."],"figList":[{"magId":"d9d2e0da-4bd6-4868-a955-ddd4f85cc581","pptUrl":"2772-8307-10-0-100095/img_1.png.ppt","labelEn":"Fig. 1.","figUrl":"2772-8307-10-0-100095/img_1.png","titleEn":"Fig. 1. The prototype of the 3-phase HTS 1 MVA 11 kV/415 V transformer: (a) the layout of the HTS transformer, (b) low voltage (LV) winding, and (c) high voltage (HV) winding.","id":"F1","captionEn":"The prototype of the 3-phase HTS 1 MVA 11 kV/415 V transformer: (a) the layout of the HTS transformer, (b) low voltage (LV) winding, and (c) high voltage (HV) winding. ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_1.png"},{"magId":"ad7e67a2-17b7-4a30-92b8-0e7f22f07871","pptUrl":"2772-8307-10-0-100095/img_2.png.ppt","labelEn":"Fig. 2.","figUrl":"2772-8307-10-0-100095/img_2.png","titleEn":"Fig. 2. Schematic of the HTS 1 MVA transformer consisting of 3-phase HV and LV windings and a three-limb iron core.","id":"F2","captionEn":"Schematic of the HTS 1 MVA transformer consisting of 3-phase HV and LV windings and a three-limb iron core. ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_2.png"},{"magId":"97d81554-9887-45d4-9a35-e81a9f37e542","pptUrl":"2772-8307-10-0-100095/img_3.png.ppt","labelEn":"Fig. 3.","figUrl":"2772-8307-10-0-100095/img_3.png","titleEn":"Fig. 3. B-H curves of silicon steel GO 3423 and 3411 used in iron cores.","id":"F3","captionEn":"<i>B</i>-<i>H</i> curves of silicon steel GO 3423 and 3411 used in iron cores. ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_3.png"},{"magId":"c9d343e4-0eb7-4b29-bd0e-6f4cbfc40d69","pptUrl":"2772-8307-10-0-100095/img_4.png.ppt","labelEn":"Fig. 4.","figUrl":"2772-8307-10-0-100095/img_4.png","titleEn":"Fig. 4. B-H curve of alloy powder core Hiflux 60 mu employed in flux diverters.","id":"F4","captionEn":"<i>B</i>-<i>H</i> curve of alloy powder core Hiflux 60 mu employed in flux diverters. ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_4.png"},{"magId":"7540c7fa-70c5-4bb8-bea7-9a751e126a9e","pptUrl":"2772-8307-10-0-100095/img_5.png.ppt","labelEn":"Fig. 5.","figUrl":"2772-8307-10-0-100095/img_5.png","titleEn":"Fig. 5. Measured hysteresis loss of Highflux 60 mu at 77 K.","id":"F5","captionEn":"Measured hysteresis loss of Highflux 60 mu at 77 K. ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_5.png"},{"magId":"8615694c-673e-4453-b935-d09d497c5204","pptUrl":"2772-8307-10-0-100095/img_6.png.ppt","labelEn":"Fig. 6.","figUrl":"2772-8307-10-0-100095/img_6.png","titleEn":"Fig. 6. Boundaries of the homogenous bulk.","id":"F6","captionEn":"Boundaries of the homogenous bulk. ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_6.png"},{"magId":"980e3702-37c0-4267-80c8-22264b059bde","pptUrl":"2772-8307-10-0-100095/img_7.png.ppt","labelEn":"Fig. 7.","figUrl":"2772-8307-10-0-100095/img_7.png","titleEn":"Fig. 7. Structured meshes for a quarter model of the single-phase transformer windings (upper half): (a) meshes for the model, (b) meshes for the transformer windings, presented in an enlarged view.","id":"F7","captionEn":"Structured meshes for a quarter model of the single-phase transformer windings (upper half): (a) meshes for the model, (b) meshes for the transformer windings, presented in an enlarged view. ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_7.png"},{"magId":"609a8f4b-aa4f-4629-89c4-10772cb6310d","pptUrl":"2772-8307-10-0-100095/img_8.png.ppt","labelEn":"Fig. 8.","figUrl":"2772-8307-10-0-100095/img_8.png","titleEn":"Fig. 8. Comparison of the simulated results in a single-phase transformer (TX) winding without the iron core with its experimental data (f = 50 Hz). WOIC stands for without the iron core.","id":"F8","captionEn":"Comparison of the simulated results in a single-phase transformer (TX) winding without the iron core with its experimental data (<i>f</i> = 50 Hz). WOIC stands for without the iron core. ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_8.png"},{"magId":"e556ab6e-2544-47ca-890e-2f3c341d7d9e","pptUrl":"2772-8307-10-0-100095/img_9.png.ppt","labelEn":"Fig. 9.","figUrl":"2772-8307-10-0-100095/img_9.png","titleEn":"Fig. 9. Structured meshes for the 3-phase 1 MVA transformer with the three-limb iron core.","id":"F9","captionEn":"Structured meshes for the 3-phase 1 MVA transformer with the three-limb iron core. ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_9.png"},{"magId":"2d0e4864-5714-491c-acb6-8d13b3591487","pptUrl":"2772-8307-10-0-100095/img_10.png.ppt","labelEn":"Fig. 10.","figUrl":"2772-8307-10-0-100095/img_10.png","titleEn":"Fig. 10. Rated currents in each phase of the transformer (f = 50 Hz): (a) applied currents in HV windings, (b) applied currents in LV windings.","id":"F10","captionEn":"Rated currents in each phase of the transformer (<i>f</i> = 50 Hz): (a) applied currents in HV windings, (b) applied currents in LV windings. ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_10.png"},{"magId":"bac57af6-3dc4-44cb-b973-75b0f34a2511","pptUrl":"2772-8307-10-0-100095/img_11.png.ppt","labelEn":"Fig. 11.","figUrl":"2772-8307-10-0-100095/img_11.png","titleEn":"Fig. 11. Simulated AC losses of the stand-alone LV winding with/without the iron core (f = 50 Hz). WIC stands for with the iron core.","id":"F11","captionEn":"Simulated AC losses of the stand-alone LV winding with/without the iron core (<i>f</i> = 50 Hz). WIC stands for with the iron core. ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_11.png"},{"magId":"4c91baec-95f5-4044-bf29-22b805510a9f","pptUrl":"2772-8307-10-0-100095/img_12.png.ppt","labelEn":"Fig. 12.","figUrl":"2772-8307-10-0-100095/img_12.png","titleEn":"Fig. 12. Loss in each disc of the stand-alone LV winding WIC/WOIC (f = 50 Hz, Irated = 1964 A).","id":"F12","captionEn":"Loss in each disc of the stand-alone LV winding WIC/WOIC (<i>f</i> = 50 Hz, <i>I</i><sub>rated</sub> <i>=</i> 1964 A). ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_12.png"},{"magId":"d73dfb2e-c74d-45dc-b325-de0f110d9822","pptUrl":"2772-8307-10-0-100095/img_13.png.ppt","labelEn":"Fig. 13.","figUrl":"2772-8307-10-0-100095/img_13.png","titleEn":"Fig. 13. Bperp distributions and magnetic flux lines of the end six discs in the stand-alone LV winding WIC/WOIC. (f = 50 Hz, Irated = 1964 A, t = 3/4 T): (a) WIC, and (b) WOIC. The red dashed rectangles highlight the area with a large perpendicular magnetic field.","id":"F13","captionEn":"<i>B</i><sub>perp</sub> distributions and magnetic flux lines of the end six discs in the stand-alone LV winding WIC/WOIC. (<i>f</i> = 50 Hz, <i>I</i><sub>rated</sub> <i>=</i> 1964 A, <i>t</i> = 3/4 <i>T</i>): (a) WIC, and (b) WOIC. The red dashed rectangles highlight the area with a large perpendicular magnetic field. ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_13.png"},{"magId":"1310febe-3961-4468-a16c-b8c18cc18136","pptUrl":"2772-8307-10-0-100095/img_14.png.ppt","labelEn":"Fig. 14.","figUrl":"2772-8307-10-0-100095/img_14.png","titleEn":"Fig. 14. J/Jc distributions of the end six discs in the stand-alone LV winding WIC/WOIC (f = 50 Hz, Irated = 1964 A, t = 3/4 T): (a) WIC, and (b) WOIC.","id":"F14","captionEn":"<i>J</i>/<i>J</i><sub>c</sub> distributions of the end six discs in the stand-alone LV winding WIC/WOIC (<i>f</i> = 50 Hz, <i>I</i><sub>rated</sub> <i>=</i> 1964 A, <i>t</i> = 3/4 <i>T</i>): (a) WIC, and (b) WOIC. ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_14.png"},{"magId":"3bf4808a-b47f-4770-9a7b-22fc0508fda0","pptUrl":"2772-8307-10-0-100095/img_15.png.ppt","labelEn":"Fig. 15.","figUrl":"2772-8307-10-0-100095/img_15.png","titleEn":"Fig. 15. AC losses of phase B WIC/WOIC (f = 50 Hz).","id":"F15","captionEn":"AC losses of phase B WIC/WOIC <i>(f</i> = 50 Hz). ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_15.png"},{"magId":"d3c56c62-fe60-4514-965a-be54625c19f0","pptUrl":"2772-8307-10-0-100095/img_16.png.ppt","labelEn":"Fig. 16.","figUrl":"2772-8307-10-0-100095/img_16.png","titleEn":"Fig. 16. Loss value of each disc within the HV and LV windings of phase B WIC/WOIC at Irated (f = 50 Hz): (a) HV winding, and (b) LV winding.","id":"F16","captionEn":"Loss value of each disc within the HV and LV windings of phase B WIC/WOIC at <i>I</i><sub>rated</sub> (<i>f</i> = 50 Hz): (a) HV winding, and (b) LV winding. ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_16.png"},{"magId":"cf5f67de-f663-4b5d-b07c-2f0ab341e8a5","pptUrl":"2772-8307-10-0-100095/img_17.png.ppt","labelEn":"Fig. 17.","figUrl":"2772-8307-10-0-100095/img_17.png","titleEn":"Fig. 17. Bperp distributions and magnetic flux lines for phase B WIC/WOIC at Irated (f = 50 Hz, t = 3/4 T).","id":"F17","captionEn":"<i>B</i><sub>perp</sub> distributions and magnetic flux lines for phase B WIC/WOIC at <i>I</i><sub>rated</sub> (<i>f</i> = 50 Hz, <i>t</i> = 3/4 <i>T</i>). ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_17.png"},{"magId":"f3c07331-ec1a-4325-ab83-a24aa538dfc2","pptUrl":"2772-8307-10-0-100095/img_18.png.ppt","labelEn":"Fig. 18.","figUrl":"2772-8307-10-0-100095/img_18.png","titleEn":"Fig. 18. Comparisons of loss results between the stand-alone LV winding and phase B with different iron cores at various currents (f = 50 Hz).","id":"F18","captionEn":"Comparisons of loss results between the stand-alone LV winding and phase B with different iron cores at various currents (<i>f</i> = 50 Hz). ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_18.png"},{"magId":"5e469d49-f783-4713-9699-344d6e5c6ddc","pptUrl":"2772-8307-10-0-100095/img_19.png.ppt","labelEn":"Fig. 19.","figUrl":"2772-8307-10-0-100095/img_19.png","titleEn":"Fig. 19. Magnetic flux density distributions and flux lines of the stand-alone LV winding with different iron cores (f = 50 Hz, Irated = 1964 A, t = 3/4): (a) low saturation, and (b) high saturation.","id":"F19","captionEn":"Magnetic flux density distributions and flux lines of the stand-alone LV winding with different iron cores (<i>f</i> = 50 Hz, <i>I</i><sub>rated</sub> <i>=</i> 1964 A, <i>t</i> = 3/4): (a) low saturation, and (b) high saturation. ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_19.png"},{"magId":"0e096e22-3cab-4d05-a6b5-5108ae687df4","pptUrl":"2772-8307-10-0-100095/img_20.png.ppt","labelEn":"Fig. 20.","figUrl":"2772-8307-10-0-100095/img_20.png","titleEn":"Fig. 20. The positions and dimensions of FDs attached to the ends of the HV and LV windings.","id":"F20","captionEn":"The positions and dimensions of FDs attached to the ends of the HV and LV windings. ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_20.png"},{"magId":"9e495680-6c0f-485a-833f-d6d6f6f7b1cd","pptUrl":"2772-8307-10-0-100095/img_21.png.ppt","labelEn":"Fig. 21.","figUrl":"2772-8307-10-0-100095/img_21.png","titleEn":"Fig. 21. Bperp distributions and magnetic flux lines of the stand-alone LV winding with the iron core and different FDs (f = 50 Hz, Irated = 1964 A, t = 3/4): (a) WIC, (b) WIC_FDs_1, (c) WIC_FDs_2. The black dashed rectangles highlight the area with a large perpendicular magnetic field.","id":"F21","captionEn":"<i>B</i><sub>perp</sub> distributions and magnetic flux lines of the stand-alone LV winding with the iron core and different FDs (<i>f</i> = 50 Hz, <i>I</i><sub>rated</sub> <i>=</i> 1964 A, <i>t</i> = 3/4): (a) WIC, (b) WIC_FDs_1, (c) WIC_FDs_2. The black dashed rectangles highlight the area with a large perpendicular magnetic field. ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_21.png"},{"magId":"4d191085-b6b0-4adc-b361-9678d9dc8ccb","pptUrl":"2772-8307-10-0-100095/img_22.png.ppt","labelEn":"Fig. 22.","figUrl":"2772-8307-10-0-100095/img_22.png","titleEn":"Fig. 22. Bperp distributions and magnetic flux lines of phase B with the iron core and different FDs at Irated (f = 50 Hz, t = 3/4): (a) WIC, (b) WIC_FDs_C1, (c) WIC_FDs_C2. The red and blue dashed rectangles highlight the area with a large perpendicular magnetic field.","id":"F22","captionEn":"<i>B</i><sub>perp</sub> distributions and magnetic flux lines of phase B with the iron core and different FDs at <i>I</i><sub>rated</sub> (<i>f</i> = 50 Hz, <i>t</i> = 3/4): (a) WIC, (b) WIC_FDs_C1, (c) WIC_FDs_C2. The red and blue dashed rectangles highlight the area with a large perpendicular magnetic field. ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_22.png"},{"magId":"b0704283-2d89-455f-a4eb-4b33510ba7f2","pptUrl":"2772-8307-10-0-100095/img_23.png.ppt","labelEn":"Fig. 23.","figUrl":"2772-8307-10-0-100095/img_23.png","titleEn":"Fig. 23. Loss dependency of phase B on dts with the iron core and FDs_C1 at Irated (f = 50 Hz).","id":"F23","captionEn":"Loss dependency of phase B on <i>d</i><sub>ts</sub> with the iron core and FDs_C1 at <i>I</i><sub>rated</sub> (<i>f</i> = 50 Hz). ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_23.png"},{"magId":"43d2c3e4-4cde-4a32-93df-b8e47db7ad12","pptUrl":"2772-8307-10-0-100095/img_24.png.ppt","labelEn":"Fig. 24.","figUrl":"2772-8307-10-0-100095/img_24.png","titleEn":"Fig. 24. AC loss values of each disc within the LV winding in phase B with the iron core and FDs_C1 for varied dts and Irated (f = 50 Hz).","id":"F24","captionEn":"AC loss values of each disc within the LV winding in phase B with the iron core and FDs_C1 for varied <i>d</i><sub>ts</sub> and <i>I</i><sub>rated</sub> (<i>f</i> = 50 Hz). ","thumbnailUrl":"2772-8307-10-0-100095/thumbnail/img_24.png"}],"article":{"juan":"10","endNoteUrl_en":"https://www.qk.sjtu.edu.cn/supercon/EN/article/getTxtFile.do?fileType=EndNote&id=48222","bibtexUrl_cn":"//www.sghhindu.com/www.qk/supercon/CN/article/getTxtFile.do?fileType=BibTeX&id=48222","articleType":"A","abstractUrl_en":"https://www.qk.sjtu.edu.cn/supercon/EN/10.1016/j.supcon.2024.100095","qi":"0","id":48222,"nian":2024,"bianHao":"1720084968166-932298104","juanUrl_en":"https://www.qk.sjtu.edu.cn/supercon/EN/Y2024","shouCiFaBuRiQi":"2024-04-13","qiShiYe":"100095","accepted":"2024-03-31","received":"2024-01-20","qiUrl_cn":"//www.sghhindu.com/www.qk/supercon/CN/Y2024/V10/I0","pdfSize":"4938KB","risUrl_cn":"//www.sghhindu.com/www.qk/supercon/CN/article/getTxtFile.do?fileType=Ris&id=48222","doi":"10.1016/j.supcon.2024.100095","jieShuYe":"","keywordList_en":["High-temperature superconducting transformer","T-A formulation","AC losses","Iron core","Flux diverters"],"endNoteUrl_cn":"//www.sghhindu.com/www.qk/supercon/CN/article/getTxtFile.do?fileType=EndNote&id=48222","zhaiyao_en":"

High-temperature superconducting (HTS) technology provides an alternative approach to achieve compact transformers. Addressing AC loss in the HTS winding is crucial for HTS transformer applications. Most numerical AC loss studies on HTS transformers have neglected the influence of iron cores. This work carries out an AC loss study to explore the impact of an iron core on the HTS windings in a 3-phase HTS 1 MVA transformer coupled with it. AC loss simulations for the transformer winding both with and without the iron core are conducted by adopting the three-dimensional (3D) T-A homogenization method. When the iron core is incorporated, the saturation magnetic fields of iron materials, flux diverters (FDs) with different geometries, and variations in turn spacings in the LV winding composed of Roebel cables are considered to investigate their influence on the AC loss of the transformer winding. The inclusion of the iron core leads to a 1.2% increase in AC loss for the transformer winding while simulating at the rated current. We attribute this slight difference to the non-inductive winding structure of the transformer winding, where a strong magnetic field generated in the space between the LV and HV windings effectively shields the influence of the iron core.

","bibtexUrl_en":"https://www.qk.sjtu.edu.cn/supercon/EN/article/getTxtFile.do?fileType=BibTeX&id=48222","abstractUrl_cn":"https://www.qk.sjtu.edu.cn/supercon/CN/10.1016/j.supcon.2024.100095","juanUrl_cn":"https://www.qk.sjtu.edu.cn/supercon/CN/Y2024","lanMu_en":"Research article","qiUrl_en":"https://www.qk.sjtu.edu.cn/supercon/EN/Y2024/V10/I0","risUrl_en":"https://www.qk.sjtu.edu.cn/supercon/EN/article/getTxtFile.do?fileType=Ris&id=48222","title_en":"AC loss study on a 3-phase HTS 1 MVA transformer coupled with a three-limb iron core","revised":"2024-03-26","hasPdf":"true"},"authorList_en":[{"deceased":false,"xref":"a, b","name_cn":"Yue Wu","xref_en":"a, b","name_en":"Yue Wu"},{"deceased":false,"xref":"b","name_cn":"Shuangrong You","xref_en":"b","name_en":"Shuangrong You"},{"deceased":false,"xref":"a, *","name_cn":"Jin Fang","email":"jfang@bjtu.edu.cn","xref_en":"a, *","name_en":"Jin Fang"},{"deceased":false,"xref":"b","name_cn":"Rodney A. Badcock","xref_en":"b","name_en":"Rodney A. Badcock"},{"deceased":false,"xref":"b","name_cn":"Nicholas J. Long","xref_en":"b","name_en":"Nicholas J. Long"},{"deceased":false,"xref":"b, *","name_cn":"Zhenan Jiang","email":"zhenan.jiang@vuw.ac.nz","xref_en":"b, *","name_en":"Zhenan Jiang"}]}">

AC loss study on a 3-phase HTS 1 MVA transformer coupled with a three-limb iron core

Yue Wu, Shuangrong You, Jin Fang, Rodney A. Badcock, Nicholas J. Long, Zhenan Jiang

Superconductivity››2024, Vol. 10››Issue (0): 100095.

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Superconductivity ›› 2024, Vol. 10 ›› Issue (0) : 100095. DOI: 10.1016/j.supcon.2024.100095

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AC loss study on a 3-phase HTS 1 MVA transformer coupled with a three-limb iron core

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{{article.zuoZheCn_L}}.{{article.title_cn}}[J]. {{journal.qiKanMingCheng_CN}}, 2024, 10(0): 100095 https://doi.org/10.1016/j.supcon.2024.100095
{{article.zuoZheEn_L}}.{{article.title_en}}[J]. {{journal.qiKanMingCheng_EN}}, 2024, 10(0): 100095 https://doi.org/10.1016/j.supcon.2024.100095
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