scholarly journals AC loss and contact resistance in REBCO CORC®, Roebel, and stacked tape cables

2020 ◽  
Vol 33 (8) ◽  
pp. 085009 ◽  
Author(s):  
K Yagotintsev ◽  
V A Anvar ◽  
P Gao ◽  
M J Dhalle ◽  
T J Haugan ◽  
...  
Keyword(s):  
Author(s):  
Jianfeng Huang ◽  
Y. Ilyin ◽  
W.A.J. Wessel ◽  
Ruben Lubkemann ◽  
Erik Krooshoop ◽  
...  

Abstract The inter-strand contact resistance and AC losses were measured on an ITER PF Coil joint in a parallel applied AC magnetic field. In addition, the hysteresis loss was measured as a function of the angle with the applied magnetic field on a NbTi strand of the same type as in the joint with a Vibrating Sample Magnetometer (VSM). The AC loss measurements were performed at four applied field conditions for combinations of 0 or 1 T offset field and 0.2 or 0.4 T sinusoidal amplitude. The hysteresis loss of the joint was compared with the measured AC loss density of the NbTi strand for the same field conditions as the joint AC loss measurement but with varying the angle of the applied field. The subsequent cable twist angles affect the hysteresis loss since the critical current and penetration field depend on the angle of the applied field. It is found that 15.5° is an effective angle for the calculation of the hysteresis loss of joint when compared to the single strand measurement. The inter-strand contact resistance measurements cover all the typical strand combinations from the five cabling stages of the individual conductors, as well as the strand combinations across the two conductors to characterize the inter-strand including the copper sole resistivity. It’s the first time to measure the contact resistances and AC losses of the full-size ITER PF joint. By comparing the measured and simulated data in the JackPot-ACDC model, it’s also the first time to obtain the accurate inter-strand, inter-petal and strand to copper sole contact resistivities, which are the main input parameters for the further quantitative numerical analysis of the PF joints, in any current and magnetic field conditions.


2000 ◽  
Vol 10 (1) ◽  
pp. 1090-1093 ◽  
Author(s):  
A. Nijhuis ◽  
H.H.J. ten Kate ◽  
V. Pantsyrny ◽  
M. Santini

2020 ◽  
Vol 161 ◽  
pp. 111898
Author(s):  
V.A. Anvar ◽  
J. Qin ◽  
Y. Wu ◽  
T. Bagni ◽  
A. Devred ◽  
...  

Author(s):  
M. D. Sumption ◽  
E. W. Collings ◽  
R. M. Scanlan ◽  
A. Nijhuis ◽  
H. H. J. Kate

2001 ◽  
Vol 14 (11) ◽  
pp. 888-897 ◽  
Author(s):  
M D Sumption ◽  
E W Collings ◽  
R M Scanlan ◽  
S W Kim ◽  
M Wake ◽  
...  
Keyword(s):  

Cryogenics ◽  
1999 ◽  
Vol 39 (1) ◽  
pp. 1-12 ◽  
Author(s):  
M.D. Sumption ◽  
E.W. Collings ◽  
R.M. Scanlan ◽  
A. Nijhuis ◽  
H.H.J. ten Kate
Keyword(s):  

Materials ◽  
2019 ◽  
Vol 12 (23) ◽  
pp. 3883
Author(s):  
Limei Liu ◽  
Jiangtao Yan ◽  
Keyang Wang ◽  
Yang Liu ◽  
Wurui Ta ◽  
...  

Contact resistance is key for stable operation of electrical contact equipment, and can also be extensively applied. For Tokomak devices in fusion reactors, contact resistance of the superconductor magnet system strongly relates to the alternating current (AC) loss of the cable; the cable is assembled using a certain number of contacting superconducting tapes coated with copper layers on both sides. The contact resistance of a metal solid surface is affected by many factors. In this work, the contact resistance of copper surface samples was studied experimentally under variable normal cyclic load, temperature and number of contact surfaces. This is consistent with real-world working conditions, as the structure of superconducting cables can be changed, and such cables are used under cyclic electromagnetic forces in temperatures which range from room to working temperature. Experimental results showed that contact resistance decreased rapidly with an increase of load. Further, when temperature was varied from 77 to 373 K, the load–unload contact resistance lag decreased. When the number of contact surfaces was increased, contact resistance increased. Finally, a fitted formula describing the relationship between contact resistance and cyclic times, temperature and number of contact interfaces was determined. This formula can be used to predict variation trends of contact resistance in complex environments and provide more accurate contact resistance parameters for calculating the AC loss of superconducting cables.


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