TY - JOUR
T1 - Influence of inter-layer contact resistances on quench propagation in YBa2Cu3Ox coated conductors
AU - Chan, Wan Kan
AU - Masson, Philippe J.
AU - Luongo, Cesar A.
AU - Schwartz, Justin
N1 - Funding Information:
Manuscript received August 26, 2008. First published May 27, 2009; current version published July 15, 2009. This research was partially supported by the Air Force Research Laboratory through Universal Technology Corporation. W.-K. Chan is with the National High Magnetic Laboratory, Tallahassee, FL 32310 USA (e-mail: [email protected]). P. J. Masson is with the Advanced Magnet Lab, Palm Bay, FL 32905 USA (e-mail: [email protected]). C. A. Luongo is with the FAMU-FSU College of Engineering, Tallahassee, FL 32310, USA. He is also with ITER in Cadarache, France (e-mail: Luongo@ magnet.fsu.edu). J. Schwartz is with the National High Magnetic Laboratory, Tallahassee, FL-32310, USA. He is also with FAMU-FSU College of Engineering, Tallahassee, FL 32310 USA (e-mail: [email protected]). Color versions of one or more of the figures in this paper are available online at http://ieeexplore.ieee.org. Digital Object Identifier 10.1109/TASC.2009.2018514
PY - 2009/6
Y1 - 2009/6
N2 - Superconducting power devices are considered for many applications, including airborne applications. For the devices of interest the operating temperature needs to remain around 70 K in order to minimize the weight and volume of the associated cooling system. The use of YBa2 Cu 3 Ox (YBCO) coated conductors allows for operation at fairly high temperature (65-77 K) while maintaining high current carrying capabilities. Unfortunately, when a hot spot is created in a coated conductor wound magnet, the quench propagates so slowly that it cannot be detected using conventional methods and therefore those magnets may remain unprotected. To address this quench detection issue, we must better understand the physics of the quench and the phenomena that drive it so it can be accurately simulated. We have modeled YBCO tapes using Finite Element Analysis to assess the role of the contact resistance between the different layers composing the tape. Indeed, if the temperature rises, the YBCO layer becomes highly resistive and the current redistributes into the stabilization layers. The contact resistance between the YBCO layer and the copper is likely to play a very important role in terms of the current sharing length and voltage difference between the layers. This paper presents a model implemented in COMSOL Multiphysics, simulation results and a discussion.
AB - Superconducting power devices are considered for many applications, including airborne applications. For the devices of interest the operating temperature needs to remain around 70 K in order to minimize the weight and volume of the associated cooling system. The use of YBa2 Cu 3 Ox (YBCO) coated conductors allows for operation at fairly high temperature (65-77 K) while maintaining high current carrying capabilities. Unfortunately, when a hot spot is created in a coated conductor wound magnet, the quench propagates so slowly that it cannot be detected using conventional methods and therefore those magnets may remain unprotected. To address this quench detection issue, we must better understand the physics of the quench and the phenomena that drive it so it can be accurately simulated. We have modeled YBCO tapes using Finite Element Analysis to assess the role of the contact resistance between the different layers composing the tape. Indeed, if the temperature rises, the YBCO layer becomes highly resistive and the current redistributes into the stabilization layers. The contact resistance between the YBCO layer and the copper is likely to play a very important role in terms of the current sharing length and voltage difference between the layers. This paper presents a model implemented in COMSOL Multiphysics, simulation results and a discussion.
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U2 - 10.1109/TASC.2009.2018514
DO - 10.1109/TASC.2009.2018514
M3 - Article
AN - SCOPUS:68649126017
SN - 1051-8223
VL - 19
SP - 2490
EP - 2495
JO - IEEE Transactions on Applied Superconductivity
JF - IEEE Transactions on Applied Superconductivity
IS - 3
M1 - 4982566
ER -