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Temporal resistance variation of the second generation HTS tape during superconducting-to-normal state transition
SpringerPlus volume 2, Article number: 599 (2013)
The quench process in high-temperature superconducting (HTS) wires plays an important role in superconducting power devices, such as fault current limiters, magnets, cables, etc. The superconducting device should survive after the overheating due to quench.
We studied the evolution of the resistance of the YBCO tape wire during the quench process with 1 ms time resolution for various excitation voltages.
The resistive normal zone was found to be located in a domain of about 1-4 cm long. The normal state nucleation begins in 40-60 ms after voltage is applied across the HTS tape. In subsequent 200-300 ms other normal state regions appear. The normal domain heating continues in the following 5-10s that results in a factor of 2–3 increase of its resistance.
Formation of the normal domain during the quench process follows the same stages for different excitation voltages. Characteristic domain sizes, lifetimes and temperatures are determined for all stages.
The quench process in high-temperature superconducting (HTS) wires plays an important role in superconducting fault current limiter operation. It occurs when current in a wire exceeds the critical value and as a result, the wire resistance becomes nonzero. The problem of quench stability is related to the heat transfer and is especially crucial for the Second Generation HTS wires on highly resistive substrates. We present here the results of studies of the normal zone generation.
Methods and results
We studied the process of quench in HTS tapes using the experimental procedure described in (Fleishman et al., 2010). The sample was 12 mm wide and 100 mm long SuperPower YBCO tape SF12100 (Super-power). Both nominal and measured critical currents at 77 K are about 300A. It consists of 100 mu of Hastelloy substrate, 1 mu YBCO (critical temperature Tc = 91 K) and 1.5mu Ag layers. Measurements were performed with the tape immersed in liquid nitrogen. The AC (50 Hz) voltage step with the amplitude V0 was applied to the sample at the time t0. After that, during the subsequent 40s, we registered the current I and sample AC resistance Z with 1 ms time resolution.
Figures 1 and 2 show the resistance Z as a function of time t for V0 = 379 mV. Time dependence of Z observed in all measurements may be divided into three stages. At the first stage the normal zone forms in a “weak” segment due to exceeding of the local critical current, and Z increases up to Z1 at the moment t1. At the second stage from t1 to t2, the normal region grows due to heat generation inside the initial normal zone, and Z increases up to Z2. At the third stage, t > t2, the resistance increases to the equilibrium value Z3 as a result of temperature growth in the newly formed normal domain and decrease of current.
The sample resistances Z1, Z2, and Z3 as functions of voltage step magnitude V0 are shown in Figure 3. These resistances grow monotonically with V0. Up to V0 = 300 mV heating processes are weak and all the three stages merge. At V0 = 1 V the initial stage resistance Z1 is about 30% of the final value Z3.
The normal domain size can be estimated using the voltage dependence of the domain temperature and temperature dependence of the wire resistance. Maximal temperature TM(K) is expressed the following way (Mal’ginov et al., 2013):
Equation (1) is experimentally proven to be valid in the range 0.5 V < V_0 < 0.8 V. In order to estimate the length of the normal zone we do assume that this formula is applicable also outside the specified range. The resistance Z (mOhm) of the zone where the YBCO layer is in the normal state (T(K) > Tc) is given by the following expression:
here L (mm) is the length of the zone where T > Tc for t > t1, V0 (mV) is the applied voltage magnitude.
Using (1) and (2) and assuming that Z1 is the domain resistance at liquid nitrogen temperature and Z3 is the resistance at the maximum temperature, one can obtain the domain size (L1) and the size of zone with TM (L3) as function of V0:
Figure 4 shows L1 and L3 values versus V0 calculated from (3) and (4).
From the above results we conclude that during the superconducting-to-normal state transition in HTS tape the normal phase is limited to a single domain. The domain nucleates in 40-60 ms after the voltage is applied. In the subsequent 5-10s the domain heats up; it results in 2–3 times increase of the resistance. Central part of the domain is about 20-30 mm long. Inside the both of the 3-5 mm long edges of the domain the temperature falls from the maximal temperature TM to 90 K.
Fleishman LS, Mal’ginov VA, Mal’ginov AV: Ways for increasing the rated capacity of a superconducting current-limiting device. Thermal Engineering 2010, 57(14):1216-1221. 10.1134/S0040601510140077
Mal’ginov AV, Yu Kuntsevich A, Mal’ginov VA, Fleishman LS: Normal domain temperature profile in second generation HTS tape wire. SpringerPlus 2013, 2: 535. 10.1186/2193-1801-2-535
This work was supported by Russian Foundation for Basic Research (Grant 14-08-00418-a and Grant 12-08-31415-mol-a), Programs of Russian Academy of Sciences, Russian Ministry of Education and Sciences (Grant 8203), Russian science support foundation and using facilities of the Shared Research Equipment Center at LPI.
The authors declare that they have no competing interests.
All authors planned and designed the experiment, read and approved the final manuscript.
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Malginov, V.A., Malginov, A.V. & Fleishman, L.S. Temporal resistance variation of the second generation HTS tape during superconducting-to-normal state transition. SpringerPlus 2, 599 (2013). https://doi.org/10.1186/2193-1801-2-599
- High-temperature superconductors
- Normal zone propagation