# Temporal resistance variation of the second generation HTS tape during superconducting-to-normal state transition

- Vladimir A Malginov
^{1}Email author, - Andrey V Malginov
^{1}and - Leonid S Fleishman
^{2}

**2**:599

https://doi.org/10.1186/2193-1801-2-599

© Malginov et al.; licensee Springer. 2013

**Received: **16 May 2013

**Accepted: **1 November 2013

**Published: **9 November 2013

## Abstract

### Background

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.

### Methods

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.

### Findings

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.

### Conclusions

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.

## Keywords

## Introduction

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 T_{c} = 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 V_{0} was applied to the sample at the time t_{0}. After that, during the subsequent 40s, we registered the current I and sample AC resistance Z with 1 ms time resolution.

_{0}= 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 Z

_{1}at the moment t

_{1}. At the second stage from t

_{1}to t

_{2}, the normal region grows due to heat generation inside the initial normal zone, and Z increases up to Z

_{2}. At the third stage, t > t

_{2}, the resistance increases to the equilibrium value Z

_{3}as a result of temperature growth in the newly formed normal domain and decrease of current.

_{1}, Z

_{2,}and Z

_{3}as functions of voltage step magnitude V

_{0}are shown in Figure 3. These resistances grow monotonically with V

_{0}. Up to V

_{0}= 300 mV heating processes are weak and all the three stages merge. At V

_{0}= 1 V the initial stage resistance Z

_{1}is about 30% of the final value Z

_{3}.

_{M}(K) is expressed the following way (Mal’ginov et al., 2013):

_{_}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) > T

_{c}) is given by the following expression:

here L (mm) is the length of the zone where T > T_{c} for t > t_{1}, V_{0} (mV) is the applied voltage magnitude.

_{1}is the domain resistance at liquid nitrogen temperature and Z

_{3}is the resistance at the maximum temperature, one can obtain the domain size (L

_{1}) and the size of zone with T

_{M}(L

_{3}) as function of V

_{0}:

## Conclusions

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 T_{M} to 90 K.

## Declarations

### Acknowledgements

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.

## Authors’ Affiliations

## References

- 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/S0040601510140077View ArticleGoogle Scholar - 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. 10.1186/2193-1801-2-535View ArticleGoogle Scholar - Super-power http://www.superpower-inc.com/

## Copyright

This article is published under license to BioMed Central Ltd. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.