Abstract

Fast quench detection is a key requirement for the successful implementation of superconducting magnet technology. In high temperature superconductor magnets, this issue is especially challenging due to the low quench propagation velocity, and presently represents one of the main factors limiting their application. A new detection technique based on stray-capacitance monitoring is proposed. The capacitance between electrically-insulated magnet elements, such as magnet structure and end parts, is utilized as an indication of local heat deposition in the conductor. In fact, the relative permittivity of helium drops when it changes from the liquid to the gaseous phase. Thus, when heating occurs, part of the helium impregnating the insulation layers boils off, and the monitored stray-capacitance decreases. The proposed technique is successfully demonstrated on three small-scale Bi-2212 magnets manufactured at the Lawrence Berkeley National Laboratory. Results from the detection of thermal runaways and spot-heater induced quenches are reported and discussed. Advantages and limitations of the stray-capacitance method with respect to conventional quench detection methods are assessed.

Highlights

  • Detection of the quench development is critical for the protection of superconducting magnets

  • The highest electrical permittivity change occurs when the fluid is transferred from the liquid to the gaseous phase

  • The main mechanism causing the capacitance variation is the change of electrical permittivity of the cryogenic fluid impregnating the insulation layers

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Summary

Introduction

Detection of the quench development is critical for the protection of superconducting magnets. Fast quench detection in high-temperature superconductor (HTS) magnets is more challenging due to the very low normal zone propagation velocity [3,4,5] This feature is one of the factors currently limiting wider application of HTS magnets. Various alternative quench detection methods have been explored in the past These attempts include systems monitoring the voltage across coils magnetically coupled to the protected coil [6, 7], mechanical vibrations [8,9,10,11,12,13], local variations of magnetization and current distribution [14,15,16,17,18,19,20], variation of fiber refraction index with temperature [21,22,23,24,25,26,27], or voltage across non-contact capacitive sensors [28, 29]

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