Measurement and Modeling of Initial Quench Development in Nb3Sn Accelerator Magnets

被引:0
|
作者
Keijzer, Ruben [1 ]
Willering, Gerard [2 ]
Rogacki, Piotr [2 ]
Fiscarelli, Lucio [2 ]
Russenschuck, Stephan [2 ]
Dhalle, Marc [1 ]
Ten Kate, Herman [1 ]
机构
[1] Univ Twente, NL-7522 Enschede, Netherlands
[2] CERN, CH-1211 Geneva, Switzerland
关键词
Magnets; Power cables; Antenna measurements; Voltage measurement; Harmonic analysis; Superconducting cables; Voltage; Magnetic field measurement; Dipole antennas; Accelerator magnets; Nb3Sn; quench antenna; quench modelling; rutherford cable; RUTHERFORD CABLES; PROPAGATION; LOCALIZATION; LHC;
D O I
10.1109/TASC.2025.3540833
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
Accelerator magnets are equipped with voltage taps and, on the test bench, with so-called quench antenna's to monitor the transient effects occurring during a magnet quench. Proper identification and localization of a quench origin is vital for understanding performance issues in Nb3Sn accelerator magnets. In this paper, we describe the physical phenomena that occur during the first few milliseconds of a developing quench and how they affect the signals as intercepted with the diagnostic tools. A better understanding of these phenomena allows for better resolution on determination of the quench start location. Measurements from Nb3Sn accelerator magnets are compared with a 3D thermal-electric PEEC-FEM model of a Rutherford cable. The voltage measured over the cable shows an accelerating build-up attributed to the transverse quench propagation in the cable cross-section, which is dominated by inductive effects that results in an avalanche of quenching strands. A slow-down in the voltage build-up then indicates the point at which all strands in the cable cross-section have quenched. This phase of the quench involves a significant current redistribution that creates a magnetic dipole moment picked up by a quench antenna. The harmonic quench antenna used in this work is used to reconstruct the location, magnitude, and direction of this dipole moment, which strongly depends on the start location of the quench in the cable cross-section, on the inter-strand contact resistances and on the magneto-resistance of the copper. It is shown how the quench start location in the cable cross-section can be determined from the time integral of the reconstructed dipole moment.
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页数:7
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