2008
DOI: 10.12693/aphyspola.114.235
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The Influence of the Sample Shape on the Flux Jumps Dynamics in Conventional NbTi Superconductor

Abstract: We investigated giant flux jumps, caused by thermomagnetic avalanches, in two cylindrical samples of conventional NbTi-50% superconductor of the same diameter -14 mm, but of different heights -4 mm and 20 mm. We studied the influence of demagnetizing effects on the flux jumps occurrence, the amount of the magnetic flux entering the sample during the following jumps and on the flux jumps dynamics. The dynamics of the magnetic flux entering the sample is compared with the dynamics of the stray field.

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Cited by 2 publications
(2 citation statements)
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“…Figures 2(a The width of the region of instability in the magnetic field increased from µ 0 H 1 tFJ = 2 T in the disc to µ 0 H 1 tFJ = 3.1 T in the ring. The average period between avalanches on the hysteresis loop decreased more than five times from ∆B ext = 0.26 T to ∆B ext = 0.05 T. At a temperature of 2 K for a superconducting ring, the instability region is ∼±7.5 T, which is much wider than that of a superconducting disc [27,28], where it is ∼±5.7 T. A change in the sign of the magnetization on the M(B ext ) loop as a result of the avalanche jump of the magnetic flux was observed for the ring (see the inset in the lower left corner of figure 2(c)). This phenomenon has been experimentally observed in superconducting film rings [29] and cylinders [30], and is associated with a change in the sign of the local surface self-field of a conventional NbTi superconductor [17].…”
Section: Dynamics Of the Magnetic Flux: Ring And Discmentioning
confidence: 90%
“…Figures 2(a The width of the region of instability in the magnetic field increased from µ 0 H 1 tFJ = 2 T in the disc to µ 0 H 1 tFJ = 3.1 T in the ring. The average period between avalanches on the hysteresis loop decreased more than five times from ∆B ext = 0.26 T to ∆B ext = 0.05 T. At a temperature of 2 K for a superconducting ring, the instability region is ∼±7.5 T, which is much wider than that of a superconducting disc [27,28], where it is ∼±5.7 T. A change in the sign of the magnetization on the M(B ext ) loop as a result of the avalanche jump of the magnetic flux was observed for the ring (see the inset in the lower left corner of figure 2(c)). This phenomenon has been experimentally observed in superconducting film rings [29] and cylinders [30], and is associated with a change in the sign of the local surface self-field of a conventional NbTi superconductor [17].…”
Section: Dynamics Of the Magnetic Flux: Ring And Discmentioning
confidence: 90%
“…In our experimental works [9,10] we studied the dynamics of flux jumps in NbTi disk and cylinder. We analyzed the duration of the following flux jumps as a function of the external magnetic field.…”
Section: Discussionmentioning
confidence: 99%