2021
DOI: 10.1209/0295-5075/134/46002
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Local measurement of vortex statistics in quantum turbulence

Abstract: The density fluctuations of quantum vortex lines are measured in a turbulent flow of superfluid He, at temperatures corresponding to superfluid fractions of 16%, 47% and 81%. The probe is a micro-fabricated second sound resonator allowing for local and small-scale measurements in the core of the flow, downstream a grid at a 10-mesh size. Remarkably, all the vortex power spectra collapse on a single master curve, independently from the superfluid fraction and the mean velocity. By contrast with previous measure… Show more

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Cited by 6 publications
(12 citation statements)
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“…24 displays the selectivity of two second sound tweezers of size L = 250 µm and L = 1 mm respectively, depending on the shift X sh and the mode number n (where k = nπ). The simulation was run with a quantum vortex line density L = 2 × 10 10 m −2 and U = 1 m/s, in accordance with the typical values observed in the experiments of [WVR21]. It can be seen that large tweezers (L = 1 mm) can reach a vortex selectivity R ξ > 90% for a small shift and low mode number, which means that they can be used for direct quantum vortex measurements.…”
Section: Kenelly Circle Centermentioning
confidence: 76%
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“…24 displays the selectivity of two second sound tweezers of size L = 250 µm and L = 1 mm respectively, depending on the shift X sh and the mode number n (where k = nπ). The simulation was run with a quantum vortex line density L = 2 × 10 10 m −2 and U = 1 m/s, in accordance with the typical values observed in the experiments of [WVR21]. It can be seen that large tweezers (L = 1 mm) can reach a vortex selectivity R ξ > 90% for a small shift and low mode number, which means that they can be used for direct quantum vortex measurements.…”
Section: Kenelly Circle Centermentioning
confidence: 76%
“…Aside from vortex density measurements, the second sound can also provide information on the fluid temperature -since the second sound velocity depends on it-and on the velocity of the background He-II flow when it induces a phase shift or Doppler effect on the second sound (e.g. see [DL77,WPHE81,WVR21]).…”
Section: From Macroscopic Second Sound Sensors To Microscopic Tweezersmentioning
confidence: 99%
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