2021
DOI: 10.1038/s41467-021-21966-y
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Anatomy of subcritical submarine flows with a lutocline and an intermediate destruction layer

Abstract: Turbidity currents are sediment-laden flows that travel over a sloping bed under a stagnant ambient fluid, driven by the density difference between the current and the ambient. Turbidity currents transport large amounts of carbon, nutrients and fresh water through oceans and play an important role in global geochemical cycling and seafloor ecosystems. Supercritical currents are observed in steeper slopes. Subcritical currents are observed in milder slopes, where the near-bed and interface layers are prevented … Show more

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Cited by 14 publications
(12 citation statements)
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References 54 publications
(118 reference statements)
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“…Turbulence modulation and formation of a concentration plateau show similarities with the two-layer structure separated by a lutocline well known for fine-sediment transport (Ozdemir, Hsu & Balachandar 2010; Salinas et al. 2021). However, the mechanism at play is fundamentally different.…”
Section: Resultssupporting
confidence: 58%
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“…Turbulence modulation and formation of a concentration plateau show similarities with the two-layer structure separated by a lutocline well known for fine-sediment transport (Ozdemir, Hsu & Balachandar 2010; Salinas et al. 2021). However, the mechanism at play is fundamentally different.…”
Section: Resultssupporting
confidence: 58%
“…For configuration F512, the development of the fluid Reynolds stresses is inhibited by the formation of the plateau around flow reversal (150 • , 0 • and 30 • ) suggesting a strong modulation of turbulence by the particles. Turbulence modulation and formation of a concentration plateau show similarities with the two-layer structure separated by a lutocline well known for fine-sediment transport (Ozdemir, Hsu & Balachandar 2010;Salinas et al 2021). However, the mechanism at play is fundamentally different.…”
Section: Shear Stress Profilesmentioning
confidence: 60%
“…(ii)In panels (d, f,h) (subcritical current), two horizontal surfaces of zero turbulent production marked as z| P=0 are shown. The layer of fluid between these planes is termed 'destruction layer', since turbulence production is negative, and is the result of the interaction between near-wall hairpins ('HP' in zoom-in view I) and counter-rotating vortices ('CV') (see Salinas et al 2021b). (iii)Comparing the different terms of the momentum equation, it can be seen that in the interface layer (above the maximum of velocity), the balance is mainly between ∂(ũ w)/∂ z (zoom-in view IV) and ∂( ũ w )/∂ z (zoom-in view III) in the supercritical current, while it is between ∂(ũ w)/∂ z (zoom-in view VI) and ∂ 2 ũ/∂ z2 /Re in (zoom-in view V) in the subcritical current.…”
Section: Slow Evolution To Near-self-similar Statementioning
confidence: 99%
“…Depending on the slope of the bed, three different flow regimes have been identified (Sequeiros 2012;Salinas et al 2020Salinas et al , 2021bSalinas, Balachandar & Cantero 2021a). At steeper slopes of S 0.05, the current evolves to a near-self-similar supercritical state, which is characterized by a turbulent near-wall layer close to the bottom boundary and a turbulent interface layer where the current vigorously mixes with the ambient (Salinas et al 2021a).…”
Section: Introductionmentioning
confidence: 99%
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