4.7 Article

Minimal energy thresholds for sustained turbulent bands in channel flow

期刊

JOURNAL OF FLUID MECHANICS
卷 942, 期 -, 页码 -

出版社

CAMBRIDGE UNIV PRESS
DOI: 10.1017/jfm.2022.364

关键词

nonlinear instability; shear-flow instability; transition to turbulence

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In this study, nonlinear variational optimization is applied to find minimal seeds for the formation of turbulent bands in channel flow. The minimal energy threshold for obtaining spatially patterned turbulence is found to scale with the Reynolds number to the power of -8.5 for Reynolds numbers greater than 1000. The minimal seed exhibits spot-like structure and low-amplitude large-scale quadrupolar flow. Its evolution depends on the Reynolds number and initial energy, and two different formation mechanisms are observed.
In this work, nonlinear variational optimization is used for obtaining minimal seeds for the formation of turbulent bands in channel flow. Using nonlinear optimization together with energy bisection, we have found that the minimal energy threshold for obtaining spatially patterned turbulence scales with Re-8.5 for Re > 1000. The minimal seed, which is different to that found in a much smaller domain, is characterized by a spot-like structure surrounded by a low-amplitude large-scale quadrupolar flow filling the whole domain. This minimal-energy perturbation of the laminar flow has dominant wavelengths close to 4 in the streamwise direction and 1 in the spanwise direction, and is characterized by a spatial localization increasing with the Reynolds number. At Re less than or similar to 1200, the minimal seed evolves in time, creating an isolated oblique band, whereas for Re greater than or similar to 1200, a quasi-spanwise-symmetric evolution is observed, giving rise to two distinct bands. A similar evolution is found also at low Re for non-minimal optimal perturbations. This highlights two different mechanisms of formation of turbulent bands in channel flow, depending on the Reynolds number and initial energy of the perturbation. The selection of one of these two mechanisms appears to be dependent on the probability of decay of the newly created stripe, which increases with time, but decreases with the Reynolds number.

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