High-Reynolds-number fractal signature of nascent turbulence during transition. Wu, Z., Zaki, T., A., & Meneveau, C. Proceedings of the National Academy of Sciences, 117(7):3461-3468, National Academy of Sciences, 4, 2020.
High-Reynolds-number fractal signature of nascent turbulence during transition [link]Website  doi  abstract   bibtex   6 downloads  
Transition from laminar to turbulent flow occurring over a smooth surface is a particularly important route to chaos in fluid dynamics. It often occurs via sporadic inception of spatially localized patches (spots) of turbulence that grow and merge downstream to become the fully turbulent boundary layer. A long-standing question has been whether these incipient spots already contain properties of high-Reynolds-number, developed turbulence. In this study, the question is posed for geometric scaling properties of the interface separating turbulence within the spots from the outer flow. For high-Reynolds-number turbulence, such interfaces are known to display fractal scaling laws with a dimension D ≈ 7 / 3 , where the 1/3 excess exponent above 2 (smooth surfaces) follows from Kolmogorov scaling of velocity fluctuations. The data used in this study are from a direct numerical simulation, and the spot boundaries (interfaces) are determined by using an unsupervised machine-learning method that can identify such interfaces without setting arbitrary thresholds. Wide separation between small and large scales during transition is provided by the large range of spot volumes, enabling accurate measurements of the volume–area fractal scaling exponent. Measurements show a dimension of D = 2.36 ± 0.03 over almost 5 decades of spot volume, i.e., trends fully consistent with high-Reynolds-number turbulence. Additional observations pertaining to the dependence on height above the surface are also presented. Results provide evidence that turbulent spots exhibit high-Reynolds-number fractal-scaling properties already during early transitional and nonisotropic stages of the flow evolution.
@article{
 title = {High-Reynolds-number fractal signature of nascent turbulence during transition},
 type = {article},
 year = {2020},
 keywords = {Fractal dimension,Transitional boundary layer,Turbulent spots},
 pages = {3461-3468},
 volume = {117},
 websites = {http://www.pnas.org/lookup/doi/10.1073/pnas.1916636117},
 month = {4},
 publisher = {National Academy of Sciences},
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 abstract = {Transition from laminar to turbulent flow occurring over a smooth surface is a particularly important route to chaos in fluid dynamics. It often occurs via sporadic inception of spatially localized patches (spots) of turbulence that grow and merge downstream to become the fully turbulent boundary layer. A long-standing question has been whether these incipient spots already contain properties of high-Reynolds-number, developed turbulence. In this study, the question is posed for geometric scaling properties of the interface separating turbulence within the spots from the outer flow. For high-Reynolds-number turbulence, such interfaces are known to display fractal scaling laws with a dimension D ≈ 7 / 3 , where the 1/3 excess exponent above 2 (smooth surfaces) follows from Kolmogorov scaling of velocity fluctuations. The data used in this study are from a direct numerical simulation, and the spot boundaries (interfaces) are determined by using an unsupervised machine-learning method that can identify such interfaces without setting arbitrary thresholds. Wide separation between small and large scales during transition is provided by the large range of spot volumes, enabling accurate measurements of the volume–area fractal scaling exponent. Measurements show a dimension of D = 2.36 ± 0.03 over almost 5 decades of spot volume, i.e., trends fully consistent with high-Reynolds-number turbulence. Additional observations pertaining to the dependence on height above the surface are also presented. Results provide evidence that turbulent spots exhibit high-Reynolds-number fractal-scaling properties already during early transitional and nonisotropic stages of the flow evolution.},
 bibtype = {article},
 author = {Wu, Zhao and Zaki, Tamer A and Meneveau, Charles},
 doi = {10.1073/pnas.1916636117},
 journal = {Proceedings of the National Academy of Sciences},
 number = {7}
}

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