2006
DOI: 10.1063/1.2187069
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Coherent structures in an airfoil boundary layer and wake at low Reynolds numbers

Abstract: Mitigation of preferential concentration of small inertial particles in stationary isotropic turbulence using electrical and gravitational body forces Phys. Fluids 24, 073301 (2012) Axisymmetric intrusions in two-layer and uniformly stratified environments with and without rotation Phys. Fluids 24, 036603 (2012) Wavelet decomposition of forced turbulence: Applicability of the iterative Donoho-Johnstone threshold Phys. Fluids 24, 025102 (2012) Maximizing dissipation in a turbulent shear flow by optimal control … Show more

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Cited by 124 publications
(70 citation statements)
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“…The shape of the C p profiles is very similar to that measured experimentally for laminar separation bubbles with transition followed by reattachment [38][39][40] . Following transition, C f reaches a minimum negative value, indicative of the 'reverse flow vortex' 41 .…”
Section: Figsupporting
confidence: 67%
See 1 more Smart Citation
“…The shape of the C p profiles is very similar to that measured experimentally for laminar separation bubbles with transition followed by reattachment [38][39][40] . Following transition, C f reaches a minimum negative value, indicative of the 'reverse flow vortex' 41 .…”
Section: Figsupporting
confidence: 67%
“…This peak is very close to the frequency f 2 = 7.4 of the straight trailing edge case and corresponds to the natural shear layer instability. Indeed, if the appropriate as before length and velocity scales are used, which for the blunt airfoil are ψ 0 ≈ 0.075C and U es = 1.34U ∞ respectively, the corresponding non-dimensional frequency f * = f bl,2 ψ 0 /U es ≈ 0.42, which is again close, albeit slightly below, the range of observed values 40 . Despite the presence of the natural instability, the shedding mode at f bl,1 = 4.5 is significantly more dominant, both in the DMD spectrum ( Figure 11) and in the point spectra in the wake and suction side of the airfoil (Figures 14 and 15 respectively).…”
Section: Resultsmentioning
confidence: 58%
“…Yarusevych, Sullivan & Kawall (2009) showed that the length scale of the wake vortices decreased significantly and the vortex pattern became less organized when separation bubbles were formed over the airfoil. Huang & Lin (1995), Yarusevych, Sullivan & Kawall (2006) and Yarusevych & Boutilier (2011) investigated the turbulent wake development of NACA four-digit series airfoils at low Reynolds numbers, and demonstrated that the dimensionless vortex shedding frequency increased linearly with the Reynolds number. Hain, Kähler & Radespiel (2009) showed that the K-H instability led to a spanwise vortex formation in the shear layer above the separation bubble over an SD7003 aerofoil at the Reynolds number of Re = 66 000.…”
Section: Laminar Separation Bubblesmentioning
confidence: 99%
“…Strong coupling between the membrane oscillation and the vortex shedding at the wake, specially for post-stall incidences has been reported by Song and Breuer, 8 Gordnier 11 and Rojratsirikul et al 9 Yarusevych et al 12 has shown that the vortex shedding frequency for symmetrical aerofoils has a linear dependancy on Reynolds numbers at low Reynolds numbers. They also found that the Strouhal number of the wake vortex shedding may increase significantly in this regime.…”
mentioning
confidence: 92%