2016
DOI: 10.1063/1.4943520
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Impact of orifice orientation on a finite-span synthetic jet interaction with a crossflow

Abstract: The formation and evolution of flow structures associated with a finite-span synthetic jet issued into a zero-pressure gradient boundary layer were investigated experimentally using stereoscopic particle image velocimetry. A synthetic jet with an aspect ratio of AR = 18 was mounted on a flat plate and its interaction with a free stream, having a velocity of U∞ = 10 m/s (Reδ = 2000) at momentum coefficients of Cμ = 0.08, 0.33, and 0.75, was studied. The effect of the orifice pitch (α = 20∘–90∘) and skew (β = 0∘… Show more

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Cited by 25 publications
(27 citation statements)
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“…In addition, the virtual blockage of the jet was reduced with the decreased AR. In another similar study, Van Buren et al (2016 b ) investigated the orifice orientation with pitch (20°−90°) and skew (0°−90°) angles on the vortex formation of an AR = 18 rectangular orifice. Three types of scenarios, i.e.…”
Section: Introductionmentioning
confidence: 99%
“…In addition, the virtual blockage of the jet was reduced with the decreased AR. In another similar study, Van Buren et al (2016 b ) investigated the orifice orientation with pitch (20°−90°) and skew (0°−90°) angles on the vortex formation of an AR = 18 rectangular orifice. Three types of scenarios, i.e.…”
Section: Introductionmentioning
confidence: 99%
“…and Amitay, 2006, Travnicek et al 2011, McGuinn et al 2013 and in mixing enhancement (Freund andMoin 2000, Al-Atabi 2011). The applications of synthetic jets in cross-flow have also been reported in boundary layer control and drag reduction (Lardeau et al 2011, Laouedj et al 2015, Buren and Leong 2016, Kumar and Karn 2018.…”
Section: Introductionmentioning
confidence: 99%
“…The current work expands on that study by increasing the reduced frequency to values expected on the CART3 turbine, using its associated airfoil, by pitching into both shallow and deep stall, and by utilizing more advanced synthetic jet technology including a pitched orifice with higher flow velocities. A further description of the mechanisms by which synthetic jets add momentum and vorticity into the flow is detailed in Glezer and Amitay, Van Buren et al, and Sahni et al The strength of an array of synthetic jets is described by the momentum coefficient, C μ , which is the ratio of momentum injected during the outsroke of the synthetic jet to the momentum of flow over the airfoil, given by Cμ=ntrueIj12ρU2S, where n is the number of active synthetic jets, and trueIj is the time‐averaged synthetic jet momentum during outstroke and can be written as trueIj=1τρAsj0trueτusj2false(tfalse)dt. …”
Section: Introductionmentioning
confidence: 99%