TY - JOUR
T1 - Airfoil flow separation control with plasma synthetic jets at moderate Reynolds number
AU - Zong, Haohua
AU - van Pelt, Timo
AU - Kotsonis, Marios
PY - 2018/11/1
Y1 - 2018/11/1
N2 - Abstract: An array of 26 plasma synthetic jet actuators (PSJA) is flush-mounted on a NACA-0015 airfoil model to control the leading-edge flow separation at moderate Reynolds number (Rec= 1.7 × 10 5). The stall angle of this airfoil is postponed from 15. 5 ∘ to approximately 22 ∘, and the peak lift coefficient is increased by 21%. PSJAs exhibit distinctive separation control mechanisms depending on the relative location between actuation and separation and reduced frequency of actuation (F∗). At an angle of attack of α= 15. 5 ∘, the non-actuated flow separates approximately 4 % chord length downstream of the jet orifices. Plasma synthetic jets (PSJs) applied at F∗≥ 0.5 can displace the separation point downstream to mid-chord position, as a result of the energizing of the incoming boundary layer through mixing enhancement. As a comparison, with actuation frequency of F∗≤ 0.25 , the separation point at α= 15. 5 ∘ remains near the leading edge and the zero-velocity line is periodically swept towards the suction surface by the convecting spanwise vortices generated from PSJ actuation, leading to a reduction of time-averaged backflow area. For the case of separation control at α= 22 ∘, the separation point resides always upstream of the actuation position, regardless of actuation frequency. The peak lift coefficient is attained at F∗= 1 , and the decreasing lift at high actuation frequency (F∗= 2) is ascribed to the severe interaction between adjacent spanwise vortices at short spacing. Graphical abstract: [Figure not available: see fulltext.].
AB - Abstract: An array of 26 plasma synthetic jet actuators (PSJA) is flush-mounted on a NACA-0015 airfoil model to control the leading-edge flow separation at moderate Reynolds number (Rec= 1.7 × 10 5). The stall angle of this airfoil is postponed from 15. 5 ∘ to approximately 22 ∘, and the peak lift coefficient is increased by 21%. PSJAs exhibit distinctive separation control mechanisms depending on the relative location between actuation and separation and reduced frequency of actuation (F∗). At an angle of attack of α= 15. 5 ∘, the non-actuated flow separates approximately 4 % chord length downstream of the jet orifices. Plasma synthetic jets (PSJs) applied at F∗≥ 0.5 can displace the separation point downstream to mid-chord position, as a result of the energizing of the incoming boundary layer through mixing enhancement. As a comparison, with actuation frequency of F∗≤ 0.25 , the separation point at α= 15. 5 ∘ remains near the leading edge and the zero-velocity line is periodically swept towards the suction surface by the convecting spanwise vortices generated from PSJ actuation, leading to a reduction of time-averaged backflow area. For the case of separation control at α= 22 ∘, the separation point resides always upstream of the actuation position, regardless of actuation frequency. The peak lift coefficient is attained at F∗= 1 , and the decreasing lift at high actuation frequency (F∗= 2) is ascribed to the severe interaction between adjacent spanwise vortices at short spacing. Graphical abstract: [Figure not available: see fulltext.].
UR - http://www.scopus.com/inward/record.url?scp=85055278896&partnerID=8YFLogxK
U2 - 10.1007/s00348-018-2624-y
DO - 10.1007/s00348-018-2624-y
M3 - Article
AN - SCOPUS:85055278896
VL - 59
JO - Experiments in Fluids: experimental methods and their applications to fluid flow
JF - Experiments in Fluids: experimental methods and their applications to fluid flow
SN - 0723-4864
IS - 11
M1 - 169
ER -