Research / Dynamic stall

Dynamic stall

When an airfoil pitches beyond its static stall angle, a large vortex forms on the suction side, briefly boosting lift before it detaches. My Ph.D. at Johns Hopkins connected the flow, the pressure field and the loads during this cycle.

Vorticity and pressure coefficient fields around a pitching airfoil
Phase-averaged (a) vorticity and (b) pressure coefficient around a pitching NACA 0015 airfoil at Re = 91,000 and reduced frequency k = 0.39. From Jose, Lu, Agarwal & Katz, AIAA J. (2026).

A NACA 0015 airfoil oscillated over reduced frequencies of 0.047 to 1.571 and Reynolds numbers of 13,600 to 136,000. Refractive-index matching allowed stereo PIV on both sides of the transparent airfoil at once, and the pressure field was obtained by integrating the material acceleration. Integrating the surface pressure then gives the lift, pressure drag and moment.

The broad low-pressure region carried by the dynamic-stall vortex delays stall onset and raises the peak lift and drag. The vortex detaches at a fixed fraction (0.3) of the oscillation period and migrates at about 30% of the free-stream speed for all conditions, so once time is shifted by the detachment time, the lift and drag curves collapse.

Space-time maps of surface pressure on a pitching airfoil
Surface pressure over one cycle: (a) suction side, (b) pressure side, (c) their difference and (d) its phase average. The dashed line is the angle of attack. From Jose, Lu, Agarwal & Katz, AIAA J. (2026).