Study of the wall pressure variations on the stall inception of a thick cambered profile at high Reynolds number

We present an experimental study of the aerodynamic forces on a thick and cambered airfoil at a high Reynolds number (Re) (3.6 x 10), which is of direct relevance for wind turbine design. Unlike thin airfoils at low chord-based Reynolds numbers, no consistent de- scription currently exists for the stall process on such airfoils. We consider two chordwise rows of instantaneous wall pressure measurements, taken simultaneously at two spanwise locations over a range of angles of attack. We show that around maximum lift conditions, a strong asymmetry is observed in the statistics of the normal force on each chord. In this range of angles of attacks, the pressure fluctuations are largest in the adverse pressure gradient region, and the fluctuation peak along the chord is systematically located directly upstream of the mean steady separation point, indicating intermittent flow separation. Moreover, the fluctuations are characterized by bistability in both space and time: For each spanwise location, large excursions of the local wall pressure between two different levels can be observed in time (jumps), and these excursions are highly anticorrelated between the two spanwise locations (spatial switches). The characteristic timescale for the switches is found to be well correlated with the amplitudes of the fluctuations. Application of proper orthogonal decomposition (POD) analysis to each row of sensors confirms that the flow separation is an inherently local, three-dimensional, and unsteady process that occurs in a continuous manner when the angle of attack increases. The correlation between the dominant POD mode amplitudes is found to be a good indicator of bistability. For all angles of attack, most of the fluctuations can be captured with the two most energetic POD modes. This suggests that force fluctuations near the maximal lift could be modelled by a low-order approach for monitoring and control purposes.