Abstract

Transonic buffet behaviour of the supercritical airfoil OAT15A was investigated experimentally at flow conditions Ma=0.7 and alpha =3.5^circ , using schlieren and particle image velocimetry (PIV). The general behaviour of the buffet cycle was characterised with short-exposure schlieren visualisation and phase-averaged PIV measurements. A spectral analysis showed that the shock oscillation occurs with a dominant contribution at 160 Hz (St = 0.07, in good agreement with the literature) and between 25 and 55 % of the chord of the airfoil. Proper Orthogonal Decomposition (POD) was applied to the PIV data to extract the main modes connected with buffet. It is found that the first three most energetic modes capture around 65 % of the total fluctuating kinetic energy. The first and the third modes have a main frequency peak at 160 Hz and are well representing the separated area and the shock oscillation. The second mode was, instead, associated with an asymmetrical behaviour of the separated area and of the shear layer and displays a main peak at 320 Hz, being double the main buffet cycle frequency. Finally, it was shown that by using the 11 most energetic POD modes, an accurate reduced-order model (ROM) is obtained, which when subtracted from the instantaneous velocity fields allows the visualisation of the small-scale structures present in the flow, such as the upstream travelling waves (UTWs) and the vortex shedding in the separated area near the trailing edge. The analysis allowed to estimate the velocity of the UTWs, obtaining values in good agreement with the literature. In contrast, the analysis of the vortex dynamics in the trailing edge area revealed that vortices shed at the shock foot, which convect downstream in an area detached from the airfoil surface, cannot be considered responsible for the creation of UTWs in view of the mismatch in frequency of the two phenomena.Graphic abstract

Highlights

  • Transonic buffet consists of an oscillation of the shockwave (SW) on the suction side of a wing/airfoil that may occur for a certain range of Ma, and Re values

  • In addition to characterising the main features of the buffet cycle, Proper Orthogonal Decomposition (POD) will be used to further construct an efficient reduced-order model (as in Hall et al (2000)), which allows to extract the small structures in the flow field, like upstream travelling waves (UTWs) and vortices being shed in the separated area

  • The present investigation has addressed the dynamics of transonic buffet of the OAT15A airfoil, using highspeed schlieren and particle image velocimetry (PIV), supported with a phase-averaged description as well as modal analysis by means of snapshot POD

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Summary

Introduction

Transonic buffet consists of an oscillation of the shockwave (SW) on the suction side of a wing/airfoil (for Type II buffet, which is object of this study) that may occur for a certain range of Ma, and Re values. During the upstream shock movement, the widened area of separated flow reduces the formation of DTWs and of UTWs; the shock upstream movement is no longer sustained by the UTWs and stops its upstream movement, closing the feedback loop According to this description, the UTWs are supposed to be created during the whole buffet cycle and with a strength modulated by the buffet frequency. In addition to characterising the main features of the buffet cycle, POD will be used to further construct an efficient reduced-order model (as in Hall et al (2000)), which allows to extract the small structures in the flow field, like UTWs and vortices being shed in the separated area. Experiments in Fluids (2021) 62:214 paper is concluded with a discussion of the buffet mechanism, based on the results obtained (Sect. 7)

Facility
Experimental measurements techniques
Data processing
Uncertainty analysis
Flow dynamics
Spectral analysis
Time‐average velocity field
Phase definition
Phase average velocity fields
Modal description of flow features
POD analysis
POD energy spectrum
First POD mode
Second POD mode
Third POD mode
Reduced‐order model based on the first three modes
Time coefficients
First‐mode time coefficient
Second‐mode time coefficient
Third‐mode time coefficient
UTWs and vortex dynamics
Shear layer vortices
Findings
Discussion and conclusions

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