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Supersonic Turbulent Boundary-Layer Separation Control Using a Morphing Surface

Vilas Shinde, Datta V. Gaitonde, Jack J. McNamara

2021AIAA Journal29 citationsDOI

Abstract

Separated flows arising due to shock-wave/turbulent boundary-layer interactions can cause problematic low-frequency unsteadiness with potentially severe structural response. High-fidelity large-eddy simulations are employed to examine surface morphing as a way to reduce the size of the separation region, and thus favorably alter the unsteadiness characteristics. The configuration considers a turbulent Mach 2.7 flow at a Reynolds number of subjected to an impinging shock system with a pressure ratio of , which results in separation and the presence of structurally relevant low-frequency unsteadiness. The control surface, centered about the shock impingement location and extending over the separation region, is allowed to deform under material property-based realizability constraints until an asymptotic state is achieved. The criterion for deformation uses a measure proportional to the directional surface shear stress. At an asymptotic state, the deformed surface reveals a shape consistent with aerostructural optimization and a maximum height of . Control mitigates the sharp initial pressure gradient of the uncontrolled flow to delay and reduce separation extent (by 50%) with diminution of low-frequency content and turbulent kinetic energy. Modal decomposition highlights these effects in the energy content of the prominent modes. Morphing may thus provide a means to adjust the local surface deflection in a manner that reduces some of the problems associated with turbulent separation.

Topics & Concepts

MechanicsMach numberTurbulenceFlow separationBoundary layerSupersonic speedTurbulence kinetic energyShock (circulatory)Angle of attackMaterials scienceReynolds numberPhysicsClassical mechanicsAerodynamicsMedicineInternal medicineComputational Fluid Dynamics and AerodynamicsFluid Dynamics and Turbulent FlowsPlasma and Flow Control in Aerodynamics
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