In this paper, the passive control of flow past a semi-circular cylinder is investigated. This control is achieved by adding a porous medium between the solid obstacle and the incompressible fluid in order to reduce drag forces and regularize the flow. A vortexpenalization method is chosen to easily model the flow in the different media. Several configurations of the porous layer are investigated and parametric studies are performed in order to determine the most efficient passive flow control devices. This control study can be considered as a first step to propose efficient strategies to regularize the flow around a side-view mirror.
NOMENCLATUREC D drag coefficient D computational domain F, S fluid domain and solid domain F D drag force Re Reynolds number Z enstrophy d non-dimensional diameter h reference mesh size k intrinsic permeability l ref height of the obstacle u ref reference velocity u = (u,v) velocity field u s body rigid motion u¯mean velocity magnitude u ∞ free stream velocity Γ D computational domain boundaries Δt time step Φ porosity λ penalization parameter μ dynamic viscosity ν kinematic viscosity r density of the fluid τ porous layer thickness χ S characteristic function ω vorticity field
INTRODUCTIONOn a ground vehicle, the outside mirrors, due to their spanwise position, indeed generate a nonnegligible wake which interferes with the flow past car sides. They are responsible of up to 10% of the total vehicle drag but they only represent 0.5% of the total projected surface, which accounts for a good motivation to perform flow control past these obstacles. This work is devoted to the control of flow past a two-dimensional semi-circular cylinder which can be considered as a simplified section of a sideview mirror. As it was shown in [1, 2], a flow past a square back obstacle is not dominated by longitudinal three-dimensional vortical structures, therefore a preliminary two-dimensional study can be useful to supply information and general trends for a further control study in three dimensions around a hemisphere. The aim is to use a control device easy to set up, low cost and allowing to keep the geometry unchanged. As active control devices can be hardly implemented in such a case, an efficient passive strategy seems to be a good alternative. A suitable solution has already been proposed by Bruneau and Mortazavi in [3][4][5][6][7]. It consists in adding a porous sheath on the obstacle surface in order to reduce the vorticity generation of the boundary layer. The presence of a porous medium at the solid-fluid interface indeed imposes a kind of mixed boundary condition intermediate between the noslip and the slip one on the solid boundary [8]. As a result, the shear forces are decreased and the flow dynamics is smoothed. Consequently, the problem we have to solve involves three different media, namely the solid obstacle, the porous layer and the fluid. An easy way to tackle it is to use the penalization method [9]. This method is based on a unique model, the Brinkman-Navier-Stokes equations, which ...