RANSONIC flow past an airfoil at a high freestream Mach number is traditionally defined as consisting of large supersonic regions embedded within a subsonic flowfield. The pressure fluctuations initiated by the shock/boundary-layer interaction may excite intense levels of buffeting. 1 Therefore, to extend the buffet boundaries for a particular airfoil, a technique is required which is capable of controlling either the boundary layer, or alternatively, the shock strength. Boundary-layer control may be performed by employing either blowing or suction within the interaction region. Blowing has a twofold effect, namely, an increase in the boundary-layer thickness coupled with a reduction in the skin friction, whereas suction induces a contrasting decrease in boundary-layer thickness and increase in skin friction. Passive control of the shock/boundary-layer interaction is a technique which provides a combination of blowing and suction forward and aft of the shock, respectively, without the need for a pump. A passive control device (Fig. 1) consists of a porous region and plenum which are positioned at the interaction region. The static pressure rise across the shock wave results in the flow traveling through the plenum to the region of lower pressure forward of the shock position. The increased communication across the shock stimulates the development of a thicker boundary layer forward of the shock. This process effectively changes the airfoil's geometry in a manner which produces a weaker lambda shock system. Moreover, passive control's inherent damping characteristics have been shown experimentally25 to reduce the pressure fluctuations initiated by the shock/boundary-layer interaction and, therefore, delay buffet onset. In the present study, time-accurate flow over an 18%-thick porous circular-arc airfoil is computed in an attempt to ascertain whether passive control will damp, or even eliminate, the flow periodicity detected in the corresponding solid airfoil (CSA) computation,6 thus extending the airfoil's buffet boundary. The following sections briefly describe both the numerical procedure and the results. Numerical Model An explicit Navier-Stokes finite volume scheme MGENS has been developed which is capable accurately predicting viscous flow over an arbitrary airfoil using an orthogonal boundary conforming hyperbolic grid MGHYPR. A detailed description of both the