The drag of three-dimensional rectangular cavities |
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Authors: | Eric Savory Norman Toy Peter J. Disimile Russell G. Dimicco |
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Affiliation: | (1) Fluid Mechanics Research Group, Department of Civil Engineering, University of Surrey, GU2 5XH Guildford, United Kingdom;(2) Department of Aerospace Engineering and Engineering Mechanics, University of Cincinnati, 45221 Cincinnati, Ohio, USA |
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Abstract: | ![]() Cavities and other surface cut-outs are present on aircraft in numerous forms, from cargo bays and landing gear housing to rivet depressions and panel handles. Although these surface imperfections make a significant contribution to the overall drag on an aircraft, relatively little is known about the flow mechanisms associated with cavities, particularly those which have a strongly three-dimensional geometry. The present work is a wind tunnel investigation of the drag forces and flow regimes associated with cavities having a 2:1 rectangular planform geometry. The effects of both the cavity depth and the flow incidence angle have been examined in terms of the overall cavity drag increment and the mean surface pressure distributions. The drag forces have been determined from both integrated pressures and direct force balance measurements. For the model normal to the flow direction the flow within the cavity was remarkably symmetrical in all the configurations examined. In most cases the cavity flow is dominated by a single large eddy. However, for cavities yawed to other incidence angles there is considerable flow asymmetry, with strong vorticity shedding and high drag in some cases, notably with depth/narrowest width ratio of 0.4–0.5 at 45–60° incidence. The present data correspond well with established results and extend the scope of information available for design purposes and for the development of numerical models.Nomenclature Ap planform area of model - CD pressure drag coefficient (FD/(Ap · q)) - CD drag coefficient increase due to cavity (CD – cf) - cf local skin friction coefficient - CL pressure lift coefficient (FL/(Ap · q)) - Cp mean surface pressure coefficient (P – Ps)/q) - FD drag force - FL lift force - h depth - L longest planform dimension of model - P surface pressure on model - Ps freestream static pressure - Pt freestream total pressure - q freestream dynamic pressure (Pt – Ps) - Re Reynolds number (UR · W/v) - UR freestream velocity - W narrowest planform dimension of model - Z vertical cartesian coordinate - incidence angle - kinematic viscosity |
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