Errata: Passive-Pressure Drag Control in a Plane Wake

We report results of a study of the transition region of a compressible (subsonic) plane wake at moderately high Reynolds numbers, based on the numerical solution of the inviscid time-dependent flow equations. The focus is placed on the flow dynamics in the region of vortex formation and the near wake. A thin interference plate along the wake centreline, which can either be attached or detached from the bluff-body base, is used as a means for passive pressure-drag control by affecting the vortex formation process directly. The results show that the inclusion of an interference plate in the flow configuration can significantly decrease the magnitude of the base pressure coefficient by factors of up to 3, depending on the length of the plate and its separation from the base. The calculated results are in good agreement with the available experimental data and include the detached case for which little or no data exists. The observed self-sustained (global) instabilities in the present simulations were found to be intrinsic features of the flows investigated and are consistent with the local absolute/global instability picture currently favoured.

[1]  Elaine S. Oran,et al.  Vortex-ring dynamics in a transitional subsonic free jet. A numerical study , 1990 .

[2]  W. K. Blake,et al.  HYDROELASTIC VARIABLES INFLUENCING PROPELLER AND HYDROFOIL SINGING , 1977 .

[3]  F. Grinstein,et al.  Effective viscosity in the simulation of spatially evolving shear flows with monotonic FCT models , 1992 .

[4]  E. S. Oran,et al.  Three-dimensional numerical simulation of compressible, spatially evolving shear flows , 1989 .

[5]  J. P. Boris,et al.  Direct numerical simulation of axisymmetric jets , 1986 .

[6]  Peter W. Bearman,et al.  Investigation of the flow behind a two-dimensional model with a blunt trailing edge and fitted with splitter plates , 1965, Journal of Fluid Mechanics.

[7]  Triantafyllou,et al.  Absolute instabilities and self-sustained oscillations in the wake of circular cylinders. , 1987, Physical review letters.

[8]  D. Favier,et al.  Vortex shedding and lock-on of a circular cylinder in oscillatory flow , 1986, Journal of Fluid Mechanics.

[9]  F. H. Barnes,et al.  A comparison of the structure of the wake behind a circular cylinder in a steady flow with that in a perturbed flow , 1987 .

[10]  J. Chomaz,et al.  Bifurcations to local and global modes in spatially developing flows. , 1988, Physical review letters.

[11]  Owen M. Griffin,et al.  Universal Similarity in the Wakes of Stationary and Vibrating Bluff Structures , 1981 .

[12]  D. Rockwell,et al.  On vortex formation from a cylinder. Part 2. Control by splitter-plate interference , 1988, Journal of Fluid Mechanics.

[13]  J E L Simmons,et al.  Similarities Between Two-Dimensional and Axisymmetric Vortex Wakes , 1977 .

[14]  J. P. Boris,et al.  New insights into large eddy simulation , 1992 .

[15]  P. Monkewitz,et al.  Absolute and convective instabilities in free shear layers , 1985, Journal of Fluid Mechanics.

[16]  K. Bütefisch,et al.  V. Karman Vortices and their Frequency Determination in the Wakes of Profiles in the Sub- and Transonic Regimes , 1976 .

[17]  P. Monkewitz,et al.  LOCAL AND GLOBAL INSTABILITIES IN SPATIALLY DEVELOPING FLOWS , 1990 .

[18]  A. Roshko On the Wake and Drag of Bluff Bodies , 1955 .