Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/8257
Title: Turbulent near wake of an Ahmed vehicle model
Authors: Wang, XW
Zhou, Y
Pin, YF
Chan, TL 
Issue Date: 2013
Publisher: Springer
Source: Experiments in fluids, 2013, v. 54, no. 4, 1490 How to cite?
Journal: Experiments in Fluids 
Abstract: The lasting high fuel cost has recently inspired resurgence in drag reduction research for vehicles, which calls for a thorough understanding of the vehicle wake. The simplified Ahmed vehicle model is characterized by controllable flow separation, thus especially suitable for this purpose. In spite of a considerable number of previous investigations, our knowledge of flow around this model remains incomplete. This work aims to revisit turbulent flow structure behind this model. Two rear slant angles, i.e., α = 25° and 35°, of the model were examined, representing two distinct flow regimes. The Reynolds number was 5.26 × 104 based on the model height (H) and incident flow velocity. Using particle image velocimetry (PIV), flow was measured with and without a gap (g/H = 0.174) between the vehicle underside and ground in three orthogonal planes, viz. the x-z, x-y and y-z planes, where x, y, and z are the coordinates along longitudinal, transverse, and spanwise directions, respectively. The flow at g/H = 0 serves as an important reference for the understanding of the highly complicated vehicle wake (g/H ≠ 0). While reconfirming the well-documented major characteristics of the mean flow structure, both instantaneous and time-averaged PIV data unveil a number of important features of the flow structure, which have not been previously reported. As such, considerably modified flow structure models are proposed for both regimes. The time-averaged velocities, second moments of fluctuating velocities, and vorticity components are presented and discussed, along with their dependence on g/H in the two distinct flow regimes.
URI: http://hdl.handle.net/10397/8257
ISSN: 0723-4864
DOI: 10.1007/s00348-013-1490-x
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