Active flow control on an Ahmed body - An experimental study

Author(s):  
Jonathan W. McNally ◽  
Farrukh S. Alvi ◽  
Nicolas Mazellier ◽  
Azeddine Kourta
2021 ◽  
Vol 932 ◽  
Author(s):  
Yiqing Li ◽  
Wenshi Cui ◽  
Qing Jia ◽  
Qiliang Li ◽  
Zhigang Yang ◽  
...  

We address a challenge of active flow control: the optimization of many actuation parameters guaranteeing fast convergence and avoiding suboptimal local minima. This challenge is addressed by a new optimizer, called the explorative gradient method (EGM). EGM alternatively performs one exploitive downhill simplex step and an explorative Latin hypercube sampling iteration. Thus, the convergence rate of a gradient based method is guaranteed while, at the same time, better minima are explored. For an analytical multi-modal test function, EGM is shown to significantly outperform the downhill simplex method, the random restart simplex, Latin hypercube sampling, Monte Carlo sampling and the genetic algorithm. EGM is applied to minimize the net drag power of the two-dimensional fluidic pinball benchmark with three cylinder rotations as actuation parameters. The net drag power is reduced by 29 % employing direct numerical simulations at a Reynolds number of $100$ based on the cylinder diameter. This optimal actuation leads to 52 % drag reduction employing Coanda forcing for boat tailing and partial stabilization of vortex shedding. The price is an actuation energy corresponding to 23 % of the unforced parasitic drag power. EGM is also used to minimize drag of the $35^\circ$ slanted Ahmed body employing distributed steady blowing with 10 inputs. 17 % drag reduction are achieved using Reynolds-averaged Navier–Stokes simulations at the Reynolds number $Re_H=1.9 \times 10^5$ based on the height of the Ahmed body. The wake is controlled with seven local jet-slot actuators at all trailing edges. Symmetric operation corresponds to five independent actuator groups at top, middle, bottom, top sides and bottom sides. Each slot actuator produces a uniform jet with the velocity and angle as free parameters, yielding 10 actuation parameters as free inputs. The optimal actuation emulates boat tailing by inward-directed blowing with velocities which are comparable to the oncoming velocity. We expect that EGM will be employed as efficient optimizer in many future active flow control plants as alternative or augmentation to pure gradient search or explorative methods.


2013 ◽  
Vol 275-277 ◽  
pp. 402-408
Author(s):  
Bing Xin Wang ◽  
Zhu Hui ◽  
Zhi Gang Yang

The numerical investigations presented in this paper deal with active flow control approach at the rear end of the Ahmed body model with the slant angle of 25°.Results of the velocity, pressure and vorticity field demonstrate the main reasons that cause the pressure drag. The influence of the spanwise and streamwise vortices rolling up from the slant and the edges on the recirculation zone behind the body is examined. A control slot is set on the separated line at the conjunction of the roof and the slant. Two different actuation concepts by blowing and suction steady jets through the slot lead to a drug increase of 5.61% and a drug reduction of 13.20% with the efficiency of 12.53% respectively.


Author(s):  
Bansal Shah ◽  
Debashis Basu

Abstract A numerical study is conducted to investigate fluidic actuation with steady injection for active flow control and drag reduction in an Ahmed body. Numerical results are obtained for the unsteady three-dimensional Navier Stokes equations for both baseline as well as steady injection cases. This study examines the use of active flow control devices at the rear of the 25-deg Ahmed model to reduce drag by controlling an unsteady wake. The present work demonstrates that URANS model with grid refinement at critical locations can accurately describe the aerodynamics around the bluff body with computational time of several days compared to several weeks with traditional LES simulations. In order to modify the wake and reduce the pressure drag, active flow control technique using steady blowing was applied through a narrow slit along all rear edges of the model. The effect of inlet velocity for the baseline simulations was analyzed. Computed Results showed AFC achieves significant reduction in the drag coefficient (Cd) values over the baseline simulations.


Author(s):  
Jonathan McNally ◽  
Erik Fernandez ◽  
Rajan Kumar ◽  
Farrukh Alvi

Author(s):  
Matthew Metka

Aerodynamic drag accounts for a sizable portion of transportation energy consumption. Transportation of goods and people always involves moving objects through air, which leads to a force opposing motion. This force can account for more than 60% of power consumed by a ground vehicle, such as a car or truck, at highway speeds. There is a wide range of drag coefficient seen on ground vehicles with a strong correlation to vehicle shape. The shape of the vehicle is often determined by functional necessity or aesthetics, which places a limit on vehicle aerodynamic improvements. It is desirable to increase the aerodynamic performance of a vehicle with little penalty to these design considerations, which leads to the investigation of active flow control methods. Active flow control methods can involve a type of air jet at critical locations on the vehicle shell and require little to no shape modification. The focus of this experimental study is drag reduction on an Ahmed body vehicle analogue using a variety of configurations involving fluidic oscillators to promote attachment and reduce wake size. A fluidic oscillator is a simple device that converts a steady pressure input into a spatially oscillating jet. This type of actuator may be more efficient at influencing the surrounding flow than a steady jet. The model was tested in the OSU subsonic wind tunnel. Changes in drag were measured using a load cell mounted within the vehicle model. Different flow visualization methods were used to characterize the flow structure changes behind the model. A 7% drag decrease was realized with the 25° spanwise oscillator array configuration, attributed to the reduction of the closed recirculation bubble size. Testing showed that attachment is promoted on high angle configurations with a Coanda surface and steady blowing however this led to a drag increase, possibly due to the formation of longitudinal vortices. This indicates that future methods may require vortex control in conjunction with separation control to achieve a net base pressure increase on the high angle configurations.


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