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STEADY STATE EXTERNAL FLOW SIMULATION OVER AN AHMED BODY TO STUDY ITS AERODYNAMIC PROPERTIES USING ANSYS FLUENT AIM Our aim is to simulate a steady state external flow over an Ahmed body to study the properties of lift and drag using ANSYS FLUENT and perform grid independent study. THEORY/EQUATIONS/FORMULAE USED ANSYS…
Ramkumar Venkatachalam
updated on 29 Jan 2022
STEADY STATE EXTERNAL FLOW SIMULATION OVER AN AHMED BODY TO STUDY ITS AERODYNAMIC PROPERTIES USING ANSYS FLUENT
Our aim is to simulate a steady state external flow over an Ahmed body to study the properties of lift and drag using ANSYS FLUENT and perform grid independent study.
ANSYS FLUENT academic version CFD package is used to carry out the simulation. It is a user friendly interface which provides high productivity and easy-to-use workflows. Workbench contains all workflow needed for solving a problem such as pre-processing, solving and post-processing.
Structure of ANSYS FLUENT simulations
The basic steps for a simulation are as follows,
Ahmed Body
Ahmed body is a representation of a standard passenger car. Actually a passenger car has complex design in reality but the Ahmed body is a simplified design which has car like features. The flow over Ahmed body helps us capturing the essential features such as lift, drag and its coefficients, flow behavior such as velocity profiles around the wall. So it is majorly used to validate the CFD codes and understand the behavior of flow and start improvising. It was first defined and characterized in the experimental work of S.R. Ahmed in 1984, as the name suggests Ahmed Body.
Fig: Dimensions of Ahmed Body
Concept of Wall Function
Wall function is an important defining criterion that tells the solver about the approach to solve near the boundary wall as it’s different for every case.
The boundary wall may be laminar or turbulent as well.
There are three regions in the turbulent boundary layer.
As our problem requires the study of essential features such as lift, drag, drag coefficient on the Ahmed Body wall, so wall treatment is required. Also it’s a turbulent flow, so we need to choose a turbulence model, and each model will have a wall function.
K-epsilon is best suited for flow away from the walls and K-omega is best suited for flow near the walls, high Reynolds number. Our interest lies in the average values over the wall such as lift, drag where the choice between the above mentioned turbulence model does not make a difference.
Y+ value
Y+ value is used to determine the first cell height based on whether to use wall function or not. Wall functions are required as the gradients of velocity, temperature, etc. close to the wall are large.
Y+ = y * Ut
ν
where y is Cell height, Ut is frictional velocity, and ν is Kinematic Viscosity of the fluid.
There are two approaches for solving i.e,
Problem – Flow over a Cylinder
Calculation
Reference values - Ahmed Body
Length = 1.044 m, Breadth = 0.389 m, Height = 0.288 m
Projected Area = Breadth x Height = 0.065 m2
Fluid chosen for the problem – Air
Density of Air = 1.225 kg/m3, Dynamic viscosity = 1.7894e-5 kg/ms, Velocity of fluid = 25 m/s, Characteristic length = 1.044 m
So, Reynolds Number, Re = 1.78e-6
Calculation of first cell height with an assumption of Y+ = 50 (As K-Epsilon Turbulence Model is used)
Skin Friction Coefficient, Cf
Cf = 0.058 * Re(-0.2) [External Flow]
Cf = 0.079 * Re(-0.25) [Internal Flow]
So, Cf = 0.00323 [using External Flow Eq.]
Wall Shear Stress, τw
τw = 0.5Cf ρu2
τw = 1.236 N/m2
Frictional Velocity, Ut
Ut = (τw / ρ)(1/2)
Ut = 1 m/s
Cell Height, y
y = Y+ * ν
Ut
Where y = 0.73 mm
Lift, Drag and Coefficient of drag needs to be calculated for different mesh, so the size of elements in body sizing, face sizing differs for each setting.
3. PROCEDURE
Part 1
Part 2
4. NUMERICAL ANALYSIS (Software used – ANSYS 2018 R1)
The 3D geometry of Ahmed Body with flow domain is created in SpaceClaim as per the figure given below. In order to study the external flow behavior, the domain width of 0.5m is created. Also a space of 2m before the Ahmed body and more importantly 5m after the Ahmed body is created to capture the flow.
3D Geometry with the flow domain – Ahmed Body
Fig: Edge Sizing on the wall
Fig: Inflation Layers
Fig: Final Mesh for the complete domain
Fig: Boundaries for the complete domain
4. Energy equation was switched off for the analysis process as we are not interested in temperature of the system.
5. K-epsilon turbulence model was used for the analysis as the Reynolds number used for simulation is in the range of 1780000.
6. The fluid material chosen is air.
7. Plane named as cut-plane is created at -0.1 m in z-plane from the centre of the geometry as shown in the below figure to observe the velocity and pressure contours in the domain.
8. Report definitions of forces on the cut-plane are set up as we are interested in the physical quantity such as Lift, Drag and Coefficient of drag.
9. Convergence Criteria are checked as it might take some more time and we want to run the complete number of iterations or time step set for the simulation in order to witness the physics behind of the problem.
10. Solution methods – SIMPLE Scheme used for Pressure-Velocity coupling and the methods for Spatial Discretization are as per the below image.
11. Hybrid initialization is done and numbers of iterations are set for running the steady simulation and time step size and number of time step for transient simulation.
12. Velocity and pressure contours are set in order to monitor the fluctuations during run time and also animations are added.
Initial Setup and Boundary Condition
Zone |
Type |
Boundary Condition |
Additional conditions (if any) |
Inlet |
Velocity - Inlet |
Velocity – 25 m/s, |
Steady State, Transient State, Pressure Based, Absolute
Switched OFF Energy equation
Turbulence Model – k-epsilon & k-omega |
Outlet |
Pressure - Outlet |
Gauge pressure of 0Pa |
|
Symmetry |
Symmetry |
Symmetry |
|
Wall |
Wall |
Stationary wall without slip |
5. RESULTS
Fig: Baseline Mesh Fig: Case 1
Fig: Case 2 Fig: Case 3 k-e
Fig: Case 3 k-omega
Fig: Baseline Mesh Fig: Case 1
Fig: Case 2 Fig: Case 3 k-e
Fig: Case 3 k-w
Fig: Baseline Mesh Fig: Case 1
Fig: Case 2 Fig: Case 3 k-e
Fig: Case 3 k-w
Fig: Baseline Mesh Fig: Case 1
Fig: Case 2 Fig: Case 3 k-e
Fig: Case 3 k-w
Fig: Baseline Mesh Fig: Case 1
Fig: Case 2 Fig: Case 3 k-e
Fig: Case 3 k-w
Fig: Baseline Mesh Fig: Case 1
Fig: Case 2 Fig: Case 3 k-e
Fig: Case 3 k-w
Fig: Baseline Mesh Fig: Case 1
Fig: Case 2 Fig: Case 3 k-e
Fig: Case 3 k-w
Fig: Baseline Mesh
Fig: Case 1 Fig: Case 2
Fig: Case 3 k-e Fig: Case 3 k-w
Fig: Baseline Mesh Fig: Case 1
Fig: Case 2 Fig: Case 3 k-e
Fig: Case 3 k-w
Grid Independent Study
6. CONCLUSION
7. REFERENCES
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