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2D flow past an airfoil with different angles of
attack
Submitted to Submitted by
- Dr Harish Dixit -Apurva Bhagat(me13m1026)
-Harshal Gijare (me13m1028)
-Rahul Devnagare(me13p1008)
Introduction to problem
●AIM:-To use CFD as a tool to illustrate the
concept of separation and how the airfoil angle of
attack affects the flow.
●Parameters Varied 1. Reynolds Number 2. Angle
of attack
Mesh Details
● ICEM-CFD is used to prepare a Mesh
● Quadrilateral cells are used because they can be streched
easily to account for different flow gradients in different
directions
● Mesh is more fine (High aspect ratio) near the airfoil surface.
● Parabola is choosen for far field boundary it has no
discontinuties in slope.
● .msh file is generated and imported to openFoam
● No of cells-9800.
Solver Details
● IcoFoam-Incompressible solver is used.
● Incompressible N-S equations are used for discretization
in this solver.
● Finite Volume Method is used for discretization.
● Euler scheme is used for time steping and Gauss linear
scheme is used for Pressure and velocity solution.
● Courant no < 0.5
Cases Studied.
● Kinematic Viscosity is fixed = 0.01
● Flow over aerofoil is observed at different angles of attack
1 degree to 15 degree at fixed reynolds number Re=500.
Flow seperation is observed.
● Reynolds number is varied by changing free stream
velocity. Re=100 to Re=20000
Velocity Contours at different angle of
attack (Re=500)
● Alpha = 1°
● Alpha = 7°
● Alpha = 15°● Alpha = 11°
Velocity contours at Re=500,angle of
attack = 1°
Velocity contours at Re=500,angle of attack = 3°
Velocity contours at Re=500,angle of
attack = 5°
Velocity contours at Re=500,angle of
attack = 7°
Velocity contours at Re=500,angle of
attack = 9°
Velocity contours at Re=500,angle of
attack = 11°
Velocity contours at Re=500,angle of
attack = 13°
Velocity contours at Re=500,angle of
attack = 15°
Pressure variation w.r.t angle of
attack
● Angle of attack = 3° ● Angle of attack = 7°
● Angle of attack = 15°● Angle of attack = 11°
Lift & Drag coefficients w.r.t. angle
of attack
● Typical Aerofoil Lift & Drag Curve ● Lift & Drag curve of Aerofoil under
study
Velocity contours at Re=100,angle of
attack = 5°
Velocity contours at Re=500,angle of
attack = 5°
Velocity contours at Re=1000,angle of
attack = 5°
Velocity contours at Re=5000,angle of
attack = 5°
Velocity contours at Re=10000,angle of
attack = 5°
Velocity contours at Re=20000,angle of
attack = 5°
Behaviour of flow w.r.t Reynolds no. (Velocity
contours)
● Re=100 ● Re = 500 ● Re =1000
● Re = 20000● Re = 10000● Re = 5000
Variation of coefficient of drag w.r.t. Re
Conclusion
● Reynolds number has no effect on the laminar separation point.
● Increasing Reynolds number can cause a transition to turbulent boundary layer
ahead of separation and effectively move the separation point downstream.
● Coefficient of lift increases as angle of attack increases (till stall angle) at fixed
Reynold no.
●Coefficient of drag increases as angle of attack increases (at fixed Re).
●Pressure drag dominates friction drag as angle of attack increases (at fixed
Re).
● Coefficient of drag decreases as Re increases (at fixed angle of attack)
Thank You!

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Openfoam analysis of flow over aerofoil

  • 1. 2D flow past an airfoil with different angles of attack Submitted to Submitted by - Dr Harish Dixit -Apurva Bhagat(me13m1026) -Harshal Gijare (me13m1028) -Rahul Devnagare(me13p1008)
  • 2. Introduction to problem ●AIM:-To use CFD as a tool to illustrate the concept of separation and how the airfoil angle of attack affects the flow. ●Parameters Varied 1. Reynolds Number 2. Angle of attack
  • 3. Mesh Details ● ICEM-CFD is used to prepare a Mesh ● Quadrilateral cells are used because they can be streched easily to account for different flow gradients in different directions ● Mesh is more fine (High aspect ratio) near the airfoil surface. ● Parabola is choosen for far field boundary it has no discontinuties in slope. ● .msh file is generated and imported to openFoam ● No of cells-9800.
  • 4. Solver Details ● IcoFoam-Incompressible solver is used. ● Incompressible N-S equations are used for discretization in this solver. ● Finite Volume Method is used for discretization. ● Euler scheme is used for time steping and Gauss linear scheme is used for Pressure and velocity solution. ● Courant no < 0.5
  • 5. Cases Studied. ● Kinematic Viscosity is fixed = 0.01 ● Flow over aerofoil is observed at different angles of attack 1 degree to 15 degree at fixed reynolds number Re=500. Flow seperation is observed. ● Reynolds number is varied by changing free stream velocity. Re=100 to Re=20000
  • 6. Velocity Contours at different angle of attack (Re=500) ● Alpha = 1° ● Alpha = 7° ● Alpha = 15°● Alpha = 11°
  • 7. Velocity contours at Re=500,angle of attack = 1°
  • 8. Velocity contours at Re=500,angle of attack = 3°
  • 9. Velocity contours at Re=500,angle of attack = 5°
  • 10. Velocity contours at Re=500,angle of attack = 7°
  • 11. Velocity contours at Re=500,angle of attack = 9°
  • 12. Velocity contours at Re=500,angle of attack = 11°
  • 13. Velocity contours at Re=500,angle of attack = 13°
  • 14. Velocity contours at Re=500,angle of attack = 15°
  • 15. Pressure variation w.r.t angle of attack ● Angle of attack = 3° ● Angle of attack = 7° ● Angle of attack = 15°● Angle of attack = 11°
  • 16. Lift & Drag coefficients w.r.t. angle of attack ● Typical Aerofoil Lift & Drag Curve ● Lift & Drag curve of Aerofoil under study
  • 17. Velocity contours at Re=100,angle of attack = 5°
  • 18. Velocity contours at Re=500,angle of attack = 5°
  • 19. Velocity contours at Re=1000,angle of attack = 5°
  • 20. Velocity contours at Re=5000,angle of attack = 5°
  • 21. Velocity contours at Re=10000,angle of attack = 5°
  • 22. Velocity contours at Re=20000,angle of attack = 5°
  • 23. Behaviour of flow w.r.t Reynolds no. (Velocity contours) ● Re=100 ● Re = 500 ● Re =1000 ● Re = 20000● Re = 10000● Re = 5000
  • 24. Variation of coefficient of drag w.r.t. Re
  • 25. Conclusion ● Reynolds number has no effect on the laminar separation point. ● Increasing Reynolds number can cause a transition to turbulent boundary layer ahead of separation and effectively move the separation point downstream. ● Coefficient of lift increases as angle of attack increases (till stall angle) at fixed Reynold no. ●Coefficient of drag increases as angle of attack increases (at fixed Re). ●Pressure drag dominates friction drag as angle of attack increases (at fixed Re). ● Coefficient of drag decreases as Re increases (at fixed angle of attack)