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Numerical Analysis of Vertical Axis Wind 
Turbine 
Mohammad Rashedul Hasan, Md. Rasedul Islam, 
G.M Hasan Shahariar and Dr. Mohammad Mashud 
Department of Mechanical Engineering 
Khulna University of Engineering & Technology, Khulna, Bangladesh 
IFOST-2014, Bangladesh
OUTLINE 
 Introduction 
 Objectives 
 Boundary condition 
 Mesh generation 
 Assumptions 
 Mathematical formula 
 Results 
 Conclusion 
IFOST-2014, Bangladesh
INTRODUCTION 
A wind turbine is a rotating device which converts kinetic energy of wind 
into electrical energy 
Horizontal Axis Wind Turbine Vertical Axis Wind Turbine 
IFOST-2014, Bangladesh
OBJECTIVES 
 Numerical modeling of a 2D Vertical Axis Wind Turbine 
 CFD analysis of various performance parameters 
IFOST-2014, Bangladesh
BOUNDARY CONDITION 
IFOST-2014, Bangladesh
CHOOSEN AIRFOIL 
NACA 0018 
Chord length: 420mm 
 High lift 
 Better stall characteristics and 
low drag 
IFOST-2014, Bangladesh
MESH GENERATION (Rotating Domain) 
IFOST-2014, Bangladesh
MESH GENERATION (Airfoil Section) 
IFOST-2014, Bangladesh
MESH GENERATION (Stationary Domain) 
IFOST-2014, Bangladesh
MESH GENERATION (Total Structure Domain) 
 Nodes: 112929, Elements: 74532 
 Nature of the element: Quad 
 The first cell height used such that they y+ values from the flow solutions did not exceed 1 
and the criterion is used to refine the mesh for a thickness equivalent to y+=30. 
 The skewness of the cells such that the maximum is observed to be less than 0.6 
IFOST-2014, Bangladesh
SLIDING MESH TECHNIQUE 
IFOST-2014, Bangladesh
ASSUMPTIONS 
 The incompressible, unsteady Reynolds Averaged Navier Stokes (URANS) 
equations are solved using finite volume method. 
 The RNG k-ε model is adopted for the turbulence closure with standard wall 
functions on Near-wall treatment. 
 A Sliding Mesh technique is used to rotate the rotor blade. 
 Intensity of inlet and outlet turbulence is fixed to 5% and turbulence viscosity 
ratio 10 
The unsteady Reynolds Average Navier Stokes equations are make out applying 
the green-gauss cell based gradient option. 
 The SIMPLE pressure-based solver is selected having a second order implicit 
transient formulation for better result. All of the solution variables are 
calculated with second order upwind discretization scheme. 
IFOST-2014, Bangladesh
MATHEMATICAL FORMULA 
• Theoretical power, Pt= 
1 
2 
∗ 휌퐴V3 
• Practical power, Pa = Tω 
• Torque, 푇 = 
1 
2 
휌퐴CtV2 
• Angular velocity, 휔 = 
휆푉 
푅 
1 
2 
• Power co-efficient, Cp= Tω/( 
휌퐴V3 ) 
Where, T= Torque (Nm) 
A= Swept area (m2) 
=2Rl 
R= Rotor radius (m) 
V= Free stream velocity (m/s) 
ω= Angular velocity (rpm) 
ρ= Density of air (kg/m3) 
λ= Tip speed ratio 
Ct= Torque Co-efficient 
IFOST-2014, Bangladesh
MATHEMATICAL FORMULA 
IFOST-2014, Bangladesh
RESULTS 
2.00E+00 
1.50E+00 
1.00E+00 
5.00E-01 
0.00E+00 
-5.00E-01 
-1.00E+00 
0 50 100 150 200 250 300 350 400 
Torque coefficient, Ct 
Azimuthal angle,θ 
Figure 1: Torque coefficient vs Azimuthal angle for tip speed ratio (λ=2.0) 
6.00E+00 
5.00E+00 
4.00E+00 
3.00E+00 
2.00E+00 
1.00E+00 
0.00E+00 
-1.00E+00 
-2.00E+00 
0 50 100 150 200 250 300 350 400 
Torque coefficient, Ct 
Azimuthal angle,θ 
Figure 2: Torque coefficient vs Azimuthal angle for tip speed ratio (λ=4.5) 
IFOST-2014, Bangladesh
RESULTS (Cont’d) 
Figure 3: Power co-efficient vs Tip speed ratio for 9 m/s 
* Biadgo Mulugeta Asressa, Simonović Aleksandarb, Komarov Draganb, Stupar Slobodanb “Numerical and Analytical Investigation 
of Vertical Axis Wind Turbine”, FME Transactions 2013, vol. 41, iss. 1, pp. 49-58 
IFOST-2014, Bangladesh
RESULTS (Cont’d) 
IFOST-2014, Bangladesh
CONCLUSION 
 In this thesis, a 2-D numerical analysis has been completed using sliding mesh 
technique, to predict the efficiency or power co-efficient of vertical axis wind 
turbine 
 From the performance curve, an optimum power co-efficient 0.34 is obtained at 
tip speed ratio 4.5 
 This results may helpful for practical implementation of vertical axis wind 
turbine 
IFOST-2014, Bangladesh
REFERENCES 
[1] Sathyajith, M, “Wind Energy Fundamentals, Resource Analysis and Economics,” Springer-Verlag 
Berlin Heidelberg, Netherlands, 2006. 
[2] Claessens, M.C., “The Design and Testing of Airfoils for Application in Small Vertical Axis Wind 
turbines,” Delft University, November 2009. 
[3] Louis Angelo Danao, Jonathan Edwards, Okeoghene Eboibi , Robert Howell, “A numerical 
investigation into the influence of unsteady wind on the performance and aerodynamics of a 
vertical axis wind turbine,” Proceedings of the World Congress on Engineering 2013 Vol III, WCE 
2013, July 3 - 5, 2013, London, U.K. 
[4] Asress Mulugeta Biadgo, Aleksandar Simonovic, Dragan Komarov, Slobodan Stupar, “Numerical 
and Analytical Investigation of Vertical Axis Wind Turbine,” FME Transactions (2013) 41, pp. 49-58. 
[5] Chao Li, Songye Zhu, You-lin Xu, Yiqing Xiao, “2.5D large eddy simulation of vertical axis 
wind turbine in consideration of high angle of attack flow,” Renewable Energy, Volume 51, March 2013, 
pp 317-330. 
[6] Naveed Durrani, Haris Hameed, Hammad Rahman and Sajid Raza Chaudhry, “A detailed 
Aerodynamic Design and analysis of a 2D vertical axis wind turbine using sliding mesh in CFD,” 
49th AIAA Aerospace Sciences Meeting including the New Horizons Forum and Aerospace Exposition 
4-7 January 2011, Orlando, Florida. 
[7] Marco Raciti Castelli, Stefano De Betta and Ernesto Benini, “Effect of Blade Number on a Straight- 
Bladed Vertical-Axis Darreius Wind Turbine”, World Academy of Science, Engineering and Technology 
61 2012. 
IFOST-2014, Bangladesh
Thanks To All 
IFOST-2014, Bangladesh

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Numerical analysis of Vertical Axis Wind Turbine

  • 1. Numerical Analysis of Vertical Axis Wind Turbine Mohammad Rashedul Hasan, Md. Rasedul Islam, G.M Hasan Shahariar and Dr. Mohammad Mashud Department of Mechanical Engineering Khulna University of Engineering & Technology, Khulna, Bangladesh IFOST-2014, Bangladesh
  • 2. OUTLINE  Introduction  Objectives  Boundary condition  Mesh generation  Assumptions  Mathematical formula  Results  Conclusion IFOST-2014, Bangladesh
  • 3. INTRODUCTION A wind turbine is a rotating device which converts kinetic energy of wind into electrical energy Horizontal Axis Wind Turbine Vertical Axis Wind Turbine IFOST-2014, Bangladesh
  • 4. OBJECTIVES  Numerical modeling of a 2D Vertical Axis Wind Turbine  CFD analysis of various performance parameters IFOST-2014, Bangladesh
  • 6. CHOOSEN AIRFOIL NACA 0018 Chord length: 420mm  High lift  Better stall characteristics and low drag IFOST-2014, Bangladesh
  • 7. MESH GENERATION (Rotating Domain) IFOST-2014, Bangladesh
  • 8. MESH GENERATION (Airfoil Section) IFOST-2014, Bangladesh
  • 9. MESH GENERATION (Stationary Domain) IFOST-2014, Bangladesh
  • 10. MESH GENERATION (Total Structure Domain)  Nodes: 112929, Elements: 74532  Nature of the element: Quad  The first cell height used such that they y+ values from the flow solutions did not exceed 1 and the criterion is used to refine the mesh for a thickness equivalent to y+=30.  The skewness of the cells such that the maximum is observed to be less than 0.6 IFOST-2014, Bangladesh
  • 11. SLIDING MESH TECHNIQUE IFOST-2014, Bangladesh
  • 12. ASSUMPTIONS  The incompressible, unsteady Reynolds Averaged Navier Stokes (URANS) equations are solved using finite volume method.  The RNG k-ε model is adopted for the turbulence closure with standard wall functions on Near-wall treatment.  A Sliding Mesh technique is used to rotate the rotor blade.  Intensity of inlet and outlet turbulence is fixed to 5% and turbulence viscosity ratio 10 The unsteady Reynolds Average Navier Stokes equations are make out applying the green-gauss cell based gradient option.  The SIMPLE pressure-based solver is selected having a second order implicit transient formulation for better result. All of the solution variables are calculated with second order upwind discretization scheme. IFOST-2014, Bangladesh
  • 13. MATHEMATICAL FORMULA • Theoretical power, Pt= 1 2 ∗ 휌퐴V3 • Practical power, Pa = Tω • Torque, 푇 = 1 2 휌퐴CtV2 • Angular velocity, 휔 = 휆푉 푅 1 2 • Power co-efficient, Cp= Tω/( 휌퐴V3 ) Where, T= Torque (Nm) A= Swept area (m2) =2Rl R= Rotor radius (m) V= Free stream velocity (m/s) ω= Angular velocity (rpm) ρ= Density of air (kg/m3) λ= Tip speed ratio Ct= Torque Co-efficient IFOST-2014, Bangladesh
  • 15. RESULTS 2.00E+00 1.50E+00 1.00E+00 5.00E-01 0.00E+00 -5.00E-01 -1.00E+00 0 50 100 150 200 250 300 350 400 Torque coefficient, Ct Azimuthal angle,θ Figure 1: Torque coefficient vs Azimuthal angle for tip speed ratio (λ=2.0) 6.00E+00 5.00E+00 4.00E+00 3.00E+00 2.00E+00 1.00E+00 0.00E+00 -1.00E+00 -2.00E+00 0 50 100 150 200 250 300 350 400 Torque coefficient, Ct Azimuthal angle,θ Figure 2: Torque coefficient vs Azimuthal angle for tip speed ratio (λ=4.5) IFOST-2014, Bangladesh
  • 16. RESULTS (Cont’d) Figure 3: Power co-efficient vs Tip speed ratio for 9 m/s * Biadgo Mulugeta Asressa, Simonović Aleksandarb, Komarov Draganb, Stupar Slobodanb “Numerical and Analytical Investigation of Vertical Axis Wind Turbine”, FME Transactions 2013, vol. 41, iss. 1, pp. 49-58 IFOST-2014, Bangladesh
  • 18. CONCLUSION  In this thesis, a 2-D numerical analysis has been completed using sliding mesh technique, to predict the efficiency or power co-efficient of vertical axis wind turbine  From the performance curve, an optimum power co-efficient 0.34 is obtained at tip speed ratio 4.5  This results may helpful for practical implementation of vertical axis wind turbine IFOST-2014, Bangladesh
  • 19. REFERENCES [1] Sathyajith, M, “Wind Energy Fundamentals, Resource Analysis and Economics,” Springer-Verlag Berlin Heidelberg, Netherlands, 2006. [2] Claessens, M.C., “The Design and Testing of Airfoils for Application in Small Vertical Axis Wind turbines,” Delft University, November 2009. [3] Louis Angelo Danao, Jonathan Edwards, Okeoghene Eboibi , Robert Howell, “A numerical investigation into the influence of unsteady wind on the performance and aerodynamics of a vertical axis wind turbine,” Proceedings of the World Congress on Engineering 2013 Vol III, WCE 2013, July 3 - 5, 2013, London, U.K. [4] Asress Mulugeta Biadgo, Aleksandar Simonovic, Dragan Komarov, Slobodan Stupar, “Numerical and Analytical Investigation of Vertical Axis Wind Turbine,” FME Transactions (2013) 41, pp. 49-58. [5] Chao Li, Songye Zhu, You-lin Xu, Yiqing Xiao, “2.5D large eddy simulation of vertical axis wind turbine in consideration of high angle of attack flow,” Renewable Energy, Volume 51, March 2013, pp 317-330. [6] Naveed Durrani, Haris Hameed, Hammad Rahman and Sajid Raza Chaudhry, “A detailed Aerodynamic Design and analysis of a 2D vertical axis wind turbine using sliding mesh in CFD,” 49th AIAA Aerospace Sciences Meeting including the New Horizons Forum and Aerospace Exposition 4-7 January 2011, Orlando, Florida. [7] Marco Raciti Castelli, Stefano De Betta and Ernesto Benini, “Effect of Blade Number on a Straight- Bladed Vertical-Axis Darreius Wind Turbine”, World Academy of Science, Engineering and Technology 61 2012. IFOST-2014, Bangladesh
  • 20. Thanks To All IFOST-2014, Bangladesh