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Design & Analysis of a Helical 
cross-flow Hydrokinetic Turbine (CFHT) 
Using CFD 
Project Guide 
Dr. Pravin P Patil 
(Dean Research) 
Graphic Era University, Dehradun 
Submitted by : 
Arpit Dwivedi (2002689) 
Himanshu Joshi (2003236) 
Anish Anand (2002673)
CONTENTS 
Introduction 
Project motivation 
Cross flow Turbine and Power Generation 
Literature Survey 
Important Parameters 
Design Methodology 
Design Parameters & Boundary Conditions 
Results 
Conclusions 
Scope of Future Work 
References
INTRODUCTION 
Need for Untainted , environmentally benign 
Energy . (Why Renewables ?) 
K.E of water Currents in Rivers, Oceans & 
Estuaries 
Development of wind turbines & Research in 
MHK. 
Axial Flow Vs Cross Flow Turbines 
Drag Type Vs Lift Types Turbines
Project Motivation 
Energy Crisis and its impact 
250000 MW hydro potential in India 
Still only 14.5 % is utilized (a lot of scope there……………….!) 
Research in Wind Turbine analysis has reached a saturation level . 
The Industry for Marine Hydrokinetic Turbine is still in its 
infancy 
Concepts of wind turbine analysis are utilized there, 
literature is still to be developed (intensive research going on)
Cross Flow Turbine and Power 
Generation 
Rotates at twice the velocity of water current flow. 
Rotates in the same direction, independent of water flow direction 
No fluctuations in Torque 
No cavitation even at Higher speeds 
Modular in Design 
 In the report Gorlov prepared for the DOE(dept of energy) in 
1998 he claims an efficiency value of “about 35%" for a 3 bladed, 
24" diameter by 34" height turbine in free water flow of 5 ft/s .
Literature Survey 
A wide variety of Literature regarding Design and Analysis of wind & MHK 
Turbines was done. 
These were the findings. 
The power available is proportional to the velocity cubed. 
The flow field is unsteady and 3-dimensional 
Drag and lift coefficients are largely dependent on angle of attack. 
NACA Symmetrical profiles are selected as forces reverse after 180 degrees 
of rotation 
The Drag and Lift forces generated due to flow, generate a torque about the 
central axis.
Important Parameters 
NACA 0018 Symmetrical 
profile 
With 18 % thickness to chord 
length ratio 
Blade Profile : Cubic Spline 
Pitch = 706 mm 
Taper angle = 2
Design Methodology 
Solidity Ratio ( σ) = nC/пd 
Inclination Angle (Φ) = tan‾1(nh/пd) 
Figure 2 Top View (Gorlov Turbine)
Modelling was done in Catia V5 with modifications in Ansys 14.5
Design Parameters & Boundary 
Conditions
MESHING 
Meshing was chosen as fine and relevance was taken 0. 
No of nodes obtained were 1329267, and no of elements 
created were 7447633. Cross section of the turbine 
Fine meshing across the region of 
turbine cross section. 
Meshing on Proximity and 
Curvature
Aluminium 5086 (marine grade aluminium) was defined with density of 
2660 kg/m3. Water was selected as a fluid medium. 
After boundary conditions were applied the hydrostatic pressure was 
defined according to the depth of the turbine from the free surface and the 
inlet velocity was chosen as 1.5m/sec and the pressure was taken as 
104255 pascals(Pa) which was kept uniform at inlet and outlet.
RESULTS 
Figure : (a) Profile of Dynamic Pressure (b) Contours of 
Pressure Coefficient
FIGURE : (a) Profile of Velocity Magnitude (b) Contours of Turbulent 
Kinetic Energy
Figure : (a)Profile of Velocity in Y Direction (b) Velocity Vector Colored by 
Velocity magnitude
Wall Shear Vector
SCALED RESIDUES
Cl and Cd
Conclusions and Future work 
This project specifies the parameters on which the static analysis of a cross flow 
turbine depends. It specifies the difference between usual wind turbine theories and 
their applicability in tidal turbine analysis. 
This successful implementation of this project will help in eradicating power 
demands. 
This project is capable of producing energy both in small and large magnitudes with 
very less cost implementation than any other hydro power project which involve 
constructions of large dams and then tunnels. Thus this project has a vast scope in a 
country like India where number of seasonal and non seasonal river flows.
FUTURE SCOPE 
The same analysis can be performed for varying solidity ratio, by 
changing the no. of blades or the chord length of the profile or 
changing the radius of the plate, it’s dependency can be checked and 
verified. 
We have performed the analysis for tip speed ratio = 0 , behavior 
can be studied by varying it. 
Torque and power can be calculated by defining specific UDF(user 
defined functions) 
Dynamic Analysis of the rotating turbine can be done by using 
SRF(Single reference model), MRF(Multiple Reference model) and 
Sliding Mesh Technique.
Due to it’s wide applicability in Hydrokinetic applications, the 
analysis can be performed for different areas with different 
boundary conditions. 
As per literature Survey the Results obtained by CFD studies 
are in accordance with the experimental investigations. However 
with regard to local Flora and fauna , experimental investigation 
can be performed by making a suitable scale model and 
calculation of parameters.
REFERENCES 
[1] Oliver Paish , “Small hydro power: technology and current status” Renewable 
and Sustainable Energy Reviews 6 (2002) 537–556 
[2] http://www.gcktechnology.com/GCK/pg2.html 
[3] Energy Alternatives India (EAI), http://www.eai.in/ref/ae/hyd/hyd.html 
[4] S. Latin and C. Osorio. Simulation and evaluation of a straight-bladed Darrieus-type 
cross flow marine turbine. Journal of Scientific & Industrial Research, 69 
(12):906–912, 2010. 
[5] S. Li and Y. Li. Numerical study on the performance effect of solidity on the 
straight-bladed vertical axis wind turbine. 2010 Asia-Pacific Power and Energy 
Engineering Conference, APPEEC 2010 - Proceedings, pages IEEE Power and 
Energy Society (PES); State Grid of China; Siemens Ltd.; Sichuan University; 
[6] Experimental and Analytical Study of Helical Cross-Flow Turbines for a Tidal 
Micropower Generation System Adam L. Niblick 
[7] M.R. Castelli and E. Benini. Effect of Blade Inclination Angle on a Darrieus 
Wind Turbine. Journal of Turbomachinery-Transactions of the ASME, 134(3), 
2012.
[8] P. Fraenkel. Tidal turbines harness the power of the sea. Reinforced Plastics, 48 
(6):44 { 47, 2004. 
[9] S. Antheaume, T. Maitre, and J. Achard. Hydraulic darrieus turbines e_ciency 
for free uid ow conditions versus power farms conditions. Renewable Energy, 
33(10):2186 { 2198, 2008. 
[10] J. Zanette, D. Imbault, and A. Tourabi. A design methodology for cross ow 
water turbines. Renewable Energy, 35(5):997 { 1009, 2010. 
[11] A.S. Bahaj and L.E. Myers. Fundamentals applicable to the utilisation of marine 
current turbines for energy production. Renewable Energy, 28(14):2205 { 2211, 
2003. 
[12] W.M.J. Batten, A.S. Bahaj, A.F. Molland, and J.R. Chaplin. Hydrodynamics 
of marine current turbines. Renewable Energy, 31(2):249{256, Feb 2006. 
[13] P. Fraenkel. Windmills below the sea: A commercial reality soon? Refocus, 5 
(2):46 { 50, 2004. 
[14] T. Matre, J.L. Achard, L. Guittet, and C. Ploesteanu. Marine turbine devel-opment: 
numerical and experimental investigations. Scientific Bulletine of the 
Politehnica University of Timisoara, 50(64):59–66, 2005 
[15] T Javaherchi. Numerical modeling of tidal turbines: Methodology development 
and potential physical environmental effects. Master’s thesis, University of Wash-ington, 
2010. 
[16] X. Sun, J. P. Chick, and I. G. Bryden. Laboratory-scale simulation of energy 
extraction from tidal currents. Renewable Energy, 33:1267{1274, 2008.

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Design & Analysis of a Helical Cross Flow Turbine

  • 1. Design & Analysis of a Helical cross-flow Hydrokinetic Turbine (CFHT) Using CFD Project Guide Dr. Pravin P Patil (Dean Research) Graphic Era University, Dehradun Submitted by : Arpit Dwivedi (2002689) Himanshu Joshi (2003236) Anish Anand (2002673)
  • 2. CONTENTS Introduction Project motivation Cross flow Turbine and Power Generation Literature Survey Important Parameters Design Methodology Design Parameters & Boundary Conditions Results Conclusions Scope of Future Work References
  • 3. INTRODUCTION Need for Untainted , environmentally benign Energy . (Why Renewables ?) K.E of water Currents in Rivers, Oceans & Estuaries Development of wind turbines & Research in MHK. Axial Flow Vs Cross Flow Turbines Drag Type Vs Lift Types Turbines
  • 4. Project Motivation Energy Crisis and its impact 250000 MW hydro potential in India Still only 14.5 % is utilized (a lot of scope there……………….!) Research in Wind Turbine analysis has reached a saturation level . The Industry for Marine Hydrokinetic Turbine is still in its infancy Concepts of wind turbine analysis are utilized there, literature is still to be developed (intensive research going on)
  • 5. Cross Flow Turbine and Power Generation Rotates at twice the velocity of water current flow. Rotates in the same direction, independent of water flow direction No fluctuations in Torque No cavitation even at Higher speeds Modular in Design  In the report Gorlov prepared for the DOE(dept of energy) in 1998 he claims an efficiency value of “about 35%" for a 3 bladed, 24" diameter by 34" height turbine in free water flow of 5 ft/s .
  • 6. Literature Survey A wide variety of Literature regarding Design and Analysis of wind & MHK Turbines was done. These were the findings. The power available is proportional to the velocity cubed. The flow field is unsteady and 3-dimensional Drag and lift coefficients are largely dependent on angle of attack. NACA Symmetrical profiles are selected as forces reverse after 180 degrees of rotation The Drag and Lift forces generated due to flow, generate a torque about the central axis.
  • 7. Important Parameters NACA 0018 Symmetrical profile With 18 % thickness to chord length ratio Blade Profile : Cubic Spline Pitch = 706 mm Taper angle = 2
  • 8. Design Methodology Solidity Ratio ( σ) = nC/пd Inclination Angle (Φ) = tan‾1(nh/пd) Figure 2 Top View (Gorlov Turbine)
  • 9. Modelling was done in Catia V5 with modifications in Ansys 14.5
  • 10. Design Parameters & Boundary Conditions
  • 11. MESHING Meshing was chosen as fine and relevance was taken 0. No of nodes obtained were 1329267, and no of elements created were 7447633. Cross section of the turbine Fine meshing across the region of turbine cross section. Meshing on Proximity and Curvature
  • 12. Aluminium 5086 (marine grade aluminium) was defined with density of 2660 kg/m3. Water was selected as a fluid medium. After boundary conditions were applied the hydrostatic pressure was defined according to the depth of the turbine from the free surface and the inlet velocity was chosen as 1.5m/sec and the pressure was taken as 104255 pascals(Pa) which was kept uniform at inlet and outlet.
  • 13.
  • 14. RESULTS Figure : (a) Profile of Dynamic Pressure (b) Contours of Pressure Coefficient
  • 15. FIGURE : (a) Profile of Velocity Magnitude (b) Contours of Turbulent Kinetic Energy
  • 16. Figure : (a)Profile of Velocity in Y Direction (b) Velocity Vector Colored by Velocity magnitude
  • 20. Conclusions and Future work This project specifies the parameters on which the static analysis of a cross flow turbine depends. It specifies the difference between usual wind turbine theories and their applicability in tidal turbine analysis. This successful implementation of this project will help in eradicating power demands. This project is capable of producing energy both in small and large magnitudes with very less cost implementation than any other hydro power project which involve constructions of large dams and then tunnels. Thus this project has a vast scope in a country like India where number of seasonal and non seasonal river flows.
  • 21. FUTURE SCOPE The same analysis can be performed for varying solidity ratio, by changing the no. of blades or the chord length of the profile or changing the radius of the plate, it’s dependency can be checked and verified. We have performed the analysis for tip speed ratio = 0 , behavior can be studied by varying it. Torque and power can be calculated by defining specific UDF(user defined functions) Dynamic Analysis of the rotating turbine can be done by using SRF(Single reference model), MRF(Multiple Reference model) and Sliding Mesh Technique.
  • 22. Due to it’s wide applicability in Hydrokinetic applications, the analysis can be performed for different areas with different boundary conditions. As per literature Survey the Results obtained by CFD studies are in accordance with the experimental investigations. However with regard to local Flora and fauna , experimental investigation can be performed by making a suitable scale model and calculation of parameters.
  • 23. REFERENCES [1] Oliver Paish , “Small hydro power: technology and current status” Renewable and Sustainable Energy Reviews 6 (2002) 537–556 [2] http://www.gcktechnology.com/GCK/pg2.html [3] Energy Alternatives India (EAI), http://www.eai.in/ref/ae/hyd/hyd.html [4] S. Latin and C. Osorio. Simulation and evaluation of a straight-bladed Darrieus-type cross flow marine turbine. Journal of Scientific & Industrial Research, 69 (12):906–912, 2010. [5] S. Li and Y. Li. Numerical study on the performance effect of solidity on the straight-bladed vertical axis wind turbine. 2010 Asia-Pacific Power and Energy Engineering Conference, APPEEC 2010 - Proceedings, pages IEEE Power and Energy Society (PES); State Grid of China; Siemens Ltd.; Sichuan University; [6] Experimental and Analytical Study of Helical Cross-Flow Turbines for a Tidal Micropower Generation System Adam L. Niblick [7] M.R. Castelli and E. Benini. Effect of Blade Inclination Angle on a Darrieus Wind Turbine. Journal of Turbomachinery-Transactions of the ASME, 134(3), 2012.
  • 24. [8] P. Fraenkel. Tidal turbines harness the power of the sea. Reinforced Plastics, 48 (6):44 { 47, 2004. [9] S. Antheaume, T. Maitre, and J. Achard. Hydraulic darrieus turbines e_ciency for free uid ow conditions versus power farms conditions. Renewable Energy, 33(10):2186 { 2198, 2008. [10] J. Zanette, D. Imbault, and A. Tourabi. A design methodology for cross ow water turbines. Renewable Energy, 35(5):997 { 1009, 2010. [11] A.S. Bahaj and L.E. Myers. Fundamentals applicable to the utilisation of marine current turbines for energy production. Renewable Energy, 28(14):2205 { 2211, 2003. [12] W.M.J. Batten, A.S. Bahaj, A.F. Molland, and J.R. Chaplin. Hydrodynamics of marine current turbines. Renewable Energy, 31(2):249{256, Feb 2006. [13] P. Fraenkel. Windmills below the sea: A commercial reality soon? Refocus, 5 (2):46 { 50, 2004. [14] T. Matre, J.L. Achard, L. Guittet, and C. Ploesteanu. Marine turbine devel-opment: numerical and experimental investigations. Scientific Bulletine of the Politehnica University of Timisoara, 50(64):59–66, 2005 [15] T Javaherchi. Numerical modeling of tidal turbines: Methodology development and potential physical environmental effects. Master’s thesis, University of Wash-ington, 2010. [16] X. Sun, J. P. Chick, and I. G. Bryden. Laboratory-scale simulation of energy extraction from tidal currents. Renewable Energy, 33:1267{1274, 2008.