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A numerical study of the effect of the central shaft on the

performance of a VAWT

Citation for published version (APA):

Rezaeiha, A., Kalkman, I. M., & Blocken, B. (2016). A numerical study of the effect of the central shaft on the performance of a VAWT. In XIV Conference of the Italian Association for Wind Engineering (IN-VENTO 2016), 25-28 September 2016, Terni, Italy

Document license: CC BY

Document status and date: Published: 25/09/2016

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IN-VENTO 2016 XIV Conference of the Italian Association for Wind Engineering

25-28 September 2016, Terni, Italy

A numerical study of the effect of the central shaft on the performance of a

VAWT

Abdolrahim Rezaeiha1, Ivo Kalkman1 and Bert Blocken1,2

1Building Physics and Services, Department of the Built Environment, Eindhoven University of Technology, P.O. Box 513, 5600 MB Eindhoven, The Netherlands

2Building Physics Section, Department of Civil Engineering, KU Leuven, Kasteelpark Arenberg 40 – Bus 2447, 3001 Leuven, Belgium

Corresponding author: A. Rezaeiha, a.rezaeiha@tue.nl

Abstract

Vertical axis wind turbines (VAWT) have recently received growing interest for application in urban environments due to their omni-directional capabilities. However, further research is required to optimize their performance. The central shaft is an inseparable part of a VAWT whose effect on turbine performance is currently not fully understood. In this paper the effect of the central shaft on the power coefficient (CP) and thrust coefficient (CT) of a VAWT is studied for different shaft-to-turbine diameter ratios (γ) using 2D unsteady Reynolds-Averaged Navier-Stokes (URANS) CFD simulations. The study shows that the presence of the shaft with γ=4% results in a 2.5% and 1.1% reduction in CP and CT, respectively. This is mainly due to the wake of the shaft which results in a region of lower velocity directly downstream and a dip in the moment coefficient and thrust force at an azimuthal position of 270o.

1 Introduction

Vertical axis wind turbines have regained interest during the last decade due to their omni-directional capabilities and the growing interest in harvesting wind energy in urban environments where this feature is highly desirable (Gsanger & Pitteloud, 2015). However, a significantly lower amount of research in the past three decades has resulted in VAWT performance falling behind that of their horizontal axis counterparts. Further research is therefore required on performance optimization of VAWT in urban environments (Rezaeiha et al., 2016b). Several research efforts have highlighted the complexities of the flow around a VAWT (Rezaeiha et al., 2016a; Simão Ferreira et al., 2008; Tescione et al., 2014). The central shaft is an inseparable component of the turbine which affects the flow in the centerline of the turbine, though its effect on turbine performance is largely unknown. Therefore, the current study investigates the effect of the central shaft with different shaft-to-turbine diameter ratios on the power and thrust coefficient of a VAWT in order to develop effective optimization strategies. The results of the CFD simulation are validated with experimental data.

2 VAWT geometry, mesh and computational settings

A 2-bladed H-type VAWT with straight blades was simulated. The turbine has a diameter (D) of 1 m and a solidity (σ) of 0.12. The blade sections were typical VAWT symmetric NACA0018 airfoil with a chord (c) of 0.06 D oriented normal to the radial line from the center of rotation. The turbine shaft diameter was 0.04 D (γ=4%) and the shaft was rotating in the same direction as the turbine. The turbine was operated at a tip speed ratio (λ) of 4.5. The freestream velocity was 9.3 m/s and the rotational speed (ω) is 84 rad/s. The approach-flow turbulence intensity of the freestream was 5% while the incident flow turbulence intensity was 3.96% (Blocken et al., 2007). The simulation was performed on a computational domain of 40D length × 20D width and a mesh of 526,006 cells using

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REZAEIHA et al. A numerical study of the effect of central shaft on the performance of a VAWT

the commercial CFD software package ANSYS Fluent version 16.1 using URANS calculations. A steady-state RANS result was used for initialization and final data were sampled after 20 revolutions of the turbine. Turbulence modeling was done using the 4-equation transition SST turbulence model (Menter et al., 2006). Sensitivity analyses for domain and mesh size, azimuthal increment and number of revolutions of the turbine were performed to ensure accuracy of the results.

3 Results and discussion

In order to validate the results normalized instantaneous streamwise velocities at x/R of 1.5 were compared with experimental results (Tescione et al., 2014) for which the turbine geometry and operational settings were the same. The average deviation from the experimental data was 12%. Comparison of the results for cases with and without the central shaft showed that the wake generated by the shaft, visible as a region of lower velocity, results in temporary reductions of the moment coefficient and thrust force when the blade passes downstream of the shaft. This resulted in a 2.5% reduction in CP and a 1.1% reduction in CT compared to the case without the shaft (see Table 1) for γ=4%. The full paper will include results for other γ-values as well as a comparison with a stationary shaft with a rough surface.

Table 1. VAWT performance parameters for the case with and without a rotating central shaft. Performance parameter Shaft-to-turbine diameter ratio CP CT

Without shaft - 0.40 0.89

With shaft 4% 0.39 0.88

4 Conclusion

CFD simulations of a VAWT with and without a rotating central shaft were conducted using URANS calculations with Transition SST turbulence modeling. The results showed that the central shaft with a shaft-to-turbine diameter ratio of 4% results in a 2.5% reduction in CP and a 1.1% reduction in CT compared to the case without shaft. The final results including various γ-values might be used to minimize the shaft effect.

References

Blocken, B., Stathopoulos, T. and Carmeliet, J., 2007. CFD simulation of the atmospheric boundary layer: wall function problems. Atmospheric Environment 41, 238-252.

Gsanger, S. and Pitteloud, J.D., 2015. 2015 small wind world report summary. World Wind Energy Association (WWEA), Bonn, Germany.

Menter, F.R., Langtry, R.B., Likki, S.R., Suzen, Y.B., Huang, P.G. and Völker, S., 2006. A correlation-based transition model using local variables—part I: model formulation. Journal of Turbomachinery 128, 413. Rezaeiha, A., Kalkman, I.M. and Blocken, B., 2016a. The effect of pitch angle on the performance of a vertical

axis wind turbine. Proceedings of International Sustainable Built Environment Conference, Malta. Rezaeiha, A., Kalkman, I.M. and Blocken, B., 2016b. A short review of recent research activities for

aerodynamic optimization of vertical axis wind turbines. Proceedings of 1st International TU1304 WINERCOST Conference, Ankara, Turkey.

Simão Ferreira, C., van Kuik, G., van Bussel, G. and Scarano, F., 2008. Visualization by PIV of dynamic stall on a vertical axis wind turbine. Experiments in Fluids 46, 97-108.

Tescione, G., Ragni, D., He, C., Simão Ferreira, C. and van Bussel, G.J.W., 2014. Near wake flow analysis of a vertical axis wind turbine by stereoscopic particle image velocimetry. Renewable Energy 70, 47-61.

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