Abstract

Our research group is developing computational fluid dynamics (CFD)-based software for wind resource and energy production assessments in complex terrain called RIAM-COMPACT (Research Institute for Applied Mechanics, Kyushu University (RIAM)-Computational Prediction of Airflow over Complex Terrain), based on large eddy simulation (LES). In order to verify the prediction accuracy of RIAM-COMPACT, we conduct a wind tunnel experiment that uses a two-dimensional steep ridge model with a smooth surface. In the wind tunnel experiments, airflow measurements are performed using an I-type hot-wire probe and a split film probe that can detect forward and reverse flows. The results of the numerical simulation by LES are in better agreement with the wind tunnel experiment using the split film probe than the results of the wind tunnel experiment using the I-type hot wire probe. Furthermore, we calculate that the two-dimensional ridge model by changing the length in the spanwise direction, and discussed the instantaneous flow field and the time-averaged flow field for the three-dimensional structure of the flow behind the model. It was shown that the eddies in the downwind flow-separated region formed behind the two-dimensional ridge model were almost the same size in all cases, regardless of the difference in the length in the spanwise direction. In this study, we also perform a calculation with a varying inflow shear at the inflow boundary. It was clear that the size in the vortex region behind the model was almost the same in all the calculation results, regardless of the difference in the inflow shear. Next, we conduct wind tunnel experiments on complex terrain. In the wind tunnel experiments using a 1/2800 scale model, the effect of artificial irregularities on the terrain surface did not significantly appear on the airflow at the hub height of the wind turbine. On the other hand, in order to investigate the three-dimensional structure of the airflow in the swept area in detail, it was clearly shown that LES using a high-resolution computational grid is very effective.

Highlights

  • At present, a significant reduction of carbon dioxide is an urgent issue to prevent global warming.Along with this, the effective use of wind energy and clean and environmentally friendly natural energy is attracting attention

  • It was revealed that the results of the numerical at z*/h < 2, the result of the I-type hot wire probe is considerably overestimated compared with the simulation by large eddy simulation (LES) are in better agreement with the wind tunnel experiment using the split film probe result of the split film probe

  • We showed that the wind tunnel experiment using the I-type hot wire probe is an effective method for understanding local speed-up ratios at wind turbine hub height for probe is an effective method for understanding local speed-up ratios at wind turbine hub height for 16 wind sectors

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Summary

Introduction

A significant reduction of carbon dioxide is an urgent issue to prevent global warming. In order to verify the prediction of RIAM-COMPACT, conducted a wind is that it is possible to accurately predict the accuracy temporal change of the topographicwe effect on the wind tunnel experiment two-dimensional steep model. First,the in influence order to verify the prediction accuracy of RIAM-COMPACT, we conducted a wind and a experiments, of topographic surface roughness and inflow turbulence was omitted, tunnel experiment using a two-dimensional steep ridge model. This is because we wanted to verify complicated turbulent flow field past a simple steep terrain placed in a uniform flow was targeted. Wind Tunnel Experiments and Numerical Simulations for a Two-Dimensional Ridge Model

Overview of the Wind Tunnel Equipment
Airflow
Overview of LES-Based CFD Approach
Results
Overview of Noma Wind Park in Kagoshima Prefecture
14. Figure
11. Complex
Scale Model for the Complex Three-Dimensional Terrain
Measurement
19. Figure
20. Comparison
Overview of Numerical Simulations
22. The of grid points
Results andthe
25. Vertical distributionofoftime-averaged time-averaged velocity at at
Conclusions
35. Comparison of local speed-up ratios
Comparison of simulations local speed-up ratios
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