Comparisons between the Wake of a Wind Turbine Generator Operated at Optimal Tip Speed Ratio and the Wake of a Stationary Disk
The wake of a wind turbine generator (WTG) operated at the optimal tip speed ratio is compared to the wake of a WTG with its rotor replaced by a stationary disk. Numerical simulations are conducted with a large eddy simulation (LES) model using a nonuniform staggered Cartesian grid. The results from...
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2011-01-01
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Series: | Modelling and Simulation in Engineering |
Online Access: | http://dx.doi.org/10.1155/2011/749421 |
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doaj-cd48a7f9c2b9468a815eb731fbe8d8122020-11-24T21:17:16ZengHindawi LimitedModelling and Simulation in Engineering1687-55911687-56052011-01-01201110.1155/2011/749421749421Comparisons between the Wake of a Wind Turbine Generator Operated at Optimal Tip Speed Ratio and the Wake of a Stationary DiskTakanori Uchida0Yuji Ohya1Kenichiro Sugitani2Research Institute for Applied Mechanics, Kyushu University, 6-1 Kasugakoen, Kasuga, Fukuoka 816-8580, JapanResearch Institute for Applied Mechanics, Kyushu University, 6-1 Kasugakoen, Kasuga, Fukuoka 816-8580, JapanResearch Institute for Applied Mechanics, Kyushu University, 6-1 Kasugakoen, Kasuga, Fukuoka 816-8580, JapanThe wake of a wind turbine generator (WTG) operated at the optimal tip speed ratio is compared to the wake of a WTG with its rotor replaced by a stationary disk. Numerical simulations are conducted with a large eddy simulation (LES) model using a nonuniform staggered Cartesian grid. The results from the numerical simulations are compared to those from wind-tunnel experiments. The characteristics of the wake of the stationary disk are significantly different from those of the WTG. The velocity deficit at a downstream distance of 10𝐷 (𝐷: rotor diameter) behind the WTG is approximately 30 to 40% of the inflow velocity. In contrast, flow separation is observed immediately behind the stationary disk (≤2𝐷), and the velocity deficit in the far wake (10𝐷) of the stationary disk is smaller than that of the WTG.http://dx.doi.org/10.1155/2011/749421 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Takanori Uchida Yuji Ohya Kenichiro Sugitani |
spellingShingle |
Takanori Uchida Yuji Ohya Kenichiro Sugitani Comparisons between the Wake of a Wind Turbine Generator Operated at Optimal Tip Speed Ratio and the Wake of a Stationary Disk Modelling and Simulation in Engineering |
author_facet |
Takanori Uchida Yuji Ohya Kenichiro Sugitani |
author_sort |
Takanori Uchida |
title |
Comparisons between the Wake of a Wind Turbine Generator Operated at Optimal Tip Speed Ratio and the Wake of a Stationary Disk |
title_short |
Comparisons between the Wake of a Wind Turbine Generator Operated at Optimal Tip Speed Ratio and the Wake of a Stationary Disk |
title_full |
Comparisons between the Wake of a Wind Turbine Generator Operated at Optimal Tip Speed Ratio and the Wake of a Stationary Disk |
title_fullStr |
Comparisons between the Wake of a Wind Turbine Generator Operated at Optimal Tip Speed Ratio and the Wake of a Stationary Disk |
title_full_unstemmed |
Comparisons between the Wake of a Wind Turbine Generator Operated at Optimal Tip Speed Ratio and the Wake of a Stationary Disk |
title_sort |
comparisons between the wake of a wind turbine generator operated at optimal tip speed ratio and the wake of a stationary disk |
publisher |
Hindawi Limited |
series |
Modelling and Simulation in Engineering |
issn |
1687-5591 1687-5605 |
publishDate |
2011-01-01 |
description |
The wake of a wind turbine generator (WTG) operated at the optimal tip speed ratio is compared to the wake of a WTG with its rotor replaced by a stationary disk. Numerical simulations are conducted with a large eddy simulation (LES) model using a nonuniform staggered Cartesian grid. The results from the numerical simulations are compared to those from wind-tunnel experiments. The characteristics of the wake of the stationary disk are significantly different from those of the WTG. The velocity deficit at a downstream distance of 10𝐷 (𝐷: rotor diameter) behind the WTG is approximately 30 to 40% of the inflow velocity. In contrast, flow separation is observed immediately behind the stationary disk (≤2𝐷), and the velocity deficit in the far wake (10𝐷) of the stationary disk is smaller than that of the WTG. |
url |
http://dx.doi.org/10.1155/2011/749421 |
work_keys_str_mv |
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