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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Main Authors: Takanori Uchida, Yuji Ohya, Kenichiro Sugitani
Format: Article
Language:English
Published: Hindawi Limited 2011-01-01
Series:Modelling and Simulation in Engineering
Online Access:http://dx.doi.org/10.1155/2011/749421
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spelling 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
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