Experimental study on the wind-turbine wake meandering inside a scale model wind farm placed in an atmospheric-boundary-layer wind tunnel

N. Coudou, S. Buckingham, J. van Beeck
2017 Journal of Physics, Conference Series  
Qualitative analysis of wind-turbine wakes over hilly terrain A Hyvärinen and A Segalini -Modelling of Wind Turbine Loads nearby a Wind Farm B Roscher, A Werkmeister, G Jacobs et al. -Wind-turbine wakes responding to stably stratified flow over complex terrain Antonia Englberger and Andreas Dörnbrack -This content was downloaded from IP address 193.191.134.1 on 17/06 Abstract. Increasing use of wind energy over the years results in more and larger clustered wind farms. It is therefore
more » ... l to have an in-depth knowledge of wind-turbine wakes, and especially a better understanding of the well-known but less understood wake-meandering phenomenon which causes the wake to move as a whole in both horizontal and vertical directions as it is convected downstream. This oscillatory motion of the wake is crucial for loading on downstream turbines because it increases fatigue loads and in particular yaw loads. In order to address this phenomenon, experimental investigations were carried out in an atmosphericboundary-layer wind tunnel using a 3 × 3 scaled wind farm composed of three-bladed rotating wind-turbine models subject to a neutral atmospheric boundary layer (ABL) corresponding to a slightly rough terrain, i.e. to offshore conditions. Particle Image Velocimetry (PIV) measurements were performed in a horizontal plane, at hub height, in the wake of the three wind turbines in the wind-farm centreline. From the PIV velocity fields obtained, the wakecentrelines were determined and a spectral analysis was performed to obtain the characteristics of the wake-meandering phenomenon. In addition, Hot-Wire Anemometry (HWA) measurements were performed in the wakes of the same wind turbines to validate the PIV results. The spectral analysis performed with the spatial and temporal signals obtained from PIV and HWA measurements respectively, led to Strouhal numbers St = f D/U hub 0.20 − 0.22.
doi:10.1088/1742-6596/854/1/012008 fatcat:vne6a3w2pfb7vaaovg6c76cn7a