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Wake Measurements of a Multi-MW Wind Turbine with Coherent Long-Range Pulsed Doppler Wind Lidar

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Long-range Doppler wind light detection and ranging (lidar) measurements at a wind turbine were carried out for the first time. The turbine was of the type Areva M5000 and is located at a site near the coastline in Bremerhaven, in the northern part of Germany. This wind turbine is the prototype for the German offshore test site ‘‘alpha ventus’’ and has a rated power of 5 MW. Information about the ambient wind field before and after this multimegawatt wind turbine was obtained. In this paper the measurement technique is discussed and the results of measurements in the diurnal layer and in the stable nocturnal boundary layer are shown. The main focus of this work is to determine the reduction of the wind speed at certain distances downstream from the rotor.
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Wake Measurements of a Multi-MW Wind Turbine with Coherent
Long-Range Pulsed Doppler Wind Lidar
YVONNE KA
¨SLER,STEPHAN RAHM,AND RUDOLF SIMMET
Deutsches Zentrum fu
¨r Luft- und Raumfahrt, Institut fu
¨r Physik der Atmospha
¨re, Wessling, Germany
MARTIN KU
¨HN
Research Group Wind Energy Systems—ForWind, Center for Wind Energy Research,
University of Oldenburg, Oldenburg, Germany
(Manuscript received 15 April 2010, in final form 8 June 2010)
ABSTRACT
Long-range Doppler wind light detection and ranging (lidar) measurements at a wind turbine were carried
out for the first time. The turbine was of the type Areva M5000 and is located at a site near the coastline in
Bremerhaven, in the northern part of Germany. This wind turbine is the prototype for the German offshore
test site ‘‘alpha ventus’’ and has a rated power of 5 MW. Information about the ambient wind field before and
after this multimegawatt wind turbine was obtained. In this paper the measurement technique is discussed and
the results of measurements in the diurnal layer and in the stable nocturnal boundary layer are shown. The
main focus of this work is to determine the reduction of the wind speed at certain distances downstream from
the rotor.
1. Measurement technique
Lidar is a remote sensing technique that transmits
alaserbeamintotheatmosphereandthebackscat-
tered light is detected. The pulsed Doppler wind lidar,
which was used for the measurements in Bremerhaven,
Germany, takes advantage of the fact that the center
frequency of the received laser pulses is shifted compared
to the outgoing pulses because of the Doppler effect,
which occurs from backscattering on moving particles.
This shift in frequency provides information about the
line-of-sight (LOS) component (component in beam di-
rection) of the wind vector. The Doppler lidar of the
German Aerospace Center [Deutsches Zentrum fu
¨r
Luft- und Raumfahrt (DLR)] is based on a WindTracer
transceiver unit of Lockheed Martin (which acquired
Coherent Technologies, Inc. and its division CLR
Photonics, Inc.; Ko
¨pp et al. 2004). It has been modi-
fied by the DLR and has been used for wind and tur-
bulence measurements from the ground, as well as from
its research aircraft in the past (Rahm and Smalikho 2008;
Smalikho et al. 2005). The most important aspect was the
addition of a scanner that makes different scan patterns at
variable scan speeds possible. The measurement range on
ground is between 500 m and 10 km. The maximum range
used for the measurements in Bremerhaven was 3 km.
The main system parameters and important information
for data acquisition and processing are summarized in
Table 1. The specifications of the lidar do not completely
coincide with those discussed in Smalikho et al. (2005)
because of modifications of the laser system.
Figure 1a shows a map of the area in Bremerhaven
(using the software program OpenStreetMaps). The 2-mm
lidar is located at a distance of about 1820 m north-
east of the wind turbine M5000. Technical data of the
wind turbinecan be found in Table 2. Furthermore, it can
be seen in Fig. 1a that there are other wind turbines in the
measurement area. One of them is of the same type as the
Areva Multibrid M5000. Two different scanning tech-
niques to analyze the ambient wind field of the prototype
of the Multibrid M5000 were carried out: azimuth scans
(Fig. 1a) and elevation scans (Fig. 1b). For the azimuth
scans, the elevation of the laser beam was constant and the
azimuth angle was continuously changed. The duration of
an azimuth scan was 15 s and the scan speed 28s
21
. For
Corresponding author address: Yvonne Ka
¨sler, Deutsches
Zentrum fu
¨r Luft- und Raumfahrt, Mu
¨nchner Str. 20, Oberpfaffen-
hofen, D-82234 Wessling, Germany.
E-mail: yvonne.kaesler@dlr.de
SEPTEMBER 2010 K A
¨SLER ET AL. 1529
DOI: 10.1175/2010JTECHA1483.1
Ó2010 American Meteorological Society
the elevation scans, the azimuth angle was not changed
but the elevation was increased continuously. One single
elevation scan measurement took 10 s. The scan speed
for these types of scans was 18s
21
. The great advantage
of the measurements is that it is possible to obtain in-
formation about the airflow in front and behind the wind
turbine at the same time. This is in contrast to wake
measurements that were carried out previously with
a focused continuous wave lidar system (Bingo
¨l et al.
2010; Trujillo et al. 2010).
2. Results
Figure 2 shows two measurements of the ambient
field of the Multibrid M5000 in the nocturnal boundary
layer: one elevation scan (Fig. 2a) and one azimuth scan
(Fig. 2b). The wind was blowing from the northeast di-
rection, parallel to the laser beam. Atmospheric conditions
were very stable when the measurements were taken. The
turbulence intensity at hub height (102 m) upstream
from the wind turbine was only 2.8%. This means that the
wake effects are expected to be very distinct (Barthelmie
et al. 2003). To determine this turbulence intensity, the
LOS velocity at a range of two rotor diameters upstream
from the M5000 at hub height was observed for 10 min.
This corresponds to 46 scans or a time series with
46 values. The turbulence intensity I was then calculated as
I5sLOS
LOS .
In this equation s
LOS
is the standard deviation and LOS
is the mean of the time series of the line-of-sight velocity
(Stull 1988).
It needs to be considered that s
LOS
and I, which were
determined by the lidar data, are significantly damped in
comparison to anemometer measurements because of
the long pulse length (cf. Table 1) of the pulsed wind
lidar.
In Fig. 2a, the elevation scan through the rotor blades,
only the wake effects of the prototype of the Multibrid
M5000 can be seen. The range is the distance from the
2-mm lidar, and the height reflects the elevation of the
TABLE 1. The 2-mm lidar system parameters and data acquisition.
FWHM is the full width at half maximum.
Slave laser (Tm:LuAG)
Wavelength 2.022 mm
Repetition rate 500 Hz
Pulse energy 1.5 mJ
Pulse length (FWHM) 0.5 ms575 m (0.5 ms3cO2)
c: speed of light
Telescope Off-axis type
Aperture: 108 mm at lidar
with afocal setting
Scanner Double wedge with
variable speed
Measurement range Maximum: 500 m to .10 km
Processed data: 500 m to 3 km
Data acquisition
Sample length 0.3 m
Width of lidar
range gates
512 30.3 m 5154 m
Number of range gates
in 3 km
50
Sampling rate between
two scans
Elevation scan: 14 s
Azimuth scan: 22 s
FIG. 1. (a) Map of the area in Bremerhaven with the position of
the 2-mm lidar and the wind turbines. A top view of an azimuth scan
is given in the layout plan. (b) Side view of an elevation scan.
1530 JOURNAL OF ATMOSPHERIC AND OCEANIC TECHNOLOGY VOLUME 27
laser beam. The position of the wind turbine and the
wind direction are indicated in the picture. Between
1800 and 2600 m, a decrease of the absolute value of the
LOS component of the wind vector downstream from
the Multibrid M5000 can be clearly observed. One rotor
diameter (116 m 51D) downstream from the LOS ve-
locity at hub height is reduced about 66% (the maximum
of LOS velocity reduction) in comparison to the values
upstream. After 7Ddownstream (18% reduction of the
LOS velocity at hub height), the wind field only recovers
very slowly. The velocity deficit downstream from the
wind turbine is shown in Fig. 3. Because of data storage,
the maximum range recorded in this measurement was
9Ddownstream. At this range the reduction of the LOS
velocity was 16% of the initial value. The black and red
horizontal lines at a range between approximately 1700
and 2100 m in Fig. 2a indicate the areas where the laser
beam hits the rotor blades. The backscatter of the blades
is several orders of magnitude stronger than the atmo-
spheric backscatter. The two lines represent two differ-
ent rotor blades. The position of the wind turbine is at
a range of 1823 m. One needs to consider that the pulse
length of the laser (0 to 0) is approximately 400 m. When
the beginning of the laser pulse hits the blades, there are
120 m in front of the turbine that are influenced by the
blade because of the length of the laser pulse. With a
symmetric laser pulse, one would expect that the black
lines would end approximately 120 m after the turbine
(i.e., at a range of approximately 1940 m) when the end
of the laser pulse hits a part of the blades. The laser pulse
has a small tail containing little energy. Therefore, the
horizontal lines are longer after the turbine than in front
of the turbine. As a result, the shadows are approximately
400 m long and not only 240 m. If not only part of the
laser beam but the whole beam hits a blade, there is a
black line behind the position of the turbine until the end
of the measurement range (cf. Fig. 4). The different colors
of the horizontal lines (black and red) therefore depend
on the LOS velocity of the blades.
In Fig. 2b an azimuth scan through the rotor blades
can be seen. The width indicates the different azimuth
angles. The elevation was 3.38for this measurement.
This resulted in a scan through the rotor blades only
somewhat above hub height. In comparison to Fig. 2a,
this scan also covers the disturbance of the wind field by
other wind turbines near the Multibrid M5000 prototype
(M5000-1). The location of the different wind turbines
can be estimated by the horizontal lines where the laser
beam hits the rotor blades. There is another wind tur-
bine (M5000-2) of the same type as M5000-1 and two
turbines of different types. According to the horizontal
lines, the laser beam hits one blade of the M5000-2 and
TABLE 2. Technical data of the M5000.
Rotor diameter 116 m
Hub height 102 m
Length of a rotor blade 62 m
Rated power 5 MW
Rated wind speed 12 m s
21
Maximum elevation height of the rotor 164 m
Speed range of the rotor 4.5–14.8 min
21
610%
FIG. 2. (a) Results for the LOS component of the wind vector for
an elevation scan through the rotor blades at night. The wind was
blowing from the northeast parallel to the laser beam. Wind di-
rection and position of the wind turbine are indicated in the figure.
The white vertical line indicates the rotor disc. (b) Azimuth scan at
night covering the ambient wind field of several wind turbines,
including the M5000-1 prototype. The vertical white lines indicate
the position of the rotor discs of M5000-1 and M5000-2.
FIG. 3. Velocity deficit downstream from the wind turbine derived
from the elevation scan in Fig. 2a.
SEPTEMBER 2010 K A
¨SLER ET AL. 1531
two blades of the M5000-1. It needs to be considered that
it is possible to hit one or more blades with one azimuth
scan. It seems as if the turbines different from M5000
have a smaller effect on the wind field. But the shorter
wakes are due to the elevation of the azimuth scan. This
means that for these wind turbines, the wake is only cut
by the scan. By analyzing the length of the wake of the
M5000 wind turbines of this measurement, it can be
found that the results correspond to the results of the
elevation scan. Thus, it can be shown that for the mea-
surements of the Multibrid M5000 turbines, the eleva-
tion scan as well as the azimuth scan captured the whole
wake and not only cut it.
Figure 4 shows an azimuth scan during daytime with
a turbulence intensity of more than 15%, two rotor di-
ameters upstream from the wind turbine at hub height.
Notice that this measurement was taken on another day,
and that the wind was blowingfrom a southwest direction
parallel to the laser beam. As mentioned before, wake
effects are supposed to be less distinct in a turbulent at-
mosphere (Barthelmie et al. 2003). This is evident when
Fig. 2b is compared to Fig. 4: the length of the wakes of
the M5000 turbines is shorter in Fig. 4.
To sum up, it can be said that ithas been shown that the
2-mm Doppler lidar is a convenient tool for wind energy
research and could help to improve the modeling of wind
turbine wakes for single turbines, as well as for wind
parks. A method for wake capturing has been developed.
We plan a detailed analysis for these measurements in
the nocturnal boundary layer, and of measurements, were
taken during daytime in a more turbulent atmosphere.
Furthermore, a comparison with the Parallelized Large-
Eddy Simulation (LES) Model (PALM; Steinfeld et al.
2009; Raasch 2010) is already in preparation.
Acknowledgments. This work is done in the framework
of the project ‘‘LIDAR-Development of LIDAR tech-
nologies for the German offshore test field’’ of the German
Federal Environment Ministry (BMU; Contract 0327642).
Thanks are given to Areva - Multibrid GmbH for pro-
viding access to the M5000 wind turbine and to the whole
Lidar group of the Endowed Chair of Wind Energy at
the University of Stuttgart, especially Juan Jose
´Trujillo
for his helpful discussions and cooperation.
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1532 JOURNAL OF ATMOSPHERIC AND OCEANIC TECHNOLOGY VOLUME 27
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An experiment for airborne Doppler lidar measurement of wake vortices generated by a large transport aircraft in the free atmosphere has been successfully carried out. In this paper, the description of the experiment, data processing procedure, and measurement results are given. It was shown that the use of smoke generators placed on large transport aircraft wings allows some high-quality wake vortex measurements with 2/μm coherent Doppler lidar installed in a second aircraft. Copyright © 2008 by the American Institute of Aeronautics and Astronautics, Inc. All rights reserved.
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The 2-μm pulsed Doppler lidar, already successfully used for wind and turbulence measurements, has been modified for long-range wake-vortex characterization. In particular, a four-stage data processing algorithm has been developed to achieve precise profiles of tangential velocities from which the vortex parameters such as trajectories, core separation, tilt angle, and circulation can be derived. The main advantage of the pulsed lidar is its long-range capability of more than 1 km. This allows for observations over long periods from the moment of wake generation to a progressed state of vortex decay. With the field experiment at Tarbes airfield the potential of the 2-μm pulsed Doppler lidar for full-scale wake-vortex characterization has been demonstrated. Two examples showing the parameters of wake vortices generated by large transport aircraft (LTA)-type aircraft will be presented.
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The vast majority of wind turbines are today erected in wind farms. As a consequence, wake-generated loads are becoming more and more important. In this first of two parts, we present a new experimental technique to measure the instantaneous wake deficit directly, thus allowing for quantification of the wake meandering, as well as the instantaneous wake expansion expressed in a meandering frame of reference. The experiment was conducted primarily to test the simple hypothesis that the wake deficit is advected passively by the larger-than-rotor-size eddies in the atmospheric flow, and that the wake at the same time widens gradually, primarily because of mixing caused by small-scale atmospheric eddies. In this first paper, we focus on our new measurement technique, and test if the wake meandering follows the wind direction fluctuations, i.e. if it is advected passively in the lateral direction. The experimental results are used as a preliminary verification of a wake meandering model that essentially considers the wake as a passive tracer. Copyright © 2009 John Wiley & Sons, Ltd.
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The 2-mum pulsed Doppler lidar, already successfully used for wind and turbulence measurements, has been modified for long-range wake-vortex characterization. In particular, a four-stage data processing algorithm has been developed to achieve precise profiles of tangential velocities from which the vortex parameters such as trajectories, core separation, tilt angle, and circulation can be derived. The main advantage of the pulsed lidar is its long-range capability of more than 1 km. This allows for observations over long periods from the moment of wake generation to a progressed state of vortex decay. With the field experiment at Tarbes airfield the potential of the 2-mum pulsed Doppler lidar for full-scale wake-vortex characterization has been demonstrated. Two examples showing the parameters of wake vortices generated by large transport aircraft (LTA)-type aircraft will be presented.