round robin numerical flow simulation in wind energy - dewi
TRANSCRIPT
Francesco Durante, Volker Riedel
Ulrike Bunse, Peter Busche, Harald Mellinghoff, Dr. Kai Mönnich, Till Schorer
DEWI GmbH - Deutsches Windenergie-Institut
Wilhelmshaven, Germany
2008-03-08
This project was sponsored by the German Federal Ministry for the Environment, Nature Conservation
and Nuclear Safety, FKZ 0329965.
Round Robin
Numerical Flow Simulation in Wind Energy
Final Report
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 2 / 173
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 3 / 173
Disclaimer
The following results refer to one single site with three met masts installed, they refer to the model in
the version and configuration used in the test and they refer to a specific model operator/team. Under
no circumstances can these results be considered as a general statement about the quality of the
service provided by each company, nor can these results be considered as a general quality assessment
of the computer model used. In particular, if a third party flow model is used by the participant, the
results cannot be considered as a statement of quality of the third party model. The reasons are as
follows:
1. Flow models in general have many parameters to set and simulation design decisions have to be
made, depending on the site under consideration and depending on the experience of the model
operator. It is not clear if the model operator during the Round Robin Test will be the same than
during normal business model operation.
2. Wind farm sites are very different, especially regarding orographic complexity. The results that
refer to this site are not transferable to any other site and are valid only for this specific site.
3. Measurement uncertainties specified below refer to the standard uncertainty, assuming a normal
distributed error. Although less likely, the actual deviation between measurement value and real
value can be higher than the standard error.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 4 / 173
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 5 / 173
Table of Content
1 Preface ...........................................................................................................................................9
2 Sponsors .......................................................................................................................................10
3 Setup of the Round Robin test.......................................................................................................11
3.1 The aim...................................................................................................................................11
3.2 The choice of the test site .......................................................................................................11
3.3 The dummy Run......................................................................................................................12
4 Description of the Participating Models.........................................................................................13
5 Description of the Main Test .........................................................................................................20
5.1 Input Data-set.........................................................................................................................20
5.1.1 Elevation..........................................................................................................................21
5.1.2 Land Cover.......................................................................................................................23
5.1.3 Meteorological data.........................................................................................................25
5.1.4 Coordinates .....................................................................................................................28
5.2 Output Data-set ......................................................................................................................28
5.2.1 Mean Horizontal Wind Speed for terrain-following surfaces............................................28
5.2.2 Mean Wind Speed for the target locations .......................................................................29
5.2.3 Wind Statistics for target locations in 80 m above Ground Level ......................................29
6 Assessment of the Results.............................................................................................................30
6.1 Weibull A- and k-Parameter....................................................................................................30
6.2 Mean Horizontal Wind Speed for a terrain-following surface at different heights ...................33
6.3 General Remarks on the Evaluations Regarding Wind Speed...................................................43
6.3.1 Technical details on the assessment of the statistics ........................................................43
6.4 Important Remarks regarding the Results of the Participant ANM...........................................46
6.5 Incomplete Data Submitted by Participant UNJ.......................................................................49
6.6 Incomplete Data Submitted by Participant REP .......................................................................49
6.7 Evaluations Regarding Mean Wind Speed ...............................................................................50
6.7.1 Quantitative Evaluations with Respect to the Sector-wise Speed-Up Factors....................51
6.7.2 Deviations from all Participants Mean Values...................................................................54
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 6 / 173
6.7.3 Mean Absolute Values of Sector-wise Errors ....................................................................55
6.7.4 Overall Direction Independent Wind Speed Prediction Error ............................................56
6.8 Evaluations Regarding Mean Squared Wind Speed..................................................................67
6.9 Evaluations Regarding Mean Cubed Wind Speed ....................................................................77
6.10 Evaluations Regarding Wind Direction ....................................................................................86
6.10.1 Qualitative Evaluation Regarding Veer Angles ..................................................................86
6.10.2 Qualitative Evaluation Regarding Veer Angles: Target Mast 1...........................................86
6.10.3 Qualitative Evaluation Regarding Veer Angles: Target Mast 2...........................................87
6.10.4 Evaluations Regarding the Overall Wind Direction Distributions.......................................88
6.10.5 Assessment of Average Sector-Wise Wind Direction Errors ..............................................90
6.10.6 Assessment of the Directional Dispersion of the Single Sector Wind Direction Results .....90
6.11 Single Turbine AEP................................................................................................................104
6.12 Energy Yield Results: Single Turbine AEP ...............................................................................105
6.13 Wind Farm Energy Yield Results ............................................................................................113
7 Conclusions.................................................................................................................................121
8 Appendix ....................................................................................................................................125
8.1 Overview of the properties of the on-site measurements .....................................................125
8.1.1 Wind Direction Effects ...................................................................................................129
8.1.2 Speed-up Factors ...........................................................................................................132
8.1.3 Turbulence Intensity ......................................................................................................135
8.1.4 Sector-wise Wind Speed Correlation Properties .............................................................142
8.1.5 Filling of a Gap in Target Mast 1 Data .............................................................................148
8.1.6 Filling of a Gap in Target Mast 2 Data .............................................................................152
8.2 Issues related to the site selection process............................................................................156
8.2.1 General Considerations..................................................................................................156
8.2.2 Wind Speed Measurement ............................................................................................157
8.2.3 Spatial Arrangement ......................................................................................................158
8.2.4 Wind Direction Measurements ......................................................................................158
8.2.5 Exemplary illustrations of some problematic effects found during site search................161
8.2.6 Maps .............................................................................................................................166
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 7 / 173
8.2.7 Forest ............................................................................................................................166
8.2.8 Coordinates ...................................................................................................................167
8.2.9 Data from Numerical Site Calibrations ...........................................................................168
8.3 Output data Format..............................................................................................................170
8.3.1 Mean Horizontal Wind Speed for terrain following surfaces - Data Format.....................170
8.3.2 Mean Wind Speed for target locations - Data Format.....................................................170
8.3.3 Wind Statistics for target locations - Data Format ..........................................................171
9 References..................................................................................................................................173
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 8 / 173
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 9 / 173
1 Preface
Wind energy has successfully developed world wide during the last years. Along with this good
development, there have been continuous improvements of the tools used for the simulation of the
wind flow conditions. Future installations are foreseen to concentrate over off-shore areas and to
develop more and more over internal complex terrain sites. With the exploitation of wind energy over
internal areas, the complexity of the surface and flow conditions makes the requirements for a proper
wind resource assessment and for a correct definition of the financing risks even higher. Despite a
general improvement of several aspects of resource assessment methods (such as the analysis of the
anemometers effects, the long term correlation techniques etc. ), the methods for extrapolation of
wind conditions from a measurement mast to a wind turbine site has remained more or less unchanged
since the early nineties: The European Wind Atlas is a „de facto“ standard method for most of the
energy yield calculations. Limitations and weaknesses of this methodology are well known and under
complex terrain conditions (or other non-standard situations) large systematic errors are to be
expected. An alternative solution to improve the reliability of resource assessment over complex
orography is represented by the use of fluid dynamical numerical models. Presently, different
typologies of numerical models and methodologies are adopted for wind resource evaluation. Most of
them have been initially developed for purposes marginally related to wind energy applications such as
automotive industry or weather forecasting. While in other sectors of research and engineering the
numerical solution of the fluid dynamic equations has become a standard approach for the derivation
of the flow properties, in wind energy the adoption of numerical flow models as an accepted standard
method still lacks the necessary experience and still requires a systematic classification and a scientific
evaluation of errors and of the related uncertainties. Such an evaluation would support decisions for a
wide range of wind energy actors like banks, financing companies, developers, etc. It is believed that
the presence of a scientific classification and an independent assessment of the myriad of different
wind simulation methods will eventually improve the acceptability of the concept of numerical
simulation on the whole. This project aims, as much as possible, to fill the aforementioned gaps.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 10 / 173
2 Sponsors
This research was sponsored by the following parties:
- German Federal Ministry for the Environment, Nature Conservation and Nuclear Safety
- Bremer Landesbank
- Commerzbank
- Deutsche Immobilien Leasing GmbH
- GE Energy
- HSH Nordbank AG
- Nord/LB
- Ostwind Verw.ges.
- WPD Beteiligungs GmbH
- DEWI GmbH
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 11 / 173
3 Setup of the Round Robin test
3.1 The aim
Numerical models are currently widely used in wind energy analysis to extrapolate the wind conditions
from a point where wind conditions are measured to other points of a wind farm area where wind
conditions are unknown. Despite a certain number of numerical models do exist which do not use on-
site wind measurements at all, the extrapolation of punctual measurements is the primary use of
numerical models in micrositing, site assessment and energy yield analysis. Accordingly, the Round
Robin test aims to systematically evaluate the capabilities of the considered models of extrapolating
wind measurements.
Therefore the participants were requested to perform a simulation which takes as input wind
measurements at one reference point of the site, (along with topographic and climatic data) and
calculate wind conditions for two other target points for which wind measurements are available but
unknown to the participants.
3.2 The choice of the test site
DEWI has a database of many hundred sites for which wind measurements have been carried out.
Many of the measurements of this database are directly performed by DEWI according to the IEC
standard (IEC 61400-12-1, IEC 61400-12), MEASNET and the IEA recommendations, both for wind
potential studies and for power performance measurements including site calibrations. The remaining
sites are equipped with third-party wind measurements and mainly used in previous wind potential
studies executed world-wide by DEWI during the last years. In order to set-up a proper model
verification, a certain number of requirements should be satisfied. These requirements refer both to
the site characteristics and to the properties of the measurement equipment. Table 1 shows a list of
minimum requirements that should be fulfilled by the pair „site/measurement equipment”. During the
selection of a site suitable for the main test it turned out that the difficulty of this task was by far
underestimated. A list of examples of problems encountered during the selection of the site is reported
in detail in Appendix 8.2. The by-product of this selection process represents by itself, in our point of
view, an unexpected, new and valuable result. Having investigated a large number of complex terrain
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 12 / 173
wind measurements from the last years and different sources, we put forward the hypothesis that in
general the measurement errors in complex terrain are underestimated, even if the equipment fully
conforms to the standards. This is especially true for the wind direction measurement, whose high
importance is not enough recognized. We were not fully aware of the meaning of these difficulties for
the Round Robin test and, accordingly, we underestimated by far the effort for site selection.
Requirement Relevance Condition satified in
the main test
More than one high quality measurement mast present at the site. High Yes
Data collected at least for wind speed and wind direction for a reasonably long common period (at least
several months, 1 year desirable).
High Yes
Distance between in the order of a few kilometers Medium Yes
Availability of a detailed documentation of the measurement equipment. High Yes
The measurement heights should be at least 30m. Preferably at least one measurement should be at hub
height of current modern wind turbines.
Medium Yes
Anemometers have to be individually calibrated (preferably MEASNET or DAP approved) and should
preferably be of type Thies First Class, Risoe or Vector.
High Yes
The site should present strong complex features (steep slopes, flow channeling, flow separation). Medium No
The wind distribution at the target points should not be easily obtainable with „standard” techniques (e.g.
WAsP)
Medium Unknown
The site must be free of operating wind turbines. High Yes
The wind data-set must not be public available, particularly, wind data should not have been given
previously to any of the participants.
High Yes
Ownership issues. The owner of the data set must agree to the use of the data in the test. High Yes
Table 1: List of requirements to be fulfilled by the couple „site/measurement equipment”.
3.3 The dummy Run
The DEWI Round Robin Test on Numerical Flow Simulation started with a test of the test procedure
itself, which was called „Dummy-Run”. This test was designed to identify possible problems in the data
transfer between DEWI and the participants and vice versa. In particular, attention was paid in order to
ensure that the data that is submitted to DEWI by the participants was delivered in the correct data
format. During this test it was also possible to ensure that the participants are provided with all the
information needed to run their model. The whole „Dummy-Run” was therefore designed in a similar
way as the final run and it was useful for the participants to get confidence with the test and practice
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 13 / 173
with several data and respective data formats. From the point of view of today, the dummy-run was
very useful and successful and without the dummy-run the main test may have failed.
4 Description of the Participating Models
In total, 8 participants took part in the Round Robin test. All of them used different models. The
participants were from Germany (6), France (1) and Japan (1). A list of names of participants, address
and contact person is reported in Table 2.
It should be noted that the participant CeBeNetwork GmbH did not manage to perform the requested
simulations. Therefore it was not possible to evaluate this participant within this test. Nevertheless
CeBeNetwork has expressed his wish to actively take part in the project in future in case of further
tests.
During the preparation phase of the Round Robin test, the participants were asked to fill in a
questionnaire collecting information about the applied models. The main goal of this questionnaire was
to help DEWI in designing the Round Robin test regarding the required input and output data and its
format for the test. Table 3 summarizes the information returned by the participants about the
technical description of their models. Throughout the report, the participant's contributions are
referred to by their shorthand symbols, that are specified on top of Table 3 .
Besides the contributions of the 8 participants, 2 further („virtual“) participants are added and shown in
all results, where applicable. The first of those has the shorthand symbol „MES” and represents the
actually measured data at the target masts, to that the participants contributions are compared. This
data was not made available to the participants during the test. The second „virtual“ participant has the
shorthand symbol „SPL“, which stands for the „simple“ method, which uses the reference mast data as
it is, without any transformation or modification, i.e. the „SPL” method neglects any horizontal or
vertical variation of the wind conditions in the area in question, therefore representing the reference
mast data.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 14 / 173
Istitution/Company Address Contact Person
Anemos
Gesellschaft fuer Umweltmeteorologie mbH
Bunsenstrasse 8
D-21365 Adendorf, Germany
H.-T. Mengelkamp, Sven Huneke
CeBeNetwork GmbH Gewerbepark ATP
Hein-Saß-Weg 36
D-21129 Hamburg
René Volkert
GEO-NET Umweltconsulting GmbH Große Pfahlstraße 5
D-30161 Hannover, Germany
Peter Trute, Ingo Wendt
Lahmeyer International GmbH Friedberger Str. 173
D-61118 Bad Vilbel, Germany
Volodimir Kremenetskiy, Oliver Heil
Meteodyn 75 Bd, Alexandre Oyon
72100 LE MANS
Aurélien Chantelot
RWTÜV SYSTEMS GmbH Langemarckstraße 20 45141 Essen - Germany H.O.Wulf
Fachhochschule KIEL , FB Maschinenwesen Grenzstrasse 3 D-24149 Kiel - Germany Prof. Dr. Alois Schaffarczyk
Kyushu University Department of Mechanical Engineering Science,
Kyushu University
744 Moto-oka, Nishi-ku, Fukuoka, 819-0395 JAPAN
Prof. Hikaru Matsumiya
Repower Systems AG Alsterkrugchaussee 378
D-22335 Hamburg
Tomas Blodau-Konick
Table 2: List of participants, respective addresses and contact persons.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 15 / 173
Anemos GmbH Geo-Net
GmbH
Lahmeyer
International
GmbH
Meteodyn Tüv Nord Uni-Kiel Kyushu-University REpower
Shorthand
Symbol
ANM GEO LAM MET RTV UNK UNJ REP
Name and version
of the used model
MM5 + METRAS FITNAH KLIMM_32 Meteodyn WT
2.0
Austal2000 FLUENT 5 LES Windsim
Developer of the
model
MM5: Pennsylvania
Atate
University/NCAR
Metras: Univ. HH
G. Gross,
Hannover
Institute of
Atmospheric
Physics,
University of
Mainz, Lahmeyer
International
METEODYN Ingenieurbüro
Janicke, Dunum
FLUENT Inc. Kyushu Univercity,
CRC Research
Institute, Inc.
Name of
underlying model
and version
MM5: MM5V3.7
METRAS: Version
1.0
not specified Version 3.2 Meteodyn WT
2.0
not specified Fluent not specified not specified
Developer of the
underlying model
MM5: Pennsylvania
State University /
National Center for
Atmospheric
Research, Metras:
Univ. HH
not specified not used METEODYN not specified not specified not specified not specified
References on the
model
MM5:
http://www.mmm.u
car.edu/mm5/
Metras: Schlünzen,
K.H., Bigalke K.,
Lüpkes C. &
Niemeier U. von
Salzen K. (1996):
Concept and
realization of the
mesoscale
transport- and fluid-
model METRAS.
Meteorologisches
Institut Universität
Hamburg. METRAS
Techn. Report, 5, pp
156
e.g.
Meteorol.Ztsc
hr.,2002, 295-
302;
J.Geophys.Re
s. 1998, 7875-
7886,
Numerical
simulation of
canopy flows,
Springer
Verlag 1993
Beitr. Phys.
Atmosph.,
November 1997,
p.301-317, A
Three-
Dimensional
Viscous
Topography
Mesoscale
Model
www.meteodyn.
com ; „For a
reliable wind
assessment
whatever the
terrain“,
D,Delaunay,
poster EWEC 04.
„Wind field
evaluaiton in
complex terrain
for transport
safety
applications“,
D.Delaunay,
ERCOFTAC 04.
not specified not specified Kogaki,
T.,Kobayashi, T.,
Taniguchi, N.,
1999,
„Conservative
Finite Difference
Schemes for
Incompressible
Turbulent Flow in
Generalized
Coordinates”,
Turbulence and
Shear Flow
Phenomena -1:
First International
Symposium, Santa
Barbara,
California.
not specified
Table 3 (Part 1 of 5): Model description as reported by the participants.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 16 / 173
Anemos GmbH Geo-Net
GmbH
Lahmeyer
International
GmbH
Meteodyn Tüv Nord Uni-Kiel Kyushu-University REpower
Shorthand Symbol ANM GEO LAM MET RTV UNK UNJ REP
Field Variables used
by the model
MM5: all
Mtetras: all
Wind vector,
temperature,
humidity, pressure,
turbulent kinetic
energy, soil
variables
(temperature,
water)
Wind Vector V,
Temperature
gradient, Pressure
P, Turbulent Kinetic
Energy
Wind vector V,
Pressure P,
Turbulente Kinetic
Energy
not specified Wind Vector V,
Potential
Temperature T
Pressure P,
Turbulent Kinetic
Energy TKE, TKE-
Dissipation-Rate
EPS, ...
Wind Vector V,
Pressure P
not specified
Does your model use
the hydrostatic
approximation?
MM5: no
Metras: no
No No No not specified not specified No not specified
Does your model
treat the
atmosphere as
compressible?
MM5: No
Metras:: no
No No not specified not specified yes, possible No not specified
Does your model
describe the effect of
the Coriolis force?
MM5: Yes
Metras:: Yes
Yes Yes No not specified yes, possible No not specified
Space discretization MM5: finite
differences
Metras: finite
differences
Finite differences Finite volumes Finite Volume not specified FV Finite differences not specified
General Type of Grid MM5: Cartesian
Metras: Cartesian
Variable
(horizontal), terrain
followinf (vertical)
Cartesian Structured grid with
vertical and
horizontal
refinement
not specified unstructured BFC Structured/Boundary
Fitted
not specified
Structured grid
topology
MM5: nested if
requied
Metras: nested if
requied
Nested grids Single-Block,
Rendering
Single-Block not specified unstructured BFC Single-Block not specified
Unstructured grid
cell type
0 0 - 0 not specified tets, hex, pyramids
prims
not specified
Variable horizontal
grid spacing?
MM5: Yes
Metras: Yes
Yes Yes Yes not specified Yes, possible Yes not specified
Typical vertical
grid spacing [m]
(If variable please
specify the range)
MM5: variable to
be decided
Metras: variable
to be decided
5m near the
ground 500 m at
top (typically
6000-8000 m)
20 m up to 1000
m, if required
5m at the ground
to 200m at the
top
not specified variable
depending on
topography
Variable not specified
Table 3 (Part 2 of 5): Model description as reported by the participants.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 17 / 173
Anemos GmbH Geo-Net
GmbH
Lahmeyer
International
GmbH
Meteodyn Tüv Nord Uni-Kiel Kyushu-University REpower
Shorthand Symbol ANM GEO LAM MET RTV UNK UNJ REP
Minimum usable
horizontal grid
spacing in complex
terrain [m] (estimate)
MM5: 1km
Metras: 50m
1 m for airflow
around individual
obstacles (e.g.
buildings) , 50-100
m for wind energy
studies
20 m up to 200 m,
typically 50 m to
100 m grid cell
resolution is
applied
5m 30m 1/1000 of
computational
horizontal
extension
0.5m not specified
Typical number of
horizontal grid points
(if appropriate)
MM5: to be
decided
Metras: to be
decided
200 x 200 typically 400 * 400
* 40 -> 6.400.000
depending on
hardware/processi
ng
220x220 not specified 150 x 150 200x300 not specified
Typical number of
grid points in the
vertical direction (if
appropriate)
MM5: to be
decided
Metras: to be
decided
30-50 typically 30 to 50
vertical cells
40 not specified 50 70 not specified
Is the structured grid
smoothed, e.g. by
Laplace-Type or
Poisson-Type
smoothing
operations?
MM5: no
Metras: no
no if converging
problems appear,
the grid can be
smoothed with
several methods
other not specified laplace (ICEM/CFD) Poisson not specified
Iteration type MM5 : impicit
Metras: impicit
explicit Implicit Implicit not specified both possible Semi implicit
(Adams-Bashforth
for convection
terms and Crank-
Nicolson for
diffusion terms)
not specified
Convection scheme(s)
used
MM5: Kain-
Fritsch 2
(includes
shallow
convection), tbd
Metras: tbd
centered
differencing
ADI - method UDS not specified 2nd order upwind
schema
second-order
upwind scheme
(QUICK Scheme)
not specified
Type of Wind
Velocity Vector
MM5: cartesian cartesian Cartesian not specified not specified cartesian at cell
centre
Cartesian not specified
Variable arrangement
and type of
horizontal staggering
MM5: B-grid
staggering
Metras:
Arakawa C grid
Arakawa C equidistant in x and
y - direction
Colocated not specified co-located
(probably)
Colocated not specified
How do you state
that your
simulation has
converged? (if it
applies)
residuals Mean
differences in a
5 min interval
falls below
threshold
Maximum
change in
variable falls
below threshold
Residuals fall
below a
threshold
not specified residuals falls
three orders of
magnitude,
changing of
special varables
Residuals fall
below a
threshold
not specified
Table 3 (Part 3 of 5): Model description as reported by the participants.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 18 / 173
Anemos GmbH Geo-Net
GmbH
Lahmeyer
International
GmbH
Meteodyn Tüv Nord Uni-Kiel Kyushu-University REpower
Shorthand Symbol ANM GEO LAM MET RTV UNK UNJ REP
Sub-grid turbulence
parametrization
(turbulence closure)
MM5: tke based
MY 2 .5 closure
Metras: MY level
2.5
TKE 1st order scheme,
TKE based
TKE Based not specified standart k-epsilon Large eddy
simulation or
Pseudo large eddy
simulation
not specified
Type of k-epsilon
model (if applies)
not specified not specified None not specified not specified launder-spalding,
spalard-allmeras
not specified not specified
Planetary
Boundary Layer
parameterization
(If any)
MM5: Eta PBL
(predicts TKE
and has local
vertical mixing),
tke
Metras: tke
not specified None M.O not specified None not specified not specified
Land-surface model
(if any)
MM5: 5-layer
soil model, tbd
Metras: tbd
FITNAH (surface)
(e.g. Meteorol
Rdsch. 1991, 97-
112)
Viscosity - model not specified not specified None not specified not specified
Radiation
parametrization
(if any)
MM5: Cloud-
radiation
scheme
Metras: tbd
FITNAH (radiation)
(e.g. Meteorol.
Rdsch. 1991, 97-
112)
None not specified not specified None not specified not specified
Other
parametrizations
MM5: Cumulus:
New Kain-Fritsch
Metras: tbd
cloud microphysics,
urban canopy,
forest canopy
None not specified not specified None not specified not specified
Time dependent
simulation with
time dependent
boundary
conditions or
steady state
simulations?
MM5: Time
dependent
simulation with
time dependent
boundary
conditions
Metras: both
probably
steady state
simulation
Steady state
simulation
Steady State
simulation
not specified steady state
prefered, transient
possible but CPU-
time consuming
Time dependent
simulation with
fixed boundary
condition
not specified
Do you use
domain nesting?
One-way or two-
way? How many
domains?
MM5: depends
on the area
Metras: depends
on the area
nesting with 4
domains
Nesting No nesting not specified do you mean
multi-griding ?
Yes not specified
Table 3 (Part 4 of 5): Model description as reported by the participants.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 19 / 173
Anemos GmbH Geo-Net
GmbH
Lahmeyer
International
GmbH
Meteodyn Tüv Nord Uni-Kiel Kyushu-University REpower
Shorthand Symbol ANM GEO LAM MET RTV UNK UNJ REP
Typical calculation
time to obtain
information on wind
conditions in a wind
farm in complex
terrain (about
1km2). If you run
time dependent
simulations,
consider a period of
one year.
MM5: 1-2 month
Metras: 1-2 month
1-3 days Typically 20 m
resolution with 50
x 50 x 40 cells
require 2 days for
stationary
condition on a
modern PC
One day not
specified
2-4 hours of CPU
time for one run
(time step)
Several years with
finest scale
analysis
not specified
Table 3 (Part 5 of 5): Model description as reported by the participants.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 20 / 173
5 Description of the Main Test
The Dummy Run was a useful step to identify issues in the data requirement and to improve the data
flow between DEWI and the participants. Since all major issues in the data requirement and in the data
flow were clarified, it was possible to use the same data-set type and the same structure as used for the
„Dummy Run“. The participants already had, in some way, familiarity with this data-set type and the
respective format. Similarly, the variables requested as output are basically of the same kind and with
the same format as those requested during the Dummy Run.
5.1 Input Data-set
The input data for the test was a set of gridded and punctual data describing elevation, land cover and
meteorological situation for an area close to the site (about 8 km around the point of interest) and for
the mesoscale area surrounding the site (for an area extending approximately 200 km around the
location of interest). The aim was to provide the relevant input data for both microscale and mesoscale
models. The participant was free to choose the data that he requires among those that are provided by
DEWI. The use of other data outside this data-set was not allowed. Information about the source and
format of the input data-set is provided in Table 4.
Variable Format File name
Elevation – fine scale ASCII Surfer Grid data/elevation/fine/elevation-fine.grd.zip
Elevation – large scale Geotiff data/elevation/large/elevation-large.tif.zip
Land cover – fine scale ASCII Surfer Grid data/landcover/fine/landcover-fine.grd
Roughness Lenght - fine scale ASCII Surfer Grid data/landcover/fine/roughness-fine.grd
Land cover- large scale Geotiff Data/landcover/large/landcover-large.tif.zip
Wind conditions close to the site MS Excel file Data/meteo/winddata/winddata.xls
Reanalysis data NetCDF Data/reanalysis/XXX.200X.nc.zip
Upper soundings ASCII Data/soundings/sound.zip
Reference mast coordinates MS Excel file Data/coordinates/reference.xls
Target coordinates MS Excel file Data/coordinates/target.xls
Table 4: Summary of the input data for the main test
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 21 / 173
5.1.1 Elevation
Two data-sets were provided:
- a high resolution digital elevation model for the area close to site;
- a coarser-resolution digital elevation model for the mesoscale area around the site.
5.1.1.1 Elevation close to the site
This data, derived by topographic maps edited by Istituto Geografico Militare (IGM), describes the
terrain elevation of an area extending about 16.5 km in the South-North direction and 18 km in the
West-East direction. This area is approximately centred on the location of the reference mast. The grid
spacing is equal to 10 m. Values of elevation are in meters. The coordinates were given in UTM zone 32,
the datum was according to WGS84. The format was ASCII Surfer grid.
H:\gruppe\micrositing\Forschung\RoundRobinSimulation\doc\final_report_tables_figures\cutted\
Figure 1: Fine scale elevation data-set used by the participants. The position of the three measurement masts used
for the assessment of the models is reported.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 22 / 173
5.1.1.2 Elevation ~ 200 km from the site
A second elevation data-set, derived from the Shuttle Radar Topography Mission (SRTM), describes the
terrain elevation for a rectangular area extending approximately 500x400 km. The grid spacing is
0.0008333° (~90 m). Elevation values are expressed in meters above the mean sea level. The
coordinates are given in the geographical latitude-longitude coordinate system with the ellipsoid
according to the WGS84 datum. Provided format was GeoTiff.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 23 / 173
5.1.2 Land Cover
Two data-sets of land cover at two different resolutions were provided to the participants. Both data-
set are derived by the EU „CORINE land cover 2000 vector by countries” data-set and checked against
photographs taken during a site visit and topographic maps for the area close to the measuring masts.
The land cover data-set was given to derive values of roughness length or whatever other property
required by the model (evaporation, albedo etc.). The participants were asked to assign values for this
properties according to their usual practice. Among these variables, the roughness length usually plays
an important role in fluid-dynamic simulations and together with elevation represent the only two
variable needed to describe the lower boundary conditions for most of the microscale models used in
wind energy. For this reason, for the area close to the site, the participants were directly provided with
an additional data-set of roughness length. Since the derivation of the roughness length from the
observation of land cover properties is in itself a somehow arbitrary process (and, above all, models
may use different roughness length definitions), the participants were asked to check, and possibly
modify, the roughness values against the corresponding land use categories.
5.1.2.1 Land cover close to the site
This data-set describes land cover for an area extending about 16.5 km in the SN direction and 18 km in
the WE direction. The area is approximately centred on the location of the reference mast. The grid
spacing of this data-set is equal to 10 m. The coordinates system is UTM, zone 32, ellipsoid is according
to WSG84. Provided format is Surfer ASCII grid. A table which relates each land cover category to the
respective codes was given as separate MsExcel file.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 24 / 173
Figure 2: Fine scale land use data-set used by the participants. The position of the three measurement masts used for
the assessment of the models is reported.
5.1.2.2 Roughness length close to the site
Values of roughness length according to the European Wind Atlas classification are given in the file
roughness-fine.grd. These data describe the surface roughness length for an area extending about 12.5
km in the South-North direction and 14 km in the West-East direction. This area is approximately
centred on the location of the reference mast. The grid spacing is equal to 10 m. The coordinates
system is UTM, zone 32, ellipsoid is according to WSG84. Provided format is Surfer ASCII grid. For the
reasons mentioned in Section 5.1.2, the participants were encouraged to check and possibly modify
these values according to the respective land cover categories.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 25 / 173
5.1.2.3 Land cover ~ 200km from the site
A second land cover data-set, derived from the EU CORINE database, classifies terrain land cover for a
rectangular area extending approximately 500x400 km.
The grid spacing of this data-set is 0.0008333° (~90m). The coordinates were given as geographical
latitude longitude, Coordinate system and ellipsoid are according to WGS84 datum. Format is Geo-Tiff.
A table which relates each land cover category to the respective codes was given as separate MsExcel
file.
5.1.3 Meteorological data
Three sets of meteorological data were provided:
1. Wind measurements from a cup anemometer and wind vane at the site;
2. Upper soundings for one locations in the same mesoscale domain;
3. Global reanalysis data.
A description of each data-set is given in the following.
5.1.3.1 Wind measurements at the site (file WindData.xls)
The participants received wind measurements at the site for the reference point x=XXXXX, y=XXXXX
(coordinates in UTM WGS 84, Zone 32). Wind speed was measured at 43 m above ground level by a
Thies „First Class” cup anemometer, that was calibrated according to MEASNET standard. The wind
direction sensor (a „Thies compact” wind vane) measured wind direction at a height of about 42 m
above ground. The sampling frequency was 1 Hz. The averaging interval is 10 minutes. The data spans
the period 09/11/2005 – 30/06/2006. All data showing wind direction in the range [83° - 172°] have
been excluded from the data-set in order to minimize the effect of the mast top tube on the
measurements. For this reason several gaps affect the data-set. The wind speed time series is provided
as MS-Excel file. A photograph of the measuring mast is reported in Figure 3. As can be noticed, an
additional anemometer, of the type Thies „Classic“ is mounted on the top of the vertical boom. Many
studies have enlighten that the outdoor dynamic behaviors of the anemometers of different types can
lead to difference in the measured wind speed of some percent. Since all anemometers mounted on
the two target masts are of the type „Thies First Class“ we decide not to use the top anemometer as
reference (despite its better position) and to prefer, on the contrary, the use of the boom-mounted
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 26 / 173
„Thies First Class“ anemometer. In this way it has been possible to perform the comparison with an
homogeneous set of sensors. In order to separate as much as possible the evaluation of the wind
speed and wind direction and to obtain a more complete information on the performance of the
models, DEWI additionally provided 24 time series, one for each 15° direction sector. Each time series
contains only data with wind direction falling in a certain sector, therefore the data had several gaps.
The participants were asked to calculate the wind conditions at the target positions for each wind
direction sector (more details are given in Section 5.2).
Manufacturer and Type of Sensor Height above ground level Direction of the boom
Thies clima 4.3350.00.000 43 m 309°
Thies clima 4.3129.00.012 42 m 209°
Table 5: properties of the two sensors mounted on the reference mast.
Figure 3: Detail of the sensors mounted on the top section of the measuring mast (left) and picture of the entire
measuring system (right).
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 27 / 173
5.1.3.2 Upper sounding
A set of 6 hourly sounding reports for the period from October 2005 to November 2006 was provided
for the location Cagliari (9.05° W, 39.25° N). The soundings were not continuous, therefore gaps (even
of several days) occur in the time series. The following atmospheric variables were measured:
- Air pressure
- Height a.s.l.
- Air temperature
- Dew Point
- Relative humidity
- Mixing ratio
- Wind direction
- Wind speed (knots!)
- Potential temperature
- Equivalent potential temperature
- Virtual potential temperature
Each file contains upper-air reports for one month. Data were provided as ASCII files.
5.1.3.3 Global Reanalysis
Data from the „50 years NCEP/NCAR Reanalysis Project” were delivered for year 2005 and 2006 for the
following variables:
- U (zonal) component of the wind
- V (meridian) component of the wind
- Relative humidity
- Air temperature
- Geopotential Height
- Sea level pressure
- Skin temperature
All data, except skin temperature, were given on a regular grid with a resolution of 2.5° with a temporal
resolution of 6 hours. Skin temperature was given on a Gaussian grid. Longitude points for skin
temperature are listed in the self-describing file. The coverage for all variables was global. The grids for
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 28 / 173
u,v, relative humidity and air temperature have values on 17 vertical pressure levels. Grids for Sea Level
Pressure and Skin Temperature are two-dimensional. The reanalysis data-set has been provided to the
participants as NetCDF files.
5.1.4 Coordinates
The coordinates of the reference mast and the coordinates of the target points (i.e. points for which
wind mean wind speed and wind statistics shall be calculated) were given to the participants as two
MsExcel files.
5.2 Output Data-set
Participants were asked to submit results regarding the following quantities:
- Mean Horizontal Wind Speed for three terrain following surfaces (40m, 60m and 80m above
Ground Level);
- Mean Wind Speed for two target locations at 40m, 60m and 80m above Ground Level;
- Wind Statistics for two target locations at 80 m. Wind statistics „per sectors”.
All results were required to be calculated for the time periods for which values in the input wind data
file are available. Described differently: The results (mean, statistics, etc) should not comprise the wind
conditions occurring during periods of no data availability (gaps). Participants were instructed to not
correlate the on-site wind data with wind data from other sources to fill the gaps in this time series.
This condition is particularly important because the evaluation is bound to exactly those time steps that
are present in the on-site wind data time series. We would like to point out that the aim of the Round
Robin is to assess the capability of the models to transfer wind speed times series from one point to
another, correlation methods are not subject of this test. A description of the requested variables and
their respective format is given in the following sections.
5.2.1 Mean Horizontal Wind Speed for terrain-following surfaces
The participants were asked to calculate, for the time steps present in the input on-site wind data
(winddata_all.xls), the mean wind speed for three different heights (40m, 60m, 80m) above ground for
the following rectangular area (all coordinates in UTM WGS 84 Zone 32):
EAST: From X1 = XXXXX m to X2 = XXXXX m
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 29 / 173
NORTH: From Y1 = XXXXX m to Y2 = XXXXX m
The horizontal grid should consist therefore of 1067 (west-east) by 1098 (north-south) grid cells. The
required grid spacing was equal to 10 m. This grid spacing only refers to the format of the data to be
submitted to DEWI. Participants were allowed to perform the simulation at any desired resolution.
5.2.2 Mean Wind Speed for the target locations
For the time steps present in the input on-site wind data, the participants were asked to calculate the
mean wind speed at 40m, 60m, 80 above ground for the positions of the two target masts.
5.2.3 Wind Statistics for target locations in 80 m above Ground Level
With „Wind Statistics“ we refer to the percentage share of data that falls in a combined wind direction
and wind speed interval. For the time steps present in the input file winddata-all.xls, the participants
were asked to calculate the wind statistics for the location reported in the file target.xls at 80 m height
above ground level. In order to better separate wind direction effects, the participants were asked to
provide 24 separate directional wind statistics. Each directional wind statistics should describe the wind
conditions occurring during the periods contained in each of the 24 given time series at the target mast.
i.e. one statistics for the time steps contained in winddata_000.xls, one for the time steps contained in
winddata_015.xls, etc.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 30 / 173
6 Assessment of the Results
6.1 Weibull A- and k-Parameter
DEWI has compared Weibull A and k parameters calculated from the predicted tab with parameters
obtained from observed wind data at the target masts. The Weibull fit was calculated according to the
method specified in the European Wind Atlas method. The measured and predicted parameters are
reported in Figure 4 (A (scale) parameter) and Figure 5 (k (shape) parameter).
No (relative) difference is calculated or shown. The actual differences in the k-parameter at the
reference and at the target masts are, in this case, approximately equal to 0.04. It can be noticed that
all models but „RTV” and „UNK” were under-predicting the scale parameter for both masts.
A very interesting result comes from the observation of the shape parameter. A large number of
models were basically reproducing the shape parameter of the reference mast („SPL” in the plot)
without improving the initial information. This can be seen as an hint that these models are affected by
difficulties in capturing horizontal and vertical variations of the shape parameter.
It is very difficult to find a single clear explanation for the errors found for the wind distribution. It can
be advanced the hypothesis that a certain number of participants have performed steady state
simulations with fixed boundary conditions only for a single wind speed. This hypothesis cannot be
confirmed at the present stage without collecting further information on the way the participants
applied their models and on the applied post-processing methods.
The present evaluation focuses on the ability of the considered models to properly predict energy
yields. Nevertheless it is worthwhile to recall here the importance of a reliable prediction of the wind
speed distribution for the estimation of the extreme winds. It is true that for a proper extreme wind
assessment a linear scaling of the wind conditions can lead to a wrong prediction of the actual intensity
of the extreme winds in complex terrain. The participant “GEO”, for instance, under-predicted by far
the shape parameter, with the difference between modelled and measured k parameter approximately
equal to 0.28. As mentioned above, this kind of underestimation might have important effects if the
calculations would be used as basis for the standards methods of estimation of the extreme winds.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 31 / 173
5.5
6
6.5
7
7.5
5.5 6 6.5 7 7.5
Wei
bull
A at
Tar
get
Mas
t 2 [
m/s
]
Weibull A at Target Mast 1 [m/s]
Weibull scale parameter A
6.8,6.0 ANM
5.8,6.2 GEO
6.0,6.5 LAM
6.8,6.6 MES
6.3,6.2 MET
5.9,5.8 REP
7.3,7.2 RTV
5.6,5.6 SPL
6.4,6.3 UNJ
6.2,6.6 UNK
Figure 4: Weibull scale parameter.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 32 / 173
1.5
1.6
1.7
1.8
1.9
2
1.5 1.6 1.7 1.8 1.9 2
Wei
bull
k at
Tar
get
Mas
t 2 [
-]
Weibull k at Target Mast 1 [-]
Weibull shape parameter k
1.68,1.79 ANM
1.58,1.57 GEO
1.89,1.92 LAM
1.85,1.84 MES
1.79,1.80 MET
1.78,1.77 REP
1.80,1.80 RTV
1.81,1.81 SPL
1.80,1.79 UNJ
1.67,1.70 UNK
Figure 5: Weibull shape parameter.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 33 / 173
6.2 Mean Horizontal Wind Speed for a terrain-following surface at different heights
Separately for three terrain following surfaces (40 m, 60 m, 80 m) the participants calculated the wind
conditions for an area of 1067 (west-east) by 1098 (north-south) grid cells.
DEWI has averaged the wind speed maps provided by the participants point by point to three average
wind speed maps. Afterwards, for each participant and height level, the relative deviation of the map
from the averaged map is calculated and afterwards displayed together with the mean map.
The calculated mean of all models at the points of the target masts in 80 m is equal to 5.79 m/s for
target mast 1 and 5.78 m/s for target mast 2. These values differs from the measured wind speed of
about 5% for target mast 1 and about 3% for target mast 2. Since there is no way to compare these
results with measurements over all points of the domain, the following considerations will have mainly
a qualitative nature. Nevertheless this comparison represents a useful diagnostic for a better
understanding of results of the tests described in the previous and following sections.
Figure 6 shows the point-by-point mean of all participants for three different heights. Figure 7 to Figure
13 reports the mean wind speed (left side) and relative deviation from the all mean (right side) for all
participants. The relative deviation from the mean (RDM in the following) at different height can give
useful information about the vertical variation of the wind conditions of each model. For instance a low
RDM at 40 m and a high RDM at 80 can be a signal for a too high wind shear, that, in turn, can be the
effect of a too high atmospheric stability and/or too high roughness length. It can be argued that this
was the case for participant „RTV”. This can be also an explanation for the overestimation of the wind
conditions by this participant in the remaining tests. The other participants seem to approximately
maintain constant RDM at different heights.
Another information can be derived by the observation of the grid resolution. Participants delivered
information about the typical resolution of their model before the beginning of the test (see Table 3). It
is not certainly known at which resolution the participants executed the simulation for this specific test.
Anyway some of the considered models produce significant spatial differences in wind speed over
scales of few tens of meters. As an example, “UNJ” and “LAM” present relatively high horizontal
variation, especially for the north part of domain. For these participants, mean wind speed can vary, in
some areas, by 3% over distances of 30m. Such gradients are confirmed by our site calibration
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 34 / 173
measurements in complex terrain, where sometimes gradients of 15% are observed for distances of
180 m. It is clear that a model, which operates with a resolution coarser than about 20m to 30m, can
not sufficiently capture high variations. This seems to be the case for the participant “ANM” for which
the horizontal structure of the wind field suggests that a comparably coarse resolution was used.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 35 / 173
Figure 6: Point-by-point mean of all participants. Wind speed at 40 m (above), 60 m (centre) and 80 m (below).
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 36 / 173
Figure 7: Participant „ANM”. Mean wind speed at 40 m (above, left), 60 m (centre left), 80 m (below left) and relative
difference from the mean of all models at 40 m , 60 m , 80 m (Right column).
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 37 / 173
Figure 8: Participant „GEO”. Mean wind speed at 40 m (above, left), 60 m (centre left), 80 m (below left) and relative
difference from the mean of all models at 40 m , 60 m , 80 m (Right column).
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 38 / 173
Figure 9: Participant „LAM”. Mean wind speed at 40 m (above, left), 60 m (centre left), 80 m (below left) and relative
difference from the mean of all models at 40 m , 60 m , 80 m (Right column).
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 39 / 173
Figure 10: Participant „MET”. Mean wind speed at 40 m (above, left), 60 m (centre left), 80 m (below left) and relative
difference from the mean of all models at 40 m , 60 m , 80 m (Right column).
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 40 / 173
Figure 11: Participant „RTV”. Mean wind speed at 40 m (above, left), 60 m (center left), 80 m (below left) and relative
difference from the mean of all models at 40 m , 60 m , 80 m (Right column).
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 41 / 173
Figure 12: Participant „UNJ”. Mean wind speed at 40 m (above, left), 60 m (center left), 80 m (below left) and relative
difference from the mean of all models at 40 m , 60 m , 80 m (Right column).
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 42 / 173
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 43 / 173
Figure 13: Participant „UNK”. Mean wind speed at 40 m (above, left), 60 m (center left), 80 m (below left) and relative
difference from the mean of all models at 40 m , 60 m , 80 m (Right).
6.3 General Remarks on the Evaluations Regarding Wind Speed
As detailed before and in the appendix, the common time series of the wind speed and direction data
of the reference mast and the two target masts is considered (common time steps). From this time
series, all data sets are excluded that show a wind direction at the reference mast in between 82.5
degree and 172.5 degree in order to minimise effects from the mast top tube on the wind speed sensor.
This time series is then subdivided into 15 degree wind directions sectors with respect to the wind
direction measured at the reference mast. DEWI provided the participants with the time series of wind
speed and direction at the reference mast (without the disturbed sector), in the form of 10 minute
average values of wind speed, direction, wind speed maximum, minimum and standard deviation for
each 10 minute interval. The participants were asked to transform this data towards the two target
masts and to submit the resulting wind statistics (TABs) for the two target masts to DEWI as their result.
Additionally, the participants were asked to transform towards the two target masts also the time
series that contain only data from within one 15 degree wind direction sector at a time and return to
DEWI the transformed data from each of those sectors as a result. The second step regarding the
sector-wise transformation enabled DEWI to carry out detailed wind direction dependent analyses that
allow a more detailed model assessment compared to the use of just one output statistics for all
undisturbed sectors.
6.3.1 Technical details on the assessment of the statistics
The quantitative evaluations of the wind statistics (TABs) was conducted as follows:
1. No sector-wise evaluations of the overall TAB were conducted (i.e. of the TAB that the participants
submitted as a result of their transformation of the time series containing all data except the
disturbed sector). The reason is that if we would compare this TAB to the measured one sector by
sector, we would mix model errors regarding wind speed with those that are related to wind
direction. Those mixing errors have significant influence on the sector-by-sector comparison but
will in a real wind resource assessment by far not play such a significant role. As a result, the overall
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 44 / 173
tab, as it is defined above, is only evaluated regarding the overall, wind direction independent wind
speed distribution and regarding the single turbine and farm energy yield that is calculated with
that statistics. For the comparison of the overall, direction independent values of mean wind speed,
mean squared wind speed and mean cubed wind speed, these values are calculated from the TABs
(wind statistics) in the following way: The relative share of data that falls into each wind speed
interval of 1 m/s width is multiplied by the average of the upper and lower wind speed class
boundaries (i.e. 0.5 m/s for the wind speed interval [0m/s, 1m/s[) and taken to the power of 1,2 or
3, depending on the type of assessment (mean wind, mean squared, mean cubed wind speed).
Resulting values are summed over all wind speed intervals containing data. Relative shares given in
the TAB files regarding wind direction and wind speed are normalised separately such that the
relative shares always sum to 1.
2. The mean, mean squared and mean cubed wind speed of the sector-wise statistics (i.e. those
statistics that are the result of the transformation of the reference mast data that is reduced to one
15 degree wind direction sector at a time) is also evaluated according to the summing procedure as
detailed above.
3. As a result, for the evaluations regarding wind speed (squared, cubed wind speed), the statistics
(TABs) from the participants are evaluated only regarding the wind speed. The fact that the data in
the wind statistics may be slightly dispersed over different sectors even for the „single sector TABs“
has no influence on the results. This dispersion is considered in the assessments regarding wind
direction.
4. The participants results are compared to the measured data. The measured mean (sector-wise and
overall) wind speed, mean squared and mean cubed wind speed is also calculated by first creating a
statistics (TAB) and afterwards summing up the statistics as detailed above. An alternative way
would be to calculate the measured values directly from the time series, without using an
intermediate statistics. However, if a participant would submit exactly the correct measured
statistics, he should get assigned a relative deviation from the measured data of 0.0%, i.e. an exact
match. If we would compare participants results to values obtained directly from the time series,
this exact match would not be guaranteed, due to the wind speed resolution of 1m/s of the
statistics. For the test, we considered the use of TABs also for the measured data as most
appropriate, because otherwise we should have asked the participants to provide time series for
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 45 / 173
the target masts instead of statistics. But most models do by default output only statistics and not
time series. As the participants provide statistics with a resolution of 1m/s, we find it reasonable to
compare that to the values obtained from such a statistics also.
The participants were asked to submit result statistics (TABs) for the target mast. In addition, they were
asked to submit to DEWI mean wind speeds for the positions of the two target masts for the height
levels 40m, 60m and 80m. A comparison of the different submissions is shown in Table 6.
It can be observed that for participants ANM, MET, REP and UNJ there are no significant differences
between the mean wind speed that they submitted as a number and the mean wind speed that DEWI
calculated from the statistics that the participants submitted for the target masts. For GEO, LAM, RTV
and UNK there are significant deviations: The mean wind speed that they submitted as a number is
higher than the mean wind speed that DEWI calculated from the submitted statistics (up to 7%).
This shows once again that there are different methods for the calculation of mean wind speed. It may
be calculated from the time series directly, it may be calculated from a statistics or it may be calculated
from Weibull parameters that are fitted in some way to the statistics. It is not known to DEWI, how the
participants calculated the mean wind speed. In order to maintain overall consistency, we decided to
use for the main comparison between the models regarding mean wind speed only the mean wind
speed that we calculated from the submitted statistics, because otherwise we would possibly compare
mean wind speeds calculated with different methods and because we consider the mean wind speed
calculated from the statistics as an appropriate measure.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 46 / 173
Partici-
pant ID
Target Mast
1 (80m)
Target Mast
2 (80m)
Target
Mast 1
(40m)
Target
Mast 1
(60m)
Target
Mast 1
(80m)
Target
Mast 2
(40m)
Target
Mast 2
(60m)
Target
Mast 2
(80m)
Target
Mast 1
(80m)
Target
Mast 2
(80m)
Target
Mast 1
(80m)
Target
Mast 2
(80m)
Target
Mast 1
(80m)
Target
Mast 2
(80m)
ANM 6.04 5.31 5.31 5.77 6.04 4.57 5.04 5.31 100% 100% 99% 89% 99% 89%
GEO 5.38 5.87 4.68 5.04 5.33 5.06 5.44 5.74 99% 98% 87% 96% 87% 96%
LAM 5.38 5.82 4.96 5.32 5.68 5.13 5.58 5.97 106% 103% 93% 100% 93% 100%
MET 5.69 5.59 5.04 5.40 5.68 5.03 5.34 5.59 100% 100% 93% 93% 93% 94%
REP 5.29 5.22 n.s. n.s. 5.29 n.s. n.s. 5.23 100% 100% 87% 87% 87% 88%
RTV 6.55 6.48 5.16 6.17 6.87 4.84 5.82 6.54 105% 101% 113% 109% 113% 110%
UNJ 5.79 5.69 4.95 5.50 5.78 4.94 5.43 5.69 100% 100% 95% 95% 95% 96%
UNK 5.55 5.88 4.96 5.42 5.76 5.64 6.01 6.30 104% 107% 94% 105% 94% 106%
n.s. : value not submitted
Target mast 1, mean wind speed calculated from the measured time series: 6.10 m/s
Target mast 2, mean wind speed calculated from the measured time series: 5.95 m/s
Target mast 1, mean wind speed calculated from the measured wind statistics: 6.11 m/s
Target mast 2, mean wind speed calculated from the measured wind statistics: 5.98 m/s
Ratio of wind speed, submitted as a number, to ...
Mean Wind Speed,
calculated by DEWI from
Target Mast Statistics
submitted by Participants
[m/s]
Mean Wind Speed, submitted to DEWI as a
Number [m/s]
...wind speed as
calculated by DEWI
from the submitted
Statistics [%]
...measured wind
speed as calculated
by DEWI from
Statistics [%]
...measured wind
speed as calculated
by DEWI from the
time series [%]
Table 6: Comparison of submissions regarding mean wind speed.
6.4 Important Remarks regarding the Results of the Participant ANM
Looking at the wind data analysis (see appendix) and the data that the participants finally submitted as
their results, this direction dependent evaluation strategy must be considered as fully appropriate, with
the exception of the results of the participant ANM. As an example consider the wind direction
distribution shown in Figure 14. This wind direction distribution refers to target point 1 and is the result
of the participant's transformation of the wind data from within the 15 degree wind direction sector
centred at north at the reference mast. Similar but in general less pronounced situations are observed
for the other directions. It can be observed that besides the peak in the distribution for the second
sector centred at 15 degree, there is a secondary peak for wind from west. Other wind directions are
also present with a small relative share. There is no indication that the secondary peak at west and the
overall small relative share of data in all sectors corresponds to the measured data (Figure 15).
It is likely that the participant ANM did not obtain the target mast results by transforming the data sets
provided by DEWI. The target mast data may be obtained directly by other means (e.g. mesoscale time
dependent simulation) and then somehow filtered to get the sector-wise results. This strategy differs
from the strategy that is most likely applied by all the other participants. This other strategy aims at
obtaining and applying information on a transformation function between reference mast and the
target masts with the help of flow models. In the simplest case, this function may be a direction
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 47 / 173
dependent wind speed scaling factor and a wind speed offset, but other, more sophisticated functional
relationships are possible (depending on wind speed / nonlinear, depending on other external
parameters).
Evaluations in the following chapters will give some information on the performance of the different
strategies for this site. However, the sector-wise evaluations with the wind direction sectors defined at
the reference mast and the „same time criterion“ that is used to obtain the suitable target mast data
does not fit very well to the evaluation of the sector-wise data of the participant ANM. Especially the
evaluations regarding wind direction effects in later chapters are of questionable applicability to the
sector-wise data of participant ANM. In particular, it is reasonable to calculate a mean wind direction
for the distribution in Figure 15 but a mean wind direction has no meaning for the distribution shown in
Figure 14).
The sector independent results of participant ANM (the result of the transformation of all the data) may
also be affected by this problem due to the gaps in the data (excluded sector). As all participants agreed
to the test evaluation procedure (including the sector-wise assessment) and expect us to carry out the
assessment in the way specified, we decided to assess also the sector-wise data of the participant ANM
in exactly the same way than the data of the others, with special remarks where necessary. Finally, we
are still convinced that our proposed sector-wise evaluation method is a suitable method to assess the
participants results, although the applicability to the data of participant ANM is questionable. The
sector-wise assessment regarding wind direction sectors defined at the reference mast is the method
that is also used in similar form in a site calibration in the context of a IEC power curve measurement.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 48 / 173
N
W E
S
Figure 14: Wind direction distribution submitted by participant ANM for target mast 1 (reference mast wind direction
sector centred at 0 degree (north).
N
W E
S
Figure 15: Measured wind direction distribution for target mast 1 (reference mast wind direction sector centred at 0
degree (north).
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 49 / 173
6.5 Incomplete Data Submitted by Participant UNJ
The participant UNJ did not submit to DEWI the sector-wise results, i.e. the results of the
transformation of the time series that contained only one 15 degree wind direction sector at a time.
This is a severe restriction on the assessment of the results of this participant and as a result, no
complete comparison is possible between the results of UNJ and the other results.
From a practical point of view, we decided not to exclude participant UNJ from the test, although this
might be considered as unfair by other participants. It is mentioned in the conclusions that no full
comparison is possible regarding the results from UNJ. Nevertheless, the other results from participant
UNJ can be compared to those of the other participants.
We hope that the other participants agree to this procedure. Participant UNJ is located in Japan. In
particular, unfortunately there was a special general holiday in Japan during the time that the
participants had for the preparation of the results. We did not know that in advance and we were then
not able to consider that due to the already present project delays. The participant had in some way to
cope with that and we are happy that he did take part.
6.6 Incomplete Data Submitted by Participant REP
The participant REP did not submit complete results.
Regarding the sector-wise results, REP did only submit the tabs containing transformed data of the 15
degree sectors centred at 180 degree and 270 degree. REP provided these tabs for each of the two
target masts. With the exception of the sector-wise results the submitted data of REP is complete.
We decided to include the sector-wise results of REP wherever possible. Possible further tests in future
must have restrictive contracts that state how the case of partial result submission is handled. Clearly,
in any average taken over sector-wise results (e.g. mean absolute values of sector-wise errors), REP is
excluded. Only in the analysis of the sector-wise deviations of the participants results from the sector-
wise mean of the participants results is REP included.
The results of REP are not directly comparable to the results of the other participants, which is
mentioned in the conclusions.
In the sector-wise plots, the results of participant REP appear in the form of two dots and not as lines,
as with the other participants.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 50 / 173
6.7 Evaluations Regarding Mean Wind Speed
Accurate calculation of mean wind speed is mainly important for site classification according to the IEC
wind turbine classes.
Figure 16 and Figure 17 report the sector-wise mean wind speeds for target mast 1 and 2, respectively,
as calculated by the participants along with the measured mean wind speed and the results of the
„virtual“ participant SPL, who neglects any horizontal and vertical variation in the wind conditions and
therefore represents the measured data from the reference mast.
At target mast 1 and 2 there is a general trend towards higher mean wind speeds for southerly winds
and increasingly lower wind speeds towards north.
All participants follow this general trend. It cannot be stated if participant REP also follows that trend
due to the fact that he only submitted results for two sectors.
There is relatively large variation among the participants sector-wise mean wind speed results: At
target point 1 the largest variation within a sector can be found at 15 degree, where participants results
vary between 3.1m/s and 6m/s, whereas the measured mean wind speed in this sector amounts to
4.2m/s. This means that the participants results range from to an underestimation of -25.7% to an
overestimation of 43.4%, which must be considered as a extremely large range of results.
Figure 18 and Figure 19 report the sector-wise percentage errors in mean wind speed for target mast 1
and 2 respectively. At target mast 1 (Figure 18), the result of MET (+43.3% error) must be considered as
an outliner, regarding the results of the other participants in this sector and regarding the results of
MET for the neighbouring sectors 0 degree and 30 degree.
Participant RTV is the only participant who overestimates sector-wise mean wind speed in all sectors at
target mast 1. With the exception of the sectors 0 degree and 15 degree, participant RTV shows for
each sector the highest overestimation.
The most pronounced underestimation of mean sector-wise wind speed at target mast 1 shows
participant GEO (sector 330 degree, -32.3% underestimation).
The situation regarding deviations from measured values is different at target mast 2 (Figure 19). As
detailed in the appendix, there is a pronounced increase of the speed-up factors regarding target mast
2 and the reference mast for the wind direction range 195 to 315 degree.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 51 / 173
For the wind direction sector centred at 15 deg, there is peak-like behaviour not only for MET (as for
target mast 1) but also for UNK.
In general, the models tend to underestimate wind speed for the range 330 deg to 75 deg. For the wind
direction range 180 deg to 330 deg, overall model performances are dominated by the fact that most of
them they fail to reproduce the strong change of the ratio of wind speeds measured at target mast 2 to
those at the reference mast. The fact that participants LAM and UNK provide an approximation of the
change of this ratio with wind direction (for the wind direction range 180 deg to 330 deg) confirms that
it has a meteorological reason and is not a measurement error.
6.7.1 Quantitative Evaluations with Respect to the Sector-wise Speed-Up Factors
Within the analysis of the measured data from the site (see appendix), a pronounced directional
pattern regarding the sector-wise speed-up factors for target mast 2 was found. Therefore it is checked
in how far the results of the participants show this pattern. The comparison is done only in a qualitative
way in order to assess if the models are in general able to reproduce these important site
characteristics. Quantitative evaluations are not conducted regarding the speed-up factors because
they have no direct meaning in terms of wind resource assessment and the ultimate goal of the
modelling efforts is not to calculate accurate speed-up factors, but to calculate accurate energy yields.
Additionally, the speed-up factors only capture simple affine sector relationships and do not account
for non-linear or otherwise determined functions.
Figure 20 and Figure 21 show the measured and simulated speed-up factors for target mast 1 and 2
respectively. Note that the measured speed-up factors are derived from the sector-wise wind statistics
due to the reasons explained in section 6.3. Therefore these speed-up factors differ slightly from those
reported in the measurement data evaluation in the appendix, where the speed-up factors were
derived from the time series. The difference is negligible for the present qualitative assessment.
6.7.1.1 Speed-up Factors at Target Mast 2
Overall, there is little similarity between measured and calculated speed-up factors, which is a
disappointing results. Only the speed-up factors calculated from the results of LAM at target mast 2 and
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 52 / 173
of ANM at target mast 1 show some similarity to the measured ones for all wind directions. In those
two cases can one assume that the models capture site specific wind flow characteristics.
For smaller wind direction ranges, many models show similarity of the calculated to the measured
speed-up factors, in particular UNK and MET (target mast 2; 180 deg to 240 deg), RTV (target mast 2;
315, 330, 345 deg) and UNK (target mast 1; 315 to 345 deg).
Regarding target mast 2 and the wind direction range 195 deg to 315 degree, measured data shows a
pronounce increase of the speed-up factor with increasing wind direction (clockwise turning).
Qualitatively, this increase is reasonably modelled only by the participant UNK, although UNK predicts
decreasing speed-up factors for wind directions greater than 300 deg.
For the sectors 180 deg up to 240 deg, the shape of the speed-up factor function is reproduced very
well by the participants UNK and MET. MET predicts increasing speed-up factors up to wind directions
of 255 deg, which fully conforms to the measured ones. Results of ANM fit very well the minimum
speed-up factor at 195 deg. To some degree also LAM reproduces the general shape of the speed-up
factor function for the wind direction range 180 deg to 345 deg, although details are visible that are not
present in the data.
Although participant ANM matches the minimum speed-up factor quite well, he fails to reproduce the
overall increasing shape of the speed-up factor function. On the contrary, ANM predicts decreasing
speed-up factors for clockwise direction turning.
Results of the participant RTV differ completely from all the other results. RTV predicts no significant
change of the speed-up factor for all directions, which does not conform to the measured data. It
seems that RTV did mainly model an average vertical wind speed increase and did by far not enough
take into account site specific smaller scale wind flow effects.
Regarding the wind direction range from 0 deg to 75 deg, the unrealistic peaks in the sector-wise
predictions of MET and UNK become obvious. The general shape of the speed-up function for this wind
direction range is not reproduced by any of the participants.
Overall, for target mast 2 and all wind directions, the results of participant LAM provide, qualitatively,
some approximation of the variation of the speed-up factors with wind direction, although it seems
that details are modelled that are not present in the measured data. Participants MET and UNK model
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 53 / 173
the shape of the speed-up function for southerly and south-westerly winds nearly perfect, but show
large differences for other directions.
6.7.1.2 Speed-up Factors at Target Mast 1
Overall, the shape of the speed-up factor function versus wind direction is best reproduced in a
qualitative sense by participant ANM.
For the wind speed range 180 deg to 345 deg, participant UNK predicts the same overall shape of the
speed-up function than for target mast 2, although the measured function is completely different
(decreases for increasing wind directions). On the other hand, participant UNK provides the best fit to
the measured function in a qualitative sense for the directions 315 deg to 345 deg.
Regarding participant RTV, the predicted speed-up function does not change much at target mast 1
compared to target mast 2. There is hardly any change with wind direction.
Results of participant MET show a peak behaviour for the direction 15 deg, similar to the peak at the
same direction for target mast 2. On the other hand, for participant UNK the peak that was present at
target mast2 at 15 deg is not present at target mast 1.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 54 / 173
6.7.2 Deviations from all Participants Mean Values
If one investigates the participants results without referring to the measured data at the target masts,
one can relate the sector-wise predicted mean wind speeds to the sector-wise mean wind speed of all
participants. This type of analysis is the base for the Round Robin tests conducted by MEASNET for
anemometer calibration, where one aims at maintaining consistent, comparable measurements and
does not refer to an externally measured value. This sector-wise „all-participants-mean“ is calculated
while taking care to not consider „SPL“ and „MES“ in the average and to consider that REP has provided
results only for two sectors. Results are shown in Figure 22 (target mast 1) and Figure 23 (target mast
2).
It can be noticed that for target mast 1 and the sector centred at 345 deg, the participants results can e
divided into a centre cluster, close to the mean value of all participants, and one outliner towards large
positive deviations from the mean (RTV) and one outliner towards large negative deviations (GEO). The
situation is similar for 330 deg and also 315 deg, although at 315 deg UNK separates from the centre
cluster towards positive deviations from the mean.
Overall, RTV provides for most sectors the highest positive deviation from all participants.
The situation is different at target mast 2. RTV does not in all cases provide the highest positive
deviation, but especially for 285 deg to 330 deg, participant UNK delivers higher positive deviations.
UNK remains in the centre cluster of the participants for the wind direction range 180 deg to 240 deg
but with further increasing wind direction UNK moves towards higher positive deviations, leaving
behind RTV at 285 deg to 330 deg.
At 330 deg there appears to be an obvious discrepancy between predictions by LAM and GEO. For 15
deg there is peak-behaviour for MET and UNK.
As a result of the evaluation of the sector-wise deviations from the sector-wise mean of all participants,
one can state that there is considerable variation of these quantities from sector to sector, which would
complicate the definition of a Round Robin „passed“ criterion similar to MEASNET anemometer
calibration round robins. Also, outliners and peak behaviour weaken the meaning of a mean value
calculated from the participants results. And lastly, the models under consideration in this test are
inhomogeneous regarding their general approach and it may be necessary to average their results
within distinct groups.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 55 / 173
6.7.3 Mean Absolute Values of Sector-wise Errors
As shown in the measurement data evaluation in the appendix, the relationship between the reference
mast and the two target masts changes much with direction, especially at target mast 2. There are
different demands on the models for different wind directions. If in each sector the absolute value of
the error in mean wind speed is considered and averaged over all wind directions, one yields an
average mean absolute wind speed error that is based on a larger, dispersed data set than the wind
speed error gained from all wind directions simultaneously. Therefore, we consider that the results
presented in Figure 24 provide the best condensed overview of the model performance regarding mean
wind speed for this site. Whether or not there is systematical bias in the predictions will be investigated
in more detail in the next chapter.
By chance, MET shows the same mean error for both target masts (11.1%). Also RTV and UNK show
similar magnitudes of the error for both masts. For the other participants, there are larger differences
in the errors regarding the two masts.
ANM shows the smallest error for target mast 1 from all participants but the largest from all for target
mast 2. That ANM shows the smallest error for target mast 1 confirms our qualitative statement that
ANM provides the best approximation of the overall shape of the direction dependent speed-up
function for target mast 1.
The same is true for LAM regarding target mast 2. LAM provided a good approximation of the sector-
wise speed-up values and, accordingly, shows the smallest error for target mast 2. However, at target
mast 2, LAM does not perform that much better than the others as it is observed for ANM at target
mast 2.
Surprisingly, RTV mixes well among the other participants, although it was shown in section 6.7.1 that
RTV does hardly predict any change of the speed-up factors with wind direction. This is an indication
that the other models may partly introduce flow details and complexity that is not present in reality.
It must be noted that these evaluation regarding mean wind speed have no direct meaning for energy
yield prognosis, where accuracy in higher moments of wind speed is more important due to the power
performance behaviour of the wind turbines. But in terms of site assessment according to IEC wind
turbine classes, accurate calculation of mean wind speed is very important.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 56 / 173
6.7.4 Overall Direction Independent Wind Speed Prediction Error
As detailed in the previous section, a sector-wise evaluation provides a broader base for quantitative
conclusions about overall model performance for this site, except for participant ANM, as detailed in
section 6.4. For ANM, the sector-wise evaluation may lead to wrong conclusions about site specific
model performance.
In this section, the mean wind speed that the participants calculated for the target masts, is evaluated
independent of direction from the statistics (TAB) that contain all sectors with the exception of the
disturbed ones. This evaluation relates to the percentage error in mean wind speed and not to its
absolute value and therefore provides information about any bias present in the participants results.
Figure 25 provides on overview of the wind speed errors of the different models.
All participants, except RTV underestimate mean wind speed for both masts. RTV as the only
participant overestimates mean wind speed at both masts.
As in the sector-wise evaluation, RTV and MET have similar errors for both masts, in the present
analysis this is additionally true for REP.
ANM confirms its comparably small error for target mast 1, the same is true for LAM in the case of
target mast 2.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 57 / 173
0
1
2
3
4
5
6
7
8
0 30 60 90 120 150 180 210 240 270 300 330 360
Mea
n W
ind S
pee
d [
m/s
]
Wind Direction Sector Centre [deg]
Target Point 1 - Mean Wind Speed
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNK
ANM GEO LAM MES MET REP RTV SPL UNJ UNK
0 3.9 2.6 4.0 3.4 3.3 - 3.9 3.0 - 3.1
15 4.5 3.1 4.6 4.2 6.0 - 4.6 3.5 - 3.6
30 5.3 4.9 5.5 5.8 6.0 - 6.3 4.9 - 5.1
45 4.6 4.1 4.7 4.8 4.8 - 5.4 4.2 - 4.2
60 5.0 5.0 4.0 4.7 4.9 - 5.5 4.2 - 4.3
75 5.2 5.5 4.8 5.0 5.6 - 6.3 4.9 - 5.0
180 7.7 6.8 6.9 7.8 6.9 6.4 7.8 6.0 - 6.4
195 6.8 6.1 6.0 6.7 5.8 - 7.0 5.4 - 5.5
210 7.1 6.3 5.9 7.1 6.0 - 7.3 5.6 - 5.8
225 7.2 7.0 5.9 7.4 5.9 - 7.7 5.9 - 6.4
240 6.2 5.4 4.3 6.0 4.7 - 6.2 4.7 - 5.2
255 6.0 5.7 5.4 6.2 5.6 - 6.4 4.9 - 5.7
270 5.9 5.7 5.0 6.2 5.6 5.4 6.6 5.0 - 6.1
285 6.4 5.5 5.6 6.9 6.5 - 7.3 5.7 - 7.0
300 6.0 4.9 5.6 6.1 5.6 - 6.8 5.3 - 6.5
315 5.6 4.6 5.5 6.0 5.4 - 6.3 4.9 - 5.9
330 5.1 3.8 5.0 5.7 5.4 - 6.1 4.8 - 5.5
345 4.3 3.1 4.1 4.2 4.3 - 4.8 3.8 - 4.1
Figure 16
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 58 / 173
0
1
2
3
4
5
6
7
8
0 30 60 90 120 150 180 210 240 270 300 330 360
Mea
n W
ind S
pee
d [
m/s
]
Wind Direction Sector Centre [deg]
Target Point 2 - Mean Wind Speed
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNK
ANM GEO LAM MES MET REP RTV SPL UNJ UNK
0 3.5 3.5 4.2 4.0 3.1 - 3.9 3.0 - 3.4
15 4.2 4.1 4.5 4.8 5.7 - 4.6 3.5 - 5.4
30 5.1 5.9 6.0 6.5 5.2 - 6.2 4.9 - 5.4
45 4.5 5.0 5.5 5.7 4.2 - 5.3 4.2 - 4.5
60 4.9 5.5 4.9 5.6 4.2 - 5.4 4.2 - 4.7
75 5.1 6.2 5.4 6.0 5.7 - 6.2 4.9 - 5.6
180 6.6 6.9 6.7 6.8 6.6 6.2 7.7 6.0 - 6.7
195 5.8 6.3 6.0 5.7 5.7 - 6.9 5.4 - 5.8
210 6.0 6.5 6.3 6.0 5.9 - 7.2 5.6 - 6.0
225 6.1 7.3 6.4 6.4 6.3 - 7.6 5.9 - 6.5
240 5.2 5.5 5.2 5.4 5.3 - 6.0 4.7 - 5.4
255 5.1 5.7 5.9 5.7 5.9 - 6.3 4.9 - 5.9
270 5.1 5.7 6.0 5.9 5.6 5.7 6.5 5.0 - 6.4
285 5.6 6.4 6.1 6.8 6.3 - 7.3 5.7 - 7.5
300 5.3 6.0 6.2 6.5 6.0 - 6.8 5.3 - 7.0
315 4.9 5.7 5.8 6.4 5.4 - 6.3 4.9 - 6.5
330 4.5 4.7 5.9 6.2 5.1 - 6.1 4.8 - 6.2
345 3.8 4.3 4.4 4.9 4.0 - 4.8 3.8 - 4.6
Figure 17
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 59 / 173
-40
-30
-20
-10
0
10
20
30
40
50
0 30 60 90 120 150 180 210 240 270 300 330 360
Per
centa
ge
Err
or
in M
ean W
ind S
pee
d [
%]
Wind Direction Sector Centre [deg]
Target Point 1 - Percentage Error in Mean Wind Speed
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNK
ANM GEO LAM MES MET REP RTV SPL UNJ UNK
0 15.8 -24.5 16.1 0.0 -4.1 - 15.6 -10.7 - -8.9
15 7.8 -25.7 8.9 0.0 43.4 - 9.4 -15.3 - -13.9
30 -7.7 -15.6 -5.2 0.0 3.8 - 9.4 -15.8 - -12.5
45 -4.0 -13.9 -0.7 0.0 -0.2 - 13.0 -13.1 - -12.2
60 7.5 7.3 -14.6 0.0 5.3 - 18.0 -9.5 - -7.5
75 2.9 9.4 -5.1 0.0 11.1 - 25.6 -3.7 - -0.4
180 -0.4 -11.7 -10.8 0.0 -10.8 -17.9 0.8 -22.2 - -17.6
195 1.2 -8.8 -10.3 0.0 -13.2 - 3.4 -19.8 - -17.7
210 0.1 -10.3 -16.3 0.0 -15.2 - 3.3 -20.6 - -17.6
225 -2.3 -5.3 -19.9 0.0 -20.1 - 5.0 -19.7 - -13.8
240 2.1 -11.0 -28.1 0.0 -22.4 - 2.3 -21.6 - -13.6
255 -3.2 -7.2 -12.9 0.0 -9.8 - 4.4 -20.2 - -7.3
270 -4.8 -8.0 -19.3 0.0 -9.9 -12.6 6.4 -18.6 - -1.7
285 -7.0 -19.8 -19.3 0.0 -6.4 - 6.0 -18.1 - 1.7
300 -1.0 -19.5 -8.4 0.0 -8.1 - 12.4 -12.8 - 6.5
315 -6.2 -23.4 -7.4 0.0 -10.4 - 5.6 -17.3 - -1.7
330 -9.1 -32.3 -11.1 0.0 -4.7 - 8.7 -14.6 - -2.2
345 3.5 -25.3 -1.7 0.0 1.3 - 15.2 -10.5 - -2.8
Figure 18
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 60 / 173
-30
-20
-10
0
10
20
30
0 30 60 90 120 150 180 210 240 270 300 330 360
Per
centa
ge
Err
or
in M
ean W
ind S
pee
d [
%]
Wind Direction Sector Centre [deg]
Target Point 2 - Percentage Error in Mean Wind Speed
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNK
ANM GEO LAM MES MET REP RTV SPL UNJ UNK
0 -11.6 -10.9 5.2 0.0 -22.5 - -1.3 -23.4 - -13.9
15 -13.2 -14.3 -5.9 0.0 17.9 - -5.2 -26.3 - 13.1
30 -22.4 -9.2 -8.4 0.0 -19.7 - -4.5 -25.4 - -16.5
45 -20.4 -12.0 -2.8 0.0 -26.8 - -6.9 -27.0 - -20.8
60 -12.2 -2.3 -12.7 0.0 -25.7 - -3.3 -24.4 - -16.4
75 -15.2 3.6 -10.0 0.0 -4.3 - 4.0 -18.7 - -6.6
180 -2.9 1.9 -1.7 0.0 -3.0 -8.9 14.1 -11.0 - -1.5
195 1.5 10.1 5.6 0.0 0.8 - 21.2 -5.2 - 1.0
210 0.0 8.1 5.0 0.0 -1.2 - 20.4 -6.1 - 0.1
225 -4.8 12.9 -0.7 0.0 -2.1 - 17.7 -8.0 - 1.0
240 -2.9 1.8 -3.7 0.0 -2.2 - 12.0 -12.4 - -0.7
255 -10.9 0.2 4.0 0.0 3.9 - 10.9 -13.7 - 4.3
270 -13.5 -4.1 1.5 0.0 -4.5 -2.8 10.8 -14.5 - 8.6
285 -17.3 -6.9 -11.4 0.0 -7.8 - 7.1 -17.2 - 9.8
300 -18.6 -7.9 -5.0 0.0 -7.5 - 5.5 -18.2 - 8.7
315 -23.1 -11.0 -8.3 0.0 -14.3 - -0.6 -22.2 - 2.9
330 -26.8 -24.1 -4.4 0.0 -17.2 - -1.0 -22.3 - 0.1
345 -22.0 -11.1 -9.2 0.0 -17.8 - -0.9 -23.0 - -6.5
Figure 19
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 61 / 173
0.7
0.8
0.9
1
1.1
1.2
1.3
1.4
1.5
1.6
1.7
0 30 60 90 120 150 180 210 240 270 300 330 360
v (
Tar
get
Mas
t 1
) /
v (
Ref
eren
ce M
ast)
[-]
Wind Direction Sector Centre [deg]
Speedup Factor at Target Mast 1Participant ANM
ANMMeasured
0.7
0.8
0.9
1
1.1
1.2
1.3
1.4
1.5
1.6
1.7
0 30 60 90 120 150 180 210 240 270 300 330 360v
(T
arg
et M
ast
1)
/ v
(R
efer
ence
Mas
t) [
-]Wind Direction Sector Centre [deg]
Speedup Factor at Target Mast 1Participant GEO
GEOMeasured
0.7
0.8
0.9
1
1.1
1.2
1.3
1.4
1.5
1.6
1.7
0 30 60 90 120 150 180 210 240 270 300 330 360
v (
Tar
get
Mas
t 1
) /
v (
Ref
eren
ce M
ast)
[-]
Wind Direction Sector Centre [deg]
Speedup Factor at Target Mast 1Participant LAM
LAMMeasured
0.7
0.8
0.9
1
1.1
1.2
1.3
1.4
1.5
1.6
1.7
0 30 60 90 120 150 180 210 240 270 300 330 360
v (
Tar
get
Mas
t 1)
/ v (
Ref
eren
ce M
ast)
[-]
Wind Direction Sector Centre [deg]
Speedup Factor at Target Mast 1Participant MET
METMeasured
0.7
0.8
0.9
1
1.1
1.2
1.3
1.4
1.5
1.6
1.7
0 30 60 90 120 150 180 210 240 270 300 330 360
v (
Tar
get
Mas
t 1
) /
v (
Ref
eren
ce M
ast)
[-]
Wind Direction Sector Centre [deg]
Speedup Factor at Target Mast 1Participant RTV
RTVMeasured
0.7
0.8
0.9
1
1.1
1.2
1.3
1.4
1.5
1.6
1.7
0 30 60 90 120 150 180 210 240 270 300 330 360
v (
Tar
get
Mas
t 1
) /
v (
Ref
eren
ce M
ast)
[-]
Wind Direction Sector Centre [deg]
Speedup Factor at Target Mast 1Participant UNK
UNKMeasured
Figure 20: Speed-up Factors for Target Mast 1 versus Reference Mast.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 62 / 173
0.7
0.8
0.9
1
1.1
1.2
1.3
1.4
1.5
1.6
1.7
0 30 60 90 120 150 180 210 240 270 300 330 360
v (
Tar
get
Mas
t 2)
/ v (
Ref
eren
ce M
ast)
[-]
Wind Direction Sector Centre [deg]
Speedup Factor at Target Mast 2Participant ANM
ANMMeasured
0.7
0.8
0.9
1
1.1
1.2
1.3
1.4
1.5
1.6
1.7
0 30 60 90 120 150 180 210 240 270 300 330 360v (
Tar
get
Mas
t 2)
/ v (
Ref
eren
ce M
ast)
[-]
Wind Direction Sector Centre [deg]
Speedup Factor at Target Mast 2Participant GEO
GEOMeasured
0.7
0.8
0.9
1
1.1
1.2
1.3
1.4
1.5
1.6
1.7
0 30 60 90 120 150 180 210 240 270 300 330 360
v (
Tar
get
Mas
t 2
) /
v (
Ref
eren
ce M
ast)
[-]
Wind Direction Sector Centre [deg]
Speedup Factor at Target Mast 2Participant LAM
LAMMeasured
0.7
0.8
0.9
1
1.1
1.2
1.3
1.4
1.5
1.6
1.7
0 30 60 90 120 150 180 210 240 270 300 330 360
v (
Tar
get
Mas
t 2
) /
v (
Ref
eren
ce M
ast)
[-]
Wind Direction Sector Centre [deg]
Speedup Factor at Target Mast 2Participant MET
METMeasured
0.7
0.8
0.9
1
1.1
1.2
1.3
1.4
1.5
1.6
1.7
0 30 60 90 120 150 180 210 240 270 300 330 360
v (
Tar
get
Mas
t 2
) /
v (
Ref
eren
ce M
ast)
[-]
Wind Direction Sector Centre [deg]
Speedup Factor at Target Mast 2Participant RTV
RTVMeasured
0.7
0.8
0.9
1
1.1
1.2
1.3
1.4
1.5
1.6
1.7
0 30 60 90 120 150 180 210 240 270 300 330 360
v (
Tar
get
Mas
t 2
) /
v (
Ref
eren
ce M
ast)
[-]
Wind Direction Sector Centre [deg]
Speedup Factor at Target Mast 2Participant UNK
UNKMeasured
Figure 21: Speed-up Factors for Target Mast 2 versus Reference Mast.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 63 / 173
-30
-20
-10
0
10
20
30
40
50
0 30 60 90 120 150 180 210 240 270 300 330 360Dev
iati
on f
rom
all
Par
tici
pan
ts M
ean W
ind S
pee
d [
%]
Wind Direction Sector Centre [deg]
Target Point 1 - Deviation from all Participants Mean Wind Speed
ANM
GEO
LAM
MET
REP
RTV
UNK
ANM GEO LAM MES MET REP RTV SPL UNJ UNK
0 13.9 -25.8 14.2 0.0 -5.7 - 13.7 -12.2 - -10.4
15 2.7 -29.3 3.8 0.0 36.6 - 4.3 -19.4 - -18.0
30 -3.2 -11.5 -0.6 0.0 8.8 - 14.7 -11.7 - -8.2
45 -1.0 -11.2 2.3 0.0 2.9 - 16.5 -10.4 - -9.5
60 4.7 4.5 -16.8 0.0 2.6 - 14.9 -11.9 - -9.9
75 -4.1 2.0 -11.5 0.0 3.6 - 17.1 -10.2 - -7.1
180 10.3 -2.1 -1.2 0.0 -1.1 -9.0 11.7 -13.8 - -8.6
195 9.4 -1.3 -3.0 0.0 -6.0 - 11.9 -13.2 - -11.0
210 10.4 -1.1 -7.7 0.0 -6.5 - 13.9 -12.4 - -9.1
225 7.9 4.5 -11.6 0.0 -11.8 - 15.8 -11.4 - -4.8
240 15.7 0.9 -18.6 0.0 -12.0 - 16.0 -11.1 - -2.1
255 3.0 -1.3 -7.3 0.0 -4.1 - 11.1 -15.0 - -1.3
270 2.5 -0.9 -13.1 0.0 -3.0 -5.9 14.6 -12.4 - 5.8
285 0.6 -13.3 -12.8 0.0 1.1 - 14.5 -11.5 - 9.9
300 2.0 -17.0 -5.6 0.0 -5.3 - 15.9 -10.1 - 9.8
315 1.2 -17.4 -0.2 0.0 -3.4 - 13.9 -10.9 - 6.0
330 -0.8 -26.1 -2.8 0.0 4.1 - 18.7 -6.8 - 6.9
345 5.2 -24.1 -0.1 0.0 2.9 - 17.2 -9.0 - -1.2
Figure 22
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 64 / 173
-30
-20
-10
0
10
20
30
0 30 60 90 120 150 180 210 240 270 300 330 360Dev
iati
on f
rom
all
Par
tici
pan
ts M
ean W
ind S
pee
d [
%]
Wind Direction Sector Centre [deg]
Target Point 2 - Deviation from all Participants Mean Wind Speed
ANM
GEO
LAM
MET
REP
RTV
UNK
ANM GEO LAM MES MET REP RTV SPL UNJ UNK
0 -2.7 -1.9 15.8 0.0 -14.7 - 8.7 -15.6 - -5.2
15 -12.1 -13.2 -4.7 0.0 19.4 - -4.0 -25.4 - 14.6
30 -10.4 4.9 5.8 0.0 -7.2 - 10.4 -13.8 - -3.5
45 -6.4 3.5 14.3 0.0 -14.0 - 9.4 -14.2 - -6.8
60 -0.1 11.2 -0.6 0.0 -15.5 - 10.0 -14.0 - -4.9
75 -11.0 8.8 -5.5 0.0 0.5 - 9.2 -14.6 - -2.0
180 -2.6 2.2 -1.4 0.0 -2.7 -8.6 14.4 -10.7 - -1.2
195 -4.9 3.2 -1.0 0.0 -5.5 - 13.6 -11.1 - -5.4
210 -5.1 2.6 -0.4 0.0 -6.3 - 14.3 -10.9 - -5.1
225 -8.5 8.6 -4.6 0.0 -5.8 - 13.2 -11.6 - -2.9
240 -3.6 1.1 -4.4 0.0 -2.9 - 11.3 -13.0 - -1.4
255 -12.7 -1.8 1.9 0.0 1.8 - 8.6 -15.4 - 2.2
270 -13.0 -3.6 2.0 0.0 -3.9 -2.2 11.4 -14.0 - 9.2
285 -13.5 -2.6 -7.3 0.0 -3.6 - 12.1 -13.4 - 14.8
300 -15.1 -3.9 -0.9 0.0 -3.5 - 10.1 -14.7 - 13.4
315 -15.4 -2.2 0.9 0.0 -5.8 - 9.3 -14.4 - 13.1
330 -16.6 -13.5 9.0 0.0 -5.7 - 12.7 -11.5 - 14.0
345 -12.1 0.2 2.3 0.0 -7.4 - 11.7 -13.3 - 5.4
Figure 23
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 65 / 173
0
5
10
15
20
0 5 10 15 20
Mea
n A
bso
lute
Err
or
in
Mea
n S
ecto
rwis
e W
ind S
pee
d
at
Tar
get
Mas
t 2 [
%]
Mean Absolute Error in Mean Sectorwise Wind Speed
at Target Mast 1 [%]
4.8,13.3 ANM
ANM
15.5,8.5 GEO
GEO
12.0,5.9 LAM
LAM
0.0,0.0 MES
MES
11.1,11.1 MET
MET
9.1,8.2 RTV
RTV
15.8,17.7 SPL
SPL
8.9,7.3 UNK
UNK
Figure 24
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 66 / 173
-20
-15
-10
-5
0
5
10
15
20
-20 -15 -10 -5 0 5 10 15 20
Err
or
in M
ean W
ind S
pee
d
at
Tar
get
Mas
t 2 [
%]
Error in Mean Wind Speed at Target Mast 1 [%]
-1.0,-11.2 ANM
ANM
-11.9,-1.9 GEO
GEO
-11.8,-2.7 LAM
LAM
0.0,0.0 MES
MES
-6.9,-6.5 MET
MET-13.3,-12.7 REP
REP
+7.2,+8.3 RTV
RTV
-17.4,-15.7 SPLSPL
-5.2,-4.9 UNJ
UNJ
-9.1,-1.6 UNK
UNK
Figure 25
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 67 / 173
6.8 Evaluations Regarding Mean Squared Wind Speed
While the assessment regarding mean wind speed is important especially for IEC wind turbine class
assessment and the assessment regarding mean cubed wind speed represents model performance
regarding calculation of the energy content of the wind, the importance of an assessment regarding
mean squared wind speed is not obvious.
However, if one aims at checking the model errors regarding power production of wind turbines, the
error in the mean squared wind speed provides a fairly good measure for that. It is in particular more
suitable than the evaluations regarding mean or mean cubed wind speed. On the one hand, errors in
mean wind speed will lead to much higher errors in power production. On the other hand, using the
measure that is in proportion to the energy content, mean cubed wind speed, one yields errors that are
in general too large because turbines can only extract part of the wind energy and because there is no
sensitivity of the power output on the wind speed if the turbine operates well at rated power.
As a result, the errors in mean squared wind speed, in particular the sector-wise evaluations, are of
central importance in the round robin test. Figure 26 to Figure 31 provide an overview of the sector-
wise results, similar to the evaluations regarding mean wind speed in the previous chapter. Compared
to that evaluation, the relative errors are larger but besides that the overall comparison of the single
sector results between the models leads to the same results. Therefore Figure 26 to Figure 31 are only
reported for reference.
The main result of the mean squared wind speed evaluation is shown in Figure 32 (mean sector-wise
error) and Figure 33 (mean absolute value of sector-wise error).
There is hardly any difference between model results of RTV and MET regarding the mean absolute
error in squared wind speed, whereas for the mean absolute error in mean wind speed, RTV performed
significantly better than MET.
ANM showed significantly lower errors regarding mean wind speed (sector-wise absolute values) than
any other model (at target mast 1).
Regarding mean absolute values of errors in squared wind speed, ANM shares the lowest errors with
UNK for target mast 1, which means that the accuracy of the UNK results is higher for squared wind
speed than for wind speed. In general, the differences between the mean and mean squared evaluation
are more pronounced in the case of target mast 1.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 68 / 173
The overall picture regarding systematical bias (Figure 32) changes only little compared to the same
evaluation regarding mean wind speed. While all models except RTV underestimated mean wind speed
for both target masts, GEO and UNK slightly overestimate mean squared wind speed at target mast 2
and ANM slightly overestimates mean squared wind speed at target mast 1.
REP provides the most conservative results regarding mean squared wind speed for both target masts,
although ANM and LAM provide almost as conservative results for target mast 1 and 2 respectively.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 69 / 173
0
10
20
30
40
50
60
70
80
90
100
0 30 60 90 120 150 180 210 240 270 300 330 360
Mea
n S
quar
ed W
ind S
pee
d [
m2/s
2]
Wind Direction Sector Centre [deg]
Target Point 1 - Mean Squared Wind Speed
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNK
ANM GEO LAM MES MET REP RTV SPL UNJ UNK
0 21.8 8.7 18.3 14.4 13.2 - 19.1 11.3 - 12.5
15 28.4 13.2 25.2 22.5 45.4 - 26.5 15.8 - 17.4
30 37.8 34.2 38.8 44.9 49.0 - 54.0 31.8 - 36.5
45 30.8 24.9 30.3 30.5 31.4 - 39.7 23.3 - 25.5
60 40.1 36.0 22.7 29.5 34.8 - 43.4 25.3 - 28.0
75 43.6 41.3 31.3 35.3 43.5 - 55.0 32.2 - 35.5
180 85.5 58.0 57.0 75.3 58.8 49.9 74.9 44.4 - 51.0
195 67.2 48.9 45.9 58.7 44.7 - 62.9 37.7 - 41.2
210 68.7 52.0 44.5 63.7 47.1 - 69.3 40.8 - 45.8
225 67.3 64.4 44.5 68.3 45.4 - 77.5 45.2 - 54.3
240 49.4 37.4 24.4 44.3 28.9 - 49.5 28.9 - 37.4
255 46.3 43.3 35.9 46.4 40.5 - 53.7 31.4 - 45.0
270 42.7 40.4 31.6 45.6 39.2 36.8 54.1 31.5 - 48.7
285 49.0 40.1 38.0 55.8 51.6 - 65.8 39.1 - 63.3
300 44.4 31.8 37.5 44.5 39.4 - 58.7 35.0 - 55.1
315 40.1 28.8 37.8 45.3 37.2 - 51.2 31.3 - 46.4
330 34.2 20.1 31.9 42.0 38.5 - 49.5 30.5 - 42.3
345 26.0 13.8 21.5 23.9 24.5 - 31.3 18.8 - 23.9
Figure 26
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 70 / 173
0
10
20
30
40
50
60
70
80
90
100
0 30 60 90 120 150 180 210 240 270 300 330 360
Mea
n S
quar
ed W
ind S
pee
d [
m2/s
2]
Wind Direction Sector Centre [deg]
Target Point 2 - Mean Squared Wind Speed
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNK
ANM GEO LAM MES MET REP RTV SPL UNJ UNK
0 16.9 14.9 20.4 19.0 11.7 - 18.8 11.3 - 15.3
15 23.9 21.3 24.7 28.8 40.5 - 26.2 15.8 - 42.4
30 32.7 48.9 45.4 55.4 37.3 - 52.3 31.8 - 42.4
45 28.1 35.0 40.3 41.5 24.1 - 38.2 23.3 - 29.5
60 35.4 44.3 33.6 42.5 25.1 - 41.7 25.3 - 33.1
75 36.9 55.2 39.4 47.5 45.9 - 52.9 32.2 - 44.1
180 59.2 59.7 53.1 56.6 53.1 46.7 73.1 44.4 - 55.1
195 46.5 51.9 45.5 42.8 43.0 - 61.8 37.7 - 43.8
210 48.1 55.3 49.7 47.7 45.7 - 67.3 40.8 - 47.9
225 48.1 70.9 51.9 53.7 51.8 - 74.1 45.2 - 56.4
240 35.5 39.7 34.0 36.8 36.5 - 47.6 28.9 - 39.3
255 33.4 43.1 43.9 41.5 45.9 - 51.7 31.4 - 48.1
270 31.9 39.6 44.1 42.6 39.9 41.2 53.4 31.5 - 53.2
285 37.6 49.6 45.0 56.4 49.0 - 65.8 39.1 - 71.4
300 34.1 44.3 46.4 51.5 45.3 - 58.7 35.0 - 64.7
315 30.2 41.2 42.4 49.1 38.4 - 51.2 31.3 - 57.2
330 26.5 31.2 44.5 47.4 34.9 - 49.5 30.5 - 53.3
345 19.9 24.8 25.9 30.4 21.8 - 31.3 18.8 - 30.0
Figure 27
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 71 / 173
-60
-40
-20
0
20
40
60
80
100
0 30 60 90 120 150 180 210 240 270 300 330 360
Per
centa
ge
Err
or
in M
ean S
quar
ed W
ind S
pee
d [
%]
Wind Direction Sector Centre [deg]
Target Point 1 - Percentage Error in Mean Squared Wind Speed
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNK
ANM GEO LAM MES MET REP RTV SPL UNJ UNK
0 51.0 -39.8 27.2 0.0 -8.2 - 32.4 -21.5 - -13.0
15 26.1 -41.5 12.1 0.0 101.7 - 17.8 -29.9 - -22.7
30 -15.8 -23.8 -13.4 0.0 9.2 - 20.3 -29.1 - -18.8
45 0.9 -18.2 -0.6 0.0 3.0 - 30.4 -23.7 - -16.2
60 35.9 22.0 -23.1 0.0 17.8 - 47.0 -14.3 - -5.4
75 23.2 16.9 -11.6 0.0 23.1 - 55.6 -8.9 - 0.3
180 13.6 -22.9 -24.2 0.0 -21.9 -33.7 -0.5 -41.0 - -32.2
195 14.4 -16.7 -21.9 0.0 -23.9 - 7.1 -35.9 - -29.8
210 7.9 -18.4 -30.2 0.0 -26.0 - 8.8 -36.0 - -28.0
225 -1.5 -5.8 -34.9 0.0 -33.5 - 13.4 -33.9 - -20.6
240 11.7 -15.5 -44.9 0.0 -34.7 - 11.9 -34.7 - -15.5
255 -0.4 -6.7 -22.7 0.0 -12.8 - 15.7 -32.3 - -3.0
270 -6.4 -11.4 -30.8 0.0 -14.1 -19.4 18.7 -31.0 - 6.8
285 -12.1 -28.1 -31.9 0.0 -7.5 - 18.1 -29.9 - 13.5
300 -0.3 -28.5 -15.7 0.0 -11.5 - 31.8 -21.3 - 23.8
315 -11.4 -36.4 -16.5 0.0 -17.9 - 13.0 -30.9 - 2.4
330 -18.5 -52.3 -24.0 0.0 -8.3 - 17.9 -27.5 - 0.6
345 8.6 -42.2 -10.3 0.0 2.3 - 30.8 -21.5 - 0.0
Figure 28
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 72 / 173
-60
-40
-20
0
20
40
60
0 30 60 90 120 150 180 210 240 270 300 330 360
Per
centa
ge
Err
or
in M
ean S
quar
ed W
ind S
pee
d [
%]
Wind Direction Sector Centre [deg]
Target Point 2 - Percentage Error in Mean Squared Wind Speed
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNK
ANM GEO LAM MES MET REP RTV SPL UNJ UNK
0 -10.6 -21.3 7.8 0.0 -38.2 - -0.7 -40.3 - -19.5
15 -17.2 -26.0 -14.2 0.0 40.4 - -9.2 -45.3 - 47.0
30 -41.1 -11.8 -18.1 0.0 -32.7 - -5.7 -42.6 - -23.6
45 -32.3 -15.5 -2.9 0.0 -41.9 - -7.9 -43.9 - -28.8
60 -16.7 4.5 -20.8 0.0 -40.9 - -1.7 -40.4 - -22.1
75 -22.3 16.3 -17.1 0.0 -3.4 - 11.5 -32.1 - -7.1
180 4.6 5.4 -6.1 0.0 -6.1 -17.5 29.2 -21.5 - -2.7
195 8.6 21.2 6.3 0.0 0.5 - 44.3 -12.0 - 2.3
210 0.9 16.0 4.1 0.0 -4.3 - 41.1 -14.6 - 0.3
225 -10.4 32.0 -3.3 0.0 -3.5 - 38.0 -15.8 - 5.1
240 -3.6 7.8 -7.6 0.0 -0.8 - 29.3 -21.5 - 6.6
255 -19.4 4.0 5.9 0.0 10.7 - 24.8 -24.2 - 16.0
270 -25.2 -7.1 3.3 0.0 -6.3 -3.4 25.2 -26.2 - 24.8
285 -33.3 -12.1 -20.3 0.0 -13.1 - 16.7 -30.7 - 26.5
300 -33.8 -13.9 -9.9 0.0 -12.0 - 14.1 -31.9 - 25.7
315 -38.6 -16.1 -13.7 0.0 -21.8 - 4.2 -36.2 - 16.5
330 -44.2 -34.3 -6.2 0.0 -26.3 - 4.4 -35.7 - 12.4
345 -34.4 -18.3 -14.8 0.0 -28.2 - 3.1 -38.1 - -1.1
Figure 29
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 73 / 173
-60
-40
-20
0
20
40
60
80
100
0 30 60 90 120 150 180 210 240 270 300 330 360
Dev
iati
on f
rom
all
Par
tici
pan
ts M
ean S
quar
ed W
ind S
pee
d [
%]
Wind Direction Sector Centre [deg]
Target Point 1 - Deviation from all Participants Mean Squared Wind Speed
ANM
GEO
LAM
MET
REP
RTV
UNK
ANM GEO LAM MES MET REP RTV SPL UNJ UNK
0 39.5 -44.4 17.5 0.0 -15.2 - 22.3 -27.5 - -19.7
15 9.1 -49.4 -3.0 0.0 74.5 - 1.9 -39.4 - -33.1
30 -9.4 -18.1 -6.9 0.0 17.5 - 29.4 -23.7 - -12.6
45 1.1 -18.1 -0.5 0.0 3.1 - 30.5 -23.6 - -16.1
60 17.4 5.4 -33.5 0.0 1.8 - 27.1 -25.9 - -18.2
75 4.5 -0.9 -25.0 0.0 4.4 - 31.9 -22.7 - -14.9
180 37.5 -6.6 -8.2 0.0 -5.4 -19.8 20.5 -28.6 - -17.9
195 29.7 -5.6 -11.5 0.0 -13.7 - 21.4 -27.3 - -20.4
210 25.9 -4.8 -18.5 0.0 -13.7 - 27.0 -25.3 - -16.0
225 14.3 9.3 -24.5 0.0 -22.8 - 31.5 -23.3 - -7.8
240 30.6 -1.1 -35.6 0.0 -23.7 - 30.9 -23.6 - -1.2
255 4.9 -1.8 -18.7 0.0 -8.2 - 21.8 -28.8 - 2.1
270 1.9 -3.6 -24.7 0.0 -6.6 -12.3 29.1 -24.9 - 16.2
285 -4.4 -21.9 -26.0 0.0 0.5 - 28.4 -23.8 - 23.4
300 -0.2 -28.5 -15.7 0.0 -11.4 - 31.9 -21.3 - 23.9
315 -0.3 -28.5 -6.0 0.0 -7.6 - 27.1 -22.2 - 15.3
330 -5.2 -44.4 -11.5 0.0 6.8 - 37.2 -15.5 - 17.1
345 10.6 -41.1 -8.7 0.0 4.2 - 33.2 -20.1 - 1.9
Figure 30
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 74 / 173
-60
-40
-20
0
20
40
60
0 30 60 90 120 150 180 210 240 270 300 330 360
Dev
iati
on f
rom
all
Par
tici
pan
ts M
ean S
quar
ed W
ind S
pee
d [
%]
Wind Direction Sector Centre [deg]
Target Point 2 - Deviation from all Participants Mean Squared Wind Speed
ANM
GEO
LAM
MET
REP
RTV
UNK
ANM GEO LAM MES MET REP RTV SPL UNJ UNK
0 3.6 -8.7 25.0 0.0 -28.4 - 15.1 -30.7 - -6.7
15 -20.0 -28.5 -17.1 0.0 35.7 - -12.2 -47.1 - 42.1
30 -24.3 13.3 5.2 0.0 -13.5 - 21.1 -26.3 - -1.8
45 -13.6 7.7 23.8 0.0 -26.0 - 17.3 -28.5 - -9.2
60 -0.5 24.8 -5.4 0.0 -29.5 - 17.4 -28.8 - -6.9
75 -19.3 20.7 -13.9 0.0 0.3 - 15.7 -29.5 - -3.5
180 3.6 4.4 -7.0 0.0 -7.0 -18.3 28.0 -22.3 - -3.6
195 -4.6 6.4 -6.7 0.0 -11.7 - 26.7 -22.7 - -10.1
210 -8.0 5.8 -5.1 0.0 -12.7 - 28.6 -22.1 - -8.5
225 -18.3 20.4 -11.8 0.0 -12.0 - 25.9 -23.2 - -4.1
240 -8.5 2.4 -12.2 0.0 -5.7 - 22.8 -25.4 - 1.2
255 -24.7 -2.8 -1.0 0.0 3.5 - 16.7 -29.1 - 8.4
270 -26.4 -8.6 1.7 0.0 -7.8 -4.9 23.2 -27.4 - 22.8
285 -29.1 -6.6 -15.3 0.0 -7.7 - 24.1 -26.3 - 34.5
300 -30.4 -9.4 -5.2 0.0 -7.4 - 20.0 -28.4 - 32.3
315 -30.5 -5.1 -2.4 0.0 -11.6 - 17.9 -27.9 - 31.8
330 -33.8 -22.0 11.3 0.0 -12.6 - 23.9 -23.8 - 33.4
345 -22.3 -3.2 1.0 0.0 -15.0 - 22.2 -26.7 - 17.2
Figure 31
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 75 / 173
-30
-20
-10
0
10
20
30
-30 -20 -10 0 10 20 30
Err
or
in M
ean S
quar
ed W
ind S
pee
d
at
Tar
get
Mas
t 2 [
%]
Error in Mean Squared Wind Speed at Target Mast 1 [%]
+4.9,-17.5 ANM
ANM
-17.9,+0.6 GEO
GEO
-23.2,-6.3 LAM
LAM
0.0,0.0 MES
MES
-12.2,-10.1 MET
MET -23.8,-21.5 REP
REP
+16.4,+20.1 RTV
RTV
-31.3,-27.4 SPLSPL
-9.2,-7.3 UNJ
UNJ
-12.2,+3.3 UNK
UNK
Figure 32
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 76 / 173
0
5
10
15
20
25
30
35
0 5 10 15 20 25 30 35
Mea
n A
bso
lute
Err
or
in
Mea
n S
ecto
rwis
e S
quar
ed W
ind S
pee
d
at
Tar
get
Mas
t 2 [
%]
Mean Absolute Error in Mean Sectorwise Squared Wind Speed
at Target Mast 1 [%]
14.4,22.1 ANM
ANM
24.8,15.8 GEO
GEO
22.0,10.1 LAM
LAM
0.0,0.0 MES
MES
21.0,18.4 MET
MET
21.7,17.3 RTVRTV
28.0,30.7 SPL
SPL
14.0,16.0 UNK
UNK
Figure 33
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 77 / 173
6.9 Evaluations Regarding Mean Cubed Wind Speed
Errors in mean cubed wind speed are in proportion to errors in the energy content of the wind. As
turbines extract only part of that, these errors are much larger than those expected for energy
production of any turbines. The results are therefore reported only for reference (Figure 34 to Figure
41).
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 78 / 173
0
100
200
300
400
500
600
700
800
900
1000
1100
1200
1300
0 30 60 90 120 150 180 210 240 270 300 330 360
Mea
n C
ubed
Win
d S
pee
d [
m3/s
3]
Wind Direction Sector Centre [deg]
Target Point 1 - Mean Cubed Wind Speed
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNK
ANM GEO LAM MES MET REP RTV SPL UNJ UNK
0 154.6 35.8 96.7 74.9 64.3 - 109.8 50.0 - 62.4
15 218.4 69.3 160.3 147.3 411.6 - 182.8 83.4 - 102.8
30 307.8 296.7 324.2 418.5 485.2 - 555.1 250.8 - 320.8
45 269.5 198.1 236.2 240.8 258.9 - 362.1 160.9 - 196.2
60 417.6 332.3 162.4 228.4 308.2 - 427.2 188.8 - 226.6
75 464.3 379.1 248.6 313.7 411.1 - 578.4 258.3 - 301.5
180 1114.0 573.1 533.7 844.9 575.3 449.8 824.3 374.8 - 470.7
195 803.1 473.1 413.0 611.0 412.4 - 683.3 315.0 - 371.7
210 800.9 511.3 396.7 679.5 443.8 - 785.6 352.1 - 434.9
225 719.0 708.2 391.8 733.8 412.8 - 909.6 403.8 - 548.6
240 465.1 321.4 167.5 380.4 216.4 - 477.6 211.9 - 331.4
255 421.1 412.7 286.7 413.0 362.6 - 550.1 245.9 - 449.1
270 350.6 344.4 241.7 386.6 330.0 298.9 530.5 232.4 - 481.3
285 417.1 350.1 302.0 504.0 481.0 - 690.4 312.9 - 680.7
300 370.8 245.6 287.7 368.5 322.1 - 582.8 266.6 - 551.6
315 333.3 220.7 296.2 403.2 303.9 - 486.9 232.5 - 437.4
330 269.1 130.2 237.3 378.3 331.3 - 476.5 230.0 - 392.9
345 195.4 79.9 133.2 174.9 177.5 - 253.1 117.3 - 181.1
Figure 34
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 79 / 173
0
100
200
300
400
500
600
700
800
900
1000
1100
1200
1300
0 30 60 90 120 150 180 210 240 270 300 330 360
Mea
n C
ubed
Win
d S
pee
d [
m3/s
3]
Wind Direction Sector Centre [deg]
Target Point 2 - Mean Cubed Wind Speed
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNK
ANM GEO LAM MES MET REP RTV SPL UNJ UNK
0 103.8 73.4 114.2 106.1 53.2 - 106.8 50.0 - 84.1
15 163.5 134.7 155.6 204.8 344.7 - 178.6 83.4 - 404.2
30 237.3 502.6 406.0 557.4 322.4 - 528.9 250.8 - 404.2
45 216.3 317.0 352.5 358.8 175.1 - 341.7 160.9 - 245.5
60 316.1 462.4 287.0 396.5 189.3 - 401.4 188.8 - 294.9
75 328.1 617.7 350.8 456.3 454.5 - 546.3 258.3 - 424.1
180 615.5 609.0 484.2 542.2 495.5 406.0 795.5 374.8 - 521.0
195 444.7 526.8 410.3 391.4 388.3 - 664.8 315.0 - 400.4
210 460.3 581.9 464.8 465.5 422.9 - 752.4 352.1 - 458.7
225 428.4 828.1 493.0 527.0 500.8 - 850.0 403.8 - 578.1
240 282.0 354.0 265.8 301.5 306.4 - 453.2 211.9 - 352.8
255 257.1 408.6 389.9 368.8 437.9 - 518.9 245.9 - 487.3
270 226.9 333.2 383.2 363.8 339.3 353.0 520.2 232.4 - 539.1
285 278.8 452.8 390.6 544.6 445.7 - 690.4 312.9 - 801.6
300 250.1 383.4 400.6 476.1 396.5 - 582.8 266.6 - 696.8
315 217.9 361.6 357.4 435.4 318.8 - 486.9 232.5 - 597.6
330 183.5 257.4 389.9 421.4 284.7 - 476.5 230.0 - 556.7
345 131.7 180.7 188.9 230.1 149.0 - 253.1 117.3 - 255.4
Figure 35
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 80 / 173
-80
-60
-40
-20
0
20
40
60
80
100
120
140
160
180
200
0 30 60 90 120 150 180 210 240 270 300 330 360
Per
centa
ge
Err
or
in M
ean C
ubed
Win
d S
pee
d [
%]
Wind Direction Sector Centre [deg]
Target Point 1 - Percentage Error in Mean Cubed Wind Speed
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNK
ANM GEO LAM MES MET REP RTV SPL UNJ UNK
0 106.3 -52.2 29.0 0.0 -14.2 - 46.5 -33.3 - -16.7
15 48.3 -53.0 8.8 0.0 179.5 - 24.1 -43.4 - -30.2
30 -26.4 -29.1 -22.5 0.0 15.9 - 32.7 -40.1 - -23.4
45 11.9 -17.7 -1.9 0.0 7.5 - 50.3 -33.2 - -18.5
60 82.8 45.5 -28.9 0.0 34.9 - 87.0 -17.3 - -0.8
75 48.0 20.9 -20.8 0.0 31.1 - 84.4 -17.6 - -3.9
180 31.8 -32.2 -36.8 0.0 -31.9 -46.8 -2.4 -55.6 - -44.3
195 31.4 -22.6 -32.4 0.0 -32.5 - 11.8 -48.4 - -39.2
210 17.9 -24.7 -41.6 0.0 -34.7 - 15.6 -48.2 - -36.0
225 -2.0 -3.5 -46.6 0.0 -43.7 - 24.0 -45.0 - -25.2
240 22.3 -15.5 -56.0 0.0 -43.1 - 25.6 -44.3 - -12.9
255 1.9 -0.1 -30.6 0.0 -12.2 - 33.2 -40.5 - 8.7
270 -9.3 -10.9 -37.5 0.0 -14.6 -22.7 37.2 -39.9 - 24.5
285 -17.2 -30.5 -40.1 0.0 -4.6 - 37.0 -37.9 - 35.1
300 0.6 -33.3 -21.9 0.0 -12.6 - 58.1 -27.7 - 49.7
315 -17.3 -45.3 -26.5 0.0 -24.6 - 20.8 -42.3 - 8.5
330 -28.9 -65.6 -37.3 0.0 -12.4 - 26.0 -39.2 - 3.9
345 11.7 -54.3 -23.9 0.0 1.5 - 44.7 -32.9 - 3.5
Figure 36
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 81 / 173
-60
-40
-20
0
20
40
60
80
100
0 30 60 90 120 150 180 210 240 270 300 330 360
Per
centa
ge
Err
or
in M
ean C
ubed
Win
d S
pee
d [
%]
Wind Direction Sector Centre [deg]
Target Point 2 - Percentage Error in Mean Cubed Wind Speed
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNK
ANM GEO LAM MES MET REP RTV SPL UNJ UNK
0 -2.1 -30.8 7.6 0.0 -49.8 - 0.6 -52.9 - -20.8
15 -20.2 -34.3 -24.0 0.0 68.3 - -12.8 -59.3 - 97.3
30 -57.4 -9.8 -27.2 0.0 -42.2 - -5.1 -55.0 - -27.5
45 -39.7 -11.7 -1.7 0.0 -51.2 - -4.8 -55.1 - -31.6
60 -20.3 16.6 -27.6 0.0 -52.2 - 1.2 -52.4 - -25.6
75 -28.1 35.4 -23.1 0.0 -0.4 - 19.7 -43.4 - -7.1
180 13.5 12.3 -10.7 0.0 -8.6 -25.1 46.7 -30.9 - -3.9
195 13.6 34.6 4.8 0.0 -0.8 - 69.8 -19.5 - 2.3
210 -1.1 25.0 -0.1 0.0 -9.1 - 61.6 -24.3 - -1.5
225 -18.7 57.1 -6.4 0.0 -5.0 - 61.3 -23.4 - 9.7
240 -6.5 17.4 -11.8 0.0 1.6 - 50.3 -29.7 - 17.0
255 -30.3 10.8 5.7 0.0 18.7 - 40.7 -33.3 - 32.1
270 -37.6 -8.4 5.3 0.0 -6.7 -3.0 43.0 -36.1 - 48.2
285 -48.8 -16.9 -28.3 0.0 -18.2 - 26.8 -42.6 - 47.2
300 -47.5 -19.5 -15.9 0.0 -16.7 - 22.4 -44.0 - 46.4
315 -50.0 -17.0 -17.9 0.0 -26.8 - 11.8 -46.6 - 37.2
330 -56.5 -38.9 -7.5 0.0 -32.4 - 13.1 -45.4 - 32.1
345 -42.8 -21.5 -17.9 0.0 -35.2 - 10.0 -49.0 - 11.0
Figure 37
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 82 / 173
-80
-60
-40
-20
0
20
40
60
80
100
120
140
0 30 60 90 120 150 180 210 240 270 300 330 360
Dev
iati
on f
rom
all
Par
tici
pan
ts M
ean C
ubed
Win
d S
pee
d [
%]
Wind Direction Sector Centre [deg]
Target Point 1 - Deviation from all Participants Mean Cubed Wind Speed
ANM
GEO
LAM
MET
REP
RTV
UNK
ANM GEO LAM MES MET REP RTV SPL UNJ UNK
0 77.1 -59.0 10.8 0.0 -26.3 - 25.8 -42.8 - -28.5
15 14.4 -63.7 -16.0 0.0 115.7 - -4.2 -56.3 - -46.1
30 -19.3 -22.3 -15.0 0.0 27.1 - 45.5 -34.3 - -16.0
45 6.3 -21.9 -6.8 0.0 2.1 - 42.8 -36.5 - -22.6
60 33.7 6.4 -48.0 0.0 -1.3 - 36.8 -39.6 - -27.5
75 16.9 -4.5 -37.4 0.0 3.5 - 45.6 -35.0 - -24.1
180 71.7 -11.7 -17.7 0.0 -11.3 -30.7 27.1 -42.2 - -27.4
195 52.7 -10.1 -21.5 0.0 -21.6 - 29.9 -40.1 - -29.4
210 42.4 -9.1 -29.4 0.0 -21.1 - 39.7 -37.4 - -22.6
225 16.9 15.1 -36.3 0.0 -32.9 - 47.9 -34.3 - -10.8
240 41.0 -2.6 -49.2 0.0 -34.4 - 44.8 -35.8 - 0.5
255 1.8 -0.2 -30.7 0.0 -12.4 - 33.0 -40.6 - 8.6
270 -4.8 -6.5 -34.3 0.0 -10.4 -18.8 44.1 -36.9 - 30.7
285 -14.3 -28.1 -38.0 0.0 -1.2 - 41.8 -35.7 - 39.8
300 -5.8 -37.6 -26.9 0.0 -18.1 - 48.1 -32.2 - 40.2
315 -3.8 -36.3 -14.5 0.0 -12.3 - 40.6 -32.9 - 26.3
330 -12.1 -57.5 -22.5 0.0 8.2 - 55.6 -24.9 - 28.3
345 14.9 -53.0 -21.7 0.0 4.4 - 48.9 -31.0 - 6.5
Figure 38
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 83 / 173
-80
-60
-40
-20
0
20
40
60
80
100
0 30 60 90 120 150 180 210 240 270 300 330 360
Dev
iati
on f
rom
all
Par
tici
pan
ts M
ean C
ubed
Win
d S
pee
d [
%]
Wind Direction Sector Centre [deg]
Target Point 2 - Deviation from all Participants Mean Cubed Wind Speed
ANM
GEO
LAM
MET
REP
RTV
UNK
ANM GEO LAM MES MET REP RTV SPL UNJ UNK
0 16.3 -17.7 27.9 0.0 -40.4 - 19.6 -44.0 - -5.8
15 -29.0 -41.5 -32.4 0.0 49.7 - -22.4 -63.8 - 75.6
30 -40.7 25.6 1.4 0.0 -19.4 - 32.1 -37.3 - 1.0
45 -21.3 15.4 28.3 0.0 -36.3 - 24.4 -41.4 - -10.6
60 -2.8 42.2 -11.7 0.0 -41.8 - 23.4 -41.9 - -9.3
75 -27.7 36.2 -22.7 0.0 0.2 - 20.4 -43.0 - -6.5
180 9.7 8.6 -13.7 0.0 -11.7 -27.6 41.8 -33.2 - -7.1
195 -5.9 11.5 -13.2 0.0 -17.8 - 40.7 -33.3 - -15.3
210 -12.1 11.2 -11.2 0.0 -19.2 - 43.7 -32.7 - -12.4
225 -30.1 35.1 -19.6 0.0 -18.3 - 38.6 -34.1 - -5.7
240 -16.0 5.5 -20.8 0.0 -8.7 - 35.0 -36.9 - 5.1
255 -38.3 -1.9 -6.4 0.0 5.1 - 24.5 -41.0 - 17.0
270 -41.1 -13.5 -0.5 0.0 -11.9 -8.3 35.1 -39.6 - 40.0
285 -45.3 -11.2 -23.4 0.0 -12.6 - 35.4 -38.6 - 57.2
300 -44.6 -15.1 -11.3 0.0 -12.2 - 29.0 -41.0 - 54.3
315 -44.1 -7.3 -8.4 0.0 -18.3 - 24.8 -40.4 - 53.2
330 -48.8 -28.1 8.9 0.0 -20.5 - 33.1 -35.8 - 55.4
345 -31.8 -6.4 -2.2 0.0 -22.8 - 31.1 -39.2 - 32.2
Figure 39
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 84 / 173
-40
-30
-20
-10
0
10
20
30
40
-40 -30 -20 -10 0 10 20 30 40
Err
or
in M
ean C
ubed
Win
d S
pee
d
at
Tar
get
Mas
t 2 [
%]
Error in Mean Cubed Wind Speed at Target Mast 1 [%]
+13.3,-23.4 ANM
ANM
-20.8,+7.2 GEO
GEO
-33.5,-10.4 LAM
LAM
0.0,0.0 MES
MES
-16.7,-12.8 MET
MET -32.6,-28.6 REP
REP
+26.9,+34.3 RTV
RTV
-42.7,-37.3 SPLSPL
-12.7,-8.9 UNJ
UNJ
-13.3,+10.6 UNK
UNK
Figure 40
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 85 / 173
0
5
10
15
20
25
30
35
40
45
0 5 10 15 20 25 30 35 40 45
Mea
n A
bso
lute
Err
or
in
Mea
n S
ecto
rwis
e C
ubed
Win
d S
pee
d
at
Tar
get
Mas
t 2 [
%]
Mean Absolute Error in Mean Sectorwise Cubed Wind Speed
at Target Mast 1 [%]
28.7,29.7 ANM
ANM
30.9,23.2 GEO
GEO
30.2,13.5 LAM
LAM
0.0,0.0 MES
MES
30.6,24.7 MET
MET
36.7,27.9 RTV
RTV
38.2,41.3 SPL
SPL
21.4,27.7 UNK
UNK
Figure 41
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 86 / 173
6.10 Evaluations Regarding Wind Direction
Accurate calculation of the wind direction distribution for wind turbine positions is an important part of
any site assessment. Wind farm optimisation (or more specific: the wake effect calculation) depends to
a large part on the wind direction distribution and if the calculated distribution differs from the actually
observed one, the farm efficiency may be affected in a negative way.
For the Round Robin test, wind direction calculations are assessed in two different ways, as for the wind
speed calculations. Firstly, the results that the participants returned to DEWI based on the tab
containing all wind directions except the disturbed ones is compared to the measured ones at the two
target masts and the difference is evaluated in terms of the chi squared measure. Secondly, the results
of the participants regarding the single sector input tabs for 15 degree wind direction sectors are
evaluated, separately for each sector defined at the reference mast, regarding systematical deviations
in mean wind direction.
It must be noted that the following evaluation regarding sector-wise wind direction effects may be
inappropriate regarding the results of participant ANM, due to reasons detailed in section 6.4.
6.10.1 Qualitative Evaluation Regarding Veer Angles
If one considers the average wind direction difference between the reference mast and the two target
masts, resolved by wind direction at the reference mast, one can qualitatively investigate in how far the
participants are able to model systematic wind direction effects. Figure 60 and Figure 61 show the
measured an calculated wind direction differences (veer angles) for target mast 1 and 2 respectively.
Participant GEO does not calculate any change in wind direction at target mast 1 and 2, therefore
showing a flat calculated veer angle of zero for both masts.
Participants RTV calculates a constant veer angle of -15 deg regarding target mast 1 and 2. It is not clear
if this is intended by the participant or simply a technical issue in the calculation of the TAB (shifting by
one sector).
6.10.2 Qualitative Evaluation Regarding Veer Angles: Target Mast 1
The first characteristic feature of the sector-wise veer angles for target mast 1 versus the reference
mast is the clockwise turning of the wind direction at target mast 1 for wind from south-south-west.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 87 / 173
The results of ANM can not by fully evaluated sector-wise, but ANM clearly shows that clockwise
turning, although he slightly overpredicts that.
A slight clockwise turning is also present in the results of LAM, but LAM heavily underpredicts the veer
angle for that direction.
MET completely fails to reproduce the clockwise turning for south-south-west wind.
Results of participant UNK show a clockwise turning quite similar to the measured one, but the
calculated peak of that veer angle is shifted clockwise by about 45 degree (this is the same „shift“ that
is also present in the speed-up factors of UNK).
The second important feature of the veer angle for target mast 1 versus the reference mast is the anti-
clockwise turning of the wind direction for wind from west and north-west.
ANM predicts that, but by far overestimates this effect. LAM predicts, on the contrary, a clockwise
turning for that direction range, while MET falis to calculate this anti-clockwise turning. Participant UNK
predicts some small anti-clockwise turning, but not for wind from west, but only for wind directions
close to north. Also the predicted turning angle is by far to small.
6.10.3 Qualitative Evaluation Regarding Veer Angles: Target Mast 2
The most characteristic feature of the veer angle regarding target mast 2 versus the reference mast is
the clockwise turning for wind from south-west, west and north-west, with the maximum veer angle
located at west. A secondary maximum of the veer angle can be found for wind from north-east.
The overall situation regarding errors in the veer angle at target mast 2 is somewhat better than at
target mast 1. From all participants, participant UNK best predicts the overall shape of the veer angle
function for the south-west, west and north-west sectors, but underestimates the effect and shows an
outliner at 15 deg. That at least one participant is able to reproduce this shape does further support the
meteorological basis of that effect and indicates that it is not a measurement error regarding the
direction. UNK also reproduces the small anti-clockwise turning for north-westerly winds.
For the north-east sector, the veer angle function of UNK shows a peak at 15 degree, i.e. the same
sector where the results of UNK showed a peak in the sector-wise speed-up factors.
Participant MET predicts some systematical change of the veer angle for south-west, west and north-
west but by far underestimates that effect. For north-west wind, MET to some degree reproduces the
small anticlockwise direction turning.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 88 / 173
The general shape of the veer angle function calculated by LAM shows some similarity to the measured
on but for south-west, west and north-west the effect is by far underestimated.
Participant ANM predicts an overall veer angle function for target mast 2 that does only slightly differ
from that at target mast 1. It shows similarity to the measured one, with a tendency towards
overprediction, but as detailed above, sector-wise results of ANM are not fully comparable to the
results of the other participants.
6.10.4 Evaluations Regarding the Overall Wind Direction Distributions
In this section it is assessed in how far the overall measured wind direction distributions at the two
target masts can be reproduced by the participants. For that, the statistics (TABs) are considered that
the participants calculated for the two target masts on base of the wind data from the reference mast
with all wind directions except the disturbed ones. As this evaluation is not done on base of wind
direction sectors defined at the reference mast, according restrictions for sector-wise assessments
regarding participant ANM do not apply.
Figure 42 to Figure 59 show measured and calculated wind direction distributions for the two target
masts and all participants, including the „virtual“ participant SPL, for comparison. SPL represents the
reference mast data.
Figure 62 shows the results regarding the chi-squared measure which is calculated according to
( )( )∑−
=18
2
2
io
i
o
i
c
i
f
ffχ
,
where c
if is the calculated frequency and o
if is the observed frequency in the i-th undisturbed
direction sector.
Regarding the chi-squared evaluation, it turns out that differences between model performances are
much higher for target mast 2 than for target mast 1. At target mast 1 only RTV separates itself from
the other results with a significantly higher chi-squared, while there is hardly any difference in between
the other model results. Participants GEO and RTV both calculated a constant veer angle for both
masts, zero in the case of GEO and -15 in the case of RTV. While GEO well mixes among the other
results regarding chi-squared, the constant angle of -15 deg for RTV is the reason for its comparably
high chi-squared value.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 89 / 173
Regarding the north-east wind direction range and target mast 1, all participants provide reasonable
approximations of the relative frequencies there, except RTV (for the reason see above) and ANM, who
predicts a too small share of data for that wind direction range.
Regarding the south to north-west wind direction range, the results of participant ANM differ from the
others. ANM is the only participant who approximates the relatively small share of data that falls in the
south wind direction range, which is understandable looking at the fact that ANM did provide a
reasonable (although overestimating) approximation for the veer angle function for that wind direction
range, i.e. ANM did predict a clockwise turning for wind from south-south-west.
The situation is different at target mast 2. At this mast the different models clearly perform much
different regarding their wind direction simulation performance.
That the wind direction distribution predicted by UNK fits best to the measured one at target mast 2
can be traced back to the fact that UNK did provide a reasonable approximation of the direction
dependent veer angle function, despite the unrealistic peak at 15 degree. The predicted wind direction
distribution of UNK for target mast 2 confirms the impression from the veer angle function that the
clockwise turning of the wind direction for wind from west is modelled, but underpredicted.
Although also ANM provided some approximation of the sector-wise veer angle function, the wind
direction distribution predicted by ANM for target mast 2 shows a larger deviation from the measured
one for the west sector.
Regarding the wind direction results of LAM for target mast 2 it can be observed that LAM predicts a
significant peak of the wind direction distribution function in the sector centred at 270 deg. The reason
for this peak is that, according to the veer angle function for LAM, there is clockwise turning for wind
directions smaller than 270 deg and anticlockwise turning for wind directions larger than 270 deg, while
there is no turn angle for 270 deg. Such a simulated configuration is typical for flow channelling
phenomena but it is not measured in the present case.
Surprisingly, the wind direction results of GEO mix well among the other methods regarding the chi
squared evaluation, although GEO did not predict any significant change of wind direction. This is an
indication that the other participants might partly introduce artificial flow features not present in reality
and that the assumption of a zero veer angle may produce similar or even better results than a varying
veer angle.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 90 / 173
6.10.5 Assessment of Average Sector-Wise Wind Direction Errors
The situation regarding systematical bias in the sector-wise wind direction prediction can be
investigated on base of the results shown in Figure 67 (mean sector-wise error in wind direction).
Model results separate into three groups: A very small bias is associated with the results of ANM and
UNK while a comparably high anti-clockwise direction bias can be found in the results of RTV, LAM and
GEO. MET shows a small negative bias at target mast 2 but a high anti-clockwise direction bias at target
mast 1.
Regarding the average absolute values of sector-wise wind direction errors (Figure 68), UNK clearly
outperforms the other models at target mast 1, although at target mast 2 MET gives a comparably small
error. The constant offset of -15 deg, applied by RTV, leads to a smaller value of the absolute values of
the sector-wise errors than the application of no direction effect at all (GEO).
6.10.6 Assessment of the Directional Dispersion of the Single Sector Wind Direction Results
The participants were asked to transform to the target masts the data from the reference mast
separately for each 15 degree wind direction sector defined at the reference mast.
In the previous sections the result is assessed with respect to the mean value of the wind direction for
each of the resulting statistics (TABs). In this section, the width of the resulting wind direction
distributions is assessed, i.e. it is checked what wind direction range the resulting statistics cover.
Technically, the discrete wind direction sector probability distribution as provided by the TAB files is
considered. It is assumed that the data is equally distributed with respect to wind direction within each
15 degree wind direction sector (step-function probability). The distribution is centred at the mean
wind direction, such that clockwise turned wind directions (wrt. mean direction) cover the range 0 deg
to 180 deg and anti-clockwise turned wind directions cover the range -180 deg to 0 deg.
Starting at -180 deg, the probability function is numerically integrated until 2.5% of the data is covered.
Similar integration is performed starting at 180 deg in anti-clockwise direction. The wind direction
range, starting at the wind direction of the lower integration end point and ending at the upper
integration end point is considered as the wind direction range in that 95% of the data falls, giving
indication on the spreading of the wind direction distribution function. Clearly, this approach is based
on the assumption that the distribution is unimodal and falls off quickly. This is not the case for
participant ANM.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 91 / 173
Figure 65 and Figure 66 report that range for the measured data and the participating models.
For both masts, the model results can clearly be separated into two groups: All models, except ANM
show small direction spreadings below 30 degree where GEO and RTV show a spreading equal to that of
the measured sector-wise data at the reference mast, reflecting the fact that GEO did not apply any
direction change and RTV did apply a constant change of -15 degree.
That the spreading of ANM is significantly higher than that of the other participants can be traced to
their different treatment of the site-to-site relationships for the sector-wise evaluation in the test (see
section 6.4).
In can be observed that the measured spreading is significantly higher than that predicted by the
participants (except for ANM who predicts a higher spreading). The measured dispersion of the sector-
wise wind direction varies in between 60 deg and 90 deg for target mast 1 and between 55 deg and
208 deg for target mast 2, which is significantly higher than predicted by all participants except ANM. It
should however be noted that the evaluations could only be performed using the whole wind speed
range, although wind vanes tend to show meandering behaviour for low wind speeds, which should be
the main reason for the higher measured spreading. On the other hand, for models that base on the
determination of direction dependent site-to-site transfer functions, the introduction of some wind
direction fluctuation may possibly be worth to consider. In the case of turbine wake modelling the
meandering of the wakes (wind direction fluctuations) at least plays some role.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 92 / 173
5
10
5 10
ANM - Target Point 1Chi Squared=5.43E-006
E
S
W
N
ANM Measured
Figure 42
5
10
5 10
ANM - Target Point 2Chi Squared=1.54E-005
E
S
W
N
ANM Measured
Figure 43
5
10
5 10
GEO - Target Point 1Chi Squared=4.98E-006
E
S
W
N
GEO Measured
Figure 44
5
10
5 10
GEO - Target Point 2Chi Squared=7.90E-006
E
S
W
N
GEO Measured
Figure 45
5
10
5 10
LAM - Target Point 1Chi Squared=6.64E-006
E
S
W
N
LAM Measured
Figure 46
5
10
5 10
LAM - Target Point 2Chi Squared=1.49E-005
E
S
W
N
LAM Measured
Figure 47
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 93 / 173
5
10
5 10
MET - Target Point 1Chi Squared=6.07E-006
E
S
W
N
MET Measured
Figure 48
5
10
5 10
MET - Target Point 2Chi Squared=7.90E-006
E
S
W
N
MET Measured
Figure 49
5
10
5 10
REP - Target Point 1Chi Squared=6.15E-006
E
S
W
N
REP Measured
Figure 50
5
10
5 10
REP - Target Point 2Chi Squared=8.08E-006
E
S
W
N
REP Measured
Figure 51
5
10
5 10
RTV - Target Point 1Chi Squared=1.10E-005
E
S
W
N
RTV Measured
Figure 52
5
10
5 10
RTV - Target Point 2Chi Squared=1.91E-005
E
S
W
N
RTV Measured
Figure 53
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 94 / 173
5
10
5 10
SPL - Target Point 1Chi Squared=4.95E-006
E
S
W
N
SPL Measured
Figure 54
5
10
5 10
SPL - Target Point 2Chi Squared=7.83E-006
E
S
W
N
SPL Measured
Figure 55
5
10
5 10
UNJ - Target Point 1Chi Squared=6.70E-006
E
S
W
N
UNJ Measured
Figure 56
5
10
5 10
UNJ - Target Point 2Chi Squared=1.32E-005
E
S
W
N
UNJ Measured
Figure 57
5
10
5 10
UNK - Target Point 1Chi Squared=5.07E-006
E
S
W
N
UNK Measured
Figure 58
5
10
5 10
UNK - Target Point 2Chi Squared=3.93E-006
E
S
W
N
UNK Measured
Figure 59
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 95 / 173
-40
-30
-20
-10
0
10
20
30
40
0 30 60 90 120 150 180 210 240 270 300 330 360
dir
(T
arg
et M
ast
1)
- d
ir (
Ref
eren
ce M
ast)
[-]
Wind Direction Sector Centre [deg]
Veer Angle at Target Mast 1Participant ANM
ANMMeasured
-20
-10
0
10
20
0 30 60 90 120 150 180 210 240 270 300 330 360d
ir (
Tar
get
Mas
t 1
) -
dir
(R
efer
ence
Mas
t) [
-]Wind Direction Sector Centre [deg]
Veer Angle at Target Mast 1Participant GEO
GEOMeasured
-20
-10
0
10
20
0 30 60 90 120 150 180 210 240 270 300 330 360
dir
(T
arg
et M
ast
1)
- d
ir (
Ref
eren
ce M
ast)
[-]
Wind Direction Sector Centre [deg]
Veer Angle at Target Mast 1Participant LAM
LAMMeasured
-20
-10
0
10
20
0 30 60 90 120 150 180 210 240 270 300 330 360
dir
(T
arget
Mas
t 1)
- dir
(R
efer
ence
Mas
t) [
-]
Wind Direction Sector Centre [deg]
Veer Angle at Target Mast 1Participant MET
METMeasured
-20
-10
0
10
20
0 30 60 90 120 150 180 210 240 270 300 330 360
dir
(T
arg
et M
ast
1)
- d
ir (
Ref
eren
ce M
ast)
[-]
Wind Direction Sector Centre [deg]
Veer Angle at Target Mast 1Participant RTV
RTVMeasured
-20
-10
0
10
20
0 30 60 90 120 150 180 210 240 270 300 330 360
dir
(T
arg
et M
ast
1)
- d
ir (
Ref
eren
ce M
ast)
[-]
Wind Direction Sector Centre [deg]
Veer Angle at Target Mast 1Participant UNK
UNKMeasured
Figure 60: Veer Angles for Target Mast 1 versus Reference Mast.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 96 / 173
-40
-30
-20
-10
0
10
20
30
40
0 30 60 90 120 150 180 210 240 270 300 330 360
dir
(T
arget
Mas
t 2)
- dir
(R
efer
ence
Mas
t) [
-]
Wind Direction Sector Centre [deg]
Veer Angle at Target Mast 2Participant ANM
ANMMeasured
-20
-10
0
10
20
0 30 60 90 120 150 180 210 240 270 300 330 360dir
(T
arget
Mas
t 2)
- dir
(R
efer
ence
Mas
t) [
-]Wind Direction Sector Centre [deg]
Veer Angle at Target Mast 2Participant GEO
GEOMeasured
-20
-10
0
10
20
0 30 60 90 120 150 180 210 240 270 300 330 360
dir
(T
arg
et M
ast
2)
- d
ir (
Ref
eren
ce M
ast)
[-]
Wind Direction Sector Centre [deg]
Veer Angle at Target Mast 2Participant LAM
LAMMeasured
-20
-10
0
10
20
0 30 60 90 120 150 180 210 240 270 300 330 360
dir
(T
arg
et M
ast
2)
- d
ir (
Ref
eren
ce M
ast)
[-]
Wind Direction Sector Centre [deg]
Veer Angle at Target Mast 2Participant MET
METMeasured
-20
-10
0
10
20
0 30 60 90 120 150 180 210 240 270 300 330 360
dir
(T
arg
et M
ast
2)
- d
ir (
Ref
eren
ce M
ast)
[-]
Wind Direction Sector Centre [deg]
Veer Angle at Target Mast 2Participant RTV
RTVMeasured
-20
-10
0
10
20
0 30 60 90 120 150 180 210 240 270 300 330 360
dir
(T
arg
et M
ast
2)
- d
ir (
Ref
eren
ce M
ast)
[-]
Wind Direction Sector Centre [deg]
Veer Angle at Target Mast 2Participant UNK
UNKMeasured
Figure 61: Veer Angles for Target Mast 2 versus Reference Mast.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 97 / 173
2
4
6
8
10
12
14
16
18
20
2 4 6 8 10 12 14 16 18 20
Chi
Squar
ed
at
Tar
get
Mas
t 2 *
1E
6 [
-]
Chi Squared at Target Mast 1 * 1E6 [-]
5.43,15.37 ANM
4.98,7.90 GEO
6.64,14.89 LAM
6.07,7.90 MET
6.15,8.08 REP
11.03,19.10 RTV
4.95,7.83 SPL
6.70,13.18 UNJ
5.07,3.93 UNK
Figure 62
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 98 / 173
-30
-25
-20
-15
-10
-5
0
5
10
15
20
25
30
35
40
0 30 60 90 120 150 180 210 240 270 300 330 360
Err
or
in M
ean W
ind D
irec
tion [
deg
]
Wind Direction Sector Centre [deg]
Target Point 1 - Error in Mean Wind Direction
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNK
ANM GEO LAM MES MET REP RTV SPL UNJ UNK
0 -21.9 1.8 6.8 0.0 1.8 - -13.2 1.8 - 1.0
15 -9.2 -0.7 0.9 0.0 -1.4 - -15.7 -0.7 - -0.2
30 -7.5 -0.8 1.2 0.0 -2.7 - -15.8 -0.8 - 0.4
45 8.6 -0.3 1.5 0.0 -3.0 - -15.3 -0.3 - 1.8
60 35.2 0.3 1.2 0.0 -0.7 - -14.7 0.3 - 3.5
75 25.7 5.8 6.5 0.0 5.8 - -9.2 5.8 - 9.0
180 9.0 -5.6 -3.4 0.0 -6.5 -5.8 -20.6 -5.6 - -6.5
195 5.1 -9.6 -8.6 0.0 -9.6 - -24.6 -9.6 - -8.3
210 7.8 -8.3 -7.1 0.0 -8.3 - -23.3 -8.3 - -4.7
225 6.1 -3.6 -3.1 0.0 -3.6 - -18.6 -3.6 - 1.2
240 5.4 -1.0 2.4 0.0 0.3 - -16.0 -1.0 - 4.9
255 9.0 3.1 7.3 0.0 4.3 - -11.9 3.1 - 9.1
270 7.6 4.2 5.0 0.0 4.2 4.4 -10.8 4.2 - 8.6
285 1.5 3.6 7.3 0.0 4.6 - -11.4 3.6 - 6.2
300 -6.8 4.9 8.2 0.0 5.7 - -10.1 4.9 - 5.5
315 -13.5 4.2 7.5 0.0 4.2 - -10.8 4.2 - 4.2
330 -17.7 4.2 10.1 0.0 5.2 - -10.8 4.2 - 3.0
345 -17.4 5.1 11.7 0.0 5.1 - -9.9 5.1 - 4.0
Figure 63
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 99 / 173
-30
-25
-20
-15
-10
-5
0
5
10
15
20
25
30
35
40
0 30 60 90 120 150 180 210 240 270 300 330 360
Err
or
in M
ean W
ind D
irec
tion [
deg
]
Wind Direction Sector Centre [deg]
Target Point 2 - Error in Mean Wind Direction
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNK
ANM GEO LAM MES MET REP RTV SPL UNJ UNK
0 -14.3 4.5 4.7 0.0 3.7 - -10.5 4.5 - 2.0
15 -8.6 -4.1 -3.4 0.0 -5.7 - -19.1 -4.1 - 10.2
30 -8.2 -4.9 -2.9 0.0 -5.8 - -19.9 -4.9 - -5.6
45 -0.2 -4.6 -1.3 0.0 -6.0 - -19.6 -4.6 - -2.5
60 21.6 -4.5 -1.1 0.0 -2.3 - -19.5 -4.5 - -0.3
75 16.5 -1.7 2.2 0.0 0.4 - -16.7 -1.7 - 3.0
180 14.2 -2.3 -0.2 0.0 -4.1 -3.2 -17.3 -2.3 - -4.9
195 11.2 -6.7 -5.4 0.0 -7.8 - -21.7 -6.7 - -7.5
210 14.3 -9.6 -8.5 0.0 -8.7 - -24.6 -9.6 - -6.3
225 5.8 -9.4 -7.7 0.0 -8.3 - -24.4 -9.4 - -4.5
240 2.3 -11.5 -6.5 0.0 -9.3 - -26.5 -11.5 - -5.0
255 1.1 -10.9 -6.7 0.0 -8.8 - -25.9 -10.9 - -3.6
270 -3.3 -12.2 -12.2 0.0 -11.4 -12.8 -27.2 -12.2 - -5.8
285 -9.0 -10.2 -13.4 0.0 -9.2 - -25.2 -10.2 - -6.0
300 -11.8 -5.7 -9.5 0.0 -5.7 - -20.7 -5.7 - -4.4
315 -12.0 -0.2 -5.5 0.0 -1.3 - -15.2 -0.2 - -0.2
330 -15.9 1.2 0.0 0.0 -2.0 - -13.8 1.2 - 0.2
345 -14.4 3.7 2.2 0.0 2.6 - -11.3 3.7 - 0.7
Figure 64
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 100 / 173
0
30
60
90
120
150
180
210
240
270
300
330
360
0 30 60 90 120 150 180 210 240 270 300 330 360Win
d D
irec
tion R
ange
wit
h 9
5%
of
Dat
a In
side
[deg
]
Wind Direction Sector Centre [deg]
Target Point 1 - Wind Direction Range with 95% of Data Inside
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNK
ANM GEO LAM MES MET REP RTV SPL UNJ UNK
0 279.2 14.2 28.3 84.0 14.2 - 14.4 14.2 - 22.7
15 288.7 14.2 26.0 70.3 21.4 - 14.2 14.2 - 19.2
30 302.2 14.2 27.4 62.1 26.6 - 14.2 14.2 - 24.7
45 342.3 14.2 26.4 78.1 27.5 - 14.2 14.2 - 27.1
60 301.2 14.2 23.2 81.8 23.9 - 14.2 14.2 - 27.8
75 283.7 14.2 22.0 93.5 14.2 - 14.2 14.2 - 27.8
180 236.9 14.3 27.0 74.0 23.1 14.5 14.3 14.3 - 23.1
195 254.4 14.3 23.9 79.1 14.3 - 14.3 14.3 - 25.1
210 237.1 14.3 25.0 71.9 14.3 - 14.3 14.3 - 28.0
225 255.4 14.3 18.8 68.7 14.3 - 14.3 14.3 - 28.3
240 247.9 14.3 27.9 58.6 25.2 - 14.3 14.3 - 28.4
255 245.3 14.3 28.1 60.3 24.7 - 14.3 14.3 - 28.4
270 215.1 14.3 22.2 63.3 14.3 14.5 14.3 14.3 - 28.2
285 191.0 14.3 28.1 61.4 23.7 - 14.3 14.3 - 27.4
300 180.2 14.4 27.8 68.0 23.0 - 14.3 14.4 - 19.7
315 211.4 14.4 27.9 65.3 14.4 - 14.4 14.4 - 14.4
330 234.5 14.4 28.4 70.0 23.8 - 14.4 14.4 - 24.7
345 246.1 14.4 28.5 79.7 14.4 - 14.4 14.4 - 24.6
Figure 65
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 101 / 173
0
30
60
90
120
150
180
210
240
270
300
330
360
0 30 60 90 120 150 180 210 240 270 300 330 360Win
d D
irec
tion R
ange
wit
h 9
5%
of
Dat
a In
side
[deg
]
Wind Direction Sector Centre [deg]
Target Point 2 - Wind Direction Range with 95% of Data Inside
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNK
ANM GEO LAM MES MET REP RTV SPL UNJ UNK
0 270.7 14.2 21.0 208.2 22.7 - 14.4 14.2 - 27.3
15 317.0 14.2 31.7 139.3 26.0 - 14.2 14.2 - 29.0
30 294.2 14.2 38.0 104.1 23.6 - 14.2 14.2 - 29.0
45 319.4 14.2 27.9 104.2 25.6 - 14.2 14.2 - 27.4
60 283.5 14.2 27.9 113.2 27.0 - 14.2 14.2 - 28.1
75 278.9 14.2 28.0 126.6 26.9 - 14.2 14.2 - 28.3
180 274.3 14.3 26.9 70.2 26.4 23.1 14.3 14.3 - 27.4
195 284.6 14.3 25.4 91.2 24.5 - 14.3 14.3 - 32.8
210 222.7 14.3 24.4 83.9 23.6 - 14.3 14.3 - 27.9
225 241.7 14.3 26.2 85.2 24.4 - 14.3 14.3 - 28.3
240 226.5 14.3 28.3 88.8 27.0 - 14.3 14.3 - 28.5
255 232.0 14.3 28.1 85.4 26.9 - 14.3 14.3 - 28.5
270 209.5 14.3 14.3 64.4 22.7 19.8 14.3 14.3 - 28.5
285 187.1 14.3 27.8 55.1 23.7 - 14.3 14.3 - 28.1
300 174.1 14.4 28.1 66.9 14.4 - 14.3 14.4 - 25.2
315 205.2 14.4 30.7 71.9 24.4 - 14.4 14.4 - 14.4
330 206.9 14.4 25.7 86.1 27.8 - 14.4 14.4 - 23.9
345 237.1 14.4 37.4 156.7 24.2 - 14.4 14.4 - 27.7
Figure 66
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 102 / 173
-30
-25
-20
-15
-10
-5
0
5
10
-30 -25 -20 -15 -10 -5 0 5 10
Mea
n S
ecto
rwis
e E
rror
in
W
ind D
irec
tion
at
Tar
get
Mas
t 2 [
deg
]
Mean Sectorwise Error in Wind Direction
at Target Mast 1 [deg]
1.5,-0.6 ANM
-19.6,-24.9 GEO
-16.9,-24.2 LAM
0.0,0.0 MES
-19.7,-5.0 MET
-14.6,-19.9 RTV
-19.6,-24.9 SPL
2.4,-2.3 UNK
Figure 67
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 103 / 173
0
5
10
15
20
25
30
0 5 10 15 20 25 30
Mea
n A
bso
lute
Sec
torw
ise
Err
or
in
W
ind D
irec
tion
at
Tar
get
Mas
t 2 [
deg
]
Mean Absolute Sectorwise Error in Wind Direction
at Target Mast 1 [deg]
11.9,10.3 ANM
23.5,25.5 GEO
24.8,24.7 LAM
0.0,0.0 MES
24.1,5.7 MET
14.6,19.9 RTV
23.5,25.5 SPL
4.6,4.0 UNK
Figure 68
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 104 / 173
6.11 Single Turbine AEP
DEWI repeated the evaluation regarding mean wind speed with an energy yield instead of mean wind
speed. This energy yield is calculated separately with the power curves in Table 7.
The selection of these power curves is by chance. The list of turbines is not ordered according to any
particular rule. But the aim is to give an impression of the error of the models in predicting the AEP of a
contemporary, middle-class wind turbine. All these turbines and other turbines may or may not be
suitable for the site. DEWI calculated the energy yield according to the procedure specified in the latest
IEC standard on power curve measurement. The cut-out wind speed is recalculated according to
information available on the cut-out behaviour. Although necessary for energy yield assessment, no
density correction and no anemometer type correction is applied because we consider this as
meaningless for the Round Robin Test evaluations. The hub height is set equal to the height of the
anemometer at the target mast (80 m).
Siemens/AN Bonus 2.3MW MKII/Siemens 2.3MW/93-VS 80 measured Risoe-I-2444-1 (FGW Technische Richtlinien Teil 2 rev 14).
Enercon E-70 E4 measured DEWI PV 0308-08.2
GE Wind Energy 1.5 s (was Tacke) measured DEWI PV 0001-01
NEG NM82/1500 kW measured Windtest Grevenbroich LK 01 001 B1
NORDEX S-77/1500 measured Windtest Grevenbroich LK02001B1A6
Vestas V80-2.0MW 105.1 dB measured Windtest KWK WT1813/01
Table 7: Power curves used for the calculation of the single turbine AEP and the Farm Energy Yield.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 105 / 173
6.12 Energy Yield Results: Single Turbine AEP
In this section we present results concerning the capabilities of the different models of predicting the
annual energy production (AEP) of a single wind turbine. The wind turbine is ideally placed in the same
position as one of the two target masts with a hub height of 80 m. The same evaluation was repeated
for six different wind turbines and for both target masts. Information on the power curves of the wind
energy converters chosen for the test and details on the calculation procedure are reported in Section
6.11. The results of the evaluation are shown in tabular form in Table 8. It has been found that values of
relative error are approximately comprised in the range [0%-30%]. Due to the features of the selected
power curves and to properties of the of wind conditions at the site, wind turbines are generally
associated to different relative error. In other words, for the wind distribution at the site, for some wind
turbines the AEP might be „harder to predict” than for others. For this reason the relative error of one
model in predicting the energy yield of one turbine can only be compared with errors of other models
within the same turbine type. There was no clear evidence that AEP errors at target mast 1 were
significantly different from AEP errors at mast 2. As can be noticed in Figure 69 to Figure 74, for a
number of participants (namely REP, UNJ, MET, RTV ) the relative error is similar for both masts.
Despite a large spread in the results, all models were able to improve the initial information of the
reference mast and to obtain a lower relative error than SPL which was in the range [-27%, - 36%].
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 106 / 173
AN9323 EN7120 GE7015 NM8215 NOS7715 VE8020
ANM 5.62 6.59 6.49 1.21 3.96 3.65
GEO -20.28 -19.52 -20.54 -19.81 -20.55 -19.92
LAM -24.89 -26.40 -26.77 -21.06 -24.29 -24.91
MES 0.00 0.00 0.00 0.00 0.00 0.00
MET -12.25 -12.80 -12.98 -10.59 -11.99 -12.15
REP -24.97 -26.12 -26.44 -21.83 -24.50 -24.91
RTV 16.50 18.18 17.78 11.65 15.18 15.17
SPL -34.15 -35.63 -36.12 -30.08 -33.57 -34.16
UNJ -8.73 -9.12 -9.25 -7.55 -8.62 -8.70
UNK -12.84 -12.73 -13.04 -12.90 -13.29 -13.31
ANM -16.22 -17.71 -17.27 -13.86 -15.75 -16.44
GEO -3.31 -1.41 -2.61 -6.28 -4.13 -3.65
LAM -6.28 -7.22 -7.14 -4.52 -5.95 -6.47
MES 0.00 0.00 0.00 0.00 0.00 0.00
MET -10.39 -10.92 -10.93 -9.35 -10.24 -10.60
REP -23.78 -24.82 -25.06 -21.32 -23.41 -23.98
RTV 20.32 22.25 22.06 14.74 18.84 18.86
SPL -30.55 -31.87 -32.30 -27.14 -30.09 -30.72
UNJ -7.34 -7.59 -7.67 -6.80 -7.37 -7.50
UNK 3.09 4.23 4.09 0.19 2.03 2.23
Target Mast 1
Target Mast 2
Table 8: Relative error for a single turbine AEP in table form. All values in percent.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 107 / 173
-40
-30
-20
-10
0
10
20
30
40
-40 -30 -20 -10 0 10 20 30 40
Err
or
in A
EP
at
Tar
get
Mas
t 2 [
%]
Error in AEP at Target Mast 1 [%]
Relative AEP Error WTG AN9323
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNJ
UNK
Figure 69: Relative error in predicting the annual energy yield of a single AN Bonus 2.3MW turbine, ideally placed at
the position of mast 1 (x axis) and mast 2 (y axis).
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 108 / 173
-40
-30
-20
-10
0
10
20
30
40
-40 -30 -20 -10 0 10 20 30 40
Err
or
in A
EP
at
Tar
get
Mas
t 2 [
%]
Error in AEP at Target Mast 1 [%]
Relative AEP Error WTG EN7120
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNJ
UNK
Figure 70: Relative error in predicting the annual energy yield of a single Enercon E70 E4, ideally placed at the
position of mast 1 (x axis) and mast 2 (y axis).
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 109 / 173
-40
-30
-20
-10
0
10
20
30
40
-40 -30 -20 -10 0 10 20 30 40
Err
or
in A
EP
at
Tar
get
Mas
t 2 [
%]
Error in AEP at Target Mast 1 [%]
Relative AEP Error WTG GE7015
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNJ
UNK
Figure 71: Relative error in predicting the annual energy yield of a single GE Wind Energy 1.5 s, ideally placed at the
position of mast 1 (x axis) and mast 2 (y axis).
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 110 / 173
-40
-30
-20
-10
0
10
20
30
40
-40 -30 -20 -10 0 10 20 30 40
Err
or
in A
EP
at
Tar
get
Mas
t 2 [
%]
Error in AEP at Target Mast 1 [%]
Relative AEP Error WTG NM8215
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNJ
UNK
Figure 72: Relative error in predicting the annual energy yield of a single NEG NM82/1500, ideally placed at the
position of mast 1 (x axis) and mast 2 (y axis).
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 111 / 173
-40
-30
-20
-10
0
10
20
30
40
-40 -30 -20 -10 0 10 20 30 40
Err
or
in A
EP
at
Tar
get
Mas
t 2 [
%]
Error in AEP at Target Mast 1 [%]
Relative AEP Error WTG NOS7715
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNJ
UNK
Figure 73: Relative error in predicting the annual energy yield of a single NORDEX S-77/1500, ideally placed at the
position of mast 1 (x axis) and mast 2 (y axis).
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 112 / 173
-40
-30
-20
-10
0
10
20
30
40
-40 -30 -20 -10 0 10 20 30 40
Err
or
in A
EP
at
Tar
get
Mas
t 2 [
%]
Error in AEP at Target Mast 1 [%]
Relative AEP Error WTG VE8020
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNJ
UNK
Figure 74: Relative error in predicting the annual energy yield of a single Vestas V80-2.0MW, ideally placed at the
position of mast 1 (x axis) and mast 2 (y axis).
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 113 / 173
6.13 Wind Farm Energy Yield Results
The same evaluation exercise as presented in Section 6.12 for a single wind turbine was repeated for a
wind farm. For each of the two target masts, DEWI created, from the predicted wind data tab, a wind
resource grid. This resource grid has been used for the entire wind farm area. The wind resource grid
specifies the wind resource at each point in the form of overall and sector-wise Weibull A and k
parameters and wind direction frequencies. The grid contains the same wind resource at all points.
Using that resource grid, DEWI did calculate the energy yield for a wind farm of 16 turbines, arranged
on a square grid with a row and column spacing of 500 m. The rows are aligned towards geographic
north. For the wake calculations the „Jensen” Model is used with standard parameters (wake decay
0.075). It must be noted that this is a wind farm layout that is just selected to simplify the evaluation. It
is not fitted to the site in any way.
The wind farm is equipped with each of the turbines specified in Table 7 where the thrust curves are
used as specified by the manufacturer. One turbine type is used for all turbines in the farm, resulting in
6 different farms in total. The resulting farm energy yields, obtained with the participants results, will
be compared to farm energy yields obtained with the according measured data. Results are presented
as relative deviation in Table 9 and in Figure 76 - Figure 80.
Most of the considerations reported for the single turbine AEP can be applied to wind farm energy
yield. The relative errors are comprised in the range [0%- 30%]. Most of the models present similar
error for the two masts. As for the single turbine energy yield, all models were able to improve the
initial information and perform better than the virtual participant „SPL”.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 114 / 173
Table 9: Relative error for a wind Farm Energy Yield in table form. All values in percent.
AN9323 EN7120 GE7015 NM8215 NOS7715 VE8020
ANM 2,39 3,54 2,79 -0,11 1,43 2,53
GEO -24,93 -24,35 -25,42 -24,89 -25,35 -24,95
LAM -28,11 -28,87 -29,44 -24,38 -27,13 -28,09
MES 0,00 0,00 0,00 0,00 0,00 0,00
MET -14,91 -15,06 -15,36 -13,33 -14,48 -14,85
REP -29,11 -29,66 -30,29 -25,97 -28,36 -29,11
RTV 16,16 17,65 17,24 11,92 14,72 16,21
SPL -36,73 -37,53 -38,43 -32,71 -35,85 -36,78
UNJ -11,51 -11,72 -11,98 -10,33 -11,25 -11,52
UNK -15,83 -15,53 -16,16 -15,66 -16,03 -15,84
ANM -21,00 -21,37 -21,83 -18,36 -20,26 -20,92
GEO -5,98 -4,49 -5,67 -8,94 -7,37 -6,02
LAM -9,36 -9,56 -9,61 -7,45 -8,61 -9,20
MES 0,00 0,00 0,00 0,00 0,00 0,00
MET -12,70 -12,60 -12,87 -11,55 -12,32 -12,56
REP -27,17 -27,43 -28,08 -24,57 -26,52 -27,09
RTV 20,47 22,41 22,10 15,37 18,90 20,66
SPL -32,95 -33,52 -34,43 -29,43 -32,17 -32,94
UNJ -9,86 -9,85 -10,17 -9,22 -9,75 -9,83
UNK 1,54 2,76 2,23 -1,04 0,62 1,65
Target Mast 1
Target Mast 2
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 115 / 173
-40
-30
-20
-10
0
10
20
30
40
-40 -30 -20 -10 0 10 20 30 40
Err
or
in F
EY
at
Tar
get
Mas
t 2 [
%]
Error in FEY at Target Mast 1 [%]
Relative FEY Error WTG AN9323
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNJ
UNK
Figure 75: Relative error in predicting the annual energy yield of a wind farm (Siemens/AN Bonus 2.3MW MKII
WTGs).
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 116 / 173
-40
-30
-20
-10
0
10
20
30
40
-40 -30 -20 -10 0 10 20 30 40
Err
or
in F
EY
at
Tar
get
Mas
t 2 [
%]
Error in FEY at Target Mast 1 [%]
Relative FEY Error WTG EN7120
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNJ
UNK
Figure 76: Relative error in predicting a farm energy yield (Enercon E-70 E4 WTGs).
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 117 / 173
-40
-30
-20
-10
0
10
20
30
40
-40 -30 -20 -10 0 10 20 30 40
Err
or
in F
EY
at
Tar
get
Mas
t 2 [
%]
Error in FEY at Target Mast 1 [%]
Relative FEY Error WTG GE7015
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNJ
UNK
Figure 77: Relative error in predicting a farm energy yield (GE Wind Energy 1.5s WTGs)
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 118 / 173
-40
-30
-20
-10
0
10
20
30
40
-40 -30 -20 -10 0 10 20 30 40
Err
or
in F
EY
at
Tar
get
Mas
t 2 [
%]
Error in FEY at Target Mast 1 [%]
Relative FEY Error WTG NM8215
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNJ
UNK
Figure 78: Relative error in predicting a farm energy yield (NEG NM82 WTGs)
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 119 / 173
-40
-30
-20
-10
0
10
20
30
40
-40 -30 -20 -10 0 10 20 30 40
Err
or
in F
EY
at
Tar
get
Mas
t 2 [
%]
Error in FEY at Target Mast 1 [%]
Relative FEY Error WTG NOS7715
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNJ
UNK
Figure 79: Relative error in predicting a farm energy yield (NORDEX S-77/1500 WTGs)
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 120 / 173
-40
-30
-20
-10
0
10
20
30
40
-40 -30 -20 -10 0 10 20 30 40
Err
or
in F
EY
at
Tar
get
Mas
t 2 [
%]
Error in FEY at Target Mast 1 [%]
Relative FEY Error WTG VE8020
ANM
GEO
LAM
MES
MET
REP
RTV
SPL
UNJ
UNK
Figure 80: Relative error in predicting a farm energy yield (Vestas V80-2.0MW WTGs)
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 121 / 173
7 Conclusions
The results of 8 flow models operated by the participants ANM, GEO, LAM, MET, REP, RTV, UNJ and
UNK were analysed and compared to measured data regarding one site equipped with three met
masts. The results are therefore valid only for this particular site.
The results of UNJ and REP are incomplete and cannot be fully compared to the others. The results of
ANM can not in all aspects be fully compared to the other models because the modelling and/or data
processing approach of ANM differs from the others for the sector-wise data.
The site under consideration in the test is a plateau located on the island Sardinia in the Mediterranean
Sea. It turns out that the wind conditions on site are by far more complex than suggested by the height
structure. Accordingly, the model results differ from each other considerably in almost all aspects.
To some part, the difference in mean wind speed between the reference mast and the two target masts
is constituted by the measurement height difference of 37 m that has to be bridged by the models.
There is a tendency of all participant's results, except RTV, to underestimate mean wind speed. which is
a critical issue in the context of the assessment of the suitable wind turbine class for a site.
Participant RTV uses a different type of model and his results differ significantly from the others, mainly
because he calculates much less directional variation of the relationship between the test wind
measurements and because it is the only model showing a significant overestimation (and not an
underestimation) of wind speed and energy yield at this site. This is a statement regarding the
inhomogeneity of the modelling approaches and not a statement regarding the accuracy of the results
of RTV.
None of the participants is able to model the characteristic flow features for the site in all details for
both target masts but the results suggest that in some cases specific meteorological effects are
reproduced for either mast 1 or mast 2 but not for both masts at the same time by the same
participant.
The analysis of the results in terms of 15 degree wind direction sectors shows insufficient results for all
participants except for LAM (only at target mast 2), ANM (only at target mast 1) and partly for UNK. The
observed large sector-wise errors partly average out in the calculation of the energy yield.
The test was set up carefully, especially regarding the meteorological and geographical data, which is
comparable to or of better quality than what is usually used for wind and site assessment in central
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 122 / 173
Europe. That the site-specific effects can be reproduced by some models (although none of the models
reproduces all effects), substantiates that these effects are real meteorological effects and not
measurement errors. Furthermore, it indicates that the geographical and meteorological data used in
the test is sufficient for the calculation of those effects.
It must be concluded that the models partly describe flow features that are not present in reality, and,
for this site, the dominant flow effects are, with exceptions, not sufficiently modelled.
Two of the model results showed for a specific wind direction sector strong artefacts that may be either
modelling problems or problems with adaptation to the test procedure. Such artefacts should be
excluded by the participants through specific quality control methods regarding the simulation results.
Altogether, we consider the round robin test procedure established in this research as suitable to the
problem area and useful for the purpose of model testing. It may be used as a template for further,
similar tests, that should then also contain a strict criterion that states whether a model „passed“ the
test or „did not pass“ the test. Such a criterion must not only refer to the relative deviation of the
participants results from a mean value of all participants results, due to the inhomogeneity of the
models and the presence of outliners.
If, instead, the criterion is based on the deviation from measured data, there are difficult problems to
overcome: firstly, for the measurements there are very high quality demands that should be fulfilled by
wind measurements specifically adapted and operated for this purpose. These costs must not be
considered as prohibitive. Secondly, there is no easy way to define the maximum deviation from the
measured data that allows to assign a „passed“ to a model. Thirdly, there would be high nondisclosure
demands on the measured data of the target masts.
Only if further developments improve the homogeneity of the models, the deviation from the mean of
all participants can be used as a test criterion. Such a test criterion is required.
To resolve the problem, we propose to focus on improvements of the homogeneity and transparency of
the models.
In particular, model validation becomes meaningless if changes of model software (either the core or
the pre- and postprocessing) take place behind the scenes. Validation results are tied to a model in a
specific state (version). However, it is not clear what version control system the participants use.
The flow modelling is tied to the company offering the service. For both the users of commercial
software and for the users of in-house software, a harmonisation of the wind modelling work is
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 123 / 173
required. The first important step towards such a harmonisation is the present round robin test. The
next step could be the creation of board similar to MEASNET, like “SIMULNET”, which maintains
harmonisation of the services provided by the members and constantly follows the state of the art in
this field. One could benefit from the experience gained in the creation of MEASNET. In particular, one
would have to find ways to harmonise the flow modelling services and to conduct quality checks,
possibly using this round robin as a template.
From the experience acquired during this Round Robin we judge as necessary an improvement of the
documentation of the flow modelling work, especially regarding spatial resolution, directional and wind
speed resolution, domain size, convergence behaviour and exact specification and version of the model
used.
Although this is not foreseen at the moment, the further development may greatly benefit if one would
agree on one single model, which may incorporate a mesoscale model from the family of MM5/WRF
and a microscale model from the family of steady state Navier-Stokes solvers with a two equation
turbulence closure. An optimum transparency could be achieved with an open source model that is
maintained by the community along with strict application rules.
As this is not expected, significant improvements could also be achieved if one agrees on only one pre-
and postprocessing software, while keeping the flow model cores closed. In our opinion, the difference
between different microscale CFD models regarding their results may originate partly from differences
in the pre- and postprocessing and not only from differences in the core solvers.
Although the results of this round robin show that there is still a strong need of research and
development necessary in the field of CFD modelling, it is assumed that a carefully designed and
applied flow model will provide better accuracy than WASP, because there are less simplifying
assumptions regarding the processes modelled and important, relevant processes, especially in
complex terrain, are not modelled at all by WASP. Flow modelling is today a standard engineering tool
that is successfully used in many industrial sectors and one must take advantage of the capabilities for
wind energy applications. An important design driver of the WASP software were the very limited
capabilities of the computer hardware at that time. Today, there is no justification at all for the many
simplifications that are incorporated into WASP and there is no reason why one should trust more the
results of WASP than the results of an appropriate flow model. However, WASP was designed
specifically for wind energy applications, while flow models for wind energy applications are in general
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 124 / 173
adapted versions of flow models for other purposes (general CFD, large-scale meteorological
modelling). A flow model may very accurately model complex terrain wind flow, but problems may be
related to the pre- and postprocessing, e.g. the wind data or the technical properties of the wind
turbines may not be handled appropriately. It is therefore important not to focus only on the core flow
model but also on the pre- and postprocessing.
Although WASP is a standardised computer code, the results obtained with it depend on the input data
and the way it is handled (roughness map, height map, wind data, possibly heat flux adaptations,...).
This dependency is present in a WASP calculation as it is in a calculation with a flow model, although in
the case of a flow model, the model operator has flexibility regarding the spatial discretisation (grid
design). It is required to combine the higher accuracy of the flow models with the required certainty
regarding homogeneity of the results by taking next steps in the harmonisation process.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 125 / 173
8 Appendix
8.1 Overview of the properties of the on-site measurements
In this section details of the on-site wind data of the three met masts are shown. The data is
represented by the common time series (common time steps) of the following sensors:
1. Reference Mast, Anemometer at 43m height agl.(Thies First Class).
2. Reference Mast, Wind Vane at 42m height agl.
3. Target Mast 1, Anemometer at 80m height agl.(Thies First Class).
4. Target Mast 1, Wind Vane at 78m height agl.
5. Target Mast 2, Anemometer at 80m height agl. (Thies First Class).
6. Target Mast 2, Wind Vane at 78m height agl.
It has been verifies that the data logger internal clocks run synchronously. Additionally, this common
time series was filtered with respect to the wind direction at target mast 1 (42m height) such that data
from within the sector [82.5 °,172.5 °] is excluded in order to minimise influences of the mast top on
the anemometer. The resulting time series ranges from 2005-11-09 18:10:00 until 2006-07-01 00:00:00
(233 days). The total number of time steps amounts to 27254 which would correspond to a continuous,
complete time series of 189 days (18.9% missing data , mainly due to directional filtering).
Within the test, sector-wise analyses are carried out (15 degree wind direction sectors). It has been
verified that each sector contains enough data sets in order to yield representative results. The number
of data in each sector is reported in Table 11.
Table 10 summarises the mean wind speeds measured at the three masts for the wind speed sensors
used in the test. The Weibull statistics and wind direction distributions are shown in Figure 81, Figure
82 and Figure 83.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 126 / 173
Wind Speed Sensor Mean Wind Speed
(Calculated from the
Time Series) [m/s]
Ratio of Mean Wind Speed to
Mean Wind Speed Measured at
Reference Mast [-]
Reference Mast at 43m 5.07 100.0%
Target Mast 1 at 80m 6.10 120.4%
Target Mast 2 at 80m 5.95 117.5%
Table 10: Mean Wind Speeds for the site masts.
There is significant increase in mean wind speed from the reference mast to each of the two target
masts. Mean wind speed is slightly higher at target mast 1 than at target mast 2.
Regarding the overall k-factors, there is hardly any difference between the two target masts. The k-
factor is almost the same for target mast 1 and 2 (1.85/1.84). At the reference mast, the k-factor is
slightly lower (1.81).
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 127 / 173
N
W E
S
Figure 81: Wind direction and wind speed distribution at the reference mast at 43m agl.
(The mean wind U in the graphs is calculated from the wind speed distribution, which has been fitted to the binned
wind data and therefore it is usually not equivalent to the wind data itself.)
N
W E
S
Figure 82: Wind direction and wind speed distribution at the target mast 1 at 80m agl.
(The mean wind U in the graphs is calculated from the wind speed distribution, which has been fitted to the binned
wind data and therefore it is usually not equivalent to the wind data itself.)
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 128 / 173
N
W E
S
Figure 83: Wind direction and wind speed distribution at the target mast 2 at 80m agl.
(The mean wind U in the graphs is calculated from the wind speed distribution, which has been fitted to the binned
wind data and therefore it is usually not equivalent to the wind data itself.)
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 129 / 173
8.1.1 Wind Direction Effects
There are significant differences in the wind direction distributions between the three masts for wind
from south, south-west, west and north-west. For wind from north-east, the wind direction
distributions at the three masts do not differ very much. A comparison of the wind direction
distributions of the reference mast and target mast 1 shows that there is significantly more often wind
from south-west at target mast 2 than at the reference mast. Also, the share of data with a wind
direction around south decreases at target mast 1, compared to the reference mast. This fact is
associated with the fact that, on average, the wind from south is turned by about 5 degree to 10 degree
clockwise at target mast 1, compared to the reference mast. At the same time, for the wind directions
west to north-west, wind direction is turned anticlockwise by about 5 degree at target mast 1,
compared to the reference mast. This direction dependent effect is shown also in Figure 84,where the
sector-wise averaged wind direction difference between the two masts is shown. The situation
regarding systematic wind direction effects at target mast 2 is different. Wind, that blows, at the
reference mast, from east, is turned clockwise towards north-north-west at target mast 2. This effect is
also clearly visible in the wind direction difference plot (Figure 85). For wind from west and south-west
(at the reference mast), wind direction is turned clockwise by bout 10 degree. This turning vanishes for
wind from north-north-west, leading to slight peak in the wind direction distribution at target mast 2 at
north-west-west.
For the evaluations regarding wind direction differences, all data with wind speeds below 1m/s were
excluded.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 130 / 173
-60
-40
-20
0
20
40
60
0 45 90 135 180 225 270 315 360
Win
d D
irec
tion D
iffe
rence
Dir
(Tar
get
Mas
t1)
- D
ir(R
efer
ence
Mas
t) [
deg
]
Wind Direction Sector Centre (Reference Mast) [deg]
Wind Direction DifferencesTarget Mast 1 vs. Reference Mast
Figure 84: Wind direction differences between target mast 1 and reference mast.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 131 / 173
-60
-40
-20
0
20
40
60
0 45 90 135 180 225 270 315 360
Win
d D
irec
tion D
iffe
rence
Dir
(Tar
get
Mas
t2)
- D
ir(R
efer
ence
Mas
t) [
deg
]
Wind Direction Sector Centre (Reference Mast) [deg]
Wind Direction DifferencesTarget Mast 2 vs. Reference Mast
Figure 85: Wind direction difference between target mast 2 and reference mast.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 132 / 173
8.1.2 Speed-up Factors
The common time series of the wind data at the three masts is subdivided into wind direction sectors
with respect to the wind direction at the reference mast (15 deg sectors). For each sector, the ratio of
the mean wind speeds at one of the target masts to the mean wind speed at the reference mast is
evaluated and reported in Table 11 and Figure 86.
There are large differences between the speed-up factors for target mast 1 and target mast 2. For wind
from north-east, the speed-up factors are significantly higher for target mast 2 compared to target mast
1 , but the general way in that the speed up factors change with wind direction is similar between the
two target masts: There is peak at about 30 deg and the speed up becomes smaller the more the wind
turns towards east. For wind within the direction range 180 deg to 360 deg, the difference between the
two target masts is even more pronounced, in that also the general form of the speed-up function
versus wind direction changes and not only the scaling.
At target mast 2 there is strong increase of the speed-up factor all through the wind direction range
from 195 deg to 315 degree. There is hardly any change of the speed-up factor for wind directions in-
between 315 deg and 345 deg. The increase is very characteristic for the site and ranges from 104.4% at
195 deg up to 128.5% at 345 deg. At target mast 1, this systematic direction dependent increase is not
visible at all. Instead, the speed-up factors become smaller for increasing wind directions greater than
180 degree.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 133 / 173
Wind Direction
Sector Centre
[deg]
Number of
Data Sets
Reference
Mast
Target Mast
1
Target Mast
2
Mean Wind Speed at
Target Mast 1 / Mean
Wind Speed at Ref
Mast
Mean Wind Speed at
Target Mast 2 / Mean
Wind Speed at Ref
Mast
0 834 3.09 3.40 3.96 1.1004 1.2815
15 1253 3.57 4.16 4.78 1.1653 1.3399
30 1743 4.89 5.74 6.49 1.1744 1.3289
45 1229 4.16 4.75 5.66 1.1407 1.3600
60 1026 4.24 4.61 5.57 1.0872 1.3122
75 1105 4.88 5.02 5.96 1.0291 1.2211
180 2675 6.06 7.73 6.72 1.2749 1.1092
195 2309 5.42 6.71 5.66 1.2371 1.0441
210 2131 5.63 7.03 5.94 1.2473 1.0538
225 1791 5.94 7.37 6.41 1.2397 1.0791
240 1356 4.74 6.00 5.34 1.2673 1.1277
255 1605 4.96 6.15 5.69 1.2403 1.1471
270 2240 5.08 6.19 5.89 1.2196 1.1603
285 2112 5.68 6.87 6.81 1.2082 1.1980
300 1243 5.31 6.04 6.46 1.1389 1.2167
315 929 4.96 5.94 6.31 1.1980 1.2733
330 975 4.83 5.62 6.17 1.1649 1.2775
345 698 3.78 4.19 4.86 1.1077 1.2853
Mean Wind Speed [m/s]
Table 11: Sector-wise mean wind speeds (calculated from time series directly) and according speed-up
factors.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 134 / 173
1
1.1
1.2
1.3
1.4
0 45 90 135 180 225 270 315 360
Spee
d-u
p F
acto
rv(T
arget
Mas
t1)
/ v(R
efer
ence
Mas
t) [
deg
]
Wind Direction Sector Centre (Reference Mast) [deg]
Speed-up Factors
Target Mast 1Target Mast 2
Figure 86: Measured sector-wise speed-up factors (Ratio of sector-wise mean wind speed each target mast to
according mean wind speed at reference mast.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 135 / 173
8.1.3 Turbulence Intensity
Mean turbulence intensity depending on wind speed is reported for the three masts in Figure 87 to
Figure 90. There is hardly any difference in the turbulence intensity for different wind speed classes
between the two target masts. The change of the turbulence intensity with wind speed is however
slightly different at the reference mast. On the one hand there is slight increase of mean turbulence
intensity with wind speed visible. On the other hand, for the anemometer that is used for the test at
the reference mast, turbulence intensity does not increase towards very low wind speeds. At the
second anemometer at the reference mast, that is not used for the test, turbulence does increase only
slightly for low wind speeds. In general, one may conclude from the reported turbulence behaviour that
turbulence properties at the reference mast are slightly different from those at the two target masts,
who are essentially the same. There is one second important site property regarding turbulence: Figure
91 and Figure 92 report the change of turbulence intensity with wind direction for all wind speeds
(Figure 91) and wind speeds between 8m/s and 10m/s (Figure 92). Both figures show strong increase of
the turbulence intensity with increasing wind direction for the wind direction range 180 deg to 360 deg,
i.e. turbulence intensity is much higher for wind from west than from south and much higher for wind
from north than from west. Turbulence intensity increases from about 7% to about 14% within this
range, considering the wind speed interval 8m/s to 10m/s.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 136 / 173
0
5
10
15
20
25
30
35
40
1 3 5 7 9 11 13 15 0
1000
2000
3000
4000
5000
6000
7000
8000
9000
Turb
ule
nce
Inte
nsi
ty [
%]
Num
ber
of
Dat
a in
Win
d S
pee
d C
lass
Wind Speed Class Centre [m/s]
Turbulence Intensity: Reference Mast
Figure 87: Turbulence intensity at the reference mast.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 137 / 173
0
5
10
15
20
25
30
35
40
1 3 5 7 9 11 13 15 17 0
1000
2000
3000
4000
5000
6000
7000
Turb
ule
nce
Inte
nsi
ty [
%]
Num
ber
of
Dat
a in
Win
d S
pee
d C
lass
Wind Speed Class Centre [m/s]
Turbulence Intensity: Target Mast 1
Figure 88: Turbulence intensity at target mast 1.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 138 / 173
0
5
10
15
20
25
30
35
40
1 3 5 7 9 11 13 15 0
1000
2000
3000
4000
5000
6000
7000
8000
Turb
ule
nce
Inte
nsi
ty [
%]
Num
ber
of
Dat
a in
Win
d S
pee
d C
lass
Wind Speed Class Centre [m/s]
Turbulence Intensity: Target Mast 2
Figure 89: Turbulence intensity at target mast 2.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 139 / 173
0
5
10
15
20
25
30
35
40
1 3 5 7 9 11 13 15 17
Turb
ule
nce
Inte
nsi
ty [
%]
Wind Speed Class Centre [m/s]
Target Mast 2Target Mast 1
Reference Mast (Used Anemometer)Reference Mast (Thies Classic)
Figure 90: Turbulence intensity at the three masts.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 140 / 173
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
0 45 90 135 180 225 270 315 360
Turb
ule
nce
Inte
nsi
ty [
%]
Wind Direction Sector Class Centre [deg]
Turbulence Intensity versus DirectionAll Wind Speeds
Reference MastTarget Mast 1Target Mast 2
Figure 91: Change of turbulence intensity with wind direction at all three masts.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 141 / 173
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
0 45 90 135 180 225 270 315 360
Turb
ule
nce
Inte
nsi
ty [
%]
Wind Direction Sector Class Centre [deg]
Turbulence Intensity versus DirectionWind Speed Interval [8m/s,10m/s[
Reference MastTarget Mast 1Target Mast 2
Figure 92: Change of turbulence intensity with wind direction at all three masts for wind speeds in the range from
8m/s to 10m/s.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 142 / 173
8.1.4 Sector-wise Wind Speed Correlation Properties
The common time series of the three masts is analysed with respect to 30 degree wind direction
sectors, established on base of the wind direction measurement at the reference mast, excluding the
directions disturbed by the presence of the mast top. Scatter plots of the simultaneous wind speed
measurements at the reference mast and target mast 1 and target mast 2 are shown below in this
section. There is strong sector-wise correlation between the two target masts and the reference mast,
which varies slightly with wind direction (Figure 93). The correlation coefficient reaches its overall
maximum (regarding both masts and undisturbed sectors at the reference mast) at target mast 2 for
the 30 degree wind direction sector centred at 225 degree (r2=0.9324). For most sectors, correlation is
higher for the pair target mast 1 and reference mast than for the pair target mast 2 and reference mast.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 143 / 173
0 5 10 15 20 25 300
5
10
15
20
25
30[0°, 30°[ r
2=0.89473
Wind Speed at Reference Mast [m/s]
Win
d S
pe
ed
at
Ta
rge
t M
ast
1 [
m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[30°, 60°[ r
2=0.91825
Wind Speed at Reference Mast [m/s]
Win
d S
pe
ed
at
Ta
rge
t M
ast
1 [
m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[60°, 90°[ r
2=0.84052
Wind Speed at Reference Mast [m/s]
Win
d S
pe
ed
at
Ta
rge
t M
ast
1 [
m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[150°, 180°[ r
2=0.91719
Wind Speed at Reference Mast [m/s]
Win
d S
pe
ed
at
Ta
rge
t M
ast
1 [
m/s
]
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 144 / 173
0 5 10 15 20 25 300
5
10
15
20
25
30[180°, 210°[ r
2=0.92761
Wind Speed at Reference Mast [m/s]
Win
d S
pe
ed
at
Ta
rge
t M
ast
1 [
m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[210°, 240°[ r
2=0.93236
Wind Speed at Reference Mast [m/s]
Win
d S
pe
ed
at
Ta
rge
t M
ast
1 [
m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[240°, 270°[ r
2=0.87348
Wind Speed at Reference Mast [m/s]
Win
d S
pe
ed
at
Ta
rge
t M
ast
1 [
m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[270°, 300°[ r
2=0.84289
Wind Speed at Reference Mast [m/s]
Win
d S
pe
ed
at
Ta
rge
t M
ast
1 [
m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[300°, 330°[ r
2=0.87442
Wind Speed at Reference Mast [m/s]
Win
d S
pe
ed
at
Ta
rge
t M
ast
1 [
m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[330°, 360°[ r
2=0.89486
Wind Speed at Reference Mast [m/s]
Win
d S
pe
ed
at
Ta
rge
t M
ast
1 [
m/s
]
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 145 / 173
0 5 10 15 20 25 300
5
10
15
20
25
30[0°, 30°[ r
2=0.84079
Wind Speed at Reference Mast [m/s]
Win
d S
pe
ed
at
Ta
rge
t M
ast
2 [
m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[30°, 60°[ r
2=0.88916
Wind Speed at Reference Mast [m/s]
Win
d S
pe
ed
at
Ta
rge
t M
ast
2 [
m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[60°, 90°[ r
2=0.8398
Wind Speed at Reference Mast [m/s]
Win
d S
pe
ed
at
Ta
rge
t M
ast
2 [
m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[150°, 180°[ r
2=0.89335
Wind Speed at Reference Mast [m/s]
Win
d S
pe
ed
at
Ta
rge
t M
ast
2 [
m/s
]
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 146 / 173
0 5 10 15 20 25 300
5
10
15
20
25
30[180°, 210°[ r
2=0.89579
Wind Speed at Reference Mast [m/s]
Win
d S
pe
ed
at
Ta
rge
t M
ast
2 [
m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[210°, 240°[ r
2=0.87557
Wind Speed at Reference Mast [m/s]
Win
d S
pe
ed
at
Ta
rge
t M
ast
2 [
m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[240°, 270°[ r
2=0.86067
Wind Speed at Reference Mast [m/s]
Win
d S
pe
ed
at
Ta
rge
t M
ast
2 [
m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[270°, 300°[ r
2=0.87258
Wind Speed at Reference Mast [m/s]
Win
d S
pe
ed
at
Ta
rge
t M
ast
2 [
m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[300°, 330°[ r
2=0.87449
Wind Speed at Reference Mast [m/s]
Win
d S
pe
ed
at
Ta
rge
t M
ast
2 [
m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[330°, 360°[ r
2=0.86882
Wind Speed at Reference Mast [m/s]
Win
d S
pe
ed
at
Ta
rge
t M
ast
2 [
m/s
]
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 147 / 173
15 45 75 105 135 165 195 225 255 285 315 3450.82
0.84
0.86
0.88
0.9
0.92
0.94Correlation Coefficient versus Wind Direction
Wind Direction Sector Centre at Reference Mast [deg]
Corr
ela
tion C
oeffic
ient r2
Target Mast 1Target Mast 2
Figure 93: Correlation coefficient versus wind direction.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 148 / 173
8.1.5 Filling of a Gap in Target Mast 1 Data
In the common time series (common time steps) of the reference mast and the two target masts there
is no wind speed available for the used anemometer at target mast 1 for the period 2005-11-26
01:30:00 until 2005-12-19 14:50:00. It was decided that it is most appropriate for the purpose of the
test to fill this gap my means of sector-wise correlation with the anemometer at 60m height at the
same mast, du to the following reasons: Firstly, it is desired to have for the test a time series as
complete in time as possible. Would we neglect that period, that period would have to be excluded also
from the other masts. Secondly, this type of correlation (MCP correlation) is a standard procedure for
wind energy application and shows (see below) excellent correlation between the two anemometers at
the same mast.
The correlation procedure applied consists of linear regression in 36 10 degree wind direction sectors
using the regression function y=a*x+b. All data sets with wind speeds below 1m/s were filtered out
before the correlation function was fitted.
The total period 2005-11-26 01:30:00 until 2005-12-19 14:50:00 consists of 2319 time steps and
constitutes 7.1% of the total common period of the three masts.
The correlation coefficient r squared varies from sector to sector between 0.9551 and 0.9955. The
number of data in each 10 degree wind direction sector considered is sufficiently high. In order to check
the accuracy of the MCP correlation, a self consistency test was conducted. In that test, the regression
functions are applied to the data of the 60m anemometer for the common period of the 60m sensor
and the 80m sensor, i.e. for the period where there is wind speed data available from both
anemometers plus the direction data. The calculated wind speed time series for the 80m anemometer
is then compared to the measured one with respect to mean wind speed. This self consistency test
showed an error in mean wind speed of only 0.01%, indicating very good correlation.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 149 / 173
8.1.5.1 Sector-wise Scatter Plots with Regression Lines
0 5 10 15 20 25 300
5
10
15
20
25
30[0°, 10°] r
2=0.98532 N=472
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[10°, 20°] r
2=0.99079 N=741
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[20°, 30°] r
2=0.99376 N=1004
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[30°, 40°] r
2=0.99545 N=1022
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[40°, 50°] r
2=0.9919 N=889
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[50°, 60°] r
2=0.97043 N=702
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[60°, 70°] r
2=0.96918 N=789
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[70°, 80°] r
2=0.9853 N=757
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[80°, 90°] r
2=0.98899 N=618
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[90°, 100°] r
2=0.96419 N=502
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[100°, 110°] r
2=0.95513 N=458
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[110°, 120°] r
2=0.96819 N=447
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 150 / 173
0 5 10 15 20 25 300
5
10
15
20
25
30[120°, 130°] r
2=0.97958 N=269
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[130°, 140°] r
2=0.97343 N=233
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[140°, 150°] r
2=0.98461 N=245
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[150°, 160°] r
2=0.99162 N=419
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[160°, 170°] r
2=0.99519 N=862
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[170°, 180°] r
2=0.98891 N=1267
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[180°, 190°] r
2=0.98886 N=1151
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[190°, 200°] r
2=0.99034 N=940
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[200°, 210°] r
2=0.99365 N=1224
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[210°, 220°] r
2=0.99345 N=1485
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[220°, 230°] r
2=0.99477 N=1436
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[230°, 240°] r
2=0.99157 N=1132
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 151 / 173
0 5 10 15 20 25 300
5
10
15
20
25
30[240°, 250°] r
2=0.99073 N=1414
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[250°, 260°] r
2=0.98799 N=1153
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[260°, 270°] r
2=0.98875 N=1107
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[270°, 280°] r
2=0.98863 N=1363
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[280°, 290°] r
2=0.99206 N=1197
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[290°, 300°] r
2=0.988 N=689
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[300°, 310°] r
2=0.98696 N=591
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[310°, 320°] r
2=0.99233 N=664
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[320°, 330°] r
2=0.99385 N=543
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[330°, 340°] r
2=0.99203 N=529
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[340°, 350°] r
2=0.98943 N=422
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[350°, 360°] r
2=0.9831 N=410
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 152 / 173
8.1.6 Filling of a Gap in Target Mast 2 Data
For further explanations on the method used see section 8.1.5.
The period with missing wind speed data at target mast 2 reaches from 2005-12-28 06:10:00 to 2005-
12-28 09:00:00, consisting of 18 time steps. This period represents 0.05% of the total common period
of the three masts. All data sets with wind speeds below 1m/s were filtered out before the correlation
function was fitted.
The correlation coefficient r squared varies between 0.9715 and 0.9944. The number of data in each 10
degree wind direction sector considered is sufficiently high. The self consistency test showed an error in
mean wind speed of 0.02%, indicating very good correlation.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 153 / 173
8.1.6.1 Sector-wise Scatter Plots with Regression Lines
0 5 10 15 20 25 300
5
10
15
20
25
30[0°, 10°] r
2=0.98626 N=405
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[10°, 20°] r
2=0.98674 N=631
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[20°, 30°] r
2=0.99413 N=1008
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[30°, 40°] r
2=0.98917 N=1439
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[40°, 50°] r
2=0.97922 N=1241
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[50°, 60°] r
2=0.97186 N=865
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[60°, 70°] r
2=0.9903 N=706
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[70°, 80°] r
2=0.98893 N=773
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[80°, 90°] r
2=0.98307 N=708
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[90°, 100°] r
2=0.97149 N=526
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[100°, 110°] r
2=0.98749 N=590
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[110°, 120°] r
2=0.98669 N=420
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 154 / 173
0 5 10 15 20 25 300
5
10
15
20
25
30[120°, 130°] r
2=0.98869 N=310
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[130°, 140°] r
2=0.98973 N=292
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[140°, 150°] r
2=0.99016 N=363
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[150°, 160°] r
2=0.99409 N=682
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[160°, 170°] r
2=0.98745 N=1313
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[170°, 180°] r
2=0.98657 N=1898
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[180°, 190°] r
2=0.99052 N=1514
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[190°, 200°] r
2=0.99378 N=1153
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[200°, 210°] r
2=0.99428 N=1066
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[210°, 220°] r
2=0.99439 N=1233
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[220°, 230°] r
2=0.99253 N=1311
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[230°, 240°] r
2=0.99323 N=1161
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 155 / 173
0 5 10 15 20 25 300
5
10
15
20
25
30[240°, 250°] r
2=0.98685 N=994
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[250°, 260°] r
2=0.98601 N=996
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[260°, 270°] r
2=0.98585 N=1115
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[270°, 280°] r
2=0.99106 N=1139
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[280°, 290°] r
2=0.99227 N=1577
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[290°, 300°] r
2=0.99259 N=2029
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[300°, 310°] r
2=0.98793 N=1431
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[310°, 320°] r
2=0.99256 N=906
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[320°, 330°] r
2=0.99086 N=711
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[330°, 340°] r
2=0.99286 N=652
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[340°, 350°] r
2=0.99266 N=538
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
0 5 10 15 20 25 300
5
10
15
20
25
30[350°, 360°] r
2=0.98387 N=430
Wind Speed at 60m height [m/s]
Win
d S
pe
ed
at
80
m h
eig
ht
[m/s
]
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 156 / 173
8.2 Issues related to the site selection process
This section outlines the experience collected during the analysis of many wind measurements that
were taken into account during the section of the test site.
Some of the requirements listed in Table 1 are easy to check. Features like the terrain complexity or the
presence of calibrated anemometers are quickly verifiable. Ownership issues, on the other hand,
required negotiations. The project and its principles were presented to the company owning rights on
the measurements data-set and the owner had to consider the possibility of accepting that the data are
used for the project. Other features are much more difficult to investigate and often required a
preliminary CFD simulation of the wind conditions in order to confirm the flow features recorded by the
measurements.
8.2.1 General Considerations
In very complex terrain, wind measurements pose high demands and it is often difficult to reach the
high standards in all points. Complex terrain often means very difficult accessibility which can pose
problems to the transport of high quality measurement mast equipment. Up in the mountains, weather
conditions can be extreme, which often leads to problems with lightning strokes, low temperature,
icing, rain and snow and severe storms. Power supply for the logger and earthing can be difficult here.
Space for mast erection may be very limited and the anchoring of the guy wires can be difficult. We
observed major problems related to measurement equipment hit by lightning strokes. At specific
locations, this can make a wind measurement almost impossible.
In general, a significant share of wind measurements that we have to assess in the context of wind
resource assessments has major shortcomings regarding the measurement technique. Examples are:
- uncalibrated anemometers;
- anemometer calibration performed by laboratory that doesn’t have any traceable certification;
- lack of a top-mounted anemometer combined with much too short booms;
- mounting of anemometers directly on the boom without any distance tube;
- inappropriate alignment of the booms with respect to main wind directions;
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 157 / 173
- incomplete or missing measurement documentation (regarding erection, operation and
dismantling). In fact, a complete measurement documentation is rarely present;
- inappropriate lightning protection (too close to sensor, diameter too large);
- wind vane mounted on a too short boom;
- top anemometer mounted too close to the mast top;
- wrong or unknown logger configuration.
It is true that most wind measurements shown one or more of these shortcoming. Although the
situation appears to become better with recent measurements we had to exclude those measurements
from the beginning, accepting that this means a major reduction of the sites considered.
8.2.2 Wind Speed Measurement
High quality demands are posed to the wind speed measurements with cup anemometers.
Major problems with wind speed measurements in complex terrain can be related to inclined flow and
turbulence. Different anemometer types tend to respond differently on inclined flow, relating both to
mean, terrain induced inclination and fluctuating inclination attributed to turbulence. Wind tunnel
calibrations refer to steady, laminar flow. On site, however, the wind approaches the sensor also from
above and below, depending on the terrain, the turbulence intensity and the ratio of horizontal to
vertical turbulence. These turbulence conditions can change with position in complex terrain, so it
cannot simply be assumed that the effect is the same at two masts equipped with the same
anemometer type. While the turbulence intensity can be derived from a cup anemometer
measurement, the ratio of horizontal to vertical turbulence would require a sonic anemometer, which
is very rarely used.
The strongest inclination effects are observed if one compares measurements obtained with the Thies
Classic anemometer type with other anemometers. The Thies Classic anemometer measures „more
wind“, compared to a Thies First Class anemometer, because is tends to respond to the magnitude of
the flow vector and not to its horizontal projection.
It is not viable to give to the participants reference data measured with a Thies Classic and compare
calculated wind conditions to those measured with a Thies First Class anemometer, because a large part
of the wind speed difference between the two (up to several percent) must solely be attributed to the
dynamic outdoor behaviour of the anemometers.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 158 / 173
As we do not have systematical studies at hand about the dynamic outdoor behaviour of the NRG
anemometers and because we are not fully convinced of the sensor performance, we had to exclude
those from the test and, as a result, we had to exclude a major part of complex terrain wind
measurements worldwide, in particular in Spain.
Finally, one can of course get direction dependent inclination effects if the mast is not erected strictly
vertically or the sensor is not mounted vertically. It can be difficult to separate that from terrain-
induced flow inclination and other effects.
8.2.3 Spatial Arrangement
Wind measurements in complex terrain are not designed for the purpose of model verification. In
general, the spatial arrangement of many measurements aims at minimising distances between masts
and turbines. Often, single wind measurements are to be used for energy yield calculations only on the
same hill/ridge, as one is aware that the uncertainty of extrapolation from one hill to a nearby hill is
associated with considerably higher uncertainties than the extrapolation on the same hill/ridge. As a
result, the spatial arrangement of measurement masts in complex terrain is seldom satisfactory for
purposes of model verification, where one wishes to have several masts on the same hill/ridge.
8.2.4 Wind Direction Measurements
We know that the wind conditions in complex terrain strongly depend on wind direction, especially if
the site is located on a high, steep ridge. On the other hand, we found that very often there are
problems related to the wind direction measurement. In general, the main focus has been on the wind
speed measurement and the interest in the wind direction measurement has been less intensive. In our
opinion, this is a major shortcoming.
Wind direction errors that we observed, are related to different sources:
It is not always known with a high enough certainty to what direction the north mark of the wind vane
points. Comparisons of wind direction measurements at nearby masts showed in many cases that there
is, on average, a constant wind direction offset between the two. Terrain-induced wind direction
changes, on the other hand, tend to be strongly direction dependent and can not be made responsible
for a constant offset. With only two masts present at a site and the lack of backup wind vanes, there is
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 159 / 173
no way to identify, if there is a problem with the north mark alignment at one of the masts (or even on
both). The offset cannot be corrected.
There are different methods to determine the direction of the north mark. It may be aligned with the
boom and the boom direction may be measured later with a compass or a GPS device some distance
away from the mast, possibly using binoculars. It is possible that this method has major shortcomings in
very complex terrain, where one cannot easily reach any desired point around the mast and the view
can be restricted by topography. For specific cases, this method is not applicable at all due to still
ongoing demining activities in an area of south-east Europe. If the direction of the boom/north mark
has been determined with a compass, one has to transform that direction using the magnetic
declination. This declination is moderate (<10°) in central Europe and can reach considerable values in
other parts of the world. It happens that after the measurement mast has been dismantled, it can be
difficult to identify at all if the north mark direction has been determined with or without application of
the declination. Another problem with wind direction measurements is related to the wind vane type
and its mounting. Although we can not yet prove it, we put forward the hypothesis that in many cases
the wind direction measurement is significantly disturbed by the mast and by possible other equipment
that may be mounted on the same boom than the wind vane. This disturbance is caused by flow
direction changes that are induced by the pressure field developing around the mast. While it is clear
that the wind vane is exposed to higher direction fluctuations in the wake of the mast, we suppose that
especially at inflow angles around 45° /135° to the vane boom there are systematical, direction
dependent errors in the wind direction measurement.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 160 / 173
Figure 94: Sketch of the flow around a mast to illustrate our hypothesis of an influence that the mast can have on the
wind direction measurement. In this case the measured wind direction is turned by a few degrees clockwise with
respect to the ambient undisturbed mean wind. The effect should be the more pronounced the smaller the ratio of
boom length to mast diameter is and it should have its maximum if the flow is at about 45°/135° to the boom.
In practice, we sometimes found it impossible to decide if a particular wind direction effect observed
between two mast must be attributed to the terrain or to such a small-scale dynamic effect.
Unfortunately, this was the case for the most interesting site that was initially considered for the test
(see Figure 95). For another site, there was a strange wind direction effect which could not be
explained at all (see Figure 96).
We decided to exclude those sites, because we were, in the given frame, not able to state for sure if it
was a terrain induced wind direction effect or an effect that is caused by the mast itself.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 161 / 173
8.2.5 Exemplary illustrations of some problematic effects found during site search
In this section a number of images with explanations are collected that shall give a representative
overview of the problematic effects that we observed during our site selection work. All sites are
anonymous. Also, it is not specified, what companies were operating these measurements.
We show only the scatter plots and not the quantitative, bin-averaged results, because the images shall
only illustrate the problems that we faced during our work. For this purpose, we find it more useful to
display the data itself and not only average values.
One must keep in mind that all measurements described below do perfectly conform to current IEC and
IEA standards. All anemometers are calibrated according to MEASNET standard.
Figure 95: Site XX1: Wind direction scatter plot for two nearby met masts in very complex terrain. Wind directions are
centred around north (so e.g. –30° corresponds to 330°). There is a direction independent offset and a direction
dependent offset for wind from NW. Note that if this would be an effect from the mast, it should basically be
symmetric around the boom direction. In this case however, the vane booms at the two masts are aligned to
different directions.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 162 / 173
Figure 96: Site XX2: Wind direction scatter plots for two nearby met masts in very complex terrain. Wind directions
are centred around north (so e.g. –30° corresponds to 330°). There is a strange behaviour for wind for NNE. Above: All
wind speeds, below: Wind speed at ref1 between 4 m/s and 8 m/s. Note that both vanes are potentiometric wind
vanes and that the „singularity“ can not be attributed to a possible averaging problem related to the „north-jump“.
The terrain to the NNE of the masts is of only moderate complexity.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 163 / 173
Figure 97: Site XX3: Wind direction scatter plot for two nearby met masts in moderately flat terrain. There is a
direction dependent offset that reaches its maximum for wind directions of about 120°. We did not have a
satisfactory explanation for this behaviour.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 164 / 173
Figure 98: Site XX4: Wind direction scatter plot for two nearby met masts in complex terrain. There is a direction
independent offset.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 165 / 173
Figure 99: Site XX5 and XX6: Scatter plots of the ratio of wind speed measured with a top-mounted anemometer to
that measured with a backup anemometer vs. wind direction. The top anemometers are of type Risoe, the backups
are of type Vector. The measurement installations fully conform to IEC and IEA standards. The backup anemometer is
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 166 / 173
mounted on a boom pointing to 260° (above) and 251° (below), lightning protection of the top anemometer is at 80°
(above and below). No other disturbances of the sensors are expected. Vertical distance between top and backup
anemometer rotor planes is 3.3 m. A direction dependent effect in the image above, most visible from 160° to 300°, is
not easily explained. Also, the comparably large mean difference between top and backup in the image below is
difficult to explain.
8.2.6 Maps
Other, major problems are related to geographic issues.
More often than one would expect, the situation regarding high quality, high resolution up-to-date
topographical maps is not satisfactory. An example is the area of Turkey. There were extensive high
quality wind measurement campaigns in complex terrain in this area and we initially spent much time
to assess those we had access to. However, finally we were not able to obtain topographical maps of a
high enough standard. The reason is mainly the role that the military plays in the management of
geographic information in this area. High resolution up-to-date topographic data was not readily
available to us. The topographical information plays an important role in the test. It is a matter of fact
that one can in many cases have topographical information of higher and higher quality, depending on
how much money one is able to spend. We decided that it is reasonably if we demand that the quality
of the maps should be comparable to what is commonly used in wind resource assessment work in
central Europe (up-to-date topographical maps in the scale 1:25000 or 1:5000, possibly supplemented
by aerial photos, for large distances from the site possibly completed by SRTM data). For the site and
the area of several km around it we consider SRTM data as having a much too high uncertainty.
8.2.7 Forest
Modelling effects of forest on the wind flow is a major challenge by itself. Although there are „forest
models“ that can be attached to the flow models, we decided to exclude forest effects from the test as
far as possible. The difficulties of forest modelling are manifold: First of all, one has to quantify exactly
what is meant with „forest“, i.e. its height, type, density and extent has to be assessed. This information
is not readily available. Secondly, forest tends to grow. There are trees, as the very common eucalyptus
trees on the Iberian Peninsula, that can grow by a significant amount even during a measurement
campaign so that one would have to consider that in some way. Such fast growing trees also tend to be
subject to extensive felling activities, making it difficult to exactly specify the extent at all times. Lastly,
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 167 / 173
the flow structures that develop in the lee of a forest boundary have a smaller spatial scale than the
remaining flow. In the luv of a forest boundary there may be flow retardation. The modelling of those
flow features poses its own demands (grid refinement, turbulence model or empirical correction) and
has a different uncertainty attached to it. We do not want to mix model uncertainties caused by
incorrect modelling of complex terrain flow and by forest modelling. We excluded sites where there is
significant forest close to one of the measurement masts.
8.2.8 Coordinates
Today, mast coordinates are taken by GPS, which has an acceptable accuracy if properly used. The
number of satellites found by the device can be restricted by topography, leading to a higher
uncertainty of the position measurement. Sometimes GPS coordinates can be immediately verified on
site as being wrong, for some unknown reason. Also, in many cases the mast coordinates are not
recorded in the coordinate system of the map for that area. Specifically, GPS coordinates are often
recorded in geographical coordinates with a WGS84 reference frame. Topographical maps can have a
number of different coordinate systems, which are sometimes not obvious (e.g. for the area of Bosnia
and Herzegovina). For simplicity, we decided to supply all maps and coordinates in the UTM WGS84
system. Therefore, maps and coordinates have to be reprojected to that system. Specifically, paper
maps have to be scanned, georeferenced, reprojected and vectorized. This has to be done with great
care in complex terrain and can take considerable time. Having done all that, one may nevertheless
finally find that the position of the mast in the projected map does not fully conform to the visual
impression that one has gained on site. If one can confirm the correctness of the GPS measurement and
the map and projection work, one is left with the statement that the topographical map is not accurate
for that area. In those cases did we have to exclude the site from the test.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 168 / 173
8.2.9 Data from Numerical Site Calibrations
If power curves of wind turbines shall be measured according to IEC standard and the terrain on site is
„too complex“ according to IEC specifications, a measured site calibration must be carried out before
the turbine is erected. For that, a wind measurement at the planned turbine position at hub height is
installed (WTGS mast). Additionally, a wind measurement is installed at hub height at the position of
the mast that shall later be used for the power curve measurement. Both measurements are operated
until enough data in the expected power curve measurement sector is collected.
These site calibrations have to follow very high and restrictive standards and therefore give highly exact
results. Accordingly, those measurements are excellent candidates for Round Robin test sites. DEWI has
carried out a large number of those site calibrations.
This is the theory.
In reality, those measurements are not that easily accomodated in the test, due to the following
reasons:
- At the WTGS mast, that is erected at the later turbine position, there is no requirement for a wind
direction measurement and in most cases there isn’t one. If we would give to the participants the
wind speed and direction data of the reference mast and let them calculate for the site mast, we
could only compare the wind speed results and not the accuracy with which the models can model
the wind direction changes in complex terrain. For any direction dependent assessment of site mast
predictions, one would have to assume no change between reference and site mast. Looking at the
usually small distances between reference and site mast, this is a reasonable assumption, but it is
difficult to quantify the uncertainty of such an assumption.
- The site calibration and the power curve measurement is often restricted to only a small wind
direction sector, sometimes down to 30° or so. We would have to restrict the assessment to that
sector also. This restriction does however lower the practical relevance of the assessment, as the
real wind is not restricted to the measurement sector.
- The distance between the WTGS mast and the power curve measurement mast has to be
inbetween 2 and 4 rotor diameters, 2.5 rotor diameters is the recommended distance. This distance
does not correspond to typical distances for extrapolation of mast measurements to turbine
positions in wind resource assessments, except for single turbines in a farm.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 169 / 173
- Site calibrations are operated until the number of data in specified classes exceed defined limits. In
practice, site calibrations are usually operated for comparably short periods that are much shorter
than one year (in most cases site calibrations are in operation for 2 up to 3 months. Due to possible
seasonal effects it is however desirable to have about one year of data for the test.
- If there is more than one site calibration in operation in the same area, one may consider to use
their combined data for the test, i.e. give to the participants data from one reference mast and let
them calculate for the other reference mast, possibly by discarding the site masts. But this is not
easily done, as the measurements are in general designed such that data is only used from within
the measurement sectors. For other directions there may be disturbances due to sensors, lightning
protection or obstacles like other wind turbines, trees, houses, forest, or similar. The test needs
however to be restricted to a measurement sector that is common to all site calibrations installed.
Such a common sector can be even smaller than the already narrow measurement sectors, if a
common sector is found at all. Additionally, the spatial distribution of different site calibrations in
an area does not necessarily represent typical locations of met masts and wind turbines in a
complex terrain wind farm project, i.e. the spatial arrangement can be quite unrealistic. The reason
is that site calibrations tend to be operated at the outer boundary of wind farms in order to get rid
of the turbine wakes in the measurement sectors.
- By definition, site calibration measurements have to be done exclusively at hub height. There are
recent developments regarding the additional use of wind speed measurements at the height of
the lower blade tip. As a result, these measurements give in general no reference for a test
regarding the model‘s performance on vertical extrapolation. Wind measurements for the purpose
of energy yield assessment studies do rarely reach hub height, although this has changed a bit now.
So the accuracy with which the models can extrapolate vertically should be part of the test.
- In order to separate model uncertainty from measurement uncertainty, one wishes to have site
calibration factors as different from 1 as possible. There are ongoing site calibrations at extreme
sites. There measured site calibration factors can well exceed 110%. But along with increasing
factors also the scatter in the data increases and the meaning of an average factor is weakened.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 170 / 173
8.3 Output data Format
The present section contains information about the data format of the results delivered to DEWI.
8.3.1 Mean Horizontal Wind Speed for terrain following surfaces - Data Format
TAB-separated ASCII file with one grid point in each line.
Format for each line (all coordinates in UTM WGS 84 Zone 32):
East-Coordinate North-Coordinate Mean Wind Speed [m/s].
- No leading space characters allowed at the beginning of the line.
- The new-line-characters must be „CR LF“ or 0D 0A (Hexadecimal).
- Floating point numbers for the wind speed.
- No header lines allowed.
Ordering of the lines starts with the minimum east and north coordinates. The north coordinate
increases first and the east coordinate remain fixed. When the north boundary is reached, the north
coordinate resets, the east coordinate increases and so on. The values were saved in the ASCII files:
XYZ.mean40.dat, XYZ.mean60.dat, XYZ.mean80.dat where XYZ is the participant-id string which has
been assigned before the start of the Dummy-Run. (es. ANM.mean60.dat)
8.3.2 Mean Wind Speed for target locations - Data Format
TAB-separated ASCII file with one grid point in each line. Format for each line:
Point-ID East-Coordinate North-Coordinate Mean Wind Speed [m/s]
- No leading space characters allowed at the beginning of the line.
- The new-line-characters must be „CR LF“ or 0D 0A (Hexadecimal).
- Floating point numbers for the wind speed.
- No header lines allowed.
The values were saved in the ASCII files:
XYZ.points40.dat, XYZ.points60.dat, XYZ.points80.dat
where XYZ is the participant-id string which has been assigned before the start of the Dummy-Run. Es.
ANM.points40.dat
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 171 / 173
8.3.3 Wind Statistics for target locations - Data Format
This wind statistic must be provided in the common WAsP „.tab” data format with 24 wind direction
sectors of 15° width each and wind speed intervals of 1 m/s each.
The data format for this statistics is described in the European Wind Atlas and Application Program web
page: http://www.risoe.dk/vea/projects/nimo/WAsPHelp/FileFormatofTAB.htm
The specification of the coordinates and the height of the location in the tab file were not required and
they had been not be taken into account in the evaluation. Nevertheless, in order avoid any confusion
and to create tab-files conform to the WAsP program, the participant were asked to assign longitude
and latitude equal to 1. Values were saved in the tab files: XYZ.point-id.tab
where XYZ is the participant-id string which has been assigned to each participant before the start of
the Dummy-Run and point-id is the identification string relative to each point.
Additionally the participant were asked to provide 24 separate statistics. The format for these statistics
was the same as requested for the whole time-series. Since it was probable that for these statistics only
few wind sectors contain data, the participant were requested to define empty sectors by setting to 0
the sector-wise frequency of occurrence for those empty sectors (in line 4 of the Tab file) and, for the
empty sectors, to set to 1000 the frequency of the wind speed interval ranging from 0 m/s to 1 m/s.
The remaining frequencies in the empty sector should be set to zero as in the example in Table 12.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 172 / 173
No Description |
1.00 1.00 1.0
12 1.00 0.00
7.89 0.98 0.71 0.00 2.72 8.93 11.73 9.09 4.81 1.90 3.59 47.65
1.00 10.77 111.11 83.48 1000.00 34.44 9.95 5.58 8.42 17.46 55.81 27.17 1.99
2.00 96.21 368.69 283.48 0.00 162.21 77.11 46.19 46.05 62.13 186.89 144.77 18.96
3.00 168.01 291.67 286.96 0.00 261.89 179.24 77.54 39.26 81.64 204.41 148.56 38.55
4.00 136.24 131.31 160.00 0.00 222.02 216.69 90.06 53.38 100.13 158.34 144.09 48.66
5.00 123.32 54.29 128.70 0.00 122.79 200.66 83.32 82.45 116.56 134.33 105.91 63.47
6.00 115.42 12.63 46.96 0.00 80.65 122.31 100.58 93.59 121.44 110.97 90.78 73.55
7.00 108.96 12.63 10.43 0.00 71.14 77.11 117.20 107.44 143.52 76.57 65.34 72.80
8.00 82.39 13.89 0.00 0.00 29.00 39.66 114.26 119.80 120.92 37.64 57.43 68.68
9.00 47.03 3.79 0.00 0.00 15.86 25.43 93.00 128.50 91.40 13.63 37.48 72.44
10.00 20.10 0.00 0.00 0.00 0.00 16.03 89.85 95.08 54.17 5.84 22.70 71.40
11.00 30.52 0.00 0.00 0.00 0.00 8.02 67.23 90.19 41.34 5.19 25.10 67.96
12.00 13.82 0.00 0.00 0.00 0.00 7.05 53.66 63.71 29.78 9.09 18.57 67.80
13.00 14.18 0.00 0.00 0.00 0.00 4.84 22.20 40.34 13.09 0.00 17.88 60.24
14.00 15.44 0.00 0.00 0.00 0.00 5.11 14.31 19.56 4.36 1.30 13.07 52.75
15.00 7.36 0.00 0.00 0.00 0.00 5.80 9.89 8.15 0.51 0.00 11.00 43.55
16.00 3.41 0.00 0.00 0.00 0.00 3.04 8.94 2.58 1.03 0.00 13.07 38.47
17.00 2.33 0.00 0.00 0.00 0.00 1.38 3.58 1.36 0.00 0.00 9.97 30.88
18.00 2.33 0.00 0.00 0.00 0.00 0.28 2.31 0.00 0.00 0.00 7.91 23.78
19.00 0.36 0.00 0.00 0.00 0.00 0.00 0.32 0.14 0.00 0.00 13.76 22.28
20.00 0.18 0.00 0.00 0.00 0.00 0.28 0.00 0.00 0.51 0.00 11.69 15.88
21.00 1.26 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 7.22 11.79
22.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 5.85 10.23
23.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.34 7.49
24.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.34 3.39
25.00 0.36 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 4.12
26.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 3.11
27.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 1.76
28.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 1.45
29.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.98
30.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.57
31.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.41
32.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.21
33.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.10
34.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.26
35.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00
Table 12: Example TAB file with the 4th
sector empty.
Round Robin Numerical Flow Simulation in Wind Energy
DEWI GmbH - Partial Reproduction not Permitted 173 / 173
9 References
[1] Troen, E.L. Petersen: European Wind Atlas. Risø National Laboratory, Roskilde, Denmark, 1990.
[2] G. Mortensen, L. Landberg, I. Troen, E.L. Petersen: Wind Atlas Analysis and Application Program
(WASP), Risø National Laboratory, Roskilde, Denmark, 1993 and updates.
[3] MEASNET: Power Performance Measurement Procedure, 3rd Ed., November 2000.
[4] IEA: IEA Recommendation 11: Wind Speed Measurement and Use of Cup Anemometry, 1st Ed.,
1999.
[5] International Electrotechnical Commission (IEC): IEC61400-12-1 Wind turbines - Part 12-1: Power
performance measurements of electricity producing wind turbines, 1st ed., 12/2005.
[6] A. Albers, H. Klug, D. Westermann: Outdoor comparison of cup anemometers, proceedings of
DEWEK 2000, DEWI, Wilhelmshaven.
[7] A. Albers, H. Klug: Open Field Cup Anemometry, Proceedings of European Wind Energy Conference
2001, Kopenhagen, Denmark.
[8] IEC: IEC61400-1 Wind turbine generator systems - Part 1: Safety Requirements, 2nd Ed., 1998.
[9] IEC: IEC61400-1 Wind turbines - Part 1: Design Requirements, 3rd Ed. 08/2005.