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DESIGN AND POWER CHARACTERIZATION OF A SMALL WIND TURBINE MODEL IN PARTIAL LOAD
REGION
by
Abdulkarim Abdulrazek
A thesis submitted in partial fulfillment of the requirements for the degree of
Master of Science in Engineering Renewable Energy and Energy Efficiency for the MENA
Region (REMENA)
University of Kassel and Cairo University
Feb 2012
Supervised by: Prof. Dr. sc. techn. Dirk Dahlhaus, Faculty of Electrical Engineering/Computer Science, University of Kassel. Prof. Dr. Joachim Peinke, Faculty of Physics, Carl von Ossietzky University Oldenburg. Dr. Michael Hölling, Faculty of Physics, Carl von Ossietzky University Oldenburg. Dr. Basman El-Hadidi, Aerospace Engineering, Cairo University.
i
ABSTRACT
In this thesis a small wind turbine model was constructed with variable speed and pitch
control in order to investigate the effect of this control strategy on wind turbines by
characterizing its design and output power.
The small wind turbine model components were mentioned with specifications and
functions in addition to description of the LabView program.
The model was experimented in the wind tunnel exists in Oldenburg University where a
testing procedure was followed. The procedure included the way how to measure the
output voltages and currents from the generator at different wind speeds and how wiring
should be connected.
This fruitful work resulted in drawing the power and c – λ curves. Discussions of the
obtained results were made and several factors were listed. These factors, such as friction,
affected the model’s performance. These discoveries helped in proposing useful
modifications for the system in order to enhance it.
ii
TABLE OF CONTENT
Abstract .............................................................................................................................. i
Table of Content ................................................................................................................ ii
List of Figures ................................................................................................................... iv
List of Tables ...................................................................................................................... v
Acknowledgement ........................................................................................................... vi
Nomenclature ................................................................................................................. vii
Introduction ...................................................................................................................... 1
Basic Theory ...................................................................................................................... 5
Design and Setup............................................................................................................... 8
Rotor .............................................................................................................................. 9
Blades ............................................................................................................................ 9
Generator .................................................................................................................... 10
Stepper Motor ............................................................................................................. 11
Blade Pitch Mechanism ............................................................................................... 12
Main Circuit ................................................................................................................. 14
Connections ............................................................................................................. 15
Shunt Resistor ......................................................................................................... 15
Variable resistor ...................................................................................................... 15
Analog to Digital Converter (ADC) ........................................................................... 16
LABVIEW program ................................................................................................... 16
General Specifications ................................................................................................. 17
Experimental Setup ..................................................................................................... 19
Characterization .............................................................................................................. 21
Procedure .................................................................................................................... 21
Optimum Pitch Angle .................................................................................................. 25
Power Curve ................................................................................................................ 27
Cp – λ curve ................................................................................................................. 28
Limitation Factors ........................................................................................................ 30
Friction .................................................................................................................... 30
Small Modifications ................................................................................................. 31
Generator Losses ..................................................................................................... 31
iii
Manufacturing and Installation of blades ............................................................... 32
Angle of Attack (AoA) .............................................................................................. 32
Conclusion and Future Improvement ............................................................................. 36
Future Improvements ................................................................................................. 36
Appendix A ...................................................................................................................... 38
Power coefficient and resistance at different wind speeds ........................................ 38
Power coefficient and pitch angle at different wind speeds ...................................... 39
Appendix B ...................................................................................................................... 40
Appendix C ...................................................................................................................... 41
Voltage Divider Circuit ................................................................................................ 41
Design Formulas .......................................................................................................... 41
Bibliography .................................................................................................................... 42
iv
LIST OF FIGURES
Figure 1.1- Total installed capacity of wind energy worldwide from 2000 to 2011* in
megawatts [1] ................................................................................................................... 1
Figure 1.2- Number of jobs in the wind energy industry worldwide from 2005 to 2012
[4] ...................................................................................................................................... 2
Figure 2.1- Power coefficient for different wind turbine types [25] ................................. 5
Figure 2.2- Ideal Power Curve ........................................................................................... 7
Figure 3.1- Small wind turbine model's assembly ............................................................. 8
Figure 3.2- Blade dimension .............................................................................................. 9
Figure 3.3- Stepper Motor Driver .................................................................................... 12
Figure 3.4- Pitch mechanism components ...................................................................... 13
Figure 3.5- Blade pitch control mechanism .................................................................... 13
Figure 3.6- Blade pitch angle position ............................................................................. 14
Figure 3.7- Tailoring the blade ........................................................................................ 14
Figure 3.8- Variable Resistor ........................................................................................... 16
Figure 3.9- The small wind turbine model ...................................................................... 17
Figure 3.10- Wind tunnel test section with wind turbine model .................................... 19
Figure 3.11- Connection Diagram ................................................................................... 20
Figure 4.1- The relation between power coefficient, pitch angle and resistance .......... 24
Figure 4.2- 9m/s contour plot shows the location of sections ....................................... 25
Figure 4.3- Section A-A .................................................................................................... 26
Figure 4.4- Section B-B .................................................................................................... 26
Figure 4.5- Power Curve .................................................................................................. 27
Figure 4.6- The rotational frequency (ω) varies with the resistor .................................. 28
Figure 4.7- Cp – λ Curve .................................................................................................. 29
Figure 4.8- The relation between V-ω on the left hand side and I-ω on the right hand
side .................................................................................................................................. 29
Figure 4.9- Contour plot for wind speeds 4 and 5 m/s ................................................... 30
Figure 4.10- Cp – λ Curve, comparison between 1st and 2nd setups ............................. 31
Figure 4.11- Cp- AoA curve at the tip of the blade ......................................................... 32
Figure 4.12- Cp- AoA curve at the base of the blade ...................................................... 33
Figure 4.13- Cp- AoA curve at the middle of the blade ................................................... 33
Figure 4.14- Velocity Triangle acting on airfoil ............................................................... 34
Figure 4.15- AoA and Blade Length for the current and proposed blades ..................... 35
Figure A.1- Power coefficient and resistor at different wind speeds ............................. 38
Figure A.2- Power coefficient and pitch angle at different wind speeds ........................ 39
Figure B.1- LabView Front Panel ..................................................................................... 40
Figure C.1- Voltage divider circuit ................................................................................... 41
v
LIST OF TABLES
Table 3.1- Generator Specification [16] .......................................................................... 10
Table 3.2- Generator's Encoder Specification [17] ......................................................... 10
Table 3.3- Stepper Motor Specification [18] ................................................................... 11
Table 3.4- Stepper Motor's Encoder Specification [19] .................................................. 11
Table 3.5- Driver Specification [20] ................................................................................. 11
Table 3.6- Small Wind Turbine Model General Specification ......................................... 18
Table 4.1- Operation methodology at 9m/s ................................................................... 21
Table 4.2- Operation methodology at 4m/s ................................................................... 22
Table 4.3- Results Template ............................................................................................ 22
Table 4.4- Cp max at different wind speeds.................................................................... 26
vi
ACKNOWLEDGEMENT
The author wishes to express sincere appreciation to Prof. Dr. Joachim Peinke to give him
the chance to be here in wonderful team work environment and his supervisor Doctor
Michael Hölling for his fruitful assistance and main support in the accomplishing this thesis
and building up his knowledge in wind energy. In addition, special thanks to Engineer
Agnieszka Parniak who was the active and prime mover of the project in the design and
construction processes. Thanks also to the members of ForWind for their valuable input.
Moreover, he would like to thank Dr. Basman El-Hadidi for his support and guide and to
Prof. Dr. Dirk Dahlhaus on his efforts to sustain his master program.
Furthermore, the author wishes the best and very special thanks for his parents and
brothers to give him the chance and support to be here in Germany doing his master thesis
and improving his educational and career levels. He also thanks his colleagues in the master
program for the joyful time that he spent with them especially for Engineer Rana Hanfy
and Engineer Fadi Abdulhadi who was his dynamic partner in this project and big
supportive.
vii
NOMENCLATURE
Abbreviations
NI National Instruments
ADC Analog to Digital Converter
VS-VP Variable Speed Variable Pitch
VS- FP Variable Speed Fixed Pitch
FS- VP Fixed Speed Variable Pitch
FS- FP Fixed Speed Fixed Pitch
GDP Growth Domestic Product
PWM Pulse Width Modulated
Symbols
ur Rotational Speed in m/s
ures Resultant Wind Speed in m/s
u1 Incoming Wind Speed in m/s
u2 Wind Velocity at rotor plane in m/s
Greek Letters
ρ Air Density
α Angle of Attack
β Angle of Relative Wind
γ Pitch Angle
Ω Ohms
λ Tip Speed Ratio
ω Rotational Frequency
1
CHAPTER 1
INTRODUCTION
The wind energy market worldwide has grown in hasty ascending manner where
Figure 1.1 shows in 2011 the installed capacity of 236GW was reached, with an
annual average growth of 1.2% [1].
This wind energy share was supported with legislations and governmental
encouragements illustrated by emphasizes on implementing their mandatory targets
by 2020 which boosted investments towards wind energy production.
Several countries approved plans to reach certain targets in the wind energy share in
2020. As an example: Egypt plans to reach 12% of its electricity production from
wind, China is building two wind turbines every one hour and expects to install
230GW by 2020 [2], Brazil announced 1,100 MW of wind energy [3] and EU has a
target of 14% of Europe’s total electricity production from wind energy [4], etc.
These plans ensure huge job opportunities for thousands of employees in wind
energy industry as illustrated in Figure 1.2.
Figure 1.1- Total installed capacity of wind energy worldwide from 2000 to 2011* in megawatts [1]
2
However, the governmental strategic plans were not only dedicated for installing wind
turbines but also in the increase of research and development investments. In
Europe, the research and development (R&D) share for wind energy will reach 3% of
its growth domestic product (GDP) in 2020 [5]. This indicates the importance of
R&D in wind energy sector.
Although the share of investment in wind energy research is increasing, researchers
are facing many constrains that limit wind energy development. Finance is considered
one of the important constrains in wind energy development which wind turbines
installation cost between 900€/kW to 1150€/kW [6]. Moreover, the installation of
such wind turbines in atmospheric conditions produces difficulties in defining the
boundary conditions of incoming flow caused by the nonexistence of precise sensors
that can define these conditions and adding weather and operational conditions.
Despite these constrains, scientists and researchers seek for better research
environment to accomplish their research. The existence of laboratories that can
generate realistic conditions by providing wind tunnel, active and passive grid,
sensors, etc. helped in improving the wind energy field. A small wind turbine models
were constructed and tested in the wind tunnel in a controllable incoming air flow
conditions for research purposes.
Figure 1.2- Number of jobs in the wind energy industry worldwide from 2005 to 2012 [4]
3
The ongoing wind tunnel experiments focus on load characterization for small wind
turbines which shows their performance and specifies the operating conditions.
Likewise, the research group of John Hopkins University in the United States has
built a small wind turbine with 12cm rotor diameter [7]. It focused on measuring the
extracted mechanical power rather than the electrical output power due to losses in
the generator. Although it was a fruitful study, they did not focus on the quality of
their blades and thus ignoring the efficient usage of aerodynamic forces.
Another study was done to examine the effect of turbulence in wake of small wind
turbine models [8]. The purpose of this experiment is to improve understanding of
transport momentum and kinetic energy of boundary layer with wind turbines. The
used models had a rotor diameter of 12cm with low blade quality without control
systems like pitch or load control.
The department of Aerospace Engineering at the Iowa State University in United
States of America carried out another experiment exploring the effect of dynamic
loads and evolution of turbulent flow in the wake of wind turbines [9]. They had a
3bladed- rotor of 254mm in diameter and a hub height of 225mm.
In Germany, Technische Universität Berlin has developed a small wind turbine of
70cm in diameter with load and pitch control [10]. The pitch control is done manually
in order to adjust the angle of attack and the load control by the means of variable
resistor. Also, they took extra attention to produce a well designed blade.
All the laboratories experiments on small wind turbine models do not account all
factors that help increasing the extracted power from wind, such as pitch control, yaw
control, etc.
As an initiative and to be one of the pioneers in providing new techniques in wind
energy research, a small wind turbine model with pitch and variable load controls
which are known as variable pitch and variable speed control strategy (VS-VP) was
constructed. This project considered to be unique of its kind in small sizes of 50cm
rotor diameter. It opens opportunities to study, characterize, and investigate, etc. in
more advanced and realistic manners what occurs to real wind turbines.
4
This project focuses on “Design and Power Characterization of a Small Wind
Turbine Model in Partial Load Region” and “Design and Characterization of a Small
Wind Turbine Model equipped with a Pitching System” [11]. This part of the project
covers the design and output power characterization of this model. Through the
thesis, the design phase of wind turbine components will be discussed. The
experimental setup will be mentioned and then interpreting the results.
5
CHAPTER 2
BASIC THEORY
The major theoretical principles to which any wind turbine is restricted are the main
task of this chapter.
The role of wind turbines is to extract energy from wind and convert it to electrical
energy. This extraction is subjected to certain limitations represented by Betz’s limit
which is the maximum energy possible to convert kinetic energy into mechanical
energy without any losses [12]. An ideal wind turbine has a maximum power
coefficient (,) of 16/27. The theoretical limit cannot be exceeded and this
caused by the aerodynamic losses due to conversion of angular momentum, tip and
drag [12]. It is clear in Figure 2.1, that the power coefficients of all wind turbine types
are located under the theoretical power coefficient.
Figure 2.1- Power coefficient for different wind turbine types [25]
6
Accordingly, the power extracted from wind can be expressed as follows:
1
2
(2.1)
where:
ρ = density of air in kg/m3,
A = rotor swept area in m2 = πR,
u = incoming wind speed in m/s,
c !" = maximum power coefficient.
The extracted power is then converted to electrical power defined as:
#$
(2.2)
where:
P = electrical power in W,
V = voltage in V,
I = current in A.
This power can be drawn at different wind speeds as shown in Figure 2.2. This curve
is called the ideal power curve which is divided into two zones. In the first zone, the
partial load zone, the maximum power coefficient (c !" ) is tracked by controlling
the rotational frequency of the generator at fixed optimum blade pitch angle. In
theory, c !" should be constant at different wind speeds [12]. So, the purpose of
controlling the rotational frequency is to maintain a constant (c !" ). The second
zone, the power control zone, used to keep the rated power constant by altering the
pitch angle. The reason for this, is to protect the generator from exceeding its rated
power and thus from failure. This control strategy is called variable speed- variable
pitch (VS-VP).
7
The speed control in the partial load zone might attempt to maintain a constant tip
speed ratio (λ) and thus maximum power coefficient at different wind speeds [12].
The tip speed ratio is defined as the relation between rotational frequency (ω) of the
rotor at the tip and the incoming wind velocity:
% &'
(2.3)
where:
% = tip speed ratio,
& = rotational frequency in rd/s,
' = blade radius in m,
= incoming wind speed in m/s.
To achieve the control goal, the generator’s power output is connected to a variable
resistive load that controls ω and thus tries to keep λ constant. The change in variable
resistor causes changes for the current in the generator and thus in the torque which
is proportional to the current. If the current increases the torque (T) in the generator
will increase causing the rotor to slow down. Otherwise, the rotor speed will increase.
Therefore, the control system should track the optimum values of both variables T
and ω to obtain c !" by the means of variable resistor.
Figure 2.2- Ideal Power Curve
8
CHAPTER 3
DESIGN AND SETUP
The mentioned components in this section were designed, including force analysis
and CAD drawings, and manufactured in the workshop at the University of
Oldenburg. Additional standard components from various suppliers were used.
Moreover, the components of the model declaring its function and specification were
mentioned. Figure 3.1 shows the model’s components assembly.
SLIDER LINKS COUPLING
GENERATOR
BLADE
CONNECTOR
STEPPER MOTOR
MAIN SHAFT
Figure 3.1- Small wind turbine model's assembly
9
Rotor
The rotor of 0.577m in diameter is considered an important part of the wind turbine
where the extracted power from wind is converted into mechanical power in terms of
torque (T) and rotational frequency (ω).
Blades
The small wind turbine is a three bladed system. It is 0.25m length and 0.032m chord
at base, see Figure 3.2.
The length was chosen according to the dimensions of the available wind tunnel with
outlet area of 1x0.8 m2. The blades are manufactured by a rapid prototyping machine
and designed in according to MEXICO project [13] with a change in the airfoil
profile near the base. The blades are made of Resin type VeroBlue, an acrylic-based
photopolymer, which is classified as one of the plastic families [14].
The purpose of using plastic is its ability to be easily formed, shaped, casted and
pressed. However, VeroBlue is durable and degrades very slowly as all kinds of
plastics. Another reason for using plastic is its suitability of being used for the
prototyping process [15]. Rigidity is the main property of VeroBlue which makes it
resistible to applied forces.
Figure 3.2- Blade dimension
0.2m
10
Generator
The wind turbine generator was selected according to few conditions. These
conditions included the design rated wind speed and of values 12m/s and 0.4
respectively. The assumption of was based on rule of thumb. Since the model
is not an ideal wind turbine, should be lower than Betz limit. In addition, the
model is subjected to losses, due to tip and drag, and to friction in the generator and
other components. Thus, the value of was considered accordingly. Inserting
these values in the extracted power formula at rated wind speed,
1
2
(1.1)
where the air density (ρ) is 1.225 kg/m3 and the rotor swept area (A) is 0.26 m2, the
obtained rated power of 110W. Despite of this calculation and assumption, a
generator with maximum power output of 217W was chosen in order to prepare the
turbine for future experiments with different components.
The generator is a DC- micromotor [16] that has the following specifications:
Manufacturer FAULHABER Type 3863H048CR
Nominal Voltage 48 V Maximum Output Power 217 W
Maximum Rotational Speed 8000 rpm Table 3.1- Generator Specification [16]
The generator is provided with an encoder that converts the generator’s rotational
frequency to a digital format. The encoder is of type IE2 – 1024, [17]. Further
specifications are given in Table 3.2.
Manufacturer FAULHABER Type IE2 – 1024
Supply Voltage 4.5...5.5 V DC Lines per Revolution 1024
Table 3.2- Generator's Encoder Specification [17]
Generally, the encoder has different functions but it was used as an indicator for the
rotational frequency.
11
Stepper Motor
The stepper motor is used for driving the pitching mechanism. It was selected based
on moment analysis, see [11]. The stepper motor was bought from FAULHABER
with electronic driver and an encoder. The specifications of these products are
shown in the tables below:
Manufacturer FAULHABER Type AM2224-R3-AV-4.8
Nominal Voltage 3 V DC Steps per Revolution 24
Step Angle 15° Holding Torque 22mNm
Table 3.3- Stepper Motor Specification [18]
Manufacturer FAULHABER Type PE22-120
Supply Voltage 4.5...5.5 V DC Lines per Revolution 120
Table 3.4- Stepper Motor's Encoder Specification [19]
Manufacturer FAULHABER Type ADCMM1S
Power Supply Voltage Min. 10 V DC Max. 28 V DC
Table 3.5- Driver Specification [20]
The stepper motor has 24 steps per revolution where each full step corresponds to
15º step angle.
Likewise, the encoder is a FAULHABER product used not only for indication and
control of direction and rotational velocity, but also positioning. Thus, these acts are
applied to tailor the blade pitch angle.
The electronic driver has two tasks, first it supplies the stepper motor with power and
secondly it receives commands from the control system.
12
It is a basic driver which requires clock and direction signals [21]. The clock is needed
to generate pulse-width modulated (PWM) signals for driving the motor and
controlling its rotational frequency. The direction signal sets the direction of rotation,
i.e. clockwise or counter-clockwise.
As recommended from manufacturers catalogue [21 p. 7], the current was set at
position switch A and 12 V was supplied for energizing the poles [11].
Blade Pitch Mechanism
The blade pitch mechanism is used to change the blade pitch angle either in partial
load zone or in power control zone. This mechanism consists of a slider, links and
connectors. It is connected to the stepper motor on one side, which again is fixed to a
threaded rail to maintain a linear motion. The slider moves on the main shaft
forwards and backwards by the means of the stepper motor. The other side of the
mechanism holds the blades. Figure 3.4 shows the assembly of these components.
Figure 3.3- Stepper Motor Driver
13
Its only function is transferring the linear motion from the stepper motor to
rotational motion in the blades. When the motor rotates by 24 steps, the slider moves
forwards or backwards by 0.5mm causes a change in blade position. This is observed
in Figure 3.5 where the blade moves from position 1 to position 2 by moving the
slider.
Figure 3.5- Blade pitch control mechanism
Figure 3.4- Pitch mechanism components
1 2
14
Since the system is limited to a certain distance [11], the blades were fixed at a blade
pitch angle of 20° from the axis of rotation with the naked eye. Figure 3.6 shows the
blade position when it was fixed to the blade pitch mechanism. As a result, the
mechanism tailors the blade in range of pitch angle 20° to 30º as shown in Figure 3.7.
Furthermore, a force analysis was done for this system to make sure that the selected
stepper motor can maintain the motion of this mechanism [11].
Main Circuit
The main circuit consists of electrical and electronic circuits which it controls,
monitors and measures data from the system. This circuit regulates the generator’s
rotational speed, pitches the blades and measures the outputs in voltage (V) and
current (I). It consists of shunt resistor, variable resistor, DC generator, generator’s
encoder, stepper motor, stepper motor’s encoder and driver, analog to digital
convertor (ADC), and a computer with LABVIEW program as a controller and data
acquisition.
Axis of Rotation Chord Line
Figure 3.7- Tailoring the blade Figure 3.6- Blade pitch angle position
15
Connections
The circuit diagram, Figure 3.11, explains the path of connections. These connections
are divided into 5 types:
Positive power cables in red
Negative power cables in blue
Ground cables in black
Control cables in green
USB cables in brown
Shunt Resistor
The shunt resistor is used to measure the voltage drop across the resistor and then
calculate the current according to:
∆# $')
(1.2)
* $
∆#
') (1.3)
where:
∆V = voltage drop across the shunt resistor,
R+ = shunt resistor which is 6mΩ in this case,
I = current in the circuit.
The shunt resistor has 6mΩ resistance, maximum voltage drop of 0.15V and
maximum current of 25A [22]. The shunt resistor had been chosen with a small
resistive value for high precision of readings.
Variable resistor
The variable resistor varies the generator’s load and hence controls the generator’s
rotational frequency; therefore the output voltage and current of the generator. It has
a maximum resistance of 85Ω with a wiper that varies from 0 to 85Ω. It was divided
into steps with a step size of 5Ω marked by the means of a multi-meter. Figure 3.8
shows how the values of the resistor were divided.
16
The total numbers of positions are 17 steps. The expected error in this process is 10%
and the wiper was changed manually.
Analog to Digital Converter (ADC)
The role of ADC is to convert analog signals into digital for further processing on a
computer. In this project, the used ADCs were NI USB 6211 and NI USB 6008.
These instruments are products of National Instruments [23; 24]. The first differ
from the second by the resolution and number of channels. The NI USB 6211 has a
resolution of 16 bits plus counters while the NI USB 6008 of 12bits.
LABVIEW program
By the means of LabView, a program was implemented to read and log the input data
and change the blade pitch angle. The data were stored in text files on the computer.
The program’s front panel is shown in Appendix B
The program is divided into two sections, one for the generator and the other for the
stepper motor. For the generator, this program calculates the output power, rpm and
current of the generator. The current is calculated from the measured voltage drop
readings across the shunt and the rpm is measured in terms of frequency which is the
frequency of the encoder. In order to convert it to rpm, the below equation was used:
Figure 3.8- Variable Resistor
17
,-.
/ 0 60
3
(1.4)
where:
,-. = rotation per minute,
/ = frequency of the encoder in Hz,
3 = lines per revolution.
Likewise, the power is the product of the calculated current from the voltage drop
across the shunt and the measured generator’s voltage output. All these values are
mean values of 1000 samples at a sampling rate of 100Hz.
For the stepper motor, the used program controls the direction of the motor,
rotational velocity and indicates its position. Its rotational velocity is controlled by
generating PWM. The change of the width of this signal affects the rotational velocity.
The direction is controlled by Boolean control switch [11].
In order to read these signals, this program was connected to ADCs by USB
connections to the computer. Then, the connections are spread according to
connection diagram, see Figure 3.11.
General Specifications
The small wind turbine model is presented in Figure 3.9 and the following table
(Table 3.6) lists its specifications.
Figure 3.9- The small wind turbine model
18
Specifications
Rotor
Rotor Diameter 0.577m
Hub Diameter 0.077m
Hub Length 0.064m
Hub Height 0.45m
Number of Blades 3
Blades
Blades Span 0.25m
Base Chord 0.036m
Material Resin VeroBlue
Nacelle
Type Tubular
Diameter 0.077m
Length 0.188m
Material PVC
Tower
Type Tubular
Diameter 0.032m
Height 0.412m
Material PVC
Base
Type Square
Length 0.2m
Width 0.2m
Thickness 0.025m
Material PVC
Table 3.6- Small Wind Turbine Model General Specification
19
Experimental Setup
The experiment took place in the wind tunnel in Carl von Ossietzky University of
Oldenburg where a 1x0.8 m2 area wind tunnel exists. It allows for velocities ranging
from 0 to 50m/s. The model was set in front of the wind tunnel’s nozzle, in an open
test section. The wind tunnel has a control screen used for setting the speed of the
incoming flow served with indicator to measure the output flow (u1) from the nozzle.
The small wind turbine model was fixed on a table in front of the nozzle’s wind
tunnel like illustrated in Figure 3.10.
Figure 3.10- Wind tunnel test section with wind turbine model
20
The cables going out from the model, as seen in the above Figure 3.10, are connected
to the main circuit. Figure 3.11 shows how the wind turbine components are
connected to the main circuit. NI USB 6008 was used for measuring the generator’s
output voltage and NI USB 6211 for measuring the shunt resistor voltage drop. The
other two NI USB 6211 were used for the blade pitch mechanism. One of them was
for changing the pitch angle and the other for position indication. The generator’s
encoder and stepper motor driver were connected to a voltage supply.
Figure 3.11- Connection Diagram
21
CHAPTER 4
CHARACTERIZATION
Procedure
To achieve the goal, characterizing the small wind turbine power output, the
generator’s output voltage, voltage drop across the shunt resistor and the rotational
frequency of the generator’s encoder were measured.
The wind tunnel was operated in wind speed range of 4 to 9 m/s with ∆u1= 1 m/s.
At each wind speed, the required data were measured at different resistor loads (R)
and pitch angles (γ). Table 4.1 lists the pitch angle range from 20 to 30° with the
resistor load from 0 to 50Ω at 9m/s. This means for each pitch angle, the resistor was
changed 10 steps at each wind speed.
Same procedure was repeated for the mentioned wind speed range except for 4m/s
where Table 4.2 shows the range of R was set from 5 to 85Ω. The mean values of the
measured data were logged every 10 seconds into a text file.
Wind Speed (m/s) Pitch Angle (⁰⁰⁰⁰)
20 5 10 15 20 25 30 35 40 45 50
21 5 10 15 20 25 30 35 40 45 50
22 5 10 15 20 25 30 35 40 45 50
23 5 10 15 20 25 30 35 40 45 50
24 5 10 15 20 25 30 35 40 45 50
25 5 10 15 20 25 30 35 40 45 50
26 5 10 15 20 25 30 35 40 45 50
27 5 10 15 20 25 30 35 40 45 50
28 5 10 15 20 25 30 35 40 45 50
29 5 10 15 20 25 30 35 40 45 50
30 5 10 15 20 25 30 35 40 45 50
9
Resistor (Ω)
Table 4.1- Operation methodology at 9m/s
22
Table 4.3 shows an example of results template taken at 9m/s wind speed and 20º
pitch angle.
Wind Speed (m/s) Pitch Angle (⁰⁰⁰⁰)
20 5 10 15 20 25 30 35 40 45 50 55 60 65 70 75 80 85
21 5 10 15 20 25 30 35 40 45 50 55 60 65 70 75 80 85
22 5 10 15 20 25 30 35 40 45 50 55 60 65 70 75 80 85
23 5 10 15 20 25 30 35 40 45 50 55 60 65 70 75 80 85
24 5 10 15 20 25 30 35 40 45 50 55 60 65 70 75 80 85
25 5 10 15 20 25 30 35 40 45 50 55 60 65 70 75 80 85
26 5 10 15 20 25 30 35 40 45 50 55 60 65 70 75 80 85
27 5 10 15 20 25 30 35 40 45 50 55 60 65 70 75 80 85
28 5 10 15 20 25 30 35 40 45 50 55 60 65 70 75 80 85
29 5 10 15 20 25 30 35 40 45 50 55 60 65 70 75 80 85
30 5 10 15 20 25 30 35 40 45 50 55 60 65 70 75 80 85
4
Resistor (Ω)
Table 4.2- Operation methodology at 4m/s
Pitch Angle (⁰) 20
Wind Speed (m/s) Resistor (Ω) Frequency (Hz) RPM VGenerator VShunt Current (A) Power (W)
5 10714.13 632.13 2.70 0.00303 0.51 1.36
10 16051.38 947.03 5.06 0.00294 0.49 2.47
15 17734.92 1046.36 6.07 0.00232 0.39 2.34
20 18534.66 1093.54 6.65 0.00189 0.31 2.09
25 19052.76 1124.11 7.00 0.00161 0.27 1.88
30 19543.53 1153.07 7.36 0.00140 0.23 1.72
35 19819.69 1169.36 7.53 0.00125 0.21 1.57
40 19959.95 1177.64 7.69 0.00109 0.18 1.39
45 20124.65 1187.35 7.83 0.00099 0.16 1.29
50 20315.69 1198.63 7.92 0.00087 0.15 1.15
9
Table 4.3- Results Template
23
After measuring and analyzing, the blades were fixed at the optimum blade pitch
angle and the load was varied to obtain maximum power coefficient at wind speeds
from 4 to 9 m/s to produce the power curve where measurements were taken at
these points. Then the wind tunnel was operated in the range from 9.5 to 14 m/s with
∆u1= 0.5 m/s at a constant resistor load and measurements were taken in order to
maintain a constant rated power by rotating the blades.
A contour plots presenting resistor load, pitch angle and c at different wind speeds
were plotted as shown in Figure 4.1 to determine . The yellow spots indicate
highest values of c and the grid white dots are the measured points. Even though
the measured points were sparse, it was possible to locate zones in which is
located. A detailed discussion about these plots will be covered later in this chapter.
25
Optimum Pitch Angle
As mentioned before, the blades were fixed at optimum pitch angle in the partial zone
to track c !". To identify this angle, sections were made at different locations of the
contour plots (Figure 4.1). Sections A-A and B-B for 9m/s plot were taken as an
example like in Figure 4.2.
After this cut in the 9m/s plot, it clarified that the optimum pitch angle is γ = 21°and
optimum load R = 10Ω at 99.44rpm where c !" = 0.022, (see Figure 4.3 and
Figure 4.4).
Figure 4.2- 9m/s contour plot shows the location of sections
B
B
A A
26
Figure 4.3 shows the behavior of c with pitch angle where it starts to increase until it
reaches the maximum and then decreases slightly. Likewise in Figure 4.4, the c
increase with the increase of the resistor until it reaches the maximum power
coefficient where it decreases afterwards.
Several sections were made for different locations at all wind speeds to determine the
optimum pitch angle which resulted in one pitch angle of γ = 21°. The curves that
presents both with all wind velocities and sections are shown in Appendix A. The
results for these sections are listed in Table 4.4.
Wind Speed [m/s] Pitch Angle [º] Resistor [Ω] 56789
4 21 50 0.009 5 21 30 0.015 6 21 20 0.018 7 21 15 0.020 8 21 15 0.021 9 21 10 0.022
Table 4.4- Cp max at different wind speeds
Figure 4.3- Section A-A Figure 4.4- Section B-B
27
Power Curve
According to the obtained results shown in Table 4.4, the blades were set at pitch
angle of γ = 21° and then adjusting the resistance to the optimum obtained values
corresponding to its wind speed. This was used to track c !" in the partial load zone
of the power curve. Figure 4.5 demonstrates the fruitful harvest from characterizing
the small wind turbine model power curve and the black dots present the measured
data. In the control zone, the pitch angle was altered as wind velocity increased above
the rated velocity to maintain an approximately constant rated power, Figure 4.5
The conditions that the small wind turbine model works on were attained. The
model’s cut-in wind speed was 4m/s at which it started to rotate. The rated wind
speed was at 9 m/s at which the rated power of 2.5W was determined.
Figure 4.5- Power Curve
28
Cp – λ curve
Previously it was mentioned, while analyzing Figure 4.2, that the resistive load
corresponding to c !" differ from one wind speed to another, hence a question
arises in mind; why is the variable load affecting c?
According to the theory, the power coefficient (c ) is a function of λ which depends
on the rotational frequency (ω) and incoming wind velocity. Suppose that the wind
speed is constant, and the varying parameter in this case is the rotational frequency
(ω), so, by the change of ω due to change of load, the tip speed ratio will
correspondingly changes. Figure 4.6 demonstrates the relation between variable loads
and rotational frequency at different wind speeds.
In spite of these plots, the role of incoming wind speed is summarized by shifting the
operational region of ω. Therefore, the change in resistive load causes the change in ω
and thus the tip speed ratio changes.
The change in tip speed ratio causes the power coefficient (c) to change as shown in
Figure 4.7. The figure illustrates the behavior of c with tip speed ratio in the wind
speed range from 4 to 9m/s. The figure also shows that c !" at each wind speed
gives different tip speed ratio which is opposite to what mentioned in theory. This is
because of several factors will be mentioned later.
Figure 4.6- The rotational frequency (ω) varies with the resistor
29
In addition, the rotational frequency variations change the generator’s output power
presented in change of both voltage (V) and current (I). Figure 4.8 shows the relation
between ω and both voltage (V) and current (I).
Figure 4.7- Cp – λ Curve
Figure 4.8- The relation between V-ω on the left hand side and I-ω on the right hand side
30
Limitation Factors
Together Figure 4.5, Figure 4.7 and Table 4.4 show both c !" and output power are
low compared to the design values. Also they show that the maximum power
coefficient and tip speed ratio are not equal in all wind speeds although they are close
in values.
Several factors played an important role in limiting the small wind turbine model’s
performance. This is realized in different points.
Friction
It was witnessed, in the incoming low wind velocities 4 and 5 m/s, large dark areas
determine the plot, see Figure 4.9, and this occurred due to friction.
In low wind speeds, the incoming flow had difficulties to overcome the friction in the
generator and bearings. This effect decreases with the increase of wind speed. Also,
eccentric oscillations in the rotation were visible.
Figure 4.9- Contour plot for wind speeds 4 and 5 m/s
31
Small Modifications
Moreover, small modifications in the model will enhance its performance and the
difference was observed. The comparison between two setups of the model is shown
by means of plots in Figure 4.10.
One setup represents the first time when the model was assembled labeled as “1st
Setup” in the plot whereas the second setup, labeled as “2nd Setup”, represents some
modifications applied on the model exemplified by adding lubrication, modify the
alignment of the main shaft and make it more stable and adding more range to the
pitching system. It is clearly presented that c was increased in the second setup.
Generator Losses
As information from the generator’s manufacturer, FAULHABER, the selected DC-
micromotor if used as a generator, will operate on a 40% of its efficiency. Besides the
experiment that was done by John Hopkins University [7], mentioned that its
generator was operating with efficiency between 40 to 50%. There generator was also
selected from FAULHABER. But there are more losses in the generator due to
copper, iron and mechanical losses. These losses might be the cause of such low
power.
Figure 4.10- Cp – λ Curve, comparison between 1st and 2nd setups
32
Manufacturing and Installation of blades
The manufacturing precision of blades can help in enhancing or affecting the model’s
performance. Since the blades are not 100% precise in shape and each one differs
from the other, it could contribute to lower the output power. In addition, the blades
were fitted manually with small alignment (blade pitch angle) differences.
Angle of Attack (AoA)
In the previous sections, the parameters that affected the system were studied and the
reasons why c !" is low and differs from wind speed to other were discussed. But
more questions flirted in mind; are λ and angle of attack the same all over the blade?
Is this could be a reason why the power outputs are low?
To answer these questions, some calculations were made for the angle of attack
depending on the obtained measurements. Surprisingly, the angle of attack was
different all through the blade and with wind speeds. A curve was drawn shows the
angle of attack with c at the tip of the blade, see Figure 4.11. The angle of attack is
not constant and varies by ∆AoA = 1º as an average variation based on the measured
data. The maximum power coefficient ( c !") becomes closer to the red line with
the increase in wind speeds. This also indicates the presence of friction in the system.
Figure 4.11- Cp- AoA curve at the tip of the blade
33
This change in angle of attack was caused by the change in rotational frequency (ω)
due to the change in the resistor. Similar curves were drawn but at two different
locations in the blade to see if there is also difference in angle of attack along the
blade. The drawn curves are at distances from the rotor center of 0.077m and 0.15m
and are shown in Figure 4.12 and Figure 4.13 respectively. Likewise Figure 4.11, the
maximum power coefficient ( c !") becomes closer to the red line with increase in
wind speed in Figure 4.12 and Figure 4.13.
Figure 4.12- Cp- AoA curve at the base of the blade
Figure 4.13- Cp- AoA curve at the middle of the blade
34
The difference in the three plots is in the power coefficient where c is higher near
the rotor center. This is normal because it is going away from the tip losses.
In order to have a constant angle of attack for all wind speeds, calculations were done,
depending on measured % = 3.3, to find new angle of attacks and then new twist
angles for the blade. As an example, Figure 4.14 shows the act of different wind
velocities (u2), marked with orange, on an airfoil. The resultant wind velocity (ures), the
green line, is a result of the rotational velocity (ur), the violet line, and wind velocities
(u2). It is shown that the angle of resultant wind (β) is constant for all applied wind
speeds and pitch angle (γ) is constant too as it is set to γ = 21º. Thus the angle of
attack (α) is mostly constant over some range of wind speeds.
Accordingly, Figure 4.15 was drawn to show the twist angles in the current and
proposed blades. The curve plotted in green is for the current blade while the
proposed one is plotted in blue. This modification could improve the system since the
angle of attack is shifted to higher values compared to the current one.
Figure 4.14- Velocity Triangle acting on airfoil
35
The aim of this twist is to maintain a constant angle of attack all over the blade and
thus improve its efficiency.
Figure 4.15- AoA and Blade Length for the current and proposed blades
36
CHAPTER 5
CONCLUSION AND FUTURE IMPROVEMENT
Although many problems were faced that influenced the small wind turbine model, it
had generated a power curve similar to the form of the ideal power curve where the
maximum output power is 2.5W at 9 m/s wind velocity with a maximum power
coefficient of 0.022.
Unfortunately, a constant c !" could not be achieved and therefore a constant λ;<=
which affected the system’s act due to several factors mentioned previously. While a
new design approach for the blades depending on obtained readings could enhance
the performance of the model.
At last, this small wind turbine model has proved its capability to achieve realistic
results and be subjected to realistic conditions, turbulent flow as an example, which
makes it sustainable for better research methods and improvements in wind energy
research.
Future Improvements
As a step forward in continuing this project, one can work on several points that
improve this project.
The range of output voltage was between 0 and 10V while in future this range would
shift to higher ranges. In this case, a voltage divider should be implemented to the
main circuit, a brief calculation and schematic drawing of it is found in the Appendix
C. This will allow the NI USB 6211 to read the input voltage.
The implementation of a controller program by means of LabView would improve
the act of the wind turbine model. This program should consist of feedback loops
and control commands for the variable resistor which should be replaced by digital
one. In addition, a modified pitch control program should be implemented.
37
Since the c !" was low due to friction and losses, it is recommended, before taking
any action, to measure the torque acting in the system by installing strain gauges and
pressing rod and then calculate the mechanical power. As the research team in
Oldenburg University are working on similar projects and have the expertise, it would
be helpful for installation of such measuring equipment. Accordingly, proposed
solutions would be supported with detailed information and thus accurate decisions
could be taken.
Moreover, the maximum tip speed ratio obtained was 3.3 depending on the
measurements. A modification could be done on the blades to match these
measurements in order to attain a constant angle of attack all over the blade at
different wind speeds. In order to apply these changes to the blades, a certain design
procedure should be followed. Depending on the measured tip speed ratio, the twist
angle of the blade should be changed according to angle of attack and its
corresponding distance from the rotor center (r) and then the chord length with r.
Still, there are more and more things to improve in this young small wind turbine
model.
38
APPENDIX A
Power coefficient and resistance at different wind speeds
Figure A.1- Power coefficient and resistor at different wind speeds
39
Power coefficient and pitch angle at different wind speeds
Figure A.2- Power coefficient and pitch angle at different wind speeds
40
APPENDIX B
The program’s front panel was divided into several booths:
Graphical Indicator (monitor input data graphically)
Numerical Indicator (monitor input data numerically)
Channel Parameters
Timing Parameters
File Path
Figure B.1- LabView Front Panel
41
APPENDIX C
Voltage Divider Circuit
Design Formulas
To calculate the generator’s voltage the following formulas were used:
#> #?
' @ '
'A (C.1)
and the current
$> $? 1 @
'B @ ')
' @ 'A (C.2)
Figure C.1- Voltage divider circuit
42
BIBLIOGRAPHY
[1] Windindustrie in Deutschland – Exportbilanz und Inlandsmarkt. s.l. : Verband
Deutscher Maschinen- und Anlagenbau, July 2011.
[2] Li Junfeng, Shi Pengfei, Gao Hu. China Wind Power Outlook. s.l. : Chinese
Renewable Energy Industries Association, Global Wind Energy Council,
Greenpeace, 2010.
[3] Global Wind Energy Council (GWEC). Global Wind Energy Council (GWEC).
[Online] Mar 2010. [Cited: Feb 6, 2012.]
http://www.gwec.net/fileadmin/documents/Publications/Global_Wind_2007_rep
ort/GWEC_Global_Wind_2009_Report_LOWRES_15th.%20Apr..pdf.
[4] European Wind Energy Association (EWEA). European Wind Energy Association.
[Online] 2011. [Cited: Feb 6, 2012.] http:/www.ewea.org/index.php?id=195.
[5] European Wind Energy Association (EWEA). European Wind Energy Association.
[Online] 2011. [Cited: Feb 6, 2012.] http://www.ewea.org/index.php?id=198.
[6] European Wind Energy Association (EWEA). European Wind Energy Association
(EWEA). [Online]
http://www.ewea.org/fileadmin/ewea_documents/documents/publications/WET
F/Facts_Volume_2.pdf.
[7] Kang, Hynug Suk and Meneveau, Charles. Direct mechanical torque sensor for
model wind turbines. MEASUREMENT SCIENCE AND TECHNOLOGY.
2010, 21.
[8] Raúl Bayoán Cal, José Lebrón, Luciano Castillo, Hyung Suk Kang, and Charles
Meneveau. Experimental study of the horizontally averaged flow structure in a
model wind-turbine array boundary layer. J. Renewable Sustainable Energy. 2, 2010,
013106.
[9] An Experimental Investigation on the Wake Characteristics of a Wind Turbine in
an Atmospheric Boundary Layer Wind. Zifeng Yang, Partha Sarkar and Hui Hu.
Honolulu, Hawaii : American Institute of Aeronautics and Astronautics, Inc., 2011.
[10] Wallmann, Staffan and Janke, David. Konstruktion und Aufbau einer
Messeinrichtung für Modelluntersuchungen an WEA-Rotoren mit dem
Hochlaufversuch. Berlin : Technische Universität Berlin, 2008.
[11] Abdulhadi, Fadi. Design and Characterization of a Small Wind Turbine Model
equipped with a Pitching System. Kassel : Kassel University, Oldenburg University
and Cairo University, 2012.
43
[12] J. F. Manwell, J. G. McGowan and A. L. Rogers. WIND ENERGY; Theory,
Design and Application. United Kingdom : John Wiley & Sons Ltd, 2009.
[13] Schepers, J.G. and Snel, H. Model Experiments in Controlled Conditions. s.l. :
ECN Wind Energy, 2007.
[14] RTC or Rapid Technologies & Consulting. Rapid Technologies & Consulting.
[Online] 2003. [Cited: Feb 2, 2012.] http://www.rtc-
germany.com/objet/o_materialien.html.
[15] RTC or Rapid Technologies & Consulting. Rapid Technologies & Consulting.
[Online] 2003. [Cited: Feb 2, 2012.] http://www.rtc-
germany.com/objet/o_anwendung_01.html.
[16] DR. FRITZ FAULHABER GMBH & CO.KG. FAULHABER. [Online] 2011.
[Cited: Dec 23, 2011.]
http://www.faulhaber.com/uploadpk/EN_3863_CR_DFF.pdf.
[17] DR. FRITZ FAULHABER GMBH & CO.KG. FAULHABER. [Online] 2011.
[Cited: Sep 23, 2011.] http://www.faulhaber.com/uploadpk/EN_IE2-
1024_DFF.pdf.
[18] DR. FRITZ FAULHABER GMBH & CO.KG. FAULHABER. [Online] 2011.
[Cited: Dec 23, 2011.]
http://www.faulhaber.com/uploadpk/EN_AM2224R3_PCS.pdf.
[19] DR. FRITZ FAULHABER GMBH & CO.KG. FAULHABER. [Online] 2011.
[Cited: Sep 23, 2011.] http://www.faulhaber.com/uploadpk/EN_PE22-
120_PCS.pdf.
[20] DR. FRITZ FAULHABER GMBH & CO.KG. FAULHABER. [Online] 2011.
[Cited: Sep 20, 2011.]
http://www.faulhaber.com/uploadpk/EN_ADxxMxx_PCS.pdf.
[21] DR. FRITZ FAULHABER GMBH & CO.KG. FAULHABER. [Online] [Cited:
Feb 14, 2012.]
http://www.faulhaber.com/uploadpk/EN_ADCMMxS_im_PCS.pdf.
[22] Mercateo. Mercateo. [Online] 2011.
http://www.mercateo.com/pdf/Schuricht/hiShunt-250A_dat_d.pdf.
[23] National Instruments Corporation. National Instruments. [Online] May 2008.
[Cited: Dec 23, 2011.] http://www.ni.com/pdf/manuals/371303l.pdf.
[24] National Instruments Corporation. National Instruments. [Online] Apr 2009.
[Cited: Dec 23, 2011.] http://www.ni.com/pdf/manuals/371932f.pdf.
[25] Hau, E. Wind Turbines: Fundamentals, Technologies, Application, Economics.
Germany : Springer, 2006.
Declaration for the Master’s Thesis
I hereby affirm that the master thesis at hand is my own written work and that I
have used no other sources and aids others than those indicated. Only the sources
cited have been used. Those parts which are direct quotes or paraphrases are
identified as such.
Kassel, on 27 February 2012 __________________ (Signature)