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Water Pumping Based on
Wind Turbine Generation System
People's Democratic Republic of Algeria Ministry of
Higher Education and Scientific Research
University Mohamed Khider Biskra
Faculty of Science and Technology Department of
Electrical Engineering
Field: Electrical Engineering
Option: Electrical Control
A thesis submitted in fulfillment of the requirements for
the degree of:
MASTER
Directed by: ABDEDDAIM Sabrina Presented by: KHINECH Adel
Scholar year: 2017/2018
Presentation Plan
01
02
1. Introduction.
2. Wind turbine operation.
3. Wind turbine types.
4. Wind turbine conversion system.
5. Wind turbine control strategies.
6. Simulation results and future scope.
Introduction
03
04
The amount of energy extracted from renewable resources,
and specially from wind, is considered today as a competitive
and necessary alternative to fossil resources. The use of wind
energy has grown during the last few years, this has led to an
increase of research and development of larger and effective
wind turbines in order to offer renewable energy to the
customers.
• The aim of this work is to interpret wind turbines control
techniques, and develop a conversion system connected to a
water pump.
Wind turbine operation
05
06
Wind turbine is a device that is capable of converting a great amount of kinetic
energy into electricity. When wind blows a mechanical energy developed in the
turbine rotor, amplified by the gearbox , and transmitted to the generator to
produce electrical power.
Fig 1: Wind turbine operation scheme.
Wind turbine types
07
08
Fig 3: Vertical axis wind turbine.Fig 2: Horizontal axis wind turbine.
Wind turbine conversion system
09
10
𝑷 𝒘 =
𝟏
𝟐
𝝆𝑨𝒗 𝟑 (𝑾)
𝑷 𝒂 = 𝑷 𝒘. 𝑪 𝒑 (𝑾)
𝑪 𝒑= 𝒇(𝝀, 𝜷)
Wind power :
The Aerodynamic power :
The power coefficient:
The mechanical torque:
𝑻 𝒂 =
𝑷 𝒂
𝜴 𝒕
(𝑵𝒎)
Fig 4: Entering and leaving wind speeds.
The entering wind speed through turbine blades is higher than leaving speed,
Where the aerodynamic power is related to wind power and a power coefficient Cp
which is a function of tip speed ratio and blade pitch angle.
11
Ta
Fig 5: Wind turbine model scheme (𝜷 = 0).
Turbine model
12
The permanent magnet synchronous generator is used to produce electrical power due to
its high power factor and efficiency. The electrical equations in a fixed reference linked to
the stator are described by:
Generator modeling
𝑽𝒂
𝑽𝒃
𝑽𝒄
= 𝑅𝑠
𝑖𝑎
𝑖𝑏
𝑖𝑐
+
𝑑
𝑑𝑡
φ𝑎
φ𝑏
φ𝑐
𝑽 𝒅𝒔= − 𝑹 𝑺 𝒊 𝒅𝒔 − 𝒘 𝒈𝒓 𝝋 𝒒𝒔 + 𝒑𝝋 𝒅𝒔
𝑽 𝒒𝒔= − 𝑹 𝑺 𝒊 𝒒𝒔 − 𝒘 𝒈𝒓 𝝋 𝒅𝒔 + 𝒑𝝋 𝒒𝒔
To simplify the analysis, The synchronous generator is modeled
in dq-axis reference frame that gives:
𝑽 𝒅𝒔 = − 𝑹 𝑺 𝒊 𝒅𝒔 + 𝒘 𝒈𝒓 𝑳 𝒒 𝒊 𝒒𝒔 − 𝑳 𝒅 𝒑𝒊 𝒅𝒔
𝑽 𝒒𝒔= − 𝑹 𝑺 𝒊 𝒒𝒔 − 𝒘 𝒈𝒓 𝑳 𝒅 𝒊 𝒅𝒔 + 𝒘 𝒈𝒓 𝝋 𝒓 − 𝑳 𝒒 𝒑𝒊 𝒒𝒔
13
Water pump modeling
The motor–pump system includes the motor, the coupling and the pump.
The centrifugal pump is used to pump water where its parameters are
listed in equations below: Head, Hydraulic power, and resistive torque.
𝑯 = 𝑪 𝟏 𝝎 𝟐 + 𝑪 𝟐 𝝎𝑸 + 𝑪 𝟑 𝑸² (m)
𝑷 𝑯 = 𝝆′. 𝒈. 𝑸. 𝑯 (kW)
𝑻 𝒓 = 𝑲 𝑳𝒐𝒂𝒅. Ω 𝟐 (Nm)
Motor Coupling Pump
Wind turbines Control strategies
14
15
In order to ensure an optimum operation of the wind generation
system, it is essential to extract the maximum power that the wind
can offer, and deliver it among the conversion chain.
The control strategies consist of:
 Speed control using a maximum power point tracker (MPPT).
 Hysteresis band pulse width modulated current controller (PWM).
 Filed oriented control of a PMS Motor based on space vector
modulation (SV-PWM).
16
Fig 6: Control structure.
MPPT System
17
18
Fig 7: Speed controller using MPPT.
To obtain the maximum available power from wind at different wind speeds, the
turbine speed must be connected to the MPPT system which is based on PI
controller.
Hysteresis band PWM
19
20
Fig 8: Hysteresis current controller diagram.
Hysteresis modulation is a current control method where the phase current tracks a
reference waveform within a band, where The required magnitude and frequency
are generated at the output of the rectifier.
Space vector PWM
21
22
𝑽 𝜶𝜷 =
𝑽 𝜶
𝑽 𝜷
=
𝟑
𝟐
𝟏 −𝟏/𝟐 −𝟏/𝟐
𝟎 𝟑/𝟐 − 𝟑/𝟐
𝑽 𝒂
𝑽 𝒃
𝑽 𝒄
• Concordia transform:
Fig 10: Hexagon diagram.Fig 9: Applying vectors sequence.
Space vector modulation is an algorithm used to control the three phase inverter,
using Concordia transform, and applying the vectors sequence according to the
sector where the vector 𝑽 𝜶𝜷 is situated in the hexagon diagram.
Filed Oriented Control
23
24
Fig 11: Filed oriented control diagram.
𝑻 𝒆 =
𝟑
𝟐
𝒑. (𝒊 𝒒𝒔 𝝋 𝒔𝒇 + 𝑳 𝒅 − 𝑳 𝒒 𝒊 𝒅𝒔 𝒊 𝒒𝒔)• Synchronous machine electromagnetic torque:
𝑻 𝒆 =
𝟑
𝟐
𝒑. (𝒊 𝒒𝒔 𝝋 𝒔𝒇)
• Setting
The aim of this control is to achieve a model equivalent to the DC machine and perform a
realtime torque control. Both reference currents are compared separately with the real time
motor currents where they controlled by PI regulators
𝒊 𝒅𝒔 = 𝟎
25
Fig 12: Compensation diagram.
• Compensation process:
𝑽 𝒅 = 𝑹 𝒔 + 𝒑. 𝑳 𝒅 . 𝒊 𝒅 − 𝝎. 𝑳 𝒒 𝒊 𝒒 𝑽 𝒒 = 𝑹 𝒔 + 𝒑. 𝑳 𝒒 . 𝒊 𝒒 + 𝝎. 𝑳 𝒅 𝒊 𝒅 + 𝝎. 𝝋 𝒔𝒇
Simulation results
26
27
Fig 13: Wind speed profile (m/s)
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
3
3.5
4
4.5
5
5.5
6
6.5
7
7.5
8
Time (s)
WindSpeed(m/s)
Wind speed
4
5
7 m/s
28
Fig 14: Power coefficient Cp.
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
X: 0.7396
Y: 0.5475
Time (s)
PowercoefficientCp
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
0
1
2
3
4
5
6
7
X: 0.63
Y: 6.502
Time (s)
Tipspeedratio(Lamda)
Fig 15: Tip speed ratio λ.
6.502
0.547
29Fig 16: Measured and optimal Turbine speed (rad/s).
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
0
20
40
60
80
100
120
X: 0.923
Y: 104
Time(s)
Turbinespeedandoptimalturbinespeed(rad/s)
X: 0.3294
Y: 74.31
X: 0.1205
Y: 59.45
Turbine Speed
Optimal Speed
0.1999 0.2 0.2001 0.2002 0.2003 0.2004
73.95
74
74.05
74.1
74.15
74.2
74.25
74.3
74.35
74.4
Time(s)
X: 0.2003
Y: 74.31
Turbinespeedandoptimalturbinespeed(rad/s)
Turbine Speed
Optimal Speed
Zoom
0.3999 0.4 0.4001 0.4002 0.4003 0.4004 0.4005
103.5
103.6
103.7
103.8
103.9
104
104.1
104.2
Time(s)
X: 0.4004
Y: 104
Turbinespeedandoptimalturbinespeed(rad/s)
Turbine Speed
Optimal Speed
Zoom
104 rad/s
74.31
59.45
30
Fig 17: The maximum power extracted from wind (Watt).
0 10 20 30 40 50 60 70 80 90 100
0
500
1000
1500
2000
2500
3000
3500
4000
X: 59.45
Y: 728.2
Mechanical (Generator) speed (rad/s)
Aerodynamicpower(watt)
X: 74.31
Y: 1422
X: 104
Y: 3903
3903 W
31
Fig 18: Generator output
voltages 𝑽 𝒂, 𝑽 𝒃, 𝑽 𝒄:
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
-300
-200
-100
0
100
200
300
Time(s)
Generatoroutputvoltages(v)
Vc
Vb
Va
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
-6
-4
-2
0
2
4
6
Time (s)
Generatoroutputcurrents(A)
ic
ib
iaFig 19: Generator output
currents 𝒊 𝒂, 𝒊 𝒃, 𝒊 𝒄:
32
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
0
50
100
150
200
250
Time (s)
RectifieroutputvoltageVdc(V)
Fig 20: The rectifier output voltage (V).
240 v
33
Fig 21: Motor speed and turbine speed as a reference (rad/sec).
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
-20
0
20
40
60
80
100
120
X: 0.8823
Y: 104
Time (s)
TurbinespeedandMotorspeed(rad/s)
X: 0.3634
Y: 74.31
X: 0.1763
Y: 59.45
Motor speed
Turbine speed
104 rad/s
34
Fig 22: Reference stator current
𝒊 𝒒𝒔_𝒓𝒆𝒇 and measured stator
current 𝒊 𝒒𝒔.
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
-10
-5
0
5
10
15
20
25
X: 0.9585
Y: 15.09
Time (s)
Statorcurrentiqsandreferencestatorcurrentiqs-ref(A)
X: 0.3909
Y: 7.229
X: 0.1903
Y: 4.591
iqs-ref
iqs
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
-10
-8
-6
-4
-2
0
2
4
6
8
10
Time (s)
Referencestatorcurrentids-refandstatorcurrentids(V)
ids-ref
ids
Fig 23: Reference stator current
𝒊 𝒅𝒔_𝒓𝒆𝒇 and measured stator
current 𝒊 𝒅𝒔.
15 A
• Quadrature currents:
35Fig 24: Motor torque and water resistive torque (Nm).
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
-5
0
5
10
15
20
X: 0.9238
Y: 10.18
X: 0.3313
Y: 5.222
X: 0.1615
Y: 3.111
Motor torque
Resistive torque
10.18 N.m
36
Fig 25: Water pump hydraulic power (kW).
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
-0.5
0
0.5
1
1.5
2
2.5
3
3.5
4
4.5
X: 0.9702
Y: 3.677
Time (s)
Power(kw)
X: 0.3935
Y: 1.34
X: 0.1893
Y: 0.6861
3.67 kW
37
Fig 26: Water pump head (m).
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
0
20
40
60
80
100
120
X: 0.9658
Y: 89.95
Time (s)
Head(m)
X: 0.3927
Y: 45.88
X: 0.1981
Y: 29.36
89.95 m
38
Fig 27: Water pump flow rate (m3/h).
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
-2
0
2
4
6
8
10
12
14
16
X: 0.9778
Y: 15
Time (s)
FlowrateQ(m3/h)
X: 0.3955
Y: 10.72
X: 0.1932
Y: 8.574
15 m3/h
Conclusion
39
40
This work provided a wind energy conversion system control strategies
in order to extract the maximum power from wind, a permanent magnet
synchronous generator used to generate that power and deliver it to a
pumping system through the rectifier and the inverter.
The complexity of the variable speed system leads to, a reduced
reliability and power. But, as a result of using more advanced and robust
control techniques, a power quality is achieved.
Future scope
41
42
The conversion system can be optimized by:
 Performing an advanced MPPT algorithms, using pitch angle and
YAW techniques.
 Using vector control strategy to control the rectifier.
 Integrating Boost chopper and DC link voltage regulator.
 Moreover, a detailed study to a conversion system connected to the
grid, and batteries for the stand alone turbine mode.
Thank You

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Water pumping based on wind turbine generation system.

  • 1. Water Pumping Based on Wind Turbine Generation System People's Democratic Republic of Algeria Ministry of Higher Education and Scientific Research University Mohamed Khider Biskra Faculty of Science and Technology Department of Electrical Engineering Field: Electrical Engineering Option: Electrical Control A thesis submitted in fulfillment of the requirements for the degree of: MASTER Directed by: ABDEDDAIM Sabrina Presented by: KHINECH Adel Scholar year: 2017/2018
  • 3. 02 1. Introduction. 2. Wind turbine operation. 3. Wind turbine types. 4. Wind turbine conversion system. 5. Wind turbine control strategies. 6. Simulation results and future scope.
  • 5. 04 The amount of energy extracted from renewable resources, and specially from wind, is considered today as a competitive and necessary alternative to fossil resources. The use of wind energy has grown during the last few years, this has led to an increase of research and development of larger and effective wind turbines in order to offer renewable energy to the customers. • The aim of this work is to interpret wind turbines control techniques, and develop a conversion system connected to a water pump.
  • 7. 06 Wind turbine is a device that is capable of converting a great amount of kinetic energy into electricity. When wind blows a mechanical energy developed in the turbine rotor, amplified by the gearbox , and transmitted to the generator to produce electrical power. Fig 1: Wind turbine operation scheme.
  • 9. 08 Fig 3: Vertical axis wind turbine.Fig 2: Horizontal axis wind turbine.
  • 11. 10 𝑷 𝒘 = 𝟏 𝟐 𝝆𝑨𝒗 𝟑 (𝑾) 𝑷 𝒂 = 𝑷 𝒘. 𝑪 𝒑 (𝑾) 𝑪 𝒑= 𝒇(𝝀, 𝜷) Wind power : The Aerodynamic power : The power coefficient: The mechanical torque: 𝑻 𝒂 = 𝑷 𝒂 𝜴 𝒕 (𝑵𝒎) Fig 4: Entering and leaving wind speeds. The entering wind speed through turbine blades is higher than leaving speed, Where the aerodynamic power is related to wind power and a power coefficient Cp which is a function of tip speed ratio and blade pitch angle.
  • 12. 11 Ta Fig 5: Wind turbine model scheme (𝜷 = 0). Turbine model
  • 13. 12 The permanent magnet synchronous generator is used to produce electrical power due to its high power factor and efficiency. The electrical equations in a fixed reference linked to the stator are described by: Generator modeling 𝑽𝒂 𝑽𝒃 𝑽𝒄 = 𝑅𝑠 𝑖𝑎 𝑖𝑏 𝑖𝑐 + 𝑑 𝑑𝑡 φ𝑎 φ𝑏 φ𝑐 𝑽 𝒅𝒔= − 𝑹 𝑺 𝒊 𝒅𝒔 − 𝒘 𝒈𝒓 𝝋 𝒒𝒔 + 𝒑𝝋 𝒅𝒔 𝑽 𝒒𝒔= − 𝑹 𝑺 𝒊 𝒒𝒔 − 𝒘 𝒈𝒓 𝝋 𝒅𝒔 + 𝒑𝝋 𝒒𝒔 To simplify the analysis, The synchronous generator is modeled in dq-axis reference frame that gives: 𝑽 𝒅𝒔 = − 𝑹 𝑺 𝒊 𝒅𝒔 + 𝒘 𝒈𝒓 𝑳 𝒒 𝒊 𝒒𝒔 − 𝑳 𝒅 𝒑𝒊 𝒅𝒔 𝑽 𝒒𝒔= − 𝑹 𝑺 𝒊 𝒒𝒔 − 𝒘 𝒈𝒓 𝑳 𝒅 𝒊 𝒅𝒔 + 𝒘 𝒈𝒓 𝝋 𝒓 − 𝑳 𝒒 𝒑𝒊 𝒒𝒔
  • 14. 13 Water pump modeling The motor–pump system includes the motor, the coupling and the pump. The centrifugal pump is used to pump water where its parameters are listed in equations below: Head, Hydraulic power, and resistive torque. 𝑯 = 𝑪 𝟏 𝝎 𝟐 + 𝑪 𝟐 𝝎𝑸 + 𝑪 𝟑 𝑸² (m) 𝑷 𝑯 = 𝝆′. 𝒈. 𝑸. 𝑯 (kW) 𝑻 𝒓 = 𝑲 𝑳𝒐𝒂𝒅. Ω 𝟐 (Nm) Motor Coupling Pump
  • 15. Wind turbines Control strategies 14
  • 16. 15 In order to ensure an optimum operation of the wind generation system, it is essential to extract the maximum power that the wind can offer, and deliver it among the conversion chain. The control strategies consist of:  Speed control using a maximum power point tracker (MPPT).  Hysteresis band pulse width modulated current controller (PWM).  Filed oriented control of a PMS Motor based on space vector modulation (SV-PWM).
  • 17. 16 Fig 6: Control structure.
  • 19. 18 Fig 7: Speed controller using MPPT. To obtain the maximum available power from wind at different wind speeds, the turbine speed must be connected to the MPPT system which is based on PI controller.
  • 21. 20 Fig 8: Hysteresis current controller diagram. Hysteresis modulation is a current control method where the phase current tracks a reference waveform within a band, where The required magnitude and frequency are generated at the output of the rectifier.
  • 23. 22 𝑽 𝜶𝜷 = 𝑽 𝜶 𝑽 𝜷 = 𝟑 𝟐 𝟏 −𝟏/𝟐 −𝟏/𝟐 𝟎 𝟑/𝟐 − 𝟑/𝟐 𝑽 𝒂 𝑽 𝒃 𝑽 𝒄 • Concordia transform: Fig 10: Hexagon diagram.Fig 9: Applying vectors sequence. Space vector modulation is an algorithm used to control the three phase inverter, using Concordia transform, and applying the vectors sequence according to the sector where the vector 𝑽 𝜶𝜷 is situated in the hexagon diagram.
  • 25. 24 Fig 11: Filed oriented control diagram. 𝑻 𝒆 = 𝟑 𝟐 𝒑. (𝒊 𝒒𝒔 𝝋 𝒔𝒇 + 𝑳 𝒅 − 𝑳 𝒒 𝒊 𝒅𝒔 𝒊 𝒒𝒔)• Synchronous machine electromagnetic torque: 𝑻 𝒆 = 𝟑 𝟐 𝒑. (𝒊 𝒒𝒔 𝝋 𝒔𝒇) • Setting The aim of this control is to achieve a model equivalent to the DC machine and perform a realtime torque control. Both reference currents are compared separately with the real time motor currents where they controlled by PI regulators 𝒊 𝒅𝒔 = 𝟎
  • 26. 25 Fig 12: Compensation diagram. • Compensation process: 𝑽 𝒅 = 𝑹 𝒔 + 𝒑. 𝑳 𝒅 . 𝒊 𝒅 − 𝝎. 𝑳 𝒒 𝒊 𝒒 𝑽 𝒒 = 𝑹 𝒔 + 𝒑. 𝑳 𝒒 . 𝒊 𝒒 + 𝝎. 𝑳 𝒅 𝒊 𝒅 + 𝝎. 𝝋 𝒔𝒇
  • 28. 27 Fig 13: Wind speed profile (m/s) 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 3 3.5 4 4.5 5 5.5 6 6.5 7 7.5 8 Time (s) WindSpeed(m/s) Wind speed 4 5 7 m/s
  • 29. 28 Fig 14: Power coefficient Cp. 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 X: 0.7396 Y: 0.5475 Time (s) PowercoefficientCp 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 0 1 2 3 4 5 6 7 X: 0.63 Y: 6.502 Time (s) Tipspeedratio(Lamda) Fig 15: Tip speed ratio λ. 6.502 0.547
  • 30. 29Fig 16: Measured and optimal Turbine speed (rad/s). 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 0 20 40 60 80 100 120 X: 0.923 Y: 104 Time(s) Turbinespeedandoptimalturbinespeed(rad/s) X: 0.3294 Y: 74.31 X: 0.1205 Y: 59.45 Turbine Speed Optimal Speed 0.1999 0.2 0.2001 0.2002 0.2003 0.2004 73.95 74 74.05 74.1 74.15 74.2 74.25 74.3 74.35 74.4 Time(s) X: 0.2003 Y: 74.31 Turbinespeedandoptimalturbinespeed(rad/s) Turbine Speed Optimal Speed Zoom 0.3999 0.4 0.4001 0.4002 0.4003 0.4004 0.4005 103.5 103.6 103.7 103.8 103.9 104 104.1 104.2 Time(s) X: 0.4004 Y: 104 Turbinespeedandoptimalturbinespeed(rad/s) Turbine Speed Optimal Speed Zoom 104 rad/s 74.31 59.45
  • 31. 30 Fig 17: The maximum power extracted from wind (Watt). 0 10 20 30 40 50 60 70 80 90 100 0 500 1000 1500 2000 2500 3000 3500 4000 X: 59.45 Y: 728.2 Mechanical (Generator) speed (rad/s) Aerodynamicpower(watt) X: 74.31 Y: 1422 X: 104 Y: 3903 3903 W
  • 32. 31 Fig 18: Generator output voltages 𝑽 𝒂, 𝑽 𝒃, 𝑽 𝒄: 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 -300 -200 -100 0 100 200 300 Time(s) Generatoroutputvoltages(v) Vc Vb Va 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 -6 -4 -2 0 2 4 6 Time (s) Generatoroutputcurrents(A) ic ib iaFig 19: Generator output currents 𝒊 𝒂, 𝒊 𝒃, 𝒊 𝒄:
  • 33. 32 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 0 50 100 150 200 250 Time (s) RectifieroutputvoltageVdc(V) Fig 20: The rectifier output voltage (V). 240 v
  • 34. 33 Fig 21: Motor speed and turbine speed as a reference (rad/sec). 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 -20 0 20 40 60 80 100 120 X: 0.8823 Y: 104 Time (s) TurbinespeedandMotorspeed(rad/s) X: 0.3634 Y: 74.31 X: 0.1763 Y: 59.45 Motor speed Turbine speed 104 rad/s
  • 35. 34 Fig 22: Reference stator current 𝒊 𝒒𝒔_𝒓𝒆𝒇 and measured stator current 𝒊 𝒒𝒔. 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 -10 -5 0 5 10 15 20 25 X: 0.9585 Y: 15.09 Time (s) Statorcurrentiqsandreferencestatorcurrentiqs-ref(A) X: 0.3909 Y: 7.229 X: 0.1903 Y: 4.591 iqs-ref iqs 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 -10 -8 -6 -4 -2 0 2 4 6 8 10 Time (s) Referencestatorcurrentids-refandstatorcurrentids(V) ids-ref ids Fig 23: Reference stator current 𝒊 𝒅𝒔_𝒓𝒆𝒇 and measured stator current 𝒊 𝒅𝒔. 15 A • Quadrature currents:
  • 36. 35Fig 24: Motor torque and water resistive torque (Nm). 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 -5 0 5 10 15 20 X: 0.9238 Y: 10.18 X: 0.3313 Y: 5.222 X: 0.1615 Y: 3.111 Motor torque Resistive torque 10.18 N.m
  • 37. 36 Fig 25: Water pump hydraulic power (kW). 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 -0.5 0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 X: 0.9702 Y: 3.677 Time (s) Power(kw) X: 0.3935 Y: 1.34 X: 0.1893 Y: 0.6861 3.67 kW
  • 38. 37 Fig 26: Water pump head (m). 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 0 20 40 60 80 100 120 X: 0.9658 Y: 89.95 Time (s) Head(m) X: 0.3927 Y: 45.88 X: 0.1981 Y: 29.36 89.95 m
  • 39. 38 Fig 27: Water pump flow rate (m3/h). 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 -2 0 2 4 6 8 10 12 14 16 X: 0.9778 Y: 15 Time (s) FlowrateQ(m3/h) X: 0.3955 Y: 10.72 X: 0.1932 Y: 8.574 15 m3/h
  • 41. 40 This work provided a wind energy conversion system control strategies in order to extract the maximum power from wind, a permanent magnet synchronous generator used to generate that power and deliver it to a pumping system through the rectifier and the inverter. The complexity of the variable speed system leads to, a reduced reliability and power. But, as a result of using more advanced and robust control techniques, a power quality is achieved.
  • 43. 42 The conversion system can be optimized by:  Performing an advanced MPPT algorithms, using pitch angle and YAW techniques.  Using vector control strategy to control the rectifier.  Integrating Boost chopper and DC link voltage regulator.  Moreover, a detailed study to a conversion system connected to the grid, and batteries for the stand alone turbine mode.

Editor's Notes

  1. I would like to thank everyone for being here today, for my thesis presentation titled Water pumping based on Wind turbine generation system
  2. Starting with the plan ………… and finally
  3. So when wind blows a mechanical energy developed in the turbine rotor, amplified by the gearbox , and transmitted to the generator to produce electrical power.
  4. Wind turbines can be divided into two types, Vertical and Horizontal. For our project we have chosen Horizontal axis wind turbine, due to its efficiency at low wind speed.
  5. As illustrated in fig 4, the entering wind speed through turbine blades is higher than leaving speed, Where the aerodynamic power is related to wind power and a power coefficient Cp which is a function of tip speed ratio lamda and blade pitch angle beta.
  6. Based on the previous equations, The turbine model is given by the shown scheme where beta is considered zero
  7. The permanent magnet synchronous generator is used to produce electrical power due to its high power factor and efficiency. To simplify the analysis, The synchronous generator is modeled in dq-axis reference frame that gives the listed Vds and Vqs.
  8. The motor–pump system includes the motor, the pump, and the couplings. A centrifugal pump is used where its parameters are illustrated in equations below: Head, Hydraulic power, and resistive torque. What we should notice is that , there no water flow if there is no wind, so a water tank or water storage is necessary.
  9. In order to ensure an optimum operation of the wind generation system, it is essential to extract the maximum power that the wind can offer, and deliver it among the conversion chain. The control strategies consists of: Speed control using MPPT. Hysteresis band PWM and Filed oriented control based on SV-PWM.
  10. Where control structure scheme is illustrated in figure 6.
  11. To obtain the maximum available power from wind at different wind speeds, the turbine speed must be connected to an MPPT system that based on PI regulator as shown in figure 7.
  12. Hysteresis modulation is a current control method where the phase current tracks a reference waveform within a band, where The required magnitude and frequency are generated at the output of the rectifier.
  13. Space vector modulation is an algorithm used to control the three phase inverter , using Concordia transform, and applying the vectors sequence according to the sector where the vector V alfa beta is situated in the hexagon diagram as shown in figure ten.
  14. The aim of this control is to achieve a model equivalent to the DC machine and perform a realtime torque control by setting ids equal to zero and adjusting the Electromagnetic torque only by Iqs. Both reference currents are compared separately with the real time motor currents where they controlled by PI regulators as shown in figure eleven
  15. And we should notice that, There is a coupling between the axes d and q, therefore it is necessary to define the compensation terms as shown in figure twelve.
  16. Using three different wind speed, 4 and 5 then 7 meters per second as shown in figure thirteen to perform simulation.
  17. Both remain constant at an optimum values, even when the speed changes, due to the MPPT controller.
  18. The measured turbine speed increases and follows its reference turbine speed with no overshoot or error, and reach a maximum value of 104 rad/s.
  19. The power extracted from wind is always maximized even when turbine speed increased till it reaches a value around 4 kWatt
  20. Both are increased when turbine speed increased.
  21. It increased when turbine speed increased and reaches a maximum value around two hundred forty volts.
  22. It creates an overshoot then stabilizes and follows its reference turbine speed and reaches a value around 104 rad/s.
  23. Quadrature currents, The measured stator current iqs creates an overshoot then stabilizes and follows its reference when it increases and reaches a value around 15 Amperes. While the measured stator current ids remains null, both results validated the foc.
  24. As illustrated in figure 24 the motor torque follows the water resistive torque, means that the motor insures or provides the needed torque to pump water.
  25. It creates an overshoot then stabilizes , and increases when the turbine speed increases to reach a value around 3.67 kW.
  26. The head increases also when the turbine speed increased and the maximum high can reach is around ninety meters.
  27. Where the flow rate increases as well and reaches a value around 15 meters cube per hour.