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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 03 | Mar 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 3318
Electrical Simulation Model of IEC 61400-27-1 Doubly-Fed Induction
Generator (Type 3A) Based Wind Turbine
N.Bhavadharini1, B.R.Pavithra2, M.C.Lavanya3, Lavanya Dhanesh 4
1,2UG Scholars, Department of Electrical and Electronics Engineering, Panimalar Institute of Technology, Chennai
3Deputy Director, Research and Development (R&D) and Resource Data Analytic & Forecasting (RDAF), National
Institute of Wind Energy, Chennai
4Associate Professor, Department of Electrical and Electronics Engineering, Panimalar Institute of Technology,
Chennai
---------------------------------------------------------------------***---------------------------------------------------------------------
Abstract –The main objective of this project is to implement
the Electrical Simulation Model of IEC 61400-27-1 standard
TYPE 3 – DOUBLY-FED INDUCTION GENERATOR (DFIG) based
wind turbine. The dynamic models of a wind turbine are
designed by the manufacturers. These manufacturers provide
the behavior of their machines with a high level ofdetail.Before
carrying out In-situ testing of Wind Energy Conversion
System(WECS), wind turbine certification institution can
perform generic evaluation of the system with standard
parameters by using electrical simulation models which will be
effortless for the manufacturers to scrutinize the performance.
Standards make sure that the products work together safely
and reliably as intended. So different parameters given in the
model can be able to emulate the response for a wide range of
machines. By usingstandardtoolMATLAB/SIMULINK electrical
simulation of IEC 61400-27-1 DOUBLY-FED INDUCTION
GENERATOR based wind turbine is designed and implemented.
Key Words: IEC 61400-27-1, DFIG, WECS,
MATLAB/SIMULINK
1.INTRODUCTION
Wind energy utilization in power system has increased
greatly to meet the demand of the power system. Stability of
the system is concerned by the power system operators. So
the dynamic models of a wind turbine are designed by the
manufacturers. Manufacturers of wind turbines commonly
have all-inclusive data of wind turbine models. But thereare
several drawbacks for the use of such models by grid
operators. The grid operator does not have a full knowledge
of the model. So generic models have been required is
developed. Then a manufacturer only needs to provide a
parameterization for the model. This generic model
development finds the right balance between desired
accuracy and model complexity.
1.1 SCOPE
IEC 61400-27 specifies standard electrical simulation
models for wind turbines which provides procedures for
examining the specified electrical simulation models. IEC
61400-27-1 defines the universal terms and parameters
with the purpose of specifying the electrical characteristics
of a wind turbine. The models are described in a standard
way which can be applied for future wind turbine concepts.
So the dynamic simulation models are designed for wind
turbine terminals. The validation procedure specified in IEC
61400-27-1 focuses on the IEC 61400-21 tests for response
to voltage sag and transients condition.
1.2 GENERAL SPECIFICATION
The models are modular in nature. Maintain power system
stability for positive sequence dynamics like short circuit
disturbance, frequency disturbance and change in reference
values. Model should be valid for power system frequency
deviation of ±6%.Must handle the phase change control.
Steady state voltage deviation should between 0.85p.u –
1.15p.u.The typical dynamic simulation time frame of
interest is from 10 seconds to 30 seconds. It should
withstand over voltage /under voltage and over
frequency/under frequency. During power swing, turbine-
generator inertia and first drive train torsional mode are
taken into account. Protection and control systems design.
2. TYPE 3:WTWITHDOUBLY-FEDASYNCHRONOUS
GENERATORS
In this model of wind turbine both the stator and rotor are
connected to the grid through the BACK-TO -BACK POWER
CONVERTER or it is connected through any power
converters to the grid. The rotor side that is rated for partial
load. This allows an independent control of active and
reactive power within a wide speed operating range. This
form a closed loop system, so the control of speedismade by
the converters through switching devices like IGBT. There
are two parts of the converter called LSC(Line Side
Converter) and GSC(Grid Side Converter).So the reactive
power produced is compensated to the maximum extent.It
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 03 | Mar 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 3319
produces maximum efficiency even at low wind speed of 3-
5m/s. Problems such as over voltage /under voltage ride
through or over current/under current ride through gets
compensated. This model is best suited model of wind
turbine and used in all the wind farms.
2.1 MODULES OF DFIG BASED WIND TURBIBNE
1. Aerodynamic Module - One dimensional model
2. Mechanical Module - Two mass model.
3. Generator set Module
2.1.1 . AERODYNAMIC MODULE - ONE
DIMENSIONAL MODEL
The main purpose of wind turbines is to generate
energy using the wind. Hence, the aerodynamics is a very
important part of wind turbines. The wind turbine
aerodynamic and drive train block contains both the entire
mechanical representation of the wind turbineincludingthe
pitch drive and the aerodynamic model that describes the
conversion of wind speed to mechanical power.
Figure 1 - Block diagram for one-dimensional
aerodynamic model is implemented in MATLAB
The aerodynamic models presented have in common that
A large number ofparametersisrequired.Theseparameters
may to some extent be confidential and not available for
users of the model. The model is highly nonlinear, the
calculation of initial values for the simulation is therefore
possible only through iteration.Areductionofthe numberof
parameters required. The use of parameters that showclear
physical relations. A direct calculation of the initial values.
Reduction of the simulation effort.
Table 1: Parameter list for one-dimensional
aerodynamic model
2.1.2 . MECHANICAL MODULE - TWO MASS MODEL.
A two-mass model isused,several simulationsusing
a variation of the stiffness of the drive train. The impact of
using an active drive train damper in the model is compared
to a passive implementation in the model. By increasing the
damping coefficient of a two-mass drive train model, the
response of an active drive train dampercanbeemulated. .A
two-mass representation is accurate enough for
representing all relevant effects for stability studies for DFG
wind turbines. Higher order turbinerepresentationsusually
add only limited additional information at the expenseof far
more detailed models compared to a two-mass drive train.
Figure 2 - Block diagram for two mass model
mechanical model implemented in MATLAB
2.1.3 TYPE 3A GENERATOR SET MODEL
The output of the generator model is a current, injected
through a current source with parallel impedance Xs.
However, in some power system simulation software,
‘control’-parts and ‘grid’-parts of a model are treated
differently. To improve the convergence behavior of the
simulation in such cases, it is recommended to move the
parallel impedance Xs .
Symbols Base
Unit
Description Category
Θw0 deg Initial pitch angle Case
ka Pn /
deg2
Aerodynamicgain Type
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 03 | Mar 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 3320
Table 2 - Parameter list for type 3A generator set
model
Figure 3 – Block diagram for type 3A generator set
model
2.1.4 REFERENCE FRAME ROTATION
This PLL block of reference frame of rotation model is fed
with sine wave input . This block compares the sine block’s
voltage magnitude with the PLL1 magnitude voltage. This
PLL block is fed with sine wave input . This block compares
the sine block’s angle with the PLL2 magnitude voltage. The
simulation model compares the voltage and angle output of
the wind turbine terminal voltage with the PLL model. PLL1
block comparesthevoltage magnitude.PLL2block compares
the angle of the input voltage wind turbine. Angle is filtered
and/or frozen to avoid instabilities due to lack of voltage
reference.
Figure 4 – Block diagram for type 3A reference frame
model
The value of uPLL2 should be coordinated with the value of
uPLL1. Usually, uPLL2 ≤ uPLL1. uPLL2 is employed to avoid
numerical problems when voltage is close to zero and then
angle is not numerically valid. If the voltage of the PLL1 is
greater than that of PLL 2 then PLL 1 get locked gives output
1 but the PLL 2 gives the output 0.
2.1.5 GRID REFERENCE FRAME
The output of the generator model is a current, injected
through a current source with parallel impedance Xs.
However, in some power system simulation software,
‘control’-parts and ‘grid’- parts of a model are treated
differently. The losses in the generator system are neglected
setting the generator air gap power pag equal to the WT
terminal power. The air gap power and windturbinecurrent
is observed which helps to avoid malfunctioning of the wind
turbine when subjected to transients.
Figure 5 – Block diagram of grid reference frame
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 03 | Mar 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 3321
2.2 SIMULATION RESULTS
Figure 6 - Output of one dimensional aero dynamic
Simulink Model for nominal speed of the wind
Figure 7 – Output of simulink Speed of a wind turbine
rotor (ωWTR) OF TWO MASS model
Figure 8 – Output of Simulink Speed of a wind turbine
rotor ωgen of TWO MASS model
Figure 9 – output of PLL loop
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 03 | Mar 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 3322
3. CONCLUSIONS
This work mainly focused on the
development of electrical simulation models of IEC
61400-27-1 standard DOUBLY-FED INDUCTION
GENERATOR (TYPE 3A) BASED wind turbine using
MATLAB-SIMULINK. The simulation models are mainly
used by the wind turbine manufacturers who provide
parameterization for different implementations. An
electric model is designed and implemented using
standard tools which will available globally for research
works and testing purpose. These electrical models are
used for measurement and assessment of wind turbine
with the minimum number of parameters necessary to
represent all relevant effects like voltage sag, over
voltage ride through, under voltage ride through, etc.
The aerodynamic model, mechanical model, generator
set model of type 3A wind turbine is been implemented
using constant values and this model works efficiently.It
provides reactive power control and ensuresthe voltage
stability during the transient condition of the system.
Further optimizationofthe modelsusingcomplex values
will be implemented in the future work.
REFERENCES
1. Jens Fortmann, “Modeling of Wind Turbines with
Doubly Fed Generator System”, Springer Vieweg,
2014.
2. M. Berhanu, Y. Mekonnen, R. Leidhold, M. Mamo, Z.
Muluneh and A. Sarwat, “Analysis of a Doubly Fed
Induction Generator Through Modelling and
Simulation”, IEEE PES/IAS PowerAfrica. (2018)
3. Milkias Berhanu Tuka, Roberto Leidhold,Mengesha
Mamo, “Modelling and Control of a Doubly Fed
Induction Generator Using a Back-to-Back
Converters in Grid Tied Wind Power System”, IEEE
PES-IAS PowerAfrica (2017)
4. B.Chitti Babu , K.B.Mohanty “Doubly-Fed Induction
Generator for Variable Speed Wind Energy
Conversion Systems- Modelling & Simulation”,
International Journal of Computer and Electrical
Engineering, Vol. 2, No. 1, 1793-8163, 2010.
5. E. Bounadjaa,, A. Djahbarb, Z. Boudjemac, “Variable
structure control of a doubly fed induction
generator forwindenergyconversionsystems”,The
International Conference on Technologies and
Materials for Renewable Energy, Environment and
Sustainability, TMREES14, ScienceDirect, 2014.
6. Ghulam Sarwar Kaloi, Jie Wang, Mazhar Hussain
Baloch, “Active and reactive power control of the
doubly fed induction generator based on wind
energy conversion system”, 2016.
7. J.G. Slootweg, H. Polinder, W.L. Kling, “Dynamic
Modelling of a Wind Turbine with Doubly Fed
Induction Generator”, IEEE Xplore, 2001.
8. Margaris, Ioannis, Hansen, Anca Daniela, Bech,
John, Andresen, Björn Sørensen, Poul Ejnar,
“Implementation of IEC Standard Models for Power
System Stability Studies”, Proceedings of 11th
International Workshop on Large-Scale Integration
of Wind Power into Power Systems 2012.
9. LIU You-wei, CHEN Zhi-hui,SHEN Juan,“Application
of PLL in the Generator-side ConvertersforDoubly-
Fed Wind PowerGeneration Systems”,International
Conference on Future Energy, Environment, and
Materials, 2012.
10. Bakari Mwinyiwiwa, Member, IEEE, Yongzheng
Zhang, Student Member, IEEE, BaikeShen,Member,
IEEE, and Boon-Teck Ooi, Life Fellow, IEEE, “Rotor
Position Phase-Locked Loop for Decoupled P-Q
Control of DFIG for Wind Power Generation”, IEEE
TRANSACTIONS ON ENERGY CONVERSION, VOL.
24, NO. 3, SEPTEMBER 2009

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IRJET- Electrical Simulation Model of IEC 61400-27-1 Doubly-Fed Induction Generator (Type 3A) based Wind Turbine

  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 03 | Mar 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 3318 Electrical Simulation Model of IEC 61400-27-1 Doubly-Fed Induction Generator (Type 3A) Based Wind Turbine N.Bhavadharini1, B.R.Pavithra2, M.C.Lavanya3, Lavanya Dhanesh 4 1,2UG Scholars, Department of Electrical and Electronics Engineering, Panimalar Institute of Technology, Chennai 3Deputy Director, Research and Development (R&D) and Resource Data Analytic & Forecasting (RDAF), National Institute of Wind Energy, Chennai 4Associate Professor, Department of Electrical and Electronics Engineering, Panimalar Institute of Technology, Chennai ---------------------------------------------------------------------***--------------------------------------------------------------------- Abstract –The main objective of this project is to implement the Electrical Simulation Model of IEC 61400-27-1 standard TYPE 3 – DOUBLY-FED INDUCTION GENERATOR (DFIG) based wind turbine. The dynamic models of a wind turbine are designed by the manufacturers. These manufacturers provide the behavior of their machines with a high level ofdetail.Before carrying out In-situ testing of Wind Energy Conversion System(WECS), wind turbine certification institution can perform generic evaluation of the system with standard parameters by using electrical simulation models which will be effortless for the manufacturers to scrutinize the performance. Standards make sure that the products work together safely and reliably as intended. So different parameters given in the model can be able to emulate the response for a wide range of machines. By usingstandardtoolMATLAB/SIMULINK electrical simulation of IEC 61400-27-1 DOUBLY-FED INDUCTION GENERATOR based wind turbine is designed and implemented. Key Words: IEC 61400-27-1, DFIG, WECS, MATLAB/SIMULINK 1.INTRODUCTION Wind energy utilization in power system has increased greatly to meet the demand of the power system. Stability of the system is concerned by the power system operators. So the dynamic models of a wind turbine are designed by the manufacturers. Manufacturers of wind turbines commonly have all-inclusive data of wind turbine models. But thereare several drawbacks for the use of such models by grid operators. The grid operator does not have a full knowledge of the model. So generic models have been required is developed. Then a manufacturer only needs to provide a parameterization for the model. This generic model development finds the right balance between desired accuracy and model complexity. 1.1 SCOPE IEC 61400-27 specifies standard electrical simulation models for wind turbines which provides procedures for examining the specified electrical simulation models. IEC 61400-27-1 defines the universal terms and parameters with the purpose of specifying the electrical characteristics of a wind turbine. The models are described in a standard way which can be applied for future wind turbine concepts. So the dynamic simulation models are designed for wind turbine terminals. The validation procedure specified in IEC 61400-27-1 focuses on the IEC 61400-21 tests for response to voltage sag and transients condition. 1.2 GENERAL SPECIFICATION The models are modular in nature. Maintain power system stability for positive sequence dynamics like short circuit disturbance, frequency disturbance and change in reference values. Model should be valid for power system frequency deviation of ±6%.Must handle the phase change control. Steady state voltage deviation should between 0.85p.u – 1.15p.u.The typical dynamic simulation time frame of interest is from 10 seconds to 30 seconds. It should withstand over voltage /under voltage and over frequency/under frequency. During power swing, turbine- generator inertia and first drive train torsional mode are taken into account. Protection and control systems design. 2. TYPE 3:WTWITHDOUBLY-FEDASYNCHRONOUS GENERATORS In this model of wind turbine both the stator and rotor are connected to the grid through the BACK-TO -BACK POWER CONVERTER or it is connected through any power converters to the grid. The rotor side that is rated for partial load. This allows an independent control of active and reactive power within a wide speed operating range. This form a closed loop system, so the control of speedismade by the converters through switching devices like IGBT. There are two parts of the converter called LSC(Line Side Converter) and GSC(Grid Side Converter).So the reactive power produced is compensated to the maximum extent.It
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 03 | Mar 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 3319 produces maximum efficiency even at low wind speed of 3- 5m/s. Problems such as over voltage /under voltage ride through or over current/under current ride through gets compensated. This model is best suited model of wind turbine and used in all the wind farms. 2.1 MODULES OF DFIG BASED WIND TURBIBNE 1. Aerodynamic Module - One dimensional model 2. Mechanical Module - Two mass model. 3. Generator set Module 2.1.1 . AERODYNAMIC MODULE - ONE DIMENSIONAL MODEL The main purpose of wind turbines is to generate energy using the wind. Hence, the aerodynamics is a very important part of wind turbines. The wind turbine aerodynamic and drive train block contains both the entire mechanical representation of the wind turbineincludingthe pitch drive and the aerodynamic model that describes the conversion of wind speed to mechanical power. Figure 1 - Block diagram for one-dimensional aerodynamic model is implemented in MATLAB The aerodynamic models presented have in common that A large number ofparametersisrequired.Theseparameters may to some extent be confidential and not available for users of the model. The model is highly nonlinear, the calculation of initial values for the simulation is therefore possible only through iteration.Areductionofthe numberof parameters required. The use of parameters that showclear physical relations. A direct calculation of the initial values. Reduction of the simulation effort. Table 1: Parameter list for one-dimensional aerodynamic model 2.1.2 . MECHANICAL MODULE - TWO MASS MODEL. A two-mass model isused,several simulationsusing a variation of the stiffness of the drive train. The impact of using an active drive train damper in the model is compared to a passive implementation in the model. By increasing the damping coefficient of a two-mass drive train model, the response of an active drive train dampercanbeemulated. .A two-mass representation is accurate enough for representing all relevant effects for stability studies for DFG wind turbines. Higher order turbinerepresentationsusually add only limited additional information at the expenseof far more detailed models compared to a two-mass drive train. Figure 2 - Block diagram for two mass model mechanical model implemented in MATLAB 2.1.3 TYPE 3A GENERATOR SET MODEL The output of the generator model is a current, injected through a current source with parallel impedance Xs. However, in some power system simulation software, ‘control’-parts and ‘grid’-parts of a model are treated differently. To improve the convergence behavior of the simulation in such cases, it is recommended to move the parallel impedance Xs . Symbols Base Unit Description Category Θw0 deg Initial pitch angle Case ka Pn / deg2 Aerodynamicgain Type
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 03 | Mar 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 3320 Table 2 - Parameter list for type 3A generator set model Figure 3 – Block diagram for type 3A generator set model 2.1.4 REFERENCE FRAME ROTATION This PLL block of reference frame of rotation model is fed with sine wave input . This block compares the sine block’s voltage magnitude with the PLL1 magnitude voltage. This PLL block is fed with sine wave input . This block compares the sine block’s angle with the PLL2 magnitude voltage. The simulation model compares the voltage and angle output of the wind turbine terminal voltage with the PLL model. PLL1 block comparesthevoltage magnitude.PLL2block compares the angle of the input voltage wind turbine. Angle is filtered and/or frozen to avoid instabilities due to lack of voltage reference. Figure 4 – Block diagram for type 3A reference frame model The value of uPLL2 should be coordinated with the value of uPLL1. Usually, uPLL2 ≤ uPLL1. uPLL2 is employed to avoid numerical problems when voltage is close to zero and then angle is not numerically valid. If the voltage of the PLL1 is greater than that of PLL 2 then PLL 1 get locked gives output 1 but the PLL 2 gives the output 0. 2.1.5 GRID REFERENCE FRAME The output of the generator model is a current, injected through a current source with parallel impedance Xs. However, in some power system simulation software, ‘control’-parts and ‘grid’- parts of a model are treated differently. The losses in the generator system are neglected setting the generator air gap power pag equal to the WT terminal power. The air gap power and windturbinecurrent is observed which helps to avoid malfunctioning of the wind turbine when subjected to transients. Figure 5 – Block diagram of grid reference frame
  • 4. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 03 | Mar 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 3321 2.2 SIMULATION RESULTS Figure 6 - Output of one dimensional aero dynamic Simulink Model for nominal speed of the wind Figure 7 – Output of simulink Speed of a wind turbine rotor (ωWTR) OF TWO MASS model Figure 8 – Output of Simulink Speed of a wind turbine rotor ωgen of TWO MASS model Figure 9 – output of PLL loop
  • 5. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 03 | Mar 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 3322 3. CONCLUSIONS This work mainly focused on the development of electrical simulation models of IEC 61400-27-1 standard DOUBLY-FED INDUCTION GENERATOR (TYPE 3A) BASED wind turbine using MATLAB-SIMULINK. The simulation models are mainly used by the wind turbine manufacturers who provide parameterization for different implementations. An electric model is designed and implemented using standard tools which will available globally for research works and testing purpose. These electrical models are used for measurement and assessment of wind turbine with the minimum number of parameters necessary to represent all relevant effects like voltage sag, over voltage ride through, under voltage ride through, etc. The aerodynamic model, mechanical model, generator set model of type 3A wind turbine is been implemented using constant values and this model works efficiently.It provides reactive power control and ensuresthe voltage stability during the transient condition of the system. Further optimizationofthe modelsusingcomplex values will be implemented in the future work. REFERENCES 1. Jens Fortmann, “Modeling of Wind Turbines with Doubly Fed Generator System”, Springer Vieweg, 2014. 2. M. Berhanu, Y. Mekonnen, R. Leidhold, M. Mamo, Z. Muluneh and A. Sarwat, “Analysis of a Doubly Fed Induction Generator Through Modelling and Simulation”, IEEE PES/IAS PowerAfrica. (2018) 3. Milkias Berhanu Tuka, Roberto Leidhold,Mengesha Mamo, “Modelling and Control of a Doubly Fed Induction Generator Using a Back-to-Back Converters in Grid Tied Wind Power System”, IEEE PES-IAS PowerAfrica (2017) 4. B.Chitti Babu , K.B.Mohanty “Doubly-Fed Induction Generator for Variable Speed Wind Energy Conversion Systems- Modelling & Simulation”, International Journal of Computer and Electrical Engineering, Vol. 2, No. 1, 1793-8163, 2010. 5. E. Bounadjaa,, A. Djahbarb, Z. Boudjemac, “Variable structure control of a doubly fed induction generator forwindenergyconversionsystems”,The International Conference on Technologies and Materials for Renewable Energy, Environment and Sustainability, TMREES14, ScienceDirect, 2014. 6. Ghulam Sarwar Kaloi, Jie Wang, Mazhar Hussain Baloch, “Active and reactive power control of the doubly fed induction generator based on wind energy conversion system”, 2016. 7. J.G. Slootweg, H. Polinder, W.L. Kling, “Dynamic Modelling of a Wind Turbine with Doubly Fed Induction Generator”, IEEE Xplore, 2001. 8. Margaris, Ioannis, Hansen, Anca Daniela, Bech, John, Andresen, Björn Sørensen, Poul Ejnar, “Implementation of IEC Standard Models for Power System Stability Studies”, Proceedings of 11th International Workshop on Large-Scale Integration of Wind Power into Power Systems 2012. 9. LIU You-wei, CHEN Zhi-hui,SHEN Juan,“Application of PLL in the Generator-side ConvertersforDoubly- Fed Wind PowerGeneration Systems”,International Conference on Future Energy, Environment, and Materials, 2012. 10. Bakari Mwinyiwiwa, Member, IEEE, Yongzheng Zhang, Student Member, IEEE, BaikeShen,Member, IEEE, and Boon-Teck Ooi, Life Fellow, IEEE, “Rotor Position Phase-Locked Loop for Decoupled P-Q Control of DFIG for Wind Power Generation”, IEEE TRANSACTIONS ON ENERGY CONVERSION, VOL. 24, NO. 3, SEPTEMBER 2009