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K Shanmukha Rao et al Int. Journal of Engineering Research and Applications
ISSN : 2248-9622, Vol. 3, Issue 6, Nov-Dec 2013, pp.2102-2106

RESEARCH ARTICLE

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OPEN ACCESS

Analysis of Doubly Fed Induction Generator under Varies Fault
Conditions
Kappala Shanmukha Rao1, Manda vijay Kumar2
PG Scholar, Dept of EEE, GIET College Rajahmundry, AP India
Assistant Professor, Dept. of EEE, GIET College Rajahmundry, AP India
Abstract
Wind power stations much placed in remote areas; so they are characterized by weak grids and are often
submitted to power system disturbance like faults. In this paper, the behaviour of a wind energy conversion
system that uses the structure of Doubly-Fed Induction Generator (DFIG) under faulty conditions is presented.
The behavior of these machines during grid failure is an important issue. DFIG consists of an asynchronous
machine, in which the stator is connected directly to the grid and its rotor, is connected to the grid via two
electronic power converters (back-to-back converter). In the three-phase rectifier and the inverter with IGBTs
the Pulse Width Modulation (PWM) and SPWM technique is respectively used. DFIG is analysed and simulated
under varies faulty conditions in the environment of MATLAB/SIMULINK.
Index :

I.

Introduction

Wind energy technology has experienced
important gains over the last few decades [7] due to
the technological improvement of wind turbines from
fixed speed to variable speed. The Doubly Fed
Induction Generator (DFIG) has very attractive
characteristics as a wind generator in the fast growing
market. The fundamental feature of the DFIG is that
the power processed by the power converter is only a
fraction of the total power rating, that is, typically
(20-30%), and therefore its size, cost and losses are
much smaller compared to a full size power
converter.
A wind turbine with DFIG uses a frequency
converter and a pitch blade actuator to control
directly the generator speed and wind turbine output
[2]. The frequency converter has the Rotor Side
Converter (RSC) and the Grid Side Converter (GSC).
The RSC controls independently, active and reactive
power, while the GSC also controls the active power
flow through the converter by controlling the DC-link
voltage to unity.
DFIG can operate at a wider range of speeds
depending on the wind speed or other specific
operation requirements. Thus, it allows for a better
capture of wind energy [6, 11, and 12], and dynamic
slip control. Pitch control may contribute to
rebuilding the voltage at the wind turbine terminals
and maintaining the power system stability after
clearance of an external short–circuit fault [2]. In
addition, DFIGs have shown better behavior
concerning system stability during short–circuit faults
in comparison to IG, because of their capability of
decoupling the control of output active and reactive
power.

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The superior dynamic performance of the DFIG
results from the frequency converter which typically
operates with sampling and switching frequencies of
above 2 kHz [1]. At lower voltages, down to 0%, the
IGBTs (Insulated Gate Bipolar Transistors) of the
DFIG are switched off and the system remains in
standby mode [8-10, and 12]. If the voltages are
above a certain threshold value during fault, the
DFIG system is very quickly synchronized and is
back in operation again.
DFIG can operate in both sub-synchronous
and super-synchronous operation mode to impart
power to the grid or from the grid with a minimum
rotor power input in both stead and variable speed
wind turbine operation mode.
In this paper the dynamic behavior of a 1.5
MW wind farm is modelled using MATLAB. The
behaviour of the system for a single line to ground
fault is analyzed.

II.

Concept of DFIG

The basic layout of a DFIG is shown in
fig.1, Doubly fed induction generator is basically a
wound rotor induction machine with multi phase
wound rotor with multiphase slip rings assembly and
brushes enabling access to the rotor. The rotor
windings are connected to the grid through an ACDC-AC converter. The rotor and the grid currents are
controlled by controlling the converter. This enables
the control of the active power and reactive power
flow to the grid from the stator independent of the
generator’s speed. The number of turns on the rotor
of a doubly fed induction generator is 2 to 3 times
that of the stator. This means that the rotor voltages
are higher and the currents are lower. Therefore in
the typical operational speed range of +
2102 | P a g e
K Shanmukha Rao et al Int. Journal of Engineering Research and Applications
ISSN : 2248-9622, Vol. 3, Issue 6, Nov-Dec 2013, pp.2102-2106
30% of the synchronous speed, the converter has to
handle lower currents thus reducing the cost of the
converter.

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Where Wwt is the wind turbine rotor speed [rad/s]

IV.

Back-to-Back Converter

4.1 Rotor side converter (RSC)
Rotor side converter acts as a PWM rectifier
during the machine working in super synchronous
mode and as an inverter during sub synchronous
mode. The purpose of the rotor side converter’s
control is the independent control of the rotor’s active
and reactive power. To succeed it, the voltages and
the currents are transformed in d-, q- synchronously
reference frame, where the d-axis is aligned with the
air gap’s flux vector.

Figure. 1: Doubly fed induction generator.
A doubly fed induction generator has the
advantage that power can be imported from or
exported to the grid through the power electronics
converter. This allows the system to support the grid
during severe voltage disturbances thus improving
the system stability. By controlling the rotor voltages
and currents the synchronization of the machine with
the grid is maintained even when the wind speed
varies. Under light load conditions, the wind energy
is utilized more efficiently than a fixed speed wind
turbine. Only 25-30 % of the power is fed to the grid
through the converter while the remaining is fed
directly to the grid. Due to this reason, the cost of the
converter is low and the efficiency of the doubly fed
induction generator is good.

III.

Wind Turbine Model

It is well-known that the relation between
the wind speed and aerodynamic power is described
by the following equation:

and the corresponding torque is expressed as

where Pw is the aerodynamic power extracted from
the wind [W], Tw is the corresponding aerodynamic
torque [Nm], ρ the air density [kg/m3], R the wind
turbine rotor radius [m], vw the equivalent wind
speed [m/s], β the pitch angle of rotor [deg], Cp the
power coefficient with its maximum value at 0.59
(Betz limit) and λ is the tip speed ratio given by the
following equation:

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Figure 2: Rotor side converter control system
4.2 Grid Side Converter (GSC)
The grid side converter acts as a PWM
inverter during the machine working in super
synchronous mode and as a rectifier during sub
synchronous mode. In sub synchronous mode, the
rotor’s power is coming from the capacitor of the DC
link, so the voltage interconnection is dropped down.
This leads to power transportation from the grid to
the capacitor. In super synchronous mode the rotor
feeds the capacitor, its voltage increases and the grid
side converter transfers active power to the grid.
Moreover, the reactive power that is exchanged
between grid side converter and the grid, can be
controlled. In our case the upper IGBTs of the GSC
are always off, while the corresponding parallel
diodes conduct.
The control of this converter is achieved by
transforming the three phase quantities to d-, qsynchronously frame, in which the d-axis is aligned
with the vector of the grid’s voltage, because grid’s
voltage is constant.

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K Shanmukha Rao et al Int. Journal of Engineering Research and Applications
ISSN : 2248-9622, Vol. 3, Issue 6, Nov-Dec 2013, pp.2102-2106

Figure 5: Three phase to Ground fault (a) Voltage at
DFIG (b) Current at DFIG (c) Voltage at Line (d)
Currents at Line.

Figure 3: Grid side converter control system.
The converter Cgrid is used to regulate the
voltage of the DC bus capacitor. In addition, this
model allows using Cgrid converter to generate or
absorb reactive power. The system consists of an
outer regulation loop consisting of a DC voltage
regulator. The output of the DC voltage regulator is
the reference current Idgc_ref for the current
regulator. The inner current regulation loop consists
of a current regulator. The current regulatory controls
the magnitude and phase of the voltage generated by
converter Cgrid (Vgc) from the Idgc_ref produced by
the DC voltage regulator and specified Iq_ref
reference. The current regulator is assisted by feed
forward terms which predict the Cgrid output
voltage.

V.

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Figure 6: (a) Active power (b) Reactive power (c) V dc
(d) Turbine speed (Wr).

Simulation Results

A 9 MW DFIG is simulated using
MATLAB/Simulink. As shown in figure.4 of
simulink model of doubly fed induction generator
under fault condition. A three phase fault is created at
the generator terminal at t=0.1s and cleared at t
=0.15s.Fig.5 shows the voltage and current
waveforms at the generator terminal and close to MV
bus. During the fault, voltages of all three phases
reach ver y low values as sho wn in F i g . 5. Ideally
this should reach to zero, but in practice, there will be
some fault resistance and hence will have a ver y
small magnitude voltage values. Generator terminal
current will suddenly increase at the instant of fault
initiation followed by a rapid decay as determined by
the transient impedance of the generator.

Figure 7: Single phase to Ground fault (a) Voltage at
DFIG (b) Current at DFIG (c) Voltage at Line (d)
current at DFIG

A

Discrete,
Ts = 5e-006 s.

B
C

15

Wind (m/s)

0

Qref _pu

Three-Phase Fault

<Vdc_V>

A
A
N

B
C

120 kV

A
B
C

A
B
C

aA

A

a

aA

bB

B

b

bB

cC

2500 MVA
B120
X0/X1=3 (120 kV)

C

N
3.3ohms

c

120 kV/25 kV
47 MVA
A
B
C

Grounding
Transformer

cC

B25
(25 kV)

A
B
C

A
B
C
30 km line

A

a
b

bB

C

c

<wr_pu (IG speed)>

aA

B

m

cC

B575
25 kV/ 575 V
6*1.75MVA (575 V)

B

<P_pu>

C

<Q_pu>

[wr]
[P_pu]
[Q_pu]

DFIG Wind Turbine

9 MW Wind Farm
(6 x 1.5 MW)
Vabc_B575
Iabc_B575

Vabc_B575 (pu)
Iabc_B575 (pu)

[P_pu]
[Q_pu]

Q (Mv ar)

[wr]
Vabc_B25
Iabc_B25

P (MW)

-KMW
[Vdc]

Vdc (V)
wr (pu)

Vabc_B25 (pu)
Iabc_B25 (pu)

Scope

Figure 4: Simulink model of DFIG under faults.
www.ijera.com

[Vdc]

Figure 8: (a) Active power (b) Reactive power (c)
Vdc (d) Turbine speed (Wr).
2104 | P a g e
K Shanmukha Rao et al Int. Journal of Engineering Research and Applications
ISSN : 2248-9622, Vol. 3, Issue 6, Nov-Dec 2013, pp.2102-2106

Figure 9: Two phase to ground faul (a) Voltage at
DFIG (b) Current at DFIG (c) Voltage at Line (d)
Currents at Line.

Figure 10: (a) Active power (b) Reactive power (c)
Vdc (d) Turbine speed (Wr).

Figure 10: Without any fault condition (a) Active
power (b) Reactive power (c) Vdc (d) Turbine speed
(Wr).

In this paper 9 MW wind farm is modelled
using MATLAB. The effect of Phase to Ground Fault
in phase A is analyzed for the 9 MW doubly fed
Induction Generator wind farm unit and similarly two
phase to ground fault and three phase fault. Even
though the per unit value fells the system will recover
it. In case Line to Line fault occurs the system will
recover it up to 0.5 p.u voltage drop (drips it) and
increases the Active power and decrease the reactive
power. This gives the profitable operation and the
interconnected systems are protected.

VI.

Figure 11: Without any fault in DFIG (a) Voltage at
DFIG (b) Current at DFIG (c) Voltage at Line (d)
Currents at Line.

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Conclusion

In this paper a variable speed wind
generation system based on DFIG under power
system disturbance has been simulated and a suitable
controller is designed to supply the deficit reactive
power to the grid and help in grid recovery. By as the
generator and converter stay connected, the
synchronism of operation remain established during
and after the fault and normal operation can be
continued immediately after the fault has been
cleared. Here the reactive power is being supplied to
the grid during longer duration voltage dips in order
to facilitate voltage restoration. Proper controller
designed is adopted to improve the transient and
dynamic performance of DFIG coupled Wind turbine
under these abnormal grid conditions. This paper
2105 | P a g e
K Shanmukha Rao et al Int. Journal of Engineering Research and Applications
ISSN : 2248-9622, Vol. 3, Issue 6, Nov-Dec 2013, pp.2102-2106
analyzes the DFIG transient behavior and control
possibility under grid disturbances like fault and large
voltage dips etc. In this model, with the help of only
one rotor side converter we are able to control the
active and reactive power and maintain the stability
of grid under faulty conditions.

References
[1].

R.Datta and v.t.ranganathan, sep.2002,
“variable speed wind power generation
using doubly fed wound rotor induction
machine-a comparisition with alternate
schemes”,
IEEE
Trans.Energy
convers.,vol.17,no.3,pp.414-421.
[2]. S. Muller, M. Deicke, and R. W. D.
Doncker,“Doubly fed inductiongenerator
systems for wind turbine,” IEEE Ind. Appl.
Mag., vol. 8, no. 3,pp.26–33, May/Jun.
2002.
[3]. Hoboken, NJ: Wiley T.Ackermann,
2005,”wind power in power systems.
[4]. Peng Zhou, Yikang He, and Dan Sun,
Nov2009, “Improved Direct Power Control
of a DFIG-based Wind turbine during
Network unbalance”, IEEE Trans. Power
Electronics, vol.24, no.11.
[5]. Ned Mohan, Ted K. A. Brekken “Control of
a Doubly Fed Induction Wind Generator
Under
Unbalanced
Grid
Voltage
Conditions” IEEE Transaction Energy
conversion, vol.no22. 1, march 2007 page
129-135.
[6]. Ekanayake, J.B.; Holdsworth, L.; XueGuang
Wu; Jenkins, N “Dynamic Modeling of
Doubly Fed Induction Generator Wind
Turbines”.;
Power
Systems,
IEEE
Transactions on Volume 18, Issue 2, May
2003 Page(s):803.
[7]. Johan Morren , Sjoerd W. H. de Haan “ Ride
through of Wind Turbines with Doubly-Fed
Induction Generator During a Voltage Dip”
IEEE Transaction on energy conversion,
VOL. 20, NO. 2, JUNE 2005 435-441.
[8]. Paul C. Krause ,Oleg Wasynczuk “Analysis
of electrical machines & Drive system”
IEEE, ISBN 9812-53-150-2,2007.
[9]. R. Pena, J. C. Clare, and G. M. Asher,
“Doubly fed induction generator using backto-back PWM converters and its application
to variable-speed wind-energy generation,”
IEE Proc. Electr. Power Appl., vol. 143, pp.
231-241, May 1996.
[10]. D. G. Giaourakis, A. Safacas, “Review of
Wind Energy Conversion Systems for Large
Wind Turbines and Simulation of a back-toback
Electronic
Power
Converter”,
Ever2011, Monte Carlo, Monaco, 31 March3 April 2011, conference proceedings.
[11]. H. Polinder and J. Morren, “Developments
in wind turbine generator systems”,
www.ijera.com

www.ijera.com

Electrimacs 2005, Hammamet, Tunisia,
conference proceedings.
[12]. Santos, S. and H.T. Le. 2007. “Fundamental
Time-Domain Wind Turbine Models for
Wind Power Studies”. Renewable Energy.
32:2436-2452.
[13]. H.
Späth,
Steuerverfahren
für
Drehstrommaschinen:
Theoretische
Grundlagen. Berlin, Germany: SpringerVerlag, 1983.

Biography
Mr. Kappala Shanmukha rao
obtained his B.Tech in Electrical and
Electronics Engineering from Prajna
institute
of
technology
and
management.
He
is
pursuing
M.TECH in Power Systems from
Godavari institute of technology and management,
Rajahmundry, Andhra Pradesh, India. His areas of
interest include Power Systems and FACTS.
Mr. Manda Vijay Kumar obtained
his B.Tech in Electrical and
Electronics Engineering from
Mother Theresa Engineering
College. He received his M.TECH
from Jerusalem College of
engineering in MEPED, Chennai,
India. His areas of interest include Power Electronics,
Electrical Machines and Power systems.

2106 | P a g e

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Mh3621022106

  • 1. K Shanmukha Rao et al Int. Journal of Engineering Research and Applications ISSN : 2248-9622, Vol. 3, Issue 6, Nov-Dec 2013, pp.2102-2106 RESEARCH ARTICLE www.ijera.com OPEN ACCESS Analysis of Doubly Fed Induction Generator under Varies Fault Conditions Kappala Shanmukha Rao1, Manda vijay Kumar2 PG Scholar, Dept of EEE, GIET College Rajahmundry, AP India Assistant Professor, Dept. of EEE, GIET College Rajahmundry, AP India Abstract Wind power stations much placed in remote areas; so they are characterized by weak grids and are often submitted to power system disturbance like faults. In this paper, the behaviour of a wind energy conversion system that uses the structure of Doubly-Fed Induction Generator (DFIG) under faulty conditions is presented. The behavior of these machines during grid failure is an important issue. DFIG consists of an asynchronous machine, in which the stator is connected directly to the grid and its rotor, is connected to the grid via two electronic power converters (back-to-back converter). In the three-phase rectifier and the inverter with IGBTs the Pulse Width Modulation (PWM) and SPWM technique is respectively used. DFIG is analysed and simulated under varies faulty conditions in the environment of MATLAB/SIMULINK. Index : I. Introduction Wind energy technology has experienced important gains over the last few decades [7] due to the technological improvement of wind turbines from fixed speed to variable speed. The Doubly Fed Induction Generator (DFIG) has very attractive characteristics as a wind generator in the fast growing market. The fundamental feature of the DFIG is that the power processed by the power converter is only a fraction of the total power rating, that is, typically (20-30%), and therefore its size, cost and losses are much smaller compared to a full size power converter. A wind turbine with DFIG uses a frequency converter and a pitch blade actuator to control directly the generator speed and wind turbine output [2]. The frequency converter has the Rotor Side Converter (RSC) and the Grid Side Converter (GSC). The RSC controls independently, active and reactive power, while the GSC also controls the active power flow through the converter by controlling the DC-link voltage to unity. DFIG can operate at a wider range of speeds depending on the wind speed or other specific operation requirements. Thus, it allows for a better capture of wind energy [6, 11, and 12], and dynamic slip control. Pitch control may contribute to rebuilding the voltage at the wind turbine terminals and maintaining the power system stability after clearance of an external short–circuit fault [2]. In addition, DFIGs have shown better behavior concerning system stability during short–circuit faults in comparison to IG, because of their capability of decoupling the control of output active and reactive power. www.ijera.com The superior dynamic performance of the DFIG results from the frequency converter which typically operates with sampling and switching frequencies of above 2 kHz [1]. At lower voltages, down to 0%, the IGBTs (Insulated Gate Bipolar Transistors) of the DFIG are switched off and the system remains in standby mode [8-10, and 12]. If the voltages are above a certain threshold value during fault, the DFIG system is very quickly synchronized and is back in operation again. DFIG can operate in both sub-synchronous and super-synchronous operation mode to impart power to the grid or from the grid with a minimum rotor power input in both stead and variable speed wind turbine operation mode. In this paper the dynamic behavior of a 1.5 MW wind farm is modelled using MATLAB. The behaviour of the system for a single line to ground fault is analyzed. II. Concept of DFIG The basic layout of a DFIG is shown in fig.1, Doubly fed induction generator is basically a wound rotor induction machine with multi phase wound rotor with multiphase slip rings assembly and brushes enabling access to the rotor. The rotor windings are connected to the grid through an ACDC-AC converter. The rotor and the grid currents are controlled by controlling the converter. This enables the control of the active power and reactive power flow to the grid from the stator independent of the generator’s speed. The number of turns on the rotor of a doubly fed induction generator is 2 to 3 times that of the stator. This means that the rotor voltages are higher and the currents are lower. Therefore in the typical operational speed range of + 2102 | P a g e
  • 2. K Shanmukha Rao et al Int. Journal of Engineering Research and Applications ISSN : 2248-9622, Vol. 3, Issue 6, Nov-Dec 2013, pp.2102-2106 30% of the synchronous speed, the converter has to handle lower currents thus reducing the cost of the converter. www.ijera.com Where Wwt is the wind turbine rotor speed [rad/s] IV. Back-to-Back Converter 4.1 Rotor side converter (RSC) Rotor side converter acts as a PWM rectifier during the machine working in super synchronous mode and as an inverter during sub synchronous mode. The purpose of the rotor side converter’s control is the independent control of the rotor’s active and reactive power. To succeed it, the voltages and the currents are transformed in d-, q- synchronously reference frame, where the d-axis is aligned with the air gap’s flux vector. Figure. 1: Doubly fed induction generator. A doubly fed induction generator has the advantage that power can be imported from or exported to the grid through the power electronics converter. This allows the system to support the grid during severe voltage disturbances thus improving the system stability. By controlling the rotor voltages and currents the synchronization of the machine with the grid is maintained even when the wind speed varies. Under light load conditions, the wind energy is utilized more efficiently than a fixed speed wind turbine. Only 25-30 % of the power is fed to the grid through the converter while the remaining is fed directly to the grid. Due to this reason, the cost of the converter is low and the efficiency of the doubly fed induction generator is good. III. Wind Turbine Model It is well-known that the relation between the wind speed and aerodynamic power is described by the following equation: and the corresponding torque is expressed as where Pw is the aerodynamic power extracted from the wind [W], Tw is the corresponding aerodynamic torque [Nm], ρ the air density [kg/m3], R the wind turbine rotor radius [m], vw the equivalent wind speed [m/s], β the pitch angle of rotor [deg], Cp the power coefficient with its maximum value at 0.59 (Betz limit) and λ is the tip speed ratio given by the following equation: www.ijera.com Figure 2: Rotor side converter control system 4.2 Grid Side Converter (GSC) The grid side converter acts as a PWM inverter during the machine working in super synchronous mode and as a rectifier during sub synchronous mode. In sub synchronous mode, the rotor’s power is coming from the capacitor of the DC link, so the voltage interconnection is dropped down. This leads to power transportation from the grid to the capacitor. In super synchronous mode the rotor feeds the capacitor, its voltage increases and the grid side converter transfers active power to the grid. Moreover, the reactive power that is exchanged between grid side converter and the grid, can be controlled. In our case the upper IGBTs of the GSC are always off, while the corresponding parallel diodes conduct. The control of this converter is achieved by transforming the three phase quantities to d-, qsynchronously frame, in which the d-axis is aligned with the vector of the grid’s voltage, because grid’s voltage is constant. 2103 | P a g e
  • 3. K Shanmukha Rao et al Int. Journal of Engineering Research and Applications ISSN : 2248-9622, Vol. 3, Issue 6, Nov-Dec 2013, pp.2102-2106 Figure 5: Three phase to Ground fault (a) Voltage at DFIG (b) Current at DFIG (c) Voltage at Line (d) Currents at Line. Figure 3: Grid side converter control system. The converter Cgrid is used to regulate the voltage of the DC bus capacitor. In addition, this model allows using Cgrid converter to generate or absorb reactive power. The system consists of an outer regulation loop consisting of a DC voltage regulator. The output of the DC voltage regulator is the reference current Idgc_ref for the current regulator. The inner current regulation loop consists of a current regulator. The current regulatory controls the magnitude and phase of the voltage generated by converter Cgrid (Vgc) from the Idgc_ref produced by the DC voltage regulator and specified Iq_ref reference. The current regulator is assisted by feed forward terms which predict the Cgrid output voltage. V. www.ijera.com Figure 6: (a) Active power (b) Reactive power (c) V dc (d) Turbine speed (Wr). Simulation Results A 9 MW DFIG is simulated using MATLAB/Simulink. As shown in figure.4 of simulink model of doubly fed induction generator under fault condition. A three phase fault is created at the generator terminal at t=0.1s and cleared at t =0.15s.Fig.5 shows the voltage and current waveforms at the generator terminal and close to MV bus. During the fault, voltages of all three phases reach ver y low values as sho wn in F i g . 5. Ideally this should reach to zero, but in practice, there will be some fault resistance and hence will have a ver y small magnitude voltage values. Generator terminal current will suddenly increase at the instant of fault initiation followed by a rapid decay as determined by the transient impedance of the generator. Figure 7: Single phase to Ground fault (a) Voltage at DFIG (b) Current at DFIG (c) Voltage at Line (d) current at DFIG A Discrete, Ts = 5e-006 s. B C 15 Wind (m/s) 0 Qref _pu Three-Phase Fault <Vdc_V> A A N B C 120 kV A B C A B C aA A a aA bB B b bB cC 2500 MVA B120 X0/X1=3 (120 kV) C N 3.3ohms c 120 kV/25 kV 47 MVA A B C Grounding Transformer cC B25 (25 kV) A B C A B C 30 km line A a b bB C c <wr_pu (IG speed)> aA B m cC B575 25 kV/ 575 V 6*1.75MVA (575 V) B <P_pu> C <Q_pu> [wr] [P_pu] [Q_pu] DFIG Wind Turbine 9 MW Wind Farm (6 x 1.5 MW) Vabc_B575 Iabc_B575 Vabc_B575 (pu) Iabc_B575 (pu) [P_pu] [Q_pu] Q (Mv ar) [wr] Vabc_B25 Iabc_B25 P (MW) -KMW [Vdc] Vdc (V) wr (pu) Vabc_B25 (pu) Iabc_B25 (pu) Scope Figure 4: Simulink model of DFIG under faults. www.ijera.com [Vdc] Figure 8: (a) Active power (b) Reactive power (c) Vdc (d) Turbine speed (Wr). 2104 | P a g e
  • 4. K Shanmukha Rao et al Int. Journal of Engineering Research and Applications ISSN : 2248-9622, Vol. 3, Issue 6, Nov-Dec 2013, pp.2102-2106 Figure 9: Two phase to ground faul (a) Voltage at DFIG (b) Current at DFIG (c) Voltage at Line (d) Currents at Line. Figure 10: (a) Active power (b) Reactive power (c) Vdc (d) Turbine speed (Wr). Figure 10: Without any fault condition (a) Active power (b) Reactive power (c) Vdc (d) Turbine speed (Wr). In this paper 9 MW wind farm is modelled using MATLAB. The effect of Phase to Ground Fault in phase A is analyzed for the 9 MW doubly fed Induction Generator wind farm unit and similarly two phase to ground fault and three phase fault. Even though the per unit value fells the system will recover it. In case Line to Line fault occurs the system will recover it up to 0.5 p.u voltage drop (drips it) and increases the Active power and decrease the reactive power. This gives the profitable operation and the interconnected systems are protected. VI. Figure 11: Without any fault in DFIG (a) Voltage at DFIG (b) Current at DFIG (c) Voltage at Line (d) Currents at Line. www.ijera.com www.ijera.com Conclusion In this paper a variable speed wind generation system based on DFIG under power system disturbance has been simulated and a suitable controller is designed to supply the deficit reactive power to the grid and help in grid recovery. By as the generator and converter stay connected, the synchronism of operation remain established during and after the fault and normal operation can be continued immediately after the fault has been cleared. Here the reactive power is being supplied to the grid during longer duration voltage dips in order to facilitate voltage restoration. Proper controller designed is adopted to improve the transient and dynamic performance of DFIG coupled Wind turbine under these abnormal grid conditions. This paper 2105 | P a g e
  • 5. K Shanmukha Rao et al Int. Journal of Engineering Research and Applications ISSN : 2248-9622, Vol. 3, Issue 6, Nov-Dec 2013, pp.2102-2106 analyzes the DFIG transient behavior and control possibility under grid disturbances like fault and large voltage dips etc. In this model, with the help of only one rotor side converter we are able to control the active and reactive power and maintain the stability of grid under faulty conditions. References [1]. R.Datta and v.t.ranganathan, sep.2002, “variable speed wind power generation using doubly fed wound rotor induction machine-a comparisition with alternate schemes”, IEEE Trans.Energy convers.,vol.17,no.3,pp.414-421. [2]. S. Muller, M. Deicke, and R. W. D. Doncker,“Doubly fed inductiongenerator systems for wind turbine,” IEEE Ind. Appl. Mag., vol. 8, no. 3,pp.26–33, May/Jun. 2002. [3]. Hoboken, NJ: Wiley T.Ackermann, 2005,”wind power in power systems. [4]. Peng Zhou, Yikang He, and Dan Sun, Nov2009, “Improved Direct Power Control of a DFIG-based Wind turbine during Network unbalance”, IEEE Trans. Power Electronics, vol.24, no.11. [5]. Ned Mohan, Ted K. A. Brekken “Control of a Doubly Fed Induction Wind Generator Under Unbalanced Grid Voltage Conditions” IEEE Transaction Energy conversion, vol.no22. 1, march 2007 page 129-135. [6]. Ekanayake, J.B.; Holdsworth, L.; XueGuang Wu; Jenkins, N “Dynamic Modeling of Doubly Fed Induction Generator Wind Turbines”.; Power Systems, IEEE Transactions on Volume 18, Issue 2, May 2003 Page(s):803. [7]. Johan Morren , Sjoerd W. H. de Haan “ Ride through of Wind Turbines with Doubly-Fed Induction Generator During a Voltage Dip” IEEE Transaction on energy conversion, VOL. 20, NO. 2, JUNE 2005 435-441. [8]. Paul C. Krause ,Oleg Wasynczuk “Analysis of electrical machines & Drive system” IEEE, ISBN 9812-53-150-2,2007. [9]. R. Pena, J. C. Clare, and G. M. Asher, “Doubly fed induction generator using backto-back PWM converters and its application to variable-speed wind-energy generation,” IEE Proc. Electr. Power Appl., vol. 143, pp. 231-241, May 1996. [10]. D. G. Giaourakis, A. Safacas, “Review of Wind Energy Conversion Systems for Large Wind Turbines and Simulation of a back-toback Electronic Power Converter”, Ever2011, Monte Carlo, Monaco, 31 March3 April 2011, conference proceedings. [11]. H. Polinder and J. Morren, “Developments in wind turbine generator systems”, www.ijera.com www.ijera.com Electrimacs 2005, Hammamet, Tunisia, conference proceedings. [12]. Santos, S. and H.T. Le. 2007. “Fundamental Time-Domain Wind Turbine Models for Wind Power Studies”. Renewable Energy. 32:2436-2452. [13]. H. Späth, Steuerverfahren für Drehstrommaschinen: Theoretische Grundlagen. Berlin, Germany: SpringerVerlag, 1983. Biography Mr. Kappala Shanmukha rao obtained his B.Tech in Electrical and Electronics Engineering from Prajna institute of technology and management. He is pursuing M.TECH in Power Systems from Godavari institute of technology and management, Rajahmundry, Andhra Pradesh, India. His areas of interest include Power Systems and FACTS. Mr. Manda Vijay Kumar obtained his B.Tech in Electrical and Electronics Engineering from Mother Theresa Engineering College. He received his M.TECH from Jerusalem College of engineering in MEPED, Chennai, India. His areas of interest include Power Electronics, Electrical Machines and Power systems. 2106 | P a g e