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JOURNAL TITLE ‐ MONTH YEAR 1
Voltage Control in Wind Power Generation
Using Doubly Fed Induction Generators E. Toledo*1, L. Aromataris2, G. Tarnowski3, M. Oliveira4, O. Perrone5, H. Reversat6
Energy Study Center to Development (CEED), National University of Misiones (UNaM)
Oberá, Misiones, Argentina
*[email protected]; [email protected]; [email protected]; [email protected]; [email protected]
Electric Power System Analysis Group (GASEP), National University of Río Cuarto (UNRC)
Rio Cuarto, Córdoba, Argentina
Abstract
In recent years around the world, conventional generation
plants are being replaced by wind power plants. The rapid
development of wind power generation brings new
requirements for the integration of wind turbines to the
Electric Power Systems. These requirements establish that
the new technologies must provide ancillary services similar
to those of conventional plants, such as voltage control in
steady state and voltage control during faults occurring close
to the wind power plant. This paper explores and compares
the performance of two different alternatives of voltage
control using doubly fed induction generator (DFIG)
topology, which is the most used wind generation
technology nowadays. This performance is investigated in a
transmission network to a disturbance which endangers the
stability of long term voltage thereof. In the first case, the
voltage control of the terminal bus of the wind plant will be
performed only through the rotor‐side converter, while in
the second case; the voltage control will also have the
additional contribution of the reactive power delivered by
the grid side converter. The results show the importance of
this additional contribution of the reactive power to voltage
system stability.
Keywords
Wind Power; Voltage Stability; Voltage Control; Doubly Fed
Induction Generator (DFIG); LVRT; Coordinated Control;
Reactive Power Control; Control Strategies; DFIG Model.
Introduction
The rapid development of wind power generation
brings new requirements for the integration of the
wind turbines to the grid. These requirements are
related to ancillary services that wind turbines can
offer, such as voltage control and the ability to remain
connected during voltage dips (LVRT). [1]
Not all wind generation technologies are capable of
providing auxiliary services. Within existing
technologies, the most widespread is the doubly fed
induction generator (DFIG), which has the ability to
contribute with reactive power to the network voltage
control [2]. In this turbine, the stator circuit is
connected directly to the network while the rotor
circuit is connected via an electronic converter. The
power passes through the converter between 20 and
30% of the nominal power range depending only on
the variation of slip and reactive power requirements.
The losses in the power electronic converter are
reduced, compared with a system where the total
power must be converted as in the wind turbine
generator which is synchronous. This reduces the cost
of the converter which is smaller in size. As it is a
variable speed wind machine, it reduces voltage
fluctuations in the point of connection to the network
and allows having an independent control of the
active and reactive power which is delivered to the
network [3]. Another benefit is that one can adjust the
rotor speed according to the speed of the wind, so that
aerodynamic efficiency is optimal. The voltage control
through DFIG has been discussed in various papers.
Dynamic simulations illustrating the voltage control
action in variable speed turbine is presented in [4].
This article compares the different steady‐state current
of the rotor‐side converter (RSC), for different
scenarios of absorption and generation of reactive
power (Q). However, it does not consider the
contribution of the reactive power that can be
delivered by the grid side converter (GSC). Capacity
2 JOURNAL TITLE ‐ MONTH YEAR
limits to deliver reactive power from the DFIG stator is
studied in [5], but this study does not consider the
contribution of the GSC. Different voltage control
algorithms are suggested in [6], in which only the GSC
is used, without considering the significant
contributions provide by the RSC. This paper
compares the behaviour of a highly loaded
transmission network whose reactive power
requirements are close to the limit available. Under
these circumstances, a disturbance will be applied
which endangers the stability of long‐term voltage.
Not only will the conventional voltage control
produced by synchronous machines be considered,
but also the voltage control provided by a wind park
made up of DFIG turbines. In the first case, it is
considered that the voltage control in the terminal bus
of the wind turbine will be performed by the rotor‐
side converter (RSC), a system commonly used for this
type of machines, providing active and reactive power
independently. The grid side converter, GSC,
maintains a constant dc‐link voltage and adjusts
reactive power absorbed from the grid by the GSC. In
the second case, both RSC and GSC converters may
control the voltage and provide active and reactive
power. The results show that in the second case, the
additional power supply can be determinant to
maintain the voltage stability of the system.
Reactive power capability of DFIG
Fig. 1 shows the diagram of a generator DFIG where
we can see a mechanical gear system that couples the
blades with the asynchronous generator. It can also be
observed the direct connection from the stator to the
transmission network. The rotor is connected to an
electronic converter back‐to‐back which comprises two
independent electronic devices separated by a bus
which maintains a constant DC voltage level. On the
rotor side converter, it can be appreciated the RSC. On
the grid side is shown the GSC. Figure 1 shows the
schematic diagram of the DFIG system.
FIG. 1 ‐ SCHEMATIC DIAGRAM OF THE DFIG
The rotor side converter, RSC, controls the active and
reactive power of the machine independently. This
control is performed through the d q axes, which are
referenced in the stator system and are orthogonal to
each other. Thus, the d component of the rotor current
is used to control the reactive power and the q
component of the rotor current is used to control the
torque of the wind turbine. This control consists of two
cascaded PI control. The first is the PQ control, which
receives the active and reactive power measured in the
network and compares them with the reference,
passing later to the PI control that outputs the
reference currents. These signals enter the second
control, that is to say the current control, which
compares these references with the measured currents
and after a new PI control, the rotor voltage is changed
[7]. The GSC maintains the DC voltage at a set value
which is independent of the magnitude and direction
of the rotor power. In this case, the converter only
exchanges active power with the network. Therefore,
the exchange of reactive power from the DFIG is done
through the stator. Nonetheless, if an additional PI
control that takes into account the error signal voltage
is added to the GSC, is possible that the machine can
also issue additional reactive power through this
converter, increasing the supply of reactive power in
situations in which it is required.
a) b)
FIG. 2 ‐ POWERFACTORY LIBRARY MODELS. A) MODEL
INTEGRATED DFIG B) DFIG DETAILED MODEL
To perform the power system simulations on the
electric system being studied and model both types of
DFIG controls, the PowerFactory DigSilent software
was used. This software has a library model of the
DFIG which includes both types of controls. One of
the models is integrated, that is to say, the generator
and GSC and RSC controls form a block in which the
user does not have access to intermediate variables.
This model controls the terminal voltage only through
the RSC, while the GSC emits or consumes only active
power (Fig. 2.a). The library also offers another
alternative where the plant components are modeled
JOURNAL TITLE ‐ MONTH YEAR 3
separately (Fig. 2.b) [8]. In this way, intermediate
controls can be accessed so that the GSC can provide a
portion of the reactive power in order to cooperate
with the control voltage.
Case Study
As a case study, a system consisting of 14 buses
composed of different elements was considered. In fig.
3, it can be observed its topology.
FIG. 3 ‐ SYSTEM OF 14 BUSES
The generating park consists of two plants with
synchronous machines and a park with wind
generation. The demand is concentrated in three buses
where 50% of the load was modeled as static and the
other 50% as induction motors. The system has six
transformers with on load tap charguer(OLTC). Below
are the main features of the foregoing:
TABLE 1 ‐ SYNCHRONOUS GENERATORS
Generator 1 Generator 2
S rate
(MVA)
110 300
V rate
(KV)
16,5 18
Controls IEEEX1 (voltage
regulator)
IEEEX1 (voltage
regulator)
IEEEG3 (speed
regulator)
IEEEG3 (speed
regulator)
MAXEX2 (exitation
regulator)
lMAXEX2 (exitation
regulator)
TABLE 2 ‐ WIND FARM
Machine
type
S rate
(MVA)
DFIG
2,22
V rate
(KV)
0,69
TABLE 3 ‐ TABLE 4 ‐ MOTORS
Motor
1
Motor
2
Motor
3
Power rate
(MVA)
28 28 28
Voltage rate
(KV)
6 6 6
TABLE 5 ‐ LOADS IN GENERAL
Load 1 Load 2 Load 3
Type of load static static static
Active Power
(MW)
100 75 50
Reactive Power
(MVAr)
50 35 25
Voltage rate (KV) 6 6 6
Simulations
The simulations consider two cases:
a) The wind farm is modeled by 57 DFIG machines
which controls the terminal voltage of the converter
through CSR
b) The wind farm 57 is modeled by DFIG machines
where the terminal voltage is controlled through RSC
converters and GSC.
The fault that is applied in both simulations
corresponds to a short circuit and disconnection phase
with clearance in one of the lines of the system.
Output curves show the behavior of the network
variables for each case:
Case 1 ‐ Wind farm voltage control through CSR
The base case shows that before the disturbance
voltage levels are within acceptable limits. The
synchronous machines are generating reactive power
to the limit of its capacity. The wind farm is operating
at the nominal point of its capacity of active and
reactive power.
At the time of 1 second, the fault is applied on the line
wich connecting the bus 8 and 9. At 120 milliseconds
occurs the clearing of the fault and the outage of the
line. At 55 seconds, the limiter of overexcitation
(MAXEX2) of the synchronous generator 2 acts and
the terminal voltage drops progressively to the value
corresponding to the admissible field voltage. At 59
seconds, the MAXEX2 of the synchronous generator 1
acts and produces the same phenomenon occurred
with the generator 2 (Figure 4). During all this time the
transformers with load tap changers acted to recover
the voltage on the demand producing, in this way, the
4 JOURNAL TITLE ‐ MONTH YEAR
recovery of the active and reactive power of the static
Load. This process which finally reached the limit of
tap‐changer, needed the contribution of reactive
power from generators and caused, in part, the action
of the limiters MAXEX2. The wind farm kept their
terminal voltages, active and reactive power (Figure 6
and 8) at approximately constant values until the
action of MAXEX2 limiters occurred. After this, there
is a significant increase of the reactive power to sustain
DFIG voltage values at the expense of the decrease of
the active power generated thereby. The charging
voltages (Figure 10) drop to unacceptable values
which are typical in a scenario of voltage instability.
This is shown in the following table:
TABLE 6 ‐ VOLTAGE IN THE LOAD BUSES
Voltage
before the
fault (p.u.)
Voltage
after the
fault (p.u)
Load
1
0,95 0,84
Load
2
0,99 0,83
Load
3
0,98 0,71
Case 2 ‐ Wind farm with voltage control by RSC and
GSC
The base case is the same as case 1.
At the time of 1 second, the fault is applied on the line
connecting bus 8 and 9. At 120 milliseconds occurs the
clearing of the fault and the outage of the line. At 79
seconds, the limiter of overexcitation (MAXEX2) of the
synchronous generator 2 acts and the terminal voltage
drops progressively to the value corresponding to the
admissible field voltage. In this case, the action of the
limiter occurs later than in the former case due to the
additional contribution of reactive power produced by
the wind farm (Figure 5). In the case of generator 1, the
terminal voltage is maintained due to fact that the
provided additional reactive power does not
necessitate the protective action of the synchronous
generator. Under these conditions, the terminal
voltage of the wind farm (Figure 7) can be sustained in
the setpoints improving significantly the voltage
profile of the entire process. Throughout this process,
the on load tap charguer of distribution transformers
act but they do not reach the limit. The output powers
deliver by the wind farm, show a suitable output to
the type of control used where voltage control
privileges against the emission of active power. The
portion of the active power emitted by the GSC,
suffers a decrease to result in the necessary reactive
power which maintains the terminal voltage at the set
values (Figure 9). The voltage decreases in the load but
the voltage maintained within an acceptable profile for
these conditions (Figure 11). In Table 6 the results are
shown.
TABLE 7 ‐ VOLTAGE IN THE LOAD BUSES
Voltage
before the
fault (p.u.)
Voltage after
the fault (p.u)
Load
1
0,96 0,95
Load
2
0,99 0,96
Load
3
0,98 0,95
Output Curves
Below are output curves where the figures in a) belong
to the first case; while figures in b) belong to the
second.
FIG. 4 ‐ TERMINAL VOLTAGE IN THE SYNCHRONOUS
GENERATORS 1 AND 2 (CASE 1)
FIG. 5 ‐ TERMINAL VOLTAGE IN THE SYNCHRONOUS
GENERATORS 1 AND 2 (CASE 2)
JOURNAL TITLE ‐ MONTH YEAR 5
FIG. 6 ‐ TERMINAL VOLTAGE IN THE WIND PLANT (CASE 1)
FIG. 7 ‐ TERMINAL VOLTAGE IN THE WIND PLANT (CASE 2)
FIG. 8 ‐ REACTIVE AND ACTIVE POWER GENERATED BY THE
WIND PLANT (CASE 1)
FIG. 9 ‐ REACTIVE AND ACTIVE POWER GENERATED BY THE
WIND PLANT (CASE 2)
FIG. 10 ‐ VOLTAGE IN THE LOAD BUSES (CASE 1)
FIG. 11 ‐ VOLTAGE IN THE LOAD BUSES (CASE 2)
Conclusion
One of the most used technologies in wind turbines is
the doubly fed induction generator (DFIG) which is
capable of contributing to the reactive power control
in the network close to the wind plant point of
interconnection. In this type of wind turbine generator,
the stator circuit is connected directly to the network
while the rotor circuit is connected to the network
trough a back‐to‐back power electronic converter. As
it is a variable speed wind turbine, it allows reducing
voltage fluctuations in the point of connection to the
network, as well as having an independent control of
the generated active and reactive powers. The voltage
control by DFIG could be performed through the
rotor‐side converter RSC; a system which is commonly
used for such machines. This converter provides active
and reactive power independently. The grid side
converter, GSC, normally maintains a constant dc‐link
voltage and adjusts reactive power absorbed from the
grid by the GSC. However, it has been proposed in the
literature the use of the GSC to contribute to voltage
control too and to provide reactive power to the
network when it becomes necessary.
For situations of long‐term voltage stability, it has
been shown in this paper that the simultaneous use of
both RSC and GSC controls can provide additional
6 JOURNAL TITLE ‐ MONTH YEAR
reactive power. Therefore, avoid voltage instability of
a system loaded to its reactive power limit, after a
strong disturbance is avoided.
REFERENCES
Kayikci, M.; Milanovic, J.V.; , ʺReactive Power Control
Strategies for DFIG‐Based Plantsʺ, Energy Conversion,
IEEE Transactions on , vol.22, no.2, pp.389‐396, June 2007
Transactions on Energy Conversion, Vol. 22, No. 2, June
2007.
Vittal, E.; OʹMalley, M.; Keane, A.; , ʺA Steady‐State Voltage
Stability Analysis of Power Systems With High
Penetrations of Windʺ, Power Systems, IEEE
Transactions on , vol.25, no.1, pp.433‐442, Feb. 2010
Shuhui Li; Haskew, T.A.; Williams, K.A.; Swatloski, R.P.; ,
ʺControl of DFIG Wind Turbine With Direct‐Current
Vector Control Configurationʺ, Sustainable Energy, IEEE
Transactions on , vol.3, no.1, pp.1‐11, Jan. 2012.
J. G. Slootweg, S. W. H. de Haan, H. Polinder, and W. L.
Kling, “Voltage control methods with grid connected
wind turbines: a tutorial review”, Wind Eng., vol. 25, no.
6, pp. 353–365, 2001
A. Tapia, G. Tapia, J. X. Ostolaza, and J. R. Saenz, “Modeling
and control of a wind turbine driven doubly fed
induction generator,” IEEE Trans. Energy Convers., vol.
18, no. 2, pp. 194–204, Jun. 2003.
P. Ledesma and J. Usaola, “Contribution of variable‐speed
wind turbines to voltage control”, Wind Eng., vol. 26, no.
6, pp. 347–358, 2002.
Poller M, Doubly‐Fed Inducion Machine Models for Stability
Assessment of Wind Farms, DIgSILENT GmbH,
Germany.
Doc.TechRef, “Dynamic Modelling of Doubly‐Fed Induction
Machine Wind‐Generators”, Published by DIgSILENT
GmbH, Germany, 14 August 2003.
AUTHOR’S INFORMATION
Eduardo J. Toledo was born in
Resistencia, Chaco, Argentina in August
1986. He received the degree in
Electromechanical Engineering from the
National University of Misiones (UNaM),
Argentina in 2011. He is now a M.Sc
student at National University of Rio
Cuarto, Argentina (UNRC). Currently, he
is researcher at the Energy Study Center to Development
(CEED). His research interests include stability analysis of
power systems, power system modeling and analysis of
voltage stability in wind farms.
Luis Aromataris was born in Mendoza,
Argentina. He received the degree in
Electromechanical Engineering from the
Universidad Nacional de Rio Cuarto,
Argentina and Doctor of Engineering
from the Universidad Nacional de La
Plata, Argentina. Currently, he is
researcher at the Grupo de Analisis de
Sistemas Eléctricos de Potencia (GASEP). His research
interests include power systems stability and voltage
stability analysis with high penetrations of wind farms.
Germán C. Tarnowski received the
Electro‐Mechanical Engineer degree from
National University of Misiones,
Argentina in 2003; the MSc. degree in
Automation and Control from Federal
University of Rio Grande do Sul, Brazil in
2006, and the Industrial‐PhD degree from
Technical University of Denmark in 2012.
Since 2007 he is with Vestas Wind Systems, where he did his
Industrial PhD studies on Coordinated Frequency Control of
Wind Turbines. He holds today the position of Research
Engineer. His interests involve operation and control of
wind power plants, control systems and applications of
electrical machines and power electronic converters for
renewable energy.
Mario O. Oliveira was born in Capioví,
Misiones, Argentina in May 1979. He
received the degree in Electromechanical
Engineering from the National University
of Misiones (UNaM), Argentina in 2005
and Masters in Electrical Power Systems
from Universidade Federal do Rio
Grande do Sul (UFRGS), Brazil in 2009.
Currently, he is a researcher at the Energy Study Center to
Development (CEED) and associate professor at UNaM. His
areas of interest include protection of electrical machines,
power system modeling and troubleshooting electrical
systems.
Oscar E. Perrone was born in Venado
Tuerto, Santa Fe, Argentina in December
1954. He received the degree in
Electromechanical Engineering from the
Universidad Nacional de Córdoba (UNC),
Argentina in 1982. Currently, he is a
researcher at the Centro de Estudios de
Energia para el Desarrollo (CEED),
director of Electromechanical Engineering and professor at
the Universidad Nacional de Misiones. His areas of interest
include measurements and electrical installations
JOURNAL TITLE ‐ MONTH YEAR 7
Jose H. Reversat was born in Jardin
America, Misiones, Argentina in
November 1963. He received the degree
in Electrical Engineering from the
Universidad Nacional de Misiones
(UNaM) Argentina in 1996 and
specialization in Plant Engineering and
Production from UNaM in 2000.
Currently, he is a researcher at the Centro de Estudios de
Energia para el Desarrolo (CEED), and adjunct professor at
UNaM. His areas of interest include power systems and
electrical installations.