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7/25/2019 The Impact of Closed-loop Power Flow Control Strategies on Power System Stability Characteristics in a Single-ge
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34 SOUTH AFRICAN INSTITUTE OF ELECTRICAL ENGINEERS Vol.97(1) March 2006
THE IMPACT OF CLOSED-LOOP POWER FLOW CONTROL
STRATEGIES ON POWER SYSTEM STABILITY CHARACTERISTICS IN A
SINGLE-GENERATOR SYSTEM
A. Ally and B. S. Rigby
School of Electrical, Electronic and Computer Engineering, University of KwaZulu-Natal, Durban 4041
Abstract: This paper presents a theoretical study into the influence of closed-loop control of ac power flow on
the small-signal and transient stability characteristics of a single-generator study system. Both the constant power
and constant angle modes of power flow control are examined for a range of controller response times. The results
indicate that the effect of a power flow controller on system stability is dependent on both the mode of the controller
and its response time.
Key words: Power Flow Control, Small-Signal Stability, Transient Stability, Thyristor Controlled Series Capacitor.
1. INTRODUCTION
The broad objective of Flexible AC Transmission Systems
(FACTS) is to enhance the controllability and power transfer
capability of interconnected ac power systems by means of
power electronically controlled compensators [1]. Within
this broad objective, FACTS devices can be used in a
variety of ways to enhance the flexibility or controllability
of power systems. One such application is the use of FACTS
devices to provide direct control over the amount of power
flowing in a particular transmission line, or group of lines,
in an interconnected AC system [2,3]; this application has
variously been described as power scheduling [2,4], power
flow control [5,6], or closed-loop control of AC power flow
[7]. Such closed-loop control of power flow in an AC systemcan provide a number of possible benefits: preventing
unwanted loop flows in an interconnected system; allowing
power to be directed along a contract path in a transmission
system; preventing inadvertent overloading of lines already
near their thermal limits [2,6].
A FACTS devices capability to direct the flow of power
rests on its ability to control dynamically one or more
of the factors that influence power transfer in the line it
compensates. Thus, closed-loop power flow control can
be achieved using a thyristor controlled series capacitor
(TCSC), a static synchronous series compensator (SSSC),
or a unified power flow controller (UPFC), and a number
of schemes employing these different devices have
been proposed [3,4,5]. However, few researchers have
considered the possible impact of closed-loop power flow
control strategies on the stability characteristics of the rest
of the power system, or the influence of the response time
of these controllers on system stability, despite a range of
powerflow controller designs and controller response times
having been proposed in the literature.
References [2] and [4] suggest that the response time
of a closed-loop power flow controller should be on the
order of 10 to 30 seconds, whereas references [3] and [5]
report on controller designs with response times of tens
of milliseconds. Reference [4] does consider the impact
of FACTS device control on the stability characteristics of
the power system as a whole, but in that study the FACTS
device was equipped with both a power flow controller and
a stabilising damping controller acting simultaneously:
as such, it is not possible to draw conclusions from [4]
on the impact of their power flow control strategies, or
the response times of the power flow controller itself, in
isolation from the other (supplementary) control functions
of their FACTS device.
This paper examines the impact of closed-loop power
flow control on the small-signal and large-signal stabilitycharacteristics of an AC power system in isolation from
any other supplementary controllers such as FACTS power
oscillation damping controllers or power system stabilisers
this is not to imply that such supplementary controls
would not or should not be present in a power system,
merely that the objective of the paper is to focus on, and
isolate the influence of closed-loop power flow controllers
on system stability. The paper considers a single generator
infinite bus study system in order to allow the fundamental
interactions to be examined readily, and considers a TCSC
as the FACTS controllable compensator at the heart of the
power flow controller. Furthermore, the paper considers
power flow controller designs whose response times are
on the order of several seconds as considered in [2, 4].
Two distinct strategies have been proposed for implementing
closed-loop powerflow control. The first, constant power
strategy [2,4] involves forcing the uncompensated line (or
lines) in a transmission system to absorb any increase in
the power dispatched, while the second, constant angle
strategy [2,4] regulates the flow of power along a particular
line in which the controllable series compensation is
applied. This paper presents a theoretical analysis of both
the constant power and constant angle control strategies
Copyright (c) 2004 IEEE. This paper was first published in AFRICON 04,
15-17 September 2004, Gabarone, Botswana
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as well as the basic philosophy behind these two control
strategies in an interconnected AC transmission system.
The paper examines not only the impact of a power flow
controllers response time on the small-signal and large-
signal stability characteristics of a power system, but in
addition examines whether the mode of power flow control
(i.e. constant power vs. constant angle) itself has anyimpact on stability characteristics.
Figure 1: Single-line diagram of the study system.
2. DETAILS OF STUDY SYSTEM
2.1 System Overview
Fig.1 shows a diagram of the single-generator study-
system considered in this paper. The system consists of
a synchronous generator that is connected to an infinite
busbar via a transformer and two parallel transmission
lines. Transmission line L1 is compensated with a TCSC,
while line L2 is uncompensated.
The structure of the study system shown in Fig.1 is based on
that which was used to study line power scheduling in [4].However in this paper the parameters of the study system
are different from those in [4], and are based on those of
the Machines Research Laboratory at the University of
KwaZulu-Natal [9]. In addition, in this study the generator
at the sending end of the transmission line is equipped
with an automatic voltage regulator (AVR). The inclusion
of the generators AVR is important when considering the
stability characteristics of a study system, since an AVR is
known to have a significant impact on both small-signal
and transient stability characteristics [11]. A detailed
simulation model of the study system shown in Fig.1 has
been developed in the power system simulation package
PSCAD [13]. The key elements of this study system model
are discussed briefly below.
The synchronous generator is represented using a detailed
(7th-order) electro-mechanical model within PSCAD. The
generator is connected to an infinite busbar via two parallel
transmission circuits and a transformer. Each transmission line
is represented using lumped impedances, while the generator
step-up transformer is represented by its leakage reactance.
2.2 TCSC Model
Fig.2 shows a single-line diagram of a TCSC, which
comprises a capacitor in parallel with a thyristor-controlled
reactor (TCR). This device is inserted in series with the
transmission line, much like a series compensating
capacitor. The net compensating reactance -jXTCSCthat theTCSC provides to the system is the parallel combination of
itsfixed capacitive reactance -jXCand the variable inductive
reactance, jXTCR
of its TCR, where the latters magnitude is
a function of the thyristor delay angle . For the purpose of
interfacing a TCSC to a high-level controller, the devices
control input is not the thyristor delay angle but rather the
TCSCs reactance order Xorder
, where
(1)
Figure 2: Single-line diagram of the TCSC and its internal
controls.
The reactance order Xorder
of a TCSC is thus a dimensionless
ratio (gain) that defines the extent to which the devices
net compensating reactance is increased over the value of
its fixed internal capacitive reactance XC; for a practical
TCSC, the value of Xorder
can range between 1 and 4 [10].
In the PSCAD model of the TCSC used in this study, a
linearization function, in the form of a look-up table for
Xorder
to thyristor firing angle () mappings, is used to
calculate the correct value of for the demanded Xorder
value at the input to the TCSC [7].
The PSCAD model of the TCSC used in this study
represents the individual components of the device in all
three phases, including its power electronic switches and
their low-level firing controls. Although thefiring angleof
a TCSCs thyristors is measured from the zero crossings of
its capacitor voltage VC, in practice the synchronization of
the thyristor firing controls is usually carried out indirectly
by means of a phase locked loop (PLL) synchronized to
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36 SOUTH AFRICAN INSTITUTE OF ELECTRICAL ENGINEERS Vol.97(1) March 2006
the transmission line currents [12] in order to ensure stable
operation of the TCSC. The PSCAD model of the TCSC
used in this study includes a detailed representation of a
phase locked loop which calculates the instantaneous
angle of the TCSC voltages from the measured line
currents; the model also represents the low-level controls
used to generate thyristor firing signals in each phase bycomparing to . Finally, the PSCAD model includes a
surge arrester connected across each phase of the TCSC as
shown in Fig.2. Such surge arresters are always a feature
of TCSC installations in the field [10,12]; it has been found
necessary to include them in the TCSC model in transient
stability studies to ensure satisfactory performance of
the TCSCs capacitor voltages, and hence of its PLL-
based firing controls, following short-circuit faults in the
transmission line [14].
This PSCAD simulation model of the single generator
study system, together with the detailed TCSC model, was
used to investigate the performance of a closed-loop powerflow controller implemented in transmission line L1. The
theory of power flow control is discussed in the following
section.
3. POWER FLOW CONTROL THEORY
In Fig.1, the approximate expression for the active power
transfer in line L1 is given by
(2)
where |V2| and |V
3| are the magnitudes of the voltages at
buses 2 and 3 of the system and 23
is the transmission
angle between these bus voltages.
Equation 2 highlights the principle by which series
compensation can be used to manipulate the net impedance
of a particular transmission line and hence influence its
power transfer. When the TCSCs reactance is increased for
a given transmission angle 23
, the net reactance XLX
TCSC
of the compensated line is reduced, thereby increasing the
active power transfer. Hence, the magnitude of the active
power transfer in the compensated line can be increased
for a given transmission angle by increasing the amount
of TCSC compensation. Alternatively an increase in theamount of TCSC compensation can be used to reduce
the transmission angle required for a given active power
transfer in the compensated line.
These two observations underlie two distinct strategies
that have been proposed for closed-loop control of line
power flow [2]: the constant power strategy which
keeps the power flow in the compensated line constant,
and the constant angle strategy which ensures that the
compensated line transfers any increase in dispatched
power. Each of these strategies is now discussed in more
detail.
3.1 Constant Power Strategy
Consider the system shown in Fig.1 initially operating at
steady state, and then subjected to an increase in the output
power of the generator. This increase in the generator
output power (Pt) causes the common transmission angle
23
across both lines L1 and L2 to increase, and hence the
active power transfer across both lines initially increases.
However in the constant power strategy the TCSC is to be
used to keep the power flow in line L1 constant at some
desired set point value. The relationship in (2) shows that
to achieve this, the TCSCs capacitive reactance has to be
altered to counter any change in angle across line L1. In
other words, when the generator output power is increased,
the TCSCs reactance is then decreased accordingly so
that the power transfer in line L1 remains unchanged fromthe desired set point value. Consequently, in this mode
of control, all the increase in dispatched power from the
generator is then forced to flow through line L2.
3.2 Constant Angle Strategy
Consider once again, the situation when the generator
output power Ptin the system of Fig.1 is increased, but now
the TCSC is to be used to maintain a constant transmission
angle23
across both lines. From (2) in order for additional
power to be transmitted, either the capacitive reactance of
the TCSC has to be increased or the transmission angle 23
has to be increased. In this scenario, where the angle acrosslines L1 and L2 is to be kept constant, when the generator
output power increases the TCSCs capacitive reactance
has to be increased accordingly. Increasing the TCSCs
reactance in this manner results in the compensated line
L1 transferring all the additional power dispatched. This
ensures that the angle across line L1 and L2 is kept constant
and that the power transfer in the uncompensated line L2
remains unchanged.
3.3 Structure of the Power Flow Controller
A feedback control system has been developed in order
to implement TCSC-based, closed-loop control of
transmission line power flow in the study system of Fig.1; the structure of this control system has been devised in
such a way that the powerflow controller can be operated in
either the constant power mode or the constant angle mode
simply by setting a toggle switch in the PSCAD simulation
model. Figs. 3 and 4 show the structure of this feedback
control system as it appears for each of the two settings
of the toggle switch. Note that the initial setting for the
powerflow controller is always constant power mode: that
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is, the power flow controller starts, by default, in constant
power mode, and can be switched into constant angle mode
thereafter if desired.
Note also that in both power flow control modes, the
innermost part of the controller is the same in each case.
Specifically, in both Fig. 3 (constant power mode) and Fig.4 (constant angle mode) a feedback loop compares a signal
PL1
*, representing the commandedvalue of power transfer
in line L1, to the actual (measured) value of power transfer
in line L1 (PL1
) in order to generate an error signal PL1
;
this error signal PL1
is used to drive a proportional-integral
(PI) controller which adjusts the Xorder
value of the TCSC
around some set-point value Xorder 0
in order to force PL1
to
follow the commanded value PL1
*.
Figure 3: Block diagram showing the structure of the
powerflow controller as it appears in the constant power
mode of control.
Figure 4: Block diagram showing the structure of the power
flow controller as it appears in the constant angle mode ofcontrol.
The difference between the two mode settings of the power
flow controller lies in how this commanded value of PL1
*at
the input to the feedback loop is created in each case: the
actual value of PL1
*is obtained by adding the output of the
Mode Select switch to the value of a user-settable input
PL1 set
which represents the set-point value for the power
transfer in line L1.
Thus, in Fig. 3, when the Mode Select switch is set to
position A, the output of this Mode Select switch is zero
and the commanded value of power transfer in line L1
is then simply the set-point value PL1 set; in this case thefeedback loop will then maintain the power transfer P
L1in
line L1 at whatever value is chosen by the user at the input
PL1 set
, that is the controller will operate in constant power
mode.
Once the power flow controller has reached steady state in
constant power mode it can then, if desired, be switched
into constant angle mode by activating the toggle switch in
Fig. 4. When the toggle switch is activated in this way, itperforms two functions: firstly, it changes the Mode Selectswitch to position B; secondly, it activates a sample andhold circuit which takes a measurement of the active poweroutput P
tat the generator terminals and saves its value at
the onset of constant angle control to a storage variable Pt 0
.
Fig. 4 shows that a signal
Pt= Pt
Pt 0is then created whichrepresents the change in power dispatch from the generatorsince the time at which constant angle control commenced;in constant angle mode, (Mode Select switch in positionB) this signal P
tis then added to the set-point value P
L1 set
to form the new commanded value PL1
*of power transferin line L1 applied at the input to the feedback loop. In thisway, if and when the power flow controller is switched toconstant angle mode, the commanded input to the powerflow controller becomes P
L1
*= PL1 set
+ Pt, such that line
L1 is forced to transfer its initial power, plus any changeingenerator dispatch.
4. SMALL SIGNAL BEHAVIOUR
4.1 Verification of control modes
This section examines the impact of the two closed-looppowerflow control strategies on the small-signal dynamiccharacteristics of the study system in Fig.1. However, priorto considering this issue, the basic characteristics of thetwo modes of power flow control are verified by means ofthree simulation studies.
To test the performance of each control strategy, in eachcase the simulation study was started from the same steadystate condition in which the generators active power outputP
t= 0.769 p.u., and with this active power being initially
transferred by the two lines L1 and L2 as follows: PL1
=
0.462 p.u. and PL2= 0.307 p.u.
Figure 5: Response of the study system with no power
flow control.
Subsequently, the mechanical input power to the generatorwas increased by P
m= 0.04 p.u. such that the total active
power Pt dispatched was increased to 0.809 p.u. The
response of the system to this small increase in generatordispatch was then studied for the system without the power
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38 SOUTH AFRICAN INSTITUTE OF ELECTRICAL ENGINEERS Vol.97(1) March 2006
flow control activated (i.e. with the TCSCs Xorder
held
constant) as well as with the power flow control activated
in each of the two control modes.
Fig. 5 shows the simulated response of the study system
to the increase in generator dispatch without power flow
control; the variables shown are the active power transfersin each line as well as the TCSCs X
ordervalue. The result
in Fig.5 confirms that, without the power flow controller
activated, the additional power dispatched by the generator
is shared between both of the two parallel transmission
lines, with line L1 transferring a larger proportion of the
additional power: line L1 transfers a larger share of the
dispatched power since it is electrically shorter than line
L2 as a result of the (in this case) fixed value of TCSC
compensation. In this scenario (fixed TCSC compensation)
any increase in generator dispatch results in both
transmission lines transferring a portion of the increased
power, and no form of power flow control along a contract
path can be instituted.
Fig. 6 now considers the study system with the power
flow controller active and set to the constant power mode.
The results show that, following the increase in generator
dispatch, initially the power transfer in both lines L1 and L2
increases, which then results in the power flow controller
reducing the degree of capacitive compensation provided
by the TCSC. By reducing the capacitive reactance of the
TCSC, the power transfer in line L1 decreases accordingly
and returns to its nominal operating point of 0.462 p.u. All
of the additional power dispatched by the generator is thus
forced to flow through line L2, where the power transfer is
increased to 0.347 p.u. This response thus satisfies the basic
philosophy of the constant power strategy discussed inSection 3, and confirms that the constant power controller
is correctly implemented in the PSCAD model of the study
system in Fig.1.
Figure 6: Response of the study system with the power
flow controller in constant power mode.
Fig.7 shows the behaviour of the study system following
the increase in generator dispatch with the power flow
controller now set to operate in constant angle mode.
According to [2,4] the constant angle strategy should
ensure that the compensated line transfers all the additional
output power of the generator. Fig.7 shows that initially,
following the increase in generator dispatch, the active
power transferred by both lines increases; however, the
power flow controller responds by increasing the degree
of capacitive compensation provided by the TCSC such
that the power transfer in line L2 returns to its nominal
operating point of 0.307 p.u and all the additional dispatch
is transferred by line L1 (PL1
increases to 0.502 p.u). Fig.7
thus confirms that the constant angle controller is correctly
implemented in the PSCAD model of the study system in
Fig.1.
4.2 Influence of power flow control on small-signal
characteristics of the study system.
Section 4.1 has confirmed the correct operation of the power
flow controller in the constant power and constant angle
modes. This section now examines the impact that each
of these power flow control modes has on the small-signal
stability characteristics of the study system when the power
flow controller is designed to respond at different rates.
Previous work [7] has described a technique for designing
the dynamic response characteristics of the closed-loop
powerflow controller. In this section, the design method of
[7] has been used to arrive at three different settling times
for the power flow controller implemented on the study
system of Fig.1. The settling times considered are, tS= 5s;
tS
= 10s and tS
= 25s. For each of these settling times, and
for both modes of power flow control, the response of the
study system was examined for a small step increase in the
mechanical input power to the generator.
Fig.8 compares the small-signal response of the study
system to an increase in generator dispatch for the three
different settling time designs of the controller in constant
power mode. In considering the responses in Fig. 8, there
are two aspects to the behaviour of the system that are
Figure 7: Response of the study system with the power flow
controller in constant angle mode.
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affected by the design of the power flow controller. Firstly,
the rate at which the power transfer in each line is returned
to the correct post-disturbance steady state value is
different in each case, which is the expected (and intended)
consequence of adjusting the controller design. However
the results show that the damping of the generators
electromechanical oscillations is also affected by the powerflow controllers response time: close inspection of Fig. 8
shows that the rate of decay of the oscillatory components
of the line powers PL1
and PL2
becomes greater as the
settling time of the power flow controller is made shorter.
The electromechanical swing mode of the generator in
this system has a frequency of approximately 1 Hz. As
such, one would expect that the power flow controller
would be more likely to influence the characteristics of
this electromechanical swing mode (via the associated
oscillations in the line power transfers) as the response
of the controller is made faster. Conversely, one would
expect the power flow controller to have less influence
on the characteristics of the systems electromechanical
oscillations when its response time is designed to be
significantly longer than the period of these oscillations.
However, the results in Fig. 8 show not only that the
power flow controller has a greater influence on the
electromechanical oscillations of the study system as its
response time is made shorter, but in addition that this
influence is to increasethe damping of these oscillations,
at least in constant power mode.
Fig.9 once again compares the response of the system to
an increase in dispatch at the three different settling times
of the power flow controller, but with the controller now
operating in constant angle mode. As in the case of constantpower mode, the design of the controllers settling time
influences not only the rate at which the power transfers in
each line are returned to their correct steady state values,
but also the damping of the post-disturbance oscillatory
components present in these power transfers as a result of
the generators electromechanical swings.
Figure 9: Small-signal response for different powerflow controller
settling times: constant angle mode.
Close inspection of Fig. 9 shows that in constant angle
mode, the influence of the power flow controller is to
decrease the damping of the systems electromechanical
oscillations: the results show that as the settling time of
the power flow controller is made shorter, the systems
electromechanical oscillations take progressively longer to
die out following the disturbance.
The results of the small-signal investigations in this section
have thus shown that in both modes of operation, the
closed-loop power flow controller has a more pronounced
influence on the damping of the systems electromechanical
oscillations as its response time is made shorter. However
the natureof this influence of the power flow controller
is dependent on its mode of operation: in constant power
mode the influence is beneficial, adding to the inherent
damping of the system; in constant angle mode the influence
is detrimental, acting to diminish the systems inherent
damping. The reasons for the opposite influences on system
damping in the two power flow control modes requiresfurther investigation, but the conclusion is clear: operation
in constant angle mode is detrimental to the inherent
damping of the system, particularly at short settling times
of the power flow controller; as a result, careful design of a
constant-angle controller would be required, in conjunction
with any other damping controllers present in the system,
prior to practical implementation of such a scheme.
5. LARGE SIGNAL BEHAVIOUR
The previous section has considered the impact of power
flow controller design, and controller mode, on the small
signal characteristics of the study system. This sectionnow examines the impact of closed-loop power flow
control on the behaviour of the study system under the
transient conditions that typically follow a large system
disturbance.
Once again the characteristics of the study system in Fig.1
are investigated, firstly with the power flow controller
disabled, and thereafter for each of the two modes of power
flow control, in this case for a single value of settling time
tS= 5s. The study system in Fig.1 was started from a steady
state condition at which the generators total active power
output is 0.733 p.u. A three-phase short-circuit fault was
then applied in the uncompensated line L2 and removedafter 700ms, with the fault located 33% of the way along
the line from bus 2. The fault duration of 700 ms chosen
for this study is relatively long: although faults of this
duration can occur in practice, they are relatively rare.
However, this severe disturbance to the study system has
been chosen in order to be able to demonstrate more clearly
the influence of the different power flow controller modes
under transient conditions.
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Fig. 10 shows the simulated response of the study system
following the three-phase short-circuit fault with no power
flow control. The variables shown are the generators
transmission angle relative to the infinite bus, its rotor
speed deviation, as well as the value of Xorder
at the input to
the TCSC. When such a fault occurs, the electrical output
power of the generator is reduced (since the fault is applied
midway along the line, there is still some power transfer
on the unfaulted line) while the mechanical input power
remains constant. As a result of the imbalance between the
mechanical input power and electrical output power of the
generator, the generator rotor starts to accelerate and its
transmission angle increases. When the fault is removed
the electrical output power increases abruptly, such that
the electrical output power of the generator then exceeds
the mechanical input power, hence causing the generator
to decelerate and, in this case, return to synchronism. Notealso, that with no power flow control implemented, the
amount of compensation provided by the TCSC remains
constant both during the fault, and in the post-fault transient
period.
Figure 10: Response of study system to the 3-phase short-circuit
fault: no power flow control.
Fig. 11 now shows the response of the study system with the
powerflow controller active in the constant power mode.
As before, when the fault is applied, the total output power
of the generator decreases causing the generator rotor to
accelerate. However, in this case, with the power flow
controller activated, the controller responds to the transient
swings in the power transferred by the lines by varying
the amount of compensation provided by the TCSC. In
particular, Fig. 11 shows that the response of the controllerin constant power mode is initially to increasethe TCSCs
Xorder
value in an effort to return the power transfer in the
compensated line L1 to its nominal operating point when
the fault appears. However once the fault is removed,
the electrical output power of the generator increases,
which results in the compensated lines power transfer
temporarily exceeding its nominal operating point value.
The power flow controller then decreases the TCSCs Xorder
accordingly in order to return the power in the compensated
line to its pre-disturbance operating point value.
Fig. 12 now shows the response of the study system with
the power flow controller in constant angle mode. Theresults show that in this mode of operation, the power flow
controller responds to the short circuit fault by initially
sharply decreasingthe compensation in line L1.
Recall that in constant angle mode the controller is designed
to respond to a reduction in generator dispatch by reducing
the degree of compensation of line L1 in order to maintain a
Figure 8: Small-signal response for different powerflow controller
settling times: constant power mode.
Figure 11: Response of the study system to the 3-phase short-
circuit fault: constant power mode.
Figure 12: Response of the study system to the 3-phase short-
circuit fault: constant angle mode.
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constant angle across both lines. In this case, the reduction
in generator output power is a transient one caused by a
short-circuit fault, rather than as a result of a permanent
change in system operating point, but the constant angle
control nevertheless responds to the transient swings in the
generator and transmission line power transfers.
Comparison of Figs. 11 and 12 thus shows that the power
flow controller initially responds in the opposite manner
to the same short-circuit fault in its two different modes of
operation: in constant power mode the controller initially
responds by reducing the net impedance of the compensated
line, with the effect being that the total power transfer out
of the generator during the fault is increased by the action
of the controller; in constant angle mode, the controller
initially responds by increasing the net impedance of the
compensated line, with the effect being that the total power
transfer out of the generator during the fault is reduced by
the action of the controller.
It is well known that the transient (first-swing) stability
of a generator is enhanced by any action that results in
improved transfer of active power out of the generator
during, and immediately after a fault condition [11]. The
results in Figs. 11 and 12 therefore suggest that the mode
of the power flow controller will have an effect on the
first swing characteristics of the generator in response to a
short-circuit fault. Fig. 13 therefore compares the response
of the generators transmission angle and speed deviation
to the short-circuit fault for the cases where the power flow
control is inactive; active in constant power mode; active
in constant angle mode (i.e. the results of Figs. 10, 11 and
12 are now plotted on the same axes).
Figure 13: Comparison of responses to the short-circuit fault:
constant power; constant angle; no control.
The results in Fig. 13 confirm that the powerflow controller,
and its mode of operation, both influence the first swing
characteristics of the generator: the amplitude of the first
swing of the generator angle is slightly smaller in constant
power mode than for the case when there is no power flow
control; by contrast, the amplitude of the first swing of
the generator angle is noticeably larger when the power
flow controller is in constant angle mode. The post-fault
behaviour of the generators speed deviations in Fig.13
also provide further confirmation of the findings in Section4 of the paper the small-signal damping is significantly
improved by the power flow controller in constant power
mode whereas the damping is clearly reduced by the
controller in constant angle mode.
6. CONCLUSION
This paper has considered the application of a thyristor
controlled series capacitor for closed-loop control of
power flow in both constant power and constant angle
modes of operation. The results indicate that the power
flow controllers operation has an important influence on
both the small-signal and transient stability characteristicsof a power system. In particular it has been shown that
the constant angle mode of operation can be detrimental
to system damping and first swing stability, particularly
for a relatively fast-responding power flow controller. By
contrast, the constant power mode of operation has been
shown to have a beneficial impact on both system damping
and first-swing stability under the conditions studied.
7. REFERENCES
[1] Adapa R, Baker MH, Habashi K: Proposed Terms
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42 SOUTH AFRICAN INSTITUTE OF ELECTRICAL ENGINEERS Vol.97(1) March 2006
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8. APPENDIX
Line Parameters (L1& L
2): R
L= 0.033 pu X
L= 0.75 pu
TCSC Parameters: XC= 0.124 pu XL = 0.025 puTransformer Parameters: X = 0.13 pu
Synchronous Generator Parameters documented in reference [9]
Per Unit System: Vbase
= 220 Vrms (l-l) Pbase
=3KVA
Zbase
= 16.13 Ohm Ibase
=7.87Arms