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Abstract—Time delay has adverse effects on control systems in
an electric power grid. This paper analyzes the time delay issues,
and deals with the minimization of negative effects of time delays
in smart gird system. The prediction method has been used to
minimize the negative effects of time delay. The OPRT (optimal
reclosing time) method to reclose circuit breakers are considered.
30ms and 300ms communication delays have been considered.
The effectiveness of the proposed method has been tested in the
IEEE nine-bus power system model. Both balanced and
unbalanced permanent faults are considered. Simulations are
performed using Matlab/Simulink software. The performance of
the system considering time delays with and without the
predictor has been compared. From the simulation results, it is
shown that the proposed predictor performs well in minimizing
the negative effects of time delays, and that the prediction
method works more efficiently for a smaller time delay.
Index Terms-- Balanced fault, optimal reclosing time (OPRT),
predictor, time delay, total kinetic energy, unbalanced fault,
unsuccessful reclosing.
I. INTRODUCTION
IME delay arises in a wide range of power system
measurements. However, traditional controlling strategies
in power system only use the local measuring data. And the
time delay of the local measuring data is usually very small
(<10ms) compared to the system time constants and can be
ignored [1]. Since 1990s, centralized controllers using wide-
area signals have been suggested with the new technology
PMUs (phasor measurement units) [2]. PMUs are units that
measure dynamic data of power system, such as voltage,
current, load angle, output power and frequency. All these
measurements are synchronized by GPS (global positioning
system) satellites. As explained in [1], the system dynamic
performance can be enhanced if remote signals are applied to
the controller with respect to inter-area oscillations. However,
coincidentally time delay is usually obvious in wide area
measurement and may have impact on central controller.
The time delay caused by transmission of remote signals is
one of the key factors influencing the whole system stability
and damping performance [1]. In wide-area power systems the
time delay can vary from tens to several hundred milliseconds
[3].
Authors are with the Electrical and Computer Engineering
Department, University of Memphis, Tennessee, 38152, USA
[[email protected]; [email protected];
[email protected]; [email protected]].
In the past, studies have been done in the engineering fields
that evaluate time delay impacts on the controlling mechanism
and power systems [1], [4-8], while minimizing the effect
caused by time delay [9]. In [9], a prediction method has been
mentioned that proposes an optimal reclosing scheme in extra
high voltage (EHV) lines, using the power angle, and power
angle velocity as input values to optimize the reclosing
method.
This paper analyzes the causes and effects of time delays,
and uses the prediction method [9] to minimize the negative
effects of time delay in smart grid applications. And this is the
main contribution of this work. The prediction method is
simple and efficient and easy to add to the controller without
changing the system configuration.
The effectiveness of the proposed method has been tested
in the IEEE nine-bus power system model [10]. The optimal
reclosing time (OPRT) method [10] has been used for finding
the reclosing times of circuit breakers for both balanced and
unbalanced permanent faults. The Windex (total kinetic energy
deviation index) with and without predictors are compared in
cases of different type of faults and delay times.
II. COMMUNICATION DELAY ISSUES IN SMART GRID
Communication delays in a smart grid occur mainly from
signal transmission through optical fiber, microwave, analog-
to-digital (A/D) conversion, online calculation of global input
variable, and the time synchronization of signals by GPS.
Such delay will affect the controllers and system performance
[11].
In wide area control system (WACS) communications
network, data are transmitted in the form of packets arranged
in three sections: the header, the payload, and the trailer. The
time delay has following four types [8]:
serial delays: the delay of having one bit being sent one
after another;
“between packet” serial delays: the time after a packet is
sent to when the next packet is sent;
routing delays: the time required for data to be sent
through a router, and resent to another location;
propagation delays: the time required to transmit data
over a particular communications medium.
The total signal time delay may be represented as
s b p rT T T T T (1)
ss
r
PT
D
(2)
Minimization of Negative Effects of Time Delay
in Smart Grid System Yang Zhou, Student Member, IEEE, Sagnika Ghosh, Student Member, IEEE, Mohd. Hasan Ali, Senior
Member, IEEE, and Thomas Edgar Wyatt, Senior Member, IEEE
T
978-1-4799-0053-4/13/$31.00 ©2013 IEEE
Minimization ofNegative Effects of Time Delayin Smart Grid System
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p
lT
v
(3)
where Ts is the serial delay, Tb is the between packet delay, Tp
is the propagation delay, Tr is the routing delay, Ps is the size
of the packet (bites/packet), Dr is the data rate of network, l is
the length of the communication medium, and v is the velocity
at which the data are sent though the communications
medium.
Methods have been given to calculate different kinds of
time delay [8]. Unlike the small time delay in local control, in
wide-area power systems the time delay can vary from tens to
several hundred milliseconds or more [12-15]. In the
Bonneville Power Administration (BPA) system, the latency
of fiber optic digital communication has been reported as
approximately 38 ms for one way, while latency using
modems via microwave is over 80 ms [16]. Communication
systems that involve satellites may have even longer delays.
The delay of a signal feedback in a wide-area power system is
usually considered to be in the order of 100 ms [16]. If routing
delay is included, and if a large number of signals are to be
routed, there is potential for long delays and variability
(uncertainty) in these delays. According to some other reports
[17-18], 150 to 200 milliseconds communication delay values
are considered in the design of some actual transient stability
control systems. The time delay range chosen for this work is
30ms and 300ms.
III. DESCRIPTION OF MODEL SYSTEM
For the analysis of time delay issues, the nine-bus power
system model shown in Fig.1 has been used. The nine-bus
system consists of two synchronous generators (G1 and G2),
an infinite bus, transformers, double-circuit transmission lines,
and loads. In Fig.1, the double circuit transmission line
parameters are numerically shown in the forms R+jX(jB/2),
where R, X and B represent resistance, reactance and
susceptance, respectively, per phase with two lines. The AVR
(automatic voltage regulator) and GOV (governor) control
models and the parameters of Generator 1 and Generator 2 are
mentioned in [20]. The system bases are 50 Hz and 100 MVA,
and the capacities of generators G1 and G2 are 200MVA and
130 MVA, respectively. Faults are considered to take place at
F1 (between bus 5 and 7), F2 (between bus 6 and 9), and F3
(between bus 8 and 9). In this paper, we considered 3LL
(three-line), 2LG (double-line-to-ground), 2LL (line-to-line)
and 1LG (single-line-to-ground) permanent faults.
IV. OPTIMAL RECLOSING TECHNIQUE
Compared to conventional reclosing, which adopts a
constant value of reclosing time, optimal reclosing time keeps
the system more stable, especially in case of unsuccessful
reclosing [10]. Reclosing of circuit breakers at optimal
reclosing time (ORCT) can maintain synchronism and
enhance transient stability of the system. In this paper, the
optimal reclosing time is considered as the point which meets
the following conditions:
I. Without the circuit breakers reclosing, the point when the
total kinetic energy oscillation becomes the minimum.
II. The value obtained from condition I must be greater than
TCB, the required reclosing time for circuit breakers to deionize
the fault arc. The calculation equation for TCB is from trials
and experiments done by previous researchers [19], and shown
below:
(10.5 )
34.5CB
KVT cycles
where KV indicates the line-to-line rms voltage of the system.
Here 1 cycle =20 ms. If the first minimum point in condition I
is less than TCB, the second minimum time of the kinetic
energy response should be chosen. In this paper, TCB is
calculated as 0.223 sec.
Fig. 1. IEEE Nine-bus Power system model.
This method [14] uses the kinetic energy of each generator,
which can be obtained easily. The total kinetic energy, Wtotal,
can be calculated by knowing the rotor speed of each
generator and is given by
2
1
1( )
2
N
total i mi
i
W J J
where wmi is the rotor angular velocity in mechanical rad/s, i is
generator number, N is total number of generators, and Ji is
the moment of inertia in kg·m 2 shown below
2
9 2
( )
5.48 10
i
i
i rating
i
s
H MVAJ kg m
N
In (6), Hi is inertia constant of ith generator and
120
si
fN
p
(7)
where f is system frequency, p is the number of poles, and Nsi
is the synchronous speed of the ith generator.
Fig. 2 gives an example of how to get OPRT when 2LL
fault occurred at point F3 in the nine-bus system. Fig. 2 shows
(6)
(5)
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the total kinetic energy response without reclosing operation
after fault happening. The time for the first minimum point is
0.8366 sec, which is greater than TCB.
Using the optimal reclosing technique, the values of
optimal reclosing time corresponding to different types of
permanent faults at different points are calculated from the
simulation graphs of total kinetic energy responses, and are
shown in Table I.
Fig. 2. Response for OPRT (fault type: 2LL at F3 )
TABLE I
OPRT FOR DIFFERENT TYPES OF FAULTS AT DIFFERENT POINTS
V. PREDICTION METHOD IN TIME DELAYED SYSTEM
A. Communication Delay in IEEE Nine-Bus System
In this work, simulations are carried out by
Matlab/Simulink software. During the simulation, constant
time delays (td) 30ms and 300ms are applied to controller
input. Fig. 3 illustrates the signal which has transmission delay
corrected by predictor, and then goes to the controller.
Fig.3. Figure of delay and predictor.
B. Prediction Method Used in Minimizing Negative Effects of
Communication Delay
The flow diagram for optimal reclosing including the
predictor algorithm is shown in Fig. 4. Since the predictor can
modify the delayed signal to the original curve before
inputting it into controller, the predictor easily adapts to
different kinds of controllers.
As already explained, the OPRT is the time when the total
kinetic energy response first reaches its minimum point. There
will be a delay between the measured OPRT and the actual
OPRT. If the time delay is td, the predicted OPRT can be
obtained from the measured point, previous measured point
and changing rate [9]:
p previous dTKE TKE t (8)
( 1)k kTKE TKE
t
(9)
where p is the predicted point, k is measured point, and w is
changing rate of Wtotal..
Since the total kinetic energy curve is not linear, the larger
the value of td, the greater the error in the prediction curve.
However, the delay time is generally very small and the errors
can be ignored. Fig. 5 is the OPRTs calculation for predicted,
delayed and ideal curves in case of 3LG fault at points F1 and
F3. In Fig. 5, Ti, Tp and Td are OPRTs for ideal, predicted, and
delayed system, respectively. The changing trends of predicted
curve and ideal curve are almost the same. Only the amplitude
is different, however that will have little influence on
controller.
Fig.4. Flow chart diagram of OPTR with predictor.
Fault type Fault point OPRT(sec)
3LG
F1 0.9590
F2 0.9572
F3 0.8426
3LL
F1 0.9597
F2 0.9558
F3 0.8415
2LG
F1 0.9175
F2 0.9135
F3 0.8465
2LL
F1 0.9474
F2 0.9380
F3 0.8366
1LG
F1 0.8930
F2 0.8860
F3 0.8640
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(a) 3LG Fault at F1
(b) 3LG Fault at F3
Fig.5. Responses for predicted, delayed and ideal OPRTs for different time
delay systems (a) 300ms delay and (b) 30ms delay
Fig.6. Predictor in Matlab/Simulink.
Fig. 6 illustrates the predictor which is simulated in
Matlab/Simulink. The input signal is the Wtotal, and the signals
into the scope are the delayed version of Wtotal and the
predictor signal.
VI. SIMULATION RESULTS AND DISCUSSION
In this work, 3LG, 3LL, 2LG, 2LL and 1LG permanent
faults are considered to occur at points F1, F2 and F3 of the
power system model in Fig. 1. It is assumed that the fault
occurs at 0.0 sec, circuit breakers opens at 0.1 sec, breakers
reclose at OPRT time and reopen at the time 0.1sec after the
OPRT. The delay time td is chosen as 30ms and 300ms.
The difference between the total kinetic energy (Wtotal) of
the generators at transient state and steady state is defined as
the total kinetic energy deviation, TKED.
total transient state total steady stateTKED W W (10)
For the evaluation of transient stability, the total kinetic
energy deviation index, Windex, has been used in this paper.
0
T
index
TKEDdtW
system base power
(11)
Where, T is the simulation time selected as 20.0s, TKED is the
total kinetic energy deviation as calculated in (10). It is
apparent that the system performs better for smaller values of
Windex. TABLE II
COMPARISON OF indexW IN IDEAL SYSTEM AND 30MS DELAY SYSTEM WITH
AND WITHOUT PREDICTOR
OPRT, Windex Without delay
30ms delay
without
predictor
30ms delay with predictor
Fault
type Fault
point Time Windex Time Windex Time Windex
3LG
F1 0.9590 0.3530 0.9890 0.3966 0.9620 0.3563
F2 0.9572 0.6582 0.9872 0.7291 0.9538 0.6525
F3 0.8426 0.3848 0.8726 0.4395 0.8440 0.3837
3LL
F1 0.9597 0.3467 0.9897 0.3906 0.9540 0.3407
F2 0.9558 0.6557 0.9858 0.7265 0.9586 0.6489
F3 0.8415 0.3741 0.8715 0.4271 0.8423 0.3796
2LG
F1 0.9175 0.2195 0.9475 0.2499 0.9150 0.2186
F2 0.9135 0.5919 0.9435 0.5405 0.9148 0.4950
F3 0.8465 0.3395 0.8765 0.3730 0.8534 0.3442
2LL
F1 0.9474 0.1904 0.9802 0.2032 0.9550 0.1946
F2 0.9380 0.3336 0.9680 0.3597 0.9348 0.3468
F3 0.8366 0.1958 0.8666 0.2269 0.8335 0.1950
1LG
F1 0.8930 0.09645 0.9230 0.1144 0.8960 0.1003
F2 0.8860 0.2759 0.9160 0.3023 0.8766 0.2715
F3 0.8640 0.2092 0.8940 0.2258 0.8652 0.2140
TABLE III
COMPARISON OF indexW IN IDEAL SYSTEM AND 300MS DELAY SYSTEM WITH
AND WITHOUT PREDICTOR
OPRT,Windex Without delay 30ms delay
without
predictor
30ms delay with
predictor
Fault
type Fault
point Time Windex Time Windex Time Windex
3LG
F1 0.9590 0.3253 1.259 0.6974 1.0625 0.4455
F2 0.9572 0.6582 1.2527 1.015 1.0627 0.8229
F3 0.8426 0.3848 1.2426 0.5102 0.9810 0.4990
3LL
F1 0.9597 0.3467 1.2597 0.6920 1.0625 0.4403
F2 0.9558 0.6557 1.005 0.9776 1.0627 0.8142
F3 0.8415 0.3741 1.1415 0.4213 0.983 0.4998
2LG
F1 0.9175 0.2195 1.2175 0.4744 1.015 0.2760
F2 0.9135 0.4917 1.2135 0.8684 1.004 0.5996
F3 0.8465 0.3395 1.1465 0.5690 0.9832 0.4334
2LL
F1 0.9474 0.1904 1.2474 0.3707 1.0446 0.2283
F2 0.9380 0.3336 1.2380 0.4865 1.0246 0.3995
F3 0.8366 0.1958 1.2366 0.2963 0.9632 0.2271
1LG
F1 0.8930 0.09645 1.1930 0.2488 0.9965 0.1275
F2 0.8860 0.2759 1.286 0.5269 0.9860 0.3455
F3 0.8640 0.2092 1.264 0.3954 1.004 0.2776
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Tables II and III compare the value of indexW with and
without the predictor for 30ms and 300ms delays,
respectively. The system will oscillate more when Windex is
larger. It can be seen from Tables II and III that,
1) The 3LG fault exhibits the most oscillation while the 1LG
fault shows the least. For example, under without delay
situation, the indexW value for 3LG at F1 is 0.3530 while
for 1LG is 0.09645.
2) With the same fault type and fault point, a larger time
delays in the system has larger oscillation. For example,
for the 2LG fault at F2, Windex of 300ms delayed system is
0.8684; while 30ms delayed system is 0.5405.
3) The predictor assists in maintaining system stability when
compared to the ideal and delayed system. For example,
for 300ms delayed system, when 3LL fault occurs at point
F1, the Windex for ideal, predicted and delayed system are
0.6557, 0.8142 and 0.9776, respectively.
Some of the simulation results have been shown in Figs. 7-
10. Figs. 7-10 are the total kinetic energy responses for 3LG,
and 1LG permanent faults at points F1, F2 and F3 with and
without predictor for cases of 300ms and 30ms delays. For
300ms delayed system, we can see from Figs. 7-9 that there
are significant differences among ideal, with predictor and
without predictor cases. This demonstrates that although the
predictor is useful for minimizing oscillations arising from
delay, the oscillation is still larger than in the ideal curve. In
Fig. 10, we can see that for small delayed system, the curve
with the predictor is almost similar to the ideal curve.
Fig. 7. Responses for with and without predictor in case of 3LG permanent
fault at F1 in 300ms delayed system.
Fig.8. Responses for with and without predictor in case of 3LG permanent
fault at F2 in 300ms delayed system.
Fig.9. Responses for with and without predictor in case of 1LG permanent
fault at F2 in 300ms delayed system.
Fig.10. Responses for with and without predictor in case of 3LG permanent
fault at F2 in 30ms delayed system.
VII. CONCLUSION
This paper deals with the minimization of negative effects
of time delays in a smart gird system. The prediction method
has been used to minimize the negative effects of time delay.
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The OPRT (optimal reclosing time) method to reclose circuit
breakers is considered. Time delays of 30ms and 300ms as
well as balanced and unbalanced permanent faults at different
locations have been considered. From the simulation results,
the following points are noteworthy.
a) The proposed predictor performs well in minimizing the
negative effects of time delays.
b) The predictor can work more efficiently and accurately
when the time delay is smaller.
Simulation results also show the predicted curve may have
oscillations in some scenarios. Future works should be
directed to exploring ways to: minimize oscillations in the
prediction method, combining prediction methods with
methods to minimize communication delay, and finding more
methods to minimize the effect of time delay in a smart grid.
VIII. REFERENCES
[1] Wu HX, Tsakalis KS, and T Heydt G., “Evaluation of time delay effects
to wide-area power system stabilizer design,” IEEE Trans Power Syst,
vol.19, no.4, pp. 1935-41, 2004. [2] B. Bhargave, “Synchronize phasor measurement system project at
Southern California Edison Co.,” in Proc. IEEE Power Engineering
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system small signal stability region with time delay,” MELECON 2010 -
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[4] Kamawa I, Grondin R, and Hebert Y., “Wide-area measurement based
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[6] Saad MS, Hassouneh MA, Abed EH, and Edris AA, “Delaying instability and voltage collapse in power systems using SVXs with
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[10] M. H. Ali, T. Murata, and J. Tamura, “Effect of coordination of optimal reclosing and fuzzy controlled braking resistor on transient stability
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[12] R. E. Wilson, “An investigation of time transfer accuracies over a utility microwave communications channel,” IEEE Trans. Power Delivery, vol.
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[13] B. Chaudhuri, R. Majumder, and B. C. Pal, “Wide-area measurement-based stabilizing control of power system considering signal
transmission delay,” IEEE Trans. Power Systems, vol. 19, no. 4,
pp.1971-1979, November 2004. [14] C. W. Taylor, D. C. Erickson, K. E. Martin, R. E. Wilson, and V.
Venkatasubramanian, “WACSwide-area stability and voltage control
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[15] W. Yao, L. Jiang, Q. H. Wu, J. Y. Wen, and S. J. Cheng, “Delay-
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[16] H. Wu, K. S. Tsakalis, and G. T. Heydt, “Evaluation of time delay effects to wide-area power system stabilizer design,” IEEE Trans. Power
Systems, vol. 19, no. 4, pp. 1935-1941, November 2004.
[17] H. Ota, Y. Kitayama, H. Ito, N. Fukushima, K. Omata, K. Morita, and Y. Kokai, "Development of transient stability control system (TSC
system) based on on-line stability calculation", IEEE Trans. Power
Systems, vol. 11, no.3, pp.1463-1472, August 1996. [18] M. Koaizawa, M. Nakane, K. Omata, and Y. Kokai, “Actual operating
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IEEE PES Winter Meeting, 2000. vol. 1, pp 84-89. [19] M. Yagami, T. Murata and J. Tamura, “An analysis of optimal reclosing
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Yokohama, Japan.
IX. BIOGRAPHIES
Yang Zhou (S’12) received her B.Sc. degree in Electrical Engineering & Automation from China Three Gorges University, in 2010. Currently she is
pursuing her M.Sc. degree in electrical engineering at the University of Memphis, Memphis, Tennessee, USA. Her main fields of interests includes
advanced power systems, smart-grid, renewable energy systems, energy
storage system, and power delivery. She is a student member of the IEEE.
Sagnika Ghosh (S’12) received her B.Tech in Electrical Engineering from
Academy of Technology, India, in 2010. She worked in TIL India as electrical
design engineer since September 2010 to April 2011. Currently she is pursuing her PhD degree in electrical engineering at University of Memphis,
Memphis, Tennessee, USA. Her main field of interest includes advanced
power systems, smart-grid and micro-grid systems, renewable energy systems,
energy storage systems, and flexible AC transmission systems (FACTS). She
is a student member of the IEEE.
Mohd. Hasan Ali (SM’08) received his Ph.D. Degree in Electrical and Electronic Engineering from Kitami Institute of Technology, Japan, in 2004.
He served as a lecturer in EEE dept. of RUET, Bangladesh since 1995 to 2004,
and also became an assistant professor in the same university in 2004. Dr. Ali was a Postdoctoral Research Fellow under the Japan Society for the
Promotion of Science (JSPS) Program at the Kitami Institute of Technology,
Japan, since November 2004 to January 2007. He also worked as a Research Professor in Electrical Engineering Department of Changwon National
University, South Korea since February 2007 to December 2007. He was a
Postdoctoral Research Fellow with the Electrical and Computer Engineering Department of Ryerson University, Canada, from January 2008 to June 2009.
He also worked as a Faculty at the Electrical Engineering Department,
University of South Carolina, USA, since July 2009 to August 2011. Currently he is working as an Assistant Professor at the Electrical and
Computer Engineering Department, University of Memphis, Tennessee, USA.
He leads the Electric Power and Energy Systems Laboratory of the University.
His main field of interest includes advanced power systems, smart-grid and
micro-grid systems, renewable energy systems, energy storage systems, and flexible AC transmission systems (FACTS). Dr. Ali is a Senior Member of the
IEEE Power and Energy Society (PES). Also, he is the Chair of the PES of the
IEEE Memphis Section.
Thomas Edgar Wyatt, P.E (SM ’88) received a B.S. (1973) from The
University of Tennessee at Martin, B.S.E.E. (1979) and M.S.E.E. (1985) from
Memphis State University. He was employed at Memphis Light Gas and Water Division, Memphis, Tennessee from 1980 until 2005 working in
Distribution Planning, Systems Operations and as Supervisor of the Reliability
and Power Quality Department. Mr. Wyatt joined The University of Memphis as a Research Assistant in the Center for Advanced Sensors and worked as a
Visiting Assistant Research Professor prior to becoming an Instructor in 2007.
His current interest areas are: Infrared Detection and Power Quality.