International Journal of Emerging Technology and Advanced Engineering
Website: www.ijetae.com (ISSN 2250-2459, Volume 2, Issue 4, April 2012)406
Automatic Generation Control for an Interconnected Reheat
Thermal Power Systems Using Wavelet Neural Network
Controller
R.Francis
1,
Dr. I. A.Chidambaram
21Asst. Professor, 2 Professor , Electrical Engg, Annamalai University, Annamalai Nagar, India.
1[email protected] 2[email protected]
Abstract -This paper presents optimization of integral controller gains of the two area interconnected thermal power system with the fast acting energy storaging devices. The energy storing device especially Redox Flow Batteries (RFB) can efficiently damp out electromechanical oscillation in power system because of their efficient storage capacity in addition to the kinetic energy of the generator rotor, which can share the sudden changes in power requirements. The proposed controller is designed with the feasibility of applying a wavelet neural network (WNN) approach for the automatic generation control and implemented in a two area interconnected thermal power system without and with RFB. The system was simulated and the frequency deviations in area 1 and area 2 and tie-line power deviations for 1% step- load disturbance in area 1 were obtained. The present intelligent control system trained the wavelet neural network (WNN) controller on line with adaptive learning rates. The comparison of frequency deviations and tie-line power deviations for the two area interconnected thermal power system without and with RFB reveals that the system with RFB enhances a better stability than that of system without RFB.
Keywords - Automatic generation control, Integral square error criterion, Redox flow batteries, wavelet neural network.
I. INTRODUCTION
Automatic generation control is a very important criterion in electric power system design and operation. It is well known that the main objectives of AGC in multi-area power systems are to keep the tie-line power flows in a prescribed tolerance and to fix the frequency of each area within limits. Designing load frequency controllers has received great attention of researchers in recent years, and many control strategies have been developed [1-6]. The integral controller was one of control strategy, which is still widely used nowadays in industry, although it
gives large frequency deviations due to the nonlinearities present in the power system. A linear model can be obtained by linearizing the differential equations describing the dynamic performance of the power system around an operating point.
However, power system loads are usually variable according to the load demand. Several adaptive control techniques have been suggested to overcome these
shortcomings of the conventional techniques. The main
feature of such control is to extend the stability margin of the power systems.
The artificial intelligence neural network and fuzzy
logic control approaches have been applied
successfully to the controllers used in load frequency
control. Such intelligent control systems are
independent of the power system mathematical model parameters, but they can work with the available system time responses. The wavelet neural network approach has been applied successfully to the two area interconnected thermal power systems. The proposed controller provided very fast response relative to that of the fixed gain controllers. The proposed wavelet neural network (WNN) load frequency controller has a very good and fast tracking control performance relative to that of the conventional neural network technique without prior knowledge of the controlled plant [11-14]. The stabilization of frequency oscillations in an interconnected power system became challenging when implemented in future competitive environment. The inclusion of redox flow batteries in the interconnected power system is to enhance a quality and reliable power system. The redox flow batteries (RFB) are found to be superior over the other energy storing devised because of its
Operability at normal temperature.
Small temperature changes.
Small loss during stand by and ends a long
service life.
Flexibility in layout.
International Journal of Emerging Technology and Advanced Engineering
Website: www.ijetae.com (ISSN 2250-2459, Volume 2, Issue 4, April 2012)407
II. TWO AREA INTERCONNECTED REHEAT POWERSYSTEM WITH RFB UNITS
The interconnected two area power system is considered to be divided into two control areas that are connected by tie lines. This is optimized and added with Redox Flow Batteries.
A. Integral gain optimization
The fixed gain controllers which are designed at nominal operating conditions and fail to provide best control performance over a wide range of operating conditions. But it is desirable to keep system performance near its optimum. Thus, the objective function of the optimization of the performance of the system [15] is given in equation (2.0).
.
(2.0)
B. Modeling of two area interconnected power systems with RFB
The linearized mathematical model of the two area (thermal–reheat) power system, is given by the following set of the state variable differential equations as
( ) . ( ) ( ) ( )
1)
( 1 1 1 1
1 1
1 Pg s Kc Pc s Pd s Ptie s
sTps Kps s
F
(2.1) ) ( 1 1 ) ( 1 1 1 1
1 Pt s
sTr Tr sKr s
Pg
(2.2) ) ( 1 1 ) ( 1 1
1 Xe s
sTt s t P (2.3)
( ) 1 ()
1 1 ) ( 1 1 1 1
1 F s
R s Pc sTg s Xe (2.4)
( ) ( )
. 2 )( 1 2
12 F s F s
s T s
Ptie
(2.5)
( ) . ( ) ( ) . ( )
1 )( 2 2 2 2 12
2 2
2 Pg s Kc Pc s Pd s a Pties
sTps Kps s
F
(2.6) ) ( 1 1 ) ( 2 2 2 2
2 Pt s
sTr Tr sKr s
Pg
(2.7) ) ( 1 1 ) ( 2 2
2 Xe s
sTt s t P (2.8)
( ) 1 ( )
1 1 ) ( 2 2 2 2
2 F s
R s Pc sTg s Xe (2.9)
The system state space equations are developed as
X
= Ax+ Bu +d (2.10)Where, x, u and d are the state, control and disturbance vectors. The control and disturbance vectors are given by:
System Control input vector
2 1 2 1 c c P P u u u (2.11) Disturbance vector 2 1 2 1 D D P P d d
d (2.12)
Where ,
Augmented system matrix
A C A 0
0 (2.13)
Augmented control input matrixB
0 B
(2.14)
Augmented disturbance matrix
0
(2.15)
Augmented output matrix C
0 C
(2.16)
Two state vectors ∫ ACE1 and ∫ ACE2 are in clouded
in the augmented state matrix and eleven state variables are presented in this augmented form.
∫ACEi = ∫βi ∆fi +∆Ptie i=1, 2 (2.17)
Substituting the value we get,
(2.18)
C. RFB UNITS in LFC
International Journal of Emerging Technology and Advanced Engineering
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Fig-2 BLOCK DIAGRAM OF A TWO – AREA INTERCONNECTED POWER SYSTEM WITH REDOX FLOW BATTERIES
The RFB modeling equations are
(2.20)
i
rfbi Kci Pc
P
.
(2.21)
III. WAVELET NEURAL NETWORK CONTROLLER
The structure of a four layer wavelet neural network
(WNN) controller [11-14] is shown in Fig.3.The
objective of the control problem is to track the frequency deviation to zero in the case of a load disturbance. To achieve this control means, the frequency deviation is taken as a tracking error, e.
i i i
rfbi Pc
sTd Kc
P
International Journal of Emerging Technology and Advanced Engineering
Website: www.ijetae.com (ISSN 2250-2459, Volume 2, Issue 4, April 2012)409
The input of the WNN consists of the error e and e(1 –z-1), where z-1 is the time delay, and the output of the WNN
is the control input signal U, which represents Up1, Up2. A. Description of the WNN approach
The signal propagation and the basic function in each layer can be described as follows. For every node i in the input layer, the net input and the net output can be described by the following equations:
---- (3.1)
where x11=e and x21 = e(1 – z-1 ). Moreover, the family
of wavelets is usually constructed by
translation and dilations performed on a single fixed function, called the mother wavelet.
In each layer, each node performs a wavelet Uj that is derived from its mother wavelet. The first derivative of a Gaussian function is adopted as a mother wavelet in this
study and expressed as ф(x) = -x exp(-x2
/2). For the jth
node,
-- (
3.2)
--- (3.3)
Where mij and σij are the translation and dilation in the
jth term of the ith input xi2to the node of the mother wavelet
layer, and n is the number of wavelets with respect to each input node k.
Each node k in the wavelet layer is denoted by П, which multiplies the input signals and outputs the result
of the product. Hence, for the kth rule node,
--- (3.4)
Where x3j represents the jth input to the node of the
wavelet layer, and w3jk the weights between the mother
wavelet layer and the wavelet layer, which are assumed to be unity. The number of the wavelet is given as l = n/i if each input node has the same mother wavelet nodes. The Σ is known as the single node 0 in the output layer, which computes the overall output as the summation of all its input signals:
--- (3.5)
Where the connecting weight w4 ko is the output
action strength of the oth output associated with the kth
wavelet, and x4k represents the kth input to the node of
the output layer and y41 =U. Hence, the output signal
given by the formula represents the controller signal as follows:
--- (3.6)
The same procedure can be applied for ΔUp2.
IV. SIMULATION RESULTS AND OBSERVATIONS
The integral controllers are designed and
implemented in the two area interconnected power system with and without RFB and also applied wavelet
neural network in the interconnected reheat
power
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V. CONCLUSIONS
An intelligent wavelet neural network (WNN) controller (LFC) is proposed to control the frequency of the two area interconnected thermal–reheat power systems. The integral gains are optimized by the simulation procedures adopted in the two area interconnected thermal reheat power systems. The proposed WNN controller is implemented in a two area interconnected power systems and design implementation of the controller is found that the
frequency and tie-line power deviations of the
interconnected power systems with WNN controller ensures improved transient response of the system.
ACKNOWLEDGEMENT:
The authors wish to that the authorities of Annamalai University, Annamalai nagar-608002, Tamilnadu, India for the facilities provided to prepare this paper.
Appendix-1
Data for the interconnected two area thermal power system.
Rating of each area=2000 MW Base power=2000 MVA
f= 60 Hz
R1=R2= 2.4 Hz/Pu MW
Tg1 = Tg2=0.08 sec
Tt1 = Tt2=0.3 sec.
Tp1 =Tp2= 20 sec
Kp1 = Kp2=120 Hz/Pu MW
B1=B2= 0.425 Pu MW/Hz
T12 = 0.545 MW/Hz
ΔPd1=0.01pu MW/HZ
a12 = -1.
International Journal of Emerging Technology and Advanced Engineering
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0 5 10 15 20 25 30
-0.15 -0.1 -0.05 0 0.05 0.1
Time (s)
ch
an
ge
in
fre
q.i
n a
rea
1
Integral W NN
0 5 10 15 20 25 30
-0.04 -0.03 -0.02 -0.01 0 0.01 0.02 0.03
Time (s)
ch
an
ge
in
fre
q.
in
are
a 2
Integral W NN
Fig5: Frequency Deviation of area1 and area2 in a two area interconnected thermal reheat power system with integral and WNN controller for 1% step load disturbance in area1
0 5 10 15 20 25 30
-9 -8 -7 -6 -5 -4 -3 -2 -1
0x 10
-3
Time (s)
Tie
Li
ne
P
ow
er
Integral W NN
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0 5 10 15 20 25 30
-6 -5 -4 -3 -2 -1
0x 10
-3
Time (s)
Ti
e
Li
ne
P
ow
er
Integral with RFB WNN
Fig7: Tie-line power Deviations in a two area interconnected thermal reheat power system integral and WNN controller for 1% step load disturbance in area
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Appendix-2 List of symbols: f Frequency
Kp Power system gain
Kr Reheat thermal power system gains
Tr Reheat time constants
Tt Time constant of turbine
Xe Governor Valve position
Tg Time constant of governor
Pg Turbine output power
R Regulation parameter
Tij Tie-line synchronizing coefficient
aij Operator
Tp Power system time constant
Pref The output of ACE
X State vector A, B State matrices
Δfi Frequency deviation of area i (i = 1, 2)
ΔPGi Generation deviation of area i (i = 1, 2)
ΔXEi Governor Valve position deviation of area i
(i = 1, 2)
ΔPtie Tie line power deviation of area i (i = 1, 2)
ΔPdi Step load input of area i (i = 1, 2)
ΔPri Rotor position deviation of area i (i = 1, 2)
ΔUpi Controller signal deviation of area i (i = 1, 2)
International Journal of Emerging Technology and Advanced Engineering
Website: www.ijetae.com (ISSN 2250-2459, Volume 2, Issue 4, April 2012)413
Biographies
R.Francis (1977) received
Bachelor of Engineering in Electrical and Electronics Engineering (1999), Master of Engineering in Power System Engineering (2001) from Annamalai University, Annamalainagar.From 2002 he is working as Assistant professor in the Department of Electrical Engineering, Annamalai University. He is a member of ISTE. His research interests are in Power Systems and Electrical
Measurements and Controls. (Electrical Machines
Laboratory, Department of Electrical Engineering,
Annamalai University, Annamalainagar –
608002,Tamilnadu,India) [email protected]
I.A.Chidambaram (1966) received
Bachelor of Engineering in Electrical and Electronics Engineering (1987), Master of Engineering in Power System Engineering (1992) and PhD in Electrical
Engineering (2007) from Annamalai University,
Annamalainagar. During 1988 - 1993 he was working as Lecturer in the Department of Electrical Engineering, Annamalai University and from 2007 he is working as Professor in the Department of Electrical Engineering, Annamalai University, Annamalainagar. He is a member of ISTE and ISC. His research interests are in Power Systems,
Electrical Measurements and Controls. (Electrical
Measurements Laboratory, Department of Electrical Engineering, Annamalai University, Annamalainagar – 608002, Tamilnadu, India, Tel: 9104144238501, Fax:
-91-04144-238275) [email protected],