- Open Access
- Total Downloads : 1955
- Authors : Kamlesh Kumar Vishwakarma, Hari Mohan Dubey
- Paper ID : IJERTV1IS3126
- Volume & Issue : Volume 01, Issue 03 (May 2012)
- Published (First Online): 30-05-2012
- ISSN (Online) : 2278-0181
- Publisher Name : IJERT
- License: This work is licensed under a Creative Commons Attribution 4.0 International License
Simulated Annealing Based Optimization for Solving Large Scale Economic Load Dispatch Problems
Kamlesh Kumar Vishwakarma Department of Electrical Engineering Madhav Institute of Technology & Science Gwalior (M.P), India-474005
Hari Mohan Dubey
Department of Electrical Engineering Madhav Institute of Technology & Science Gwalior (M.P), India-474005
Abstract
This paper presents a Simulated Annealing (SA) approach for solving Economic Load Dispatch (ELD) problems in electrical power system. The objectives of ELD problems in electric power generation is to programmed the devoted generating unit outputs so as to meet the mandatory load demand at lowest amount operating cost while satisfying all units and system equality and inequality constraints .Global optimization approaches is inspired by annealing process of thermodynamics. The proposed method work s very fast, this aspect of algorithm is strik ing when applied for a large ELD system. Simulation has been performed over two different cases. Case study-I consist 38 generating units and Case study-II consist 110 generating units, both cases having convex fuel cost characteristics. The proposed method results have been compared with other relative existing approaches and finally SA proves luminous feasibility, robustness and fast convergence for optimization of ELD problems.
-
Introduction
The main aim o f the economic dispatch is to include variables that affect operational cost, su ch as the generator distance from the load, type of fuel, load capacity and transmission line losses. By including these variables one will be ab le to perform economic dispatch and interconnected generators to minimize operating cost.
Economic dispatch is the process of allocating the required load demand between the available generating units such that the cost of operation is minimu m as passable. The process of solving such a problem is referred to as optimization. ELD is a constrained nonlinear optimizat ion proble m.
Simu lated Annealing (SA) has been proved to be effective and quite robust in solving the optimizat ion problems. SA can provide near g lobal solutions and can
also handle effectively the discrete control variables. SA does not stick into local optima because SA begins with many init ial points and search for the most optimu m in para lle l. SA considers only the pay -off informat ion of objective function regardless whether it is differentiable or continuous. Consequently, the most realistic cost characteristic of power plants can be formulated.
In recent times, different heuristic approaches have been proved to be effective with promising performance. These include evolutionary progra mming (EP) [1], genetic algorith m (GA) [2], differentia l evolution (DE) [3], part icle swarm optimizat ion (PSO) [4], etc. Improved fast Evolutionary programming algorith m has been successfully applied for solving the ELD proble m [5, 6]. Other a lgorith ms like improved coordination aggregated based PSO [7], SOH-PSO [8] and BFONM [9] are some of the, those which have been successfully applied to solve the ELD proble m.
Th is paper present SA approach for optimization has been used to get to the bottom of economic load dispatch problems. Simulated Annealing (SA ) is a stochastic optimization technique which is based on the process of annealing in Thermodynamics proposed by Kirkpatrick [10].
Mathematical model of simulated annealing describes how the molecules of liquidated metal move freely with respect to each other and by gradually cooling (thermodynamic process of annealing) therma l mobility are lost. The atoms start to get arranged and finally form crystals, having the minimu m energy which depends on the cooling rate. The proposed method is found to give optima l results while working with constraints in the ELD.
Th is paper provides a brief e xp lanation and
mathe matica l formu lation of ELD proble ms in Section
-
The concept of Simu lated Annealing (SA) is discussed in Section 3. Section 4 p rovides the imple mentation process of the algorith m used in the test system. The parameter settings for the test system to evaluate the performance of SA and the simulat ion
studies are discussed in Section 5. Finally, Section 6 presents the conclusions.
-
Problem Formulation
2.2 The Generator Constraints: The power generated by each generator shall be within their lo wer limit Pimin and upper limit Pimax so that
P
In a power sys tem, the unit co mmit ment proble m has various sub-problems varying fro m linear programming proble ms to co mple x non-linear
min
P
P
i i
max i
(5)
problems. The concerned problem, i.e., Economic Load Dispatch (ELD) proble m is one of the different non – linear progra mming sub-problems of unit commit ment. The ELD proble m is about minimizing the fuel cost of generating units for a specific period of operation so as to accomplish optima l generation dispatch among operating units and in return satisfying the system load demand considering generator operational constraints.
The objective function corresponding to the production cost can be approximated to be a quadratic function of the active power outputs from the generating units. Symbolica lly, it is represented as
-
Simulated Annealing Method
Simu lated Annealing (SA) a lgorith m is a nature- inspired method which is adapted from process of gradual cooling of metal in nature. In the metallurgica l annealing process, a solid is melted at high temperature until all mo lecules can move about freely and then a cooling process is performed until therma l mobility is lost. The perfect crystal is the one in which all ato ms are arranged in a lo w level pattern, so crystal reaches the minimu m energy.
It is basically a stochastic optimizat ion technique
F
which is based on the principles of statistical engineering. The search for global minima of a
Minimize
cos t t
NG
fi (Pi )
(1)
mu ltid imensional function is quite a comple x p roble m especially when a big number of local min ima
Where
f i (Pi )
a i P 2
i
bi Pi
1
ci ,
i 1,2,3, …, N G
i
(2)
correspond to the respective function. The main
purpose of the optimization is to prevent hemming about to local minima . The originality of the SA method lies in the application of a mechanis m that
is the expression for cost function corresponding to ith generating unit and ai, bi and ci are its cost coefficients. Pi is the real power output (MW) of ith generator corresponding to time period t. NG is the number of online generating units to be dispatched.
Th is constrained ELD proble m is subjected to a variety of constraints depending upon assumptions and practical imp lications. These include power balance constraints to take into account; these constraints are discussed as under
2.1 Power Balance Constraints or Demand
Constraints: This constraint is based on the principle of
NG
equilibriu m between total system generation ( Pi)
i 1
and total system loads (PD) and losses (PL). That is,
NG
guarantees the avoidance of local min ima.
Following its introduction fro m [10], simulated annealing is main ly applied to large-scale combinatoria l optimizat ion proble ms.
-
The Process of Annealing in Thermodynamics :
At high temperature, the metal is in liquid stage. The molecules of liquidated metal move freely with respect to each other, via gradual cooling (thermodynamic process of annealing) thermal mobility is lost. The atoms start to get arranged and finally fo rm crystals, having the min imu m energy which depends on the cooling rate. If the temperature is reduced at a very fast rate, the crystalline state transforms to an amorphous structure, a meta-stable state that corresponds to a local min imu m of energy [11]. Annealing process of metal influences SA algorith m.
If the system is at a therma l balance for g iven
Pi PD PL
i 1
(3)
temperature T, then the probability PT(s) that it has a configuration s depends on the energy of the corresponding configuration E(s), and is subject to the
Where the transmission loss PL is e xpressed using B- coeffic ients [20] given by
Bolt zmann distribution
e E (s) / kT
NG NG NG
PL Pi Bij Pj
B0i Pi
B00
PT (s)
e E (w) / kT
W
(6)
i 1 j 1 i 1
(4)
Where, k is the Boltzmann constant and the sum W
includes all possible states W.
Metropolises [12] we re the first to suggest a method for calcu lating a distribution of a system of ele mentary particles (mo lecules) at the thermal ba lance state.
Let the system has a configuration g, which corresponds to energy E(g). When one of the molecules of the system is displaced from its starting position, a new state occurs which corresponds to energy E(). The new configuration is compared with the old one. If E() E(g) , then the new state is accepted. If E()>E(g), then the new state is accepted with probability :
-
Starting Te mperature
-
Final Te mperature
-
Te mpe rature Decre ment
-
Iterations at each Temperature
-
Starting Te mperature
The starting temperature must be set to a big enough value, in order to make possible a big probability of acceptance for non optimized solutions during the first stages of the algorithms application. However, if the value of the starting temperature gets too big, SA algorith m beco mes non-effective because of its slow convergence and in general, the optimizat ion process
e ( E (
) E ( g ))
kT
(7)
degenerates to a random wa lk.
On the contrary, if the starting temperature is lo w
Where, k is the Boltzmann constant.
Table 1: Connection between Thermodynamic and Co mbinatoria l Optimization
Ther modynamics
simulati on
Combinatorial
Opti mization
System state
Feasible So lutions
Energy
Cost
Change of state
Neighboring So lutions
Temperature
Control Para meter
Frozen state
Heuristic Solution
The basic step of the simulated annealing algorith m is presented with the following Pseudo-code.
-
Get the initial solution S.
-
Get the initial Temp T>0
-
While not yet frozen
(a)perform the following loop L times
*peak the random neighbor, S of S
*let =cost(S)-cost(S)
*If 0 ,set S=S
/ T
then there is a greater probability of achieving local minima. There is no particular method for finding the proper starting temperature that deals with the entire range of proble ms.
Various methods for finding the appropriate starting temperature have been developed [13]. suggests to quickly raise the temperature o f the system initia lly up to the point where a certain percentage of the worst solutions is acceptable and after that point, a gradual decrement of te mperature is proposed.
-
-
Final Te mper ature
During the application of the SA algorith m it is common to let the temperature fall to zero degrees. However, if the decre ment of the temperature becomes e xponential, SA a lgorithm can be e xecuted for much longer time . Finally, the stopping criteria can either be a suitable low temperature or the point when the system is fro zen at current te mperature.
-
Te mper ature Decre ment
Since the starting and final te mperatures have been defined, it is necessary to find the way of transition fro m the starting to the final te mperature.
The way of the temperature decrement is very important for the success of the algorithm [ 14] suggested the following way to decre ment the temperature:
-
-
-
Control parameters of SA algorithm:
T (t)
d
log(t)
*If >0, set S=S with probability e
(b)set T= T (reduce Temperature) Return S
(8)
For the successful application of the SA algorithm is the annealing schedule is vital, which refers to four control parameters that directly influence its
Where d is a positive constant.
An alternative is the geometric re lation:
convergence (to an optimized solution) and consequently its efficiency [11]. The parameters are the following:
T (t)
a.t
(9)
Where parameter a, is a constant near 1. In effect, its typical values range between 0.8 and 0.99.
-
Iterations at each Te mper ature
For inc reased effic iency of the algorith m, the number of ite rations is very important. Using a certain number of iterations for each te mperature is the proper solution. [15] suggests the realizat ion of only one, iteration for each temperature, wh ile the temperature decrement should take place at a really slow pace that can be expressed as:
The key para meters of algorith m a re In itia l temperature, Fina l te mperature, Cool Sched () and ma ximu m nu mber of generations which is used here as a stopping criteria to choose the best suitable values of key parameters. The setup of SA approach was the following: In itia l te mperature = 3000C, Final temperature =1e -100C, Cool Sched () = 0.8% and ma ximu m number of generations = 1000. In each case study, 10 independent runs were made for each of the optimization methods
Each SA approach was imp le mented in MATLA B
7.1 and all the programs were run on a 2.4 GHz
T (t) t (1
.t)
(10)
Pentium IV processor with 512 M B of RAM (Random Access Memory).
Where, takes a very low value.
-
-
-
SA Algorithm Implementation of ELD Proble ms
Step 1: Initia lization of te mperature, T, para meter and ma ximu m. Find, randomly, an initia l feasible solution, which is assigned as the current solution Si and perform ELD in order to calculate the total cost, Fcost, with the preconditions (4) and (6) fulfilled.
Step 2: Set the iteration counter to =1
Step 3: Find a neighboring solution Sj through a random perturbation of the counter one and calculate the new total cost, Fcost.
Step 4: If the new solution is better, we accept it, if it is worse, we calcu late the deviation of cost
S=S -S and generate a random number
-
Case study I
This case study consists of 38 generating units. All units are within the convex fuel cost characteristics for the above system is taken fro m [16]. In this case, the load demand expected to be determined is PD = 6000 MW. The B mat rix of the transmission loss coeffic ient is not considered in this system.
Table 2 shows the minimu m, mean cost, standard deviations and CPU time per iteration, cost achieved by the SA approach. As indicated in Table 2, the SA was the approach that obtained the min imu m cost for the ELD of 38 generating units. The best result obtained for solution vector Pi, i = 1 . . . 38 by SA with minimu m cost of 9153496.59 $/h is given in Table 2 and Table 2 also compares the results obtained with the SPSO, PSO_ Cra zy, Ne w PSO and PSO_TVA C [17] this paper with those of other studies reported in the literature and the convergence behavior of Case study I is shown in Figure 1.
x 106
j i 9.5
Total Operating Cost
uniformly distributed over (0, 1).
9.4
PD=6000 MW
If e
S / t
(0,1)
(11)
9.3
Accept the new solution Sj to replace Si.
Step 5: If the stopping criterion is not satisfied, reduce temperature using para meter :
T (t) =. t and return back to Step 2.
-
-
Results and Discussion
In this paper, to evaluate the effectiveness o f the proposed SA approach, two case studies (38 and 110 generating units) of ELD proble ms were applied in which the objective functions were conve x fuel cost characteristics in the power system operation.
9.2
9.1
0 200 400 600 800 1000
Generations
Figure 1.Convergence characteristics of 38 unit system (PD=6000MW)
Generator
Power
O/P(MW)
SPSO
PSO_
Crazy
Ne w PSO
PSO_ TYAC
SA
Pg1
519.097
366.631
550
443.659
405.6512
Table2: Co mparison of results for case study I
Pg2
437.92
550
512.263
342.956
405.6512
Pg3
374.789
467.129
485.733
433.117
408.6681
Pg4
394.877
370.471
391.083
500
408.6681
Pg5
356.603
425.712
433.846
410.539
408.6681
Pg6
380.358
415.226
358.398
482.864
408.6681
Pg7
300.234
339.872
415.729
409.483
408.6681
Pg8
335.871
289.777
320.816
446.079
408.6681
Pg9
238.171
195.965
115.347
119.566
114
Pg10
218.563
170.608
204.422
137.274
114
Pg11
196.63
138.984
114
138.933
114
Pg12
234.5
262.35
249.197
155.401
117.804
Pg13
111.529
114.008
118.886
121.719
110
Pg14
100.731
92.393
102.802
90.924
90
Pg15
122.464
89.044
89.039
97.941
82
Pg16
125.31
130.555
120
128.106
325
Pg17
155.981
167.85
156.562
189.108
157.0614
Pg18
65
65.754
84.265
65
65
Pg19
70.071
65
65.041
65
65
Pg20
263.95
199.594
151.104
267.422
272
Pg21
245.065
272
226.344
221.383
272
Pg22
191.702
130.379
209.298
130.804
260
Pg23
99.123
173.544
85.719
124.269
123.6755
Pg24
15.058
13.263
10
11.535
10
Pg25
60.06
112.161
60
77.103
107.5567
Pg26
91.14
105.898
90.489
55.018
84.8289
Pg27
41.006
35.995
39.67
75
35.3695
Pg28
20.399
22.335
20
21.682
20
Pg29
34.65
30.045
20.995
29.829
20
Pg30
20.957
24.112
22.81
20.326
20
Pg31
20.219
20.494
20
20
20
Pg32
25.424
20.011
20.416
21.84
20
Pg33
26.517
27.44
25
25.62
25
Pg34
18.822
18
21.319
24.261
18
Pg35
9.173
8.024
9.122
9.667
8
Pg36
26.507
25
25.184
25
25
Pg37
24.344
20
20
31.642
21.0081
Pg38
27.181
24.371
25.104
29.935
20.3849
Table 3: Best results comparison for case study I
-
Case study II
In this case study a large scale data consisting of 110 unit generating unit system is emp loyed, having convex fuel cost characteristics without including line losses
.The input data of the entire system is taken from S. O. Orero paper [18]. In this case study, there are three load demands, Low (PD = 10000 MW), Mediu m (P D = 15000 MW) and High (PD = 20000 MW) e xpected to be determined.
Tables 5 shows the Best Power Output of 110 unit system for PD=10000MW, PD=15000MW and PD=20000MW. As indicated in Table 4, the SA was the approach that obtained the min imu m cost for the ELD of 110 generating units.
The best result obtained by SA with minimu m cost for PD=10000MW, PD=15000MW and PD=20000MW of 131973.9018 $/h, 198352.6413 $/h and 313184.2522
$/h respectively is given in Table 4 and also compares
the results obtained with the SAB, SAF [19] in this paper with those of other studies reported in the literature and the convergence behavior of Case study II is shown in Figure 2, and Table 6 shows Standard deviation and CPU time for different test cases.
Table 4: Best results comparison with diffe rent approaches for diffe rent loads for case study II
Table 5: Best power output of 110 unit system for various loads
Generator Power O/P
Power Demand (MW )
Generator Power O/P
Power Demand (MW )
10000
15000
20000
10000
15000
20000
Pg1
2.4018
2.4031
12
Pg56
25.2 25.2
96
Pg2
2.4
2.4
12
Pg57
25.2
50.0387
96
Pg3
2.4
2.4
12
Pg58
35
35
100
Pg4
2.4
2.4
12
Pg59
35
35.003
100
Pg5
2.4
2.4
12
Pg60
45
45
120
Pg6
4
4
20
Pg61
45
45
120
Pg7
4
4
20
Pg62
45
45
120
Pg8
4
4
20
Pg63
54.3
164.7334
185
Pg9
4
4
20
Pg64
54.3
184.4727
185
Pg10
15.2
15.778
76
Pg65
54.3
177.8478
185
Pg11
15.2
76
76
Pg66
54.3
185
185
Pg12
15.2
46.249
76
Pg67
70
70
197
Pg13
15.2
49.3024
76
Pg68
70
70
197
Pg14
25
25
100
Pg69
70
70
197
Pg15
25
25
100
Pg70
150
360
360
Pg16
25
25
100
Pg71
400
400
400
Pg17
109.546
155
155
Pg72
400
400
400
Pg18
95.5364
155
155
Pg73
60
104.8277
300
Pg19
110.3678
155
155
Pg74
50
146.4736
250
Pg20
105.0814
155
155
Pg75
35.2032
90
90
Pg21
68.9
68.9
197
Pg76
50
50
50
Pg22
68.9
68.9
197
Pg77
160
160
450
Pg23
68.9
68.9
197
Pg78
150
272.0709
600
Pg24
350
350
350
Pg79
50
147.4288
200
Pg25
400
400
400
Pg80
20
120
120
Pg26
400
400
400
Pg81
10
10
55
Pg27
140
500
500
Pg82
12
12
40
Pg28
140.3855
500
500
Pg83
20
20.0228
80
Pg29
50.0496
200
200
Pg84
50
200
200
Pg30
35.3865
100
100
Pg85
83.392
325
325
Pg31
10
10
50
Pg86
269.215
440
440
Pg32
12.2522
20
20
Pg87
10
35
35
Pg33
20
80
80
Pg88
20
20
55
Pg34
75
250
250
Pg89
20
75.0219
100
Pg35
196.4132
360
360
Pg90
40
220
220
Pg36
219.4718
400
400
Pg91
30.0073
45.2315
140
Pg37
14.7661
40
40
Pg92
40
77.5334
100
Pg38
20
70
70
Pg93
440
440
440
Pg39
25
100
100
Pg94
370.1674
500
500
Pg40
20
120
120
Pg95
600
600
600
Pg41
40
180
180
Pg96
305.6974
457.955
700
Pg42
50
220
220
Pg97
3.6
3.6
15
Pg43
440
440
440
Pg98
3.6
3.6
15
Pg44
560
560
560
Pg99
4.4
4.4
22
Pg45
660
660
660
Pg100
4.4
22
22
Pg46
421.9594
594.5063
700
Pg101
10
10
60
Pg47
5.4
5.4
32
Pg102
10
10
80
Pg48
5.4
5.4
32
Pg103
20
20
100
Pg49
8.4
8.4
52
Pg104
20
20
120
Pg50
8.4
8.4
52
Pg105
40
40
150
Pg51
8.4
8.4
52
Pg106
40
40
166.0789
Pg52
12
12
60
Pg107
50
50
131.9211
Pg53
12
12
60
Pg108
30
30
150
Pg54
12
12
60
Pg109
40
40
320
Pg55
12
12
60
Pg110
20
20
200
x 105
Total Operating Cost
6
4
2
0
PD=10000 MW
PD=15000 MW
PD=20000 MW
Acknowledge ment
The authors are thankful to Director, Madhav Institu te of Technology & Science (MITS), Gwa lior (M.P) India for providing support and facilit ies to carry out this research work.
References
-
H.T. Yang, P.C. Yang and C.L. Huang, Evolutionary Programming based economic dispatch for units with non- smooth fuel cost functions, IEEE Trans. Power Syst., 1996, Vol. 11, no. 1, pp. 112-118.
-
D.C. Walter and G.B. Sheble, Genetic algorithm solution
0 200 400 600 800 1000
Generations
Figure 2.Convergence characteristics of 110 unit system with various loads
Table 6: Standard deviation and CPU time fo r diffe rent test cases
TES T CAS ES
Test case I
Test case II
Standard De viation ($/hr)
0.1200
1.36
CPU time /ite ration(sec)
0.237
0.245
-
-
-
Conclusions
This paper presents the Simu lated Annealing (SA) approach for optimizat ion of Economic Load Dispatch (ELD) proble ms. Practical generator operation is modeled using with piecewise quadratic cost functions . Algorith ms have been developed for the determination of the global or near-global optima l solution for the ELD proble ms. The proposed SA approach has produced results comparable or better than those generated by other evolutionary algorithms and the solutions obtained have superior solution quality and good convergence characteristics and the strength of the method was demonstrated by the change in load demands of the problems. Because of in the deregulated environment where cost min imization not only the objective, but at the same time profit ma ximizat ion is also concern. Fast and accurate economic load dispatch solution is as usual requirement in deregulated scenario as well. Therefore, results show that SA based optimization is a pro mising technique for solving complicated and large ELD proble ms in electrica l power system.
of economic dispatch with valve-point loading IEEE Trans. Power Syst., 1993, Vol. 8, No. 3, pp. 1125-1132.
-
L.S. Coelho and V.C. M ariani, Combining of chaotic differential evolution and quadratic programming for economic dispatch optimization with valve-point effect, IEEE Trans. Power Syst., 2006, Vol. 21, No. 2, pp. 989-996.
-
J.H. Park, Y.S. Kim, I.K. Eom, and K. Y Lee., Economic Load Dispatch for price wise Quadratic Cost Function Using Hopfield Neural Network, IEEE Trans. on Power Systems, 1993, Vol. 8, No. 3, pp . 1030-1038.
-
B.H. Choudhary and S. Rahman, A review of recent advances in economic dispatch, IEEE Trans Power Syst., 1990, Vol. 5, No. 4, pp. 124859.
-
K.Y. Lee, Fuel cost minimization for both real and
reactive power dispatches, IEE Proc C, Gen Transm Distrib
1984., Vol. 131, No. 3, pp. 8593.
-
G.V. John lachogiannis and K.Y. Lee, Economic load dispatch a comparative study on heuristic optimization techniques with an improved coordinated aggregation-based PSO, IEEE Trans. Power Syst., 2009. Vol. 24, No. 2, pp. 991-1001.
-
K. T. Chaturvedi, M . Pandit and L. Srivastava, Self- Organizing Hierarchical Particle Swarm Optimization for Non-Convex Economic Dispatch, IEEE Trans. Power Syst. 2008, Vol. 23, No. 3, pp. 1079-1087.
-
B. K. Panigrahi and V. R. Pandi, Bacterial foraging optimization nelder mead hybrid algorithm for economic load dispatch. IET Gener. Transm. Distrib, 2008, Vol. 2, No. 4, pp 556-565.
-
S. Kirkpatrick, C. Gellat and M . Vecchi, Optimization by Simulated Annealing, Science, 1983, Vol. 220, pp. 45-54.
-
Farhad Kolahan and M ahdi Abachizadeh, Optimizing Turning Parameters for cylindrical Parts using simulated Annealing M ethod, International journal of Engineering and Applied Science, 2010, Vol. 6, No. 3, pp.149-152.
-
J.B. Park, K.S. Lee, J. R. Shin and K.Y. Lee, A particle swarm optimization for economic dispatch with non-smooth cost functions, IEEE Trans. Power Syst., 2005, Vol. 20, No. 1, pp. 34-42.
-
Dowsland K.A., 1995. Simulated Annealing in M odern Heuristic Techniques for Combinatorial Problem. McGraw- Hill.
-
E. Aarts, Jan H.M . Korst, Peter Laarhoven and J. M . Van, A Quantitative Analysis of the Simulated Annealing Algorithm, A Case Study for the Travelling Salesman Problem. Journal of Statistical Physics 1988, Vol. 50, pp.1-2.
-
M. Lundy, Applications of the annealing algorithm to combinatorial problems in statics, Biometrika, 1985, Vol. 75, pp. 191-198.
-
M .A. Sydulu, Very fast and effective non-iterative
Lamda Logic Based algorithm for economic dispatch of thermal units, In: Proceedings of IEEE region 10 conference TENCON, 1999, Vol. 2, pp. 14347.
-
K.T. Chaturvedi, M anjaree Pandit and Laxmi Srivastava, Particle swarm optimization with time varying acceleration coefficients for non-convex economic power dispatch, Electrical Power and Energy Systems, 2009, Vol. 31, pp.249257.
-
S. O. Orera and M . R. Irving, Large scale unit commitment using a hybrid genetic algorithm, Electrical Power & Energy Systems, 1997, vol. 19, no. 1, pp. 45-55.
-
G. S. S. Babu, D. B. Das and C. Patvardhan, Simulated
annealing variants for solution of economic load dispatch,
IE(I) J.-EL,2002,, 82, pp. 222-229.
-
Wood A.J. and B. F. Wollenberg, Power Generation Operation and Control, Wiley, New York, 2nd ed.,1996.