1 An Optimal Power Flow plus Transmission Costs Solution Pablo Oñate Y., Juan M. Ramirez, Carlos A. Coello Coello Cinvestav – Unidad Guadalajara. Av. Cientifica 1145. Col. El Bajio. Zapopan, Jal., 45015. Fax (+52)(33) 3777 3600, email : ponate[jramirez]@gdl.cinvestav.mx, ccoello@cs.cinvestav.mx. Abstract: This paper is aimed at the solution of the optimal power flow (OPF) problem with embedded security constraints (OPF-SC) by the particle swarm optimizer. The major objective is to minimize the overall operating cost while satisfying the power flow equations, system security, and equipment operating limits. The overall operating cost is composed by the generation cost, transmission cost, and the consumer benefit. A modification of the conventional particle swarm optimizer (PSO) has been used as the optimization tool, which uses reconstruction operators and dynamic penalization for handling constraints. The reconstruction operators allow the increase of the number of particles within the feasible region. The power equations mismatch, loss active power transmission, and voltages are calculated by the Newton-Raphson method. To demonstrate its robustness, the proposed algorithm was tested on systems from the open literature. Several cases have been studied to test and validate the proposed approach. Keywords: Optimal power flow, Particle swarm optimizer, Security constraints, Evolutionary computation. 1. Introduction The OPF objective is to meet the required demand at minimum production cost, satisfying units’ and system's operating constraints, by adjusting the power system control variables [1 - 3]. The power system must be capable of withstanding the loss of some or several transmission lines, transformers or generators, guaranteeing its security; such events are often termed probable or credible contingencies. Different security criteria have been used to ensure sufficient security margins. One of them is the N-1 criterion, widely used nowadays. To determine the credible contingencies, in this paper a contingency ranking is used [4]. The problem of the two precedent paragraphs, when they are put together, is termed the optimal power flow with security constraints (OPF-SC). Through an optimal power flow formulation, a method for computing the optimal pre- and post-contingency 2 operating points is presented. Likewise, constraints in generating units' limits, minimum and maximum up- and down-time, slope-down and slope-up, a voltage profile improved and coupling constraints between the pre- and the post-contingency states have been taken into account. Nowadays, with the electrical power industry deregulation, the transmission system can be considered as an independent transmission company that provides open access to all participants. Any pricing scheme should compensate transmission companies fairly for providing transmission services and allocate entire transmissions’ costs among all users. Different methods to allocate transmission costs among network users have been applied worldwide [5, 6]. This paper employs a transmission pricing scheme using a power flow tracing method [7, 8, 9] to estimate the actual contribution of generators to each flow in the links. Some conventional optimization techniques have been utilized for solving the OPFSC, for instance: linear programming, sequential quadratic programming, generalized reduced gradient method, and Newton methods [1-3]. Although some of these techniques have good convergences’ characteristics, some of their major drawbacks are related to their convergence to local solution instead of global ones, if the initial guess is located within a local solution neighborhood. The theoretical assumptions behind such algorithms may be not suitable for the OPF-SC formulation. Optimization methods such as simulated annealing (SA), evolutionary programming (EP), genetic algorithms (GA) and particle swarm optimizer (PSO) have been employed to overcome such drawbacks. Important contributions on power systems optimization applications have been presented in [10 - 19]. In [20], PSO has been used to solve the OPF. Additionally, in [21 - 22] a modified PSO, with improved convergence characteristics, is applied to the same aim. Three types of PSO algorithms are proposed in [23 - 24], all of which have been applied to solve optimization problems related to reactive power and voltage control. In this paper, for solving the OPF-SC, a particle swarm optimizer with reconstruction operators (PSO-RO) is proposed. For handling constraints, such reconstruction operators plus an external penalization are adopted. The reconstruction operators allow that all particles represent a possible solution, satisfying the units’ operating constraints, and increasing the number of particles able to search for optimal solution, thus 3 improving the achieved solution quality. 2. Particle Swarm Optimizer summary The PSO earliest version was intended to handle only nonlinear continuous optimization problems [26]. However, its further development elevated its capabilities for handling a wide class of complex optimization problems [25 - 28]. A PSO algorithm consists of a population continuously updating the searching space knowledge. This population is formed by individuals, where each one represents a possible solution and can be modelled as a particle that moves through the hyperspace. The position of each particle is determined by the vector xi ∈ Rn and its movement by the particle’s velocity vi ∈ Rn, G G G (1) xiiter +1 = xiiter + viiter +1 The information available for each individual is based on both its own experience and the knowledge of the performance of other individuals in its neighborhood. Since the relative importance of these two factors can vary, it is reasonable to apply random weights to each part, and therefore the velocity is determined by: JJJJJJG G G G viiter +1 = wviiter + C1 × rand() × ( pbest i − xi )... JJJJJG G + C2 * Rand()* ( gbest i − xi ) (2) where iter is the current iteration; C1 and C2 are two positive learning factors; rand() and Rand() are two randomly generated values within [0, 1]; w is known as the inertia weight, and it plays the role of balancing the global and local search performed by the algorithm [29, 30]. 3. Objective function The OPF-SC goal is to optimize an objective function subject to equality and inequality constraints. The optimization problem is formulated as follows: Min F obj ( u, y ) (3) g( u, y ) = 0 (4) hmin ≤ h( u, y ) ≤ hmax (5) subject to where g(·,·) represents the equality constraints set; h(·,·) is the inequality constraints set; u are the state variables; y represent both integer and continuous control variables. 3.1 Objective function In this paper, the minimization of the total cost includes the pre-contingency cost 4 (superscript 0) besides each credible contingency cost (superscript k). Thus, the objective function is constituted by three terms: (i) the generating costs, (ii) the transmission costs, and (iii) the consumer benefit [31], F obj ⎧ o K k⎫ = min ⎨C + ∑ C ⎬ k =1 ⎩ ⎭ ( (6) ) C o = ∑ U i0 * f ( PGio ) + SUCi + TC o ( FLWmo− n ) − NG i =1 ( ) C k = ∑ U ik * f ( PGik ) + SUCi + TC k ( FLWmk− n ) − NG i =1 ∑ B(P ) NLoad ∑ (B(P ) − D(P NLoad j =1 k Loadj (7) Loadj j =1 k Loadj o ,PLoadj ) ) (8) where: K is the total number of credible contingencies Co represents the base case operating cost U io i-th unit’s pre-contingency state , 1-ON, 0-OFF NG is the total number of available generators f ( PGio ) i-th generator’s function cost at time t PGio active power supplied by the i-th generator at the pre-contingency state SUCi i-th generator’s start- up cost TC o (.) pre-contingency transmission cost, (9) NLoad total number of load buses. B( PLoadj ) is the consumer benefit curve for j-th load at time t PLoadj pre-contingency active power consumption at the j-th load Ck credible contingencies’ cost D(.) represents the load interruption cost k PLoadj post-contingency active power consumption at the j-th load TC k (.) post-contingency transmission cost, defined as (9): M TC = ∑ cm ( MWgi ,m )Lm MWgi ,m m =1 where M lines set cm (.) cost per MW per unit length of line m (9) 5 Lm length of line m in miles MWgi ,m flow in line m, due to the i-th generator. 3.2 Constraints In the following, different constraints included in the OPF-SC formulation are detailed. 3.2.1 Equality constraints at the pre- and post-contingency states This is the set of nonlinear power balance equations that govern the steady-state power flow formulation, both- at pre and post-contingency state, defined as follows: NG 0 = ∑P − i =1 o Gi ∑ (P ) − P NLoad j =1 NG 0 = ∑ QGio − i =1 NG NLoad i =1 j =1 0 = ∑ PGik − NG 0 = ∑ QGik ,t − i =1 ∑ NLoad ∑Q j =1 o Loadj k PLoadj − PLoss k NLoad ∑Q j =1 o Loadj k Loadj ,t − QLosstk o Loss (10) − QLoss o (11) for k = 1, 2,....,K (12) for k = 1, 2,....,K (13) where PLoss represents the total active power losses, QLoss are the total reactive power ones, and K is the total number of credible contingencies. 3.2.2 Inequality constraints at the pre- and post-contingency states This is the set of continuous and discrete constraints representing the system’s operational and security limits as bounds. (i) The active power generated by each unit must satisfy the maximum and minimum operating limits, both for pre- and post-contingency states. PGi _ MIN ≤ PGio ≤ PGi _ MAX (14) PGi _ MIN ≤ PGik ≤ PGi _ MAX (15) (ii) Voltage magnitudes at each load bus must be close enough to the reference voltage min Vref − V j (16) where Vref is the reference voltage magnitude, Vj is the voltage magnitude at the j-th load bus. (iii) The active power flow through each branch of the network must satisfy the security limits 6 FLOWijo ≤ FLOWijo_ MAX ∀ i, j, i ≠ j (17) FLOWijk ≤ FLOWijk_ MAX ∀ i, j, i ≠ j (18) where FLOWij0_ MAX , FLOWijk_ MAX , represent the maximum active power that should flow through the branch connecting the buses i-j, during the pre-contingency and each postcontingency state, respectively. 4. Transmission cost allocation To calculate the transmission cost allocation, the average participation factor (APF) method [5, 8, 9] has been used. It is based on a general transportation problem of how the flows are distributed on a meshed network. The only requirement is related to the Kirchhoff’s first law fulfillment. Once the power flow scenario is determined, the main idea of this methodology is to determine the agents’ (generator and loads) participation factor in the flow in links. In this sense, it will be possible to trace the flow of electricity from a generator to the load buses. The principle adopted to trace these flows is the proportional sharing principle, schematized in Fig 1. The assumption made is that the bus is a perfect mixer of all incoming flows, so that it is impossible to determine which particular inflowing electron goes into which particular outgoing line. It may be assumed that each element flow leaving the i-th bus can be decomposed into M shares, where M is the number of incoming flows (generator and elements injecting power into bus i). The amount of such shares has the same proportion that the incoming flows in the total power injected into bus i [5, 8]. 5. Proposed solution The proposed methodology runs as follows: STEP 1: randomly generated initial population STEP 2: for each particle, the reconstruction operators are applied STEP 3: the Newton-Raphson routine is applied to each particle STEP 4: fitness function evaluation STEP 5: compare particles’ fitness function and determine pbest and gbest STEP 6: change of particles’ velocity and position according to (1) - (2) STEP 7: go to step 2 until a criterion is met (maximum number of generations) 5.1. Initial population 7 In this paper, a particle is composed by continuous and discrete control variables. The continuous ones include the generators’ active power output and the load’s active power; the discrete variables are associated with the transformers-tap setting and varinjection values of the switched shunt capacitors/reactors, Fig 2. The population is constituted by K+1 matrices, one for the base case and one for each of the K credible contingencies (subpopulations) of dimension (NG+ND) x NIND; where K represents the total number of accounted contingencies; NG is the number of continuous variables; ND is the number of discrete variables; NIND is the number of particles. For each scenario (pre- and post-contingency states), the initial active power is a percentile and is randomly allocated among the NG available thermal units, such that the load is satisfied (19), PGin = rand( NG ) ∑ rand( NG ) Nload * ∑P j =1 LOADj for n = 0 ,1,....,K (19) where, rand(NG) represents a vector of size NG randomly generated within the interval [0, 1]. The transformer-tap setting and var-injection values of the switched shunt capacitor/reactor (discrete variable) are randomly generated between upper and lower limits. An operator is included to ensure that each discrete variable is rounded to its nearest decimal integer value that represents the physical operating constraint of a given variable. ( round random ⎡⎣ STi min ,STi max ⎤⎦ , η ) (20) where η represents the most significant decimal. 5.2. Reconstruction operators In this paper, the reconstruction operators have been used to satisfy the units' constraints. Taking into account the inequalities within a conventional formulation, by using penalty functions, for instance, results in an execution where it is very likely to make wrong decisions, due to the use of excessively high penalty factors. Altogether, the PSO and the operators, accomplish such handling in a more efficient way, limiting the use of penalization. That is, such mechanisms control that each continuous variable fulfills the generation limits, load and discrete variable limits for the pre- and post- 8 contingencies states. For each state the following reconstruction operators have been applied. 5.2.1. Control variables operating limits This operator is defined as ⎧ PGi _ MAX ⎪ ⎪P PGi' = ⎨ Gi ⎪ PGi _ MIN ⎪⎩0 if PG ,i > PGi _ MAX if PG ,i _ MIN < PGi < PG ,i _ MAX if λ * PGi _ MIN < PGi ≤ PGi _ MIN (21) otherwise The operator, besides satisfying the active power generation limits, is useful for avoiding the use of additional variables in order to determine the units’ state; thus, for those units in which the active power is below a predefined percentage, the off state is chosen (PGi=0). Likewise, 'k PLoad ,j o ⎧ PLoad ,j ⎪ o − = ⎨ PLoad , j − Δ Load , j ⎪Pk ⎩ Load , j if k o PLoad , j > PLoad , j − k o if PLoad , j < PLoad , j − Δ Load , j otherwise (22) k = 1, 2,.....,K and j = 1,2,.....,NLoad ST j' k ⎧u max j ⎪ min = ⎨u j ⎪ ST ⎩ j if ST j > u max j min if ST j < u j otherwise (23) k = 0 ,1,.....,K and j = 1,2,.....,ND where Δ −Load , j is the maximum allowed load interruption at bus-j. 5.2.2. Handling constraints for load balance After the execution of the precedent operation, the total active power assigned to the thermal units is not necessarily equal to the demanded load. Thus, a re-dispatch is required for taking into account the available units. Such re-dispatch must deal with constraints [31]. 5.3. Newton-Raphson load flow Once the reconstruction operators have been applied and the control variables’ values are determined, for each particle a load flow run is performed. Such flow run allows evaluating the branches’ active power flow and the total losses, which are assigned to the slack bus. 5.4. Fitness function 9 To handle the active power flow limits and voltage constraints, the objective function penalization is used. By this technique, the fitness function is composed by the objective function (6) plus penalty terms for particles violating some power flow and/or voltage constraint. Such fitness function can be expressed as follows: Fi fit = Fi obj + Cte( iter ) N _ OFLW ∑ j =1 OverFlow j + Fi obj NLoad ∑ j =1 Vref − V j , i = 1,..,NIND (24) i where, N_OFLW represents the total number of lines with overflow; NIND is the number of individuals; OverFlowj,t is defined as in (25). abs( FLOWi , j _ MAX − FLOWi , j ) (25) FLOWi,j_MAX, is the maximum allowable flow across the line connecting buses i-j; Cte(iter) is a dynamically modified penalty value: Cte(iter ) = 300 iter , this one, allows an increasing penalization throughout generations. 5.5. Updating The new position and velocities can be evaluated by (1)-(2). 6. Test results The proposed algorithm was implemented in Matlab, and the IEEE New England test system is employed to validate its potential. The test system consists of ten thermal units, 39 buses, 46 transmission lines and tap-changing transformers, feeding a total load of 6097.5 MW and 1409 MVAR. A detailed description of the system’s data is available in [32]. The operating range of all transformers is set between [0.9, 1.1] with a discrete step size equal to 0.01. A quadratic fuel cost function is used, and its coefficients are displayed in Table 1. In this paper, the transmission costs are counted as a portion of the generating ones, ¡Error! No se encuentra el origen de la referencia.; their proportions are displayed in Table 2. TCgi ,m = ( agi MWgi2,m + bgi MWgi ,m + cgi )* Pm (26) Three cases are analyzed. Case 1: An OPF-SC neglecting transmission costs while improving the voltage profile. Case 2: Both the transmission costs and voltage profile improvement are considered within the objective function and fitness function, respectively. Case 3: In the previous cases, the tap-changing transformers are not included as control variables; in this case, these ones are included as such ones. In all cases, the tripping of 10 line 26-27 is considered as the contingency. To demonstrate the consistency and robustness of the developed algorithm, 20 independent runs are conducted for each case to count for the number of times in which the optimal or near optimal solution is reached; different stopping criteria are considered (maximum iterations). Results and computational times are exhibited in Table 3. Table 3 shows that with 30 iterations, the best solution is as good as with 50 iterations, although the standard deviation in the latter case is better. The best results obtained using the PSO-RO are shown in Table 4. The inclusion of a penalization term into the objective function has allowed the voltage profile improvement. The total deviation voltage is reduced from 1.1170 p.u. (case 1) to 0.9246 p.u. (case 2), and to 0.5905 p.u (case 3) for the pre-contingency state, and from 0.9738 p.u. (case 1) to 0.9058 p.u. (case 2), and to 0.5885 p.u (case 3) for the post-contingency state. The routines utilized in these studies are implemented in Matlab 7.0 on a personal computer with a Pentium 4 processor, running at 2.99Ghz and with 1GB of RAM. 7. Conclusions This paper investigates the applicability of the PSO-RO in solving the OPF-SC problem including transmission costs. Moreover, inequality constraints have been added in the formulation in order to improve the voltage profile. Traditionally, PSO handles constraints by the objective function penalization. The reconstruction operators are an alternative mechanism for managing the units' operative constraints, while particles violating some power flow or bus voltage are penalized. The use of reconstruction operators allows increasing the number of suitable particles in the searching space. Thus, the dependency of the heuristic algorithms on the appropriate definition of the penalization terms is reduced. 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C. Eberhart, “A modified particle swarm optimizer”, IEEE International Conference on Evolutionary Computation, Anchorage, Alaska, May. 4-9, 1998, pp. 69-73. 31. P. E. Oñate, J. M. Ramirez, C. A. Coello, “Optimal power flow subject to security constraints with particle swarm optimizer” IEEE Transactions on Power Systems, Feb. 2008, Vol.23, No 1, pp. 33 – 40. 14 32. M. A. Pai, Energy function analysis for power system stability, Norwell, MA: Kluwer, 1989. 15 An Optimal Power Flow plus Transmission Costs Solution Pablo Oñate Y., Juan M. Ramirez, Carlos A. Coello Coello j l 40 MW 12 MW 18 MW 60 MW i 28 MW 42 MW k m Fig. 1. Proportional sharing concept 16 An Optimal Power Flow plus Transmission Costs Solution Pablo Oñate Y., Juan M. Ramirez, Carlos A. Coello Coello i-th PARTICLE Fig. 2. Particle’s representation. …. STND STi means discrete variables …. STi …. ST2 ST1 PLoad,NL …. PLoad,i …. PLoad,2 PLoad,1 PG,NG PG,i PG,2 PG,1 …. 17 An Optimal Power Flow plus Transmission Costs Solution Pablo Oñate Y., Juan M. Ramirez, Carlos A. Coello Coello Table 1: Fuel cost coefficients 2 Bus a i [$/MW ] b i 30 0.0193 31 0.0111 32 0.0104 33 0.0088 34 0.0128 35 0.0094 36 0.0099 37 0.0113 38 0.0071 39 0.0064 [$/MW] c i [$] 6.9 3.7 2.8 4.7 2.8 3.7 4.8 3.6 3.7 3.9 0 0 0 0 0 0 0 0 0 0 18 An Optimal Power Flow plus Transmission Costs Solution Pablo Oñate Y., Juan M. Ramirez, Carlos A. Coello Coello Table 2: Coefficients of proportion (New England power system) 1 L1-2 2 L1-18 3 L2-3 4 L2-7 5 L2-8 Transmission cost coefficients (Pm) 6 7 8 9 10 11 L2-13 L2-26 L3-13 L4-8 L4-12 L5-6 12 L6-7 13 L6-11 14 L6-18 15 L6-19 16 L6-21 0.033 0.040 0.040 0.056 0.042 0.058 0.037 0.042 0.046 0.053 0.047 0.053 0.048 0.047 0.056 0.061 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 L7-9 L8-12 L9-10 L10-12 L10-19 L10-20 L10-22 L11-25 L11-26 L12-14 L12-15 L13-14 L13-15 L13-16 L14-152 L7-8 0.043 33 L15-16 0.036 0.054 0.060 0.058 0.049 0.060 0.042 0.046 0.064 0.049 0.051 0.037 0.054 0.055 0.058 34 35 36 37 38 39 40 41 42 43 44 45 46 L16-17 L16-20 L17-18 L17-21 L19-23 L19-24 L19-25 L20-21 L20-22 L21-24 L22-23 L22-24 L23-25 0.055 0.045 0.065 0.050 0.060 0.047 0.049 0.057 0.052 0.042 0.042 0.046 0.054 0.054 19 An Optimal Power Flow plus Transmission Costs Solution Pablo Oñate Y., Juan M. Ramirez, Carlos A. Coello Coello Table 3: Statistical data for cases 1-3 CASE 1 CASE 2 CASE 3 Gener NIND 20 30 50 20 30 50 30 50 36 36 36 36 36 36 36 36 Objective function Mean Best Worst 123970.0 123420 124580 123518.7 122990 124410 123223.9 122918 123810 217804.7 216130 219400 216474.7 215860 218120 216140.7 215660 216620 190090.7 176620 207440 184352.4 174940 188810 Standart Deviation 373.67 391.44 216.33 865.11 616.93 323.05 9552.04 3847.3 Average time (seg) 290 436 610 406 707 960 554 875 20 An Optimal Power Flow plus Transmission Costs Solution Pablo Oñate Y., Juan M. Ramirez, Carlos A. Coello Coello Table 4: Optimization results for the New England power system CASE 1 CASE 2 CASE 3 PG [MW] pre-cont 26-27 out pre-cont 26-27 out pre-cont 26-27 out 239.83 250.98 243.69 229.53 393.03 393.03 611.28 587.86 468.68 509.26 643.10 643.10 698.20 629.00 641.35 530.67 739.50 739.50 750.00 683.98 750.00 703.48 708.32 708.32 439.58 416.80 650.00 551.24 175.51 175.51 653.45 750.00 750.00 750.00 713.32 713.32 531.51 549.67 750.00 750.00 624.03 624.03 435.64 452.13 447.26 513.79 593.18 593.18 783.20 900.00 889.50 900.00 641.95 641.95 994.87 939.37 580.52 739.23 908.59 908.59 Position taps 1.025 1.025 1.025 1.025 0.91 1.00 1.070 1.070 1.070 1.070 1.10 1.10 1.070 1.070 1.070 1.070 1.10 1.10 1.006 1.006 1.006 1.006 1.04 0.95 1.006 1.006 1.006 1.006 0.99 1.09 1.060 1.060 1.060 1.060 1.09 1.10 1.070 1.070 1.070 1.070 1.09 1.04 1.009 1.009 1.009 1.009 1.00 1.10 1.025 1.025 1.025 1.025 0.94 0.96 1.025 1.025 1.025 1.025 1.02 0.90 1.025 1.025 1.025 1.025 0.97 0.97 Loss active power 40.06 62.29 73.51 79.70 43.03 48.59 Total deviation voltage [p. u.] 1.1170 0.9738 0.9246 0.9058 0.5905 0.5885 Total transmition cost [$] 6374.50 5895.90 5473.60 5044.90 Objective function [$] 61339.0 61579.0 63209.0 62398.0 63564 63552 Fitness function 122918.0 215660 174940 21 An Optimal Power Flow plus Transmission Costs Solution Pablo Oñate Y., Juan M. Ramirez, Carlos A. Coello Coello Figures caption Fig. 1. Proportional sharing concept Fig. 2. Particle representation. 22 An Optimal Power Flow plus Transmission Costs Solution Pablo Oñate Y., Juan M. Ramirez, Carlos A. Coello Coello Figures caption Table 1: Fuel cost coefficients Table 2: Proportions coefficients (New England power system) Table 3: Statistical data for cases 1-3 Table 4: Optimization results for the New England power system