11-E-PSS-1993 Simultaneous Coordinated Tuning of UPFC and Multi-Input PSS for Damping of Power System Oscillations Yashar Hashemi , Javad Morsali , Rasool Kazemzadeh Mohammad Reza Azizian , Ahmad Sadeghi Yazdankhah ﻣ ﺘ ﻠ ﺐ ﺳ ﺎ ﯾ ﺖ m o c . e t i S b a l t a M Sahand University of Technology Iran Keywords: Power oscillation damping, Simultaneous coordinated designing, Unified power flow controller (UPFC), Multi-input power system stabilizer (MPSS) performance than the conventional single input PSS and UPFC coordination. Abstract The objective of this work is to coordinated design controllers that will enhance damping of power system oscillations. With presence of FACTS device as UPFC Two specific classes of PSS have been investigated, the first one is a conventional power system stabilizer (CPSS) and the second is Multiinput power system stabilizer (MPSS). Since uncoordinated CPSS (or MPSS) and UPFC damping controller may cause unwanted interactions, it is necessary to simultaneous coordinated tune the controller parameters. The problem of coordinated design is formulated as an optimization problem and particle swarm optimization algorithm is employed to search for optimal parameters of controllers. A Multi-input signal PSS is introduced to maintain the robustness of control performance in a wide range of oscillation frequency. Finally in a system having a UPFC a comparative analysis between results from application of the MPSS and CPSS is presented. The eigenvalue analysis and the time domain simulation results show that the multi-input PSS and UPFC coordination provides a better 1. Introduction Power systems contain many modes of oscillation as a consequence of interactions of its components, as for example one generator rotor swinging relative to another. With the lack of sufficient damping oscillations resulting from small signal instability can be of increasing amplitude which could lead to power transfer restrictions and in extreme cases power system collapse. The frequency of these oscillations is usually in the range of 0.2-3 Hz [1]. There are two electromechanical modes of oscillations have reported [2]: a) local mode, with a frequency 0.8-3 Hz, which is related to oscillation in a single generator or a group of generators in the same area oscillate against each other; and b) inter area mode, with frequency 0.2-0.8 Hz, in which the units in one area oscillate against those in other area. Traditionally, the damping of low frequency oscillations is provided by installing a Power System Stabilizer (PSS) which uses local measurements such as rotor speed or active 1 MatlabSite.com ﻣﺘﻠﺐ ﺳﺎﯾﺖ Simultaneous Coordinated Tuning of UPFC and Multi-Input PSS for Damping of Power System Oscillations 26th International Power System Conference static phase shifting transformer using stochastic optimal control theory. Edris [9] proposed a simple control algorithm based on equal area criterion. Jiang et al [10] proposed a static phase shifting transformer control technique based on nonlinear variable structure control theory. In the literature, SVCs have been applied of a synchronous machine. Wang and Swift [11] used damping torque coefficients approach to investigate the SVC damping of a SMIB system on the basic of Phillips-Heffron model. It was shown that the SVC damping control provides the power system with negative damping when it operates at a lower load condition than the deal point, the point at which SVC control produces zero damping effect. Robust SVC controller based on H ∞ , structured singular value μ , and quantitative feedback theory QFT also have been presented to enhance system damping [12-14]. Research on the possible damping effect of UPFC, the most versatile FACTS devices, has also been conducted during the recent years. Besides the works in [15,16]. Dong, Zhang and Crow [17] proposed a PI based approach for the dynamic control of UPFC. In [18], a fuzzy logic based damping controller for UPFC was developed, and the effectiveness of this fuzzy controller was demonstrated in the simulation results of a two area four machine system. However, uncoordinated local control of FACTS devices and PSSs may cause unwanted interactions that further results in the system destabilization. To improve overall system performance, many researches were made on the coordination among conventional PSS and FACTS power oscillation damping (POD) controller [19-22]. Some of these methods are based on the complex non-linear simulation [19,20], the others are linear approaches [21,22]. A comparative analysis between results from application of the MPSS and CPSS in coordination with the UPFC as a FACTS device is presented in this paper. The problem of robust output feedback controller coordinated design is formulated as an power as feedback signals. The PSS method that is currently widely used is based on the signal ΔP formula ( ΔP − PSS ) with the effective power as the input. This method is applied to suppress the local power perturbation between generators. For the low frequency perturbation that occurs between power systems in wide-area operation, however there is little system perturbation information included in the active power, so ΔP − PSS has little effectiveness. As a solution to that problem, ΔP + Δω PSS, which uses the internal frequency or the rotational speed ( ω ) as well as the active power is effective for damping low frequency oscillations, is used. However, ω includes turbine and generator system axle torsion fluctuation, so consideration must be given to the use of a notch filter or other such devices when this input is used. Other effective way to damp power system swings is using Flexible Alternating Current Transmission Systems (FACTS) which is a genetic term for a group of technologies that radically increases the capacity of the transmission network while maintaining or improving voltage stability and grid reliability. This type of damping control is realized by adding a supplementary stabilizing signal on the primary control loops of FACTS devices. Many approaches have been adopted to design the FACTS controller. Several approaches based on modern control theory have been applied to TCSC controller design. Chen at al. [3] presented a state feedback controller for TCSC by using a pole placement technique. Chang and Chow [4] developed a time optimal control strategy for the TCSC where a performance index of time was minimized. A fuzzy logic controller for a TCSC was proposed in [5]. Heuristic optimization techniques have been implemented to search for the optimum TCSC based stabilizer parameters for the purpose of enhancing SMIB system stability [6,7]. A considerable attention has been directed to realization of various TCPS schemes. Baker et al [8] developed a control algorithm for ﻣ ﺘ ﻠ ﺐ ﺳ ﺎ ﯾ ﺖ m o c . e t i S b a l t a M 2 MatlabSite.com ﻣﺘﻠﺐ ﺳﺎﯾﺖ Simultaneous Coordinated Tuning of UPFC and Multi-Input PSS for Damping of Power System Oscillations 26th International Power System Conference optimization problem and PSO algorithm is employed to search for optimal controllers parameters. Firstly, the system eigenvalues without controllers and the second with proposed coordinating is investigated. It is quite evident that the system stability is greatly enhanced with the coordinated design of UPFC and MPSS, as the damping ratio of the electromechanical mode eigenvalue has been greatly improved. In this study the nonlinear time-domain simulation is carried out to validate the effectiveness of the proposed controllers. The controllers are simulated and tested under different operating conditions. ⎡ mE cos δ EVdc ⎤ − xE ⎤ ⎡iEd ⎤ ⎢ ⎥ 2 ⎢i ⎥ + ⎢ m sin δ V ⎥ ⎥ 0 ⎦ ⎣ Eq ⎦ ⎢ E E dc ⎥ 2 ⎣ ⎦ cos m δ V ⎡ B B dc ⎤ − xB ⎤ ⎡iBd ⎤ ⎢ ⎥ 2 ⎢i ⎥ + ⎢ m sin δ V ⎥ ⎥ 0 ⎦ ⎣ Bq ⎦ ⎢ B B dc ⎥ 2 ⎣ ⎦ ⎡VEtd ⎤ ⎡ 0 ⎢V ⎥ = ⎢ ⎣ Etq ⎦ ⎣ xE ⎡VBtd ⎤ ⎡ 0 ⎢V ⎥ = ⎢ ⎣ Btq ⎦ ⎣ xB ⎡iEd ⎤ sin δ E ]⎢ ⎥ + ⎣iEq ⎦ ⎡iBd ⎤ sin δ B ]⎢ ⎥ ⎣iBq ⎦ dVdc 3mE = [cos δ E dt 4Cdc 3mB [cosδ B 4Cdc (1) (2) ﻣ ﺘ ﻠ ﺐ ﺳ ﺎ ﯾ ﺖ m o c . e t i S b a l t a M The dynamic model of the power system presented in Fig. 1 is [23]: δ& = ω0ω (3) 2.Model of Power System Including UPFC In this section a power system consisting of a UPFC is described. Fig. 1 shows a singlemachine infinite-bus (SMIB) system with UPFC. It is assumed that the UPFC performance is based on pulse width modulation (PWM) converter. In Fig. 1 mE , mB and δ E , δ B are the amplitude modulation ratio and phase angle of reference voltage of each voltage source converter respectively. These values are input control signals of the UPFC. A linearised model of the power system is used in studying dynamic studies of power system. In order to consider the effect of UPFC in damping of low frequency oscillation (LFO), the dynamic model of the UPFC is employed, in the resistance and transient of the transformers of the UPFC can be ignored. The equations describing the dynamic performance of the UPFC can be written as [23]: Vt it Pe Qe VEt iB _ VBt ω& = E& q′ = VSC-E + xE _ Vdc mE δE − Eq + E fd ′ Tdo (5) (6) pe = Vtd itd + Vtq itq (7) Vt 2 = Vtd2 + Vtq2 (8) xBB m sin δ EVdc xBd xdE (Vb cos δ Eq′ − E + 2 xdΣ xdΣ xdΣ mB sin δ BVdc ) 2 m cos δ EVdc xBq xqE (Vb sin δ + iEq = E + 2 xqΣ xqΣ + mB cos δ BVdc ) 2 x m sin δ BVdc )+ iBd = − dt (Vb cos δ + B 2 xdΣ Vb xBV iE (4) k −1 E& fd = E fd + A (Vt 0 − Vt ) TA TA iEd = xB + xtE pm − pe − Dω M VSC-B mE sin δ EVdc xdE x + E Eq′ 2 xdΣ xdΣ iBq = − mB δB mE cos δ EVdc xqE 2 xqΣ mB cos δ BVdc ) 2 Fig. 1: A single machine connected to infinite bus with UPFC 3 MatlabSite.com ﻣﺘﻠﺐ ﺳﺎﯾﺖ − xqt xqΣ (Vb sin δ + (9) Simultaneous Coordinated Tuning of UPFC and Multi-Input PSS for Damping of Power System Oscillations 26th International Power System Conference ΔQe = 2 xq itq Δitq − ΔEq′ itd − Eq′ Δitd + 2 xd′ itd Δitd (17) By combining and linearising Equations (19), the state variable equations of the power system equipped with the UPFC can be represented as : Thus we can have: x& = Ax + Bu + k14 Δδ E + k15ΔmB + k16 Δδ B [ u = [Δu x = Δδ (10) ΔVdc ]T Δω ΔEq′ ΔE fd ΔmE pss ⎡ 0 ⎢ k ⎢ − 1 ⎢ M ⎢ k4 A=⎢ − M ⎢ ⎢ − k A k5 ⎢ TA ⎢ k ⎣ 7 ΔQe = k10 Δδ + k11ΔEq′ + k12 Δvdc + k13ΔmE Δδ E ωb D M − 2.1 UPFC Damping Controller ΔmB Δδ B ] 0 k − 2 M k − 3 ′ Tdo k k − A 6 TA k8 T 0 0 (18) The damping controller is designed to produce an electrical torque in phase with the speed deviation according to phase compensation method. The four control parameters of the UPFC ( mE , mB and δ E , δ B ) can be modulated in order to produce the 0 ⎤ k pd ⎥ − ⎥ M ⎥ kqd ⎥ − ′ ⎥ Tdo ⎥ k Ak pd ⎥ − TA ⎥ − k9 ⎥⎦ ﻣ ﺘ ﻠ ﺐ ﺳ ﺎ ﯾ ﺖ m o c . e t i S b a l t a M ⎡0 ⎢ ⎢0 ⎢ B=⎢ 0 ⎢ ⎢k ⎢ A ⎢ TA ⎣⎢ 0 − 0 0 0 0 k qe M k qe − ′ Tdo k A kve − TA kce − 0 k qδe M k qδe − ′ Tdo k A kvδe − TA kcδe 1 ′ Tdo 1 − TA 0 − 0 k pb M k qb − ′ Tdo k A kvb − TA kcb damping torque. the structure of UPFC based damping controller, as shown in Fig. 2, is similar to the PSS controllers. It consists of gain block with gain G, a signal washout block and two-stage phase compensation block with time constant T1, T2, T3 and T4. The time constant Td represents the finite delay caused by the firing controls and the natural response of the UPFC. 0 ⎤ k pδb ⎥ − M ⎥ k qδd ⎥ ⎥ − ′ ⎥ Tdo k k ⎥ − A vδb ⎥ TA ⎥ kcδb ⎦⎥ Δpe = k1Δδ + k 2 ΔEq′ + k qd ΔVdc + k qe ΔmE speed deviation (11) + k qδe Δδ E + k qb ΔmB + k qδb Δδ B ΔVt = k5 Δδ + k6 ΔEq′ + kvd ΔVdc + kve ΔmE ⎛ sTω G⎜⎜ ⎝ 1 + sTω Also in power system of Fig. 1 can be written: (14) Vtd = xqitq (15) Substituting (14) and (15) into (13) we obtain: Qe = ( xq itq )itq − ( Eq′ − xd′ itd )itd ⎞⎛ 1 + sT1 ⎟⎜ ⎟⎜ 1 + sT 2 ⎠⎝ ⎞⎛ 1 + sT3 ⎟⎟⎜⎜ ⎠⎝ 1 + sT4 ⎞ ⎟⎟ ⎠ + 3.Multi-Input Power System Stabilizer The dynamic stability of a system can be improved by providing suitably tuned power system stabilizers on selected generators to provide damping to critical oscillatory modes. Suitably tuned power system stabilizers (PSS), will introduce a component of electrical torque in phase with generator rotor speed deviations resulting in damping of low frequency power oscillations in which the generators are participating. The input to stabilizer signal may be one of the locally available signals such as changes in rotor speed, rotor frequency, accelerating power or any other suitable signal. This stabilizing signal is compensated for phase and gain to result in adequate component of electrical And ΔmE , ΔmB , Δδ E and Δδ B are the deviation of input control signals of the UPFC and explained previously. Reactive power of system expressed in d-q coordinates are obtained as: Qe = Vtd itq − Vtq itd (13) Vtq = Eq′ − xd′ itd ⎞⎛ 1 ⎟⎜ ⎟⎜ 1 + sT d ⎠⎝ U Fig. 2: structure of UPFC based damping controller (12) + kvδE Δδ E + kvb ΔmB + kvδb Δδ B Uref ks 1 + sTs + (16) Linearising the equation above we have: 4 MatlabSite.com ﻣﺘﻠﺐ ﺳﺎﯾﺖ Simultaneous Coordinated Tuning of UPFC and Multi-Input PSS for Damping of Power System Oscillations 26th International Power System Conference torque that results in damping of rotor oscillations and thereby enhance power transmission and generation capabilities. As a generator exciter control method for increasing power stability, ΔP − PSS is widely used. This method is applied to suppress the local power perturbation between generators. For the low frequency perturbation that occurs between power systems in wide-area operation, however there is little system perturbation information included in the active power, so ΔP − PSS has little effectiveness. As a solution to that problem, ΔP + Δω PSS, which uses the internal frequency or the rotational speed ( ω ) as well as the active power is effective for low frequencies, is used [24,25]. In multi input PSS, a circuit for improving transitional stability is added to achieve an excellent effect for both transitional stability and operating stability. In addition we were able to confirm that almost the same effect can included if voltage of the generator is used in place of the ω signal. The frequency signal can be detected directly by calculation from the voltage and current. Thus there is no need for equipment that has an electromagnetic sensor, and multi-input PSS can be implemented even in hydroelectric generators, where the installation of an exciter pick-up is difficult. The P+ω input PSS is shown in Fig. 3. P and ω are generator local signals which are selected as the PSS input ( Δu PSS in Fig. 3). If P input PSS and ω input PSS are optimized independently and are combined for use as P+ω input PSS, an unexpected unstable oscillation mode may occur. In this paper, the parameters of the P+ω input PSS with parameters of the UPFC controller are optimized all together. 4.Function Optimization Optimization is defined as finding the best possible solution to a problem given a set of constraints. Numerous applications of evolutionary algorithms can be found especially in electric power systems [26]. The flexibility of evolutionary algorithms to address optimization problem using any reasonable representation and objective functions gives an advantage over classical optimization procedures. A control structure with a number of adjustable gains and time constants, mathematical model of the system and objective functions is required, while the aim is to obtain the best values of controllers gains and time constants that optimize objective function subject to system constraints. Optimization problem is formulated as follow: ﻣ ﺘ ﻠ ﺐ ﺳ ﺎ ﯾ ﺖ m o c . e t i S b a l t a M ΔP G 1 + sTd sTω 1 + sTω 1 + sT1 1 + sT2 1 + sT3 1 + sT4 + Δω G 1 + sTd sTω 1 + sTω 1 + sT1 1 + sT2 Min f (Gm , Tn ) = af1 + bf 2 (19) Gm min ≤ Gm ≤ Gm max s.t Tn min ≤ Tn ≤ Tn max Where f1 = N ∑ ∑ (ξ0 − ξi, j )2 and j =1 ξ i ≤ξ 0 f2 = N ∑ ∑ (σ 0 − σ i, j )2 (20) j =1 σ i ≥σ 0 Where σ i, j , ξi, j are the real part and damping ratio of the ith eigenvalue of the jth operating point. σ 0 , ξ 0 are the desired minimum real part and damping ratio which is to be achieved. Gm , Tn are the optimization parameter and f (Gm , Tn ) is objective function where m,n are the total number of gains and time constants. The values of a and b are the weight factors for f1, f2 with regard to optimal point. In this article σ 0 , ξ 0 , a and b is chosen 2, 1, 5 and 10 sequentially. N is the total number of operating points for which the optimization is carried out. Evolutionary algorithm can be applied to any problem that can be formulated as function optimization (19). It requires data structure to represents solutions, performance index to evaluate the solutions, and variations operator to provide new solutions from the old ones. Advantage of the evolutionary algorithm comes from the ability in automating and Δu PSS 1 + sT3 1 + sT4 Fig. 3: Multi-input PSS 5 MatlabSite.com ﻣﺘﻠﺐ ﺳﺎﯾﺖ Simultaneous Coordinated Tuning of UPFC and Multi-Input PSS for Damping of Power System Oscillations 26th International Power System Conference problem solving routines. Genetic algorithm (GA) and PSO are both considered as evolutionary algorithm. Genetic algorithm is a search technique to find approximate solution to optimization technique. The algorithm uses techniques inspired by evolutionary biology such as mutation, cross over, natural selection. Despite obtaining good solutions in hard search spaces, still have some disadvantages such as tendency to converge toward local optima rather than global optimum of the problem, and hard to implement on dynamic data sets. PSO is another evolutionary technique that is not largely affected by nonlinearity and the size of the problem. The technique can easily converge to optimal solution that can be executed in search in solution space for solving multi-objective optimization problems as formulated in (19). Large number of evolutionary algorithms applications, especially for parameter estimation and tuning of control gains can be found in electric power system literature [27], [28]. Among all these techniques PSO has gained increased attention. Some advantages of PSO over other optimization techniques are: 4.1 Particle Swarm Optimization Algorithm Particle Swarm Optimization is an evolutionary algorithm developed by James Kennedy and Russell Eberhart [31]. The original objective of their research was to mathematically simulate behavior of bird flocks. The search algorithm is based on cooperation and competition among the population members. The objective is to find optimal regions of a complex search space through interaction of individuals in a population of particles. Each individual of the population has an adaptable velocity (position change), according to which it moves in the search space. Moreover, each individual has a memory remembering the best position of the search space it has ever visited. Its movement is an aggregated acceleration toward its best previously visited position. Another best value that is tracked by PSO is the best value obtained so far by any particle in the neighborhood of the particle. The main idea is to change the position and velocity of each particle toward global best (gbest) location at each time step. As a result, after number of iterations the particles among populations are found to have accumulated around one or more of the optima and tends to find the global optima among all. Given the size of the problem and the system complexities, the solution is assumed to lie in the range of an N-dimensional space, where each potential solution is called a particle. Particle has a position and a velocity and moves in the search space toward an optimal solution. Steps for PSO algorithm is given in following as shown in Fig. 4: 1. Initialize each particle with random solution in problem domain (initialization) 2. For each particle evaluate the objective function 3. For each particle, calculate the objective function and compare it with its best particle (Pbest). If the current value of the objective function is better than the Pbest then set the value as the Pbest and the current position of the particle. 4. Among all best particles, identify the particle that has the best objective function ﻣ ﺘ ﻠ ﺐ ﺳ ﺎ ﯾ ﺖ m o c . e t i S b a l t a M • It has the ability to escape local minima • It has less parameter to adjust, unlike many others • It is easy for computer implementation and coding • It is easy to implement and program with mathematical and logic operations • It does not require a good initial solution to start the iteration • It can be used with almost any realistic objective functions i.e. continuous or noncontinuous, convex or non-convex • It has more effective memory capability (local and neighboring best) A detailed survey on PSO applications to large scale power systems is covered by Alrashidi and El-Hawary [29]. Recently a comprehensive overview of PSO techniques and different applications in electric power systems are covered by del Valle et. al [30]. 6 MatlabSite.com ﻣﺘﻠﺐ ﺳﺎﯾﺖ Simultaneous Coordinated Tuning of UPFC and Multi-Input PSS for Damping of Power System Oscillations 26th International Power System Conference global searches and hence requiring less iteration for the algorithm to converge. 6. Repeat steps 2−5 until stopping criteria are met. These criteria are maximum iteration and minimum error criteria. value. The value of the objective function is assigned as gbest with its new position. start Select parameters of PSO: N, C1, C2, C, w 5.Controllability Measure SVD is employed to measure the controllability of the EM mode from each of the five inputs: u pss , m E , δ E , m B , and δ B . Generate the randomly positions and velocities of particles Initialize Pbest with a copy of the position for particle, determine gbest The minimum singular value, σ min is estimated over a wide range of operating conditions. For SVD analysis, Pe ranges from 0.05 to 1.4 pu and Qe = [-0.4, 0, 0.4]. At each loading condition, the system model is linearised, the EM mode is identified, and the SVD-based controllability measure is implemented. For comparison purposes, the minimum singular value for all inputs at Qe = -0.4, 0.0 and 0.4 pu is shown in Figs. 5–7, respectively. From these figures, the following can be noticed: Update velocities and positions according to (21), (22) Evaluate the fitness of each particle ﻣ ﺘ ﻠ ﺐ ﺳ ﺎ ﯾ ﺖ m o c . e t i S b a l t a M Update Pbest and gbest No Satisfystoping criterion Yes Optimal value of the controller parameters End Fig. 4: Flowchart of the PSO technique 5. For each particle update the velocity vector and then the position vector according to: ( ) vik +1 = ωvik + c1r1 Pidk − xidk + ( c2 r2 Pgdk − k xgd ) xidk +1 = xidk + cvidk + • (21) • (22) • The ith particle is represented by X i = ( xi1 , xi 2 ,K, xiD ) , value of the fitness for particle i (Pbest) is stored as Pi = ( pi1 , pi 2 ,K, piD ) and velocity of particle i is presented as Vi = (vi1, vi 2 ,K, viD ) . Where, Pid and Pgd are pbest and gbest . The positive constants c1 and c2 are the cognitive and social components that are the acceleration constants responsible for varying the particle velocity towards pbest and gbest , respectively. Variables r1(.) and r2(.) are two random functions based on uniform probability distribution functions in the range. The inertia weight ω is responsible for dynamically adjusting the velocity of the particles, so it is responsible for balancing between local and • EM mode controllability via δ E is always higher than that of any other input. The capabilities of δ E and m B to control the EM mode is higher than that of PSS. The EM mode is more controllable with PSS than with either m E or δ B . All control signals except m B and δ E at Qe = 0 suffer from low controllability to EM mode at low loading conditions. Fig. 4: Minimum singular value with all stabilizers at Qe = -0.4 7 MatlabSite.com ﻣﺘﻠﺐ ﺳﺎﯾﺖ Simultaneous Coordinated Tuning of UPFC and Multi-Input PSS for Damping of Power System Oscillations 26th International Power System Conference Pole-Zero Map 6 Imaginary Axis 4 0.998 0.996 0.993 0.986 0.965 0.86 0.999 2 1 100 0 1 80 60 40 20 -2 1 -4 0.999 0.998 -6 -120 -100 0.996 -80 0.993 -60 Real Axis 0.986 -40 0.965 0.86 -20 0 Fig. 7: Dominant eigenvalues of the power system in nominal loading condition with UPFC & MPSS controllers Fig. 5: Minimum singular value with all stabilizers at Qe = 0.0 ﻣ ﺘ ﻠ ﺐ ﺳ ﺎ ﯾ ﺖ m o c . e t i S b a l t a M Pole-Zero Map 10 0.996 0.99 0.98 0.96 0.91 0.7 0.998 Imaginary Axis 5 1 100 0 80 60 40 20 1 -5 0.998 0.996 -10 -120 0.99 -100 Fig. 6: Minimum singular value with all stabilizers at Qe = 0.4 -80 0.98 -60 Real Axis 0.96 -40 0.91 0.7 -20 0 Fig. 8: Dominant eigenvalues of the power system in heavy loading condition with UPFC & MPSS controllers 6. Simulation Results 6.1 Dominant Eigenvalues The dominant eigenvalues of the test system with UPFC & MPSS controllers are shown in Figures 7-9. The system data and detailed controllers parameters are given in the Appendix and Table 2 sequentially. Also The system eigenvalues without and with the proposed stabilizers with ξ 〈1 are given in Table 3 at the three operating points, nominal, light, heavy given in Table 1. This table clearly demonstrates the effectiveness of the MPSS coordination with UPFC in enhancing system stability. After the coordinated tuning of UPFC and MPSS controllers, electromechanical modes of oscillations are well damped. The results show the improvement in damping of overall power oscillations in the system as all the damping ratios are more than 50%. Pole-Zero Map 10 0.996 0.99 0.98 0.96 0.91 0.7 0.998 Imaginary Axis 5 1 100 0 80 60 40 20 1 -5 0.998 0.996 -10 -120 0.99 -100 -80 0.98 -60 Real Axis 0.96 -40 0.91 0.7 -20 0 Fig. 9: Dominant eigenvalues of the power system in light loading condition with UPFC & MPSS controllers Table II: the optimal parameter and settings of the proposed controllers controller parameters Table I: Loading conditions Loading Pe (pu) Qe (pu) Nominal 0.8 0.167 Heavy 1.2 0.4 Light 0.2 0.01 G T1 T2 T3 T4 8 MatlabSite.com ﻣﺘﻠﺐ ﺳﺎﯾﺖ coordinated design CPSS UPFC 100 1.5 1.0073 1.3639 1.5 7.1440 1.5 0.8183 1.5 1.0924 coordinated design MPSS ( ω input and P input sequential) 0.2690 0.1505 0.0646 1.5 0.05 1.5 1.5 1.5 0.05 1.5 UPFC -17.5212 0.05 1.0568 1.5 0.9054 Simultaneous Coordinated Tuning of UPFC and Multi-Input PSS for Damping of Power System Oscillations 26th International Power System Conference Table III: eigenvalues and damping ratios of power system before and after the coordinated tuning with ξ 〈1 without PSS,MPSS and UPFC CPSS & UPFC nominal eigenvalue damping ratio 0.0773±i6.5648 -0.0118 -.1795±i0.6643 0.2609 -2±i2.65 0.6019 -1.87±i2.13 0.6596 -1.77±i1.37 0.7922 -1.264±i5.25 -6.6±i1.55 -0.95±i0.11 MPSS & UPFC 0.9234 0.9736 0.9936 heavy eigenvalue damping ratio 0.0775±i6.3711 -0.0122 -.3113±i0.8209 0.3546 -2.74±i4.06 0.5593 -1.5±i0.84 0.8715 -1.18±i0.53 0.9115 -1.07±i0.36 0.9477 -9.45±i6.54 0.8221 -3.15±i1.70 0.8804 -11.93±i3.41 0.9614 -0.95±i0.11 0.9936 light eigenvalue 0.0713±i6.5243 damping ratio -0.0109 -1.99±i5.73 -1.59±i1.1 0.3277 0.8223 -5.35±i5.62 -4.63±i3.05 0.79±i0.49 0.6896 0.8355 0.8512 ﻣ ﺘ ﻠ ﺐ ﺳ ﺎ ﯾ ﺖ m o c . e t i S b a l t a M Speed deviation Speed deviation -3 0.02 20 Speed deviation 0.03 (b) (a) CPSS & UPFC x 10 15 0.01 (c) CPSS & UPFC 10 MPSS & UPFC MPSS & UPFC 5 0 2 4 6 -5 10 0 8 MPSS & UPFC 0.01 0 0 -0.01 0 CPSS & UPFC 0.02 2 Time (sec) 4 6 -0.01 10 0 8 2 4 Time (sec) 6 8 10 Time (sec) Fig. 10: Dynamic responses for speed deviatin at (a) nominal (b) heavy (c) light loading condition; Solid (MPSS & UPFC), Dashed (CPSS & UPFC) Power deviation 0.2 0.4 CPSS & UPFC 0.2 CPSS & UPFC (a) 0.2 MPSS & UPFC 0.1 0 -0.1 0 Power deviation Power deviation 0.3 2 4 6 8 10 CPSS & UPFC (b) 0.1 MPSS & UPFC 0 0 -0.2 -0.1 -0.4 0 2 Time (sec) 4 6 8 10 -0.2 0 (c) MPSS & UPFC 2 4 6 8 10 Time (sec) Time (sec) Fig. 11: Dynamic responses for power deviation at (a) nominal (b) heavy (c) light loading condition; Solid (MPSS & UPFC), Dashed (CPSS & UPFC) 6.3 Non-Linear Simulation Results Conclusion The power system stability enhancement via multi-input PSS and FACTS-based stabilizers when applied simultaneous coordinated is discussed and investigated for a SMIB system. Also a comparative performance study of a single input CPSS and a multiinput PSS coordination with UPFC is carried out to appreciate the effectiveness of MPSS in contrast to CPSS. The multi-input uses two state-space variables, rotor speed deviation and active power deviation. For the proposed controllers design problem, an objective function to minimize the power system In order to illustrate the performance of the coordinated tuning result, simulation studies are carried out as shown in Fig. 12 and a three-phase short circuit of 100 ms duration is simulated at infinite bus in the test system. While the fault occurs at the infinite bus, the original system is restored upon the clearance of the fault. Figures 10, 11 show the speed deviation and power deviation for three loading conditions. It can be readily seen that the coordinated designing of the MPSS and UPFC are more effective than the coordinated designing of the CPSS and UPFC in terms of reduction of overshoot and setting time. 9 MatlabSite.com ﻣﺘﻠﺐ ﺳﺎﯾﺖ Simultaneous Coordinated Tuning of UPFC and Multi-Input PSS for Damping of Power System Oscillations 26th International Power System Conference oscillation is used. Then, particle swarm optimization is employed to optimally and coordinately tune the controller parameters. Simulation results are presented for various loading conditions and disturbances to show the effectiveness of the proposed coordinated design approach. The proposed controllers are found to be robust to fault in operating conditions and generate appropriate stabilizing output control signals to improve stability. ω ω ωdt δ 0∫ itq xq itq Eq′ itd Vtd Pm Vtq Eq′ − xd′ itd Vtq itq Vtd itd Vtq itq + Vtd itd + Pe - ω ∫ + − D M ﻣ ﺘ ﻠ ﺐ ﺳ ﺎ ﯾ ﺖ m o c . e t i S b a l t a M Eq′ Vb Vdc mE δE Eqn. 9 mB iEd iBd iEq iBq iEd + iBd iEq + iBq itd Eq′ itd itq Vtq Vtd δB iEd iEq iBd iBq mE δE mB δB Vtd2 E fd Eq′ + (xd − xd′ )itd + Vtq2 Vt 0 Vt Eq ∫ kA (Vt 0 − Vt ) TA − Eq + E fd ′ Tdo ∫ + − 3mE [cos δ E 4Cdc + 3mB [cosδ B 4Cdc ⎡iEd ⎤ sin δ E ]⎢ ⎥ ⎣iEq ⎦ ⎡iBd ⎤ sin δ B ]⎢ ⎥ ⎣iBq ⎦ ∫ dt Eq′ E fd 1 TA Vdc Fig. 12: nonlinear simulation of test system Appendix SMIB system data: ′ : 8.0 sec ; D = 0; Machine: H = 6.5; Tdo xd′ = 0.3 ; xq = 0.6 ; xd = 1.8 ; freq = 60; v = References 1.05; Exciter: KA = 50; TA = 0.05; Efd-max = 7.3; Efdmin = -7.3; PSS: uPSS-max = 0.2; uPSS-min = -0.2; Tw = 5; Td = 0.01; Ti-min = 0.05; Ti-max = 1.5; Kmin = -100; Kmax = 100; i = 1,2,3,4; Transmission Line: xtE = 0.1; xBV = 0.6; UPFC: xE = 0.1; xB = 0.1; Ks = 1; Ts = 0.05; CDC = 3; Vdc = 2; mE-min = 0; mE-max = 2; mBmin = 0; mB-min = 0; Tw = 5; Td = 0.01; Ti-min = 0.05; Ti-max = 1.5; Kmin = -100; Kmax = 100; i = 1,2,3,4; [3] Chen. 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