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The 10th Power Systems Protection & Control Conference PSPC, January 19, 20th 2016, Tehran, Iran School of Electrical & Computer Engineering, University of Tehran A Novel Out-of-Step Protection Algorithm Based on Wide Area Measurement System Bahman Alinezhad Hossein Kazemi Karegar Faculty of Electrical and Computer Engineering Shahid Beheshti University Tehran, Iran [email protected] Faculty of Electrical and Computer Engineering Shahid Beheshti University Tehran, Iran [email protected] Abstract— This paper proposes a novel Out-of-Step protection technique based on synchronized phasor measurements and concept of Equal Area Criterion (EAC). In any disturbance, in the control center, generators are clustered into safe and risk groups based on the concept of Boundary of Angle Oscillations. At the same time, a local stability index also is sent to the control center from each generator. The latter is obtained by local phasor measurements based on EAC concept. Generator is known as unstable if it belongs to the risk cluster at the control center and its stability index is lower than one. For each generator, the acceleration area during fault condition is calculated directly using the generator output power and rotor angle measured in real-time. As soon as the fault is cleared, the deceleration area is predicted with the help of post-fault curve estimated by the least square method. The proposed technique is verified on the New-England 39-Bus test network. Keywords- Out-of-step, equal area criterion, boundary of angle oscillations, least square method, phasor measurement unit (PMU) S I. INTRODUCTION YNCHRONOUS generators are subjected to various disturbances such as faults and load variations. When the balance between mechanical input and electrical output powers of a generator is disrupted, the generator may lose its synchronism with the power system and becomes unstable. This condition is known as Out-of-Step (OOS) [1-2]. The OOS of a generator not only is a threat for its mechanical components, but also may affect the stability of the other generators in the network. Thus, early disconnection of an unstable generator can prevent other generators from instability and helps to save the rest of the system from total instability [3]. Industrial impedance-based OOS relays determine the generator instability by analysing the impedance trajectory crossing a predefined characteristic. The main disadvantage of this technique is its relatively long operation time when the generator practically loses synchronism with the power system. In addition, numerous contingency simulations as well as experimental experiences are required to obtain a reliable setting which is an expensive and tedious work in a large power system. Moreover, the settings should be modified by change of the power system parameters. The recent advent of Phasor Measurement Units (PMUs) has made it possible to renew the system states in some milliseconds and develop more efficient OOS detection schemes. So far, several research studies have been done in this subject. A relationship between the rotor angle stability and maximal Lyapunov exponent is developed in [4] to determine the rotor angle instability. In [5], a real-time dynamic stability state estimator based on Lyapunov direct energy function is proposed. This method uses synchronized measurements as input and predicts the OOS condition. An energy function based classification for distinguishing between stable and unstable states by using synchronized measurements is presented in [6-7]. A wide area based system using artificial neural network is introduced in [8] by which an intelligent technique is proposed to predict and mitigate the OOS in a large power system. In [9], comparing the postdisturbance voltage trajectories with pre-defined voltage templates is used to predict the OOS. This algorithm needs extensive simulations, which should be performed again for any change in the power system configuration. Some research studies focus on the Equal Area Criterion (EAC) to propose a new method. The conventional EAC can be applied only on the single machine infinite bus (SMIB) system. The generator stability analysis is performed in offline mode. The rotor angle is calculated mathematically based on the system equivalent inertia. In [10], authors present an adaptive OOS relay based on EAC and synchronized measurements. An algorithm for mapping the EAC from rotor angle domain to time domain is proposed in [11-13]. The OOS is estimated based on the energies obtained from the bounded area between power curve and time axis under the power-time curve. This method is simple, but it needs the Unstable Equilibrium Point (UEP) of each generator. Calculating the UEP in a large power system is very difficult. In [14], an nthorder autoregressive model is used to predict the post-fault power-angle curve. Authors suggest some techniques to find the appropriate order of autoregressive model. In [15], an approach based on the EAC and real power swing criterion The 10th Power Systems Protection & Control Conference PSPC, January 19, 20th 2016, Tehran, Iran School of Electrical & Computer Engineering, University of Tehran is proposed to detect the unstable state. It shows that the EAC method can be used even for the OOS protection of small generators. In [16], a method based on EAC and using frequency deviations of voltage and discrete Fourier transform is proposed for estimating the generator rotor angle. However, the above algorithms are not verified on a multimachine network. In multimachine networks due to interactions between generators, the conventional EAC cannot be used directly. The major problem of this technique is determining the post-fault curve. In [17], EAC and critical clearing time estimation is used for calculation of transient stability margin index for predefined areas of the power network. A fast online coherency identification technique is developed in [18-19] to identify the coherent generators. In [20], an extended EAC and real-time swing curves are used to detect the OOS condition. This method reduces the power system to one machine infinite bus system and analyses the stability of the reduced system based on the EAC concept. In [21], a special protection scheme is developed based on the one machine infinite bus and EAC to prevent the power system from blackout during the power swing. The post-fault curves are estimated using the least square method. In this paper, an online predictive OOS detection technique is developed based on the EAC concept. The main idea is clustering the generators in safe and risk groups. A new algorithm is proposed for estimating the post-fault curve parameters based on local measurements. Results show that the proposed technique is able to predict the OOS of each generator just in a few cycles after the disturbance, which is considerably earlier than the time at which the generator rotor angle meets the UEP. In addition, the proposed technique is independent of changes in power system configurations, no special setting is required and no extra measurements are required except local ones. The rest of the paper is organized as follows. In sections 2 and 3 the concepts of impedance-based OOS relays and the proposed method are discussed. Simulations are presented and discussed in sections 4. I. IMPEDANCE-BASED OOS RELAYS Step 1) Suppose all generators are equipped with a PMU to measure the generator voltage and current phasors as well as their active and reactive powers. The generator Rate of Change of Frequency (ROCOF) also is available from PMU output. Generator rotor angle can be easily calculated from its internal voltage, as: (1) Fig. 1 Impedance-based OOS relay and are generator per-phase terminal voltage where, and current. is the generator sub-transient reactance. This value can be either calculated locally or in the control center. Step 2) As seen in Fig. 2, the PMUs send the measured phasors to the control center, where the equivalent twomachine model of the network is established as shown in Fig. 3. In this model, the total network generators are replaced with an equivalent generator , which is connected to a dummy infinite bus via an equivalent impedance which simulates the transmission system effect. and , are The area active and reactive powers and where calculated from and are is the number of generators in the system. The calculated and transmitted to the control center by PMUs. However, the difference between and infinite bus voltage is is more important, but the value of phase difference important. Without losing the generality, we can assume that the equal to 1P.U. the problem is calculating the and . Fig. 1 shows a typical characteristic of an impedance-based OOS relay [22]. Generator is disconnected when the impedance trajectory passes the borders of characteristic 1 or characteristic 2 at the left side. For preventing the mechanical damages, the generator is disconnected as soon as the impedance trajectory crosses the left border of characteristic 1. For remote faults, where impedance trajectory passes of characteristic 2, generally more than one crossing is allowed before disconnecting. In this case, more time is given to the generator in order to return to the stable condition [23-24]. The values of , , , and determine the relay borders and may change when the network configuration is changed. This method often require numerous and time-consuming simulations to find a reliable settings [25]. II. THE PROPOSED APPROACH The algorithm procedure is summarized as below: Fig. 2 The communication between PMUs and control center The 10th Power Systems Protection & Control Conference PSPC, January 19, 20th 2016, Tehran, Iran School of Electrical & Computer Engineering, University of Tehran ?=@ A 9 C: 9: B (10) In (10), 1D is the equivalent rotor angle immediately before the disturbance. The value of ?=@ defines the “Safe” and “Risk” boundary for the generators rotor angles. For each generator in the network, if its rotor angle is greater than ?=@ during the disturbance, it categorized in the “Risk” cluster, otherwise it belongs to the “Safe” cluster. Step 3) The swing equation of a single generator E is defined as: ,3 97 7 9: Fig. 3 Two-machine equivalent model For this, the power-angle equations are considered as: !"# % which is simplified to ( (2) &'( (3) )$ * + : ) ) (4) &'( (5) C FG (11) In (11), 3 is the E :H generator inertia constant in seconds, 7 is the frequency of EIJ generator at its terminal, 7 is the system nominal frequency, 0 and are mechanical input and output power respectively. The system equivalent inertia constant 3454 is defined from: ) K L% , 4 M 3454 !"# FG 0 M 3 M (12) Where, M is the generator apparent power and K is its inertia. Substituting the 3 from (11) in (12) will be resulted in: FG and The value of M N are obtained from (4) and (5) as: , % !"#- . (6) % / % % (7) % 1*2* 3454 9 678 9: % (8) is the total mechanical input power equal to the where 0 electrical output powers before the disturbance. 78 is the nominal frequency and the value of 3454 is the equal inertia time constant of the whole network which should be calculated. All P.U parameters should be calculated the same reference, e.g. );;;< =. If (8) is available, then, 9 9: 678 > 3454 (13) P , In case of disturbance, the value of is changed abnormally based on the system equal inertia time constant and power unbalanced. In this situation, the dynamic behavior of the whole system should be considered. For this, first consider the well-known swing equation as: 0 3454 7C O 97 , 9: M 0 9: (9) The value of Boundary of Angle Oscillation ?=@ in each sample can be updated as: In (13), the value of Q is the Rate of Change of Frequency I (ROCOF) value which is available at PMU output. Therefore, the 3454 can be evaluated from: 3454 ) 7 , C U S@T@B M R (14) The value of 3(V( from (14) which is participated in (9) should be calculated immediately after disturbance before generator control systems such as exciters or governors will be operated. During this condition, the value of 0 will be equal to its previous values before disturbance. The disturbance can be either load switching or fault depending on the system type. Step 4) A local stability index (SI) Based on the EAC concept is calculated for each generator in the network. As shown in Fig. 4, three operation conditions may be possible, which are pre-fault B , fault B and post-fault M . In B and the rotor angle is 8 . During the fault, condition, 0 the acceleration area = is obtained and the rotor angle is increased up to WX . When the fault is cleared, the M operation is started and deceleration area =%% is appeared. In real, if =%% Y = Z =% , then the generator is stable, otherwise it is unstable. The UEP is the intersection of 0 and M curve. For calculating these areas and assessing the generator stability, both the generator rotor angle and curves for B and M are required. The 10th Power Systems Protection & Control Conference PSPC, January 19, 20th 2016, Tehran, Iran School of Electrical & Computer Engineering, University of Tehran h 1\ i 1\ 0 ] 8 !"# i &'(^ fg! i (E ^ In a matrix form, ) !"# fg! 8 h h k p q 01\] &'(^ r jh 1\ ) mm !"# fg! lm mmmnm mm mmmo ^ i i lm mmnm mo 0 ] (Em 1\ q h r 1\ i lno s (19) W The unknown matrix, ? can be obtained from pseudo inverse transformation, Fig. 4 Equal Area Criterion (EAC) ? = = - = T (20) The number of measurement samples, d has a great effect on the estimation procedure. The more sample result in better estimation but increase the instability detection time. A tradeoff is required for choosing the best sample numbers. In this paper, a value of four samples is suggested which based on the PMU reporting rate of ,;t(, the local instability detection time is approximately equal to 80ms. Fig. 5 Impedance trajectory in case of fault and post-fault As seen in Fig. 5, which shows the positive sequence trajectory from a generator terminal, the system swing during the fault is negligible. Therefore, the fault curve in Fig.4 can be evaluated by a sine shape and = can be calculated from: ) [ , , = Z 0 C (15) Signal (SI<1) is received from a generator Generator is in the Risk Cluster Fig. 6 Instability criterion in the control center 1\ 0 ] !"# 8 ^ (16) The simulation studies are carried out on the New England 39-Bus test network shown in Fig. 7 [8]. The power system frequency is 50Hz and nominal voltage of transmission system is 345kV. All simulations are performed in time domain with a step size of 100Hs based on the initial conditions obtained from power flow results. The instantaneous values of terminal voltage and phase current of all generators are sampled and saved with the frequency of 2kHz during the simulation. In (16), 8 is the DC offset of the curve, 01\ ] is its maximum value and ^ is the phase. If (16) is available, then the =% Z =%% area can be calculated continuously from: 2_1 > =% 8 `ab =% 1\ 0 ] =%% !"# ^ 0 9 (17) =% c= . The target is to estimate the values of 8 , 01\ ] , and ^ as depicted in Fig. 4. To this, a solution based on least square method is proposed in this paper. Suppose, there is d measurement pairs of 1\ e are available as: Finally, the M value is equal to, M 1\ 1\ % Send trip to the generator III. SIMULATION AND RESULTS In (15), 0 is assumed to be constant and equal to before the disturbance, E ) and E are referred to 8 and X positions, respectively. The M curve is influenced from inter-machine oscillations in the network and cannot be estimated directly. For estimation the M curve, this paper suggests the following equation as: 1\ Step 5) In control center, the generator is unstable and will be tripped if the following criterion will be satisfied, 8 1\ 0 ] !"# &'(^ fg! (E ^ 8 1\ 0 ] !"# % &'(^ fg! % (E ^ (18) Fig. 7 New-England 39-Bus test network The 10th Power Systems Protection & Control Conference PSPC, January 19, 20th 2016, Tehran, Iran School of Electrical & Computer Engineering, University of Tehran A software PMU based on IEEE C.37.118 standard is coded in MATLAB to calculate the phasor values [26]. The PMU reporting rate is equal to one frame per cycle. Although in a real network, fault can occur on any of the transmission lines, here, the first three lines of higher loading listed in Table I are selected for the purpose of stability studies. Two alternatives are available for choosing the duration of a short circuit fault. The first alternative is load switching which is a minor disturbance in the system. The next alternative is three-phase faults in which the faulted line is disconnected after 400~800ms. Table I. Lines with heavy loading in NE-39 test system Case No. From Bus To Bus Length of Line (km) 1 2 3 B5 B6 B21 B6 B7 B22 6 10 17 Line Fault Loading (%) Location (%) 84 123 104 50 50 50 A. Load disturbance The load connected to the B3, is switched on at 0.5s. Simulations show that all of the generators remain stable after the disturbance. Fig. 8Error! Reference source not found. depicts the ?=@ and generator rotor angles in this case. In Fig. 9 also the values of M is depicted for this case. As all generators are belong to the stable cluster (their rotor angle is lower than the ?=@) and all M values are greater than one, then all generators are stable. 0 G2 G3 G4 G5 G6 G7 G8 G9 G10 Fig. 9 The value of SI in case of load disturbance B. System Faults In this case, some three-phase faults are simulated in transmission lines listed in Table I. The results of the simulation studies for this case are presented here for the following scenarios: Scenario 1: Case 1 of Table I, fault duration = 390ms Scenario 2: Case 2 of Table I, fault duration = 480ms Scenario 3: Case 3 of Table I, fault duration = 320ms 0.45 0.91 0.45 2 2.33 4 3.67 5.25 7.23 5.34 6 0.86 50 8 Stability Index (SI) 100 91 98 113 139 137 123 115 101 Stability Index (SI) 150 112 Fig. 8 The value of BAO and generators rotor angles in case of load disturbance 0 G2 G3 G4 G5 G6 G7 G8 G9 G10 Fig. 10 The value of SI obtained using proposed algorithm for scenario 1 Scenario 1: In this case, according to Fig. 10, the local OOS detection says that generators G5, G7, G8, and G9 are unstable, because their SI values are lower than one. In this scenario, the ?=@ and generators rotor angles are shown in Fig. 11. As seen, the rotor angle of G4, G5, G6, G7, and G9 are greater than the ?=@ and are clustered in “Risk” group. From Fig. 6, two conditions are required to assess a generator as unstable. Therefore, G5, G7, and G9 are unstable and others are stable. A trip command is sending to theses generators to The 10th Power Systems Protection & Control Conference PSPC, January 19, 20th 2016, Tehran, Iran School of Electrical & Computer Engineering, University of Tehran disconnect them from the power system. Fig. 11 The value of BAO and generators rotor angles in case of fault (Scenario 1) is cleared. The algorithm performance was tested on the NewEngland 39-Bus test network. The major advantage of the proposed technique is fast detection of unstable generators before their rotor angle meet the UEP. For a complete verification, a field test procedure on industrial generators is required. V. REFERENCES 7.77 [1] 3.91 5.28 8.04 2 1.45 4 1.41 6 3.15 8 0.24 Stability Index (SI) 10 8.85 Scenario 2: Fig. 12 shows the values of M for this scenario. Since M is greater than one for all generators except % and it belongs to the Risk cluster, the proposed technique predicts that only % will become unstable and therefore it is disconnected from the network. This guarantees the stability of remaining generators in the system. [2] 0 G2 G3 G4 G5 G6 G7 G8 G9 G10 Fig. 12 The value of SI obtained using proposed algorithm for scenario 2 [3] [4] [5] [6] [7] 1.34 2.89 6.90 5.88 9.11 5.71 0.11 5 1.50 Stability Index (SI) 10 7.51 Scenario 3: Fig. 13 shows the values of M for this scenario. As can be seen, the proposed algorithm predicts the instability of u because it its SI is lower than one and it is a member of “Risk” group. 0 [8] G2 G3 G4 G5 G6 G7 G8 G9 G10 Fig. 13 The value of SI obtained using proposed algorithm for scenario 3 IV. CONCLUSION This paper proposes a novel technique for prediction of OOS of generators in control center. It is based on EAC and network boundary of angle oscillations immediately after fault [9] Tziouvaras D. 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