1832 IEEE TRANSACTIONS ON POWER DELIVERY, VOL. 24, NO. 4, OCTOBER 2009 Adaptive Current Differential Protection Schemes for Transmission-Line Protection Sanjay Dambhare, S. A. Soman, Member, IEEE, and M. C. Chandorkar, Member, IEEE Abstract—Throughout the history of power system protection, researchers have strived to increase sensitivity and speed of apparatus protection systems without compromising security. With the significant technological advances in wide-area measurement systems, for transmission system protection, current differential protection scheme outscores alternatives like overcurrent and distance protection schemes. Therefore, in this paper, we address this challenge by proposing a methodology for adaptive control of the restraining region in a current differential plane. First an error analysis of conventional phasor approach for current differential protection is provided using the concept of dynamic phasor. Subsequently, we extend the methodology for protection of series compensated transmission lines. Finally, we also evaluate the speed versus accuracy conflict using phasorlets. Electromagnetic Transient Program simulations are used to substantiate the claims. The results demonstrate the utility of the proposed approach. Index Terms—Adaptive protection, current differential protection, dynamic phasor, global positioning system (GPS), mutually coupled lines, phasorlets, series-compensated lines, tapped lines. I. INTRODUCTION I T is a well recognized fact that differential protection schemes provide sensitive protection with crisp demarcation of the protection zones. In principle, the differential protection is also immune to tripping on power swings. Such schemes when used for transmission systems using pilot wires are called pilot relaying schemes [1]. In 1983, Sun and Ray [2] published a seminal paper describing current differential relay system using fiber optics communication. An effective transmission rate of 55 samples per cycle at 60-Hz frequency was achieved in [2]. Since, differential comparison of the local and remote end currents must correspond to the same time instant, a delay equalizer is used with the local sequence current component signal to compensate the delay in receiving the remote end currents. The inaccuracies in such a current differential protection scheme arise, primarily, due to the following reasons: • effect of the distributed shunt capacitance current of the line is neglected; • modelling inaccuracies with series-compensated transmission line; Manuscript received May 30, 2008; revised December 13, 2008. Current version published September 23, 2009. This work was supported by PowerAnser Labs, IIT Bombay. Paper no. TPWRD-00395-2008. The authors are with the Department of Electrical Engineering, Indian Institute of Technology Bombay, Mumbai 400076, India (e-mail: dambhare@ee. iitb.ac.in; [email protected]; [email protected]). Color versions of one or more of the figures in this paper are available online at http://ieeexplore.ieee.org. Digital Object Identifier 10.1109/TPWRD.2009.2028801 • approximate delay equalization between local and remote end current;1 • current transformer (CT) inaccuracies, in particular errors due to saturation of the core in the presence of decaying dc offset current [3]. Conventional current differential schemes employing GPSsynchronized current measurements are discussed in [4]–[6]. If ultra high transmission system voltages are used (e.g., 765 kV and above), then line charging current component is significant. It causes a large variation in phase angle of the line current from one end to another. In traditional pilot wire schemes, relaying sensitivity will have to be compromised to prevent the mal-operation. Reference [7] proposes a current differential relay which uses distributed line model to consider line charging current. An adaptive GPS-synchronized protection scheme using Clarke transformation is proposed in [8]. The multiagent-based wide area current differential protection system is proposed in [9]. References [10], [11] propose the use of phasorlets for fast computation of phasors in distance and differential relaying. Analytical treatment of phasorlets is presented in [12]. If a transmission line has a series capacitor, then dependability of the conventional current differential relay may be compromised due to current inversion. Current inversion depends on degree of compensation, fault parameters and metal oxide varistor (MOV) conduction. MOVs have nonlinear V-I characteristics and they are connected in parallel with series capacitors to protect them from overvoltage. The performance of transmission system protection scheme in presence of series capacitor is discussed in [13]. In the case of distance relaying, effect of series compensation is even more serious due to presence of current or voltage inversion [14]–[16]. Even segregated phase comparison scheme may fail to operate on current inversion [17]. The paper on digital communication for relay protection [18] authored by working group H9 of IEEE Power System Relaying committee is an excellent reference to understand the implications and consequences of digital communication technologies on relaying. Modern high speed communication networks, typically use Synchronized Optical Network (SONET) or Synchronized Digital Hierarchies (SDH) standard for communication with transmission rates of the order of 274.2 Mbps or 155.5 Mb/s, respectively. They permit “network protection,” that is, during failure of a communication link, communication services are restored by reconfiguring flow of information in alternate paths. A typical example is self healing ring architecture used with SONET [19]. In such networks, synchronization by delay equalizers become difficult due to channel asymmetry. Due to channel asymmetry, communication delays for 1For example, at 50 Hz an uncompensated delay of 1 ms in communication will translate into an error of approximately 13 degrees in the phase computation. 0885-8977/$26.00 © 2009 IEEE DAMBHARE et al.: ADAPTIVE CURRENT DIFFERENTIAL PROTECTION SCHEMES transmit and receive paths are not identical. This may lead to differential currents arising out of inaccurate delay equalization, especially if, identical time for transmit and receive paths are considered. However, if current samples are time stamped by a global positioning system (GPS), then for calculation of differential current, samples corresponding to the same time instant can be compared, thereby providing immunity to channel delays, asymmetry, etc. [5], [20]. Differential current may be calculated either using instantaneous sample values, or by extracting phasors. Further, dynamic estimate of the channel delay can be easily maintained by subtracting the GPS time stamp at the transmit end from the receiving end time stamp. This permits back up operation even during GPS failure modes. The primary objective of this paper is to propose a methodology to improve sensitivity and speed of the current differential protection scheme for transmission-line protection without compromising its security. To meet this objective, we first develop a dynamic phasor model of transmission line. The model help us to analyze errors associated with steady-state phasor and are demodel of transmission line. Two parameters fine to quantify errors arising out of neglecting dynamic phasors. Subsequently, we propose an adaptive procedure to set the restrain region in the current differential plane. We show that the proposed methodology significantly improves sensitivity and speed of the current differential protection scheme without sacrificing the security. This paper is organized as follows: a current differential protection framework is introduced in Section II. In Section III, a dynamic phasor model of transmission line is developed. It is used for understanding modelling errors in current differential protection scheme. Consequently, in Section IV, the idea of adaptive restrain region is developed. Section V explains the implementation in phase co-ordinates. Section VII extends it to series-compensated and multiterminal lines. In Section VIII, we present simulation case studies in EMTP-ATP package on a 4-generator, 10-bus system with the capacitance coupled voltage transformer (CCVT) model. Section IX concludes the paper. 1833 Fig. 1. GPS-synchronized current differential protection scheme with equivalent -model of line. Hence, can be used as discriminant function to detect a fault on transmission line. This approach has been suggested by Phadke and Thorp [21, p. 257]. With a conventional relay-setting approach, operating current and restraining current for the current differential scheme can be expressed as follows: (3) and (4) The percentage differential relay pick up and operate when (5) (6) where is a pick-up current and is the restraint coefficient . However, it has been shown in [22] that numerical differential relay can be set more accurately in a current differential plane. Using the phase and magnitude information of series branch current, we calculate ratio (7) (8) II. FUNDAMENTALS Let us consider the positive sequence representation of an uncompensated transmission line. As shown in Fig. 1, the line can be represented by an equivalent -model. Equivalent circuit models the effect of distributed line parameters at the line terminals at the fundamental frequency. Let the positive sequence component of line current for refer. Then, current ence phase measured at bus be given by , in the series branch of the -equivalent line model at node can be computed as follows: (1) is the current in shunt path at bus and where is the positive sequence voltage of reference phase . Simican also be computed. larly, current in series branch at bus If there is no internal fault on the line, then (2) In absence of an internal fault, we have and As shown in Fig. 2, this can be visualized in the current differat (180 , 1). Ideally, every point other ential plane by point than indicates an internal fault. However, even in the absence of an internal fault, in real life the operating point may deviate from the point (180 , 1) due to following reasons: 1) synchronization error; 2) delay equalizer error; 3) modelling restrictions (i.e., assumptions, approximations, or inaccuracies of the algorithm); 4) ratio and phase angle errors of CT. These errors may become significant when a CT core saturates because of large currents during an external fault. Since GPS provides time synchronization of the order of 1 sec, the synchronization error can be practically eliminated. Also, if the same time stamped samples of two end are processed, delay equalizer error can be eliminated. Further, explicit 1834 IEEE TRANSACTIONS ON POWER DELIVERY, VOL. 24, NO. 4, OCTOBER 2009 where Re denotes the real part, , and represent a dynamic phasor at the th harmonic frequency. Then, dynamic phasor at fundamental frequency can be evaluated as follows: (14) Equation (14) indicates that well known phasor computation algorithms like full-cycle recursive DFT, half-cycle recursive DFT etc., actually compute a dynamic phasor. However, information of rate of change of phasor is not utilized. Rate of change of a dynamic phasor is given by the following equation: Fig. 2. Trip and the restrain region in current differential plane. modelling of the shunt capacitance of the line reduces the modelling errors. Therefore, we can reduce the width of the restrain for phase region in the current differential plane. We use error2 and % for magnitude error in current differential plane. Hence, and (refer Fig. 2). The corresponding value of in conventional relay setting approach is nearly 0.43. (15) Prior to a fault or a disturbance, . Subsequent to a disturbance, voltage and current signals are not periodic. Hence, a dynamic phasor should be preferred for modelling. Using (15), an appropriate phasor representation of (9) and (10) is given by III. ERROR ANALYSIS USING DYNAMIC PHASORS In principle, one can question the validity of phasor computation in relaying algorithms, irrespective of whether it is distance protection or differential protection, because if the relaying decision has to be arrived within one cycle of the fault inception, then, the actual voltage and current signals can differ appreciably from a sinusoid. This motivates us to develop a dynamic phasor model of transmission line. Fundamental equations used to describe propagation of a disturbance on a lossless single-phase transmission line are [21] (16) (17) where (9) (10) where and are the inductance and capacitance of the line per unit length and is distance measured from relay location. If and are assumed periodic, then, (9) and (10) can be transformed to the well-known phasor model of line (11) (12) where and denote fundamental voltage and current phasors respectively. The -equivalent circuit is an “exact” two-port equivalent of (11) and (12). In that sense, methods based upon -equivalent model are equivalent to method proposed in [7] which uses an explicit long line model. The extension of phasors for the dynamic situation is discussed in [23]. In this approach, signal can be represented as follows: (13) 2Reference [22] has suggested 640 margin for phase angle error. By comparing (16) and (17) with (11) and (12), we can conclude that inaccuracies in differential protection based upon phasor model arises due to neglecting the dynamic phasor contribution terms and in (16) and (17). Parameters and define gain associated with dynamic phasor model. Further, and do not directly depend upon the parameters of the line. Under the steady-state condition, and are unity. Hence, and measures the inaccuracies associated with the steady-state modelling of the system. Prior to a fault, the terms and are unity. After the fault, and will deviate from unity. As the transients die down, and returns back to unity. Figs. 3 and 4 shows the behavior of and for a severe three phase bus fault.3 We observe that the transmission-line steady-state phasor model is erroneous immediately after a fault. For a severe fault, model accuracy improves within two cycles. Fig. 5 shows variation of and for a less severe fault. In this case behavior of and shows that steady-state model provides a reasonably good approximation of system behavior. The behavior of error terms and suggest that threshold parameter used to detect fault in differential protection should have adaptive parameters. When model inaccuracy is high, then restraint should be high and vice versa. 3The system details are provided in Section VIII. DAMBHARE et al.: ADAPTIVE CURRENT DIFFERENTIAL PROTECTION SCHEMES Fig. 3. Variation in k and k at end i (refer Fig. 1) for phase a. The external LLL bus fault is at bus i on 230-kV system (fault resistance is 0.1 and fault occurs at 0.115 sec). Observe that both k and k are affected by a close in bus fault. 1835 Fig. 5. Variation in k and k at end i (refer Fig. 1) for phase a. The external LLL bus fault is at bus i on the 230-kV system (fault resistance is 100 and fault occurs at 0.115 s). 1) high impedance fault may not involve appreciable transients (refer Fig. 5); 2) high impedance faults should not lead to gross errors due to CT saturation and 3) large disturbances (e.g., load throw off and external faults) will cause large differential currents because 1) the phasor model is not truly valid under such situations (as shown in Fig. 3) and 2) CT errors may increase due to partial saturation; hence, large transients or disturbances demand a larger restrain region. The aforementioned observations suggest that the height of the restrain region should be a function of the current magniand . In particular, we propose the following tudes of restraining function: Fig. 4. Variation in k and k at remote end j (refer Fig. 1) for phase a. The external LLL bus fault is at bus i on the 230-kV system (fault resistance is 0.1 and fault occurs at 0.115 s). Observe that k remains close to unity for the remote bus and the behavior of k is similar to k at bus i. IV. ADAPTIVE CONTROL OF RESTRAIN REGION A protection engineer strikes balance between dependability and security of a relay by controlling the sensitivity. Dependability of a relay can be improved by increasing the sensitivity. Sensitivity of the differential relay can be improved by reducing the area of the restrain region in the Fig. 2. Since, we have already tightened the width of the restrain region, this implies that we should reduce height of the rectangle representing the restrain region. However, it is equally important to keep it large enough so that relay does not pick up on transients or external disturbance which includes a fault. Too sensitive relay setting increases the possibility of relay maloperation and hence compromises security. We now propose an important enhancement to improve sensitivity of the current differential relay without compromising on its security. Basically, sensitivity implies an ability to detect low current or high impedance fault. The proposed enhancement is based on the following observations: (18) where and are suitable constants. We assume that is greater than 1. In case the ratio is less than one, then the numerator and the denominator should be interchanged. The relay trips when either: 1) the restraining function is greater than zero or 2) when the angular separation criterion described in the earlier section is violated. 1) Selection of Constants and : Under no-fault and is equal to one. steady-state conditions, ratio depends upon line current Further, the term and hence it can be very small ( and ). This suggests that constant should be at least equal to 1. Further, for sensitive protection, constant should be chosen close to and 0.0015 unity. In particular, we have found to be a satisfactory choice. Small magnitude of is chosen because fault current range is approximately in kiloAmperes. At lower values of , possibility of relay maloperation on extreme load throwoffs have been observed. V. CURRENT DIFFERENTIAL PROTECTION IN PHASE COORDINATES Positive sequence network is excited by both ground and phase faults. Hence, in principle, current differential protection 1836 IEEE TRANSACTIONS ON POWER DELIVERY, VOL. 24, NO. 4, OCTOBER 2009 Indices , and represent the respective phases. Similarly, the line current equation at bus can be expressed as follows: (24) Thus, we conclude that there is no fault on the line if (25) (26) (27) Fig. 6. Equivalent- model of three phase transposed transmission line [24]. scheme using a positive sequence network representation can alone detect all possible faults. However, sensitivity using positive sequence component alone will vary with the type of fault. It will be maximum for a bolted three-phase (LLLG) fault. In contrast, for a single line to ground fault, the sensitivity for ground fault detection will be reduced by a factor of three approximately.4 This motivates that either all the sequence networks (positive, negative, zero) be used for decision making, or computation in phase co-ordinates should be employed. We prefer the phase domain approach because of its simplicity and accuracy. Let us consider the equivalent- model of a three phase transposed transmission line as shown in Fig. 6. Let and be the self and mutual series impedance of the line. For a transposed line, they can be easily computed from the sequence data as follows: (19) (20) where and are the positive, negative and zero sequence impedance of the transmission line. Similarly, and are self and mutual shunt susceptance of the transmission line. They can be computed as follows: In practice, each phase tripping logic can be set using the procedure described in Section IV. and can be comRemark 1: The currents phasors puted from GPS-synchronized measurements using (23) and (24). Total twelve GPS-synchronized measurements are required, three currents and three voltages at each end. Phasors are computed from most recent samples by recursive discrete Fourier transform (DFT) [21] or phasorlets [12]. An alternative and in the phase domain to estimation of currents would be computation in the time domain. However, phasor approach has been preferred because it avoids numerical differentiation. Remark 2: There is no possibility of inadvertent tripping of the transmission line due to line charging current. This is bewill be zero cause the discriminant function value even during line charging. VI. RELAYING ALGORITHM We now propose following algorithm for sensitive and secure current differential protection scheme. A. At Node “i” 1) Input line parameters, relay settings ( and ), sampling frequency and trip value for . counter 0. 2) Set 3) Acquire latest GPS-synchronized time-tagged samples and where (21) (22) It has to be noted that, usually, will be negative as . Now from Fig. 6, the line current equation at bus in phase coordinates can be expressed as follows: 4) 5) 6) 7) (23) 4Note that for LLLG fault, I =I and for LG fault I 3I . Time “t” indicates an instant corresponding to latest sample and , , and designate the three phases. Update phasors5 and . by using (23). Compute Acquire the latest phasors, from the other end. Note that due to communication latency . and by using (18) and For instant , compute (8). 5Phasors can be updated using full-cycle recursive DFT, half-cycle recursive DFT, or phasorlet. DAMBHARE et al.: ADAPTIVE CURRENT DIFFERENTIAL PROTECTION SCHEMES 1837 From the bus voltage and line current measurements at bus , we estimate current in the series capacitor-MOV combination as follows: (28) (29) (30) Similarly, current equations: can be estimated by the following (31) Fig. 7. GPS-synchronized current differential protection scheme for seriescompensated line (series capacitor at end). (32) (33) If there is no fault on the line, then we have However, if there is a fault on the line, then discriminant funcwill not be zero. tion Remark 3: The extension of the aforementioned scheme in phase coordinates is straightforward. For the simplicity of illustration, we have used sequence representation, but all calculations are carried out in phase coordinates. The method can be easily adapted even if the series compensation is not at the center of the line. Similarly, the scheme can be extended for the protection of a multiterminal line. Fig. 8. GPS-synchronized current differential protection scheme for the seriescompensated line (series capacitor at mid point). 8) Check if: OR . If TRUE, then . else, if 9) If issue the trip decision. Else, go back to step 3. Similar algorithm is also applied at node the “ ”. . VII. CURRENT DIFFERENTIAL PROTECTION SCHEME FOR SERIES-COMPENSATED TRANSMISSION LINES Series capacitor on a transmission line can be installed at either end or at the midpoint. If a line is compensated at its terminals, then the scheme described in the previous section can be applied in toto using line connected GPS-synchronized line current and bus voltage measurements (see Fig. 7). However, if midpoint compensation is used, then the basic scheme using sequence network representation (proposed in the Section II) should be modified as follows. Fig. 8 shows a line with series compensation at midpoint. The line sections of either side of series compensation are accurately modelled by the equivalent model of transmission line.6 6Each equivalent model corresponds to half of the line length of uncompensated line. Notice that with equivalent ; B 6 B= , where h corresponds to half the line length. = 2 VIII. CASE STUDIES To evaluate the performance of the proposed scheme, the following methodology has been used. 1) Simulate power system response to disturbances (e.g., faults using Electromagnetic Transient Program (EMTP) simulations. ATP [24] software has been used for simulations. 2) Samples obtained from the EMTP simulation are fed to a MATLAB program which implements the proposed differential protection scheme. Full-cycle recursive DFT, halfcycle recursive DFT, and phasorlets algorithms are used to estimate the phasors. 3) The proposed scheme is compared and contrasted with: 1) the conventional GPS-based current differential scheme of [4] and 2) a more recent method reported in [7]. We report results on a two-area, 230–kV, 4–generator, 10–bus system (refer to Fig. 9). Detailed generator, load and line data on a 100-MVA base are given in [25]. The two areas are connected by three parallel ac tie lines of 220 km each. In ATP-EMTP simulation, transmission lines are represented by Clarke’s model (distributed parameters) and a detailed model is used for representing generators. The initial values of generator voltage magnitude and angles are calculated from the load-flow analysis. The proposed scheme is applied for primary between node 3 and 13. protection of one of the tie lines The fault location is measured from bus 3. ANSI 1200:5, class C400 CT model [26] and 250 kV:100-V CVT model [27], have 1838 IEEE TRANSACTIONS ON POWER DELIVERY, VOL. 24, NO. 4, OCTOBER 2009 Fig. 9. Single-line diagram of a two-area, four-generator, ten-bus system. Fig. 10. Equivalent circuit of CT used in ATP simulation R : : . mH and R 0 0003 = 24 = 0:63 ; L = Fig. 11. Performance of proposed current differential protection scheme on external faults. Note that relay does not pick up as all the final operating points are inside the restrain region. The performance of the proposed scheme can be gauged by its ability to balance the following well-known contradictions of power systems relaying: • dependability versus security; • speed versus accuracy. We also evaluate the performance with series-compensated and mutually coupled lines. A. Dependability Versus Security TABLE I 0 i CHARACTERISTICS OF 1200:5 ANSI CT been used for obtaining realistic CT and CCVT response during EMTP simulations. In these simulations, type-98 nonlinear saturable inductor model has been used to simulate nonlinear magnetizing reactance of CT. It is connected across the secondary of ideal CT (refer Fig. 10). The Type-98 model requires nonlinear characteristics of the CT core. To convert the excitation curve pairs, the methodology described specified by in [28], [29] is used. The CT model data have been given in Table I. Since standard data do not provide hysteresis information (hysteresis loss is practically negligible), the type-98 model7 was considered most suitable to simulate magnetizing impedance. Anti-aliasing filter [21], being analog filter has to be simulated through ATP. It is a two stage R-C filter with a cutoff frequency of 360 Hz, which is well below the minimum sampling frequency of 1 kHz used in relaying and sufficiently above the 50-Hz frequency requirement for phasor extraction. Samples obtained from ATP-EMTP simulation correspond to time-synchronized GPS samples. The time step used for ATPEMTP simulations is 20 s. However, the relaying system data acquisition rate is set to 1000 Hz. 7Alternative to this was type-96 model, which requires hysteresis details. First, we consider nonadaptive setting of the relay in current differential plane which has already been outlined in Section II. Then, we provide results with the adaptive scheme. 1) External Faults: To ascertain security, it must be ascertained that the differential relay does not operate for any external fault. This verification is usually carried out on the severe external faults. All the four types of external shunt faults (LG, LL, LLG and LLL) are simulated on buses 3 and 13, as well as on adjacent lines 3–102 and lines 13–112 at 25%, 50%, and 75% length. In each case, the fault resistance is varied from 0 to 100 in steps of 10 and fault inception angle is varied from 0 to 300 in steps of 15 . For each case, we compute , and plot the final operating point (marked by “ ” in Fig. 11) on current differential plane. As the “ ” always appear in restrain region, it validates that the proposed relay will not trip on load or external fault. The figure also shows that the restrain region cannot be reduced, significantly, without compromising the relay security. Fig. 12 shows the trajectory of phase-a operating point on current differential plane for the bolted LLL fault on bus 3 (external fault) for the fault inception angle of 270 . As the relay operating point lies inside the restrain region, the relay does not pick up on external fault. Similar investigations carried out with the adaptive relay setting show that the relay does not pick up on any external fault or large disturbance like load throw off etc. However, conventional scheme of [4] tends to operate on low resistance external fault on bus 3 and 13. We conclude that proposed scheme does not pick up on external faults. 2) Internal Faults: Sensitivity of the proposed scheme can be evaluated by its ability to detect a high impedance internal fault. Fig. 13 shows the trajectory of phase-a operating points on current differential plane for one of the cases of LL fault on DAMBHARE et al.: ADAPTIVE CURRENT DIFFERENTIAL PROTECTION SCHEMES 1839 Fig. 12. Trajectory of phase-a operating point for proposed current differential protection scheme on external fault (LLL bolted fault on bus 3, fault inception angle 270 ). Note that the relay does not pick up. Fig. 14. Effect of phasor computation algorithms on relay operating time of phase-a for LLL fault at midpoint for the proposed current differential protection scheme (sampling frequency is 1 kHz). Fig. 13. Trajectory of phase-a operating point of proposed current differential protection scheme for internal fault (LL fault at the start of line, fault inception angle 270 ; fault resistance = 600 ). Note that the relay picks up. TABLE II SENSITIVITY FOR HIGH RESISTANCE INTERNAL FAULT phase a-b, at the start of line for the fault inception angle of 270 and a large fault resistance of 600 . Table II shows the highest resistance fault, that can be detected by the differential protection schemes on line , irrespective of fault location and fault inception angle. The relays were set to provide maximum sensitivity without compromising security. The table clearly shows that the proposed scheme enables far more sensitive relay setting than the conventional scheme of [4]. With nonadaptive setting, the relay sensitivity is similar to that of scheme suggested in [7]. This can be explained from the fact that both the methods account for line charging contributions. However, with the proposed adaptive setting strategy of the restrain region, we notice that sensitivity of the current differential protection scheme improves by a factor of about 2.5. We emphasize that this improvement in the sensitivity using adaptive setting strategy is not at the cost of the relay security. Remark 4: The external system can change due to various factors like, sudden large change in load or generation, outage of adjacent line, single pole tripping, non simultaneous opening of adjacent line circuit breaker etc. Simulations have been carried out to ascertain that the proposed current differential scheme is very robust and does not maloperate on any of the above system disturbances. 3) Line Charging: The energization of line under no load and heavy load condition is simulated and the performance of proposed current differential scheme is compared with other schemes. Simulation results show that the proposed scheme is immune to line charging current. This is because the actuating is independent of the line quantity of proposed scheme, charging current. 4) Effect of a Mutually Coupled Line: In principle, a current differential relay should be immune to effect of mutual coupling of double circuit transmission lines. To ascertain this, line and (refer Fig. 9) are modelled as individual continuously transposed double circuit lines with inter-circuit zero sequence coupling, using distributed parameters (Clarke-2 3) model. Proposed scheme is applied to line and is tested for all four and also on line . The fault location, types of faults on line fault resistance and fault inception angle is also varied. Simulation results confirm that proposed current differential scheme trips correctly on all internal faults and does not maloperate on any external fault. B. Speed versus Accuracy In the proposed GPS-synchronized current differential protection scheme, the phasors are updated after every sample. The scheme is very fast (refer to Figs. 14 and 15) even if the trip decision is taken on the basis of error exceeding the threshold value consistently for four samples. Simulation results show that the proposed scheme is very fast and takes less than half a cycle to operate for low resistance faults. However, it needs one to two cycles to detect the faults above 500 resistance. This is acceptable with high impedance faults as the fault current level is low and CTs will not saturate. 1) Phasor Estimation Algorithms: The relay operating time depends upon the method of phasor estimation. Fig. 14 shows the operating time with the proposed scheme when phasors are estimated by using full-cycle recursive DFT (FCDFT), halfcycle recursive DFT (HCDFT), and phasorlet with adaptive and nonadaptive settings. The studies show that with the relay setting, phasorlets provide the fastest relay operation followed by half-cycle recursive DFT and full-cycle recursive DFT, respectively, for the same sampling frequency. Similar behavior is observed for the other two phases. 1840 IEEE TRANSACTIONS ON POWER DELIVERY, VOL. 24, NO. 4, OCTOBER 2009 TABLE III SENSITIVITY FOR HIGH-RESISTANCE INTERNAL FAULT FOR SERIES-COMPENSATED LINE Fig. 15. Effect of sampling frequency on the relay operating time of phase-a for the LLL fault at midpoint for the proposed current differential protection scheme when phasors are estimated by using full-cycle recursive DFT. The results also show that relay operation is faster with the adaptive control of the restrain region irrespective of the phasor estimation algorithm. The fastest relay operation is achieved with adaptive control of restrain region and when the phasorlet algorithm is used for phasor computation. Remark 5: It is interesting to observe that time to trip has an inverse relationship to the magnitude of fault current. This behavior can be explained as follows. For the sake of simplicity, consider that the phasor is computed by using fullcycle recursive DFT and nonadaptive methodology is used. It takes one cycle for the phasor computation algorithm to latch to a fault current value. Assuming a linear change in the estimate, we see that for a fixed pick-up value, larger fault currents imply faster pick up (and vice versa). 2) Sampling Frequency: The sampling rate influences the operating time of the relay. Fig. 15 show the operating time of proposed scheme with adaptive and nonadaptive settings, for the sampling frequency of 1, 2, and 2.5 kHz using full-cycle recursive DFT algorithm for phasors estimation. The studies show that, 2.5 kHz sampling rate gives fastest relay operation followed by 2 and 1 kHz, respectively. However, marginal gains in speed reduce at higher sampling frequencies i.e., a result in concurrence with the law of diminishing marginal utility. Similar observations have been made in the context of digital distance relay in [10] and [30]. C. Performance With Series-Compensated Line Application of proposed scheme to series-compensated transmission line is discussed in Section VII. All the three tie lines between nodes 3 and 13 (refer Fig. 9) are compensated with 30% series capacitive compensation. The MOV data (connected across the series capacitors) is given in [24]. The parallel combination of series capacitor and MOVs are placed at the midpoint of lines. The initial value of generator voltage magnitudes and angles are computed from the load flow analysis of compensated system. The proposed scheme is then applied for the primary protection of tie line . All the four types of faults (LG, LL, LLG, and LLL) are simulated on both side of series capacitor on line to test the performance of proposed scheme on internal faults. Similar faults are simulated on bus 3 and bus 13 as well as on lines 3–102 and lines 13–112 to test the performance of proposed scheme on external faults. For every fault, fault location is varied from 0% to 100% in steps of 10%, fault resistance is increased from 0 in steps of 10 and fault inception angle is varied from 0 to 300 in steps of 15 . It is validated that the relay discriminates between internal and external fault and trips on internal fault only. Extensive case studies are carried out to compare the sensitivity of proposed scheme with schemes of [4] and [7]. Table III shows the highest resistance fault that can be detected by the differential protection schemes on line , irrespective of fault location and fault inception angle. Note that the proposed scheme detects very high resistance LG fault. Also, the sensitivity of proposed scheme on other types of fault is better than conventional scheme. Further, it is seen that with nonadaptive version of the proposed methodology, sensitivity of the proposed method is comparable with that of method reported in [7]. However, sensitivity improves significantly when proposed adaptive protection methodology is used. This brings out the importance of the suggested adaptive control of the relay restrain region. The proposed scheme is also compared and contrasted with segregated phase comparison scheme and distance protection scheme in presence of current and voltage inversion. It is observed that distance protection scheme maloperates for seriescompensated transmission lines and segregated phase comparison scheme fails to trip in presence of current inversion [31]. However, the proposed scheme works satisfactorily. IX. CONCLUSION Significant advances have been made in the current differential protection schemes for transmission-line protection. State of the art methods consider both: 1) modeling of shunt capacitance of line to account for line charging effect and 2) time stamped and synchronized phasors to correctly account for relative phase angle information. No doubt, these measures have significantly improved the dependability and security of the current differential protection schemes. In this paper, we have proposed enhancements to further improve the dependability and security of the current differential schemes. Salient contributions of the paper are as follows. 1) Development of dynamic phasor model of a transmissionline and error analysis of current differential protection scheme using steady-state phasor. 2) An adaptive relay setting procedure to control the area of the restrain region in the current differential plane. The area of the restraining region is made a function of line current. At lower currents, restraining area is kept small. This increases the sensitivity of the relay. At larger currents, area DAMBHARE et al.: ADAPTIVE CURRENT DIFFERENTIAL PROTECTION SCHEMES of the restraining region is increased in proportion to the current. This increases the security of the relay without compromising the sensitivity. Simulation studies show that this can improve sensitivity of the relay by at least a factor of 2.5. 3) Extension of the proposed methodology for protection of series compensated and multiterminal transmission lines. Simulation studies show that this can improve sensitivity of the relay by at least a factor of 2. 4) Comparative evaluation with state of the art methods. 5) An in depth analysis of the following contradictions: • dependability versus security; • speed versus accuracy. We conclude that the proposed adaptive control of restrain region together with phasorlet algorithm for phasor estimation provides the best solution for current differential protection of (series compensated) transmission lines. It enhances sensitivity and relaying speed without compromising the security of protection system. REFERENCES [1] J. L. Blackburn and T. J. Domin, Protective Relaying: Principles and Applications, 3rd ed. Boca Raton, FL: CRC, 2007. [2] S. C. Sun and R. E. Ray, “A current differential relay system using fiber optics communications,” IEEE Trans. Power App. Syst., vol. PAS-102, no. 2, pp. 410–419, Feb. 1983. [3] P. K. Gangadharan, T. S. Sidhu, and A. Klimek, “Influence of current transformer saturation on line current differential protection algorithums,” Inst. Eng. Technol. Proc. Gen. Transm. Distrib., vol. 1, no. 2, pp. 270–277, Mar. 2007. [4] H. Y. Li, E. P. Southern, P. A. Crossley, S. Potts, S. D. A. Pickering, B. R. J. Caunce, and G. C. Weller, “A new type of differential feeder protection relay using global positioning system for data synchronization,” IEEE Trans. Power Del., vol. 12, no. 3, pp. 1090–1099, Jul. 1997. [5] I. Hall, P. G. Beaumont, G. P. Baber, and I. Shuto, “New line current differential relay using GPS synchronization,” presented at the IEEE Bologna Power Tech Conf., Bologna, Italy, Jun. 2003. [6] G. Houlei, J. Shifang, and H. Jiali, “Development of GPS synchronised digital current differential protection,” in Proc. Int. Conf. Power System Technology, Apr. 1998, pp. 1177–1182. [7] Z. Y. Xu, Z. Q. Du, L. Ran, Y. K. Wu, Q. X. Yang, and J. L. He, “A current differential relay for a 1000-kV UHV transmission line,” IEEE Trans. Power Del., vol. 22, no. 3, pp. 1392–1399, Jul. 2007. [8] J. A. Jiang, C. W. Liu, and C. S. Chen, “A novel adaptive PMU-based transmission line relay—Design and EMTP simulation results,” IEEE Trans. Power Del., vol. 17, no. 4, pp. 930–937, Oct. 2002. [9] S. Sheng, K. K. Li, W. L. Chan, X. J. Zeng, and D. Xianzhong, “Agentbased wide area current differential protection system,” in Proc. Industry Applications Conf., Oct. 2005, pp. 453–458. [10] G. E. Alexander, “Advancements in adaptive algorithms for secure high-speed distance protection,” presented at the 23rd Annual Western Protective Relay Conf., Oct. 1996. [11] M. G. Adamiak and W. Premerlani, “A new approach to current differential protection for transmission lines,” presented at the Protective Relaying Committee Meeting, Electric Council of New England, Portsmouth, NH, Oct. 1998. [12] J. A. de la O Serna, “Phasor estimation from phasorlets,” IEEE Trans. Instrum. Meas., vol. 54, no. 1, pp. 134–143, Feb. 2005. [13] R. K. Gajbhiye, B. Gopi, P. Kulkarni, and S. A. Soman, “Computationally efficient methodology for analysis of faulted power systems with series compensated transmission lines: A phase coordinate approach,” IEEE Trans. Power Del., vol. 23, no. 2, pp. 873–880, Apr. 2008. [14] M. M. Saha, B. Kasztenny, E. Rosolowki, and J. Izykowski, “First zone algorithn for protection of series compensated lines,” IEEE Trans. Power Del., vol. 16, no. 1, pp. 200–207, Apr. 2001. [15] A. A. Girgis, A. A. Sallam, and A. K. El-Din, “An adaptive protection scheme for advanced series compensated (ASC) transmission lines,” IEEE Trans. Power Del., vol. 13, no. 2, pp. 414–420, Apr. 1998. [16] T. S. Sidhu and M. Khederzadeh, “Series compensated line protection enhancement by modified pilot relaying schemes,” IEEE Trans. Power Del., vol. 21, no. 3, pp. 1191–1198, Jul. 2006. [17] “Series capacitor bank protection,” IEEE Power System Relaying Committee Special Publication 1998, Working Group K13. 1841 [18] G. Michel et al., “Digital communications for relay protection,” [Online]. Available: http://www.pes-psrc.org/ [19] M. G. Adamaik, A. P. Apostolov, M. M. Begovic, C. F. Henville, K. E. Martin, G. L. Michel, A. G. Phadke, and J. S. Thorp, “Wide area protecion—Technology and infrastructures,” IEEE Trans. Power Del., vol. 21, no. 2, pp. 601–609, Apr. 2006. [20] I. H. G. Brunello, I. Voloh, and J. Fitch, “Current differential relayingcoping with communications channel asymmetry,” in Proc. 8th IEE Int. Conf. Developments in Power System Protection, Apr. 2004, vol. 2, pp. 821–824. [21] A. G. Phadke and J. S. Thorp, Computer Relaying for Power Systems. Taunton, U.K.: Research Studies Press, 1988. [22] M. Zhang, X. Dong, Z. Q. Bo, B. R. J. Caunce, and A. Klimek, “A new current differential protection scheme for two terminal transmission lines,” in Proc. Power Engineering Society General Meeting, Jun. 2007, pp. 1–6. [23] P. Mattavelli, G. C. Verghese, and A. M. Stankovic, “Phasor dynamics of thyristor-controlled series capacitor systems,” IEEE Trans. Power Syst., vol. 12, no. 3, pp. 1259–1267, Aug. 1997. [24] H. W. Dommel, Electromagnetic Transients Program (EMTP) Theory Book. Portland, OR: Bonneville Power Administration, 1986. [25] K. R. Padiyar, Power System Dynamics, 2nd ed. Hydrabad, India: BS Publications, 2002. [26] P. V. Chawande, “A high fidelity and robust closed loop active flux compensation scheme for mitigating CT saturation,” Ph.D. dissertation, Inst. Technol.-Bombay, Bombay, India, 2007. [27] D. Fernandes, W. L. A. Neves, and J. C. A. Vasconcelos, “Coupling capacitor voltage transformer: A model for electromagnetic transient studies,” Elect. Power Syst. Res., vol. 77, pp. 125–134, Mar. 2006. [28] W. L. A. Neves and H. W. Dommel, “On modelling iron core nonlinearities,” IEEE Trans. Power Syst., vol. 8, no. 2, pp. 417–423, May 1993. [29] D. A. Tziouvaras et al., “Mathematical models for current, voltage, and coupling capacitor voltage transformers,” IEEE Trans. Power Del., vol. 15, no. 1, pp. 62–72, Jan. 2000. [30] J. M. Kennedy, G. E. Alexander, and J. S. Thorp, “Variable digital filter response time in digital distance relay.” no. GER3798 [Online]. Available: http://www.geindustrial.com/multilin/notes/ger3798.htm [31] S. S. Dambhare, N. W. Kinhekar, S. A. Soman, and M. C. Chandorkar, “ATP-EMTP analysis of series compensated lines for distance protection scheme,” in Proc. Int. Conf. Power System Protection, Banglore, India, Feb. 2007, pp. 36–47. Sanjay Dambhare received the B.E. degree in electrical engineering from the Visvesvaraya Regional College of Engineering, Nagpur, India, in 1989, the M.Tech degree in electrical engineering from the Indian Institute of Technology, Bombay, India, in 1998, and is currently pursuing the Ph.D. degree in electrical engineering at the Indian Institute of Technology-Bombay, Mumbai. He is currently Associate Professor at the College of Engineering, Pune, India. His research interests include power system protection, numerical relays, and power system computation. S. A. Soman (M’07) received the B.E. degree in electrical engineering from the Maulana Azad College of Technology, Bhopal, India, in 1989, and the M.E. and Ph.D. degrees in electrical engineering from the Indian Institute of Science, Bangalore, India, in 1992 and 1996, respectively. Currently, he is a Professor in the Department of Electrical Engineering, Indian Institute of Technology-Bombay, Mumbai, India. He is author of the book Computational Methods for Large Power System Analysis: An Object Oriented Approach. His research interests and activities include large-scale power system analysis, deregulation, application of optimization techniques, and power system protection. M. C. Chandorkar (M’84) received the B.Tech degree in electrical engineering from the Indian Institute of Technology-Bombay, Mumbai, India, in 1984, the M.Tech degree in electrical engineering from the Indian Institute of TechnologyMadras, Chennai, India, in 1987, and the Ph.D. degree from the University of Wisconsin, Madison, in 1995. He has several years of experience in the power-electronics industry in India, Europe, and the U.S. During 1996-1999, he was with ABB Corporate Research Ltd., Baden-Daettwil, Switzerland. He is currently Professor in the Department of Electrical Engineering, Indian Institute of Technology-Bombay, Mumbai, India. His research interests include the application of power electronics to power-quality improvement, power system protection, power-electronic converters, and control of electrical drives.
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