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Article

A New Method of Fault Localization for 500 kV Transmission Lines Based on FRFT-SVD and Curve Fitting

by
Mohamed H. Saad
1,*,
Mostafa M. Fouda
2,3,* and
Abdelrahman Said
3
1
Radiation Engineering Department, National Center for Radiation Research and Technology (NCRRT), Egyptian Atomic Energy Authority, Cairo 11672, Egypt
2
Department of Electrical and Computer Engineering, College of Science and Engineering, Idaho State University, Pocatello, ID 83209, USA
3
Department of Electrical Engineering, Faculty of Engineering at Shoubra, Benha University, Cairo 11672, Egypt
*
Authors to whom correspondence should be addressed.
Energies 2023, 16(2), 758; https://doi.org/10.3390/en16020758
Submission received: 10 December 2022 / Revised: 4 January 2023 / Accepted: 6 January 2023 / Published: 9 January 2023
(This article belongs to the Section F: Electrical Engineering)

Abstract

:
The paper presents the Fractional Fourier Transform-Singular Value Decomposition (FRFT-SVD) method for the localization of various power system faults in a 200 km long, 500 kV Egyptian transmission line using sent end-line current signals. Transient simulations are carried out using Alternating Transient Program/Electromagnetic Transient Program (ATP-EMTP), and the outcomes are then examined in MATLAB to carry out a sensitivity analysis against measurement noises, sampling frequency, and fault characteristics. The proposed work employs current fault signals of five distinct kinds at nineteen intermediate points throughout the length of the line. The approach utilized to construct the localizer model is FRFT-SVD. It is much more effortless, precise, and effective. The FRFT-SVD is utilized in this technique to calculate 19 sets of indices of the greatest S value throughout the length of the line. The FRFT-SVD localizer model is also designed to be realistic, with power system noise corrupting fault signals. To generate fault curves, the curve fitting technique is applied to these 19 sets of indices. Reduced chi-squared and modified R-squared criteria are used to choose the best-suited curve. The proposed work results in a very precise localization, with only a 0.0016% average percentage error for fault localization and a maximum percentage error of 0.002% for the 200 km Egyptian transmission line. Finally, this work can be employed as a proper link between the nuclear power plant and the grid. The proposed method is an efficient fault distance estimation method that might contribute to creating a dependable transient-based approach to power system protection.

1. Introduction

In deregulated situations, accurate fault location in transmission lines saves power system recovery time, associated costs, and financial losses. Three techniques are used to locate faults in the electrical grid: approaches based on impedance [1,2], traveling wave fault location [3,4,5], and artificial intelligence [6,7,8,9,10]. While traveling wave-based methods employ high-frequency transient components produced by fault or switching operations, impedance-based methods utilize power frequency components of voltages and currents. Artificial intelligence (AI) and machine learning (ML) techniques are typically the foundation of soft computing. Singular value decomposition (SVD) techniques have drawn greater attention in recent years thanks to developments in signal processing, the ability to sample signals at high frequencies, and the creation of optical sensors. Voltage, current, power, frequency, etc., are only a few of the many variable factors of the power system as a whole. The application of SVD can reduce the size of these electrical characteristics, making it easier, faster, and more accurate to determine fault features. Furthermore, SVD is extremely efficient when dealing with noisy data. Consequently, it reduces the unpredictability of noise, making SVD more suitable for application in a noisy setting such as the power system.
The FRFT-SVD approach, which is exceedingly effective, accurate, and simple to use, was employed to construct the localizer model. To determine the characteristics of a signal in terms of the maximum S value, which is employed in this approach to calculate the indices, FRFT-SVD is a straightforward technique. In particular, for more decomposition, wavelet transform-based analysis becomes more challenging. On the other hand, neural networks need a lot of training data that are spread out over a long period of time. As a result, the proposed fault localizer is both very precise and fast. The proposed analysis might be enhanced to include fault localization in a transmission network or a system with several interconnected buses. In the event of such a system, it is first necessary to determine the bus from which the line with the problem originated. After conducting the following fault localization study, that bus might be taken as the source point. This study’s goal is to provide a technique for the efficient use of curve fitting analysis and FRFT-SVD for the sole purpose of fault site prediction.

1.1. Related Work

Scientists have used quick fault detection, classification, and location identification techniques to guarantee system stability and safety [11].
To restore the system stability in a power transmission network, the faulty phase or phases must be removed. Numerous computational tools for defect diagnostics have been created by researchers. As previously noted, the proposed work investigates the function of SVM as an upgrading simulation tool and uses it to create a fault location technique.
For the detection, categorization, and localization of faults, researchers have created numerous mathematical and computational algorithms. Nowadays, researchers use artificial intelligence (AI) widely in the study of power systems and fault analysis. One of the most popular and important techniques for studying the protection of transmission lines in power systems has been the Artificial Neural Network (ANN) and its various variations [12].
One of the most recent developments in this area is the use of neural networks for analysis powered by extreme learning machines (ELMs) [13]. As a conventional approach to fault signal analysis, Wavelet Transform (WT) has been crucial in numerous studies of fault analysis, even using contemporary compensating devices [14].
Another useful tool for fault analysis is the fuzzy inference system, which is frequently employed as a primary analytical technique alone [15], as well as in a hybrid model with wavelet analysis [16] and neural networks, known as the (ANFIS) model. To create wavelet-based ANFIS models and as a useful means of comprehensive analysis, this hybrid model has frequently been supported by WT analysis [17]. As a significant standalone method of study, (SVM) has also been utilized in numerous studies pertaining to power system protection algorithms [18].
A simple approach to classifying and locating power system defects was developed using principal component analysis (PCA). For the quick location of the faulty line, this work solely employs 14-cycle pre-fault and 12-cycle post-fault receiving side current waveforms.
Although SVM-based algorithms are also highly popular for fault analysis, they nevertheless have the issue of intensive training because of noise contamination to some extent.
Both [19] and [20] authors explore faults in OHTL with various sources linked to the system, whereas [19] authors present a method for fault identification intended for busbar zone protection, as demonstrated by the authors of [21], who provided polynomial and Gaussian radial basis functions (RBF) for fault classification, or [22], who used dyadic WT-based SVM for fault classification.
The authors of [23] use time-synchronized fault signals as modern research tools.
Other new research inclusions include measurement analysis based on magnetic flux variation [24], feature extraction techniques based on mathematical morphology [25], ensemble Kalman filter-based strategies [26], analysis based on the combination of several sensors and fuzzy inference [27], monitoring of transmission line [28,29,30], etc.
Several more methodologies can help with the development of fault analysis strategies. Considering this, the purpose of this study is to provide a technique for the efficient use of curve fitting analysis and FRFT-SVD only for fault site prediction. Consequently, the analysis is conducted with a variable fault resistance, various fault inception angles, and noise. The paper proposes the Fractional Fourier Transform-Singular Value Decomposition (FRFT-SVD) approach for localizing various power system problems in a 200 km long, 500 kV Egyptian transmission line under varied operating conditions utilizing received end-line current data. The proposed method has all the potential to become an efficient way of predicting the distance to a fault, which may help in the creation of a dependable transient-based power system protection strategy.

1.2. Motivation and Contributions

The numerous AT-detection technologies that have recently been introduced each have drawbacks. For instance, the choice of the mother wavelet affects DWT performance. Due to the aliasing phenomena, the Empirical Mode Decomposition (EMD) process has the potential to affect HHT performance. Wavelet transform-based analysis becomes increasingly complicated as the depth of decomposition increases. On the other hand, neural networks need extensive training time and widely dispersed training data.
In this paper, a new method for fault location based on FRFT-SVD and curve fitting of 500 kV long transmission lines is proposed. The purpose of this work is to provide a strategy for the efficient use of curve fitting analysis and FRFT-SVD for fault site prediction only. This method lacks the shortcomings of the methods listed above because it was designed based on algebraic operations in the time-frequency domain. The suggested algorithm addresses the finding of defects for all fault kinds under various operational scenarios. Simulations are run in the EMTP/ATP program, and the results are analyzed in MATLAB to assess how well the proposed technique performs. Through comprehensive simulations, the sensitivity analysis of measurement noises, sample frequency, and fault parameters is examined. The results of FRFT-SVD and curve fitting are examined, and the suggested method’s proper operation under various circumstances is demonstrated. Following is a summary of the suggested method’s key characteristics: (1) It is sufficiently resilient against noise. (2) It is simple to implement and has a straightforward structure. (3) Because it uses straightforward algebraic calculations, it runs quickly enough for online applications. (4) It responds appropriately without the need for structural adjustments or training in various systems and circumstances.

1.3. Organization

The organization of the paper is as follows. Section 2 describes the details of the system under study. The study of 500 kV-long transmission line fault signals is presented in Section 3. Section 4 outlines the basic tenets of the suggested detection method. In Section 5, thorough simulations are used to assess how sensitive the suggested strategy is to the system characteristics; a summary of the outcomes of contrasting the suggested method with traditional methods is also provided in Section 5. In Section 6, conclusions are presented.

2. System Description and Modelling

Figure 1 depicts the system under analysis, which is based on a typical 500 kV transmission line in Egypt with a 200 km-long line.
The most sophisticated JMARTI model, which is a frequency-dependent model and suitable for transients research [31,32], is used to simulate the considered transmission line. Table 1 lists the key characteristics of the transmission system in operation. There are two ground wires with direct tower grounding, and phase conductors are presumed to be perfectly transposed. It is assumed that the soil resistivity is 100 Ωm [31]. Figure 2 depicts the conductor arrangements and tower configuration [31].

3. Analysis of 500 kV OHTL Fault Signals

A practical Egyptian 500 kV OHTL ATP/EMTP simulation uses a 200 km transmission line model. Twenty identical blocks, each 10 km in length, are connected in a cascade to develop the 200 km OHTL model. This designed system is shown in Figure 3. Faults have been conducted at the intermediate junctions of each consecutive block, and the fault current waveforms are recorded at the sending side only. Faults depend on five main fault parameters: (fault type, fault distance, fault resistance, noise, and inception angle).
Five different fault types (Line to Ground (LG), Line to Line (LL), Line to Line to Ground (LL-G), Line to Line to Line (LLL), and Line to Line to Line to Ground (LLL-G)) are simulated in this regard, together with five fault resistances (R), five inception angles (Ɵ) (including 0°–180°), and 19 distances of the fault from the recording site (including 10 km–190 km). Following the application of LG fault type to the phases at 190 km (before the line’s end) from the transmitting side, Figure 4a–d show the faulted-phase current waveforms at different locations, fault resistance, and inception angles. Figure 4b shows the sending side signals under different locations (with fault resistance = 10 Ω, inception angle = 0° and fault location = (10 km, 50 km, 100 km, 150 km, 190 km) for the one-phase (a) to ground fault. It is evident that the faulted phase current signal peak reduced from 25 kA to 5.8 kA, or by about 77%. Figure 4c shows the sending end signals under different R (with R = (1 Ω, 10 Ω, 25 Ω, 35 Ω, 50 Ω), inception angle = 0° and fault location = 190 Km for the one-phase (a) to ground fault. It is clear that the faulted phase current amplitude reduced from 6.4 kA to 4.1 kA, or by about 36%. Figure 4d show the sending end signals under different inception angle (with fault resistance = 10Ω, Inception Angle Ɵ = (0° to 180°), and fault location = 190 km for the one-phase (a) to ground fault. Moreover, the beginning current amplitude in the case of fault at 0°, and 45° is much more than 90°, 135°, and 180°.

4. FRFT and SVD Overview

Since they are used in our suggested fault diagnosis technique, FRFT and SVD schemes will be briefly covered in this section.

4.1. Fractional Fourier Transform (FRFT)

One effective method for time-varying signal analysis is the fractional Fourier transform (FRFT). The Fourier Transform (FT) is generalized by the FRFT. FT defines a signal’s spectral content, not the timing of its spectral components [33,34,35]. Signals are rotated in the time-frequency domain by the FRFT method. As a consequence, the FRFT may transform a signal from the time domain X(t) to the frequency domain Xα(u) of the signal. The following mathematical formula can be used to define the αth order FRFT of X(t):
            X α ( u ) = F R F T α ( x ( t ) ) = x ( t ) · K α ( t , u ) d t
A fractional factor (α) with a range of 0 to 1 determines the FRFT coefficients. Therefore, in the suggested technique, we choose eigenvector FRFT as a feature extractor because of its superior advantages (with a factor between 0 and 1).

4.2. Singular Value Decomposition (SVD)

Singular value decomposition (SVD) is a matrix factorization technique that is particularly useful for a wide range of applications, including pattern identification, data dimension reduction, matrix approximation, pseudo inverse computation, and linear equation solving. As a data processing approach, SVD has been successfully used in signal processing and has been demonstrated to be effective in preventing modal aliasing. It may divide any matrix into three matrices as follows:
  A = U · S · V
where UU′ = 1 and VV′ = 1, which are referred to as the left and right singular vectors, respectively, and U and V are unitary matrices. The singular values of A, which are determined by determining the eigenvalues of AA′, are represented by the diagonal matrix S. It has the following representation:
S = ( s 1 s ρ               0                           0                                 0 0 )
where ρ is the rank of the matrix A. Note that S1 > S2 > … > Sρ, i.e., S1 is the largest singular value. Because SVD has the ability to describe the feature matrix as a collection of values (singular values), it has a dimension-reduction technique. The solitary values also have high stability. In other words, there isn’t a significant variation in the singular values of the feature matrix element as it changes.

5. Results and Discussion

5.1. Data Preparation for the Proposed Algorithm

5.1.1. Data Preparation for Training

The block diagram for the proposed method for power system fault localization using the Fractional Fourier Transform-Singular Value Decomposition (FRFT-SVD) method is shown in Figure 5.
A diagonal matrix produced by SVD over the fault current transients exhibits many of the fundamental properties of the original matrix. The vectors consist of 1500 data points, each with a pre-fault length of quarter cycles and a post-fault length of half cycles, and a sampling frequency of 2000 samples per cycle. As a result, the data matrix is produced as follows:
D n l = [ i a n l 1 i b n l 1 i c n l 1 i a n f 2 i b n l 2 i c n l 2 i a n l 1500 i b n l 1500 i c n l 1500 ] 1500 × 3
Hence, D n l = [ i a n l i a n l i a n l ] 1500 × 3 .
A fault class is represented by n denoted by 1, 2, …, 5, the location of the fault is indicated by l, and the sample index is indicated by 1, 2, … 1500. ianl, ibnl, and icnl indicate the currents for n-th class. The creation of the proposed fault localization technique makes use of fault data from 19 distinct, evenly spaced fault locations at 10, 20, 30, 40, 50, 60, 70, 80, 90, 100, 110, 120, 130, 140, 150, 160, 170, 180, and 190 km. The input training matrix for the FRFT-SVD becomes
D a l = [ i a l 10 i a l 20 i a l 190 ] 1500 × 19 D b l = [ i b l 10 i b l 20 i b l 190 ] 1500 × 19 D c l = [ i c l 10 i c l 20 i c l 190 ] 1500 × 19
where the training matrix for the n-class of fault for phases a, b, and c is represented by Dal, Dbl, and Dcl. This leads to the formation of five such matrices for each phase. The recommended fault localization methodology uses fault data for 19 distinct, evenly spaced fault sites at 10, 20, 30, 40, 50, 60, 70, 80, 90, 100, 110, 120, 130, 140, 150, 160, 170, 180, and 190 km. With a changeable fault location, the S matrix contrasts signals from a fixed phase.

5.1.2. Data Preparation for Testing

The preparation of test data is identical as well. The result is the test data matrix, which has an unknown fault location but a known fault class t:
T n t = [ i a n t 1 i b n t 1 i c n t 1 i a n t 2 i b n t 2 i c n t 2 i a n t 1500 i b n t 1500 i c n t 1500 ] 1500 × 3
Hence, T n t = [ i a n t i a n t i a n t ] 1500 × 3 , where Tnt is the test data matrix.

5.2. The Impact of Noise, Fault Resistance, and Inception Angle

The fault signals have been combined with Gaussian white noise to create noise-contaminated fault signals. By adjusting the SNR level, the fault waveform noise level can also be adjusted in four steps. The more significant point is that the proposed model is tested at a high noise level of 15 dB SNR, which is higher than the typical noise level used in most research. The impact of this undesirable noise is considered even when variations in fault type, location, and fault resistance occur concurrently. FRFT creates a signal’s intermediate time-frequency representations. SVD has a dimension reduction strategy because it expresses the feature matrix as a collection of singular values. Additionally, the singular values are stable. The maximum SVD of the FRFT for a single phase yields a single feature (maximum value S matrix). Three features are chosen for each fault state in OHTL. FRFT-SVD thus eliminates the impact of noise on discrimination. In this work, the noise immunity property is also studied. A comparison of the maximum singular value for direct standardized fault signals and that of its filtered form is shown in Table 2. Additional results are declared in Table A1, Table A2, Table A3 and Table A4. The observations demonstrate that filtering has no discernible impact on the FRFT-SVD algorithm’s results, as there is no noticeable change in the magnitude of the max singular value. Using the suggested FRFT-SVD based fault analyzer has this as a major benefit. By doing away with the need for filtering, FRFT-SVD can lessen the computational load. The SNR is varied for this purpose to observe the variation in max singular value, and the proposed algorithm is then run under more challenging conditions with higher noise levels. The maximum singular values in Table 2 and Table A1, Table A2, Table A3 and Table A4 show how the results of analyzing the filtered and unfiltered signals using maximum singular values are extremely similar. Filtering thus becomes unnecessary at the maximum singular value, saving vital computation and processing time. This demonstrates the inherent ability of FRFT-SVD to largely ignore the effect of noise.
The maximum singular values in Table 3 and Table A5, Table A6, Table A7, Table A8 and Table A9 show how the results of analyzing the filtered and unfiltered signals using maximum singular values at different fault resistance and inception are extremely similar. The results show that the proposed method is unaffected by changes in fault distance, fault resistance, noise, or fault inception angle. As a result, the proposed algorithm will work in direct form.
To demonstrate the fault localizer method, the proposed work carefully examines five different instances. As shown in Table 4 and Table A9, Table A10, Table A11 and Table A12, the maximum singular value of each faulty signal corresponding to the 19 separate fault locations throughout the length of the line is ascertained by utilizing a singular value to analyze the three-phase working signals to demonstrate this analytically.
The maximum singular values obtained for the five faults in Table 4 and Table A9, Table A10, Table A11 and Table A12 are scaled in relation to the maximum values. For each phase independently, the curve fitting technique uses these 19 scaled S values of the faulty lines as training points.
The model is built using fault data from 19 locations, namely 10, 20, 30, 40, 50, 60, 70, 80, 90, 100, 110, 120, 130, 140, 150, 160, 170, 180, and 190 km, as previously discussed. Different curves are evaluated with these scaled singular value values to determine the optimal curve fitting method, which is discussed next.

5.3. Analysis of Different Fitness Models

Best-fit approaches are used to approximate the curvilinear nature. The least reduced chi-squared and maximum adjusted R-square criteria are used to choose the top five fittest models, with the best-fit model being selected among those:
F i t 1 : f ( i ) = a 0 i + a 1
F i t 2 : f ( i ) = a 0 + a 1 i + a 2 i 2 + a 3 i 3 + a 4 i 4 + a 5 i 5 + a 6 i 6 + a 7 i 7
F i t 3 : f ( i ) = a 1 e a i + a 2 e b i + a 3 e c i
F i t 4 : f ( i ) = a 1 e ( ( ( i b 1 ) / c 1 ) 2 ) + a 2 e ( ( ( i b 2 ) / c 2 ) 2 ) + a 3 e ( ( ( i b 3 ) / c 3 ) 2 )
F i t 5 : f ( i ) = a 0 + a 1 e ( - i / c 1 )   + a 2 e ( - i / c 2 )   + a 3 e ( - i / c 3 )    
where a0, a1, c1, a2, c2, a3 and c3 are of 0.03435 ± 9.00317 × 10−4, 2.33327 ± 0.02426, 5.25993 ± 0.09922, 0.7114 ± 0.01814, 17.21614 ± 0.451, 0.25131 ± 0.00698 and 72.89877 ± 1.96831, respectively. The fifth fitting formula has an R-Square (COD) = 1, R-squared value of 1, and Reduced Chi-Sqr = 3.19786 × 10−8.
The five different fit models were progressively applied to the same set of maximum scaled singular values in order to determine which model provided the best fit with the least chi-squared and the highest adjusted R square. For the LG, LL, LL-G, LLL, and LLL-G faults, respectively, these best fit curves with the lowest reduced chi-squared and highest adjusted R-square. The best curve-fitting formula is accounted for in the fifth one. It is the most effective strategy for fault location determination. This last fitting expression employs an exponential decay with a third degree. The lowest possible error between the actual location and the predicted location is estimated using the proposed fitting formula at LG, LL, LL-G, LLL, and LLL-G faults, as depicted in Figure 6, Figure 7, Figure 8, Figure 9, and Figure 10, respectively. The difference between the predicted and real fault distances (P and A) was utilized to quantify this inaccuracy. This estimated error is equivalent to the algorithm’s accuracy. As the distance deviation rises, the algorithm’s accuracy falls. The overall accuracy is defined as the greatest estimate error throughout the whole length range of the line as well as for all conceivable fault types represented as a percentage of the total line length, C in Equation (12), and the average error (AE), is defined in Equation (13).
e r r o r     ( e ) = |   predicted   location ( P ) - actul   location ( A )     total   line   length ( C ) | × 100
( A E ) = i = 1 n e r r o r n
Table 5, Table 6, Table 7, Table 8, Table 9, Table 10, Table 11, Table 12, Table 13 and Table 14 show the locations of five faults that were predicted based on current line data and fitted using various five-curve fitting methods. Furthermore, the average error (AE) and five different fault prediction errors using line current signals and various five curve fittings are shown in these tables. The proposed work produces a localization that is extremely accurate, with a maximum percentage error of 0.002% and an average percentage error for fault localization of just 0.0016%. The proposed approach is validated with other approaches, as shown in Table 15. Both the maximum and average percentage errors are computed and compared with literature work [9,11,12,35]. A comparison between the proposed work and that experimentally published is demonstrated. This comparison was made using the same data in the form of current signals. These simulated data are generated using ATP-EMTP that was tested with the mentioned methods on [9,11,12,35]. In addition, this data corresponds to changes in power system faults in a 200 km long, 500 kV Egyptian transmission line using sent end-line current signals. The proposed work is executed using a laptop with Intel(R) Core(TM) i7-10750H and a 2.59 GHz CPU. One of the main strengths of the suggested work is the ability to use it as a link between the nuclear power plant and the grid. Moreover, the proposed method is an effective fault distance estimating method that might help to develop a reliable transient-based strategy for power system protection with minimal error.

6. Conclusions

The FRFT-SVD method, which is very effective, precise, and straightforward, was used to develop the localizer model. Here is a practical power system protection approach for long-distance power system issue prediction for a 500 kV, 50 Hz, 200 km overhead transmission line. FRFT-SVD was used to develop the suggested protective mechanism. Using the best-fit curve method, sending end current signals are evaluated after being subjected to FRFT-SVD analysis to obtain fault characteristics expressed in terms of the highest S value. Only around 0.001614% of the typical scheme is inaccurate. The lowest estimate for an LLL-G defect was 0.002%, which is also quite precise for a 200-km long line. This paper aims to provide a technique for predicting the location of faults using curve fitting analysis and FRFT-SVD. For this reason, the analysis makes use of a variety of noise, inception angle, and fault resistance variables. The proposed method may prove to be an effective way to gauge how far a problem would spread, which might be useful in creating a dependable transient-based power system security strategy. In future work, we will implement the new model in hardware and apply it in real systems with different configurations.

Author Contributions

Conceptualization, M.H.S., M.M.F. and A.S.; Methodology, M.H.S., M.M.F. and A.S.; Software, M.H.S., M.M.F. and A.S.; Validation, M.H.S., M.M.F. and A.S.; Formal analysis, M.H.S., M.M.F. and A.S.; Investigation, M.H.S., M.M.F. and A.S.; Writing—original draft, M.H.S., M.M.F. and A.S.; Writing—review & editing, M.H.S., M.M.F. and A.S.; Visualization, M.H.S., M.M.F. and A.S. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Data Availability Statement

Data is available upon a request to the authors.

Conflicts of Interest

The authors declare no conflict of interest.

Appendix A

Here, an appendix is presented for several fault results. These faults are LL fault, LL-G fault, LLL fault and LLL-G fault. The max singular values of FRFT-SVD results at various SNRs for direct and filtered signals under LL fault, LL-G fault, LLL fault, and LLL-G fault scenarios are depicted in Table A1, Table A2, Table A3 and Table A4, respectively. The results in these tables confirm that the variations of SNR values have no impact on the max singular value of the FRFT-SVD.
Table A1. Max singular value of FRFT-SVD results at various SNRs for direct and filtered signals under LL fault scenario.
Table A1. Max singular value of FRFT-SVD results at various SNRs for direct and filtered signals under LL fault scenario.
SNR = 15 dBSNR = 20 dBSNR = 25 dBSNR = 30 dB
Location (km)DirectFilteredDirectFilteredDirectFilteredDirectFiltered
102,783,9552,783,9542,783,9522,783,9522,783,9532,783,9512,783,9522,783,951
201,216,5311,216,5321,216,5301,216,5331,216,5321,216,5311,216,5311,216,532
30773,253773,252773,250773,253773,253773,253773,253773,253
40635,422635,421635,422635,424635,422635,422635,422635,420
50557,560557,565557,561557,563557,566557,562557,560557,561
60418,326418,323418,321418,322418,326418,326418,3264,183,262
70366,330366,331366,333366,330366,330366,330366,330366,330
80358,422358,421358,420358,422358,423358,424358,420358,422
90283,721283,722283,721283,723283,720283,721283,720283,721
100279,220279,221279,223279,222279,224279,221279,220279,221
110248,230248,231248,230248,231248,230248,232248,231248,230
120228,880228,882228,882228,881228,880228,883228,880228,881
130205,200205,201205,201205,200205,200205,200205,200205,200
140189,931189,930189,932189,931189,932189,933189,931189,930
150177,536177,534177,531177,533177,536177,531177,534177,532
160167,320167,322167,320167,320167,320167,322167,321167,320
170158,223158,220158,223158,223158,223158,223158,223158,223
180148,880248,231248,230248,230248,230248,230248,230248,230
190147,310147,313147,311147,313147,311147,315147,310147,313
Table A2. Max singular value of FRFT-SVD results at various SNRs for direct and filtered signals under LL-G fault scenario.
Table A2. Max singular value of FRFT-SVD results at various SNRs for direct and filtered signals under LL-G fault scenario.
SNR = 15 dBSNR = 20 dBSNR = 25 dBSNR = 30 dB
Location (km)DirectFilteredDirectFilteredDirectFilteredDirectFiltered
102,874,5842,874,5852,874,5802,874,5812,874,5822,874,5832,874,5842,874,585
201,317,2101,317,2131,317,2131,317,2101,317,2111,317,2101,317,2121,317,210
30782,500782,501782,502782,501782,500782,500782,502782,503
40662,530662,532662,533662,530662,533662,530662,531662,530
50624,440624,442624,442624,443624,441624,445624,440624,442
60437,210437,211437,210437,210437,212437,212437,210437,213
70382,501382,503382,502382,500382,503382,501382,502382,501
80368,521368,522368,520368,521368,520368,521368,520368,521
90288,823288,820288,821288,822288,823288,820288,823288,821
100276,791276,792276,790276,792276,793276,790276,790276,791
110241,230241,233241,232241,230241,232241,230241,231241,230
120228,880228,883228,882228,881228,883228,883228,882228,881
130215,200215,201215,202215,204215,201215,202215,203215,200
140187,011187,013187,013187,010187,014187,011187,010187,012
150195,012195,010195,010195,011195,012195,013195,012195,010
160168,432168,430168,431168,432168,430168,432168,433168,431
170157,882157,883157,880157,882157,882157,881157,883157,881
180151,230151,231151,230151,233151,230151,232151,230151,232
190148,001148,003148,001148,002148,003148,002148,000148,001
Table A3. Max singular value of FRFT-SVD results at various SNRs for direct and filtered signals under LLL fault scenario.
Table A3. Max singular value of FRFT-SVD results at various SNRs for direct and filtered signals under LLL fault scenario.
SNR = 15 dBSNR = 20 dBSNR = 25 dBSNR = 30 dB
Location (km)DirectFilteredDirectFilteredDirectFilteredDirectFiltered
102,938,6002,938,6022,938,6012,938,6022,938,6022,938,6012,938,6032,938,602
201,469,30014,693,0331,469,3031,469,3021,469,3011,469,3021,469,3031,469,301
30979,520979,523979,5229,795,210979,521979,521979,522979,521
40734,640734,643734,641734,642734,642734,641734,642734,640
50587,690587,694587,691587,691587,691587,691587,692587,691
60489,740489,745489,742489,741489,742489,742489,741489,740
70419,770419,772419,771419,772419,771419,772419,771419,770
80367,300367,305367,303367,301367,301367,302367,300367,301
90326,480326,482326,481326,482326,481326,481326,481326,480
100293,820293,823293,821293,821293,821293,821293,820293,821
110267,110267,113267,113267,111267,111267,113267,110267,110
120244,850244,852244,852244,851244,851244,852244,852244,852
130226,010226,013226,013226,012226,011226,011226,010226,011
140209,860209,862209,861209,861209,862209,861209,861209,862
150195,870195,873195,871195,871195,873195,871195,871195,870
160183,620183,621183,622183,621183,622183,621183,621183,622
170172,820172,822172,823172,822172,821172,822172,822172,820
180163,210163,212163,213163,211163,212163,210163,210163,211
190154,610154,615154,612154,611154,613154,611154,612154,611
Table A4. Max singular value of FRFT-SVD results at various SNRs for direct and filtered signals under LLL-G fault scenario.
Table A4. Max singular value of FRFT-SVD results at various SNRs for direct and filtered signals under LLL-G fault scenario.
SNR = 15 dBSNR = 20 dBSNR = 25 dBSNR = 30 dB
Location (km)DirectFilteredDirectFilteredDirectFilteredDirectFiltered
103,134,5033,134,5013,134,5023,134,5013,134,5003,134,5013,134,5033,134,501
201,566,9021,566,9001,566,9011,566,9011,566,9011,566,9021,566,9031,566,900
301,044,4001,044,4011,044,4021,044,4021,044,4011,044,4011,044,4021,044,400
40783,140783,142783,142783,142783,142783,140783,143783,141
50626,370626,373626,373626,372626,372626,372626,373626,372
60521,870521,875521,871521,872521,872521,871521,872521,871
70447,230447,231447,231447,232447,231447,231447,231447,231
80391,250391,251391,252391,253391,251391,252391,250391,251
90347,700347,701347,702347,703347,700347,701347,701347,702
100312,860312,862312,863312,861312,862312,862312,861312,861
110284,360284,362284,362284,361284,362284,362284,362284,361
120260,620260,621260,621260,622260,623260,623260,622260,623
130240,522240,521240,521240,521240,522240,523240,522240,523
140223,290223,293223,292223,293223,291223,293223,292223,292
150208,361208,360208,364208,363208,362208,361208,362208,362
160195,300195,301195,304195,302195,303195,301195,301195,301
170183,770183,770183,773183,771183,772183,771183,771183,772
180173,520173,521173,522173,522173,523173,521173,522173,522
190164,360164,363164,362164,361164,361164,362164,361164,361

Appendix B

Influences of both inception angles and fault resistances on the Max singular values of FRFT-SVD are declared in Appendix B. The considered inception angles are 0°, 45°, 90°, 135°, and 180°. However, the fault resistances accounted for 50 Ω, 100 Ω, 150 Ω and 200 Ω. The results of max singular values of FRFT-SVD for direct and filtered current signals at various faults and inception angles with fault resistances 50 Ω, 100 Ω, 150 Ω and 200 Ω are respectively shown in Table A5, Table A6, Table A7 and Table A8. These results conclude that both inception angles and fault resistances do not affect the proposed algorithm’s performance.
Table A5. Max singular values of FRFT-SVD results for direct and filtered current signals at various faults and inception angles with R = 50 Ω.
Table A5. Max singular values of FRFT-SVD results for direct and filtered current signals at various faults and inception angles with R = 50 Ω.
Inception Angle45°90°135°180°
FaultsLocation (km)DirectFilteredDirectFilteredDirectFilteredDirectFilteredDirectFiltered
LG102,634,6012,634,6032,634,6012,634,6012,634,6042,634,6012,634,6032,634,6012,634,6012,634,601
100263,632263,631263,630263,633263,631263,630263,631263,631263,630263,632
190138,810138,814138,810138,811138,815138,812138,812138,810138,813138,810
LL102,783,9532,783,9522,783,9552,783,9522,783,9582,783,9572,783,9552,783,9522,783,9552,783,953
100279,221279,220279,223279,221279,225279,221279,222279,220279,223279,221
190147,310147,311147,314147,310147,312147,316147,311147,310147,314147,312
LL-G102,874,5842,874,5852,874,5862,874,5842,874,5882,874,5802,874,5812,874,5842,874,5832,874,580
100276,791276,793276,791276,792276,795276,793276,790276,791276,790276,792
190148,000148,004148,001148,005148,003148,007148,002148,001148,003148,001
LLL102,938,6012,938,6032,938,6002,938,6002,938,6022,938,6052,938,6012,938,6002,938,6002,938,600
100293,822293,821293,823293,820293,821293,825293,822293,824293,820293,823
190154,610154,612154,610154,610154,613154,616154,613154,611154,613154,611
LLL-G103,134,5033,134,5023,134,5033,134,5033,134,5033,134,5003,134,5033,134,5033,134,5033,134,503
100312,864312,860312,860312,860312,862312,867312,862312,860312,863312,862
190164,364164,360164,360164,360164,361164,368164,361164,363164,360164,363
Table A6. Max singular values of FRFT-SVD results for direct and filtered current signals at various faults and inception angles with R = 100 Ω.
Table A6. Max singular values of FRFT-SVD results for direct and filtered current signals at various faults and inception angles with R = 100 Ω.
Inception Angle45°90°135°180°
FaultsLocation (km)DirectFilteredDirectFilteredDirectFilteredDirectFilteredDirectFiltered
LG102,634,6022,634,6012,634,6002,634,6032,634,6022,634,6052,634,6012,634,6032,634,6042,634,603
100263,633263,631263,632263,635263,632263,636263,633263,634263,631263,632
190138,811138,812138,811138,814138,812138,816138,810138,812138,811138,813
LL102,783,9512,783,9532,783,9522,783,9512,783,9592,783,9502,783,9522,783,9542,783,9552,783,956
100279,222279,220279,222279,224279,225279,227279,222279,221279,220279,221
190147,313147,310147,313147,312147,313147,318147,311147,310147,313147,314
LL-G102,874,5842,874,5822,874,5832,874,5812,874,5872,874,5802,874,5832,874,5842,874,5812,874,580
100276,792276,791276,790276,791276,797276,795276,794276,791276,790276,792
190148,001148,004148,002148,005148,009148,002148,003148,005148,004148,002
LLL102,938,6022,938,6032,938,6022,938,6022,938,6052,938,6072,938,6012,938,6012,938,6022,938,603
100293,821293,82429,382293,821293,825293,828293,825293,820293,822293,821
190154,613154,611154,613154,614154,614154,616154,612154,615154,612154,614
LLL-G103,134,5053,134,5033,134,5053,134,5053,134,5023,134,5013,134,5023,134,5033,134,5023,134,501
100312,861312,860312,863312,864312,865312,869312,8643,128,610312,861312,863
190164,362164,365164,363164,362164,366164,361164,364164,362164,362164,361
Table A7. Max singular values of FRFT-SVD results for direct and filtered current signals at various faults and inception angles with R = 150 Ω.
Table A7. Max singular values of FRFT-SVD results for direct and filtered current signals at various faults and inception angles with R = 150 Ω.
Inception Angle45°90°135°180°
FaultsLocation (km)DirectFilteredDirectFilteredDirectFilteredDirectFilteredDirectFiltered
LG102,634,6012,634,6052,634,6022,634,6042,634,6042,634,6012,634,6042,634,6042,634,6042,634,605
100263,631263,632263,631263,632263,635263,638263,635263,631263,631263,631
190138,813138,810138,813138,815138,818138,817138,812138,812138,811138,815
LL102,783,9512,783,9542,783,9542,783,9552,783,9542,783,9502,783,9542,783,9522,783,9542,783,955
100279,222279,221279,224279,223279,223279,220279,225279,223279,222279,221
190147,313147,312147,318147,312147,315147,315147,314147,311147,312147,313
LL-G102,874,58128,745,8342,874,5842,874,5852,874,5882,874,5852,874,5852,874,5812,874,5832,874,582
100276,791276,792276,795276,793276,795276,794276,792276,792276,790276,791
190148,003148,005148,001148,005148,008148,007148,003148,000148,002148,001
LLL102,938,6032,938,6042,938,6002,938,6052,938,6072,938,6092,938,6032,938,6022,938,6022,938,601
100293,822293,821293,820293,823293,826293,824293,824293,821293,821293,823
190154,611154,610154,610154,610154,610154,612154,612154,613154,611154,612
LLL-G103,134,5013,134,5033,134,5043,134,5033,134,5023,134,5033,134,5073,134,5053,134,5033,134,502
100312,863312,860312,864312,862312,866312,865312,864312,860312,861312,864
190164,364164,362164,363164,364164,367164,365164,365164,360164,363164,362
Table A8. Max singular values of FRFT-SVD results for direct and filtered current signals at various faults and inception angles with R = 200 Ω.
Table A8. Max singular values of FRFT-SVD results for direct and filtered current signals at various faults and inception angles with R = 200 Ω.
Inception Angle45°90°135°180°
FaultsLocation (km)DirectFilteredDirectFilteredDirectFilteredDirectFilteredDirectFiltered
LG102,634,6012,634,6032,634,6022,634,6012,634,6082,634,6032,634,6042,634,6012,634,6012,634,602
100263,631263,632263,632263,634263,636263,635263,632263,635263,633263,631
190138,814138,811138,813138,810138,817138,812138,812138,814138,811138,810
LL102,783,9532,783,9532,783,9552,783,9542,783,9502,783,9552,783,9552,783,9552,783,9552,783,953
100279,222279,223279,222279,225279,226279,223279,223279,222279,222279,220
190147,313147,311147,315147,313147,317147,314147,310147,315147,314147,314
LL-G102,874,5852,874,5812,874,5842,874,5842,874,5892,874,5842,874,5842,874,5842,874,5872,874,584
100276,790276,792276,791276,791276,798276,793276,791276,793276,798276,793
190148,000148,001148,003148,004148,008148,001148,005148,001148,001148,005
LLL102,938,6032,938,6052,938,6042,938,6052,938,6072,938,6042,938,6022,938,6022,938,6042,938,603
100293,820293,823293,820293,822293,820293,823293,823293,820293,820293,822
190154,614154,610154,611154,610154,615154,612154,610154,614154,614154,611
LLL-G103,134,5033,134,5013,134,5033,134,5033,134,5033,134,5013,134,5033,134,5033,134,5053,134,502
100312,862312,864312,864312,861312,863312,862312,863312,862312,864312,861
190164,362164,361164,365164,364164,369164,362164,360164,363164,361164,361

Appendix C

In this appendix, the maximum singular and its scaled values of FRFT-SVD at 19 different location values are investigated. These values are utilized for curve fitting to get a proper formula of fault locations. Accordingly, the maximum singular and its scaled values at 19 locations for LL fault, LL-G fault, LLL fault and LLL-G fault are declared in Table A9, Table A10, Table A11 and Table A12, respectively.
Table A9. The maximum singular and its scaled values for LL fault at 19 locations.
Table A9. The maximum singular and its scaled values for LL fault at 19 locations.
Location (km)Max Singular ValueMax Scaled Singular Value
102,783,9551
201,392,5000.436979
30928,6400.277753
40696,7200.228244
50557,5600.200276
60464,7800.150263
70398,5100.131586
80348,8100.128746
90310,1500.101913
100279,2200.100296
110253,9100.089165
120232,8200.082214
130214,9700.073708
140199,6700.068223
150186,4100.063771
160174,8000.060102
170164,5600.056834
180155,4600.053478
190147,3100.052914
Table A10. The maximum singular and its scaled values for LL-G fault at 19 locations.
Table A10. The maximum singular and its scaled values for LL-G fault at 19 locations.
Location (km)Max Singular ValueMax Scaled Singular Value
102,874,5841
201,407,2100.489535
30982,5000.341789
40699,5300.24335
50624,4400.217228
60497,2100.172968
70399,5010.138977
80368,5210.1282
90320,1500.111373
100279,9910.097402
110298,2300.103747
120238,8800.083101
130215,2000.074863
140199,7110.069475
150195,0120.06784
160178,4320.062072
170167,8820.058402
180151,2300.052609
190148,0010.051486
Table A11. The maximum singular and its scaled values for LLL fault at 19 locations.
Table A11. The maximum singular and its scaled values for LLL fault at 19 locations.
Location (km)Max Singular ValueMax Scaled Singular Value
102,938,6001
201,469,3000.500000
30979,5200.333329
40734,6400.249997
50587,6900.19999
60489,7400.166658
70419,7700.142847
80367,3000.124991
90326,4800.111101
100293,8200.099986
110267,1100.090897
120244,8500.083322
130226,0100.076911
140209,8600.071415
150195,8700.066654
160183,6200.062486
170172,8200.05881
180163,2100.05554
190154,6100.052613
Table A12. The maximum singular and its scaled values for LLL-G fault at 19 locations.
Table A12. The maximum singular and its scaled values for LLL-G fault at 19 locations.
Location (km)Max Singular ValueMax Scaled Singular Value
103,134,5001
201,566,9000.499888
301,044,4000.333195
40783,1400.249845
50626,3700.199831
60521,8700.166492
70447,2300.14268
80391,2500.124821
90347,7000.110927
100312,8600.099812
110284,3600.090719
120260,6200.083146
130240,5200.076733
140223,2900.071236
150208,3600.066473
160195,3000.062307
170183,7700.058628
180173,5200.055358
190164,3600.052436

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Figure 1. A 500 kV transmission line in Egypt with a 200 km-long line.
Figure 1. A 500 kV transmission line in Egypt with a 200 km-long line.
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Figure 2. Tower configuration and conductor arrangements.
Figure 2. Tower configuration and conductor arrangements.
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Figure 3. Simulated OHTL model.
Figure 3. Simulated OHTL model.
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Figure 4. Sending end signals LG/Phase at different location, fault resistance, and inception angles. (a). (LG)/Phase a at 190 km. (b). (LG)/Phase a at different locations. (c). (LG)/phase a at different fault resistances. (d). (LG)/Phase a at different inception angles.
Figure 4. Sending end signals LG/Phase at different location, fault resistance, and inception angles. (a). (LG)/Phase a at 190 km. (b). (LG)/Phase a at different locations. (c). (LG)/phase a at different fault resistances. (d). (LG)/Phase a at different inception angles.
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Figure 5. The block diagram for the proposed method.
Figure 5. The block diagram for the proposed method.
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Figure 6. The best fitting curve at 19 fault locations for LG fault using scaled maximum singular value.
Figure 6. The best fitting curve at 19 fault locations for LG fault using scaled maximum singular value.
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Figure 7. The best fitting curve at 19 fault locations for LL fault using scaled maximum singular value.
Figure 7. The best fitting curve at 19 fault locations for LL fault using scaled maximum singular value.
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Figure 8. The best fitting curve at 19 fault locations for LL-G fault using scaled maximum singular value.
Figure 8. The best fitting curve at 19 fault locations for LL-G fault using scaled maximum singular value.
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Figure 9. The best fitting curve at 19 fault locations for LLL fault using scaled maximum singular value.
Figure 9. The best fitting curve at 19 fault locations for LLL fault using scaled maximum singular value.
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Figure 10. The best fitting curve at 19 fault locations for LLL-G fault using scaled maximum singular value.
Figure 10. The best fitting curve at 19 fault locations for LLL-G fault using scaled maximum singular value.
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Table 1. The main parameters of the power line.
Table 1. The main parameters of the power line.
ItemsValue
Line voltage (r.m.s) in kV500
Line length in km200
Tower circuit No.1
Sub-conductors per phase No.3
Ground wires No.2
Sub-conductor diameter in mm30.6
Spacing between sub-conductor in phase in cm47
Span in meters400
Diameter of ground wire in mm11.02
Table 2. Max singular value of FRFT-SVD results at various SNRs for direct and filtered signals under LG fault scenario.
Table 2. Max singular value of FRFT-SVD results at various SNRs for direct and filtered signals under LG fault scenario.
SNR = 15 dBSNR = 20 dBSNR = 25 dBSNR = 30 dB
Location (km)DirectFilteredDirectFilteredDirectFilteredDirectFiltered
102,634,6002,634,6022,634,6012,634,6012,634,6032,634,6012,634,6022,634,601
201,317,4001,317,4041,317,4011,317,4011,317,4021,317,4011,317,4031,317,401
30878,350878,356878,353878,352878,351878,351878,351878,352
40658,810658,813658,813658,813658,812658,812658,812658,811
50527,090527,093527,091527,091527,091527,092527,092527,091
60439,270439,275439,272439,273439,273439,271439,271439,272
70376,540376,542376,543376,541376,542376,542376,544376,542
80329,500329,503329,501329,502329,501329,501329,502329,501
90292,910292,914292,911292,911292,911292,911292,913292,912
100263,630263,631263,634263,631263,632263,633263,631263,631
110239,680239,682239,683239,681239,681239,682239,682239,681
120219,710219,711219,712219,712219,712219,712219,712219,712
130202,820202,822202,821202,821202,822202,821202,821202,821
140188,340188,346188,341188,341188,343188,343188,341188,342
150175,800175,801175,802175,802175,801175,802175,802175,801
160164,820164,821164,823164,824164,822164,821164,823164,821
170155,130155,133155,132155,131155,131155,132155,132155,132
180146,520146,521146,523146,523146,521146,523146,522146,521
190138,810138,811138,810138,812138,811138,811138,810138,811
Table 3. Max singular values of FRFT-SVD results for direct and filtered current signals at various faults and inception angles with R = 10 Ω.
Table 3. Max singular values of FRFT-SVD results for direct and filtered current signals at various faults and inception angles with R = 10 Ω.
Inception Angle45°90°135°180°
FaultsLocation (km)DirectFilteredDirectFilteredDirectFilteredDirectFilteredDirectFiltered
LG102,634,6002,634,6012,634,6022,634,6002,634,6052,634,6072,634,6022,634,6032,634,6012,634,601
100263,630263,631263,633263,631263,630263,633263,631263,634263,630263,632
190138,810138,812138,811138,813138,812138,818138,810138,812138,810138,811
LL102,783,9552,783,9552,783,9542,783,9552,783,9532,783,9592,783,9552,783,9552,783,9552,783,955
100279,220279,221279,223279,220279,226279,220279,220279,223279,225279,223
190147,310147,310147,314147,310147,315147,313147,311147,313147,310147,313
LL-G102,874,5842,874,5842,874,5842,874,5852,874,5842,874,5882,874,5842,874,5842,874,5842,874,584
100276,791276,793276,791276,791276,796276,795276,791276,790276,791276,792
190148,001148,004148,000148,004148,004148,006148,001148,000148,004148,001
LLL102,938,6002,938,6022,938,6012,938,6042,938,6022,938,6072,938,6002,938,6002,938,6012,938,600
100293,820293,821293,820293,823293,821293,823293,8202,938,255293,821293,821
190154,610154,611154,611154,612154,613154,618154,610154,610154,615154,612
LLL-G103,134,5033,134,5033,134,5023,134,5033,134,5003,134,5023,134,5033,134,5033,134,5043,134,503
100312,860312,861312,861312,860312,862312,864312,860312,863312,861312,860
190164,360164,363164,362164,360164,364164,361164,361164,362164,360164,363
Table 4. The maximum singular and its scaled values for LG fault at 19 locations.
Table 4. The maximum singular and its scaled values for LG fault at 19 locations.
Location (km)The Max Singular ValueMax Scaled Singular Value
102,634,6001
201,317,4000.500038
30878,3500.33339
40658,8100.250061
50527,0900.200065
60439,2700.166731
70376,5400.142921
80329,5000.125066
90292,9100.111178
100263,6300.100065
110239,6800.090974
120219,7100.083394
130202,8200.076983
140188,3400.071487
150175,8000.066727
160164,8200.06256
170155,1300.058882
180146,5200.055614
190138,8100.052687
Table 5. Actual (A in km) and predicted (P in km) fault locations under LG fault scenario.
Table 5. Actual (A in km) and predicted (P in km) fault locations under LG fault scenario.
A (km)1030507090100120140160180190
P for Fit 1 (km)10.534030.43250.51270.62190.456100.614120.685140.752160.782180.742190.852
P for Fit 2 (km)10.321130.31250.46870.42590.562100.568120.536140.568160.311180.541190.752
P for Fit 3 (km)10.124230.21250.26570.35990.255100.352120.425140.425160.456180.342190.425
P for Fit 4 (km)10.118130.10250.12070.13090.125100.129120.235140.254160.352180.213190.246
P for Fit 5 (km)10.001030.002450.00270.002590.001100.002120.0022140.002160.003180.003190.003
Table 6. LG fault prediction error utilizing line current signals.
Table 6. LG fault prediction error utilizing line current signals.
A (km)1030507090100120140160180190AE (%)
error for Fit 1 (%)0.2670.2160.2560.31050.2280.3070.34250.3760.3910.3940.4260.319455
error for Fit 2 (%)0.16050.1560.2340.21250.2810.2840.2680.2840.15550.27050.3760.243818
error for Fit 3 (%)0.0620.1060.13260.17950.12750.1760.21250.21250.2280.1710.21250.165464
error for Fit 4 (%)0.0590.0510.060.0650.06250.06450.11750.1270.1760.10650.1230.092000
error for Fit 5 (%)0.00050.00120.0010.001250.00050.0010.00110.0010.00150.00150.00150.001095
Table 7. Actual (A in km) and predicted (P in km) fault locations under LL fault scenario.
Table 7. Actual (A in km) and predicted (P in km) fault locations under LL fault scenario.
A (km)1030507090100120140160180190
P for Fit 1 (km)10.482030.52350.62370.52890.711100.692120.695140.723160.722180.823190.722
P for Fit 2 (km)10.210130.42350.53270.41190.545100.525120.568140.622160.569180.623190.625
P for Fit 3 (km)10.151230.19850.22570.32590.456100.352120.458140.352160.355180.456190.425
P for Fit 4 (km)10.143230.11250.11070.15690.211100.125120.356140.258160.211180.254190.215
P for Fit 5 (km)10.001130.003150.002370.00290.0034100.003120.0021140.0021160.003180.0031190.0035
Table 8. LL fault prediction error.
Table 8. LL fault prediction error.
A (km)1030507090100120140160180190AE (%)
error for Fit 1 (%)0.2410.26150.31150.2640.35550.3460.34750.36150.3610.41150.3610.329273
error for Fit 2 (%)0.105050.21150.2660.20550.27250.26250.2840.3110.28450.31150.31250.256959
error for Fit 3 (%)0.07560.0990.11250.16250.2280.1760.2290.1760.17750.2280.21250.1706
error for Fit 4 (%)0.07160.0560.0550.0780.10550.06250.1780.1290.10550.1270.10750.097782
error for Fit 5 (%)0.000550.001550.001150.0010.00170.001250.001050.001050.00150.001550.001750.001282
Table 9. Actual (A in km) and predicted (P in km) fault locations under LL-G fault scenario.
Table 9. Actual (A in km) and predicted (P in km) fault locations under LL-G fault scenario.
A (km)1030507090100120140160180190
P for Fit 1 (km) 10.491030.72550.56170.56890.774100.621120.685140.711160.799180.759190.812
P for Fit 2 (km)10.321430.52650.45870.45290.538100.435120.533140.652160.653180.612190.625
P for Fit 3 (km)10.124530.352450.28870.40190.456100.211120.355140.433160.436180.355190.356
P for Fit 4 (km)10.139530.18250.12470.12890.364100.178120.244140.311160.235180.215190.282
P for Fit 5 (km)10.001230.00250.003270.002990.00296100.003120.002140.0025160.0028180.003190.0031
Table 10. LL-G fault prediction error.
Table 10. LL-G fault prediction error.
A (km)1030507090100120140160180190AE (%)
error for Fit 1 (%)0.24550.36250.28050.2840.3870.31050.34250.35550.39950.37950.4060.341182
error for Fit 2 (%)0.16070.2630.2290.2260.2690.21750.26650.3260.32650.3060.31250.263882
error for Fit 3 (%)0.062250.17620.1440.20050.2280.10550.17750.21650.2180.17750.1780.171268
error for Fit 4 (%)0.069750.0910.0620.0640.1820.0890.1220.15550.11750.10750.1410.109205
error for Fit 5 (%)0.00060.0010.00160.001450.001480.00150.0010.001250.00140.00150.001550.001303
Table 11. Actual (A in km) and predicted (P in km) fault locations under LLL fault scenario.
Table 11. Actual (A in km) and predicted (P in km) fault locations under LLL fault scenario.
A (km)1030507090100120140160180190
P for Fit 1 (km) 10.621230.52650.78570.75290.744100.511120.752140.811160.823180.835190.851
P for Fit 2 (km)10.425130.42550.52470.52690.524100.325120.652140.720160.652180.653190.666
P for Fit 3 (km)10.252030.23650.41170.45690.411100.235120.532140.511160.328180.422190.513
P for Fit 4 (km)10.174030.12550.3570.19690.354100.133120.356140.325160.311180.341190.283
P for Fit 5 (km)10.002130.002650.002970.00390.0029100.0035120.003140.003160.0034180.0032190.0035
Table 12. LLL fault prediction error.
Table 12. LLL fault prediction error.
A (km)1030507090100120140160180190AE (%)
error for Fit 1 (%)0.31060.2630.39250.3760.3720.25550.3760.40550.41150.41750.42550.364145
error for Fit 2 (%)0.21250.21250.2620.2630.2620.16250.3260.360.3260.32650.3330.276909
error for Fit 3 (%)0.1260.1180.20550.2280.20550.11750.2660.25550.1640.2110.25650.195773
error for Fit 4 (%)0.0870.06250.1750.0980.1770.06650.1780.16250.15550.17050.14150.134000
error for Fit 5 (%) 0.001050.00130.001450.00150.001450.001750.00150.00150.00170.00160.001750.001505
Table 13. Actual (A in km) and predicted (P in km) fault locations under LLL-G fault scenario.
Table 13. Actual (A in km) and predicted (P in km) fault locations under LLL-G fault scenario.
A (km)1030507090100120140160180190
P for Fit 1 (km) 10.645330.64250.78570.79890.755100.533120.811140.821160.831180.842190.896
P for Fit 2 (km) 10.493230.49850.42970.65290.623100.325120.652140.711160.599180.711190.756
P for Fit 3 (km)10.424130.32450.35970.42190.418100.253120.425140.536160.458180.635190.424
P for Fit 4 (km)10.324230.11050.19270.19990.212100.172120.352140.324160.352180.361190.213
P for Fit 5 (km)10.001520.003250.00370.003290.0036100.003120.0035140.0034160.0036180.0035190.004
Table 14. LLL-G fault prediction error.
Table 14. LLL-G fault prediction error.
A (km)1030507090100120140160180190AE (%)
error for Fit 1 (%)0.322650.3210.39250.3990.37750.26650.40550.41050.41550.4210.44800.379968
error for Fit 2 (%)0.24660.2490.21450.3260.31150.16250.3260.3550.29950.35550.37800.293100
error for Fit 3 (%)0.212050.1620.17950.21050.2090.12650.21250.2680.2290.31750.21200.212595
error for Fit 4 (%)0.16210.0550.0960.09950.1060.0860.1760.1620.1760.18050.10650.127782
error for Fit 5 (%)0.000750.00160.00150.00160.00180.00150.001750.00170.00180.001750.00200.001614
Table 15. Validation of the proposed algorithm compared to literature work in [9,11,12,35].
Table 15. Validation of the proposed algorithm compared to literature work in [9,11,12,35].
Literature & Proposed WorkMethodsMaximum Percentage Error (%)Average Percentage Error (%)
[9]PCA0.32170.1921
[11]CNN0.04970.03670
[12]ANN0.45220.2375
[35]MCSVM0.08320.06790
The ProposedFRFT-SVD0.00200.001614
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Saad, M.H.; Fouda, M.M.; Said, A. A New Method of Fault Localization for 500 kV Transmission Lines Based on FRFT-SVD and Curve Fitting. Energies 2023, 16, 758. https://doi.org/10.3390/en16020758

AMA Style

Saad MH, Fouda MM, Said A. A New Method of Fault Localization for 500 kV Transmission Lines Based on FRFT-SVD and Curve Fitting. Energies. 2023; 16(2):758. https://doi.org/10.3390/en16020758

Chicago/Turabian Style

Saad, Mohamed H., Mostafa M. Fouda, and Abdelrahman Said. 2023. "A New Method of Fault Localization for 500 kV Transmission Lines Based on FRFT-SVD and Curve Fitting" Energies 16, no. 2: 758. https://doi.org/10.3390/en16020758

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