PROTECTION DEVICE FOR HIGH RESISTANCE GROUND FAULTS

Abstract: Protection device for high resistance ground faults in a power network the fault detection principle of which is based on an indirect study of non-harmonic frequency compo­ nents of the phase currents. When such a fault has occurred, a considerable change of the energy contents of these fre­ quency current components arises. This change can be de­ tected by the device according to the invention. If by com­ parison (4e) between digitized input signals (I′) and a har­ monic Fourier model (4d) of the same signals, i.e. genera­ tion of the residuals of the system, it is found that a dif­ ference exists, and if the corresponding loss function V N (4f) for a certain time exceeds a lower limit value - all on condition that a zero sequence current (I O ) exists - then the device indicates a high resistance ground fault on any of the phases of the network.

Description: The invention relates to a protection device for high resistance ground faults according to the precharacterising part of Claim 1. The type of fault that is defined by the term "high resistance faults" occurs, for example, when a tree has fallen over the conducting wires of a transmission line and arcing arises as a result of sparkover to the vegetation. An other example is a broken or fallen conducting primary wire which is brought into contact with the ground and thereby causes a ground fault condition. Because of the high contact resistance which normally exists during faults of the above kind, the fault current is small and therefore often negligible. This also means that it will be difficult to reliably separate such faults from large load changes in the network. A consequence of this is that a high resistance fault may remain during a long period of time causing fire hazard and hazards to humans who come into contact with or in the vicinity of the conductor. Usually, this type of fault is discovered only during the continuous routine inspection of the conductor. Ever since the childhood of electrical engineering, it has been a desire to be able to detect the type of fault described above. Consequently, there have been a large number of different approaches to solve this problem. One of the reasons for this is that the neutral point of the networks in relation to ground is treated in different ways. Keeping pace with the general technical development, the technical solutions to this problem have also undergone great changes. Previous classical, analog solution principles have nowadays given way to more or less sophisticated solutions based on digital data processing techniques performed by computers, approximation of measured signal values to mathematical functions, estimation of parameters included, numerical technique and statistical methods. The state of the art will be described on the basis of the protection devices which have been developed during the last few years, based on computer technique. It is self-evident that it is desirable to be able to detect high resistance ground faults with resistance values as great as possible. By pure definition, the limit to what may be considered a high resistance fault seems to be somewhat vague. This is a consequence partly of the limits that are detectable in practice and partly of the additional requirements which are often placed on these protection devices. In addition to the desire to detect a high resistance fault, it is also desired to know in what direction the fault is located in relation to an outgoing measuring point and, if possible, the distance between the measuring point and the fault location. The types of faults described above often give rise to ground fault resistances of the order of magnitude of 5-10 kΩ. However, in IEEE Proceedings, Vol. 130, pt. C, No. 6, November 1983, page 306, in an article by Yang, Morrison and Eng entitled "Microprocessor-Based Algorithm for High-Resistance Earth-Fault Distance Protection", it is stated that a maximally allowed upper limit to a ground fault is 200Ω if it is also desired to determine the distance to the fault. In an article entitled "A Microprocessor-Based Technique for Detection of High Impedance Faults" by Balser, Clements and Lawrence, published in IEEE Trans. on PWRD, Vol. PWRD-1, No. 3, July 1986, it is stated, however, that a fault representing a considerably higher resistance can be discovered. This indicates that it should be simple to discover a fault but that it is a problem to find a model which enables the determination of the fault distance. For the protection device that is intended to react to low-ohmic faults the problem of protection can be approached in two essentially different ways. The first way makes use of a physical model of the system to be protected. This can be set up by applying Kirchhoff's laws. This leads to a relation between the different currents and voltages in the form of impedance and admittance matrices for the system. In an article by Thorp, Phadke, Horowitz and Beehler entitled "Limits to Impedance Relaying", published in IEEE Trans. on PAS, Vol. PAS-98, No. 1, January/February 1979, pp. 240-60, it has been described, however, that there are considerable limitations to structures which are based on impedance models. The second basic way to tackle the problem, used knowledge of the structure of the signals in the system to adapt some function to the measured values. This can be carried out by approximating the signal with a combination of mathematical functions. In, for example, an article entitled "A New Filtering Based Digital Distance Relay" by Girgis, published in IEEE Trans. on PAS, Vol. PAS-101, No. 9, September 1982, pp. 3471-80 and in an article entitled "Fundamental Bases for Distance Relaying with Symmetrical Components" by Phadke, Ibrahim and Hlibka in IEEE Trans. on PAS, Vol. PAS-96, No. 92, March/April 1977, pp. 635, 46, each individual signal is represented by truncated Fourier series. When successively measured values exist, the coefficients of the signal can be estimated by applying recursive algorithms. However, when the value of the fault impedance is large, problems may arise in discovering the differences between the different phase quantities. This is mostly due to the limited resolution in the implementation with a limited word length. Owing to this fact, there are advantages in estimating the Fourier components for a suitable combination of the current quantities instead of the individual phase quantities. Protection devices which are designed to operate when high resistance ground faults arise are designed in several different ways. Most conventional methods which are described in patent literature are based on impedance models for the transmission line. This may be a doubtful philosophy of approach since impedance for sinusoidal signals is really only defined for stationary conditions. During the transient condition initiated by a fault, on the other hand, the information is limited and it may therefore be difficult to carry out the analysis in the impedance plane. The measurement errors which arise in connection with high resistance ground faults are therefore particularly pronounced. The disadvantages of the impedance plane analysis have been described by Phadke, Ibrahim and Hlibka in the article cited above. One way of avoiding the problems mentioned above has been investigated by an analog implementation in the SE-A-81300787.9 (based on European patent application 81 30 0787 published as EP-A-0 035 365), where a method is described based on utilizing the propagation of travelling waves along the transmission line. Such algorithms manage to treat the transient phenomena but must be complemented with conventional distance and overcurrent relays to be able to be applied during stationary conditions. The effectiveness of the concept thus obtained has proved to be considerably higher than in corresponding impedance methods. However, since the method is, in principle, a transient-sensing method, it may be hazardous to base a decision about extremely great high resistance faults on this method. GB-B-820 428 and SE-B-403 862 describe protective devices for high resistance ground faults which are based on a comparison of the phases at the two end points of a protected section of a transmission line. US-A-4 091 433 describes a device based on the study of symmetrical components instead on the phase quantities themselves. US-A-3 614 534 and CA-A-946 928 describe devices in which the error signals are stored in the form of a magnetic flux in a magnetic core. The described method seems to operate satisfactorily for a fault resistance of the order of magnitude of 2 kΩ. As is clear from the above, quite a large number of methods and devices have been developed to discover high resistance ground faults. However, most of these devices are impedance-based and/or have a discriminating portion which has been implemented by analog technique. In other respects, the standards for how great a high fault resistances should be manageable have changed over the years. It is of the utmost interest to be able to handle as high fault resistances as possible. For this purpose, new methods are required, above all for the analyzing part of the relay unit. A description of the state of the art as regards protection for high resistance faults cannot be considered complete without briefly mentioning two major long-term research projects in the USA, dealing with high impedance ground faults. One of the projects is being carried on at Texas A&M University by order of the Electric Power Institute. An account of this project work by Aucoin and Russel is published in IEEE Trans. on power Apparatus and Systems, Vol. PAS-101, No. 6, June 1982, pp. 1596-606 and is entitled "Distribution High Impedance Fault Detection Utilizing High Frequency Current Components". This projects has been going on for many years and the object has been to investigate the properties of real high impedance faults. Analyses have been made of data gathered from faulted conductors. The detection logic is based on analyzing the energy which is present in current components having a frequency of a higher order. To this end, FFT analysis is applied to obtain the properties of the studied signals from the distribution line. In this connection, individual peaks representing noise are disregarded, and the main interest is concentrated on indicating the cumulative effect of many such peaks during a short period of time. Extensive investigations have been carried out through off-line simulation of collected data. A prototype has also been produced for verifying the methods used in real time. This is based on data being collected with a frequency of 2-10 kHz during one period. These data are then processed with the algorithm which has been produced by simulation studies. The second project is being conducted at The Electric Power Institute as an independent work. Also in this case extensive analyses of collected data from distribution lines in the field have been performed. It has then been found that high resistance faults can be classified into two groups, namely, passive and active. The former originates from such situations where a conductor has broken and thus causes an unbalance in the current which is measured at a substation. The latter type of fault arises when a conductor comes into contact with conducting material and arcing arises. In this case the unbalance occurs not only in the basic component but also in the different harmonic components and primarily in the odd-numbered harmonics. The detection algorithm is thus based on first calculating the Fourier coefficients for the 1 th , 3 th and 5 th harmonics in the phase currents. Thereafter, normalized sequence currents for each harmonic component are calculated. The covariance matrix for the estimations and a statistical test quantity are produced as a basis for the logic handling. In this method, a matrix of the same order of magnitude as the number of estimated parameters is updated. In addition, it is necessary to invert the covariance matrix. These are time-demanding procedures as far as the CPU is concerned, which has a negative effect on the highest possible sampling frequency. In the present situation, therefore, no economically realistic implementation of this algorithm exists. A very important and integral part of the invention, which will now be described, is that a concept, which is described in detail in the SE-A-8702683-7 (corresponds to European patent application 88109961.8 published as EP-A-0 297 418), can also be used, after extension, in a protection device for high impedance faults. The concept according to SE-A-8702683-7 comprises converting a measured signal, obtained from the network, after filtering and digitalization, into an analytical model in the form of a truncated Fourier series, the coefficients of which are determined in a parameter estimator operating with an estimation method in accordance with the least squares method. Starting from model values, according to the concept, calculation of the frequency can be carried out in a frequency estimator, whose output signal, on the one hand, is returned as current frequency value to the parameter estimator and, on the other hand, is a measure of the current frequency, for example for determining the limits to permissible frequency variations. Since the parameter estimation technique is an important and integral part of the invention and since concepts from this technique will be used to describe the invention, a brief summary thereof, based on the technique as described in SE-A-8702683-7, will be given. Current signals can be modelled by: which can be transformed to y(t) = ϑ T  (t) (2) where ϑ T = (a o ,-a o b o , c₁cos d₁,c₁ sin d₁,...c N cos d N c N sin d N ) (3) is a parameter estimation vector and (t) = (1, t, sinω o t, cosω o t, ... sin Nω o t, cos Nω o t) (4) is a regressive vector. Estimation of the parameters according to the least squares method means that the value of a "loss function" V N is minimized. V N can be written as where λ is a forgetting factor and where ε(t) is an estimation error function. The minimization gives the following equation for ϑ(t) The actual estimation is performed recursively with the aid of the following algorithm R(t) = λ · R(t-1) +  (t)  T (t) (7) R(0) = δ · I (8) R(t)L(t) = (t) (9) y (t) = ϑ T (t-1) (t) (10) ε(t) = y(t) - y (t) (11) ϑ (t) = ϑ (t-1) + L(t)ε (t) (12) Here, R(t) is the covariance matrix of the regression vector and P(t), as shown below, is the inverse thereof. Otherwise, the following recurrence formulas will be used: r(t) = P(t-1)  (t) (13) d(t) = λ +  T (t)r(t) (14) L(t) = r(t)/d(t) (15) P(t) = (P(t-1) - r(t)L T (t))/λ (16) P(0) = (1/δ)·I (17) ϑ(O) = ϑ o (18) Another concept, also belonging to the prior art, will be used with the invention now described. For reasons which will be given later on, modal transformations will be applied. Such transformations are described, inter alia, in Proceedings IEEE 113, June 1966, in an article entitled "Study of symmetrical and related components through the theory of linear vector spaces", as well as in the SE-A-8403226-7 (corresponds to European patent application 85107101.9 published as EP-A-0 164 711). In the present invention the possibilities of transforming phase signals to corresponding symmetrical components by an orthogonal transformation matrix are utilized. The invention aims at devising a protection device for high resistance ground faults of the above-mentioned kind which is also sensitive to ground faults with an extremely high fault resistance values unable to be detected with the hitherto technique. To achieve this aim the invention proposes a protection device for high resistance ground faults as defined in Claim 1. Further developments of the invention are characterized by the features of the additional claims. The device according to the invention complies with an important requirement that a tripping signal should not be delivered for unbalanced load currents which originate from unsymmetrical loads. In addition to the protection device being transient sensing, therefore, the invention also comprises a method whereby stationary states are taken into consideration by carrying out static analysis. To this are to be added the usual advantages of numerical technique as compared to pure analog implementation of the relay concept. The invention will now be described in greater detail with reference to the accompanying drawings showing - by way of example - in Figure 1 a preferred design of a protection device, from the hardware point of view, for high resistance ground faults according to the invention, Figure 2 a signal flow chart for a protection device for high resistance ground faults according to the invention. It has been found to be difficult to distinguish a faultless line system from a line system with a high resistance ground fault. However, it has been proved that there is a considerable difference in the harmonic content of the phase currents between the faultless and a faulty state. In the case of high resistance faults, the current signals contain a wide spectrum of different frequency components. It has also been proved that the magnitude of non-harmonic current components, or - as it can also be expressed - the energy contents of these non-harmonic current components, increases by about one hundred times when a high resistance ground fault occurs. In a faultless state, the non-harmonic components in the current signal are completely negligible, independent of the magnitude of the load. In a faultless state, however, the load signals comprise components of harmonic frequencies. Upon a change of load, transient components appear in the current signals, which disappear in the course of a few cycles. The components of non-harmonic frequencies which originate from high resistance ground faults have a longer duration than the harmonic frequency components occurring upon load changes. Taking advantage of these phenomena, the invention is based on the study of non-harmonic frequency components in the current. As has been established, a high resistance ground fault exists on the line when a considerable change or increase in the energy contents of non-harmonic frequency components can be observed and when this change or increase remains at least for a few seconds. However, there will always be a certain uncertainly in the distinction between high resistance ground faults and load changes. It is therefore suitable to use statistical methods for increasing the probability of accurate detection. The Fourier component estimation which is described in SE-A-8702683-7, together with appropriate logic handling, is well adapted to discover faults when the fault impedance is of the order of magnitude of a few hundred ohms. However, when a high resistance fault of a few thousand ohms occurs, such a fault situation cannot be distinguished, using this technique, from the noise that arises as a result of the algorithm used in SE-A-8702683-7 being implemented with a limited word length. One way of avoiding this problem is to work with symmetrical current components by modal transformation, i.e. with zero sequence, positive sequence and negative sequence components. These quantities can be obtained from the phase quantities by a transformation with the aid of an orthogonal transformation matrix. Several such matrices are available. Some of these, however, introduce complex arithmetics which renders the further processing difficult. However, according to a transformation proposed in an article by Dommel and Meyer, entitled "Computation of Electromagnetic Transients" and published in Proc. IEEE, Vol. 62, July 1974, pp. 983-993, the good properties of the symmetrical sequence quantities are retained. This transformation is exemplified here for the phase currents I A , I B , I C according to the following From this matrix it is clear that the modal component I o , i.e. the zero sequence current, can be obtained as the mean value of the phase quantities. This mean value can, of course, also be obtained directly upon measuring, thereby facilitating the hardware implementation of the protection device for high impedance ground. When a symmetrical load is connected to a line, the mean value I o is practically zero. Therefore, a detected zero sequence current is either due to an unsymmetrical load on a faultless line system, or to a fault on the line system. The previously described fault detection principle is therefore applied, although in an indirect manner, as will be described in more detail below, to the zero sequence current. After the occurrence of a high resistance fault, the zero sequence current will exhibit a periodic behaviour, which makes it possible to make a Fourier expansion of the current signal into the fundamental frequency component and the harmonic components. After the occurrence of a fault, the zero sequence current substantially consists of the fundamental frequency component and some contribution from the third and fifth harmonics. However, these harmonic contents are negligible compared with the fundamental frequency component and can be filtered out, for example by taking account of them in the selected model. The logic that is now needed to detect a high resistance fault is based on the study of the Fourier coefficients of I0. First it should be determined whether there is asymmetry, i.e. whether there is an I0 exceeding a certain lower level γ. If this is the case for a longer period of time, either the system has become unsymmetrical or something unusual has occurred. To find out which of these alternatives prevails, a study can be performed of the loss function V N and the instantaneous residuals in the estimation of I0, as described in SE-A-8702683-7. As mentioned previously, I0 can be measured as a combination of the phase currents, whereupon it is available, after conversion to digital representation, to form part of the decision-yielding data. The instantaneous residuals consist of the difference between the measured and thereafter A/D-converted signal for I0 and the signal obtained by the truncated Fourier series expansion. If, after a zero sequence current has been detected, the generated Fourier model is the correct reproduction of the measuring signal, the instantaneous residuals and hence the loss function will exhibit small values, i.e. an asymmetry caused by load asymmetry exists. If, for a certain time Δt, the loss current V N exceeds a certain value η with a duration greater than, for example, t F , this must be due to the selected Fourier model, based on harmonic components, not correctly reproducing the measured signal. This, in turn, can only be due to the measured signal for I o having more than an insignificant content of nonharmonic frequency components, i.e. a high resistance ground fault exists on the line. In addition, it is possible to study the magnitude of the harmonics via corresponding coefficients. The protection of high resistance ground faults should conveniently comprise both, the determination of the faulted phase and the direction to the fault. Phase selection can suitably take place by the study of estimated Fourier components for the phase currents. Since estimated Fourier components for I o must be available for the phase detection technique, it is sufficient to estimate the components for two of the phase currents, for example I A and I B , since estimated components for the third phase current can simply be obtained as I C = 3I o - I A - I B If the protection device is only intended to detect high resistance ground faults, it is not necessary to calculate I₁ and I₂. If the protection device should also be capable of detecting low resistance faults, it may be advantageous to base the analysis on the other two modal quantities I₁ and I₂ and these can be supplied in a simple manner by the shown orthogonal transformation matrix. To obtain as reliable an estimation of the different components as possible, an accurate value of the fundamental frequency in question must be available. This can be conveniently accomplished according to the frequency estimation technique as described in SE-A-8702683-7. This means that an estimation of the frequency components must also be performed for the different corresponding phase voltages U A , U B and U C . By studying the loss function or amplitude of the current harmonics, it can be determined in what phase a fault has occurred. The direction to a fault in relation to a measuring station can be determined by studying the polarity of the instantaneous residuals for, for example, the phase currents for a certain period of time. To get a good general view of the invention, a preferred embodiment of the invention will be described in two different stages. The first stage comprises a suitable structure of the components included from the hardware point of view. The second stage comprises the signal flow paths in a protection device for high resistance ground faults according to the invention. Figure 1 shows the large modules which are connected to form the invention. Analog signals for phase currents and phase voltages are obtained from the network. In classical conventional manner, with the aid of I A , I B and I C , the zero sequence current I o is formed in the summator 1. Conversion to digital quantities I A ′, I B ′, and I O ′ is performed in the A/D converter 2. Conversion of the phase voltages U A , U B and U C to corresponding digital quantities U A ′, U B ′, and U C ′, takes place in the A/D converter 3. The digitized values are processed in the calculating unit 4 to obtain estimated values ϑ and of the Fourier components and the current fundamental wave. With the technique described above, also estimated components for the phase current I C and the positive sequence and negative sequence currents are generated. In addition, a determination of the instantaneous residuals ε and the corresponding values of the loss function V N of the system is performed here. The estimated and generated components and the residuals and the loss function are supplied to the logic unit 5, in which an evaluation is performed in accordance with the fault detection technique described. In this unit, determination of the faulted phase and the direction to the fault is also performed, all according to the method described above. If a high resistance fault has been detected, a trip output signal T, containing information about the direction to the fault and about the faulted phase, is received via a TRIP signal unit 6, to bring the fault to attention and to possibly clear the same. The flow signal chart shown in Figure 2 has as input signal the analog phase currents I A and I B and the zero sequence current I o and the analog signals for the phase voltages. All of these signals are converted to digital representation in the converters 2 and 3. The calculating unit 4 shown in Figure 1 has here been divided into its respective constituents to be able to describe the signal paths. Member 4a supplies estimated values ϑ and I and ϑ and U of the Fourier components according to the incoming digitized current and voltage quantities. The estimated component ϑ and U is supplied to a frequency estimator 4b, whose frequency value ω and is returned to the parameter estimator 4a as a value of the frequency in question. With the aid of the estimated parameters of the incoming currents, ϑ and I , estimated parameter values of the phase current I C and the positive sequence and negative sequence currents, I₁ and I₂, can be determined in member 4c. Since now all estimated components are available, a Fourier model, based on a fundamental frequency and higher harmonic frequencies, can be formed. This is done in member 4d. The residuals of the system, in the form of the difference between digitized values of incoming currents and the model values obtained, are generated with the aid of member 4e. The loss function V N can then be generated in member 4f in accordance with the described known technique. Now all the necessary data are available in order to determine whether a high resistance ground fault exists on any of the phases. For that purpose, it must first be determined whether there is a zero sequence current I o which is greater than a lower limit value ν. Then also the loss function V N , for a longer period of time Δ t than a lower limit value t F , must have a value exceeding also a lower limit value η. If these conditions exists, a TRIP signal can be delivered. In such a fault situation, it is desirable to have knowledge of which phase is the faulted one. Phase selection can be carried out transiently with the aid of the loss function and in steady state by studying the amplitude of the current components having harmonic frequencies. It is also desirable to know in which direction the fault is located in relation to the measuring station. Knowledge of this can contribute to distinguish a high resistance fault from a load change, which may be useful in a complementary analysis. Knowledge of the direction to a fault may be obtained, as also described above, by the study of the polarity of the residuals after the occurrence of a fault. This presupposes the existence of measuring points on both sides of the protected zone and the existence of certain communication facilities between the stations. The general rule then applies that if the currents at both measuring points are directed outwards from the protected zone, the signs of the instantaneous residuals in the faulted phases at the respective measuring points shall be the same if the fault has occurred within the zone. The same criterion of the signs also applies if both currents are directed towards the interior of the protected zone. The fault is also present within the protected zone when the signs are different and when the current at one measuring point is directed towards the interior of the protected zone and the current at the other measuring point is directed away from the measuring point. The sign is determined by integrating the residuals for a certain time beginning at the instant the fault occurs. All of these decisions can be made within the logic unit 5. The indication delivered is given via the TRIP unit 6 with the output signal T. Within the scope of the invention, numerous different hardware embodiments may be used. Also, the logic sequences and decisions can be carried out in many different ways. The principle of protection has been described for a three-phase power network, but may of course, by making minor modifications, be used in multi-phase systems as well.

Claims: Protection device for high resistance ground faults in a multi-phase, preferably three-phase, network for distribution or transmission of electric power, characterised in that the protection device is supplied with analog measurement signals of all phase voltages (U A ,U B ,U C ), of two phase currents (I A ,I B ) and of the zero sequence current (I o ) of the network, the protection device comprising: means (2,3) for conversion of said analog measurement signals into digital signals (U A ′,U B ′,U C ′, I A ′,I B ′,I O ′), means (4a) for estimating, on the basis of the incoming digital signals, the coefficients ( ϑ and I ,ϑ and U ) of a truncated Fourier series approximating a measured analogue signal, means (4b) for estimating the fundamental frequency (ω and) of the network, means (4c) for estimating the coefficients (ϑ and) of truncated Fourier series approximating the third phase current (I C ) and the positive sequence and negative sequence currents (I₁,I₂) of the network, means (4d) for determining the instantaneous values of a truncated Fourier series (I and) with the estimated coefficients, means (4e) for determining the instantaneous residual value (ε = I' - I and ) associated with a truncated Fourier series, i.e. the difference at any particular instant between the measured analog signal and the corresponding value of the truncated Fourier series, means (4f) for determining the instantaneous value of the loss function (V N ) associated with a truncated Fourier series, i.e. the sum at any particular instant of the decreasingly weighted squares of a number of residual values at preceding instants, and a logic unit (5) which delivers, via a trip unit (6), a trip signal (T) indicating the existence of a high resistance ground fault on any of the phases of the network when the following conditions are met simultaneously the zero sequence current (I o ) is greater than a lower limit value (γ) the value of the loss function (V N ) of the zero sequence current (I o ) has remained greater than a predetermined value (η) for a time Δt longer than a predetermined interval (t F ). Protection device according to Claim 1, characterized in that, when a high resistance ground fault has been detected, the logic unit (5) is adapted to distinguish and indicate that phase/those phases which has/have experienced a considerable change of the loss function associated therewith, or which has/have experienced a considerable change of the amplitude of the current components at harmonic frequencies. Protection arrangement comprising two protection devices for high resistance ground faults according to Claim 1, arranged at measuring points on respective ends of a protected line zone, said protection devices being provided with means for determining the current direction at the measuring point, and with communication facilities arranged between said protection devices, wherein, when the protection devices have detected a high resistance ground fault, the logic units determine, by integration of the instantaneous residual values associated with the faulted phase over a certain time from the fault instant, the signs of the residuals and indicate, via the trip unit (6), a fault within the measuring zone when the signs of the residuals associated with the faulted phase are the same at both measuring points and the currents at the measuring points are either both directed outwards from the protected zone or are both directed towards the interior of the protected zone, or when the signs of the residuals at the measuring points are different and the current at one measuring point is directed towards the interior of the protected zone and the current at the other measuring point is directed away from the protected zone.

Inventors: BERGMAN, STEN, LJUNG, STEFAN
Applicants: ASEA BROWN BOVERI AB
Application year: 1988
Main classification: H02H3
IPC codes: G01R31, H02H1, H02H3