PHASE SELECTION FOR GROUND FAULT

Abstract: A method and a device for phase selection for single-pole tripping of high-impedance ground faults in direct grounded power networks. Starting from the ratio of the negative-sequence voltage to the zero-sequence current (U2/I0) and the ratio of the negative-sequence voltage to the positive-sequence voltage (U2/U1), two criteria with different conditions are formed, each of which indicating a faulted phase, and if both criteria indicate the same phase as faulted, single-pole tripping can take place.

Description: Phase selection for around fault TECHNICAL FIELD It is both desirable and important, in the event of a fault in a power network, not to overreact by disconnecting all the phases when, for example, there is a fault in one of the phases only. The great problem in this connection, at least for faults with a high fault resistance, is to be able to determine which phase, or which phases, has (have) faulted. The present invention relates to a method and a device for phase selection for single-pole tripping of high-impedance ground faults in direct grounded power networks. BACKGROUND ART, THE PROBLEMS Determining which phase has faulted, or which phases have faulted, will hereafter, in accordance with the terminology used within this technical field, be referred to as "phase selection" . A number of different fault types occur in a power network, for which it is desired to learn as quickly as possible in which phase or phases a fault has occurred. The reason for this is that a faulted phase/faulted phases is/are to be disconnected from the supply sources to prevent dangerous situations from arising. In relatively simple networks and in relatively simple contexts a phase selection can be made, in the event of a fault, by determining by means of phase-current measuring members that a phase current exceeds a pre-set value. An obvious and simple method, in principle, is to use as phase selection determining criterion phase current changes exceeding a certain value related to nominal phase currents. In US-A-3, 56, 671, such a method is described which is otherwise based on directional wave detectors for each phase and which comprises a phase selector for single-phase tripping of circuit breakers for a faulted phase and for three-phase tripping of the circuit breakers of all the phases when faults occur on two or three phases. In another method for phase selection, the voltage reduction of the phases involved, which a fault generally results in, is also utilized in addition to the phase currents. In principle, this comprises using a vol age-dependent overcurrent relay or, as it is called within this technical field, an underimpedance relay. Such relays are described in a number of variants, for example as in ASEA Information RK 556-300 E, Nov. 1974, "Impedance Relay Type RXZF 2" and RK 556-301 E, Feb. 1979, "Three phase impedance relay type RXZK" . These relays are activated when an impedance, calculated with measured voltages and currents, lies within an operating range, specific to the relay and defined in an R-X diagram. The methodology in this connection is somewhat different depending on whether the fault is a single-phase or a two-phase fault. Phase selection etc. with the aid of underimpedance protection is also clear from "Schutztechnik in Elektroenergiesystemen" by H. Ungrad, . inkler and A. iszniewski, Springer-Verlag, published 1991, page 117 and Figure 6.22. ϋS-A-4,864,453 describes a method for selective phase selection in case of faults in distribution systems with double transmission lines between two stations. The method is based on Fourier parameter estimation of phase currents and phase voltages. With the aid of these as well as the residuals of the signals, it is first determined whether an abrupt event has taken place, after which it can be determined, via logical decisions, whether a fault has occurred between the stations as well as which phase or phases has or have faulted. When a fault occurs in a power network, this normally results in the network becoming unsymmetrically loaded. Methods for phase selection determination, based on the use of symmetrical components, have therefore often been employed. It is clear, inter alia from GE Application and Setting Guide, 1977, section 4, that the ratio of negative- sequence current 12 to zero-sequence current 10 for both single-pole and three-pole phase selectors is utilized. For single-pole phase selectors the phase position for the symmetrical currents in each phase is compared, and a time- limit is imposed on the the comparison means to allow an output signal for a coincidence period corresponding to +/- 60°. The disadvantage of using single-pole phase selectors according to this principle is that in the case of two-phase ground faults this method tends to select the faultless phase as the faulted phase. It is therefore necessary to have a three-pole phase selector which covers every conceivable multi-phase fault. The same GE publication also describes a three-pole phase selector which uses the same tripping principle as the single-phase one but where also an additional number of criteria are stated. In an article entitled "Progress in the Protection of Series-Compensated Lines and in the Determination of Very High Earth-Fault Resistances" in Brown Boveri Rev., 2-81, pages 102/103, a phase selector is also described. The starting point for selecting the correct phase are the zero- sequence current 10 and the negative-sequence voltage U2 for the phase on which a ground fault has occurred. Since the phase position for this voltage is approximately equal to the phase position of the zero-sequence voltage U0, function is obtained in the same way as with directional ground fault relays. By using, in addition, ground fault directional relays which are based on the zero-sequence components, it is possible to determine whether a fault is a ground fault or a fault between the phases. If it is a question of a two- phase ground fault, the start relays of the distance relays are activated, and with the aid of a logic circuit it is prevented that the faultless phase is selected. In EP-B-0 276 181 a phase selection method is described which is based on different linear connections between the above-mentioned symmetrical components. The device compri¬ ses, inter alia, six filters and three phase comparators. As will become apparent from the following description of the invention, the present invention will also be based on symmetrical components. Contrary to the processes mentioned above, where symmetrical components obtained with the aid of conventional RLC filters have been used, discrete-time numerical technique will, however, be used for the determi¬ nation. Such a method is described in "Microprocessor- implemented digital filters for the calculation of symme¬ trical components" by A.J. Degens in IEE PROC, Vol. 129, Pt. C, No. 3, May 1982, pages 111-118. It is clear from this how the symmetrical components can be described as a phase- rotating operator, that is, with a certain amplitude and phase angle or as a complex quantity with real and imaginary parts. SUMMARY OF THE INVENTION As will have been clear from the introductory part, the present invention relates to a method and a device for phase selection for single-pole tripping of high-impedance ground faults in direct grounded power networks. The phase currents and phase voltages of the power network are processed in a real time system with sampled measured values and with the use of discrete-time filters. The invention is based on the use of the symmetrical components Ul, U2, 10, that is, the positive-sequence and negative-sequence voltages and the zero-sequence current which arise in a direct grounded power network when a fault occurs. The positive-sequence component Ul is calculated with the aid of a positive-sequence filter and orthogonal weighting functions according to the calcula¬ ting technique mentioned, and the result is a continuously updated complex number. The corresponding calculating technique is used for obtaining, via a negative-sequence filter, a continuously updated complex number corresponding to the negative-sequence voltage U2. The invention is based on the ratio U2/I0 and an additional determination is introduced by also utilizing the ratio U2/U1. The methods for evaluating these ratios and the formation of conditions for phase selection differ conside¬ rably from the prior art. The inventive concept comprises forming from the ratio U2/I0 a first complex quantity U2/I0 = A + jB and forming from the ratio U2/U1 a second complex quantity U2/U1 = D + jE The conditions for phase selection according to the invention are now based on the evaluation of different combinations of A, B, D and E starting from a first complex plane for the real part A and the imaginary part B and a second complex plane for the real part D and the imaginary part E, respectively. The phase selection method means that, after a fault condition has arisen, according to the first criterion stated below a faulty phase is indicated with the aid of the first complex quantity and that thereafter, according to the second criterion stated below, the same phase is indicated as faulty with the aid of the second complex quantity such that sufficient proof is obtained that the indicated phase is the faulty one. The first criterion consists of the following conditions which indicate the R-phase as faulty if A < kiB and B < 0 and indicate the S-phase as faulty if A < k2B and B > 0 and indicate the T-phase as faulty if A > k 2 B and B > 0 or if A > kiB and B < 0 where i = -tan 30° and k 2 = tan 30°. The second criterion consists of the following conditions which indicate the R-phase as faulty if D < k 3 E and E > 0 or if D < k 4 E and E < 0 and indicate the S-phase as faulty if D > ksE and E > 0 or if D > k 4 E and E < 0 and indicate the T-phase as faulty if D > 0 and E > kβD or if D < 0 and E > k 7 D k 3 = -tan 70°, k 4 = -tan 10°, ks = tan 50°, 6 = tan 40°, k 7 = -tan 20° After these two criteria and conditions have indicated a fault in the same phase, a single-pole tripping of this phase can take place. If the ground fault is not a single- phase fault, three-phase tripping is used. DESCRIPTION OF THE PREFERRED EMBODIMENTS A device for carrying out the described method for phase selection in case of a ground fault in a direct grounded power network can be designed in many different ways, for example in the form of individual separate filters, selec¬ tors, etc., designed for digital processing in discrete-time and numerical form, or in a microprocessor-integrated form. In both cases, the functional units needed for filtering, selector functions and tripping logic, etc., can be dis¬ tinguished. The accompanying figure therefore describes an embodiment which is mainly built up as functional, separate units. The conversion of analog measured phase currents and phase voltages with the aid of current and voltage instrument transformers to filtered sampled discrete-time values i- R , is i and UR, US, UT, respectively, is in this context to be regarded as conventional technique and has therefore been omitted. * The above-mentioned converted current values are now supplied to an 10 device 1 for continuously obtaining a complex value of the zero-sequence current and the above- mentioned converted voltage values are supplied to a Ul, U2 device 2 for continuously obtaining complex values of the positive-sequence and negative-sequence voltages. In a first quotient generator 3 the quotient U2/I0 is then formed as a first complex quantity with a real part A and an imaginary part B, and in a second quotient generator 4 the quotient U2/U1 is formed as a second complex quantity with a real part D and an imaginary part E. In addition to the requirement of a zero-sequence current, as will have been clear from the above summary of the invention, a first and a second criterion containing different conditions regarding the two real and imaginary parts are required in order for a phase to be indicated as the faulted one. For the R-phase to be indicated, it is required according to the the first criterion that the condition A < k B and B < 0 are fulfilled. The determination as to whether these conditions are fulfilled is made, in an embodiment according to the figure, in a comparison member Rl. For the R-phase to be selected, it is also required according to the second criterion that any of the conditions D < k 3 E and E > 0 or D < k 4 E and E < 0 are fulfilled. The determination as to whether the first of these conditions is fulfilled is made in a comparison member R2 and the deter¬ mination as to whether the second of these conditions is fulfilled is made in a comparison member R3. Via an OR- element Re, information as to whether any of the conditions in R2 or R3 is fulfilled can be passed to an AND element Ro, which is also supplied with information from the comparison member Rl as to whether this condition is fulfilled and information about the presence of a zero-sequence current. When both of the conditions of the R-phase criteria are fulfilled and when a zero-sequence current is present, a signal is delivered from the Ro-element indicating that a phase selection has been made which identifies the R-phase as faulted. For the S-phase to be indicated, it is required according to the first criterion that the conditions A < k 2 B and B > 0 are fulfilled. The determination as to whether the first of these conditions is fulfilled is made in a comparison member SI. For the S-phase to be selected, it is also required according to the second criterion that any of the conditions D > k 5 E and E > 0 or D > k 4 E and E < 0 are fulfilled. The determination as to whether the first of these conditions is fulfilled is made in a comparison member S2 and the determination as to whether the second of these conditions is fulfilled is made in a comparison member S3. Via an OR element Se, information as to whether any of the conditions in S2 or S3 is fulfilled can be passed to an AND element So which is also supplied with information from the comparison member Si as to whether this condition is fulfilled and information about the presence of a zero-sequence current. When both of the conditions of the S-phase criteria are fulfilled and when a zero-sequence current is present, a signal is delivered from the So element indicating that a phase selection has been made which identifies the S-phase as faulted. For the T-phase to be indicated, it is required according to the first criterion that any of the conditions A < k 2 B and B > 0 is fulfilled or that the conditions A < kiB and B < 0 are fulfilled. The determination as to whether the first of these conditions is fulfilled is made in the comparison member Tl and the determination as to whether the second of these conditions is fulfilled is made in a comparison member T2. For the T-phase to be selected, it is also required according to the second criterion that any of the conditions D > 0 and E > εE or D < 0 and E > k 7 E are fulfilled. The determination as to whether the first of these conditions is fulfilled is made in a comparison member T3 and the determination as to whether the second of these conditions is fulfilled is made in a comparison member T4. Via an OR element TAe, information as to whether any of the conditions in Tl or T2 is fulfilled is passed to an AND element To, and via an OR element TDe information as to whether any of the conditions in T3 or T4 is fulfilled is passed to the same AND element To, which is also supplied with information about the presence of a zero-sequence current. When both of the conditions of the T-phase criteria are fulfilled and when a zero-sequence current is present, a signal is delivered from the To element indicating that a phase selection has been made which identifies the T-phase as faulted. The value of the constants ki ... k 7 has been indicated under the summary of the invention.

Claims: CLAIMS 1. A method for phase selection for single-pole tripping of high-impedance ground faults in direct grounded power networks based on the use of filtered and sampled discrete- time values i , is, ~-τ -and UR, US, T of measured phase currents and phase voltages and wherein these values are utilized for continuously obtaining the symmetrical components zero-sequence current 10 and positive-sequence and negative-sequence voltages Ul, U2 which are expressed as complex numbers with one real part and one imaginary part, which method is characterized in that with the aid of the symmetrical components, a first ratio U2/I0 is formed as a first complex quantity in the form of a real part A and an imaginary part B and a second ratio U2/U1 is formed as a second complex quantity in the form of a real part D and an imaginary part E U2/I0 = A + jB U2/U1 = D + jE and when there is a zero-sequence current, the faulted phase is determined according to a first criterion with conditions based on the first complex quantity and a second criterion with conditions based on the second complex quantity, and when the same phase is indicated as faulted by both the first and the second criterion, single-phase tripping of this phase takes place. 2. A method for phase selection for single-pole tripping of high-impedance ground faults in direct grounded power networks according to claim 1 and which is characterized in that the R-phase is indicated as faulted by the conditions according to the first criterion if A < kiB and B < 0 and the S-phase is indicated as faulted if A < k 2 B and B > 0 and the T-phase is indicated as faulted if A > k 2 B and B > 0 or if A > kiB and B < 0 where ki = -tan 30° and k2 = tan 30°, and that the R-phase is indicated as faulted by the conditions according to the second criterion if D < k 3 E and E > 0 or if D < k 4 E and E < 0 and the S-phase is indicated as faulted if D > ksE and E > 0 or if D > k 4 E and E < 0 and the T-phase is indicated as faulted if D > 0 and E > kεD or if D < 0 and E > k 7 D k 3 = -tan 70°, k 4 = -tan 10°, ks = tan 50°, k 6 = tan 40°, k 7 = -tan 20°. 3. A device for carrying out the method for phase selection for single-pole tripping of high-impedance ground faults in direct grounded power networks where as input signals are arranged sampled discrete-time values i R , is, iϊ and UR, U S , UT of measured phase currents and phase voltages and where these values are adapted for continuously obtaining the symmetrical components zero-sequence current 10 and positive-sequence and negative-sequence voltages Ul, U2 expressed as complex numbers with one real part and one imaginary part according to claim 1, characterized in that a first quotient generator (3) forms the quotient U2/I0 as a first complex quantity in the form of a real part A and an imaginary part B and that a second quotient generator (4) forms the quotient U2/U1 as a second complex quantity in the form of a real part D and an imaginary part E, and that single-pole tripping of the R-phase is adapted to take place via comparison means (Rl, R2, R3), an OR element (Re) and an AND element (Ro) if the conditions A < kiB and B < 0 and if D < k 3 E and E > 0 or if D < k 4 E and E < 0 are fulfilled and if there is a zero-sequence current, and that single-pole tripping of the S-phase is adapted to take place via comparison means (S1,S2,S3) and an OR element (Se) and a AND element (So) if the conditions A < k 2 B and B > 0 and if D > ksE and E > 0 or if D > k 4 E and E < 0 are fulfilled and if there is a zero-sequence current, and that single-pole tripping of the T-phase is adapted to take place via comparison means (Tl,T2,T3,T4) , OR elements (TAe,TDe) and an AND element (To) if the conditions A > k 2 B and B > 0 or if A > kiB and B < 0 and if D > 0 and E > kβD or if D < 0 and E > k?D are fulfilled and if there is a zero-sequence current when ki = -tan 30°, k 2 - tan 30°, k 3 = -tan 70°, k 4 = -tan 10°, k5 = tan 50°, kg = tan 40°, k 7 = -tan 20°.

Inventors: ERIKSSON LEIF, SAHA MURARI MOHAN, SVENSSON KJELL, ERIKSSON, LEIF, SAHA, MURARI, MOHAN, SVENSSON, KJELL
Applicants: ASEA BROWN BOVERI, ASEA BROWN BOVERI AB
Application year: 1993
Main classification: H02H3
IPC codes: H02H3