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C I R E D Perturbation Measurements on Overhead C I R E D 21st International Conference on Electricity Distribution Frankfurt, 6-9 June 2011 Paper 0513- PERTURBATION MEASUREMENTS ON OVERHEAD NETWORKS USING ELECTRIC FIELD SENSORS Pedro ISSOURIBEHERE Daniel ESTEBAN Fernando ISSOURIBEHERE IITREE-UNLP – Argentina IITREE-UNLP – Argentina IITREE-UNLP – Argentina [email protected] [email protected] [email protected] ABSTRACT This paper deals with the results of testing an electric field measurement system - completely designed by the authors - for monitoring voltage Flicker and harmonics in aerial power systems [1]. To prove the viability of this technique, an electric field sensor (EFS) was installed in our University High Voltage Laboratory, and in the HV network near a steel mill. Using the output of the electric field sensor, the voltage perturbations in any of the mentioned scenarios were determined. The deduced voltage perturbations agreed with direct measurements using conventional capacitive and Fig. 1. Measuring electric field between two electrodes. resistive voltage dividers and voltage transformers. Where: This technique can be used where cost or physical location 0 = Permittivity of free space = 8,854x10-12 [F/m] drawbacks make the use of conventional methods difficult. A = Surface area [m2] E = Electric field magnitude [V/m] INTRODUCTION If an external capacitor CB is connected between the parallel plates, and if this capacitor is not influenced by the electric The public electricity service in Argentina, which was field E, as shown in Fig. 1, the capacitor potential privatized in the early nineties, is carried out by different magnitude is given by: Agents and the control is performed by a Regulatory Agency (ENRE). The IITREE provides technical assistance jIC to the utilities and the Authorities. UjIXCCC jACE 0 B (2) C Nowadays, after almost twenty years of experience, it is B possible to conclude that when it is necessary to find a This relationship is independent of frequency, and therefore, disturbing source, traditional measurements through voltage if the electric field varies randomly, also the electric transformers in many places could be impractical, time potential will follow the same rule. In general: consuming, and expensive. In this article, an alternative way of measuring voltage utCE ket (3) perturbations based on sensing the Electric Field is On the other hand, the electric field e(t) at a point between described in detail. Experimental and field measurements results validate the proposed method. two conductors of an electric system is a consequence of an electric potential difference u(t), as shown in Fig 1. DESCRIPTION OF EFS The final conclusion is that if the potential across the capacitor CB is measured, the electric potential u(t) can be Unshielded electrical power systems generate electric fields obtained as: which can be measured accurately at distances from the ut conductors that are one order of magnitude larger than ut m (4) typical system dimensions. The field at a particular location GkkVEG and time is a function of the instantaneous voltage on all Where: conductors and depends on the geometry of both the power u(t) = Potential to be determined [V]. system and its environment. um(t) = Potential measured with the EFS [V]. The electric current that flows between the plates of a GV = Voltage gain between the output of the electric field parallel-plate capacitor immersed in an electric field, as sensor and the measurement equipment [V/V]. shown in Fig. 1, is given by: 0 A CB kE = EFS transduction constant = [m]. kG = Geometric constant of the physical installation [1/m]. it AEcos t (1) C 0 For the case of sensing the waveshape, as it is the case of measured perturbations referred to the fundamental Paper No 0513 1/4 C I R E D 21st International Conference on Electricity Distribution Frankfurt, 6-9 June 2011 Paper 0513- frequency voltage, it is not necessary to know the Table I and Table II show the results of Flicker and constants GV, kE, kG, being enough to verify the linearity harmonic measurements, respectively: and the independence of frequency. Table. I: Flicker measurement results Fluctuations [changes per minute] HV LAB EXPERIENCES AND CONTRAST Flicker 1620 110 2 To verify the ability of EFS for measuring perturbations, the EFS was installed below a high voltage cable in IITREE- Pst Generated 1,05 1,81 7,99 1,05 1,93 1,03 UNLP High Voltage Lab, as shown in Fig. 2. Measured [p.u.] 1,08 1,88 8,35 1,04 1,93 1,03 with EFS Table. II: Harmonic measurement results Order Harmonics 3º 5º 7º 9º 11º 13º 15º Level Generated 2,93 2,90 2,89 2,84 2,81 2,77 2,69 Measured [%] 2,96 2,93 2,93 2,88 2,86 2,84 2,78 with EFS In the case of Flicker, the performed comparison ensures that the measurement system EFS + recording equipment meet the standardized tests to achieve a measuring error not larger than 5 %, as the one accepted in IEC 61000-4-15 [2] standard. Regarding harmonics, the performed comparison ensures that the measurement system EFS + recording equipment meet standardized tests for equipment Class I according to IEC 61000-4-7 [3] standard. Fig. 2. EFS placed in the High Voltage Lab, under a cable fed EFS FIELD MEASUREMENTS with fundamental frequency voltage and Flicker. Flicker measurements The cable was fed by a 220V/50 kV transformer, which was excited with an electronic power generator. In this In order to verify the effectiveness of this technique for generator, the voltage fluctuation amplitude and frequency detecting the presence and for quantifying the amount of can be programmed in such a way that a specific Flicker Flicker in high voltage networks, a measuring campaign level can be adjusted. The generated Flicker magnitude was was performed in Buenos Aires province transmission measured with a second IEC normalized electronic network. equipment, connected in a conventional way, as shown in Measurements were made in the surrounding area of Fig. 3. Bragado 132 kV node. A one-line-diagram transmission system is depicted in Fig. 4. Fig. 4. One-line-diagram of the Argentinean transmission system in the nearest of Bragado. Fig. 3. Electronic power generator, Flicker measured through This node was fed by a 220 kV transmission line, which is voltage measurement (black equipment over the table) and part of the main interconnected grid in 500 kV. Bragado Flicker measured through EFS (white equipment). node supplies a wide geographical area in the centre of For measuring voltage harmonics, a similar test was Buenos Aires province in 132 kV. performed. Recording equipment, measuring Flicker in the traditional Paper No 0513 2/4 C I R E D 21st International Conference on Electricity Distribution Frankfurt, 6-9 June 2011 Paper 0513- way and every 10 minutes, was installed in a low voltage and in Bragado 132 kV high voltage line with the EFS. 4,0 level of Bragado LV (380/220 V) distribution public Pst Bragado 220 V network, and was used as reference for measurements 3,5 Pst Bragado 132 kV performed below the high voltage lines with the EFS. All 3,0 measurements carried out with EFS were synchronized and 2,5 correlated with the low voltage Flicker measurements 2,0 The results of Flicker measurements in the low voltage Pst 1,5 network of Bragado city are shown in Fig. 5. 1,0 6,0 0,5 Pst 5,5 Pst95% 0,0 5,0 18:20:02 18:30:02 18:40:02 18:50:02 19:00:02 19:10:02 19:20:02 4,5 Time 4,0 Fig. 7. Simultaneous Flicker measurements in Bragado node in 3,5 LV network and in HV network with EFS. 3,0 Pst As a result of this first measurement, for high Flicker values 2,5 the upstream to downstream Flicker transfer coefficient 2,0 within 0.75 to 0.8 could be recognized. 1,5 1,0 Fig. 8 shows the results of simultaneous Flicker 0,5 measurements in Bragado LV (traditional measurement) 0,0 and in Chivilcoy 132 kV overhead line with the EFS. The 17:30 20:50 00:10 03:30 06:50 10:10 13:30 16:50 20:10 23:30 02:50 06:10 calculated Flicker level in Bragado 132 kV is also included. Time 6 Pst 220 V Fig. 5. Flicker measurements in Bragado City. Pst Chivilcoy 132 kV The Flicker value not exceeded in both time and space with 5 Pst Bragado 132 kV a 95% probability was Pst = 4. This value was 4 times higher 4 than the acceptable limit, according to international 3 standards and Argentinean regulations [4]. Pst For starting the field measurements, the EFS was placed on 2 top of a pole, approximately 2 meters above ground, to avoid the influence of nearby objects in motion that 1 eventually could change the electric field at a frequency that 0 alters Flicker measurements. Fig. 6 shows the EFS 09:10:02 09:20:02 09:30:02 09:40:02 09:50:02 10:00:02 10:10:02 placement on the rear part of a vehicle. Note: Safety Time Fig. 8. Simultaneous Flicker measurements in Bragado LV distances should be respected. Eventually, the EFS could be network and Chivilcoy HV network with EFS. placed directly on the roof of the vehicle. These precautions do not apply to harmonics. Considering the higher values, the relationship between Flicker measurements in Bragado 132 kV and Chivilcoy 132 kV was 0.71. To have solid reference values for the Flicker transfer coefficients from different nodes, the high voltage network presented in Fig.
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