Nagabhushan, J.Amarnath, D.Subbarayudu / International Journal of Engineering Research                and Applications (IJ...
Nagabhushan, J.Amarnath, D.Subbarayudu / International Journal of Engineering Research                and Applications (IJ...
Nagabhushan, J.Amarnath, D.Subbarayudu / International Journal of Engineering Research                 and Applications (I...
Nagabhushan, J.Amarnath, D.Subbarayudu / International Journal of Engineering Research                      and Applicatio...
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  1. 1. Nagabhushan, J.Amarnath, D.Subbarayudu / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 6, November- December 2012, pp.210-213 Effect Of Balanced Voltages On The Movement Of Metallic Particles In A Three Phase Common Enclosure Gas Insulated Busduct Nagabhushan*, J.Amarnath** and D.Subbarayudu*** *( P.D.A.College of Engineering, Gulbarga, India.) ** (J.N.T.U.H College of Engineering,Kukatpally,Hyderabad-85, India) ***(G.Pulla Reddy Engineering College, Kurnool, India)ABSTRACT The reliability of gas insulated d. Coating conducting particles with insulating filmssubstations can be improved by eliminating the The work reported in this paper deals witheffects of metallic particles. The purpose of this the movement of metallic particle in 3-phasepaper is to develop techniques, which will common enclosure Gas Insulated Busduct withformulate the basic equations that will govern the uncoated and coated enclosure. In order to determinemovement of particles like aluminum, copper in the axial movement in an uncoated enclosureuncoated as well as coated Busduct. system, the Monte-Carlo technique has been adopted in conjunction with motion equation. The presentKeywords – Aluminium, busduct, copper, gas paper deals with the computer simulation of particleinsulated substation, movement, particles. movement in 3-phase common enclosure GIB with coated as well as uncoated system. The specificI. INTRODUCTION work reported deals with the charge acquired by the Demand for electrical power has become particle due to macroscopic field at the tip of theone of the major challenges faced by the developing particle, the force exerted by the field on the particle,countries. Considering the relatively low per capita drag due to viscosity of the gas and random behaviorpower consumption, there is a constant need for during the movement. Wire like particles ofpower capacity addition and technological aluminium and copper of a fixed geometry in a 3-upgradation whereas non-conventional energy phase Busduct have been considered. The resultssystems have proved to be good alternative sources have been compared with the particle movement infor energy. In developing countries like India most uncoated and coated Busduct. The movement patternof the additional power has been met by for higher voltages class has been also obtained.conventional electric sources. Hence, the emphasis Monte-Carlo technique has been adopted forhas shifted towards improving the reliability of determining the axial movement of the particle. Ittransmission and distribution systems and ensuring has been assumed that at every time step the particlethat the innovations are not harmful to the can have a maximum movement 10 to 40 fromenvironment. Several authors conducted experiments vertical.on insulating particles. Insulating particles are foundto have little effect on the dielectric behavior of the II. MODELING TECHNIQUEgases [1-5]. However the presence of atmospheric The Fig. 1 and Fig. 2 show a typical horizontal threedust containing conducting particles, especially on phase busduct with and without dielectric coating.the cathode, reduces the breakdown voltage.Conducting particles placed in a uniform ac fieldlift-off at a certain voltage. As the voltage is raised,the particles assume a bouncing state reaching aheight determined by the applied voltage. With a C Bfurther increase in voltage, the bounce height and thecorona current increase until break down occurs [5].The lift off voltage is independent of the pressure of Agas. After the onset of bouncing, the offset voltage isapproximately 30% lower than the lift-off voltage. A, B, C are the conductorsSeveral methods of conducting particle control and Fig. 1 A typical 3-phase common enclosure GIBde-activation are given. Some of them are:a. Electrostatic trappingb. Use of adhesive coatings to immobilize theparticlesc. Discharging of conducting particles throughradiation, and 210 | P a g e
  2. 2. Nagabhushan, J.Amarnath, D.Subbarayudu / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 6, November- December 2012, pp.210-213 The electric field in 3-phase common enclosure GIB electrode system at the position of the particle can be written as B C E(t) = E1(t) + E2(t) + E3(t) (2) A Where, E(t) is the resultant field in vertical direction due to the field of three conductors on the surface of the particle at the enclosure. Dielectric E1(t), E2(t) and E3(t) are the components of the coating electrical field in vertical direction. The gravitationalFig. 2 Typical 3-phase common enclosure GIB with force and drag forces are considered as described bydielectric coating several authors. The enclosures are filled with SF6 gas at V. SIMULATION OF PARTICLEhigh pressure. A particle is assumed to be at rest at MOTIONthe enclosure surface, just beneath the Busbar A, Computer simulations of the motion ofuntil a voltage sufficient enough to lift the particle metallic wire particles were carried out on GIB ofand move in the field is applied. After acquiring an 64mm inner diameter for each enclosure and 500mmappropriate charge in the field, the particle lifts and outer diameter with 400KV applied to innerbegins to move in the direction of field having conductors with 1200 phase difference.overcome the forces due to its own weight and air A conducting particle motion, in an externaldrag. The simulation considers several parameters electric field will be subjected to a collectivee.g. the macroscopic field at the surface of the influence of several forces. The forces may beparticle, its weight, Reynold’s number, coefficient of divided intorestitution on its impact to both enclosures and Electrostatic Force (Fe)viscosity of the gas. During return flight, a new Gravitational Force (mg)charge on the particle is assigned based on the Drag Force (Fd)instantaneous electric field. Software was developed in C language considering the above equations and was used for all simulationIII. THEORETICAL STUDY studies. Many authors [1-4] have suggestedsolutions for the motion of a sphere or a wire like VI. RESULTS AND DISCUSSIONSmetallic particle in an isolated busduct system. The Fig. 3 shows the movement of aluminiumtheory of the particle charge and the electrostatic particle in radial direction for an applied voltage offorce on the particle is discussed elsewhere [5]. The 400KV rms. During its movement it makes severalmotion equation is given by impacts with the enclosure. The highest displacement in radial direction during its upwardmd 2 y journey is simulated to be 65mm. As the applied  Fe - mg - Fd (1) voltage increases the maximum radial movement dt 2 also increases as given in Table 1. However, it is noticed that even up to a voltage of 100kv, the Where, y is the direction of motion and Fd particle could not bridge the gap. Furtheris the drag force. The direction of the drag force is calculations may reveal the limiting voltage toalways opposed to the direction of motion. For enable the particle to reach the high voltagelaminar flow the drag force component around the conductor. A graphical representation of radialhemispherical ends of the particle is due to shock movement in relation to axial movement is given byand skin friction. Very limited publication is Monte-carlo technique as shown in Fig. 4. Theavailable for the movement of particle in a three- movement of copper particle was determined forphase Busduct, however the equation of motion is 400kv with similar parameters as above and found toconsidered to be same as that of an isolated phase have a maximum movement of 18mm in radialBusduct. direction as shown in Fig. 5. The movements are also calculated for other voltages.IV. CALCULATION OF ELECTRIC The movement of copper particle are alsoFIELD IN 3-PHASE BUSDUCT given in Table 1. It is noticed that the movement of The charge acquired by the vertical and copper particle is far less than aluminium particle ofhorizontal wire particles in contact with a bare identical size. This is expected due to higher densityenclosure and coated enclosure can be expressed as of copper particle. The axial and radial movement ofgiven by Srivastava and Anis [1]. aluminium and copper particles are calculated using Monte-carlo technique for three voltages i.e. 245kv, 211 | P a g e
  3. 3. Nagabhushan, J.Amarnath, D.Subbarayudu / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 6, November- December 2012, pp.210-213 300kv and 400kv with a solid angle of 10. It is significant to note that for all the cases considered, there is no change in maximum radial movement, even when Monte-carlo method is applied. A relatively high value of axial movement is achieved with the random angle of 10. As expected the axial movement of copper particle is lower than the aluminium. The movement of aluminium and copper particles for a coated enclosure surface is shown in Fig. 6 and 7 respectively. It can be seen that the movement has been far less than that of an uncoated system. Table 1 : Axial and Radial movement of aluminium and copper particles. Simulation time : 1 secVoltage Type Max. Monte-Carlo ( Radial =10) Fig. 4 particle Movement in 3-phase GIB Movement Radial Axial (400KV/Al / 0.1mm / 10mm / 10 Monte-Carlo (mm) (mm) (mm) technique)245KV Al 28 28 320 Cu 13 13 280300KV Al 32 32 340 Cu 14 14 300400KV Al 65 65 600 Cu 18 18 340 Table 2 : Axial and Radial movement of aluminium and copper particles with coated electrodes, thickness 50 micro meter Simulation time : 1 secVoltage Type Max. Monte-Carlo ( Radial =10) Movement Radial Axial (mm) (mm) (mm)245KV Al 0.001 0.001 100 Fig. 5 particle Movement in 3-phase GIB Cu 0.0001 0.0001 90 (400KV/Cu / 0.1mm / 10mm)300KV Al 0.02 0.02 210 Cu 0.002 0.002 183400KV Al 0.4 0.4 195 Cu 0.014 0.014 190 Fig. 6 particle Movement in 3-phase GIB on coated electrodes (400KV/Al / 0.1mm / 10mm / 50 micro meter) Fig. 3 particle Movement in 3-phase GIB (400KV/Al / 0.1mm / 10mm) 212 | P a g e
  4. 4. Nagabhushan, J.Amarnath, D.Subbarayudu / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 6, November- December 2012, pp.210-213 REFERENCES [1] M.M. Morcos, S. Zhang, K.D. Srivastava, and S.M. Gubanski, Dynamics of Metallic particle contamination in GIS with dielectric coating electrodes, IEEE Transactions on Power Delivery Vol. 15, No. 2, April 2000 p.p. 455-460. [2] J. Amarnath, B. P. Singh, C. Radhakrishna, S. Kamakshiah, Determination of particle trajectory in a Gas Insulated Busduct predicted by Monte-Carlo technique, International Conference on Electrical Insulation and Dielectric Phenomenon (CEIDP), 17-21 October 1999, Texas, Austin, USA.Fig. 7 particle Movement in 3-phase GIB on coated [3] H.Anis, K.D.Srivastava, Breakdownelectrodes (400KV/Cu / 0.1mm / 10mm / 50 micro meter) Characteristics of Dielectric Coated Electrodes in Sulphur Hexafluoride Gas VII. CONCLUSIONS with Particle Contamination, Sixth A model has been formulated to simulate International Symposium on High Voltage the movement of wire like particle in 3-phase Engineering No. 32.06, New Orleans, LA, common enclosure GIB on bare as well as coated USA. 1989. electrodes. The results obtained are presented and [4] J. Amarnath, B. P. Singh, C. Radhakrishna, analyzed. Monte-carlo simulation is also adopted to S. Kamakshiah, Influence of Power determine axial movements of particle in the Frequency and Switching Impulse Voltage busduct. Distance traveled in the radial direction is on Particle Movement in GIS – Predicted found to be same with or without Monte-carlo by Monte-Carlo Technique, IEEE simulation. The displacement on coated electrodes International High Voltage Workshop, are found to be very less compared to uncoated April 18-21, 2001, California, USA. electrode system. [5] J. Amarnath, B. P. Singh, C. Radhakrishna, S. Kamakshiah, Movement of Metallic ACKNOWLEDGEMENTS Particles in Gas Insulated Substations under The authors are thankful to management of the influence of various types of voltages, P.D.A College of Engineering, Gulbarga and JNT 11th National Power System Conference University, Hyderabad, for permission to publish (NPSC-2000), 20-22 December, 2000, IISc, this work. Bangalore, INDIA. 213 | P a g e

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