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Citation information: DOI 10.1109/TIA.2020.3020531, IEEE Transactions on Industry Applications Determine the Electrode Configuration and Sensitivity of the Enclosure Dimensions when Performing Arc Flash Analysis 1 Kaynat Zia Student member, IEEE University of Texas at Arlington 701 S Nedderman Dr Arlington, TX 76019, USA [email protected] Anusha Papasani Student member, IEEE University of Texas at Arlington 701 S Nedderman Dr Arlington, TX 76019, USA [email protected] David Rosewater Senior member, IEEE Sandia National Laboratories 1515 Eubank SE Albuquerque, NM 87123, USA [email protected] Wei-Jen Lee Fellow, IEEE University of Texas at Arlington 701 S Nedderman Dr Arlington, TX 76019, USA [email protected] Abstract -- Arc flash hazard prediction methods have become more sophisticated because the knowledge about arc flash phenomenon has advanced since the publication of IEEE Std. 1584-2002[17]. The IEEE Std. 1584-2018 [1] has added parameters for more accurate arc flash incident energy, arcing current and protection boundary estimation. The parameters in the updated estimation models include electrode configuration, open circuit voltage, bolted fault current, arc duration, gap width, working distance, and enclosure dimension. The sensitivity and effect changes of other parameters have been discussed the previous literatures [2],[8],[9],[11],[12],[15], this paper explains the fundamental theory on the selection of electrode configurations and performs sensitivity analysis of the enclosure dimension, that have been introduced in the IEEE Std. 1584-2018. According to the newly published model for incident energy (IE) estimation, the IE between VCB (Vertical Electrodes inside a metal Box) and HCB (Horizontal Electrodes inside a metal Box) can differ by a factor of two with other parameters constant. Using HCB as the worst-case scenario to determine the personal protection requirements [7],[10] may not be the best practice in all circumstances. This paper provides guidance for electrode configuration selection and a sensitivity analysis for determining a reasonable engineering margin when actual dimension is not available. Index Terms – arc flash, electrode configuration, enclosure dimensions, incident energy, plasma trajectory. I. INTRODUCTION An electric arc is formed when two physically separated and energized conducting bodies transfer charge through air [21]. The loss of insulation between conductors, due to ageing; environmental factors; human errors; and overheating, is one of the main causes of the electric arc formation [3]. The current flowing ionizes the air between the conductors, converting it into plasma and causing a rapid increase in temperature. The plasma is responsible for giving the arc its characteristic “flash” and contains the biggest part of the arc energy [20]. The high temperature, often compared to the temperature of the surface of the sun [16], brings about melting and evaporation of the conductors and other materials in the vicinity. This further increase pressure and temperature of the area near the arc. If the arc is not extinguished, the mounting pressure and temperature leads to an explosion. Severed equipment and molten debris move outwards during this explosion, burning and striking everything around it [14]. An arc starts with a series of transitions signified by their appearance in high speed film. The glow to arc transition starts with the “dark discharge” [5] or Townsend discharge [13], where electric field accelerated free electrons collide with gas molecules and as a result free more electrons, this causes an exponential increase in current versus voltage, due to the rapid ionization of air. The dark discharge stage is followed by “glow discharge” where voltage drops suddenly as current increases. The final stage involves the release of large number of electrons from the cathode [6]. The energy released during the arc are transferred through radiation, convection, and conduction. The hazard of an arc flash to humans is proportional to the temperature rise of skin due to the absorption of the released energy. If the energy absorbed by the human skin exceeds 1.2 cal/cm2 [4],[18], it can cause second degree burns according to the experiments conducted by Dr. Alice Stoll. 1 This work was partially funded by the U.S. Department of Energy, Office of Electricity, Energy Storage Program. This paper describes objective technical results and analysis. Any subjective views or opinions that might be expressed in the paper do not necessarily represent the views of the U.S. Department of Energy or the United States Government. (SAND2020-7245 J) This work is licensed under a Creative Commons Attribution 4.0 License. For more information, see https://creativecommons.org/licenses/by/4.0/. This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 10.1109/TIA.2020.3020531, IEEE Transactions on Industry Applications Incident energy (IE) is used to quantify the energy incident on the surfaces, equipment or human, near the arc flash. It is the area under the curve of the rate of heat transfer to a certain working distance, over time. By limiting the incident energy, personnel injury and equipment damage can be prevented. Electrode configuration can be a compounding factor for IE because the shape of the plasma explosion is not necessarily spherical. Right after arc initiation, a rapid increase in temperature causes the expansion of the hot air/plasma and can push the trajectory of the plasma to a direction governed by the orientation of the electrodes. According to IEEE Std. 15842018, an electric arc originating in horizontal conductors in a metal box (HCB) can have surfaces experiencing twice the IE of an electric arc originating in vertical conductors in a metal box (VCB), provided all other parameters remain the same. As engineers may or may not know the specific dimensions or electrode configuration of a panel being assessed for arc flash hazard, they often assume an HCB thinking it will provide a conservative estimate. However, using HCB as the worst-case scenario in IE calculations may not be the best practice. The contribution of this paper is to provide physics-based guidance to engineers performing arc flash analysis when there is uncertainty in the actual electrode configuration and detentions of the enclosure. II. Fig. 1 the relationship among current (I), Flux (B), and Force (F) DETERMINE ELECTRODE CONFIGURATIONS In order to avoid incorrect risk category estimation due to the electrode configurations, the right-hand rule can be employed. Fig. 1 shows the relationship among current (I), magnetic field (B), and force (F). The right-hand rule state that if the thumb of the right-hand points in the direction of current, the index finger points in the direction of the magnetic field and the middle finger will be the direction of force or the direction of motion. In this case of an arc flash, the direction of force will be the direction of the plasma flow or the plasma trajectory. For AC, the direction of current changes, causing the magnetic field to change but the direction of force remains the same. Because of this phenomenon, a worker standing at a point in the direction of F in Fig. 2, will be exposed to a much greater arc flash hazard than the one standing at any other point near the arc flash. Fig. 3 shows an example of HCB. The trajectory of the plasma travels outward to the opening of the enclosure. The red oval circle indicates the arc initiation location. Fig. 4 shows an example of VCB configuration. The blue oval circle indicates the arc initiation location. Fig. 5 shows an example of VCBB (Vertical electrodes terminated in an insulating barrier inside a metal box) configuration. The arc was initiated in the lugs of the equipment. These examples of HCB, VCB and VCBB use 2 pole and single-phase AC for simplicity. The user can expand this concept to three-phase AC as well. Fig. 2 Plasma Trajectory. Red Arrow: Current Flow; Green Arrow: Trajectory of the plasma; Arrowhead : Magnetic field goes out of paper; Arrow tail : Magnetic field goes into paper Fig. 3 An example of HCB configuration Fig. 4 An example of VCB configuration This work is licensed under a Creative Commons Attribution 4.0 License. For more information, see https://creativecommons.org/licenses/by/4.0/. This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 10.1109/TIA.2020.3020531, IEEE Transactions on Industry Applications Fig. 5 An example of VCBB configuration III. IMPACT OF THE ENCLOSURE DIMENSION ON THE IE ESTIMATION This section discusses the importance of using the exact enclosure dimensions and electrode configuration for incident energy calculation. This is done with the help of equations provided as the IEEE Std. 1584-2018’s contribution to incident energy estimation. The incident energy is calculated for the following range of values (these values are chosen based on IEEE Std. 1584-2018 model range): • Gap width: 1 in • Working distance: 18 in • Arc duration: 250ms. • Voltages: 0.48kV, 2.7kV and 14.3kV • Bolted fault current: 1kA, 50kA and 100kA for 0.48kV; and 1kA, 30kA and 60kA for both 2.7kV and 14.3kV. • Electrode configurations: VCB, VCBB (Vertical electrodes terminated in an insulating barrier inside a metal box) and HCB • Enclosure Dimensions: 20in x 20in x 20in (smaller box sizes don’t affect the incident energy values) to 49in x 49in x 49in The figures shown below indicate the trends of the incident energy with respect to the enclosure dimensions for different electrode configurations, bolted fault current, and voltage values. Some figures also compare the incident energy profiles for the three electrode configurations for all provided current categories. Fig. 6 Enclosure Dimension vs. Incident Energy for 1kA, 50kA and 100kA VCB (0.48kV) Fig. 7 Enclosure Dimension vs. Incident Energy for 1kA, 50kA and 100kA VCBB (0.48kV) Fig. 8 Enclosure Dimension vs. Incident Energy for 1kA, 50kA and 100kA HCB (0.48kV) Fig. 9 Enclosure Dimension vs Incident Energy for 1kA for VCB, VCBB and HCB (0.48kV) This work is licensed under a Creative Commons Attribution 4.0 License. For more information, see https://creativecommons.org/licenses/by/4.0/. This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 10.1109/TIA.2020.3020531, IEEE Transactions on Industry Applications Fig. 10 Enclosure Dimension vs Incident Energy for 50kA for VCB, VCBB and HCB (0.48kV) Fig. 13 Enclosure Dimension vs Incident Energy for 1kA, 30kA, 60kA VCBB (2.7kV) Fig. 11 Enclosure Dimension vs Incident Energy for 100kA for VCB, VCBB and HCB (0.48kV) Fig. 14 Enclosure Dimension vs Incident Energy for 1kA, 30kA, 60kA HCB (2.7kV) Fig. 12 Enclosure Dimension vs Incident Energy for 1kA, 30kA, 60kA VCB (2.7kV) Fig. 15 Enclosure Dimension vs Incident Energy for 1kA for VCB, VCBB and HCB (2.7kV) This work is licensed under a Creative Commons Attribution 4.0 License. For more information, see https://creativecommons.org/licenses/by/4.0/. This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 10.1109/TIA.2020.3020531, IEEE Transactions on Industry Applications Fig. 16 Enclosure Dimension vs Incident Energy for 30kA for VCB, VCBB and HCB (2.7kV) Fig. 19 Enclosure Dimension vs Incident Energy for 1kA, 30kA, 60kA VCBB (14.3kV) Fig. 17 Enclosure Dimension vs Incident Energy for 60kA for VCB, VCBB and HCB (2.7kV) Fig. 20 Enclosure Dimension vs Incident Energy for 1kA, 30kA, 60kA HCB (14.3kV) Fig. 18 Enclosure Dimension vs Incident Energy for 1kA, 30kA, 60kA VCB (14.3kV) Fig. 21 Enclosure Dimension vs Incident Energy for 1kA for VCB, VCBB and HCB (14.3kV) This work is licensed under a Creative Commons Attribution 4.0 License. For more information, see https://creativecommons.org/licenses/by/4.0/. This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 10.1109/TIA.2020.3020531, IEEE Transactions on Industry Applications 2.7kV 14.3kV Voltage 0.48kV 2.7kV 14.3kV Fig. 22 Enclosure Dimension vs Incident Energy for 30kA for VCB, VCBB and HCB (14.3kV) Fig. 23 Enclosure Dimension vs Incident Energy for 60kA for VCB, VCBB and HCB (14.3kV) TABLE 1 MAGNITUDE CHANGE IN INCIDENT ENERGY WITH CHANGING ENCLOSURE DIMENSIONS VCB Voltage 0.48kV 2.7kV 14.3kV Voltage 0.48kV 20”→21” 34”→35” 48”→49” -0.0073 -0.4274 -0.5963 -0.0182 -0.49 -0.9338 -0.0208 -0.54 -1.02 -0.0022 -0.1285 -0.1793 -0.0058 -0.16 -0.2971 -0.0081 -0.21 -0.40 -0.0012 -0.0720 -0.1004 -0.0030 -0.08 -0.1561 -0.0027 -0.07 -0.13 20”→21” -0.0075 -0.5677 -0.7683 VCBB 34”→35” 48”→49” -0.0018 -0.1342 -0.1816 -0.0012 -0.0882 -0.1193 Bolted Fault Current 1kA 50kA 100kA 1kA 30kA 60kA 1kA 30kA 60kA Bolted Fault Current 1kA 50kA 100kA -0.0167 -0.65 -1.3471 -0.0226 -0.79 -1.5778 20”→21” -0.0086 -0.4497 -0.5910 -0.0145 -0.56 -1.0885 -0.0179 -0.72 -1.4110 -0.0045 -0.18 -0.3663 -0.0089 -0.31 -0.6202 -0.0027 -0.11 -0.2168 -0.0020 -0.07 -0.1376 HCB 34”→35” 48”→49” -0.0023 -0.1222 -0.1606 -0.0045 -0.17 -0.3393 -0.0078 -0.31 -0.6138 -0.0015 -0.0759 -0.0997 -0.0024 -0.09 -0.1819 -0.0003 -0.01 -0.0206 1kA 30kA 60kA 1kA 30kA 60kA Bolted Fault Current 1kA 50kA 100kA 1kA 30kA 60kA 1kA 30kA 60kA To examine the sensitivity of incident energy to the enclosure dimension, the slope or the magnitude change in incident energy with respect to every 1 inch change in the both width and height of the enclosure dimensions at 20in, 34in, and 48in, that is, the change in incident energy when the enclosure dimensions change from 20in x 20in to 21in x 21in, 34in x 34in to 35in x 35in and 48in x 48in to 49in x 49in, are calculated for VCB, HCB and VCBB and the results are shown in Table 1. As one can see from the plotted graphs and the Table 1, the incident energy measured decreases with the increasing of the box sizes. This is because plasma expands and the bigger the box, the more room it has to expand in every direction. Since, the plasma source is not changing, the plasma intensity decreases the farther you go away from the source. Thus, the incident energy recorded at a fixed working distance away from the arc will show a decrease in magnitude with bigger box sizes. However, the plasma may not be able to fill the entire enclosure when the size of the enclosure increases beyond a certain limit as plasma intensity is a function of distance from the arc. Hence the sensitivity to the change in the box size has an inflection point, that is, the incident energy becomes somewhat independent of the box size. In case of the enclosure dimension uncertainty a larger engineering margin should be applied when this sensitivity is higher. For example, for a VCB configuration at 480V and 100kA (as seen in Fig. 6) bolted fault current, IE is more sensitive to the enclosure size when it is smaller, at 20in x 20in (magnitude change in IE is -0.0073), than when it is larger, at 49in x 49in (magnitude change in IE is -0.0012). This trend has been observed across all the electrode configurations, voltages, and currents. Table 2 shows enclosure types for IEEE Std. 1584-2018 arc flash model. It shows the equipment class and the suitable enclosure size used. The last three columns of the table show the magnitude change in incident energy at the given enclosure size values. The incident energy is calculated for a working distance of 36in and an arc duration of 1000ms across the three equipment classes. The incident energy calculated for 15kV This work is licensed under a Creative Commons Attribution 4.0 License. For more information, see https://creativecommons.org/licenses/by/4.0/. This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 10.1109/TIA.2020.3020531, IEEE Transactions on Industry Applications MCC using the correct enclosure size i.e., 36in x 36in x 36in and VCB as the electrode configuration is 33.22 cal/cm2, where the magnitude change is of the order of -0.34. Whereas, the incident energy estimated at 34in x 34in x 34in is 33.91 cal/cm2 where magnitude change is of the order of -0.38 and that at 38in x 38in x 38in is 32.61 cal/cm2 with a magnitude change of -0.29. It can also be seen that mistaking one electrode configuration for another also has a considerable impact on the incident energy values calculated. For the 5kV switchgear, provided the gap length (104mm), enclosure size (36in x 36in x 36in), bolted fault current (20kA), working distance (36in) and arc duration (1000ms) is kept constant, changing the electrode configuration from VCB to HCB changes the incident energy estimated from 20.21 cal/cm2 to 45.65 cal/cm2 with a magnitude change of -0.17 to -0.19. That is the change from VCB to HCB changes the incident energy by a factor of 2 as is evident from Fig. 9-11, Fig. 15-17 and Fig. 21-23. Incorrect incident energy calculation can have serious repercussions as it may lead to wrong PPE category selection. Human body takes about 0.19s to respond to any visual stimulus, 0.16s for an audio stimulus and 0.5s to move away from something that can potentially harm it [19]. The arc duration used here is representing the worst-case scenario. judgement and use reasonable estimated parameters when actual dimension is not readily available. REFERENCES [1] [2] [3] [4] [5] [6] [7] [8] [9] [10] TABLE 2. ENCLOSURE SIZES FOR IEEE STD. 1584-2018 ARC-FLASH MODEL ΔIE per 1in change in size Equipment class 15kV MCC 5kV Switchgear 5kV MCC Gap (mm) Enclosure size (in x in x in) IBF (kA) VCB VCBB HCB 152 36x36x36 30 -0.34 -0.54 -0.43 104 36x36x36 20 -0.17 -0.21 -0.19 104 26x26x26 20 -0.39 [11] [12] [13] IV. -0.50 -0.43 CONCLUSION With better understanding on the arc flash phenomena, the IEEE Std. 1584-2018 [1] has added more parameters to improve the accuracy of arc flash incident energy. Electrode configuration and the enclosure dimensions are two parameters that have drawn substantial discussion among industry. According to the newly published model for incident energy (IE) estimation, the difference of the IE between VCB and HCB can be more than two times with other parameters remain the same. 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Citation information: DOI 10.1109/TIA.2020.3020531, IEEE Transactions on Industry Applications This work is licensed under a Creative Commons Attribution 4.0 License. For more information, see https://creativecommons.org/licenses/by/4.0/.