By Daleep Mohla, Wei-Jen Lee, Jim Phillips, and Albert Marroquin ©ISTOCKPHOTO.COM/IKONSTUDIO Introduction to IEEE Standard 1584 GUIDE FOR PERFORMING ARC-FLASH HAZARD CALCULATIONS, 2018 EDITION SINCE IT WAS FIRST PUBLISHED IN 2002, IEEE STANDARD 1584 has been the premier standard for arc-flash hazard arcing current, incident energy, and arc-flash boundary (AFB) calculations for an arc-flash incident. After extensive testing and model development and a validation period, the long-awaited revision of IEEE 1584 has been published. The purpose of this article is to introduce IEEE Standard 1584-2018, IEEE Guide for Performing Arc-Flash Hazard Calculations, to the industry. The model range and the Digital Object Identifier 10.1109/MIAS.2020.2982574 Date of current version: 26 June 2020 rationale used for parameter selection is discussed for quantities such as voltage, bolted root-mean-square (rms) short circuit current, the gap between conductors, enclosure dimensions, fault duration, working distance, and system frequency. The rationale is provided for the selection of electrode configurations and various enclosure (box) sizes and arrangements. This model is based on more than six times the tests performed for the model used in the 2002 standard. It provides additional modeling of electrode configurations which were not included in the 2002 version. Some guidance on identifying electrode configurations is provided. 64 IEEE Industry Magazine SE PT EMDownloaded BE R/ OC TO BE Ron2020 1077-2618/20©2020IEEE Authorized licensed useApplications limited to: Juan Chavarria Araya. September 13,2023 at 17:04:39 UTC from IEEE Xplore. Restrictions apply. Overview This section provides a summary of the scope and purpose of IEEE 1584-2018 [1], and it also provides an overview of the model range of parameters. It also highlights important information on the assumptions and limitations of the model input parameter range. Scope The guide described in this article provides models and an analytical process to enable calculations of the predicted incident thermal energy (E) and the AFB. The process covers a collection of applicable field data, the consideration of power system operating scenarios, and the calculation parameters. Applications include the electrical equipment and conductors for three-phase ac voltages from 208 V to 15 kV. The calculations for single-phase ac and dc systems are not a part of this guide, but some guidance and references are provided for those applications. Recommendations for personal protective equipment (PPE) to mitigate arc-flash hazards are not included in this guide. Purpose The IEEE Standard 1584-2002 model considered only one vertical orientation and two configurations, one in VOA and the second in VCB. Lab Tests and Model Development An arc flash occurs when the insulation or isolation is not sufficient to withstand the applied voltage, and electric current jumps through an air gap from an energized conductor to another conductor to ground. Once an electric arc is established, the ionization of air and conductive materials, such as copper and aluminum, generates a hightemperature plasma and molecular cloud. Furthermore, during the arcing event, the current creates successive and r­epulsive magnetic forces that dramatically expand the plasma cloud. The direction of the plasma cloud is dictated by the right-hand rule. This magnetic expansion, combined with rapid heating, is often explosive. With Table 1. The range of input parameters for IEEE Standard 1584-2018 The purpose of the guide is to enable a qualified person(s) to analyze power systems for the purpose of calculating the incident energy (E) to which employees could be exposed during operations and maintenance work. Contractors and facility owners can use this information to provide appropriate protection for employees in accordance with the requirements of the applicable electrical workplace safety standards. Input Parameter Range Voltage (Voc)* 208–15,000-V three-phase (line to line) Bolted fault current (I bf) 208–600-V LV 500–106,000 A (rms symmetrical) Bolted fault current (I bf) 601–15,000-V MV 200 to 65,000 A (rms symmetrical) Gap (G) 208–600 V 6.35–76.2 mm (0.25–3 in) Range of the Model Gap (G) 601–15,000 V 19.05–254 mm (0.75–10 in) Working distance (D) ≥305 mm (12 in) (see [1, G.7.6]) The new arc-flash model is based on testing organized by the IEEE/National Fire Protection Association (NFPA) ArcFault-clearing time (T) No limit (see [1, G.7.8]) Flash Phenomena Collaborative Research Project. More Maximum height 1,244.6 mm (49 in) than 1,800 new tests were performed at five different testMaximum width 1,244.6 mm (49 in) ing facilities over a six-year period to ensure consistency Minimum width Four times the gap (4 × G) and ­repeatability. Opening area The range of the IEEE 1584-2018 [1] model is provided 1.549 m2 (2, 401 in 2) in Table 1 [1, Sec. 4.2]. The IEEE 1584-2002 model had Frequency 50 or 60 Hz one conductor/electrode orientation (vertical), and two * Voc refers to an actual prefault open-circuit line-to-line voltage. LV: low configurations in open air (VOA) and in a box (VCB). voltage; MV: medium voltage. The IEEE 1584-2018 model has been developed from extensive testing performed with the purpose of obtaining data to include Table 2. The conductor/electrode orientation and configurations additional conductor orientations and configurations. Three new electrode Electrode Conductor configurations were added. These are Configuration Standard Orientation Configuration Termination identified as vertical conductors in a VOA 2002-2018 Vertical Open air Open air box terminating in an insulating barVCB 2002-2018 Vertical In a box* Open air rier (VCBB), horizontal conductors in a VCBB 2018 Vertical In a box Insulating barrier box (HCB), and horizontal conductors in open air (HOA) for a total of five HOA 2018 Horizontal Open air Open air electrode configurations as shown in HCB 2018 Horizontal In a box Open air Table 2. For definitions, see [1, Sec. 3] *In a box = metal enclosure. and [1, Annex G]. S E Pat T E17:04:39 M BE R/O CT O BEfrom R 2020 IEEE Industry Applications Authorized licensed use limited to: Juan Chavarria Araya. Downloaded on September 13,2023 UTC IEEEXplore. Restrictions apply. Magazine 65 Worker Position FIGURE 1. A 480-V, three-phase arc-flash incident in an enclosure. Worker Position FIGURE 3. The plasma trajectory for vertical electrodes [1, Fig. G.7]. depict the trajectory of the plasma on vertical and horizontal electrodes. In 2004, with support from industry, the IEEE and the NFPA formed the Arc-Flash Phenomena Collaborative Research Project to support research and additional testing to increase the understanding of issues related to arc-flash phenomena. The test results provide information to help more accurately predict the hazards associated with high-energy arcing, thereby improving electrical safety standards and providing practical safeguards for employees in the workplace. The newly published IEEE 1584-2018 guide refines previous calculation methods to estimate the arcing current and incident energy for VCB and VOA electrode configurations and provides new equations for VCBB, HCB, and HOA (see the “Overview” section). FIGURE 2. The plasma trajectory for horizontal electrodes. [1, Fig. G.8]. s­ ustained arc formation, electrical energy is continuously converted into intense heat, light, and pressure. Droplets of molten metal and toxic gases are also significant hazards. Although the arc-flash event itself may only last a few cycles, it can have a lasting impact on personnel, including burns, debilitating injury, and even death. Figure 1 shows a 480-V, three-phase arc-flash incident in an enclosure. In 2002, IEEE Standard 1584, IEEE Guide for Performing Arc Flash Calculations, was published. It has become the predominant method in industry for performing arcflash calculation studies. Immediately after the release of IEEE 1584-2002, the community pointed out some deficiencies of the model and several areas of arc-flash phenomena, where further research, testing, and validation were needed. For example, the orientation of the electrodes plays an important role in determining the plasma trajectory. Figures 2 and 3 [1, Figs. G.8 and G.7] Lab Testing To maintain consistency, the laboratory test facilities were verified. The calibration procedure and the actual tests were witnessed by representatives of the project team. The laboratories were required to have an adjustable power source to supply stable, short circuit current at the desired voltage for the test duration. The following sections of IEEE 1584-2018 provide information on the lab parameter characteristics and the data measurement and recording used. 1) Lab Parameters Used in Testing: This section describes the lab test parameters and their arrangement. ••Slug calorimeters comply with the specifications of ASTM-1959. The weight of each slug calorimeter was measured and recorded to ensure that it was approximately 18 g. ••The arrangement of the calorimeters is displayed in Figure 4. When performing VCB, HCB, VOA, and HOA tests, the center row of the calorimeters 66 IEEE Industry Magazine SEPTEMBER/OCT O BE Ron2020 Authorized licensed useApplications limited to: Juan Chavarria Araya. Downloaded September 13,2023 at 17:04:39 UTC from IEEE Xplore. Restrictions apply. was placed 5 ft above the ground level and was aligned with the center electrode. The height of the electrode tips was selected to simulate the incident energy exposure an electrical worker could receive to his or her face and chest area. ••For the VCBB test, the tips of the electrodes extended to the bottom of the metal enclosure. They were terminated using an insulating material barrier. The center of the bottom row of calorimeters was aligned with the center electrode. The lower edge of the bottom row of calorimeters was aligned with the lower edge of the metal enclosure. ••Hard-drawn copper electrodes with a diameter of 19.05 mm (3/4 in) were utilized. ••AWG 20 (~0.032 in) copper wire was used as the starter wire. It was tied at 51 mm (2 in) from the tip of the electrode. An AWG 10 wire may have to be used (as stated on page 22 of IEEE 1584-2018) if the AWG 20 wire does not trigger a sustainable arc. The electrodes were cleaned after every test, and the starter wire was checked to ensure that it had firm contact with the electrode to reduce contact resistance before the next test. ••The dimensions of the metal enclosure were selected or specified based upon the test voltage class. ••A test was performed for each setup. A second test was performed for each setup if a sustainable arc was not established during the first. 2) Data Measurement and Recording: The measurement process of the tests performed was another highly important step. ••Simultaneous voltage and current measurements and recording at 20,000 samples/s were conducted. ••A temperature-rise measurement and recording were performed using seven slug calorimeters and K-type thermocouples. The sampling rate used was at least 100 samples/s for each channel. 6 in 6 in 6 in 6 in 5 ft Above Ground 6 in 6 in FIGURE 4. The arrangement of the slug calorimeters (ASTM-1959 slug calorimeters; K-type thermocouples). scenario, the dc offset and harmonic components of the current waveform are filtered when performing the arcing current estimation. Figure 6 shows the comparison between filtered and unfiltered rms values of the arcing current. A sliding window cosine filter was used to derive the filtered rms signal from the sampled data. The process of converting a rising and falling sinusoidal waveform by means of a sliding window filter introduces a delay in the rms filtered signal. This delay has no influence in the model other than to obtain an equivalent rms value. Bonded/Grounded or Unbonded/Ungrounded Systems IEEE 1584-2002 uses a coefficient called K 2 in the incident energy equation to differentiate grounded from ungrounded/high-impedance grounded systems when calculating the incident energy. As a result, an u ­ ngrounded/high-impedance grounded system ends up with higher incident energy for similar arcing incidents. After further ­analysis and Data Processing 60,000 Arcing Current for a 13.8 kV VCB Test IA IB IC 40,000 20,000 0 1 179 357 535 713 891 1,069 1,247 1,425 1,603 1,781 1,959 2,137 2,315 2,493 2,671 2,849 3,027 3,205 3,383 3,561 3,739 3,917 4,095 4,273 4,451 (A) The arcing current estimation is necessary to determine the operating time of the protective devices. Depending on the fault-inception angle and X/R ratio of the system, the arcing current may contain a dc component. As displayed in Figure 5, the decaying of the dc offset can be seen in a 13.8-kV, 20-kA arc-flash test. Although the response of the fuse operation follows the I2t, the operation on most protective relays is based on symmetrical ac current. Because we do not know when the fault will happen and normally do not know the X/R ratio of the system, based on the conservative case –20,000 –40,000 –60,000 Samples FIGURE 5. The recorded arcing current from a 13.8-kV arc-flash test. IA, IB, and IC: phase A, B, and C arc currents. S E Pat T E17:04:39 M BE R/O CT O BEfrom R 2020 IEEE Industry Applications Authorized licensed use limited to: Juan Chavarria Araya. Downloaded on September 13,2023 UTC IEEEXplore. Restrictions apply. Magazine 67 30,000 25,000 20,000 (A) performed by a group of industry experts with various backgrounds comprising researchers, academia, manufacturers, end users, and mathOriginal Signal Filtered Signal ematical model-validation and verification experts. The model-validation process was completed in the following four main phases: 1)Reviewing raw data processing: During this stage, samples of the raw data measurements were evaluated to determine how the data were converted from actual instantaneous signal measurements to final rms average values of voltage and current, which could then be used in the data regression analysis process utilized for the model’s creation. 2) Prototyping model-validation tools: This phase included the creation of mathematical models in different computing languages and also the use of statistical analysis algorithms for the purpose of graphical analysis of the model’s output results. The tools created included MATLAB models, spreadsheets, and C language-based analytical tools. 3) Establishing model performance metrics: The metrics or benchmarks used to validate the output of the new model included a direct comparison to the processed test data measurements and observing the fidelity of the model’s output. The metrics also included partial comparisons to IEEE 1584-2002. Also, comparisons were made against several published IEEE re­­ search papers with an emphasis on those that included information for the new electrode configurations. 4) Determining the final range of the model: During this stage, the effect of each input parameter was analyzed against parameter sweep plots to assess the behavior of the model’s output across the range of parameters used in the laboratory tests. This stage also included an evaluation of the typical data inputs provided in [1, Sec. 6, Tables 8 and 10]. RMS Values of the Arcing Current 15,000 10,000 5,000 1 133 265 397 529 661 793 925 1,057 1,189 1,321 1,453 1,585 1,717 1,849 1,981 2,113 2,245 2,377 2,509 2,641 2,773 2,905 3,037 0 Samples FIGURE 6. The filtered and unfiltered rms arcing current comparison. 1,233 1,121 1,009 897 785 673 561 449 337 225 1 Neutral Current 113 Current (A) 8,000 6,000 4,000 2,000 0 –2,000 –4,000 –6,000 –8,000 –10,000 –12,000 Samples (0.1 ms/sample) VCB-6-17.2-10-G VCB-6-17.2-10-UG FIGURE 7. The neutral current for bonded and unbonded enclosure tests (VOC = 480 V, six-cycle, Ibf = 17.2 kA, and gap = 10 mm). testing, it was found that some current flows through the neutral conductor in the first few cycles due to an unbalanced arcing fault. The current disappeared when the arcing fault evolved into a three-phase balanced fault. The observation of smaller neutral arc currents during the first few cycles is, understandably, what led IEEE 1584-2002 to adjust the energy of ungrounded/highresistance grounded systems. Figure 7 shows the neutral current for a grounded and an ungrounded system during an arc-flash incident at 480 V. The duration of the neutral arc currents is reduced significantly as the system voltage is increased. Testing at 2,700 V showed no difference on grounded or ungrounded systems. The results are presented in Table 3. The differentiation between grounded and ungrounded systems is no longer considered to have a significant effect on the new incident energy model. Arc-Flash Model Validation The model-validation stage was critical to ensure the consistency of the results of the new arc-flash model presented in [1, Sec. 4.4–4.10]. The model-validation process was Arc-Flash New Model Performance Improvements The model-validation process evaluated the fidelity of the IEEE 1584-2018 arc-flash model output results and produced evidence of its improved performance when compared to the 2002 model. The following performance improvements were evaluated during the model validation process. 1) Low-voltage (LV) arc current model: The arc current model has improved physical behavior across every voltage level based in the range. The IEEE 1584-2002 model produced inaccurate arc current predictions at some input voltages. Figure 8 shows clear evidence of the improved performance, in particular between 690 and 68 IEEE Industry Magazine SEPTEMBER/OCT O BE Ron2020 Authorized licensed useApplications limited to: Juan Chavarria Araya. Downloaded September 13,2023 at 17:04:39 UTC from IEEE Xplore. Restrictions apply. Arcing Current (kA) Arcing Current (kA) 1,000 V, where the arc curTable 3. A comparison of E for bonded, unbonded, and resistance ground arc-flash rent was predicted to be higher than the bolted testing (Voc = 2.7 kV, 12-cycle, Ibf = 10 kA, gap = 1.5 in, and D = 24 in) short circuit current. Arc VCB-12-10-1.5-24 current modeling improvement is certainly one of Ground Resistance the most important aspects Unbonded/Ungrounded Bonded/Grounded (100-A SLG) evaluated during the model E (cal/cm2) E (cal/cm2) E (cal/cm2) validation stage. Accurate currents lead to accurate Maximum Average Maximum Average Maximum Average fault duration determination. 4.63 3.73 4.87 3.63 4.12 3.47 2) Effect of gaps on the arc cur4.67 3.73 4.27 3.38 4.28 3.43 rent: The arc current is sen4.85 3.68 4.21 3.32 4.35 3.45 sitive to gaps for mediumvoltage (MV) systems. All 4.24 3.55 5.18 3.6 — — of the physical models 4.32 3.33 4.64 3.4 — — show that, in MV systems, SLG: single line to ground. short circuit current and gaps are the most important factors that de­­ termine arc current. The 2002 model was not sensitive to gap variation, which introVCB Arcing Current at lbf = 20 kA, Gap = 19.05 mm duced errors in the determination of the operating 30 time of overcurrent protective devices. Figure 9 demonstrates that the IEEE 1584-2002 model arc current 25 was only a function of bolted fault current and was 20 insensitive to both voltage and gaps. Figure 9 also shows that IEEE 1584-2002 did not consider arc cur15 rent variation for MV systems (because 100% of I arc 10 and minimum curves overlap). 3) LV incident energy model: Overly conservative incident 5 200 300 400 500 600 700 800 900 energy correction factors (CFs) were removed from the Voltage (V) LV portion of the model. This improvement is particularly important for equipment with short circuit current VCB1584-2002 VCBnew (Average) and voltage parameters, which approach the LV arc VCB1584-2002 (min) VCBnew (min) sustainability threshold. In [1, Sec. 4.3], it states, “Sustainable arcs are possible but less likely in three-phase FIGURE 8. The improved LV Iarc performance [1, Fig. G.32]. systems operating at 240 V nominal or less with an available short circuit current less than 2000 A.” Test observations showed that the arc can be sustained at VCB Arcing Current at 2,500 A and above. It was the decision of the working lbf = 20 kA, Gap = 76.2 mm group that arc is less likely at 2,000 A (80% of 2,500 A). 20 Figure 10 shows the significant reduction in energy 19 output of the new model. 18 4) Reduced AFB: The AFB calculation is more accurate, in particular, for MV VCB configurations. Physical AFBs 17 are significantly reduced as a result of the additional 16 testing and research. AFB reduction is certainly one of the most important improvements evaluated during the 15 model-validation stage. 14 5) Effect of enclosure dimension on incident energy: The 0 2,000 4,000 6,000 8,000 10,000 12,000 14,000 effect of the enclosure dimensions is now considered. Voltage (V) The only test-enclosure size considered for MV equipVCB1584-2002 VCBnew (Average) ment in IEEE 1584-2002 was on the larger dimension VCB1584-2002 (min) VCBnew (min) end of all enclosures in the new model (the 2002 model did not consider the effect of varying enclosure dimensions and only produced results for three standard FIGURE 9. The improved MV Iarc performance [1, Fig. G.33]. S E Pat T E17:04:39 M BE R/O CT O BEfrom R 2020 IEEE Industry Applications Authorized licensed use limited to: Juan Chavarria Araya. Downloaded on September 13,2023 UTC IEEEXplore. Restrictions apply. Magazine 69 p.u. Correction Incident Energy (cal/cm2) p.u. Correction Incident Energy (cal/cm2) Incident Energy (cal/cm2) enclosure sizes). With the increased proliferation of reduced footprint equipment, it became essential to conLV Incident Energy Comparison (1584-2018 Versus 1584-2002) sider the effect of smaller enclosures (in particular, for V = 208 V, EC = VCB, Gap = 25 mm, MV equipment). The new model predicts that enclosures Box (14 in × 12 in × 8 in), Working Distance = 18 in with smaller opening areas reflect higher energy. For 20 18 MV, the largest enclosure has a height and width of 16 1,245 mm each (49 in × 49 in). Larger enclosures can be 14 modeled but are analyzed with the largest enclosure-size 12 10 CF (to the right of region 2 in Figure 11) because the 8 plasma does not fill the enclosure volume, and the 6 changes to the enclosure opening area have a minimum 4 2 impact on the incident energy estimation. Figure 11 0 shows the CF produced by the MV incident energy 1 2 3 4 5 6 7 8 9 10 11 model for an enclosure opening area range between 400 Ibf (kA) and 2,704 in2. For HCB, the incident energy reduction 2 Incident Energy IEEE 1584-2002 (cal/cm ) effect is nearly 15% [an 0.85-per unit (p.u.) reduction]. Incident Energy IEEE 1584-2018 (cal/cm2) The depth of the enclosure is only considered in the LV part of the model when the depth is lower than FIGURE 10. The reduced incident energy for LV. 203 mm (8 in). Figure 12 depicts the depth effect for shallow enclosures (to the left of region 1). For shallow enclosures, the opening area input parameter is Voc = 13.8 kV, lbf = 18.241, Gap = 152 mm, meant to show the effect of depth Working Distance = 36 in, Fault Clearing Time = 193 ms instead of the opening area. In this 1 10.4 HCB HOA Region 1 Region 2 example, the 150-in2 opening area 0.95 9.9 point represents an enclosure where 9.4 0.9 the electrodes are near the enclosure 8.9 0.85 8.4 opening plane and where the depth 0.8 7.9 is smaller than 8 in. To account for 0.75 7.4 depth variation, the opening area 0.7 6.9 can be increased toward 400 in 2 0.65 6.4 (20 in × 20 in), which would rep5.9 0.6 200 700 1,200 1,700 2,200 2,700 resent that the depth is nearly Opening Area (in2) 8 in. As expected, once the depth is greater than 8 in, the effect of the opening area reduces the incident FIGURE 11. The MV enclosure-size CF. energy as the opening area increases. The enclosure-size CF is 1 when the depth is greater than 203 mm Enclosure-Size CF for a Shallow Enclosure: VCBB Voc = 208 V, lbf = 3.34, (8 in) and the actual enclosure openGap = 25 mm, Working Distance = 18 in, Fault Clearing Time = 25 ms ing area is smaller than or equal to 1.25 400 in2 (20 in × 20 in). The encloIf Depth> 8 in 1.2 1 sures of these dimensions were not 1.15 included in the tests; however, such dimensions are considered less com1.1 0.95 mon in actual equipment. To sum1.05 marize, the model-validation process 1 0.9 ensured the accuracy of the new arc0.98 flash model results and produced Incident Energy—Shallow Enclosure 0.9 0.85 enhanced range and performance of Region 1 End 0.85 the model. p.u. Enclosure-Size CF 0.8 150 250 350 450 550 650 Opening Area (in2) FIGURE 12. The LV enclosure-size CF. 750 850 0.8 Arc-Flash Hazard Study An arc-flash hazard study should be performed by qualified persons who are knowledgeable about power 70 IEEE Industry Magazine SEPTEMBER/OCT O BE Ron2020 Authorized licensed useApplications limited to: Juan Chavarria Araya. Downloaded September 13,2023 at 17:04:39 UTC from IEEE Xplore. Restrictions apply. system studies, power distribution equipment, installation practices, and different modes of operation. This standard provides equations for the calculation of the thermal incident energy exposure to a worker at the working distance. As previously mentioned, recommendations for PPE are not included in this guide. PPE selection is based on the arc rating performance of the materials to an electrical arc discharge and heat transfer based on the Stoll curve. Readers are advised to consult standards such as NFPA 70E and applicable ASTM standards for the proper selection of PPE. An arc-flash study requires collection of the data listed in Table 1. However, a significant amount of additional data is typically needed to develop the system’s simulation models. Just like with the 2002 edition of IEEE 1584, most of the data collection is for conducting short circuit and protective device coordination studies, which are integral parts of the arc-flash study. An arc-flash study requires information on the available short circuit currents, protective device data, modes of operation, and so forth. The following sections expand upon on each data-collection requirement. Single Line (One-Line Diagram) One of the first places to begin the study is with existing single-line diagram(s) if available. The diagrams should be up to date with any changes that may have occurred in the system. If a single-line diagram is not available, one needs to be created. Modes of Operation The different modes of operation can affect the short circuit current and protective device operation. The modes of operation include normal operation and may also include configurations with different utility feeders in service, tie devices open or closed, and other sources, such as generators. Each of the configurations may affect the arc-flash study results. Source Short Circuit Data If an up-to-date short circuit study is available, this information can be used as part of the arc-flash study. However, if the short circuit study is not up to date or does not exist, one will need to be conducted based on applicable standards such as IEEE Standard 551 (IEEE Violet Book), IEC 60909-0 Short Circuit Currents in Three-Phase a.c. Systems—Part 0: Calculation of Currents, and IEEE Standard 242 (IEEE Buff Book). If the short circuit study is being updated or performed for the first time, information regarding the available bolted rms symmetrical short circuit current, X/R ratio, voltage, and location of the short circuit current should be obtained. However, other formats may also be used, such as equivalent impedance data or short circuit MVA. The short circuit data should include conditions that yield maximum, normal, and minimum short circuit currents. The mini- mum short circuit currents can cause significantly slower protective device opening time. Temporary or alternate sources of short-circuit should be considered when selecting the operating conditions for the arc-flash study. Impedance Data Impedance data for components such as transformers and conductors are a necessary part of short circuit calculations. Tolerances in the impedance of these elements can change the short circuit current and should be considered accordingly. Positive tolerances can be assumed when determining the minimum short circuit current. Source Protective Device Data In addition, data regarding the upstream overcurrent protective device(s) of the source that serves the f­acility under study are required. This may include fuse data, overcurrent relay, circuit breaker and instrument transformer data, or circuit breaker data for low-voltage systems. The time-current characteristics are necessary to define the arc duration at the service equipment or starting point. IEEE 242 provides guidance for conducting protective device coordination studies. Enclosure Size The 2018 model includes more enclosure sizes as well as a CF to compensate for the reflectivity effect of the enclosure size on incident energy and AFB. In general, the smaller the enclosure opening, the more focused the incident energy will be (except for shallow LV enclosures where the depth has an increased effect on the spreading of the plasma). [Refer to 5) in the “Arc-Flash New Model Performance Improvements” section.] Larger enclosures with wider opening areas tend to produce less incident energy. The incident energy equations were normalized to a 508-mm (20-in) × 508-mm (20-in) opening area (which produces the highest incident energy). For enclosures larger than the range of the model, adjusting the calculations to the largest enclosure size is an alternative. In [1, Table 8], information on how test-enclosure dimensions are associated with different equipment classes is provided. It is preferred to use actual dimensions where possible and not overestimate the incident energy by using the dimension that produces the highest incident energy. A conservative approach was taken to account for the effect of each parameter in the new model; thus, data collection (including dimensions) should aim for accuracy. Protective Devices The arcing current duration is normally defined by how long it takes an upstream protective device to clear the fault. Engineering judgment must be used to determine which upstream device is to be considered. Typically, devices in a separate compartment or S E Pat T E17:04:39 M BE R/O CT O BEfrom R 2020 IEEE Industry Applications Authorized licensed use limited to: Juan Chavarria Araya. Downloaded on September 13,2023 UTC IEEEXplore. Restrictions apply. Magazine 71 ­ nclosure that is judged to not be affected by a downe stream arc flash are used. The total clearing time, which is the total time until the circuit is completely interrupted and the arcing current is extinguished, should be used. This may include time functions such as device sensing and opening times, safety margins, and auxiliary devices such as lockout relays and total melting time (in the case of fuses); in other words, the total time until the arc is fully extinguished. Gap Distance The typical gap distance between conductors is provided in IEEE 1584 based on the class of each piece of equipment that is a part of the study. This distance is necessary for the calculations. It may be prudent to ascertain the gaps in conjunction with the determination of the electrode configuration because gaps can change significantly from horizontal to vertical orientations. Working Distance The working distance is defined as the distance between the potential arc source and the face and chest of the worker performing the task. This distance has a significant effect on the available incident energy. The closer a worker is to the arc source, the higher the incident energy exposure. The list of equipment classes and working distance has increased with the 2018 edition, but the overall basic concept is the same as that of the 2002 edition. The default working distances listed in IEEE 1584 are 18 and 24 in for LV equipment (such as switchgear) and 36 in for MV equipment. This distance is based on the sum of the distance between the worker and the front R 500/5 CB_M CBF1 R1 MV Switchgear 13.8 kV 500/5 T1 1.5 MVA 5.5 %z LVCB_M Utility Source 436 MVAsc 18.2 kA 1.52567+j22.885% 13.8 kV R R2 T2 65 kVA Feeder Cable 2.6 %z 3-1/C 1/0 LVCBF1 CU 150 ft LV Switchgear 0.48 kV MCCB_M Panelboard 0.208 kV FIGURE 13. The one-line diagram used for calculation examples. opening of the equipment and the distance from the front opening to the prospective arc source inside the enclosure. For shallow enclosures, the working distance may be shorter than the default distance in the standard. However, consideration must be given to the actual task, and if known, the actual working distance should be used. For example, accessing energized switchgear from the rear may place the worker in shorter-than-default working distances. In these cases, the actual working distance should be used. Similarly, utilizing remote racking and operation devices may increase the working distances substantially. Electrode Configurations The IEEE 1584-2002 model was based on arc-flash tests using three electrodes in a vertical configuration in a VCB and in VOA. As previously mentioned in Table 2, the new IEEE 1584-2018 model includes three additional electrode configurations, which are VCBB, HCB, and HOA. As part of the data collection for the arc-flash calculations, the conductor configuration or arrangement that most closely resembles the actual electrode configurations needs to be identified. Each type of equipment, such as switchgear, panelboards, motor control centers, and so forth, may contain conductors arranged in more than one electrode configuration. Examples of how the electrode configurations used for laboratory tests correlate to actual equipment are provided in [1, Table 9]. Calculations illustrating the impact on the results as a function of the electrode configurations are illustrated in the “Calculation Examples” section of this article. Calculation Examples The purpose of this section is to present calculation examples that include the use of the parameters described in the “Arc-Flash Hazard Study” section and to provide additional calculation examples besides those provided in [1, Sec. D]. The selected examples illustrate the ­application of the arc current variation and the e ­nclosure-size CF. Consider a radial distribution system consisting of a utility service, 13.8-kV feeder, 1,500-kVA transformer, and 480-V feeder to a 2,000-A switchgear. The switchgear feeds a 208-V 200-amp panelboard. The one-line diagram is shown in Figure 13. The short circuit current and arc-flash input parameters are listed in Tables 4–6. The relevant impedance and other electrical characteristics of the system are provided as legends in the diagram. 13.8-kV Switchgear Table 4 lists the input parameters for the arc-flash incident energy calculation at the 13.8-kV switchgear. This example highlights the HCB configuration applied to an enclosure with opening dimensions, which exceed the maximum model range. The HCB configuration was selected to represent the condition when the circuit breaker is not inside the enclosure. 72 IEEE Industry Magazine SEPTEMBER/OCT O BE Ron2020 Authorized licensed useApplications limited to: Juan Chavarria Araya. Downloaded September 13,2023 at 17:04:39 UTC from IEEE Xplore. Restrictions apply. Using [1, Sec. 4, eqs. (1) and (17)], the total arc current based on the maximum bolted fault current of 18.241 kA is I arc = I arc- 2 = 16.507 kA. The total combined arc duration is obtained from relay “R1” as a combination of the relay trip time, circuit breaker “CB_M” opening time, and any additional operational delay is determined from Figure 14. The arc duration time is T = 193 ms. The enclosure dimensions can be used to calculate the enclosure-size CF. In [1, Sec. 4, eq. (11)], this equation can be solved using a width equal to 1,244.6 mm, and the solution for [1, Sec. 4, eq. (12)] is height1 = 49. Both dimensions exceed the maximum value of 1,244.6 mm (49 in). The CF is obtained from [1, Sec. 4, eqs. (13) and (14)]. In [1, Sec. 4, eq. (13)], this equation is the equivalent enclosure size and [1, Sec. 4, eq. (14)] is the CF for a “typical” enclosure: Width 1 = 8660.4 + ^ Width - 660.4 h $ ` 25.4 Voc + 10 jB 22 = 36.956 Height 1 = 49 Height 1 + Width 1 EES = = 42.978 2 2 CF = - 0.0001923 $ EES + 0.01935 $ EES + 0.6899 = 1.1764. The incident energy is calculated using [1, Sec. 4, eqs. (3)–(5) and (20)]: E = E 2 = 37.656 J/cm 2 ^8.98 cal/cm 2 h . The AFB is determined using [1, Sec. 4, eqs. (7)–(9) and (23)]: AFB = AFB 2 = 3.080 # 10 3 mm ^121.26 in h . The reduced arc current is achieved from [1, Sec. 4, eq. (2)]; however, it has no impact on the calculation because both the original and reduced arc current cause the relay to operate in its instantaneous region: 13.736 kA, the enclosure-size CF is the same at 1.176, the arc duration was also concluded at 193 ms because the relay still responded in its instantaneous region. The incident energy is 30.794 J/cm2 (7.36 cal/cm2), and the AFB is 2,731 mm (107.5 in). The arc current CF is the same as 0.988, and the minimum arc current is 13.58 kA. Table 4. The input parameters for a 13.8-kV HCB example Input Parameter Value (Imp. Units) Value (SI) Voltage 13.8 kV 13.8 kV Gap 6 in 152 mm Working distance 36 in 914 mm Height 52 in 1,321 mm Width 50 in 1,270 mm Depth 45 in 1,143 mm Maximum l bf 18.241 kA Minimum l bf 15.2 kA Imp.: imperial; SI: International System of Units. Table 5. The input parameters for a 480-V VCBB example Input Parameter Value (Imp. Units) Value (SI) Voltage 480 V 480 V Gap 1.25 in 32 mm Working distance 24 in 609 mm Height 26 in 660 mm Width 26 in 660 mm Depth 20 in 508 mm Maximum l bf 25.44 kA Minimum l bf 24.02 kA Table 6. The input parameters for a 208-V VCBB example Input Parameter Value (Imp. Units) Value (SI) Voltage 208 V 208 V VarC f = k1 $ V 6oc + k2 $ V 5oc + k3 $ V 4oc + k4 $ V 3oc + k5 $ V 2oc + k6 $ Voc + k7 = 0.024 1 - 0.5 $ VarC f = 0.988 Gap 1 in 25 mm Working distance 18 in 457 mm Height 19 in 482 mm Width 14 in 355 mm I arc_min = I arc_2 = 16.310 kA. Depth 8 in 203 mm Maximum l bf 3.34 kA Minimum l bf 3.23 kA The same process is identical for the minimum available short circuit current of 15.2 kA. The arc current is S E Pat T E17:04:39 M BE R/O CT O BEfrom R 2020 IEEE Industry Applications Authorized licensed use limited to: Juan Chavarria Araya. Downloaded on September 13,2023 UTC IEEEXplore. Restrictions apply. Magazine 73 480-V LV Switchgear Table 5 shows the input parameters selected for this example. This example highlights the application of the new arc-flash model to a VCBB configuration with typical enclosure dimensions. The example also highlights the effect of the arc current variation and its relationship to the minimum available bolted fault current. Using the maximum bolted fault current and [1, Sec. 4, eqs. (1) and (25)]: I arc = 1 0.6 2 $ 1 - 0.6 2 - Voc2 c mE c m ; Voc I arc_6002 0.6 2 $ I bf2 Height 1 + Width 1 = 25.948 2 CF = -0.0002976 $ EES 2 + 0.0320 $ EES + 0.4790 = 1.1089. EES = The incident energy is achieved from [1, Sec. 4, eq. (6)] using the coefficients of [1, Table 3] for VCBB: E = E # 600 = 10.531 J/cm 2 ^2.517 cal/cm 2 h . The AFB is verified with [1, Sec. 4, eq. (10)] using the coefficients of [1, Sec. 4, Table 3] for VCBB: AFB = AFB # 600 = 916.18 mm ^36.07 inh . I arc = 20.39 kA. The LV power circuit breaker opening time is 70 ms based on the characteristic time-current curve (TCC) displayed in Figure 15. The TCC curve includes both the trip and breaker opening time: The arc current variation can be ascertained using [1, Sec. 4, eq. (2)]. The arc current reduction value is 0.882: I arc_min = I arc_2 = 17.97 kA. T = 70 ms. 00 5, 0 00 10 0 ,0 00 3, 00 0 1, 0 30 0 10 30 50 10 5 3 1 0. 5 (s) By inspecting Figure 15, the expected arc duration is only a few milliseconds longer, and thus, this reduced The enclosure-size CF is ascertained using the folarc current solution does not produce a higher incident lowing equations from [1, Table 6] of IEEE 1584-2018 energy. The same equations and steps can be used for because both the width and height are between 508 the minimum available bolted fault current value of and 660.4 mm and the equivalent height (Height1) and 24.02 kA, so the intermediate steps can be omitted. equivalent width (Width1) are The arc current is 19.303 kA, and the enclosure-size CF is the same at 1.1089. The arc duration was concluded Width 1 = 0.03937 $ Width = 25.9842 to be approximately 71.6 ms because the arc current is still in the instantaneous band region. The incident Height 1 = 0.03937 $ Height = 25.9842. energy is 10.083 J/cm2 (2.41 cal/cm2), and the AFB is The CF is derived from [1, Sec. 4, eqs. (13) and (14)]: 899.41 mm (35.41 in). However, the reduced arc current obtained using the minimum available bolted short circuit current is 10 now a potential problem. The arc current CF is the same as 0.882, and the 5 minimum arc current is 17.025 kA. 3 The expected arc duration for this Utility Source arc fault current can be as high as 436 MVASC 240 ms because the reduced cur1 R1-P-51 R OC1 rent is between the instantaneous R1 0.5 CB_M and short-time regions of the TCC, as 0.3 R1-P-50 shown in Figure 15. The estimated MV Switchgear OC1 incident energy using this arc duration is 29.120 J/cm2 (6.96 cal/cm2), and 0.1 Iarc Minimum the corresponding AFB is 1,610.6 mm 13.58 kA at 13.8 kV 0.05 (63.41 in). This incident energy and Iarc Maximum 0.03 AFB can be considered worst-case 16.507 kA at 13.8 kV results for this location. This example illustrated the appli0.01 cation of VCBB enclosure-size CFs, arc current variation, and the need to Amps × 100-MV Switchgear (Nominal kV = 13.8, Plot Reference kV = 13.8) consider both the maximum and minimum bolted fault current in the calculations, as described in [1, Sec. 6.3]. FIGURE 14. The relay trip-time determination. 74 IEEE Industry Magazine SEPTEMBER/OCT O BE Ron2020 Authorized licensed useApplications limited to: Juan Chavarria Araya. Downloaded September 13,2023 at 17:04:39 UTC from IEEE Xplore. Restrictions apply. 10 10 5 3 5 0.3 0.1 Table 6 shows the input parameters selected for this example. This example illustrates the calculations for a 208-V panelboard fed by a 65-kVA transformer. This example also illustrates how to use the box CF when the depth of the enclosure is 203.2 mm (8 in) or lower. Using [1, Sec. 4, eqs. (1) and (25)], the arc current can be determined for the maximum bolted fault current of 3.344 kA: 0.05 LVCB M larc: 100% (lbf Maximum) 0.1 20.388 kA at 0.48 kV 3, 00 5, 0 00 10 0 ,0 00 0 0 30 1, 00 0 50 10 30 10 5 0.01 3 0.01 1 0.05 0.03 0. 5 0.03 Amps × 100-LV Switchgear (Nominal kV = 0.48, Plot Reference kV = 0.48) FIGURE 15. The LV power CB opening-time determination. larc: 85.6% (lbf Minimum) 1.3 kA at 0.208 kV 1 I arc = 1.569 kA. MCCB_M 0.5 1 0.5 larc: 85.6% (lbf Maximum) 0.3 1.34 kA at 0.208 kV 0.3 Panelboard 3, 00 1, 0 30 0 10 50 30 10 5 3 1 5 0. 00 5, 0 00 10 0 ,0 00 0.01 0 0.01 (s) 0.05 0.03 larc: 100% (lbf Minimum) 1.515 kA at 0.208 kV 0.1 larc: 100% (lbf Maximum) 0.05 1.569 kA at 0.208 kV 0.03 MCCB_M 0.1 T = 25 ms. The enclosure-size CF is determined using the following equations from [1, Table 6] of IEEE 1584-2018 because both the width and height are fewer than 508 mm: 3 larc: 88.2% (lbf Maximum) 1 17.97 kA at 0.48 kV 0.5 larc: 100% (lbf Minimum) 0.3 19.303 kA at 0.48 kV LV Switchgear 0.5 208-V LV Panelboard The arc duration is obtained based on the LV molded case circuit breaker. The opening time is estimated based on the time-current characteristic curve displayed in Figure 16. Once again, the TCC curve includes the trip and breaker opening times: Iarc: 88.2% (Ibf Minimum) 17.02 kA at 0.48 kV LVCB_M 1 (s) This example shows how the model can be used to predict and select instantaneous protective device settings. The results of this example lead to the conclusion that improvements in the protective device instantaneous pickup are needed to ensure that the instantaneous pickup is below all of the possible arc currents. Amps × 100-LV Panelboard (Nominal kV = 0.208, Plot Reference kV = 0.208) FIGURE 16. The molded-case CB opening-time determination. Width 1 = 0.03937 $ Width = 18.976 Height 1 = 0.03937 $ Height = 13.976. The CF is derived from [1, Sec. 4, eqs. (13) and (15)]: Height 1 + Width 1 = 16.476 2 1 CF = - 0.0002778 $ EES 2 + 0.1194 $ EES - 0.2778 = 1.06914. EES = The incident energy is concluded from [1, Sec. 4, eq. (6)] using the coefficients of [1, Table 3] for VCBB: E = E # 600 = 0.326 J/cm 2 ^0.078 cal/cm 2 h . The AFB is determined with [1, Sec. 4, eq. (10)] using the coefficients of [1, Table 3] for VCBB: AFB = AFB # 600 = 100.6 mm ^3.96 in h . The arc current variation can be obtained using [1, Sec. 4, eq. (2)]. The arc current reduction value is 0.856. The arc current variation factor is the highest on the lower end of the voltage range. The reduced arc current is I arc_min = I arc_2 = 1.34 kA. The reduced arc current does not produce a significant change to the expected operating time of the molded case circuit breaker, as depicted in Figure 16. The incident energy based on the reduced S E Pat T E17:04:39 M BE R/O CT O BEfrom R 2020 IEEE Industry Applications Authorized licensed use limited to: Juan Chavarria Araya. Downloaded on September 13,2023 UTC IEEEXplore. Restrictions apply. Magazine 75 arc current at 25 ms is 0.268 J/cm 2 (0.064 cal/cm 2) and the AFB is 90.68 mm (3.57 in). For the sake of brevity, the calculation example for the minimum bolted fault current is omitted, but it is not expected to produce a significant difference in the arc duration. Figure 16 shows that the expected arc current for the minimum bolted fault current case is not expected to exceed 25 ms. This example illustrated the application of the enclosure-size CF for a “shallow” enclosure with a VCBB configuration. The selected voltage and bolted fault current are still above the 2,000-A bolted fault current sustainability value presented in [1, Sec. 4.2]. Conclusions The quantification of arc-flash hazard energy has been an active topic of discussion between safety professionals since it was first identified as one of the causes of burn injuries to electrical workers more than 25 years ago. The first effort to quantify incident energy was IEEE 15842002, which was the first IEEE standard featuring a model based on only 300 tests. This article is intended to be a primer on the substantial advancements made in IEEE 1584-2018, which is based on more than 1,800 tests. This article covered the scope, test procedures, model development, input parameters required, and actual calculation examples based on IEEE 1584-2018. It also addressed how to determine the different electrode orientations and configurations necessary for the proper application of IEEE 1584-2018. Arc-flash hazard energy quantification is an evolutionary work, and standards will need to be updated as we learn more and perform further testing. It can be concluded that IEEE 1584-2018 is a significant improvement in this evolutionary process. Author Information Daleep Mohla (d.c.mohla@ieee.org) is with DCM Electrical Consulting Services, Inc., Missouri City, Texas. Wei-Jen Lee is with the University of Texas at Arlington. Jim Phillips is with Brainfiller, Scottsdale, Arizona. Albert Marroquin is with ETAP, Irvine, California. Mohla is a Life Fellow of the IEEE. Lee is a Fellow of the IEEE. Phillips and Marroquin are Senior Members of the IEEE. This article first appeared as “Introduction to IEEE Standard. 1584 IEEE Guide for Performing ArcFlash Hazard Calculations—2018 Edition” at the 2019 IEEE IAS Petroleum and Chemical Industry Conference. It was reviewed by the IAS Petroleum & Chemical Industry Committee. 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