2025-08-10

The Formation and Hazards of Arc Flash

 The cause of Arc Flash can be attributed to accidental contact, protective devices with insufficient short-circuit current ratings, contaminated insulating surfaces, deteriorated or corroded equipment or parts, and other reasons.

Arc Flash is a phenomenon that occurs when a large amount of lethal energy is discharged due to a short-circuit of an exposed conductor, causing the air to ionize. During the period of air ionization, a large amount of arc fault current generates tremendous heat, with temperatures that can reach up to 35,000 degrees Fahrenheit, higher than the temperature on the surface of the sun. This can cause serious burns on human skin and even ignite clothing. It can also liquefy or vaporize nearby metal objects, such as copper, aluminum wires or iron components. At this time, the volume of metal rapidly expands due to its change in state from solid to vapor, causing explosive pressure and sound waves. The strong sound wave impact may cause deafness, and the accompanying bright light can cause temporary or permanent blindness. Solid metal fragments and other loose items such as tools may become lethal flying projectiles, causing serious harm to human beings. The phenomena that may occur during Arc Flash are shown in Figure 1.

Figure 1 The phenomena during Arc Flash

Arc Flash Introduction

 Introduction

To the general public, an electric arc may seem like just a visual flash of light with little relevance to themselves. However, the high temperature and energy released by an electric arc pose a much greater threat to the safety of personnel working in the vicinity than flame burns. During routine system operation, there is always a risk of electric arc hazards when circuit breakers or switches are used to switch power or equipment is inspected. The threat to personnel and equipment safety in the work area is significant, and news reports of accidents caused by electric arcs are common, often with disturbing images.

Although fatalities caused by electric arcs do not occur more frequently than those caused by electrical shocks, they still have a significant impact, with a high mortality rate. According to statistics, there are nearly 30,000 electric arc accidents of varying degrees in the United States each year, with around 1,000 fatalities. In advanced societies that value human life, prevention is an essential issue.

For many years, the US government has invested significant resources and manpower into researching and discussing the potential harm that electric arcs can cause to personnel and equipment. The results of the research and experiments have been translated into practical, quantifiable values and classifications, and the electrical regulations have been updated and strictly enforced to improve the working environment for electrical workers. If the requirements are violated, heavy penalties are imposed, and there is no leniency. As a result, positive results have been achieved.

Compared to the United States, where various agencies have actively improved the working environment for electrical personnel by revising relevant regulations, such as NESC, NEC, NFPA-70E, and IEEE 1584, domestic regulations in this area are far behind. Apart from the second chapter of the Occupational Safety and Health Act of the Executive Yuan's Ministry of Labor, which states that "employers must have necessary safety and health equipment and measures in place to prevent hazards caused by electricity, heat, or other sources," there is a lack of concrete and specific guidelines to follow.

As a result of the vigorous enforcement of US regulatory agencies, electric arc flash evaluation and analysis have become a hotly debated topic. Around 2002, major power system analysis software companies began publishing electric arc flash calculation modules, and with the combination of existing short circuit calculation and protection coordination modules, they quickly gained market share. After years of updates and revisions, electric arc flash calculations are now relatively mature and widely used.

2024-03-21

IEEE 1584-2018 Arc-Flash calculation Steps [2]

 

Step 9 Calculate the incident energy

To determine the incident energy

1.      Determine the enclosure size correction factor.

2.      If the system voltage is 600 V < Voc ≤ 15000 V, use Equation (6), Equation (7), and Equation (8) to find intermediate values. Use Equation (10), Equation (11), Equation (12) to find the final value of the incident energy.

3.      If the system voltage is 208 V ≤ Voc ≤ 600 V, use Equation (9) to determine the final incident energy.

Formula as below

Find intermediate values        (6)

(7)

         (8)

(9)

 where

E600 is the incident energy at Voc = 600 V (J/cm2)

E2700 is the incident energy at Voc = 2700 V (J/cm2)

E14300 is the incident energy at Voc = 14 300 V (J/cm2)

E≤600 is the incident energy for Voc ≤ 600 V (J/cm2)

T the arc duration (ms)

Gthe gap distance between conductors (electrodes) (mm)

Iarc_600 the rms arcing current for 600 V (kA)

Iarc_2700 the rms arcing current for 2700 V (kA)

Iarc_14300 the rms arcing current for 14 300 V (kA)

Iarcrms arcing current for Voc ≤ 600 V [using Equation (25)] (kA)

Ibf bolted fault current for three-phase faults (symmetrical rms) (kA)

D the distance between electrodes and calorimeters (working distance) (mm)

CF correction factor for enclosure size (CF = 1 for VOA and HOA configurations)

lg log10

k1to k13 the coefficients provided in Table 4, Table 5, and Table 6.

Table 4 Coefficients for Equation (6), Equation (9), Equation (13), and Equation (16)


Table 5 Coefficients for Equation (7), Equation (14)

Table 6 Coefficients for Equation (8), Equation (15)

Find final value (600 V < Voc ≤ 15000 V)

                  (10)                (11)                  (12)

 where

E1 the first E interpolation term between 600 V and 2700 V (J/cm2)

E2 the second E interpolation term used when Voc is > 2700 V (J/cm2)

E3 the third E interpolation term used when Voc is < 2700 V (J/cm2)

When 0.600 < Voc ≤ 2.7, the final values of incident energy is given as follows

E = E3

When Voc > 2.7, the final values of incident energy is given as follows

E = E2

Find final value (Voc ≤ 600 V)

The incident energy is given as follows

E = E≤600

where

E≤600 the incident energy for Voc ≤ 600 V determined using Equation (9) solved using the arc current determined from Equation (1) and Equation (5) (J/cm2)

E the final incident energy at specified Voc (J/cm2)

Step 10 Determine the arc-flash boundary for all equipment

To determine the arc-flash boundary

1.    Determine the enclosure size correction factor

2.    If the system voltage is 600 V < Voc ≤ 15000 V, use Equation (13), Equation (14), and Equation (15) to find intermediate values. Use Equation (17), Equation (18), Equation (19) to find the final value of the arc-flash boundary.

3.    If the system voltage is 208 V ≤ Voc ≤ 600 V, use Equation (16) to determine of the final arc-flash boundary.

Formula as below

Find intermediate values

(14)

 

(15)




where

AFB600 the arc-flash boundary for Voc = 600 V (mm)

AFB2700 the arc-flash boundary for Voc = 2700 V (mm)

AFB14300 the arc-flash boundary for Voc = 14 300 V (mm)

AFB600 the arc-flash boundary for Voc ≤ 600 V (mm)

G the gap between electrodes (mm)

Iarc_600 the rms arcing current for 600 V (kA)

Iarc_2700 the rms arcing current for 2700 V (kA)

Iarc_14300 the rms arcing current for 14 300 V (kA)

Iarc the rms arcing current for Voc ≤ 600 V [obtained using Equation (5)] (kA)

Ibf the bolted fault current for three-phase faults (symmetrical rms) (kA)

CFthe correction factor for enclosure size (CF=1 for VOA and HOA configurations)

Tthe arc duration (ms)

lg log10

k1 to k13 are the coefficients provided in Table 4, Table 5, and Table 6.

Find final value (600 V < Voc ≤ 15000 V)

      (17)                                

       (18)

       (19)

 where

AFB1 the first AFB interpolation term between 600 V and 2700 V (mm)

AFB2 the second AFB interpolation term used when Voc is greater than 2700 V (mm)

AFB3 the third AFB interpolation term used when Voc is less than 2700 V (mm)

When 0.600 < Voc ≤ 2.7, the final values of arc-flash boundary are given as follows

AFB = AFB3

When Voc > 2.7, the final values of arc-flash boundary are given as follows

AFB = AFB2

Find final value (Voc ≤ 600 V)

The arc-flash boundary is given as follows

AFB = AFB≤600

where

AFB600arc-flash boundary for Voc ≤ 600V determined using Equation(16) solved using the arc current determined from Equation (1) and Equation (5) (mm)

AFBthe final arc-flash boundary at specified Voc (mm)

Step 11 Determine second arcing current

It must account for the arcing current variation. Repeat step 8, step 9, and step 10 using the reduced arcing current. It is possible that the incident energy and arc-flash boundary results obtained using the reduced arcing current are different. The final incident energy or arc-flash boundary is the higher of the two calculated values.

(20)

 where

VarCf the arcing current variation correction factor

Iarcthe final or intermediate rms arcing current(s) (kA) (see note)

Iarc_min a second rms arcing current reduced based on the variation correction factor (kA)

Voc the open-circuit voltage between 0.208 kV and 15.0 kV

k1 to  k7 the coefficients provided in Table 7

Table 7 Coefficients for Equation (20)


NOTE—The correction factor (1 – (0.5 × VarCf)) is applied as follows

208 V ≤ Voc ≤ 600 V To Iarc (final current only)

600 V < Voc ≤ 15000 V To Iarc_600, Iarc_2700, and Iarc_14300 (intermediate average arcing currents). The final Iarc value inherits the correction factor.

The “0.5” coefficient indicates that variation is applied to the average arcing current to obtain a lower-bound value arcing current.

IEEE 1584-2018 Arc-Flash calculation Steps [1]

 

According to IEEE 1584-2018 Guide follow 11 Steps to perform calculation of Arc-Flash Boundary (AFB) and Incident Energy (IE), as below.

Step 1Collect the system and installation data

While the data required for this study is similar to data collected for typical short-circuit and protective-device coordination studies, it goes further in that all low-voltage distribution and control equipment plus its feeders and large branch circuits must be included.

Step 2Determine the system modes of operation

In a site with a simple radial distribution system there is only one mode of operation.

Step 3Determine the bolted fault currents

Input  all  data  from  the  single-line  diagrams  and  the  data  collection  effort  into  a  short-circuit  program. Run and get the faulted currents.

Step 4Determine typical gap and enclosure size based upon system voltages and classes of equipment

Typical gaps between conductors (or bus gaps) as shown in Table 1 which also provides information on the enclosure sizes used for each voltage class.


Table 1 Classes of equipment and typical bus gaps

Equipment class

Typical bus

Gaps (mm)

Enclosure Size (H × W × D)

SI units (metric)

15 kV switchgear

152

1143 × 762 × 762 mm

15 kV MCC

152

914.4  × 914.4  × 914.4 mm

5 kV switchgear

104

914.4  × 914.4  × 914.4 mm

5 kV switchgear

104

1143  × 762  × 762 mm

5 kV MCC

104

660.4  × 660.4  × 660.4 mm

Low-voltage switchgear

32

508  × 508  × 508 mm

Shallow low-voltage

MCCs and panel boards

25

355.6  × 304.8mm  × ≤203.2 mm

Deep low-voltage MCCs

and panel boards

25

355.6  × 304.8mm  × >203.2 mm

Cable junction box

13

355.6  × 304.8 mm × ≤203.2 mm  or

355.6  × 304.8 mm × >203.2 mm

 

Step 5 Determine the equipment electrode configuration

The following electrode configurations are defined and listed according to their order of use within the incident energy model

— VCB Vertical conductors/electrodes inside a metal box/enclosure

— VCBB Vertical conductors/electrodes terminated in an insulating barrier inside a metal box/enclosure

— HCB Horizontal conductors/electrodes inside a metal box/enclosure

— VOA Vertical conductors/electrodes in open air

— HOA Horizontal conductors/electrodes in open air

Step 6 Determine the working distances

Typical working distances can be found in Table 2 based on the class of equipment.

Table 2 Classes of equipment and typical working distances

Equipment class

Working distance (mm)

15 kV switchgear

914.4

15 kV MCC

914.4

5 kV switchgear

914.4

5 kV MCC

914.4

Low-voltage switchgear

609.6

Shallow low-voltage MCCs and panelboards

457.2

Deep low-voltage MCCs and panelboards

457.2

Cable junction box

457.2

 

Step 7 Calculation of arcing current

To determine the arcing current

1.           Determine the applicable equipment electrode configuration.

2.           If the system voltage is 600 V < Voc ≤ 15 000 V, use Equation (1) to find intermediate values at 600 V, 2700 V, and 14300 V. Use Equation (2), Equation (3), Equation (4) to find the final value of the arcing current.

3.           If the system voltage is 208 V ≤ Voc ≤ 600 V, use Equation (1) to find the intermediate value (600 V only) and Equation (5) to find the final value.

Formula as below

Find intermediate valu(1)


where

I bf the bolted fault current for three-phase faults (symmetrical rms) (kA)

I arc_600 the average rms arcing current at Voc = 600 V (kA)

I arc_2700 the average rms arcing current at Voc = 2700 V (kA)

I arc_14300 the average rms arcing current at Voc =14 300 V (kA)

G the gap distance between electrodes (mm)

k1 to k10 are the coefficients provided in Table 3

lg log10

Table 3—Coefficients for Equation (1)



Find final value (600 V < Voc ≤ 15000 V)       (2)

 (3)                     (4)

 where

I arc_1 the first I arc interpolation term between 600 V and 2700 V (kA)

I arc_2 the second I arc interpolation term used when Voc > 2700 V (kA)

I arc_3 the third I arc interpolation term used when Voc is < 2700 V (kA)

Voc the open-circuit voltage (system voltage) (kV)

When 0.600 < Voc ≤ 2.7, the final value of arcing current is given as follows

I arc = I arc_3

When Voc > 2.7, the final value of arcing current is given as follows

I arc = I arc_2

Find final value (Voc ≤ 600 V)

                    (5)

where

Vocthe open-circuit voltage (kV)

Ibf the bolted fault current for three-phase faults (symmetrical rms) (kA)

Iarc the final rms arcing current at the specified Voc (kA)

Iarc_600 the rms arcing current at Voc=600 V found using Equation (1) (kA)

Step 8 Determine the arc duration

The arc duration is most commonly dependent on the operating time of a time-overcurrent protective device.