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Arc-Flash Incident Energy Calculator

Estimate arc-flash incident energy and boundary with the Lee and Doughty equations, as a first pass before a full IEEE 1584 study.

E = 793 × F × V × t / D²  [Lee, open air, >600V]

Arc-Flash Incident Energy

Doughty equations (≤600V) are only validated for 16–50 kA bolted fault current and working distances of 18 in or more — the tool will flag it if you're outside that range.
Arc duration is your upstream protective device's actual clearing time (breaker + relay, from a coordination study) — there's no universal default, since it's the single biggest driver of incident energy. Bolted fault current can come from the Fault Current Estimate calculator, or an actual short-circuit study. The 1.2 cal/cm² boundary threshold is the standard "just curable" second-degree-burn value from NFPA 70E Annex D — bump it to 1.5 cal/cm² if you're above 600V with a clearing time of 0.1s or less, per the same Annex D guidance.

Incident energy is the thermal energy an arc would deliver to a surface at a working distance, in calories per square centimeter. It determines the PPE category and the arc-flash boundary that must appear on the equipment label. Two inputs dominate it, and only one is obvious: available fault current, and how long the upstream device takes to clear. Halving clearing time roughly halves incident energy, which is why protection settings matter more to arc-flash exposure than almost anything else.

The formula

Above 600 V the Lee equation models an open-air arc; at 600 V and below the Doughty equations cover open-air and arc-in-a-box cases. In all of them, incident energy is directly proportional to arcing time, rises with available fault current, and falls steeply with working distance.
Bolted fault currentFrom the fault-current calculation at that point
Clearing timeHow long the upstream protective device takes to interrupt, in seconds
Working distanceDistance from the arc to the worker's face and chest, commonly 18 inches for LV gear
System voltageAbove 600 V the calculator uses the Lee equation; at 600 V and below, the Doughty equations. Both are from NFPA 70E Annex D

Worked example

At 480 V in an enclosure, with 22.6 kA bolted fault current and an 18 in working distance, the Doughty equation gives 4.3 cal/cm² at 0.1 s clearing and 8.5 cal/cm² at 0.2 s. Double the time, double the energy: incident energy is directly proportional to arcing time. The arc-flash boundary grows less, from about 3.6 ft to 5.7 ft, because energy falls off steeply with distance. A breaker setting change that shaves 100 ms off clearing can move a task into a lower PPE category without touching the hardware.

Which standard governs this

The Lee and Doughty equations are documented in NFPA 70E Annex D. IEEE 1584 is the governing standard for a full arc-flash calculation. NFPA 70E sets the workplace requirements: risk assessment, approach boundaries, PPE, and equipment labeling.

What this calculation does not account for

The Lee equation is a theoretical open-air model and tends to be conservative. The Doughty equations used at 600 V and below are empirical, and valid only within the 16–50 kA range they were fitted to. Neither models electrode configuration, arc gap or enclosure size the way the IEEE 1584 arcing-current method does. This is a screening estimate only. Labeling and PPE selection require a full study by a qualified engineer.

This is a screening estimate. It is here to get you to the right order of magnitude and the right conversation — not to replace a stamped calculation by a qualified engineer.

Common mistakes

Treating a screening number as a labeling result. Using a clearing time from the device curve without accounting for the arcing current being lower than bolted fault current, which can put the device on a slower part of its curve. Assuming higher fault current always means higher incident energy — sometimes it clears the device faster and lowers it.

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