Fire spread - Revision history

Peter: Improve FSE wiki article: Fire spread; source, clarity and calculation review (GPT-6)

2026-11-02T17:34:45Z

Improve FSE wiki article: Fire spread; source, clarity and calculation review (GPT-6)

Sanne: Add diagrams fse-fire-spread-v1.svg, fse-fire-spread-v2.svg, fse-fire-spread-v3.svg (level-1 visual plan)

2026-11-02T07:16:12Z

Add diagrams fse-fire-spread-v1.svg, fse-fire-spread-v2.svg, fse-fire-spread-v3.svg (level-1 visual plan)

← Older revision		Revision as of 08:16, 2 November 2026
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	Direct flame contact supplies intense local heating and a pilot. Radiation can act across a gap without flame or smoke touching the target, while convection carries hot gases to remote surfaces. Conduction transmits energy through solids, including walls and structural boundaries.<ref name="VR-5.1">Van Rossum (2027), §5.1.</ref><ref name="IFEG-1.6-7" />		Direct flame contact supplies intense local heating and a pilot. Radiation can act across a gap without flame or smoke touching the target, while convection carries hot gases to remote surfaces. Conduction transmits energy through solids, including walls and structural boundaries.<ref name="VR-5.1">Van Rossum (2027), §5.1.</ref><ref name="IFEG-1.6-7" />
			[[File:fse-fire-spread-v1.svg\|thumb\|upright=1.5\|alt=Fire reaching new fuel through flames, radiation, a wall and flying embers.\|Four fire-spread pathways to new fuel. Based on Australian Building Codes Board et al. (2005), p. 1.6-7.]]

	The target's arrangement affects each route. Thin or light items can respond quickly, while thick items can absorb energy internally. Orientation changes convective flow and the area exposed to flame radiation, and nearby surfaces can provide shielding or additional reflected and emitted energy.<ref name="Quintiere-2-247">Quintiere (2002), p. 2-247.</ref><ref name="Tien-1-75">Tien, Lee, and Stretton (2002), p. 1-75.</ref>		The target's arrangement affects each route. Thin or light items can respond quickly, while thick items can absorb energy internally. Orientation changes convective flow and the area exposed to flame radiation, and nearby surfaces can provide shielding or additional reflected and emitted energy.<ref name="Quintiere-2-247">Quintiere (2002), p. 2-247.</ref><ref name="Tien-1-75">Tien, Lee, and Stretton (2002), p. 1-75.</ref>
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	Conductive failure can occur when enough heat passes through a barrier to meet a failure criterion, even without loss of integrity or stability. Combustibles in the next enclosure can then be exposed on the unexposed side. The barrier can remain physically intact while this thermal pathway develops.<ref name="IFEG-1.6-7" />		Conductive failure can occur when enough heat passes through a barrier to meet a failure criterion, even without loss of integrity or stability. Combustibles in the next enclosure can then be exposed on the unexposed side. The barrier can remain physically intact while this thermal pathway develops.<ref name="IFEG-1.6-7" />
			[[File:fse-fire-spread-v2.svg\|thumb\|upright=1.5\|alt=Three panels: heat through intact wall, cracked barrier and collapsed barrier.\|Barrier failure can be thermal, integrity-related or structural. Based on Australian Building Codes Board et al. (2005), p. 1.6-7.]]

	Loss of integrity involves cracks, fissures or failure of firestopping. Hot gases, flames and radiation can then reach adjacent fuel through paths that were previously limited. The timing of such failure can also change smoke movement and ventilation.<ref name="IFEG-1.6-7" />		Loss of integrity involves cracks, fissures or failure of firestopping. Hot gases, flames and radiation can then reach adjacent fuel through paths that were previously limited. The timing of such failure can also change smoke movement and ventilation.<ref name="IFEG-1.6-7" />
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	The 2005 guidelines describe a grid approximation for large enclosures, using time offsets as fire moves between grid areas. Where object locations and ignition criteria are known, spatial development can instead be based on individual items. Both methods require defensible fuel arrangement and spread timing.<ref name="IFEG-2.6-12" />		The 2005 guidelines describe a grid approximation for large enclosures, using time offsets as fire moves between grid areas. Where object locations and ignition criteria are known, spatial development can instead be based on individual items. Both methods require defensible fuel arrangement and spread timing.<ref name="IFEG-2.6-12" />
			[[File:fse-fire-spread-v3.svg\|thumb\|upright=1.5\|alt=Large floor grid with fire moving between regions at different times.\|Grid time offsets represent spread across a large enclosure. Based on Australian Building Codes Board et al. (2005), p. 2.6-12.]]

	Vertical shafts and concealed spaces extend the relevant enclosure beyond the room of origin. Flame and hot gas can reach other floors through these routes. Analysis limited to horizontal spread across one floor would miss them.<ref name="IFEG-1.6-7" />		Vertical shafts and concealed spaces extend the relevant enclosure beyond the room of origin. Flame and hot gas can reach other floors through these routes. Analysis limited to horizontal spread across one floor would miss them.<ref name="IFEG-1.6-7" />

Jan: New FSE wiki article: Fire spread (written by Kimi Code CLI)

2026-11-01T22:50:54Z

New FSE wiki article: Fire spread (written by Kimi Code CLI)

New page

'''Fire spread''' is the extension of combustion from its initial location to additional fuel, spaces or structures. It can occur as continuous flame movement, successive ignition of separate objects, heat transfer through a barrier, burning debris carried to a new location or a combination of these routes. The process links ignition with fire growth beyond the first burning item.<ref name="Kanury-2-229">Kanury (2002), p. 2-229.</ref><ref name="IFEG-1.6-7">Australian Building Codes Board et al. (2005), p. 1.6-7.</ref>

Spread changes both the size and the location of the fire. Additional fuel can increase heat release rate, while new openings and spaces can alter ventilation and smoke movement. A developing fire therefore cannot be assessed only from its initial source and fuel package.<ref name="IFEG-1.6-3">Australian Building Codes Board et al. (2005), p. 1.6-3.</ref><ref name="Drysdale-1-95">Drysdale (2002), p. 1-95.</ref>

The relevant scale ranges from millimetres across a surface to flames and brands travelling between buildings. Each scale has different controlling heat-transfer and ignition conditions. Spread rate and direction are consequently scenario properties rather than fixed material constants.<ref name="Quintiere-2-246">Quintiere (2002), p. 2-246.</ref><ref name="IFEG-2.6-12">Australian Building Codes Board et al. (2005), p. 2.6-12.</ref>

== Successive ignition and heat transfer ==

Kanury describes fire spread over combustibles as continuous ignition of successive upstream material. The existing fire heats fuel ahead of the burning region until that fuel reaches its own ignition condition. Fuel production, mixing and heat loss at the new location all influence the time required.<ref name="Kanury-2-229" /><ref name="Kanury-2-230">Kanury (2002), p. 2-230.</ref>

Direct flame contact supplies intense local heating and a pilot. Radiation can act across a gap without flame or smoke touching the target, while convection carries hot gases to remote surfaces. Conduction transmits energy through solids, including walls and structural boundaries.<ref name="VR-5.1">Van Rossum (2027), §5.1.</ref><ref name="IFEG-1.6-7" />

The target's arrangement affects each route. Thin or light items can respond quickly, while thick items can absorb energy internally. Orientation changes convective flow and the area exposed to flame radiation, and nearby surfaces can provide shielding or additional reflected and emitted energy.<ref name="Quintiere-2-247">Quintiere (2002), p. 2-247.</ref><ref name="Tien-1-75">Tien, Lee, and Stretton (2002), p. 1-75.</ref>

Heat received by a target is not equal to total fire heat release. Only part reaches the object, and that part is balanced against losses and storage. Spread analysis therefore requires source exposure, target ignition response and time, not just the size of the original fire.<ref name="Rockett-Milke-1-29">Rockett and Milke (2002), p. 1-29.</ref><ref name="IFEG-2.4-4">Australian Building Codes Board et al. (2005), p. 2.4-4.</ref>

== Flame spread over continuous fuel ==

[[Flame spread]] over a solid or liquid involves a moving gas-phase flame close to the condensed fuel that supplies its vapour. Quintiere distinguishes the visible flame front from the evaporation or pyrolysis front in the fuel. The movement of the latter defines surface flame-spread velocity.<ref name="Quintiere-2-246" />

The flame must heat material ahead of itself for spread to continue. If that heating is too weak or heat losses are too large, the front can slow or stop. If preheating is strong, spread can accelerate as more fuel becomes involved.<ref name="Quintiere-2-247" />

Direction matters because fire-induced flow changes with orientation. Upward spread can preheat a large region above the flame, whereas lateral or downward spread relies on different forward heat-transfer paths. Opposed and wind-aided flow can therefore produce very different rates on the same material.<ref name="Quintiere-2-247" /><ref name="VR-4.3">Van Rossum (2027), §4.3.</ref>

Spread over a continuous surface differs from flame propagation through a premixed gas cloud. In the latter, fuel and oxidiser are already distributed in the gas phase. Surface spread instead requires continuing evaporation or decomposition at the condensed-fuel boundary.<ref name="Quintiere-2-246" />

== Spread between separate objects ==

Separate objects introduce gaps across which heat must travel. Flame contact, radiation and burning debris can bridge these gaps, while convective flow can expose objects farther away. The time of each new ignition determines the spatial development of the overall fire.<ref name="IFEG-1.6-7" /><ref name="IFEG-2.4-4" />

The 2005 International Fire Engineering Guidelines describe a simplified pre-flashover method for radiant ignition of a second item. It neglects radiation from the upper layer and room surfaces and uses flame radiation from the first item. This assumption belongs to that stage and method, and is unsuitable for a developed hot compartment.<ref name="IFEG-2.4-4" />

[[Fire spread between buildings]] can involve radiation through closed or fixed windows, direct flame contact and burning debris. The guidelines note that radiation can pass through glass without glass breaking. If breakage occurs, it can create both a new spread route and a ventilation change.<ref name="IFEG-1.6-7" />

[[Firebrands]] and embers add discontinuous spread. Burning material can rise in a thermal plume and be carried by wind before igniting a remote target. The 2005 guidelines caution that travel distance is difficult to establish with certainty, so precise brand trajectories should not be invented.<ref name="IFEG-2.6-12" />

== Barriers and compartmentation ==

[[Fire compartmentation]] divides a building into enclosures intended to limit fire and smoke spread. Its effectiveness depends on barriers, openings, firestopping, structural stability and the combustibles on both sides. An assessment therefore considers failure modes as well as nominal fire resistance.<ref name="IFEG-1.6-3" /><ref name="IFEG-1.6-7" />

Conductive failure can occur when enough heat passes through a barrier to meet a failure criterion, even without loss of integrity or stability. Combustibles in the next enclosure can then be exposed on the unexposed side. The barrier can remain physically intact while this thermal pathway develops.<ref name="IFEG-1.6-7" />

Loss of integrity involves cracks, fissures or failure of firestopping. Hot gases, flames and radiation can then reach adjacent fuel through paths that were previously limited. The timing of such failure can also change smoke movement and ventilation.<ref name="IFEG-1.6-7" />

Loss of stability involves collapse of the barrier, whether or not it is a structural element. This can create a large opening and expose new areas to flames and radiation. Structural failure and integrity failure are therefore distinct events in spread analysis.<ref name="IFEG-1.6-7" />

Doors and windows introduce time-dependent opening states. The guidelines suggest obtaining door-opening times from evacuation analysis and evaluating glass breakage from fire severity. These changes connect occupant movement and component response with the fire's ventilation and spread path.<ref name="IFEG-1.6-7" />

== Compartment fire and flashover ==

Within a compartment, flames, hot gases and heated boundaries preheat additional fuel. As more objects ignite, heat release rate and gas temperature can increase, producing stronger feedback. Spread is therefore coupled with the compartment energy balance rather than being a simple sequence of independent objects.<ref name="VR-4.3" /><ref name="Drysdale-1-95" />

[[Flashover]] represents a transition towards widespread involvement of combustible surfaces in the compartment. It can follow successive ignition and radiative preheating, but its timing depends on the complete enclosure and ventilation scenario. Spread before flashover should not be modelled with assumptions intended for the fully developed stage.<ref name="IFEG-2.4-4" /><ref name="VR-4.3" />

After widespread involvement, unburnt volatiles can leave the compartment and burn outside after mixing with air. This external flaming can expose upper facades and neighbouring surfaces. The location of heat release consequently extends beyond the original fuel and room.<ref name="Drysdale-1-95" />

[[Facade fire]] introduces exterior surfaces, cavities and cladding arrangements into the spread problem. The 2005 guidelines specifically include concealed spaces behind exterior cladding and flames projecting through windows among possible paths. These arrangements require their own geometry and material assessment rather than a room-only model.<ref name="IFEG-1.6-7" /><ref name="IFEG-1.6-3" />

== Large spaces and travelling involvement ==

Large open-plan enclosures make simultaneous burning of the whole floor unrealistic in many scenarios. Travel time between fuel packages becomes significant relative to the duration of a localised fire. Assuming the entire area burns at once can produce unrealistically high temperatures.<ref name="IFEG-2.6-12" />

The 2005 guidelines describe a grid approximation for large enclosures, using time offsets as fire moves between grid areas. Where object locations and ignition criteria are known, spatial development can instead be based on individual items. Both methods require defensible fuel arrangement and spread timing.<ref name="IFEG-2.6-12" />

Vertical shafts and concealed spaces extend the relevant enclosure beyond the room of origin. Flame and hot gas can reach other floors through these routes. Analysis limited to horizontal spread across one floor would miss them.<ref name="IFEG-1.6-7" />

Fire spread can also alter suppression and evacuation conditions. New ignition locations change detection, available escape time and the area requiring intervention. The guidelines use spread and barrier-failure times as inputs to these wider assessments.<ref name="IFEG-1.6-3" />

== Rates, acceleration and extinction ==

Spread accelerates when newly involved fuel increases heat release and preheating faster than losses and fuel depletion limit them. Quintiere compares spread time with burn time: rapid spread relative to burning can accelerate growth, while slow spread can allow the original fuel to burn out before new ignition occurs.<ref name="Quintiere-2-246" />

The process is therefore unstable rather than inherently steady. A small change in heat flux, initial temperature or fuel arrangement can shift the balance towards acceleration or extinction. Initial temperatures closer to the ignition condition reduce additional heating required ahead of the front.<ref name="Quintiere-2-247" />

Representative rates illustrate scale rather than universal values. Quintiere gives lateral or downward spread on thick solids as roughly 0.1 cm/s in order of magnitude, compared with 1 to 100 cm/s for upward spread and several other phenomena. These ranges from the 2002 handbook should not be assigned to an untested material without matching conditions.<ref name="Quintiere-2-247" />

Spread can stop when heat transfer ahead of the flame becomes insufficient, fuel becomes discontinuous or oxygen and combustion conditions no longer support propagation. Fire growth is therefore not inevitable even after a substantial initial fire.<ref name="Quintiere-2-246" /><ref name="Drysdale-1-97">Drysdale (2002), p. 1-97.</ref>

== Assessment and uncertainty ==

A spread assessment should identify the first item, potential targets, heat-transfer routes and barrier states. It then needs timing for each new ignition or failure and the corresponding changes in heat release and ventilation. This structure makes the assumed path explicit.<ref name="IFEG-1.6-3" />

Source and target data must share compatible conditions. Flame-spread tests, ignition tests and barrier tests answer different questions, and their results cannot be substituted without a model. Geometry and scale should remain visible throughout.<ref name="Quintiere-2-247" /><ref name="IFEG-1.6-7" />

Firebrand travel and large-space spread carry particular uncertainty. Precise distances and simultaneous involvement should not be asserted without supporting evidence. Sensitivity to target location and ignition timing can show whether the overall conclusion changes.<ref name="IFEG-2.6-12" />

Finally, an intact-looking barrier or a gap between objects does not prove that spread has stopped. Conduction, radiation and concealed paths can continue, and hot fuel can ignite later. The full time history is needed to distinguish delayed spread from genuine extinction.<ref name="Rockett-Milke-1-29" /><ref name="IFEG-1.6-7" />

A route-by-route review can prevent omissions. Openings require flame, radiation and debris to be considered; solid boundaries require conduction, integrity and stability; and remote targets require brands and external exposure. Each route can have a different initiation time and a different effect on ventilation.<ref name="IFEG-1.6-7" />

The treatment of glazing illustrates this timing. Radiation can cross intact glass, so ignition on the other side may precede breakage. If the glass later fails, the opening changes both the fire's air supply and the paths available to flames and smoke. These are sequential events rather than one interchangeable criterion.<ref name="IFEG-1.6-7" />

Barrier assessment also needs the receiving side. Conductive heating becomes a spread problem when combustibles are present and arranged so that they can ignite. A calculated barrier temperature alone does not describe the resulting fire without that fuel disposition and an ignition criterion.<ref name="IFEG-1.6-7" /><ref name="Kanury-2-230" />

For large floors, spatial offsets avoid an unrealistic step from local burning to total involvement. The grid method in the 2005 guidelines sums regional heat release with spread delays. Its usefulness depends on defensible offsets and a fuel layout that remains meaningful over the building's life.<ref name="IFEG-2.6-12" />

Source editions must remain visible in these methods. The International Fire Engineering Guidelines date from 2005, and the SFPE Handbook chapter from 2002. Their examples and correlations describe the evidence and assumptions available there, rather than current regulation for every country or building type.<ref name="IFEG-1.6-7" /><ref name="Quintiere-2-247" />

Sensitivity analysis can test the most uncertain links. Target separation, initial temperature, opening time and brand exposure can all change the predicted sequence. If a safety conclusion reverses when one of these assumptions varies, that dependence should be reported rather than hidden in a single spread time.<ref name="IFEG-2.6-12" /><ref name="Kanury-2-231">Kanury (2002), pp. 2-231–2-232.</ref>

After an incident, the same framework supports reconstruction. Physical evidence can be compared with candidate routes and times, including concealed spaces and delayed ignition. The first area discovered is not necessarily the first area ignited, because spread can produce several later sources.<ref name="NUREG-1805-F36">U.S. Nuclear Regulatory Commission (2005), p. F-36.</ref><ref name="Kanury-2-229" />

Spread timing can be compared with the time available for evacuation and intervention. Earlier ignition in an adjacent enclosure shortens the period before that space becomes hazardous, while delayed barrier failure can preserve separation for longer. These consequences make accurate sequencing more useful than a simple statement that spread is possible.<ref name="IFEG-1.6-3" />

The same sequencing applies to suppression. A fire that crosses a boundary can create a second area requiring detection and attack, while external flaming can expose targets beyond the original compartment. Resource and access assessments therefore need the predicted location as well as the expected heat release. Both can change while the analysis is underway.<ref name="IFEG-1.6-3" /><ref name="Drysdale-1-95" />

== See also ==

* [[Car park fire]]
* [[Cavity barrier]]
* [[Heat transfer]]
* [[Wildfire]]

== Notes ==

<references />

== References ==

* Australian Building Codes Board, National Research Council of Canada, International Code Council, & Department of Building and Housing New Zealand. (2005). ''International fire engineering guidelines'' (2005 ed.). Australian Building Codes Board.
* Drysdale, D. D. (2002). Thermochemistry. In P. J. DiNenno (Ed.), ''SFPE handbook of fire protection engineering'' (3rd ed.). National Fire Protection Association.
* Kanury, A. M. (2002). Flaming ignition of solid fuels. In P. J. DiNenno (Ed.), ''SFPE handbook of fire protection engineering'' (3rd ed.). National Fire Protection Association.
* Quintiere, J. G. (2002). Surface flame spread. In P. J. DiNenno (Ed.), ''SFPE handbook of fire protection engineering'' (3rd ed.). National Fire Protection Association.
* Rockett, J. A., & Milke, J. A. (2002). Conduction of heat in solids. In P. J. DiNenno (Ed.), ''SFPE handbook of fire protection engineering'' (3rd ed.). National Fire Protection Association.
* Tien, C. L., Lee, K. Y., & Stretton, A. J. (2002). Radiation heat transfer. In P. J. DiNenno (Ed.), ''SFPE handbook of fire protection engineering'' (3rd ed.). National Fire Protection Association.
* U.S. Nuclear Regulatory Commission. (2005). ''Fire dynamics tools: Quantitative fire hazard analysis methods for the U.S. nuclear regulatory commission fire protection inspection program'' (NUREG-1805). Author.
* Van Rossum, E. (2027). ''Introduction to Fire Safety Engineering''. Fire Safety Academy.

[[Category:Ignition & Flame Spread]]