Ignition source - Revision history

Jan: Remove links to pages that do not exist; retain displayed text (wiki-wide link audit).

2026-11-02T21:33:59Z

Remove links to pages that do not exist; retain displayed text (wiki-wide link audit).

← Older revision		Revision as of 22:33, 2 November 2026
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	== Hazardous areas and prevention ==		== Hazardous areas and prevention ==

	For [[Hazardous area classification]], the source inventory has to be related to the potential presence of a flammable atmosphere. The IFEG gas and vapour discussion identifies mixture concentration as a separate part of ignition prevention. Removing one possible source does not establish that the atmosphere is outside its flammable range.<ref name="IFEG-3.3-2" />		For Hazardous area classification, the source inventory has to be related to the potential presence of a flammable atmosphere. The IFEG gas and vapour discussion identifies mixture concentration as a separate part of ignition prevention. Removing one possible source does not establish that the atmosphere is outside its flammable range.<ref name="IFEG-3.3-2" />

	Prevention can address an activity, the flammable atmosphere or the separation of fuel from energy. Detection and response act on a fire after ignition. The suitable combination depends on whether the source is permanent equipment, a temporary task or an internal reaction. One generic prohibition cannot cover all these mechanisms.<ref name="IFEG-2.4-4" /><ref name="NUREG-6850-6-21" />		Prevention can address an activity, the flammable atmosphere or the separation of fuel from energy. Detection and response act on a fire after ignition. The suitable combination depends on whether the source is permanent equipment, a temporary task or an internal reaction. One generic prohibition cannot cover all these mechanisms.<ref name="IFEG-2.4-4" /><ref name="NUREG-6850-6-21" />
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	* [[Fire triangle]]		* [[Fire triangle]]
	* [[Photovoltaic system fire]]		* Photovoltaic system fire

	== Notes ==		== Notes ==

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

2026-11-02T17:47:56Z

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

Show changes

Sanne: Add diagrams fse-ignition-source-v2.svg, fse-ignition-source-v3.svg (level-1 visual plan)

2026-11-02T07:16:11Z

Add diagrams fse-ignition-source-v2.svg, fse-ignition-source-v3.svg (level-1 visual plan)

← Older revision		Revision as of 08:16, 2 November 2026
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	Ignition sources can also occur in sequence. NUREG-1805 describes a burning wastebasket becoming a source for a chair, after which the chair can ignite other fuel. The initial device and subsequent burning objects therefore play different roles in the developing fire. Every later burning object must be assessed both as a target and as a potential new source.<ref name="NUREG-1805-F36">U.S. Nuclear Regulatory Commission (2005), p. F-36.</ref>		Ignition sources can also occur in sequence. NUREG-1805 describes a burning wastebasket becoming a source for a chair, after which the chair can ignite other fuel. The initial device and subsequent burning objects therefore play different roles in the developing fire. Every later burning object must be assessed both as a target and as a potential new source.<ref name="NUREG-1805-F36">U.S. Nuclear Regulatory Commission (2005), p. F-36.</ref>
			[[File:fse-ignition-source-v2.svg\|thumb\|upright=1.5\|alt=Wastebasket ignites a chair and the chair becomes a source for another object.\|Burning objects can become later ignition sources. Based on U.S. Nuclear Regulatory Commission (2005), p. F-36.]]

	== Flames, sparks and hot surfaces ==		== Flames, sparks and hot surfaces ==
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	The critical condition depends on material chemistry, ambient temperature, size and shape. Larger bodies can favour runaway because heat is retained more effectively, while higher ambient temperature reduces the relative thermal driving force for cooling. No single external ignition device is required in these cases.<ref name="Gray-2-211" /><ref name="Gray-2-212">Gray (2002), p. 2-212.</ref>		The critical condition depends on material chemistry, ambient temperature, size and shape. Larger bodies can favour runaway because heat is retained more effectively, while higher ambient temperature reduces the relative thermal driving force for cooling. No single external ignition device is required in these cases.<ref name="Gray-2-211" /><ref name="Gray-2-212">Gray (2002), p. 2-212.</ref>
			[[File:fse-ignition-source-v3.svg\|thumb\|upright=1.5\|alt=Heat generated inside a body exceeds losses and produces internal runaway.\|Self-heating can create an internal ignition source. Based on Gray (2002), pp. 2-211–2-212.]]

	Preheated products add another variable. Hot laundry, recently manufactured chipboard and hot porous food products require attention to the material's own stacking temperature as well as ambient conditions. Gray explains that time to ignition can be much shorter for preheated bodies than for material stacked at ambient temperature.<ref name="Gray-2-211" /><ref name="Gray-2-213">Gray (2002), p. 2-213.</ref>		Preheated products add another variable. Hot laundry, recently manufactured chipboard and hot porous food products require attention to the material's own stacking temperature as well as ambient conditions. Gray explains that time to ignition can be much shorter for preheated bodies than for material stacked at ambient temperature.<ref name="Gray-2-211" /><ref name="Gray-2-213">Gray (2002), p. 2-213.</ref>

Sanne: Add diagram fse-ignition-source-v1.svg (level-1 visual plan)

2026-11-02T06:25:31Z

Add diagram fse-ignition-source-v1.svg (level-1 visual plan)

← Older revision		Revision as of 07:25, 2 November 2026
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	The target is the fuel exposed to the source. Its physical and chemical properties determine how it responds, including conductivity, heat capacity, decomposition behaviour and geometry. A source-target description should retain these properties rather than treating ignition as a property of the source alone.<ref name="Kanury-2-229">Kanury (2002), p. 2-229.</ref>		The target is the fuel exposed to the source. Its physical and chemical properties determine how it responds, including conductivity, heat capacity, decomposition behaviour and geometry. A source-target description should retain these properties rather than treating ignition as a property of the source alone.<ref name="Kanury-2-229">Kanury (2002), p. 2-229.</ref>
			[[File:fse-ignition-source-v1.svg\|thumb\|upright=1.5\|alt=Source heating a target while vapour, oxygen and heat losses shape ignition.\|Ignition depends on source-target interaction and heat loss. Based on Kanury (2002), pp. 2-230–2-232.]]

	For a solid, incoming energy is partitioned into internal conduction, reradiation and convection to adjacent gas. Moisture evaporation and pyrolysis then modify the response. The source can be steady in the model while the net heating of the target changes substantially over time.<ref name="Kanury-2-232" />		For a solid, incoming energy is partitioned into internal conduction, reradiation and convection to adjacent gas. Moisture evaporation and pyrolysis then modify the response. The source can be steady in the model while the net heating of the target changes substantially over time.<ref name="Kanury-2-232" />

Jan: New FSE wiki article: Ignition source (written by Kimi Code CLI)

2026-11-01T22:51:14Z

New FSE wiki article: Ignition source (written by Kimi Code CLI)

New page

An '''Ignition source''' is a localised supply of energy or reactive condition that initiates combustion in a fuel-oxidiser system. Flames, sparks, heated wires, incandescent particles and hot surfaces can act as sources, while internal chemical self-heating can create the initiating condition within a material. Effectiveness depends on the fuel, mixing and heat losses at the point of contact. The same source can initiate a gas-phase reaction, evaporate a liquid or supply energy for decomposition in a solid. Identifying that role clarifies the relevant source properties and target conditions, while separating prevention of the initial reaction from control of the developing fire and its wider consequences.<ref name="Kanury-2-230">Kanury (2002), p. 2-230.</ref><ref name="Gray-2-211">Gray (2002), p. 2-211.</ref>

The source is only one part of [[Ignition]]. A flammable mixture and suitable thermal conditions must also be present. A source that is too small or loses energy too quickly can fail, while a modest flame or spark can initiate a much larger fire when the surrounding mixture is favourable.<ref name="Kanury-2-232">Kanury (2002), p. 2-232.</ref><ref name="IFEG-2.4-4">Australian Building Codes Board et al. (2005), p. 2.4-4.</ref>

Ignition sources can also occur in sequence. NUREG-1805 describes a burning wastebasket becoming a source for a chair, after which the chair can ignite other fuel. The initial device and subsequent burning objects therefore play different roles in the developing fire. Every later burning object must be assessed both as a target and as a potential new source.<ref name="NUREG-1805-F36">U.S. Nuclear Regulatory Commission (2005), p. F-36.</ref>

== Flames, sparks and hot surfaces ==

A small pilot flame initiates a reaction in an already suitable fuel-air mixture. Its role is not necessarily to heat the whole fuel body or generate all the pyrolysis gases. Once the reaction begins, it can propagate away from the pilot through the connected mixture.<ref name="Kanury-2-230" />

Sparks and heated filaments can perform a similar pilot function. Their effect depends on energy, size, exposure time and the thermal and chemical properties of the mixture. Heat loss to surrounding gas and surfaces can quench the initial reaction before propagation develops.<ref name="Kanury-2-232" />

Hot surfaces create a different exposure because they can heat a fuel continuously. Surface temperature alone does not determine ignition: contact area, airflow, fuel thickness and exposure duration affect the energy balance. A small hot object can therefore produce a different outcome from a large surface at the same nominal temperature.<ref name="Kanury-2-231">Kanury (2002), pp. 2-231–2-232.</ref>

Open flames introduce both a pilot and a heat source for further fuel production. They can ignite a gas mixture rapidly or heat liquids and solids until vapour and pyrolysis products become involved. These distinct roles should be identified when reconstructing a fire scenario.<ref name="Kanury-2-230" /><ref name="VR-4.1">Van Rossum (2027), §4.1.</ref>

Electrical faults can produce local overheating or arcing. In one NUREG-1805 case, improperly grounded equipment caused fault current to overheat conductors and ignite material in two locations. This nuclear-plant incident illustrates a specific electrical sequence, not a universal frequency for cable ignition.<ref name="NUREG-1805-H24">U.S. Nuclear Regulatory Commission (2005), pp. H-24–H-25.</ref>

Temporary activities change both the timing and location of source exposure. Equipment may be brought into a compartment for a limited task, used near transient combustibles and removed later. Assessment should therefore describe the work period and housekeeping state rather than treating the annual average layout as sufficient.<ref name="NUREG-6850-6-21" />

The response pathway also needs to be credible. NUREG/CR-6850 links a continuous watch with quicker human detection, while fixed detection can dominate in unoccupied spaces. A watch is most relevant when the person is present, attentive and able to initiate suppression, rather than existing only as an administrative entry.<ref name="NUREG-6850-11-28" />

Administrative prohibition can reduce the frequency of a temporary source. The nuclear guidance assigns a low maintenance influence where welding and cutting are prohibited during power operation. This example concerns a specialised analytical method, but it illustrates how a procedure can change the likelihood of the source being present at all.<ref name="NUREG-6850-6-22" />

[[Hot work]] includes activities using heat, sparks or open flame, such as cutting, welding and grinding. These activities can introduce an ignition source into areas where it is not normally present. Fuel arrangement and work procedures therefore form part of the source assessment.<ref name="NUREG-1805-F37">U.S. Nuclear Regulatory Commission (2005), p. F-37.</ref><ref name="NUREG-6850-6-21">U.S. Nuclear Regulatory Commission (2005), p. 6-21.</ref>

Oxygen-acetylene torches provide a particularly intense source. NUREG-1805 gives a hottest-flame value of approximately 3,500 °C for the torch conditions described. That value concerns the flame itself and does not equal the temperature reached by every target or the energy required for ignition.<ref name="NUREG-1805-3-9">U.S. Nuclear Regulatory Commission (2005), p. 3-9.</ref>

The 2005 nuclear fire-analysis guidance links welding and cutting frequency with maintenance activity, hot-work procedures and housekeeping. It treats these as plant-specific influences rather than fixed properties of a compartment. Similar reasoning applies to temporary work in other settings, although the numerical bins are specific to the nuclear method.<ref name="NUREG-6850-6-21" />

A continuous fire watch can shorten detection time when hot work ignites fuel. The same guidance states that such fires are likely to be detected quickly when a watch has been posted. This is a response measure, not proof that ignition has been prevented.<ref name="NUREG-6850-11-28">U.S. Nuclear Regulatory Commission (2005), p. 11-28.</ref>

== Ignition energy and flammable atmospheres ==

[[Minimum ignition energy]] is the lowest energy associated with ignition of a specified fuel-oxidiser mixture under stated conditions. It is relevant when a spark or other short-duration source contacts a flammable atmosphere. Composition, temperature, pressure and flow can change the requirement.<ref name="Kanury-2-232" /><ref name="Beyler-2-172">Beyler (2002), p. 2-172.</ref>

The 2005 International Fire Engineering Guidelines note that fuel-air mixtures within the flammable region can often be ignited by sources of only millijoules. The actual value depends on the mixture and test method. A small electrical or static source can therefore be significant even without a large hot surface.<ref name="IFEG-3.3-1">Australian Building Codes Board et al. (2005), p. 3.3-1.</ref>

Flammability limits remain essential when interpreting this energy. Outside the propagating range, a source can create local combustion without a flame travelling through the wider mixture. Beyler distinguishes this local effect from sustained flame propagation within the limits.<ref name="Beyler-2-172" />

Prevention commonly keeps gas or vapour concentrations well below the lower flammable limit. The guidelines caution against relying on a mixture above the upper limit because subsequent dilution can return it to the flammable region. Ignition-source control works together with concentration control rather than replacing it.<ref name="IFEG-3.3-1" />

== Self-heating as an internal source ==

[[Self-heating]] occurs when chemical reactions inside a material generate energy faster than it can be lost. The material then supplies part of the initiating heat itself. Poor thermal conductivity and insulating containers can help retain this energy.<ref name="Gray-2-211" />

The critical condition depends on material chemistry, ambient temperature, size and shape. Larger bodies can favour runaway because heat is retained more effectively, while higher ambient temperature reduces the relative thermal driving force for cooling. No single external ignition device is required in these cases.<ref name="Gray-2-211" /><ref name="Gray-2-212">Gray (2002), p. 2-212.</ref>

Preheated products add another variable. Hot laundry, recently manufactured chipboard and hot porous food products require attention to the material's own stacking temperature as well as ambient conditions. Gray explains that time to ignition can be much shorter for preheated bodies than for material stacked at ambient temperature.<ref name="Gray-2-211" /><ref name="Gray-2-213">Gray (2002), p. 2-213.</ref>

Spontaneous runaway often begins at the centre of a low-conductivity body. Charring or ash can therefore be found inside while the exterior appears less affected. This evidence can inform investigation, but it must be assessed alongside other possible ignition sources and preheating.<ref name="Gray-2-212" />

== Source and target interaction ==

The target is the fuel exposed to the source. Its physical and chemical properties determine how it responds, including conductivity, heat capacity, decomposition behaviour and geometry. A source-target description should retain these properties rather than treating ignition as a property of the source alone.<ref name="Kanury-2-229">Kanury (2002), p. 2-229.</ref>

For a solid, incoming energy is partitioned into internal conduction, reradiation and convection to adjacent gas. Moisture evaporation and pyrolysis then modify the response. The source can be steady in the model while the net heating of the target changes substantially over time.<ref name="Kanury-2-232" />

Mixing has a dual effect. It is necessary to bring fuel vapour and oxygen together, but it can also cool and dilute the mixture. Spontaneous ignition needs both suitable composition and sufficient thermal condition at the same location. More airflow is therefore not always more favourable.<ref name="Kanury-2-232" />

For piloted ignition, the pilot can be small relative to the target because it only initiates the reaction. It still cannot be infinitely small: reaction can be quenched if the source region does not exceed the mixture's critical dimensions and energy requirements. The relevant threshold belongs to the whole mixture-source arrangement.<ref name="Kanury-2-232" />

== Fire statistics and frequency analysis ==

[[Fire statistics]] can show which sources and first-ignited materials occur in reported incidents. Such evidence helps prioritise prevention and estimate ignition frequencies. It does not by itself establish the cause of an individual fire or the probability of ignition during one particular exposure.<ref name="IFEG-2.4-4" /><ref name="NUREG-6850-6-21" />

Nuclear fire probabilistic risk analysis uses detailed ignition-source counts and weighting factors. The method considers equipment, maintenance, occupancy and storage when assigning compartment-specific influences. These categories belong to US nuclear power plant analysis and should not be presented as universal building values.<ref name="NUREG-6850-6-21" />

The 2005 guidance recommends work-order counts and staff information to assess maintenance-related transient fires. It separately addresses welding and cutting, including procedures that prohibit these activities during power operation. This demonstrates how administrative controls can alter the frequency assigned to a source scenario.<ref name="NUREG-6850-6-22">U.S. Nuclear Regulatory Commission (2005), p. 6-22.</ref>

Data quality remains important. The 2005 guidelines note that ignition statistics can support quantitative frequency studies and qualitative comparisons, but general prediction of ignition potential remained uncertain. Source identification and statistical frequency answer different questions.<ref name="IFEG-2.4-4" />

== Hazardous areas and prevention ==

[[Hazardous area classification]] assesses where flammable atmospheres may occur and informs control of potential ignition sources. Release rate, ventilation and the extent of the flammable region are needed alongside the source inventory. A room containing electrical equipment is not described adequately without these conditions.<ref name="IFEG-3.3-1" />

Prevention can eliminate or substitute an activity, control the flammable atmosphere, separate fuel from energy or introduce detection and response. The suitable combination depends on whether the source is permanent equipment, a temporary task or an internal reaction. One generic prohibition cannot cover all these mechanisms.<ref name="IFEG-2.4-4" /><ref name="NUREG-6850-6-21" />

Hot-work procedures provide a temporary-source example. Housekeeping reduces available fuel, work controls affect source generation and a fire watch reduces response time. Evaluating only the torch or spark would miss the wider scenario that determines whether a small ignition becomes a damaging fire.<ref name="NUREG-6850-6-21" /><ref name="NUREG-6850-11-28" />

For self-heating storage, source prevention can involve size, stacking temperature and heat dissipation rather than electrical exclusion. The source is distributed within the fuel body, so separating it from the fuel is not a meaningful description. Geometry and storage conditions become the principal controls.<ref name="Gray-2-211" />

== Fire investigation ==

[[Fire investigation]] seeks to establish the sequence and conditions of ignition from evidence. Potential sources are evaluated together with target materials, heat transfer and subsequent fire development. Finding a device capable of ignition is not alone proof that it initiated the event.<ref name="Kanury-2-229" /><ref name="Gray-2-212" />

Electrical evidence can include fault paths and conductor damage. The Palo Verde incident in NUREG-1805 linked simultaneous fires to a common overheated conductor caused by grounding faults. The value of that example lies in tracing the complete sequence rather than assigning every cable fire to an electrical fault without evidence.<ref name="NUREG-1805-H24" />

Self-heating evidence can include deep central charring and a comparatively intact exterior. Gray nevertheless stresses the need to consider solar exposure, recent processing and other preheating. Unknown cause can also be more common in large destructive fires because evidence is lost.<ref name="Gray-2-211" /><ref name="Gray-2-212" />

A reliable investigation distinguishes initial ignition from later sources. A burning object found at one location may have started the fire there or may itself have been ignited by an earlier object. Reconstructing this order prevents the first discovered burning item from being misidentified as the original igniter.<ref name="NUREG-1805-F36" />

== Limits and common misunderstandings ==

A high source temperature does not guarantee ignition. Energy transfer rate, exposure time, target response and heat loss all matter. Conversely, a low-energy spark can ignite a suitable gas mixture. Source temperature and minimum ignition energy are not interchangeable measures.<ref name="Kanury-2-232" /><ref name="IFEG-3.3-1" />

An ignition source is not necessarily external to the fuel. Self-heating and spontaneous runaway can develop within a reactive material. Treating every fire as requiring a separate flame, spark or hot device excludes this established pathway.<ref name="Gray-2-211" />

A fire watch does not remove the ignition source or prevent every ignition. It provides observation and faster response, while fuel and source controls address prevention. These roles should remain distinct in assessment and reporting.<ref name="NUREG-6850-11-28" />

Finally, the first source is not always the largest. Small initial events can ignite progressively larger fuel packages, while a large energy release can fail to create persistent combustion if heat losses dominate. The entire sequence determines the eventual fire.<ref name="Kanury-2-230" /><ref name="NUREG-1805-F36" />

== See also ==

* [[Fire triangle]]
* [[Photovoltaic system fire]]
* [[Ignition]]

== 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.
* Beyler, C. L. (2002). Flammability limits of premixed and diffusion flames. In P. J. DiNenno (Ed.), ''SFPE handbook of fire protection engineering'' (3rd ed.). National Fire Protection Association.
* Gray, B. (2002). Spontaneous combustion and self-heating. 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.
* 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.
* U.S. Nuclear Regulatory Commission. (2005). ''Fire probabilistic risk assessment methods enhancements'' (NUREG/CR-6850, Vol. 2). Author.
* Van Rossum, E. (2027). ''Introduction to Fire Safety Engineering''. Fire Safety Academy.

[[Category:Ignition & Flame Spread]]