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

2026-11-02T17:34:27Z

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

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

2026-11-02T06:25:29Z

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

← Older revision		Revision as of 07:25, 2 November 2026
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	Free convection occurs when temperature differences create the flow. Hot combustion products have lower density than surrounding cooler air, so [[Buoyancy]] drives them upwards. Cooler air moves into the region and the process continues while heating and density differences persist.<ref name="VR-5.3" /><ref name="Kandola-1-5">Kandola (2002), pp. 1-4–1-5.</ref>		Free convection occurs when temperature differences create the flow. Hot combustion products have lower density than surrounding cooler air, so [[Buoyancy]] drives them upwards. Cooler air moves into the region and the process continues while heating and density differences persist.<ref name="VR-5.3" /><ref name="Kandola-1-5">Kandola (2002), pp. 1-4–1-5.</ref>
			[[File:fse-convection-v1.svg\|thumb\|upright=1.5\|alt=Hot gas rising naturally and a fan forcing gas across a warm surface.\|Natural and forced convection use different driving influences. Based on Van Rossum (2027), §5.3.]]

	Forced convection is imposed by an external cause such as a fan, pump, wind or mechanical smoke exhaust. These forces can strengthen, redirect or oppose the flow that the fire generates. The resulting pattern depends on their combined influence rather than on one label alone.<ref name="VR-5.3" />		Forced convection is imposed by an external cause such as a fan, pump, wind or mechanical smoke exhaust. These forces can strengthen, redirect or oppose the flow that the fire generates. The resulting pattern depends on their combined influence rather than on one label alone.<ref name="VR-5.3" />
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	When the rising flow reaches a ceiling, it turns and spreads horizontally as a [[Ceiling jet]]. This hot, relatively fast-moving layer transfers heat to the ceiling and to objects near it. Flame-zone and ceiling-jet calculations are used in the guidelines to inform evaluations of fire resistance, detectors and sprinklers.<ref name="IFEG-2.5-2" />		When the rising flow reaches a ceiling, it turns and spreads horizontally as a [[Ceiling jet]]. This hot, relatively fast-moving layer transfers heat to the ceiling and to objects near it. Flame-zone and ceiling-jet calculations are used in the guidelines to inform evaluations of fire resistance, detectors and sprinklers.<ref name="IFEG-2.5-2" />
			[[File:fse-convection-v2.svg\|thumb\|upright=1.5\|alt=Rising plume turning sideways into a hot ceiling jet with surface heat transfer.\|A plume feeds a convective ceiling jet. Based on Van Rossum (2027), §5.3 and Australian Building Codes Board et al. (2005), p. 2.5-2.]]

	The ceiling jet later interacts with walls, openings and the accumulating upper layer. Its behaviour therefore connects local surface heating with wider smoke movement. Treating the plume as ending at the ceiling would omit these subsequent transport processes.<ref name="VR-5.3" /><ref name="IFEG-2.5-2" />		The ceiling jet later interacts with walls, openings and the accumulating upper layer. Its behaviour therefore connects local surface heating with wider smoke movement. Treating the plume as ending at the ceiling would omit these subsequent transport processes.<ref name="VR-5.3" /><ref name="IFEG-2.5-2" />
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	The density calculation illustrates why units require attention. Van Rossum's exhaust example uses kelvin to determine smoke density, while the temperature difference between smoke and ambient air can be evaluated in degrees Celsius. Confusing these two uses of temperature would change the estimated energy transport.<ref name="VR-5.3" />		The density calculation illustrates why units require attention. Van Rossum's exhaust example uses kelvin to determine smoke density, while the temperature difference between smoke and ambient air can be evaluated in degrees Celsius. Confusing these two uses of temperature would change the estimated energy transport.<ref name="VR-5.3" />
			[[File:fse-convection-v3.svg\|thumb\|upright=1.5\|alt=Exhaust carries 100 m³/s at 463 °C with ambient 20 °C and result 21.35 MW.\|Example of convective power carried by an exhaust flow. Based on Van Rossum (2027), §5.3.]]

	== Applying convective analysis ==		== Applying convective analysis ==

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

2026-11-01T22:27:19Z

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

New page

'''Convection''' is heat transfer associated with the movement of a gas or liquid. In a fire, hot smoke and heated air carry energy as they rise, move through openings or flow along surfaces. Convection also describes the resulting heat exchange between that moving fluid and walls, ceilings, structural members and other objects.<ref name="VR-5.3">Van Rossum (2027), §5.3.</ref>

The process combines fluid motion with molecular heat transfer and, where relevant, radiation. Atreya therefore distinguishes it conceptually from conduction and radiation: convection depends on a transporting medium in motion. Natural movement caused by the fire and forced movement caused by wind or equipment can occur together.<ref name="Atreya-1-44">Atreya (2002), p. 1-44.</ref>

Convection matters because it can transport heat far beyond the original fuel. It influences fire plumes, ceiling jets, smoke spread, structural heating and the activation of heat-responsive devices. The amount of energy transported and the heat delivered to a particular surface are related but distinct quantities.<ref name="VR-5.3" /><ref name="IFEG-2.5-2">Australian Building Codes Board et al. (2005), p. 2.5-2.</ref>

== Transport by moving gas and liquid ==

A flowing fluid carries its thermal energy with it. Hot combustion products leaving a flame therefore form a moving heat source, not only a cloud of combustion products. As this fluid travels, it can heat objects along its path and transfer energy into other rooms.<ref name="VR-5.3" />

Two descriptions are needed for different engineering questions. The first follows energy carried by a volume or mass flow and gives a rate of energy transport. The second evaluates heat flux from fluid to a surface. Van Rossum notes that these approaches produce different result forms and should not be confused.<ref name="VR-5.3" />

For energy carried by a flow, temperature, density, specific heat capacity and volumetric flow all matter. The temperature difference is taken against a defined reference, such as incoming ambient air. Changing any of these inputs alters the calculated energy transport.<ref name="VR-5.3" />

For surface heating, the temperature difference between gas and surface is combined with a convective heat-transfer coefficient. That coefficient summarises the effect of fluid properties and flow conditions. It is not a universal constant for air, smoke and water, or for every orientation and velocity.<ref name="VR-5.3" /><ref name="Atreya-1-45">Atreya (2002), p. 1-45.</ref>

== Free, forced and mixed convection ==

Free convection occurs when temperature differences create the flow. Hot combustion products have lower density than surrounding cooler air, so [[Buoyancy]] drives them upwards. Cooler air moves into the region and the process continues while heating and density differences persist.<ref name="VR-5.3" /><ref name="Kandola-1-5">Kandola (2002), pp. 1-4–1-5.</ref>

Forced convection is imposed by an external cause such as a fan, pump, wind or mechanical smoke exhaust. These forces can strengthen, redirect or oppose the flow that the fire generates. The resulting pattern depends on their combined influence rather than on one label alone.<ref name="VR-5.3" />

Mixed convection is common in buildings. A hot plume rises naturally while ordinary ventilation, wind at openings or a smoke-control system changes the surrounding pressure field. Even equipment not designed as fire equipment can affect heat and smoke transport.<ref name="VR-5.3" /><ref name="VR-6.6">Van Rossum (2027), §6.6.</ref>

Atreya further distinguishes flows inside bodies, such as pipes, from external flows around objects. Fire assessments commonly emphasise external natural convection around surfaces and within rooms. The chosen geometry determines which measured relationships and boundary conditions are appropriate.<ref name="Atreya-1-44" />

== Fire plumes and ceiling jets ==

A [[Fire plume]] forms as hot gases rise above a fire. Turbulent motion draws surrounding air into this rising stream. The plume's mass flow consequently increases while its temperature and combustion-product concentrations become more diluted.<ref name="VR-5.3" /><ref name="IFEG-2.5-2" />

Entrained air can greatly exceed the mass of burned fuel in the rising flow. The International Fire Engineering Guidelines therefore allow the fuel mass flow to be neglected in particular smoke-development methods. This does not mean the fuel is unimportant; its heat release establishes the buoyant flow that entrains the air.<ref name="IFEG-2.5-2" />

A small fire can consequently produce a much larger flow of warm, diluted smoke. Convective heat transport is not proportional only to the visible flame volume. Air entrainment, plume height and surrounding geometry influence the quantity delivered upwards.<ref name="VR-5.3" />

When the rising flow reaches a ceiling, it turns and spreads horizontally as a [[Ceiling jet]]. This hot, relatively fast-moving layer transfers heat to the ceiling and to objects near it. Flame-zone and ceiling-jet calculations are used in the guidelines to inform evaluations of fire resistance, detectors and sprinklers.<ref name="IFEG-2.5-2" />

The ceiling jet later interacts with walls, openings and the accumulating upper layer. Its behaviour therefore connects local surface heating with wider smoke movement. Treating the plume as ending at the ceiling would omit these subsequent transport processes.<ref name="VR-5.3" /><ref name="IFEG-2.5-2" />

== Coefficients, conservation and measurement ==

A convective [[Heat transfer]] coefficient has units of watts per square metre-kelvin when used for surface heat flux. Van Rossum also describes its reciprocal as a surface resistance. A larger coefficient means less resistance under the selected flow model, but it does not provide the total heat flow without area and temperature difference.<ref name="VR-5.3" />

The coefficient summarises processes within the boundary layer rather than a fixed property of the fluid alone. Surface orientation, roughness, flow velocity, turbulence and temperature-dependent properties can all influence it. Published coefficients and correlations therefore carry an application range.<ref name="Atreya-1-45" /><ref name="VR-5.3" />

Conservation laws provide the underlying framework. Atreya identifies conservation of mass, momentum and energy, supplemented by relationships for viscosity, conduction and diffusion. For turbulent flow, this framework often guides empirical correlations rather than yielding a simple universal solution.<ref name="Atreya-1-45" />

Measurement must match the intended result. A gas-temperature reading alone does not determine the surface coefficient, and a surface heat-flux reading does not directly give the energy carried through an opening. Flow rate, density and reference temperature are needed for the transported-energy description.<ref name="VR-5.3" />

The density calculation illustrates why units require attention. Van Rossum's exhaust example uses kelvin to determine smoke density, while the temperature difference between smoke and ambient air can be evaluated in degrees Celsius. Confusing these two uses of temperature would change the estimated energy transport.<ref name="VR-5.3" />

== Applying convective analysis ==

Convective transport can ignite light combustible materials at a considerable distance from the original fire. Van Rossum identifies this possibility when hot gases travel through buildings. The receiving material still needs a suitable time-dependent exposure and ignition condition; transport alone does not prove ignition.<ref name="VR-5.3" /><ref name="IFEG-2.4-4">Australian Building Codes Board et al. (2005), p. 2.4-4.</ref>

Radiation can act alongside convection along the same path. A surface may receive radiation from a flame or hot gas layer while hot gas flows over it. Calculating only one contribution can underestimate exposure, while adding values based on different reference areas or times can create another error.<ref name="VR-5.4">Van Rossum (2027), §5.4.</ref><ref name="Tien-1-73">Tien, Lee, and Stretton (2002), p. 1-73.</ref>

System operation changes the pressure field and therefore the convective path. Smoke exhaust can remove energy, ordinary ventilation can redistribute it, and wind can alter flow through openings. The analysis needs a defined system state rather than an assumption that all equipment either stops or operates as intended.<ref name="VR-6.6" />

Plume models likewise apply to specified geometries. The 2005 guidelines describe axisymmetric models for fires away from walls, where air can be entrained from all sides. A wall, corner or obstruction changes that symmetry and should trigger a different treatment rather than unrestricted use of the same entrainment result.<ref name="IFEG-2.5-2" />

Sensitivity to heat release rate, gas temperature and flow rate should be made visible. These quantities vary during fire growth and decay, so a single steady calculation cannot show when a detector, structural element or remote fuel package reaches a critical condition. Time selection is part of the engineering assumption.<ref name="VR-5.1" /><ref name="IFEG-2.5-2" />

Flow determination comes before surface heat transfer. Van Rossum emphasises that the gas movement must first be described, after which its thermal effect can be calculated. Assuming a heat-transfer coefficient before establishing whether the surface encounters plume, ceiling jet or slower room gas reverses that logic.<ref name="VR-5.3" />

Natural and forced components can also change differently with time. A growing fire can strengthen buoyant flow while a fan operates at a fixed setting or a smoke-control system changes state. The combined flow therefore cannot always be scaled from fire size alone.<ref name="VR-5.3" /><ref name="VR-6.6" />

Results should be checked against their physical meaning. A surface heat flux needs a receiving area to become total heat flow, while transported power needs a defined flow crossing. Comparing these outcomes without conversion would mix local exposure with energy passing through the building.<ref name="VR-5.3" />

== Boundary layers and turbulence ==

Fluid immediately at a solid surface is approximately stationary, while velocity increases away from the surface. The resulting boundary layer contains strong velocity and temperature gradients. Heat crossing from the main gas flow to the surface must pass through this region.<ref name="VR-5.3" />

In laminar flow, fluid moves in comparatively orderly layers with limited crosswise mixing. In turbulent flow, eddies transport fluid and energy across the main flow direction. Van Rossum explains that this stronger mixing generally increases convective heat transfer to a surface.<ref name="VR-5.3" />

Turbulence is common near fires, openings and obstacles. Velocity, geometry and fluid properties all affect whether flow remains laminar or becomes turbulent. A coefficient obtained for one configuration cannot be transferred to another merely because both involve hot air.<ref name="VR-5.3" /><ref name="Atreya-1-45" />

The convective [[Heat flux]] to a surface depends on the gas-to-surface temperature difference and the heat-transfer coefficient. Higher gas temperature can increase this driving difference, while greater turbulence can increase the coefficient. Both effects must be considered when comparing exposures.<ref name="VR-5.3" />

At the surface itself, molecular conduction remains part of the process even when the wider flow is turbulent. Convection therefore does not eliminate conduction; it changes the temperature and flow conditions under which that local transfer occurs.<ref name="Atreya-1-44" /><ref name="Atreya-1-45" />

== Convection in smoke spread ==

Convection carries heated combustion products into upper parts of enclosures and through available openings. The resulting [[Smoke movement]] can expose locations remote from the fire. This remote exposure includes heat as well as reduced visibility and combustion-product concentration.<ref name="VR-5.3" /><ref name="IFEG-2.5-2" />

Van Rossum gives an example in which a smoke-exhaust flow of 100 m³/s, with smoke at 463 °C and surroundings at 20 °C, transports approximately 21.35 MW under the stated assumptions. The example uses air properties and a calculated density, and illustrates that a large volume flow can carry substantial power.<ref name="VR-5.3" />

The example is not a default value for an exhaust system. Actual smoke temperature, density, flow rate and reference conditions vary during a fire. It demonstrates the meaning of convective energy transport rather than providing a design result for another building.<ref name="VR-5.3" />

Wind and mechanical systems can modify or reverse expected paths. Natural pressure differences from heating occur together with expansion, stack effect and equipment-induced pressures. The whole pressure field must therefore be represented when assessing flow through openings.<ref name="VR-6.6" />

== Engineering use and limitations ==

Convection calculations support estimates of upper-layer energy, smoke production, boundary heating and device exposure. The required input can include heat release rate, plume entrainment, gas temperature and surface conditions. These inputs are often time-dependent and uncertain.<ref name="IFEG-2.5-2" /><ref name="VR-5.1">Van Rossum (2027), §5.1.</ref>

A steady surface calculation can provide an order-of-magnitude estimate, but a real fire changes both source and receiver temperatures. Assuming a fixed heat-transfer coefficient can hide these changes. A more detailed transient model is needed when the timing of exposure is central to the result.<ref name="VR-5.1" /><ref name="VR-5.3" />

Convective heat transfer is also not simply a direct result of air temperature. Two gas streams at the same temperature can deliver different heat fluxes because their velocities, turbulence and surface geometries differ. Conversely, a high coefficient cannot create heat transfer without a temperature difference.<ref name="VR-5.3" />

Finally, convection and smoke toxicity are separate aspects of the same transport. Dilution by entrained air can reduce concentration while increasing total mass flow. A diluted stream can still carry substantial energy and combustion products to another location.<ref name="VR-5.3" /><ref name="IFEG-2.5-2" />

The direction of heat exchange can reverse as surface and gas temperatures change. A construction that initially absorbs heat from smoke can later lose heat to cooler gas. Retaining the sign and time history of the temperature difference prevents this reversal from being lost in a single positive design number.<ref name="VR-5.3" /><ref name="Rockett-Milke-1-29">Rockett and Milke (2002), p. 1-29.</ref>

This changing exchange also affects interpretation of measurements. A sensor can respond to the gas, to a heated surface or to both, depending on its position and construction. Interpreting that response as convective exposure requires a clear account of the local flow and thermal environment.<ref name="IFEG-2.5-2" /><ref name="VR-5.3" />

A complete description also states whether the analysis concerns instantaneous conditions or an average over time. Averaging can smooth peaks that matter for ignition or device response, while an instantaneous value can obscure the total energy transported. The choice must follow the fire-safety question rather than the convenience of the available data.<ref name="VR-5.1" /><ref name="IFEG-2.5-2" />

== See also ==

* [[Adiabatic surface temperature]]
* [[Biot number]]
* [[Heat transfer]]

== Notes ==

<references />

== References ==

* Atreya, A. (2002). Convection heat transfer. In P. J. DiNenno (Ed.), ''SFPE handbook of fire protection engineering'' (3rd ed.). National Fire Protection Association.
* 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.
* Kandola, B. S. (2002). Introduction to mechanics of fluids. 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.
* Van Rossum, E. (2027). ''Introduction to Fire Safety Engineering''. Fire Safety Academy.

[[Category:Physics & Heat Transfer]]

Convection - Revision history

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

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

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