Deflagration - Wikipedia, The Free Encyclopedia

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    A log in a fireplace.

    DeflagrationFrom Wikipedia, the free encyclopedia

    Deflagration[1] (Lat: de + flagrare, "to burn down") is a term

    describing subsonic combustion propagating through heat transfer; hot

    burning material heats the next layer of cold material and ignites it.

    Most "fire" found in daily life, from flames to explosions, isdeflagration. Deflagration is different from detonation, which is

    supersonic and propagates through shock.

    Deflagration is a rapid high energy release combustion event that

    propagates through a gas or an explosive material at subsonic speeds,

    driven by the transfer of heat.

    Contents

    1 Applications

    2 Oil/wax fires and water

    3 Flame physics

    4 Damaging deflagration events

    5 See also

    6 References

    Applications

    In engineering applications, deflagrations are easier to control than detonations. Consequently, they are better

    suited when the goal is to move an object (a bullet in a gun, or a piston in an internal combustion engine) with the

    force of the expanding gas. Typical examples of deflagrations are the combustion of a gas-air mixture in a gas

    stove or a fuel-air mixture in an internal combustion engine, and the rapid burning of gunpowder in a firearm or

    of pyrotechnic mixtures in fireworks. Deflagration systems and products can also be used in mining, demolition

    and stone quarrying via gas pressure blasting as a beneficial alternative to high explosives.

    Oil/wax fires and water

    Adding water to a burning hydrocarbon such as oil or wax produces a deflagration. The water boils rapidly and

    ejects the burning material as a fine spray of droplets. A deflagration then occurs as the fine mist of oil ignites

    and burns extremely rapidly. These are particularly common in chip pan fires, which are responsible for one in

    five household fires in Britain.[2]

    Flame physics

    The underlying flame physics can be understood with the help of an idealized model consisting of a uniform one-

    dimensional tube of unburnt and burned gaseous fuel, separated by a thin transitional region of width in which

    the burning occurs. The burning region is commonly referred to as the flame or flame front. In equilibrium,

    thermal diffusion across the flame front is balanced by the heat supplied by burning.

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    There are two characteristic timescales which are important here. The first is the thermal diffusion timescale ,

    which is approximately equal to

    ,

    where is the thermal diffusivity. The second is the burning timescale that strongly decreases with

    temperature, typically as

    ,

    where is the activation barrier for the burning reaction and is the temperature developed as the result o

    burning; the value of this so-called "flame temperature" can be determined from the laws of thermodynamics.

    For a stationary moving deflagration front, these two timescales are equal: The heat generated by burning is

    equal to the heat carried away by heat transfer. This makes it possible to calculate the characteristic width of

    the flame front:

    ,

    thus

    .

    Now, the thermal flame front propagates at a characteristic speed , which is simply equal to the flame width

    divided by the burn time:

    .

    This simplified model neglects the change of temperature and thus the burning rate across the deflagration front.

    This model also neglects the possible influence of turbulence. As a result, this derivation gives only the laminar

    flame speed -- hence the designation .

    Damaging deflagration events

    Damage to buildings, equipment and people can result from a large-scale, short-duration deflagration. The

    potential damage is primarily a function of the total amount of fuel burned in the event (total energy available),

    the maximum flame velocity that is achieved, and the manner in which the expansion of the combustion gases iscontained.

    In free-air deflagrations, there is a continuous variation in deflagration effects relative to the maximum flame

    velocity. When flame velocities are low, the effect of a deflagration is to release heat. Some authors use the term

    flash fire to describe these low-speed deflagrations. At flame velocities near the speed of sound, the energy

    released is in the form of pressure and the results resemble a detonation. Between these extremes both heat and

    pressure are released.

    When a low-speed deflagration occurs within a closed vessel or structure, pressure effects can produce damage

    due to expansion of gases as a secondary effect. The heat released by the deflagration causes the combustion

    gases and excess air to expand thermally. The net result is that the volume of the vessel or structure must expand

    to accommodate the hot combustion gases, or the vessel must be strong enough to withstand the additional

    internal pressure, or it fails, allowing the gases to escape. The risks of deflagration inside waste storage drums is

    a growing concern in storage facilities.

    https://en.wikipedia.org/wiki/Detonationhttps://en.wikipedia.org/wiki/Flash_firehttps://en.wikipedia.org/wiki/Laminar_flame_speedhttps://en.wikipedia.org/wiki/Turbulencehttps://en.wikipedia.org/wiki/Heat_transferhttps://en.wikipedia.org/wiki/Thermal_diffusivity
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    See also

    Pressure piling

    References

    1. ^ http://www.hutchisonrodway.co.nz/Auckland/Technical/Glossary-D-H2. ^ UK Fire Service advice (http://www.fireservice.co.uk/safety/chip-pans) on chip pan fires

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