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Introduction to Fire Safety Management

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<strong>Introduction</strong> <strong>to</strong> <strong>Fire</strong> <strong>Safety</strong> <strong>Management</strong><br />

In contrast the speed of travel of the fl ame front<br />

during a de<strong>to</strong>nation is supersonic. In a fuel/air cloud a<br />

de<strong>to</strong>nation wave will move at speeds of between 1500<br />

and 2000 m/s and the peak pressure in front of the<br />

fl ame can reach 15 <strong>to</strong> 20 bar. This pressure front when<br />

enclosed can cause substantial damage including the<br />

collapse of structures.<br />

In an explosion of a fuel/air cloud ignited by a spark,<br />

the fl ame will normally start out with a velocity of the<br />

order of 3–4 m/s. If the cloud is truly unconfi ned and<br />

unobstructed (i.e. no equipment or other structures are<br />

engulfed by the cloud) the fl ame is unlikely <strong>to</strong> accelerate<br />

<strong>to</strong> velocities of more than 20–25 m/s, and the overpressure<br />

will be negligible if the cloud is not confi ned.<br />

In a building or other enclosed space when the<br />

mixture is burning the temperature will increase and the<br />

fuel/air mixture is likely <strong>to</strong> expand by a fac<strong>to</strong>r of up <strong>to</strong> 8<br />

or 9, accelerating the fl ame front <strong>to</strong> several hundreds of<br />

metres per second.<br />

If the ignition source is from a weak source, e.g. a<br />

hot surface or a spark, the explosion will initially start as<br />

a slow burning defl agration. Due <strong>to</strong> obstructing objects<br />

and confi nement, the defl agration can accelerate and<br />

become fast burning. When a defl agration becomes<br />

suffi ciently rapid, a sudden transition from defl agration<br />

<strong>to</strong> de<strong>to</strong>nation may occur.<br />

If this transition occurs, very high pressure loads,<br />

up <strong>to</strong> 50 bar, can be reached locally and severe damage<br />

can be expected within the compartment. If a de<strong>to</strong>nation<br />

has been established in the compartment it may also<br />

propagate in<strong>to</strong> any unconfi ned cloud outside, potentially<br />

creating a UVCE.<br />

A defl agration propagating in<strong>to</strong> a large truly<br />

unconfi ned and unobstructed cloud will slow down<br />

Figure 7.24 Explosions at the Buncefi eld oil depot<br />

128<br />

and the pressure generation will normally be negligible.<br />

A de<strong>to</strong>nation, however, will propagate through the entire<br />

cloud at a high velocity and cause severe blast waves.<br />

The possibilities of transition <strong>to</strong> de<strong>to</strong>nation will mainly<br />

depend on the:<br />

➤ Type of fuel<br />

➤ Size of cloud<br />

➤ Enclosure conditions, such as obstructing objects<br />

and confi nement.<br />

Explosive limits and the fl ammable/explosion<br />

range<br />

The explosive limits or fl ammable/explosion range refers<br />

<strong>to</strong> the range in which the concentration of a fl ammable<br />

100%<br />

Too much<br />

oxygen<br />

0%<br />

Methane<br />

Hydrogen<br />

LEL<br />

Explosive limits<br />

FUEL<br />

OXYGEN<br />

UEL<br />

Too little<br />

oxygen<br />

5 % 15 %<br />

4 %<br />

74 %<br />

Figure 7.25 Illustration of explosive limits

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