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Vaporization of JP-8 Jet Fuel in a Simulated Aircraft Fuel Tank ...

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6.2.2 <strong>Fuel</strong> <strong>Tank</strong> Under Vary<strong>in</strong>g Ambient Conditions<br />

The FAR rule and Le Chatelier’s ratio rule were aga<strong>in</strong> used to determ<strong>in</strong>e the level <strong>of</strong><br />

flammability for the second example, an <strong>in</strong>itially heated fuel tank exposed to simulated<br />

flight conditions. Figures 6.11 and 6.12 show, respectively, the calculated FAR and the<br />

calculated Le Chatelier’s ratio, both calculated us<strong>in</strong>g the fuel compositions with<br />

flashpo<strong>in</strong>ts <strong>of</strong> 115°F and 120°F [21]. From figure 6.11, the mixture was not <strong>in</strong> the<br />

flammable region until the ambient pressure was decreased dur<strong>in</strong>g ascent. This was due<br />

to the fact that the component vapor pressures are functions <strong>of</strong> temperature only, and<br />

although the ambient pressure outside <strong>of</strong> the fuel tank was decreas<strong>in</strong>g, the component<br />

vapor pressures are fixed for the liquid fuel temperature. So <strong>in</strong> order for the fuel vapors<br />

to exert the same pressure on the enclosure at a reduced ambient pressure, more fuel<br />

molecules were required to vaporize <strong>in</strong>to the ullage space. Le Chatelier’s rule was aga<strong>in</strong><br />

seen to be more conservative than the FAR rule by compar<strong>in</strong>g figures 6.11 and 6.12, so<br />

the FAR rule will aga<strong>in</strong> be used to assess the effects <strong>of</strong> fuel temperature and mass load<strong>in</strong>g<br />

on flammability for this flight pr<strong>of</strong>ile test.<br />

The liquid temperature effects on flammability are shown <strong>in</strong> figures 6.13 and<br />

6.14. Three different liquid temperature pr<strong>of</strong>iles were used <strong>in</strong> the model to calculate the<br />

FAR and LCR us<strong>in</strong>g the fuel composition <strong>of</strong> the 115°F flashpo<strong>in</strong>t fuel. The orig<strong>in</strong>al<br />

average measured liquid temperature pr<strong>of</strong>ile is referred to as TLIQ and the other two<br />

pr<strong>of</strong>iles were obta<strong>in</strong>ed by add<strong>in</strong>g 5°F and 10°F to TLIQ and are referred to as TLIQ+5<br />

and TLIQ+10, respectively. Figure 6.13 <strong>in</strong>cludes the predicted LFL range us<strong>in</strong>g the FAR<br />

criterion from reference [26]. It shows that for the conditions tested, the tank ullage was<br />

with<strong>in</strong> the LFL range for part <strong>of</strong> the level flight at 30,000’ altitude. However, <strong>in</strong>creas<strong>in</strong>g<br />

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