Flight-Testing of the FAA Onboard Inert Gas Generation System on ...
Flight-Testing of the FAA Onboard Inert Gas Generation System on ...
Flight-Testing of the FAA Onboard Inert Gas Generation System on ...
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<str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> permeate venting, because high OEA venting backpressure was measured <strong>on</strong> <str<strong>on</strong>g>the</str<strong>on</strong>g> twomembrane<br />
test. The result from this backpressure would be to reduce <str<strong>on</strong>g>the</str<strong>on</strong>g> ASMs ability to flow<br />
permeate, decreasing <str<strong>on</strong>g>the</str<strong>on</strong>g> overall efficiency and total flow out <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> ASM. As <str<strong>on</strong>g>the</str<strong>on</strong>g> system is<br />
switched to high-flow mode in descent for both c<strong>on</strong>figurati<strong>on</strong>s, <str<strong>on</strong>g>the</str<strong>on</strong>g> NEA flow tends to be more<br />
representative <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> expected relati<strong>on</strong>ship. This is c<strong>on</strong>sistent with <str<strong>on</strong>g>the</str<strong>on</strong>g> analysis <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> problem in<br />
that <str<strong>on</strong>g>the</str<strong>on</strong>g> effect <str<strong>on</strong>g>of</str<strong>on</strong>g> decreasing <str<strong>on</strong>g>the</str<strong>on</strong>g> ASM inlet pressure would be less permeate flow and, thus, less<br />
permeate backpressure. The problem is observed at cruise and higher altitudes, which is also <str<strong>on</strong>g>the</str<strong>on</strong>g><br />
point at which permeate backpressure was <str<strong>on</strong>g>the</str<strong>on</strong>g> greatest. This c<strong>on</strong>clusi<strong>on</strong> is also supported by <str<strong>on</strong>g>the</str<strong>on</strong>g><br />
measured permeate backpressure <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> two-membrane c<strong>on</strong>figurati<strong>on</strong>, which was about three<br />
times <str<strong>on</strong>g>the</str<strong>on</strong>g> backpressure <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> single-membrane c<strong>on</strong>figurati<strong>on</strong>.<br />
Oxygen C<strong>on</strong>centrati<strong>on</strong> (%vol)<br />
20<br />
18<br />
16<br />
14<br />
12<br />
10<br />
8<br />
6<br />
4<br />
2<br />
0<br />
1 Membrane<br />
2 Membranes<br />
NEA Line O2 (%) NEA Line O2 (%)<br />
ASM Inlet Pressure (Psig) ASM Inlet Pressure (Psig)<br />
NEA Flow (SCFM) NEA Flow (SCFM)<br />
70 72 74 76 78 80 82 84 86 88 90<br />
Time (min)<br />
FIGURE 9. SYSTEM FLOW AND PURITY WITH ASM PRESSURE FOR BOTH<br />
MEMBRANE CONFIGURATIONS DURING DESCENT<br />
The relati<strong>on</strong>ship between ASM pressure and NEA flow shown in figures 8 and 9 are correlated<br />
in figure 10. Again, this correlati<strong>on</strong> is <strong>on</strong>ly valid for a similar flight pr<str<strong>on</strong>g>of</str<strong>on</strong>g>ile with bleed air<br />
schedule, as NEA flow is a str<strong>on</strong>g functi<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> pressure altitude. This is why <str<strong>on</strong>g>the</str<strong>on</strong>g> cruise curves<br />
indicate a much lesser slope than <str<strong>on</strong>g>the</str<strong>on</strong>g> ascent and descent curves. The changing altitude causes<br />
vast changes in membrane permeability and a wider range in NEA flows, while <str<strong>on</strong>g>the</str<strong>on</strong>g> cruise<br />
porti<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> flight exhibits no altitude change effects and, thus, gives a true correlati<strong>on</strong> between<br />
pressure and flow with <str<strong>on</strong>g>the</str<strong>on</strong>g> given low-flow fixed orifice at 39,000 feet. The ascent and descent<br />
porti<strong>on</strong>s <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> graph illustrates <str<strong>on</strong>g>the</str<strong>on</strong>g> large increase in normalized NEA flow from <str<strong>on</strong>g>the</str<strong>on</strong>g> system,<br />
given a relatively small change in ASM pressure, exhibiting a benefit <str<strong>on</strong>g>of</str<strong>on</strong>g> using HFM technology<br />
to generate inert gas at altitude. Only selected data for each flight phase were plotted because<br />
widely varying throttle settings produce rapid changes in <str<strong>on</strong>g>the</str<strong>on</strong>g> system causing uncorrelated data<br />
for brief periods due to delays in some instrumentati<strong>on</strong>.<br />
14<br />
50<br />
45<br />
40<br />
35<br />
30<br />
25<br />
20<br />
15<br />
10<br />
5<br />
0<br />
Flow (scfm) / Pressure (Psig)