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Aviation and the Global Atmosphere

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<strong>Aviation</strong> <strong>and</strong> <strong>the</strong> <strong>Global</strong> <strong>Atmosphere</strong><br />

as <strong>the</strong> fuel/air mass ratio. The dependence of NO x on fuel/air ratio is shown in Figure 7-15. As illustrated, peak NO x formation coincides with peak temperature, which<br />

occurs close to <strong>the</strong> stoichiometric fuel/air ratio (or equivalence ratio = 1). In current gas turbine engine combustors, <strong>the</strong>re are always some regions of <strong>the</strong> flame that<br />

burn stoichiometrically, so NO x formation is very strongly linked to combustor inlet temperature.<br />

Table 7-3: Improvements in emissions levels of GE CF6-50E2 engine.<br />

Levels for Levels for<br />

Applicable Original "Low Emissions"<br />

ICAO Production Production<br />

Emission St<strong>and</strong>ard Engine Engine<br />

Smoke (SN) 18.8 6.5 12.5<br />

HC (g kN-1) 19.6 57.8 3.4<br />

CO (g kN-1) 118 97.3 29.8<br />

NOx (g kN-1) 100 58.2 51.6<br />

"Soot" generally refers to particulates in emissions. These particles are composed primarily of carbonaceous material, <strong>the</strong> sum of graphite carbon <strong>and</strong> primary organics<br />

resulting from incomplete combustion of carbonaceous material (Novakov, 1982; Chang <strong>and</strong> Novakov, 1983). "Smoke" refers to combustion emissions particulates that<br />

contribute to a visible plume. The formation of soot <strong>and</strong> its partial oxidation in gas turbine combustors are very complex processes. Soot is produced mainly in <strong>the</strong> fuelrich<br />

primary zone of <strong>the</strong> combustor, <strong>the</strong>n oxidized in <strong>the</strong> high-temperature regions of <strong>the</strong> dilution <strong>and</strong> intermediate zone. A simplified description of <strong>the</strong> soot production<br />

mechanism is provided in Figure 7-16 (Mullins, 1988).<br />

Estimates of <strong>the</strong> fleet averaged emission index of soot is 0.04g/kg fuel burned (Döpelheuer, 1997). However, <strong>the</strong> derivation of this estimate carries considerable<br />

uncertainty <strong>and</strong> at best is only within a factor of 2. The formation of soot in gas turbine combustors <strong>and</strong> <strong>the</strong> precise design features <strong>and</strong> conditions that can influence<br />

<strong>the</strong> process continue to be subjects of important ongoing research. Since 1990, <strong>the</strong>re has been a marked improvement in <strong>the</strong> engine soot <strong>and</strong> aerosol emissions<br />

database through skilled use of <strong>the</strong> most modern aerosol measurement techniques (Hagen et al., 1992; Rickey, 1995; Pueschel et al., 1997; Petzold <strong>and</strong> Schröder,<br />

1998). State-of-<strong>the</strong>-art instrumentation permits detection of particles as small as 3 nm in diameter (Alofs et al., 1995). These data also show that jet engines emit soot<br />

particles, which have log normal-type size distributions peaking in <strong>the</strong> 20-30 nm range. Concentrations range between 10 6 <strong>and</strong> 10 7 particles cm -3 (Hagen et al., 1992;<br />

Whitefield <strong>and</strong> Hagen, 1995; Schumann et al., 1996; Pueschel et al., 1997; Anderson et al., 1998; Petzold <strong>and</strong> Schröder, 1998). Number-based emission indices fall<br />

within <strong>the</strong> range of 10 12 soot particles per kg of fuel burned for current advanced combustors to 10 15 for older type engines (Howard et al., 1996; Whitefield et al.,<br />

1996). A general range for most engines operating in <strong>the</strong> current commercial fleet is 10 14 -10 15 particles per kg fuel burned (Hagen et al., 1996; Döpelheuer, 1997;<br />

Anderson et al., 1998; Petzold <strong>and</strong> Schröder, 1998; Petzold et al., 1999).<br />

http://www.ipcc.ch/ipccreports/sres/aviation/100.htm (2 von 3)08.05.2008 02:43:32

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