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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 />

aircraft RF components from <strong>the</strong> NASA-1992* scenario in Figure 6-14b (note <strong>the</strong> change of<br />

scale; see also Table 6-1). Aircraft RF is qualitatively different from overall anthropogenic<br />

RF: The CH4 RF is negative, <strong>the</strong> O3-RF is greater than <strong>the</strong> co 2 -RF, <strong>and</strong> <strong>the</strong> aerosol-cloud<br />

effects are positive (because of persistent contrails) ra<strong>the</strong>r than negative. Within <strong>the</strong> error<br />

bars, <strong>the</strong> effects of co 2 , O3, <strong>and</strong> contrails are comparable; that of methane is also<br />

comparable, but negative. A caveat here is that we are unable to derive a best estimate for<br />

<strong>the</strong> indirect effects from aircraft on "natural" clouds; <strong>the</strong>se effects might be negligible or may<br />

be comparable to that of contrails. Thus, for 1992 our best estimate is that aviation causes<br />

RF (without additional cirrus) of approximately +0.05 W m-2 <strong>and</strong> is responsible for about<br />

3.5% of <strong>the</strong> total anthropogenic RF of about +1.4 W m-2 for greenhouse gases plus<br />

aerosols (+2.7 W m-2 for greenhouse gases alone).<br />

Bar charts for <strong>the</strong> 2050 atmosphere are presented in Figure 6-15a. The same qualitative<br />

differences apply. However, in 2050 <strong>the</strong> contribution by contrails is almost twice as large as<br />

<strong>the</strong> contribution from aircraft co 2 or O3. Thus, in 2050 for <strong>the</strong> Fa1 scenario, our best<br />

estimate is that aviation RF (without additional cirrus) grows to about +0.19 W m-2, which is<br />

5% of <strong>the</strong> total anthropogenic radiative forcing anticipated for IS92a of +3.8 W m-2 for<br />

greenhouse gases plus aerosols (+5.8 W m-2 for greenhouse gases alone). This fraction is<br />

more than doubled for E-type scenarios (Table 6-1). There is considerable scientific<br />

uncertainty in <strong>the</strong>se estimates-a factor of 2 or more at <strong>the</strong> 67% confidence level-that is<br />

separate from <strong>the</strong> potential error in projecting future scenarios for aviation <strong>and</strong> IS92a.<br />

Individual RF components in 2050 attributable to <strong>the</strong> impact of adding a supersonic fleet are<br />

shown in Figure 6-15c (see also Table 6-1). The white bars denote <strong>the</strong> direct RF of HSCTs;<br />

<strong>the</strong> black bars denote <strong>the</strong> RF from displaced subsonic air traffic. As already discussed, RF<br />

from stratospheric H 2 O contributes <strong>the</strong> largest component, comparable in magnitude to <strong>the</strong><br />

big three RFs CO 2 , O3, contrails) from <strong>the</strong> subsonic fleet (Figure 6-15b). RFs for <strong>the</strong><br />

combined fleet (Fa1H) are listed separately in Tables 6-1 <strong>and</strong> 6-2.<br />

http://www.ipcc.ch/ipccreports/sres/aviation/083.htm (2 von 4)08.05.2008 02:43:12<br />

below <strong>the</strong> graph are relative appraisals of <strong>the</strong> level of scientific<br />

underst<strong>and</strong>ing associated with each component.<br />

Figure 6-14b: Bar charts of radiative forcing from aviation effects in<br />

1992. Note scale change from (a) to (b). In (b), best estimate (bars)<br />

<strong>and</strong> high-low 67% probability intervals (whiskers) are given. No best<br />

estimate is shown for <strong>the</strong> cirrus clouds; ra<strong>the</strong>r, <strong>the</strong> dashed line<br />

indicates a range of possible estimates. The evaluations below <strong>the</strong><br />

graph are relative appraisals of <strong>the</strong> level of scientific underst<strong>and</strong>ing<br />

associated with each component.

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