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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 />

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

Table of contents | Previous page | Next page<br />

3.4. Contrail Occurrence <strong>and</strong> Persistence <strong>and</strong> Impact of Aircraft Exhaust on Cirrus<br />

O<strong>the</strong>r reports in this collection<br />

Aircraft cause visible changes in <strong>the</strong> atmosphere by forming contrails that represent artificially induced cirrus clouds. The conditions under which contrails form are<br />

discussed in Section 3.2.4. This section describes <strong>the</strong> formation, occurrence, <strong>and</strong> properties of persistent contrails <strong>and</strong> how <strong>the</strong>y compare with natural cirrus.<br />

3.4.1. Cirrus <strong>and</strong> Contrails<br />

Cirrus clouds (Liou, 1986; Pruppacher <strong>and</strong> Klett, 1997) contain mainly ice crystals (Weickmann, 1945). The distinctive properties of cirrus <strong>and</strong> contrails derive from <strong>the</strong><br />

physics of ice formation. Ice particle nucleation occurs ei<strong>the</strong>r through homogeneous nucleation (when pure water droplets or liquid aerosol particles freeze) or through<br />

heterogeneous nucleation, when freezing of <strong>the</strong> liquid is triggered by a solid particle or surface that is in contact with <strong>the</strong> liquid or suspended within <strong>the</strong> liquid. Both<br />

processes depend strongly on temperature <strong>and</strong> relative humidity (Heymsfield <strong>and</strong> Miloshevich, 1995; see Section 3.2.4.2).<br />

Comparisons of model simulations with observations suggest that we may underst<strong>and</strong> homogeneous nucleation (Ström et al., 1997; Jensen et al., 1998b) <strong>and</strong> are<br />

making headway in underst<strong>and</strong>ing <strong>the</strong> potential contribution of heterogeneous nucleation (DeMott et al., 1998; Rogers et al., 1998). Each of <strong>the</strong>se freezing<br />

mechanisms requires that <strong>the</strong> atmosphere be highly supersaturated with respect to <strong>the</strong> vapor pressure of ice before crystals can form. For instance, supersaturations<br />

in excess of 40-50% with respect to ice are needed for sulfuric acid particles to freeze homogeneously (Tabazadeh et al., 1997) at temperatures above 200 K.<br />

Observations of relative humidity with respect to ice at <strong>the</strong> leading edges of wave clouds are consistent with <strong>the</strong> requirement of large ice supersaturations for<br />

nucleation of ice on <strong>the</strong> bulk of <strong>the</strong> atmospheric aerosol (Heymsfield et al., 1998a; Jensen et al., 1998c). Hence, <strong>the</strong>re is a large supersaturation range in which<br />

heterogeneous nuclei could lead to cirrus formation before <strong>the</strong> bulk of <strong>the</strong> atmospheric particles freeze (DeMott et al., 1997). This potential for heterogeneous nuclei to<br />

cause ice formation at ice supersaturations that are relatively low compared to those needed to freeze sulfate particles leads to concern about <strong>the</strong> role of aircraft<br />

exhaust in modifying ambient clouds (Jensen <strong>and</strong> Toon, 1997).<br />

Ice crystal number densities are limited by competition between increasing saturation as a<br />

result of cooling in vertical updrafts <strong>and</strong> decreasing saturation as a result of growth of ice<br />

crystals. The depletion of vapor as a result of growth of <strong>the</strong> first few ice crystals nucleated<br />

http://www.ipcc.ch/ipccreports/sres/aviation/038.htm (1 von 10)08.05.2008 02:42:05

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