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The CH4 Density in the Upper Atmosphere of Titan

✍ Scribed by L.M. Lara; M. Banaszkiewicz; R. Rodrigo; J.J. Lopez-Moreno


Publisher
Elsevier Science
Year
2002
Tongue
English
Weight
171 KB
Volume
158
Category
Article
ISSN
0019-1035

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✦ Synopsis


Previous modeling by

Banaszkiewicz et al. (2000a,b) showed that the CH 4 thermospheric mixing ratio on Titan could vary as much as 35-40% due to ion-neutral chemical reactions. A new vertical methane profile has been computed by simultaneously modifying the stratospheric methane mixing ratio and the K(z) previously considered by Lara et al. (1996) and Banaszkiewicz et al. (2000a,b).

A satisfactory fit of the methane thermospheric abundance and stratospheric mixing ratio of other minor constituents is achieved by placing the homopause at ∼1000 km and increasing the methane stratospheric mixing ratio (q CH 4 ) up to 3.8%. The new proposed eddy diffusion coefficient steadily rises from 1 Γ— 10 7 cm 2 s -1 at 700 km to 1 Γ— 10 10 cm 2 s -1 at 1500 km, whereas the stratospheric values are in the range (4-20) Γ— 10 3 cm 2 s -1 . Other likely ionization sources that can influence the methane distribution are (i) a metallic ion layer produced by micrometeoroid infall and (ii) frequent X-rays solar flares. Analysis of the effects of these ionization sources on the methane distribution indicates that, unlike previously assumed, CH 4 can suffer considerable variations. These variations, although proved in this work, must be cautiously regarded since several assumptions have to be made on the rate of N 2 and CH 4 ionization by the processes previously mentioned. Hence, these results are only indicative of methane sensitivity to ionospheric chemistry.


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