Estimates of atomic deuterium abundance and Lyman‐alpha airglow in the thermosphere of Jupiter
Identifieur interne : 000313 ( France/Analysis ); précédent : 000312; suivant : 000314Estimates of atomic deuterium abundance and Lyman‐alpha airglow in the thermosphere of Jupiter
Auteurs : C. D. Parkinson [Canada] ; E. Griffioen [Canada] ; J. C. Mcconnell [Canada] ; L. Ben Jaffel [États-Unis] ; A. Vidal-Madjar [France] ; J. T. Clarke [États-Unis] ; G. R. Gladstone [États-Unis]Source :
- Geophysical Research Letters [ 0094-8276 ] ; 1999-10-15.
Abstract
We have made calculations of the atomic D distribution in the thermosphere of Jupiter. The principal reactions determining the D abundance appear to be generation by reaction of H with vibrationally hot HD and loss by reaction of D with H2(υ=0,1) and CH3. The H and CH3 distributions have been calculated using a 1‐D photochemical‐diffusion model with the column H constrained using the Lyman‐α airglow. For H2 effective vibrational temperatures, Tυ, between 1 and 4 times kinetic we find D columns between 4×1011 and 2×1013 atoms cm−2. HD can be vibrationally excited due to VV energy transfer from H2(υ=1). Using a radiative transfer model with coupling of the H and D Lyman‐α lines we have calculated line profiles and total intensities across the Jovian disk and on the limb. For the above D columns and a H column ∼3.5×1017 cm−2, compatible with equatorial Lyman‐α airglow observations, the disk D intensity varies from 80 to 600 R for overhead Sun and viewing, whereas on the terminator the D maximum total intensity is ∼60 R at ∼860 km above the 1 bar level for the maximum D column.
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DOI: 10.1029/1999GL003650
Affiliations:
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<front><div type="abstract">We have made calculations of the atomic D distribution in the thermosphere of Jupiter. The principal reactions determining the D abundance appear to be generation by reaction of H with vibrationally hot HD and loss by reaction of D with H2(υ=0,1) and CH3. The H and CH3 distributions have been calculated using a 1‐D photochemical‐diffusion model with the column H constrained using the Lyman‐α airglow. For H2 effective vibrational temperatures, Tυ, between 1 and 4 times kinetic we find D columns between 4×1011 and 2×1013 atoms cm−2. HD can be vibrationally excited due to VV energy transfer from H2(υ=1). Using a radiative transfer model with coupling of the H and D Lyman‐α lines we have calculated line profiles and total intensities across the Jovian disk and on the limb. For the above D columns and a H column ∼3.5×1017 cm−2, compatible with equatorial Lyman‐α airglow observations, the disk D intensity varies from 80 to 600 R for overhead Sun and viewing, whereas on the terminator the D maximum total intensity is ∼60 R at ∼860 km above the 1 bar level for the maximum D column.</div>
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