Densities and vibrational distribution of H3+in the Jovian auroral ionosphere
Autor: | Jane L. Fox, H. S. Porter, Y. H. Kim |
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Rok vydání: | 1992 |
Předmět: |
Physics
Atmospheric Science Ecology Infrared Atmosphere of Jupiter Paleontology Soil Science Energy flux Electron precipitation Forestry Aquatic Science Oceanography Jovian Geophysics Space and Planetary Science Geochemistry and Petrology Trihydrogen cation Earth and Planetary Sciences (miscellaneous) Emission spectrum Atomic physics Ionosphere Earth-Surface Processes Water Science and Technology |
Zdroj: | Journal of Geophysical Research. 97:6093 |
ISSN: | 0148-0227 |
DOI: | 10.1029/92je00454 |
Popis: | Observations of the H3+ infrared emission at 2 and 4 μm have suggested that H3+ is in local thermodynamic equilibrium (LTE) in the region of the Jovian ionosphere from which the emissions originate. We have tested this assumption by calculating the vibrational distribution of H3+ over the altitude range of 350 to 1500 km above the methane cloud tops (1 to 4 × 10−3 μbar). We have constructed a model of the Jovian auroral ionosphere in which the neutral temperatures are enhanced over those of the mid-latitude ionosphere, as suggested by observations and models of the auroral region. We have modeled the precipitation of 10-keV electrons with an energy flux of 1 erg cm−2 s−1. Both the energy and energy flux are less than those that are implicated in the production of the UV aurora. We have computed the densities and vibrational distribution of H3+ and find that the distribution of the six lowest states of H3+ can be determined fairly well in spite of uncertainties in the atomic and molecular data. Since the nearly resonant transfer of vibration from H2(υ=1) is an important process in populating the H3+(υ1=0,υ2=2) state, it is necessary to model the vibrational distribution of H2 as well. The computed altitude profiles and vibrational distributions of H3+ and H2 are consistent with the observations of infrared emission in the 2-and 4-μm regions. The H3+ is not in LTE near and above the H3+ peak, since loss of the H3+(υ1=0,υ2=1) and H3+(υ1=0,υ2=2) states by radiation is approximately equal to the collisional loss rate. |
Databáze: | OpenAIRE |
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