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    The Escape of H2 from Titan

    Source: Journal of the Atmospheric Sciences:;1973:;Volume( 030 ):;issue: 004::page 726
    Author:
    Hunten, D. M.
    DOI: 10.1175/1520-0469(1973)030<0726:TEOHFT>2.0.CO;2
    Publisher: American Meteorological Society
    Abstract: The stability of light gases in various hypothetical Titan atmospheres is examined. Only tiny amounts are free of blowoff unless the mean mass is greater than 4 atomic units. In a mixture of H2 (or He) with a heavier gas, a diffusive upward flux, due to buoyancy, must exist. Its value is insensitive to any parameters except the mixing ratio f1 of light to heavy gas, and is of order 2?1011 cm?2 sec?1 for fl=0.1. Normally, fl is independent of height except at great altitudes, and the extent of mechanical mixing of the atmosphere is therefore nearly irrelevant. The structure of the high atmosphere adjusts itself to accommodate the buoyant flux; the exospheric temperature affects this structure, but does not control the escape rate. The heavy gas is most probably N2 or CH4, (or both), and several existing models of this type are discussed. All seem acceptable as long as there is a large source of H2 near or below the surface. Photolysis of NH3 seems adequate, but only if solar ultraviolet penetrates deep enough. Thermal, chemical, or radioactive dissociation of NH3 in the deep interior offer possibilities for further study.
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      The Escape of H2 from Titan

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    https://yetl.yabesh.ir/yetl1/handle/yetl/4152154
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    contributor authorHunten, D. M.
    date accessioned2017-06-09T14:16:57Z
    date available2017-06-09T14:16:57Z
    date copyright1973/05/01
    date issued1973
    identifier issn0022-4928
    identifier otherams-16378.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4152154
    description abstractThe stability of light gases in various hypothetical Titan atmospheres is examined. Only tiny amounts are free of blowoff unless the mean mass is greater than 4 atomic units. In a mixture of H2 (or He) with a heavier gas, a diffusive upward flux, due to buoyancy, must exist. Its value is insensitive to any parameters except the mixing ratio f1 of light to heavy gas, and is of order 2?1011 cm?2 sec?1 for fl=0.1. Normally, fl is independent of height except at great altitudes, and the extent of mechanical mixing of the atmosphere is therefore nearly irrelevant. The structure of the high atmosphere adjusts itself to accommodate the buoyant flux; the exospheric temperature affects this structure, but does not control the escape rate. The heavy gas is most probably N2 or CH4, (or both), and several existing models of this type are discussed. All seem acceptable as long as there is a large source of H2 near or below the surface. Photolysis of NH3 seems adequate, but only if solar ultraviolet penetrates deep enough. Thermal, chemical, or radioactive dissociation of NH3 in the deep interior offer possibilities for further study.
    publisherAmerican Meteorological Society
    titleThe Escape of H2 from Titan
    typeJournal Paper
    journal volume30
    journal issue4
    journal titleJournal of the Atmospheric Sciences
    identifier doi10.1175/1520-0469(1973)030<0726:TEOHFT>2.0.CO;2
    journal fristpage726
    journal lastpage732
    treeJournal of the Atmospheric Sciences:;1973:;Volume( 030 ):;issue: 004
    contenttypeFulltext
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    DSpace software copyright © 2002-2015  DuraSpace
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