The depth of the convective boundary layer on Mars
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作者:
Hinson, D. P.
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Stanford Univ, Dept Elect Engn, Stanford, CA 94305 USA
SETI Inst, Carl Sagan Ctr, Mountain View, CA 94043 USAStanford Univ, Dept Elect Engn, Stanford, CA 94305 USA
Hinson, D. P.
[1
,2
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Paetzold, M.
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机构:
Univ Cologne, Rhein Inst Umweltforsch, Cologne, GermanyStanford Univ, Dept Elect Engn, Stanford, CA 94305 USA
Paetzold, M.
[3
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Tellmann, S.
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Univ Cologne, Rhein Inst Umweltforsch, Cologne, GermanyStanford Univ, Dept Elect Engn, Stanford, CA 94305 USA
Tellmann, S.
[3
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Haeusler, B.
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Univ Bundeswehr Munchen, Inst Raumfahrttech, Neubiberg, GermanyStanford Univ, Dept Elect Engn, Stanford, CA 94305 USA
Haeusler, B.
[4
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Tyler, G. L.
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Stanford Univ, Dept Elect Engn, Stanford, CA 94305 USAStanford Univ, Dept Elect Engn, Stanford, CA 94305 USA
Tyler, G. L.
[1
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机构:
[1] Stanford Univ, Dept Elect Engn, Stanford, CA 94305 USA
[2] SETI Inst, Carl Sagan Ctr, Mountain View, CA 94043 USA
We are using observations obtained with Mars Express to explore the structure and dynamics of the martian lower atmosphere. We consider a series of radio occultation experiments conducted in May-August 2004, when the season on Mars was midspring of the northern hemisphere. The measurements are widely distributed in latitude and lougitude, but the local time remained within a narrow range, 17.0-17.2 h. Most of the atmospheric profiles retrieved from these data contain a distinct, well-mixed convective boundary layer (CBL). We have accurately determined the depth of the CBL and its spatial variations at fixed local time through analysis of these profiles. The CBL extends to a height of 3-10 km above the Surface at the season and locations of these measurements. Its depth at fixed local time is clearly correlated with variations in surface elevation oil planetary scales, with a weaker dependence oil spatial variations in surface temperature. In general, the CBL is deep (8-10 km) where the surface elevation is high, as in Tharsis Montes and Syrtis Major, and shallow (4-6 km) where the surface elevation is low, as in Amazonis and Utopia. This variability results from the combined effects of conditions near the surface and in the atmosphere above the CBL. Convection arises from solar hearing of the ground, and the impact of this heat source oil thermal structure is largest where the surface pressure and atmospheric density are smallest, at high surface elevations. The vertical extent of the CBL is in turn constrained by the static stability of the overlying atmosphere. These results greatly reduce the long-standing uncertainty concerning the depth of the CBL. (C) 2008 Elsevier Inc. All rights reserved.
机构:
Penn State Univ, Dept Meteorol & Atmospher Sci, University Pk, PA 16802 USAPenn State Univ, Dept Meteorol & Atmospher Sci, University Pk, PA 16802 USA
Banghoff, John R.
Stensrud, David J.
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Penn State Univ, Dept Meteorol & Atmospher Sci, University Pk, PA 16802 USAPenn State Univ, Dept Meteorol & Atmospher Sci, University Pk, PA 16802 USA
Stensrud, David J.
Kumjian, Matthew R.
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Penn State Univ, Dept Meteorol & Atmospher Sci, University Pk, PA 16802 USAPenn State Univ, Dept Meteorol & Atmospher Sci, University Pk, PA 16802 USA