CO2 CONDENSATION IN THE MARTIAN ENVIRONMENT Xin Guo, Claire E' Newman, Mark I' Richardson, Stephen E - PowerPoint PPT Presentation

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CO2 CONDENSATION IN THE MARTIAN ENVIRONMENT Xin Guo, Claire E' Newman, Mark I' Richardson, Stephen E

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Title: CO2 CONDENSATION IN THE MARTIAN ENVIRONMENT Xin Guo, Claire E' Newman, Mark I' Richardson, Stephen E


1
CO2 CONDENSATION IN THE MARTIAN ENVIRONMENT Xin
Guo, Claire E. Newman, Mark I. Richardson,
Stephen E. WoodPlanetary Science, Division of
Geological and Planetary Sciences, California
Institute of Technology, Pasadena, CA
P23A-0041
  • ABSTRACT
  • It has been suggested that cirrus cloud formed of
    CO2 gas may have significantly affected the early
    history of the climate of Mars. Evidence of the
    existence of CO2 ice clouds in the current
    atmosphere of Mars has also been reported. We
    implement a CO2 microphysics scheme to the
    PlanetWRF Model and focus on its applications in
    the Martian environment. This physical scheme
    includes heterogeneous nucleation, homogenous
    nucleation, ion nucleation and CO2 ice particle
    growth. CO2 ice physics is coupled with the dust
    cycle, CO2 cycle and possibly water cycle. With
    followed radiative transfer study and comparison
    with spacecraft data products, we hope to have
    better insight into the history of the climate of
    Mars and its current circulating cycles. Complete
    understanding of the role that CO2 ice clouds
    play in the Martian climate system requires both
    modeling and laboratory work of CO2 ice formation
    processes, which have become two of the most
    urgent tasks in the Mars science community.
  • Coupling the microphysics model to PlanetWRF
    Figure 2. Schematic flowchart showing
    the relationships between microphysical
    and atmospheric processes
    involved in modeling the
    nucleation and
    growth/evaporation of ice crystals in
    the planetary atmosphere. Adopted from
    figure 1.1 of Wood, 1999 2.
  • PlanetWRF is the atmospheric
    model we use. Radiative transfer
    model,
    sedimentation model are
    currently
    being tested.
  • 1D SIMULATIONS
  • 1D annual cycle for Latitude 60 ºN. Log normal
    distributed dust with mean radius of 2 microns.
    No sedimentation of aerosols. CO2 ice is not
    radiative active. No direct surface condensation.
  • Figure 3. (a) Temperature annual cycle (b)
    CO2 vapor super saturation (c) CO2 ice mass
    mixing ratio
  • CO2 is super saturated in the winter. Dust
    particles become condensation nuclei. CO2
    ice particles are formed and then diffuse in
    the atmosphere.
  • Figure 4. (a) Dust spectral amount at Ls300
    º (Northern Winter) (b) CO2 ice particle
    spectral amount at Ls300º (c) Surface
    Pressure Annual Cycle
  • In the steady state, CO2 ice particles has
    radii of hundreds of microns. Consistent
    with Ivanov and Muhleman, 20014

3D SIMULATIONS
(PlanetWRF)
Figure 5 (upper left). Zonal average of CO2 ice
mass mixing ratio (color) and temperature
(contour) in northern winter. Figure 6 (upper
right). Same as Figure 5 but in southern
winter. Figure 7 (lower right). CO2 ice spatial
distribution and temperature at layer 16 (roughly
1km above the surface ) in southern winter
  • PLANETWRF 1
  • http//www.planetwrf.com
  • Dynamic core
  • Dynamics conserve mass and angular momentum to
    high accuracy, highly parallel, large suite of
    physics parameterizations and a modular form,
    uses Arakawa C-grid.
  • Nesting capability 1-way or 2-way nesting
    capability
  • Rotated pole capability better spatial
    resolution at polar region
  • CO2 Microphysics model2,3
  • Nucleation JnucF(P, T, qco2, Nnuc, rnuc) m-3
    s-1
  • Homogeneous (huge super saturation, less
    favored)
  • Ion (less super saturation, poor knowledge of
    ions, less favored)
  • Heterogeneous (dust as nuclei, favored)
  • Particle growth rate JmF(P, T, qco2, rnuc,
    Qrad) m s-1
  • Figure 1. Ice particle growth rate (for given
    size of crystal, given
  • pressure and CO2 mass mixing ratio) as a
    function of CO2 super saturation.
    Reproduction of figure 8.7 of Wood, 1999 2.

Cloud heights are consistent with Ivanov and
Muhleman, 2001 4 and Neumann et al. 2003 5
  • FUTURE WORK
  • Sedimentation scheme
  • Coupling with dust cycle
  • Radiative active CO2 cloud
  • More comparison with data
  • Paleoclimate simulation
  • The numerical simulations for this research were
    performed on Caltech's Division of Geological and
    Planetary Sciences Dell cluster (CITerra)
  • http//aeolis.gps.caltech.edu/wiki

References 1 Richardson MI, Toigo AD, Newman
CE. The Planetary WRF Model A General Purpose,
Local to Global Numerical Model for Planetary
Atmospheric and Climate Dynamics. In preparation
2006 2 Wood SE. Nucleation and growth of CO2
ice crystals in the Martian atmosphere, in Earth
and Space Sciences, University of California, Los
Angeles, Los Angeles, 1999. 3 Maattanen, A., H.
Vehkamaki, A. Lauri, S. Merikallio, J. Kauhanen,
H. Savijarvi, and M. Kulmala, Nucleation studies
in the Martian atmosphere, Journal of Geophysical
Research, 110 (E2), 2005. 4 Ivanov, A.B., and
D.O. Muhleman, Cloud reflection ovservations
Results from the Mars Orbiter Laser Altimeter,
Icarus, 154, 190-206, 2001. 5 Neumann, G.A.,
D.E. Smith, and M.T. Zuber, Two Mars years of
clouds detected by the Mars Orbiter Laser
Altimeter, Journal of Geophysical Research, 108
(E4), 5023-5039, 2003.
Corresponding author. Tel. 1-626-395-5896
Fax 1-626-585-1917. Email address
xin_at_gps.caltech.edu (Guo, Xin)
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