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Correlation of subsurface ice content and gully locations on Mars; testing the shallow aquifer theory of gully formation

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CORRELATION OF SUBSURFACE ICE CONTENT AND GULLY LOCATIONS ON MARS: TESTING THE SHALLOW AQUIFER THEORY OF GULLY FORMATION. S. J. Edlund

1

and J. L. Heldmann

2

,

1

Luleå University of Technology, Luleå, Sweden, jeanette.edlund@gmail.com ,

2

NASA Ames Research Center, Moffett Field, CA, USA, jheldmann@mail.arc.nasa.gov

Introduction: Images from the Mars Orbiter Camera on the Mars Global Surveyor show gully features re- sembling water-carved gullies on Earth. Geomorphic evidence suggests that the gullies were formed within the past few million years by fluvial activity [1]. One theory of gully formation contends that the source of the water feeding the gullies is a shallow liquid water aquifer. This theory requires a relatively dry overbur- den to maintain liquid water at the observed alcove base depths [2, 3]. We quantitatively test the shallow aquifer theory by calculating the temperature and pres- sure of the Martian subsurface at the measured alcove base depths using measured Gamma Ray Spectrometer (GRS) ice contents to determine if liquid water can exist at these locations.

Methodology: We calculate the thermal conductivity and density of the regolith overlying the hypothesized liquid aquifers by assuming an overburden ice content consistent with that measured by the Gamma Ray Spectrometer (GRS) at each gully site. We then calcu- late subsurface temperature and pressure fields based on this data to determine if liquid water can exist at the gully sites. Gully sites were identified in previous works for both the southern [2] and northern hemi- spheres on Mars [4].

Equation 1 Equation 2

Equation 1 and Equation 2 were used to calculate the temperature and the pressure at the alcove base depth, where T

0

is the mean surface temperature as measured by TES, z is the alcove base depth as measured from MOC and MOLA data, q is the thermal heat flux, g is the gravity constant, ρ is the density of the soil and k is the thermal conductivity of the soil [2, 3].

The density and the thermal conductivity of the soil affect the calculated pressure and temperature at dif- ferent depths in the Martian soil. Since the density and thermal conductivity of the soil is dependent on the amount of ice in the soil, the ice-to-soil ratio is a very important factor. This factor can be determined using the GRS data from the Mars Odyssey spacecraft. Fig- ure 1 shows the ice concentration of the Martian sub- surface in the upper one meter and the locations of the gully formations while Figure 2 shows the distribution

of ice contents for the gully locations. The ice concen- tration between -45˚ and +45˚ of latitude are assumed to be zero since ice cannot be stable there. Instead the hydrogen signature measured by GRS is assumed to come from hydrated minerals [5]. The measurements above the latitude of 60˚ are not accurate since a polar cap was present at the time of these measurements.

Therefore we only analyze gullies between 60˚S-60˚N.

Results: As shown in Figure 3, 59% of the gullies fall outside of the temperature and pressure regime of liq- uid water at the alcove base depth when assuming an overburden consistent with the observed GRS ice con- tent. However, it may be unrealistic to assume that the measured GRS ice content extends down to the depth of the gully alcoves. We therefore estimate the thick- ness of a dry layer that must exist within the overbur- den column for the water to be liquid at the alcove base depth. These calculations assume that the soil has a fraction of overburden with dry and icy components where the icy layer has the same concentration of ice as measured by GRS. Figure 4 shows the calculated thickness of the required dry layer vs. the measured alcove base depth. The gullies to the right of the solid line can have liquid water underneath the soil at the alcove base depth using the multi layer system. Ac- cording to these calculations, liquid water could exist in approximately 81% of the gully locations.

The remaining 19% of the gully locations could not have liquid water at the depth of the alcove base be- cause the required thickness of the dry layer exceeds the alcove base depth. We didn’t find any outstanding characteristics for the albedo, elevation, channel length or thermal inertia for the gullies where liquid water cannot exist in the subsurface aquifer compared with the other gullies where liquid water could exist in the subsurface aquifer. However, the 19% of gullies which cannot support a shallow liquid water aquifer accord- ing to these calculations had very shallow alcove bases as shown in Figure 4.

It is possible that the gullies that could not have liquid water at the alcove base depth have been formed in a different way than the other gullies such as melting ground ice [6, 7], snowmelt [8] or a deep aquifer source [9]. Additionally, the resolution of GRS is on the order of several hundred km, which is much larger then the scale of the gully formations. Hence the GRS measurement may not be precisely indicative of the

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Lunar and Planetary Science XXXVII (2006) 2049.pdf

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subsurface ice content at the exact location of the gul- lies.

Figure 1: Plot showing the locations for the gullies and subsurface ice concentration in the upper one meter of Mars based on Mars Odyssey GRS measurements.

Figure 2: Plot showing a histogram of the ice content at the gully locations.

Figure 3: Plot showing the phase diagram of water. The asterisks represent the calculated temperature and pressure at the alcove base depth of the gullies with an icy overburden layer based on GRS ice content.

Figure 4:

Plot showing the alcove base depth and the thickness of a calculated dry layer required to maintain temperatures of 273K at observed alcove base depths. Here we assume that the soil has a fraction of overburden with dry and icy components where the icy layer has the same concentration of ice as measured by GRS. The solid line represents where the depth to the alcove base is the same as the thickness of the dry layer.

References:

[1] Malin M.C and Edgett K.S. (2000), Science 288 [2] Heldmann J.L. and Mellon M.T. (2004) Icarus, 168 [3] Mellon M.T. and Philips R.J. (2001) J. Geophys.

Res. 106

[4] Heldmann, J.L., Johansson, H., Carlsson, E., and M.T. Mellon (2004) LPSC abstract #1271

[5] Fialips, C., Carey, J.W., Vaniman, D.T., Bish, D.L., Feldman, W.C., and M.T. Mellon (2005) Icarus 178 [6] Costard F., Forget, F., Mangold, N., and J.P. Peul- vast (2002) Science 295

[7] Gilmore M.S. Philip E.L. (2002) Geology 30 [8] Christensen, P.R. (2003) Nature 422 [9] Gaidos E.J. (2001) Icarus 153

Lunar and Planetary Science XXXVII (2006) 2049.pdf

References

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