Mathematics – Logic
Scientific paper
Sep 2008
adsabs.harvard.edu/cgi-bin/nph-data_query?bibcode=2008epsc.conf..683t&link_type=abstract
European Planetary Science Congress 2008, Proceedings of the conference held 21-25 September, 2008 in Münster, Germany. Online a
Mathematics
Logic
Scientific paper
Introduction On the planets having atmosphere such as Mars various types of interactions between the atmosphere and the ground surface cause observable change in the surface pattern. Polar caps and aeolian features are typical examples. With the accumulation of satellitebased exploratory data, time-variable surface patterns have been focused and investigated extensively [1,2], because they can be direct indicators of the changing surface environments. Here we report two types of time-variable surface patterns that have been unidentified until now. One is dark halo near the top of high altitude volcanoes in Tharsis region. The other is brightness of the Outer Lobe of Double Layered Ejecta crater at the northern lowlands. Both have almost no associated topography and they are only recognized in visible/IR images as albedo patterns. Dark halo near the top of high altitude volcanoes in the Tharsis region Fig. 1 shows MOC wide-angle image of Pavonis Mons (R1400388NRed). The large caldera can be seen at the top of the volcano. Surrounding the caldera there exists a dark halo. Fig. 1B is MOC wide-angle image which shows detailed structure of the dark halo in the SW part. The dark zone is not uniform and instead it is composed of many slender dark stripes aligned in radial direction from the top (caldera center). Each unit is spindle-shaped with length of 30- 50km and width at the middle part of 5km. Spindles seem to start from higher position because it is always clear and darker. The initiation point is quite narrow region, which can be considered as a point. In many cases, there exist no recognisable obstacles at the initiation point. This is a remarkable difference from the wind streaks, which is caused by erosion/sedimentation of wind by local turbulence behind topographical anomaly. This makes us to consider something is emanating from subsurface, blown off by the mountain winds and deposited in downwind part. Similar pattern is observed in high altitude large volume volcanoes in Tharsis region such as Olympus Mons, Arsia Mons, Ascraeus Mons and Alba Patera EPSC Abstracts, Vol. 3, EPSC2008-A-00513, 2008 European Planetary Science Congress, Author(s) 2008 whereas it is not recognized in Celaunius Tholus, Tharsis Tholus and Elysium Mons. Because of the numbers of available images and stable climate situation, we have intensively investigated the pattern at Pavonis Mons. MOC wide-angle images and THEMIS-VIS images are used to check the temporal variation of the pattern from 1999 to 2007. In Fig. 2 the time-sequential images taking the SW flank show temporal pattern change of the dark halo. The drastic change can be found between 2000 and 2003. The assemblage of dark spindle-shaped pattern at higher positions before 2003 completely disappeared in the 2003 and the front of the halo receded to lower position. In 2001, a huge global dust storm has occurred. The resultant effect on the global climate by this dust storm is decrease in global daytime temperature and increase in global nighttime temperature due to the dust green house effect [2]. Since the dark halo appears to be formed in nighttime (the pattern is consistent with down-slope wind, which would be dominant at nigh time on the surface of high mountain.), the increase of the nighttime temperature should be responsible for erasing the pattern. Not only the position of the front of the dark halo but also the darkness changes with time. DN at the front position is determined by taking the difference from the reference point near the caldera. The maximum contrast around Ls=50 deg. and the minimum contrast around Ls=270 deg. are obtained. This indicates seasonal variation, which strongly suggests meteorological variation such as the atmospheric pressure controls the surface pattern. Fig. 3 shows THEMIS-VIS image, THEMIS-IRNighttime image and THEMIS-IR-Daytime image of the southern flank. THEMIS-VIS image clearly shows the upper boundary of the dark halo; brighter near the summit and darker in the lower position. THEMIS-IRDaytime image shows brighter color in the dark halo, which indicates higher temperature. The boundary completely coincides with that in VIS. THEMIS-IRNighttime image also shows brighter color in the dark halo. This variation in the brightness and hence the surface temperature in IR images is not consistent with general thermal inertia control between daytime and nighttime by the change of grain size. This enigmatic behavior may indicate the surface of dark halo has different thermal response to the irradiation by the sunlight at daytime and radiative cooling at nighttime. This might be possible if the surface is covered by mixture of fine silicate particles supported by continuous phase of ice. References [1] Geissler, P. E., (2005) JGR, 110, E02001. [2] Armstrong, J. C. et al., (2007) GRL, 34, L01202. [3] Smith M. D., (2004) Icarus, 167, 148-165. [4] Neakrase, L. et al., (2005) LPSC XXXZVI, P1898.
Kawaguchi Kentaro
Kurita Kazuyoshi
Toyota Takenobu
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