T44 Impact Craters: Structures, Drilling, Ages, and Geophysics
Sunday, 22 October 2006
1:30 PM - 5:30 PM
MOHO UPWARPING BENEATH THE CHICXULUB IMPACT CRATER
Paper number: T44-9
Program: Technical Sessions
Time: 3:45 PM – 4:00 PM
Authors
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Sean GulickJohn A. and Katherine G. Jackson School of Geosciences, Austin, TX
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Joanna MorganImperial College London, London
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Mike WarnerImperial College London, London, N/A
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Penny BartonUniversity of Cambridge, Cambridge, N/A
Abstract
Moho upwarping has also been observed beneath lunar craters, and has been attributed to rapid mantle uplift following impact (e.g., Taylor, 1982; Neumann et al., 1996). These craters are not in isostatic equilibrium, implying that the lithosphere is strong enough to maintain these stress states. The Chicxulub crater is also not in isostatic equilibrium. Scaling laws place the depth of the transient cavity at 35-40 km below the transient crater rim for the Chicxulub impact crater (Morgan et al., 1997). This depth suggests that deformation from the impact may have reached the base of the crust, although it should be noted that transient cavity depth is measured from the transient crater rim which could have had a maximum uplift of ~8 km (Morgan et al., 1997). Asthenospheric flow is a component of the ring tectonic theory of multiring crater formation (Melosh and McKinnon, 1978); this flow may result in the Moho topography constrained by our data. The relationships between ring locations, crustal faulting, and Moho topography should provide new insights into the mechanics of multiring crater formation.
References: Melosh, H.J. and W.B. McKinnon (1978), Geophys. Res. Lett. 5, 985-988. Morgan, J. et al. (1997), Nature 390, 472-476. Neumann et al. (1996), J. Geophys. Res., 101, 16,841-16,843. Taylor (1982), Planetary Science: A Lunar Perspective.