2012
DOI: 10.1029/2012je004062
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Density and porosity of the lunar crust from gravity and topography

Abstract: [1] Newly obtained gravity and topography data of the Moon, combined with a lithospheric flexure model that considers both surface and subsurface loading, are used to place constraints on the density of the upper crust from a localized spectral admittance analysis. Subsurface loads are found to be relatively unimportant in the highlands, and when subsurface loads are neglected, the best fitting bulk densities for a number of highland regions are found to vary from 2590 to 2870 kg m À3 , with a mean value of 26… Show more

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Cited by 85 publications
(80 citation statements)
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“…Although the depth dependence of porosity is not well constrained, it must extend at least several kilometers below the surface and perhaps into the upper mantle. These high porosities are almost certainly a result of fractures generated by billions of years of impact cratering and are consistent with impact-induced porosities associated with small impact craters on Earth (see also Huang and Wieczorek, 2012).…”
Section: The Moonsupporting
confidence: 53%
“…Although the depth dependence of porosity is not well constrained, it must extend at least several kilometers below the surface and perhaps into the upper mantle. These high porosities are almost certainly a result of fractures generated by billions of years of impact cratering and are consistent with impact-induced porosities associated with small impact craters on Earth (see also Huang and Wieczorek, 2012).…”
Section: The Moonsupporting
confidence: 53%
“…In order to make progress on inverting for the thickness of the mare, it was found necessary to set one or more of these parameters to fixed values based on a priori information. To start, we made use of a mare basalt grain density map, estimated from Lunar Prospector gamma‐ray spectrometer iron and titanium abundances [ Prettyman et al , ], along with an empirical density‐composition relation based on petrological considerations from Huang and Wieczorek []. We assumed a bulk porosity of 6% (which reduces the density by the same factor) and also considered a higher value of 12%, which is the porosity of the upper highland crust derived from GRAIL gravity data [ Wieczorek et al , ].…”
Section: Resultsmentioning
confidence: 99%
“…As shown in Figure , the model contains a constant thickness layer of dense mare basalts overlying less dense highland materials. For the upper mare layer, we assume that the density of the basalts does not vary with depth, and the bulk density is calculated using an assumed constant porosity along with the grain density derived from remote sensing and petrological considerations [ Huang and Wieczorek , ]. For the highland layer, we assume that the density increases linearly with depth due to the reduction of porosity with depth [ Besserer et al , ], reaching a maximum value where the porosity is zero.…”
Section: Methodsmentioning
confidence: 99%
“…1). At half wavelengths greater than ~68 km, the correlation between topography and gravity is weak (Wieczorek et al, 2006) due to the effects of crustal thickness variations (Neumann et al, 1996;Wieczorek and Phillips, 1998;Namiki et al, 2009;Huang and Wieczorek, 2012;Wieczorek et al, 2013;Zuber et al, 2013b), mascon loading (AndrewsHanna, 2013; Melosh et al, 2013;Freed et al, 2014), and lithospheric flexure. These longwavelength signals are commonly inverted for global crustal thickness modeling, where the assumption is made that the crust of the Moon is characterized by either a constant density or by long-wavelength variations in regional density (Wieczorek et al, 2006;Wieczorek et al, 2013).…”
Section: Introductionmentioning
confidence: 99%