Abstract:To explore the mechanisms of support of surface topography on Mercury, we have determined the admittances and correlations of topography and gravity in Mercury's northern hemisphere from measurements obtained by NASA's MErcury Surface, Space ENvironment, GEochemistry, and Ranging (MESSENGER) spacecraft. These admittances and correlations can be interpreted in the context of a number of theoretical scenarios, including flexural loading and dynamic flow. We find that long-wavelength (spherical harmonic degree l … Show more
“…The thermal and compositional structure of the mantle shown in Figure is in conflict with the mantle structure that James et al . [] suggest for Mercury in some of their models. In these models that are based on analyses of the gravity anomalies observed over the swells of the planet, they assume that there is a compositionally dense layer with laterally varying thickness on the CMB and suggest that this lateral variation dynamically supports the swells.…”
Section: Discussionmentioning
confidence: 99%
“…However, the thickness of this layer is laterally uniform, because the viscosity is only 10 19 –10 22 Pa after 2 Gyr in the deep mantle (see Figure g for 2.13 and 4.42 Gyr); lateral density variations are quickly relaxed at such a low viscosity, as Figure 11 of James et al . [] predicts. The low viscosity in the deep mantle is a consequence of the high temperature there maintained by the persistent compositional stratification of the mantle.…”
Section: Discussionmentioning
confidence: 99%
“…The third is the consistency with the observed topography and gravity anomalies of Mercury [ James et al ., ]. In Figures a and c the deep mantle is compositionally homogeneous after 3 Gyr, and the viscosity there is less than 10 20 Pa s throughout the calculated history of the mantle.…”
Section: Discussionmentioning
confidence: 99%
“…[] suggest that mantle convection ceases within 3–4 Gyr after the planetary formation. More detailed studies are now in progress to further impose and/or revise observational constraints on Mercury's interior [e.g., Weider et al ., , ; Byrne et al ., ; James et al ., ], and more refined numerical models are needed to understand outcome of these studies in the context of mantle evolution.…”
To discuss mantle evolution in Mercury, I present two‐dimensional numerical models of magmatism in a convecting mantle. Thermal, compositional, and magmatic buoyancy drives convection of temperature‐dependent viscosity fluid in a rectangular box placed on the top of the core that is modeled as a heat bath of uniform temperature. Magmatism occurs as a permeable flow of basaltic magma generated by decompression melting through a matrix. Widespread magmatism caused by high initial temperature of the mantle and the core makes the mantle compositionally stratified within the first several hundred million years of the 4.5 Gyr calculated history. The stratified structure persists for 4.5 Gyr, when the reference mantle viscosity at 1573 K is higher than around 1020 Pa s. The planet thermally contracts by an amount comparable to the one suggested for Mercury over the past 4 Gyr. Mantle upwelling, however, generates magma only for the first 0.1–0.3 Gyr. At lower mantle viscosity, in contrast, a positive feedback between magmatism and mantle upwelling operates to cause episodic magmatism that continues for the first 0.3–0.8 Gyr. Convective current stirs the mantle and eventually dissolves its stratified structure to enhance heat flow from the core and temporarily resurrect magmatism depending on the core size. These models, however, predict larger contraction of the planet. Coupling between magmatism and mantle convection plays key roles in mantle evolution, and the difficulty in numerically reproducing the history of magmatism of Mercury without causing too large radial contraction of the planet warrants further exploration of this coupling.
“…The thermal and compositional structure of the mantle shown in Figure is in conflict with the mantle structure that James et al . [] suggest for Mercury in some of their models. In these models that are based on analyses of the gravity anomalies observed over the swells of the planet, they assume that there is a compositionally dense layer with laterally varying thickness on the CMB and suggest that this lateral variation dynamically supports the swells.…”
Section: Discussionmentioning
confidence: 99%
“…However, the thickness of this layer is laterally uniform, because the viscosity is only 10 19 –10 22 Pa after 2 Gyr in the deep mantle (see Figure g for 2.13 and 4.42 Gyr); lateral density variations are quickly relaxed at such a low viscosity, as Figure 11 of James et al . [] predicts. The low viscosity in the deep mantle is a consequence of the high temperature there maintained by the persistent compositional stratification of the mantle.…”
Section: Discussionmentioning
confidence: 99%
“…The third is the consistency with the observed topography and gravity anomalies of Mercury [ James et al ., ]. In Figures a and c the deep mantle is compositionally homogeneous after 3 Gyr, and the viscosity there is less than 10 20 Pa s throughout the calculated history of the mantle.…”
Section: Discussionmentioning
confidence: 99%
“…[] suggest that mantle convection ceases within 3–4 Gyr after the planetary formation. More detailed studies are now in progress to further impose and/or revise observational constraints on Mercury's interior [e.g., Weider et al ., , ; Byrne et al ., ; James et al ., ], and more refined numerical models are needed to understand outcome of these studies in the context of mantle evolution.…”
To discuss mantle evolution in Mercury, I present two‐dimensional numerical models of magmatism in a convecting mantle. Thermal, compositional, and magmatic buoyancy drives convection of temperature‐dependent viscosity fluid in a rectangular box placed on the top of the core that is modeled as a heat bath of uniform temperature. Magmatism occurs as a permeable flow of basaltic magma generated by decompression melting through a matrix. Widespread magmatism caused by high initial temperature of the mantle and the core makes the mantle compositionally stratified within the first several hundred million years of the 4.5 Gyr calculated history. The stratified structure persists for 4.5 Gyr, when the reference mantle viscosity at 1573 K is higher than around 1020 Pa s. The planet thermally contracts by an amount comparable to the one suggested for Mercury over the past 4 Gyr. Mantle upwelling, however, generates magma only for the first 0.1–0.3 Gyr. At lower mantle viscosity, in contrast, a positive feedback between magmatism and mantle upwelling operates to cause episodic magmatism that continues for the first 0.3–0.8 Gyr. Convective current stirs the mantle and eventually dissolves its stratified structure to enhance heat flow from the core and temporarily resurrect magmatism depending on the core size. These models, however, predict larger contraction of the planet. Coupling between magmatism and mantle convection plays key roles in mantle evolution, and the difficulty in numerically reproducing the history of magmatism of Mercury without causing too large radial contraction of the planet warrants further exploration of this coupling.
“…(a) Color composite of Mercury with the Mercury Dual Imaging System 1,000, 750, and 430 nm narrow-band filters in the red, green, and blue channels, respectively. (f) LRM map overlain on crustal thickness map fromJames et al (2015) The yellow boxes indicate the locations of craters A-Akutagawa, SA-Sholem-Aleichem, B-Basho, T-Tolstoj, R-Rachmaninoff, and C-Craters within Caloris, and three regional enhancements, R1-3.…”
We examine the global distribution and spectral properties of low‐reflectance material (LRM) across Mercury to estimate the relative carbon abundance of prominent exposures and to test hypotheses for the origin of carbon in LRM. Our mapping demonstrates that LRM is consistently excavated from depth and that the spectral curvature attributed to carbon becomes more subdued as these surface deposits age. We find that the 600‐nm band depth in LRM deposits is related to carbon content and can be used to estimate carbon enrichment. LRM deposits excavated by basins and large craters may be enriched with as much as 4 wt% carbon over the local mean. Regional deposits, associated with the most heavily cratered terrains, are enriched by an average of ~2.5 wt% carbon. The association of LRM with excavation from depth shows that the carbon in LRM is native to the planet, rather than deposited over time by impacts.
The surface of Mercury is dominated by contractional tectonic landforms that are evidence of global‐scale crustal deformation. Using MESSENGER orbital high‐incidence angle imaging and topographic data, large‐scale lobate thrust fault scarps have been mapped globally. The spatial distribution and areal density of the contractional landforms are not uniform; concentrations occur in longitudinal bands and between the north and south hemispheres. Their orientations are generally north‐south at low latitude to midlatitude and east‐west at high latitudes. The spatial distribution and distribution of orientations of these large‐scale contractional features suggest that planet‐wide contraction due to interior cooling cannot be the sole source of global stresses. The nonrandom orientations are best explained by a combination of stresses from global contraction and tidal despinning combined with an equator‐to‐pole variation in lithospheric thickness, while the nonuniform areal density of the contractional features may indicate the influence of mantle downwelling or heterogeneities in lithospheric strength.
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