• DOI:10.1002/jgre.20091
• Corpus ID: 17668886

The curious case of Mercury's internal structure

@article{Hauck2013TheCC,
  title={The curious case of Mercury's internal structure},
  author={Steven A. Hauck, and Jean-Luc Margot and Sean C. Solomon and Roger J. Phillips and Catherine L. Johnson and Frank LeMoine and Erwan M. Mazarico and Timothy J. Mccoy and Sebastiano Padovan and Stanton J. Peale and Mark E. Perry and David E. Smith and Maria T. Zuber},
  journal={Journal of Geophysical Research: Planets},
  year={2013},
  volume={118},
  pages={1204 - 1220}
}

• S. Hauck,, J. Margot, +10 authors M. Zuber
• Published 1 June 2013
• Physics
• Journal of Geophysical Research: Planets

The recent determination of the gravity field of Mercury and new Earth‐based radar observations of the planet's spin state afford the opportunity to explore Mercury's internal structure. These observations provide estimates of two measures of the radial mass distribution of Mercury: the normalized polar moment of inertia and the fractional polar moment of inertia of the solid portion of the planet overlying the liquid core. Employing Monte Carlo techniques, we calculate several million models of the radial density structure of Mercury consistent with its radius and bulk density and constrained by these moment of inertia parameters. We estimate that the top of the liquid core is at a radius of 2020 ± 30 km, the mean density above this boundary is 3380 ± 200 kg m−3, and the density below the boundary is 6980 ± 280 kg m−3. We find that these internal structure parameters are robust across a broad range of compositional models for the core and planet as a whole. Geochemical observations of Mercury's surface by MESSENGER indicate a chemically reducing environment that would favor the partitioning of silicon or both silicon and sulfur into the metallic core during core‐mantle differentiation. For a core composed of Fe–S–Si materials, the thermodynamic properties at elevated pressures and temperatures suggest that an FeS‐rich layer could form at the top of the core and that a portion of it may be presently solid.