P53A-2104
The Low-Degree Shape of Mercury

Friday, 18 December 2015
Poster Hall (Moscone South)
Mark E Perry, Applied Physics Laboratory Johns Hopkins, Laurel, MD, United States
Abstract:
The shape of Mercury, particularly when combined with its geoid, provides clues to the planet’s internal structure, thermal evolution, and rotational history. Twenty-five million elevation measurements of the northern hemisphere, acquired by the Mercury Laser Altimeter on the MErcury Surface, Space ENvironment, GEochemistry, and Ranging spacecraft, were combined with 378 occultation measurements of radio-frequency signals from the spacecraft in the planet’s southern hemisphere to reveal the low-degree shape of Mercury. We solved for the spherical-harmonic coefficients through degree and order 128 and found that Mercury’s mean radius is 2439.36±0.02 km. The offset between the planet’s centers of mass and figure is negligible (40±40 m) along the polar axis and modest (140±50 m) in the equatorial plane.

Mercury’s spherical-harmonic shape spectrum is dominated by degree 2, and the planet’s first-order shape is that of a triaxial ellipsoid with semimajor axes a, b, and c. The polar radius, c, is 1.65 km less than (a+b)/2, and the equatorial difference, a-b, is 1.25 km. The long axis is rotated 15° west of Mercury’s dynamically defined principal axis. Mercury’s geoid is similarly dominated by degree 2 and well described by a triaxial ellipsoid. The degree-2 geoid and shape are highly correlated, but the power spectral density of the geoid at degree 2 is only 1% of its shape counterpart, implying substantial compensation of elevation variations on a global scale and that Mercury is not in hydrostatic equilibrium.