Mixed-model gravity representations for small celestial bodies using mascons and spherical harmonics

When designing and navigating space missions to asteroids and comets, mascon models can be attractive because they are simple to compute, implement, and parallelize. However, to achieve a reasonable surface accuracy, mascon models typically require too many elements to compete with other models. Here, mascon models are revisited, with the intent to minimize the number of elements, optimize the placement of the elements, and modify the base model of elements in order to improve computational efficiency, while enabling their use at low altitudes. The addition of small radius spherical harmonics elements, buried within a mascon model, is shown to offer model evaluation speedups and reduced memory footprints at little or no accuracy cost over homogeneous mascon models. In addition, such hybrid models are shown to provide runtimes over an order of magnitude faster than low-resolution polyhedral models for equivalent accuracy. This hybrid gravity model approach is designed for use at small celestial bodies having any regular or irregular shape; a demonstrative and detailed analysis is presented for the case of 433 Eros.

[1]  Oliver Baur,et al.  Tailored least-squares solvers implementation for high-performance gravity field research , 2009, Comput. Geosci..

[3]  Jason M. Pearl,et al.  Asteroid Gravitational Models Using Mascons Derived from Polyhedral Sources , 2016 .

[4]  M. Watkins,et al.  Quantifying and reducing leakage errors in the JPL RL05M GRACE mascon solution , 2016 .

[5]  Allan Cheuvront,et al.  The OSIRIS-REx Asteroid Sample Return Mission operations design , 2015, 2015 IEEE Aerospace Conference.

[6]  R. Bijani,et al.  Three-dimensional gravity inversion using graph theory to delineate the skeleton of homogeneous sources , 2015 .

[7]  K. Koch,et al.  A simple layer model of the geopotential from a combination of satellite and gravity data , 1970 .

[8]  R. Park,et al.  Estimating Small-Body Gravity Field from Shape Model and Navigation Data , 2008 .

[9]  Veverka,et al.  Radio science results during the NEAR-shoemaker spacecraft rendezvous with eros , 2000, Science.

[10]  K. Koch,et al.  Earth's gravity field represented by a simple-layer potential from Doppler tracking of satellites , 1971 .

[11]  Anil N. Hirani,et al.  Adaptive Gravitational Force Representation for Fast Trajectory Propagation Near Small Bodies , 2008 .

[12]  Samuel Pines,et al.  Uniform Representation of the Gravitational Potential and its Derivatives , 1973 .

[13]  Ricardo Vieira,et al.  A 3-D gravity inversion tool based on exploration of model possibilities , 2002 .

[14]  Nitin Arora,et al.  Global Point Mascon Models for Simple, Accurate, and Parallel Geopotential Computation , 2012 .

[15]  Daniel J. Scheeres,et al.  Surface Gravity Fields for Asteroids and Comets , 2013 .

[16]  W. Sjogren,et al.  A surface‐layer representation of the lunar gravitational field , 1971 .

[17]  W. M. Kaula,et al.  Theory of Satellite Geodesy: Applications of Satellites to Geodesy , 2000 .

[18]  H. Melosh Mascons and the moon's orientation , 1975 .

[19]  D. A. Cicci Improving gravity field determination in ill-conditioned inverse problems , 1992 .

[20]  G. Romain,et al.  Ellipsoidal Harmonic expansions of the gravitational potential: Theory and application , 2001 .

[21]  L. C. Ramos,et al.  Efficient gravity inversion of discontinuous basement relief , 2015 .

[22]  D. Scheeres,et al.  Exterior gravitation of a polyhedron derived and compared with harmonic and mascon gravitation representations of asteroid 4769 Castalia , 1996 .

[23]  Nitin Arora,et al.  Efficient Interpolation of High-Fidelity Geopotentials , 2016 .

[24]  Zuber,et al.  The shape of 433 eros from the NEAR-shoemaker laser rangefinder , 2000, Science.

[25]  Srinivas Bettadpur,et al.  High‐resolution CSR GRACE RL05 mascons , 2016 .

[26]  M. A. Pérez-Flores,et al.  Refinement of three-dimensional multilayer models of basins and crustal environments by inversion of gravity and magnetic data , 2005 .

[27]  J. Anderson,et al.  Mass Anomalies on Ganymede , 2004 .

[28]  Foster Morrison,et al.  Algorithms for computing the geopotential using a simple density layer , 1976 .

[29]  Robert A. Werner Spherical harmonic coefficients for the potential of a constant-density polyhedron , 1997 .

[30]  Simon Tardivel,et al.  The Limits of the Mascons Approximation of the Homogeneous Polyhedron , 2016 .

[31]  Georges Balmino,et al.  Gravitational potential harmonics from the shape of an homogeneous body , 1994 .

[32]  R. Jaumann,et al.  Dawn arrives at Ceres: Exploration of a small, volatile-rich world , 2016, Science.

[33]  Anil N. Hirani,et al.  Structure Preserving Approximations of Conservative Forces for Application to Small-Body Dynamics , 2008 .