Abstract

1 Summary A second-order approximation of the tesseroid method has been presented in the paper “A comparison of the tesseroid, prism and point-mass approaches for mass reductions in gravity field modelling” (Heck and Seitz 2007) for the gravitational potential and its first radial derivative. In the paper “Optimizedformulasforthegravitationalfieldofatesseroid” (Grombein et al. 2013) this analytical approach was optimized and extended to all first- and second-order derivatives of the potential. In both papers the general expression of the Taylor series expansion contains a formal error and needs to be corrected. As will be shown, this correction or rather erratum has no impact on the published and widely used second-order tesseroid formulas.

Highlights

  • In both papers the general expression of the Taylor series expansion contains a formal error and needs to be corrected

  • The disadvantage of the tesseroid method is that no analytical solutions of the respective mass integrals exist

  • Heck and Seitz (2007) presented an approximation approach for calculating the gravitational potential and its first radial derivative of a spherical tesseroid based on Taylor expansion (see Eqs. (21)–(23) and (32)–(33))

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Summary

Introduction

In both papers the general expression of the Taylor series expansion contains a formal error and needs to be corrected. Heck and Seitz (2007) presented an approximation approach for calculating the gravitational potential and its first radial derivative of a spherical tesseroid based on Taylor expansion The Taylor expansion of the integral kernel

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