Abstract
This work presents an elegant formalism to model the evolution of the full two rigid body problem. The equations of motion, given in a Cartesian coordinate system, are expressed in terms of spherical harmonics and Wigner D-matrices. The algorithm benefits from the numerous recurrence relations satisfied by these functions allowing a fast evaluation of the mutual potential. Moreover, forces and torques are straightforwardly obtained by application of ladder operators taken from the angular momentum theory and commonly used in quantum mechanics. A numerical implementation of this algorithm is made. Tests show that the present code is significantly faster than those currently available in literature.
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Notes
If we denote by \(\{C^{(T)}_{lm},S^{(T)}_{lm}\}\) the Stokes coefficients defined in (Tricarico 2008, Eqs. 14, 15), those of the present paper are given by \(\{C_{lm}, S_{lm}\} = N_{lm} \{C^{(T)}_{lm},S^{(T)}_{lm}\}\) with
$$\begin{aligned} N_{lm} = \frac{2}{1+\delta _{m,0}}\frac{(l-m)!}{(l+m)!} . \end{aligned}$$
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Boué, G. The two rigid body interaction using angular momentum theory formulae. Celest Mech Dyn Astr 128, 261–273 (2017). https://doi.org/10.1007/s10569-017-9751-2
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DOI: https://doi.org/10.1007/s10569-017-9751-2