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The uniform, regular differential equations of the KS transformed perturbed two-body problem

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Abstract

The Newtonian differential equations of motion for the two-body problem can be transformed into four, linear, harmonic oscillator equations by simultaneously applying the regularizing time transformation dt/ds=r and the Kustaanheimo-Stiefel (KS) coordinate transformation. The time transformation changes the independent variable from time to a new variables, and the KS transformation transforms the position and velocity vectors from Cartesian space into a four-dimensional space. This paper presents the derivation of uniform, regular equations for the perturbed twobody problem in the four-dimensional space. The variation of parameters technique is used to develop expressions for the derivatives of ten elements (which are constants in the unperturbed motion) for the general case that includes both perturbations which can arise from a potential and perturbations which cannot be derived from a potential. These element differential equations are slightly modified by introducing two additional elements for the time to further improve long term stability of numerical integration.

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References

  • Burdet, C. A.: 1968,Z. Angew. Math. Phys. 19, 345–368.

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  • Stiefel, E. L. and Scheifele, G.: 1971,Linear and Regular Celestial Mechanics, Springer, Berlin.

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Bond, V.R. The uniform, regular differential equations of the KS transformed perturbed two-body problem. Celestial Mechanics 10, 303–318 (1974). https://doi.org/10.1007/BF01586860

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