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Titlebook: Recent Advances in Dynamical Astronomy; Proceedings of the N B. D. Tapley,V. Szebehely Conference proceedings 1973 D. Reidel Publishing Com

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0067-0057 nal Restricted Problem 135 c. G. ZAGOURAS / Planar Periodic Orbits Using Second and Third Variations 146 E. RABE / Elliptic Restricted Problem: Fourth-Order Sta978-94-010-2613-0978-94-010-2611-6Series ISSN 0067-0057 Series E-ISSN 2214-7985
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Conference proceedings 1973care 109 G. KATSIARIS / The Three-Dimensional Elliptic Problem 118 P. G. KAZANTZIS / Second and Third Order Variations of the Three Dimensional Restricted Problem 135 c. G. ZAGOURAS / Planar Periodic Orbits Using Second and Third Variations 146 E. RABE / Elliptic Restricted Problem: Fourth-Order Sta
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The Application of Recurrence Relations to Special Perturbation Methodsase of two body motion. The Taylor method is then applied in turn to the methods of Cowell and Encke in rectangular coordinates, and to a set of perturbational equations using as an example the restricted three body problem. An indication is given of the conditions under which each method is most efficient.
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The Three-Dimensional Elliptic Probleme system used is the rotating-pulsating one in which the two primaries are at rest. After developing the method for calculation of three-dimensional periodic orbits and of their stability characteristics, we proceed to present numerical results which were obtained by using the computer 1906A ICL of the University of Manchester.
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A Linear Theory of the Perturbed Two-Body Problem (Regularization)Discussion of the numerical solution of Keplerian motion. Singularities and instability of the classical differential equation. Regularization and stabilization by the KS-transformation. Abbreviated description of that transformation and application to the perturbed two-body problem. Orbital elements.
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Regularization Using a Time-Transformation OnlyIt is possible to regularize the perturbed Kepler problem by performing a transformation of the time only. The regularized equations are derived and interpreted, and they are shown to have properties of value in analytic and in numerical applications.
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The Particular Solutions of Levi-CivitaTo every invariant manifold (.) of an Hamiltonian system (.) is associated a particular solution. The trajectory is the set of points of (.) for which . is extremal. The time is determined by quadratures..This is an extension of the well-known steady solution associated with an ignorable coordinate.
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