<p>For the <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40295_2025_514_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(J_2\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>J</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation>-problem, the mean-to-osculating transformation that guarantees the exact separation of long- and short-period terms up to the second order of <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40295_2025_514_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(J_2\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>J</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> has been recently reported by the author. The transformation was computed in Delaunay canonical variables. However, because such kind of solution is derived from a vectorial generating function, it can be obtained in arbitrary variables—either singular or not, canonical or non-canonical—without need of recomputing the perturbation solution. The procedure is illustrated for the insightful set of semi-equinoctial variables. It could be equally applied, if desired, to compute a second-order, closed-form, analytical model truly consistent with the Draper semianalytical satellite theory.</p>

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Purely Periodic, Second-Order Terms of the \(J_2\)-Problem in Closed Form and Arbitrary Variables

  • Martin Lara

摘要

For the \(J_2\) J 2 -problem, the mean-to-osculating transformation that guarantees the exact separation of long- and short-period terms up to the second order of \(J_2\) J 2 has been recently reported by the author. The transformation was computed in Delaunay canonical variables. However, because such kind of solution is derived from a vectorial generating function, it can be obtained in arbitrary variables—either singular or not, canonical or non-canonical—without need of recomputing the perturbation solution. The procedure is illustrated for the insightful set of semi-equinoctial variables. It could be equally applied, if desired, to compute a second-order, closed-form, analytical model truly consistent with the Draper semianalytical satellite theory.