Abstract <p>A new method is used to study a current version of the two-planet problem on the secular evolution of planetary orbits with small eccentricities and mutual inclinations, having an arbitrary orientation relative to the main (picture) plane. A model has been developed that describes a wide class of exoplanetary systems with an inclination angle of orbits different from <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11444_2025_1707_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="33" /> </InlineMediaObject> <EquationSource Format="TEX">\(\pi {\text{/}}2.\)</EquationSource> <!--AstEng2570202Kondratev-m1--> </InlineEquation> The orbits of the planets are modeled by the Gaussian rings, the perturbing function is represented by the mutual gravitational energy of these rings in the form of a series up to terms of second order of smallness. To describe the evolution of orbits, instead of osculating Keplerian elements, a new set of variables is introduced: the unit vector <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11444_2025_1707_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="16" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathbf{R}}\)</EquationSource> <!--AstEng2570202Kondratev-m2--> </InlineEquation> of normal to the plane of the ring and two Poincaré variables <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11444_2025_1707_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="45" /> </InlineMediaObject> <EquationSource Format="TEX">\(\left( {p,q} \right);\)</EquationSource> <!--AstEng2570202Kondratev-m3--> </InlineEquation> for eight independent variables, a system of differential equations is obtained and analytically solved. The method is applied to study the secular evolution of the two-planet system Kepler-117 (KOI-209) with non-resonant orbits of exoplanets. It has been established that in this system the oscillations of the same components of the orientation vector <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11444_2025_1707_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="16" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathbf{R}}\)</EquationSource> <!--AstEng2570202Kondratev-m4--> </InlineEquation> for each of the orbits, as well as the values <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11444_2025_1707_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="62" /> </InlineMediaObject> <EquationSource Format="TEX">\(\left( {e,i,{{\Omega }}} \right),\)</EquationSource> <!--AstEng2570202Kondratev-m5--> </InlineEquation> occur strictly in antiphase. The eccentricities of both orbits oscillate with the period <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11444_2025_1707_Article_IEq6.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="124" /> </InlineMediaObject> <EquationSource Format="TEX">\({{T}_{\kappa }} \approx 182.3\;{\text{years}},\)</EquationSource> <!--AstEng2570202Kondratev-m6--> </InlineEquation> and the inclinations of the orbits and the longitudes of the ascending nodes change in the libration mode with the same period <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11444_2025_1707_Article_IEq7.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="124" /> </InlineMediaObject> <EquationSource Format="TEX">\({{T}_{g}} \approx {\text{174}}.5\;{\text{years}}.\)</EquationSource> <!--AstEng2570202Kondratev-m7--> </InlineEquation> The lines of the orbital apsides rotate unevenly counterclockwise with the periods of secular rotation <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11444_2025_1707_Article_IEq8.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="123" /> </InlineMediaObject> <EquationSource Format="TEX">\({{T}_{{{{g}_{2}}}}} \approx 178.3\;{\text{years}}\)</EquationSource> <!--AstEng2570202Kondratev-m8--> </InlineEquation> (for a light planet), and <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11444_2025_1707_Article_IEq9.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="119" /> </InlineMediaObject> <EquationSource Format="TEX">\({{T}_{{{{g}_{1}}}}} \approx 8140\;{\text{years}}\)</EquationSource> <!--AstEng2570202Kondratev-m9--> </InlineEquation> (for a more massive planet).</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

A Two-Planet Problem with an Arbitrary Inclination of a Pair of Orbits. Secular Evolution of the Kepler-117 Exosystem

  • B. P. Kondratyev,
  • V. S. Kornoukhov

摘要

Abstract

A new method is used to study a current version of the two-planet problem on the secular evolution of planetary orbits with small eccentricities and mutual inclinations, having an arbitrary orientation relative to the main (picture) plane. A model has been developed that describes a wide class of exoplanetary systems with an inclination angle of orbits different from \(\pi {\text{/}}2.\) The orbits of the planets are modeled by the Gaussian rings, the perturbing function is represented by the mutual gravitational energy of these rings in the form of a series up to terms of second order of smallness. To describe the evolution of orbits, instead of osculating Keplerian elements, a new set of variables is introduced: the unit vector \({\mathbf{R}}\) of normal to the plane of the ring and two Poincaré variables \(\left( {p,q} \right);\) for eight independent variables, a system of differential equations is obtained and analytically solved. The method is applied to study the secular evolution of the two-planet system Kepler-117 (KOI-209) with non-resonant orbits of exoplanets. It has been established that in this system the oscillations of the same components of the orientation vector \({\mathbf{R}}\) for each of the orbits, as well as the values \(\left( {e,i,{{\Omega }}} \right),\) occur strictly in antiphase. The eccentricities of both orbits oscillate with the period \({{T}_{\kappa }} \approx 182.3\;{\text{years}},\) and the inclinations of the orbits and the longitudes of the ascending nodes change in the libration mode with the same period \({{T}_{g}} \approx {\text{174}}.5\;{\text{years}}.\) The lines of the orbital apsides rotate unevenly counterclockwise with the periods of secular rotation \({{T}_{{{{g}_{2}}}}} \approx 178.3\;{\text{years}}\) (for a light planet), and \({{T}_{{{{g}_{1}}}}} \approx 8140\;{\text{years}}\) (for a more massive planet).