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Albedo effects in the ER3BP with an oblate primary, a triaxial secondary and a potential due to belt
We have examined the effects of Albedo in the Elliptic Restricted Three-Body Problem (ER3BP) with an oblate primary, a triaxial secondary, and potential due to belt for the Earth–Moon system. We have found that as the perturbed parameters increases, the possible boundary regions of the primary come...
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Formato: | Online Artículo Texto |
Lenguaje: | English |
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Nature Publishing Group UK
2023
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10017830/ https://www.ncbi.nlm.nih.gov/pubmed/36922508 http://dx.doi.org/10.1038/s41598-023-30671-3 |
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author | Singh, Jagadish Richard, Tyokyaa K. |
author_facet | Singh, Jagadish Richard, Tyokyaa K. |
author_sort | Singh, Jagadish |
collection | PubMed |
description | We have examined the effects of Albedo in the Elliptic Restricted Three-Body Problem (ER3BP) with an oblate primary, a triaxial secondary, and potential due to belt for the Earth–Moon system. We have found that as the perturbed parameters increases, the possible boundary regions of the primary come closer to one other, allowing particles to travel from one region to the next freely and possibly merge the permissible regions. Our study has revealed that the formation of triangular libration points depends on the Albedo effects, semi-major axis, the Eccentricity of the orbits, triaxiality, and the potential due to the belt. As the parameters mentioned above increase, the triangular positions [Formula: see text] and [Formula: see text] move towards the center of origin in cases 1, 2, 3, and 4 and away from the center of the origin in cases 5, 6, and 7. Considering the range of a stable and unstable libration point for the problem under study given as [Formula: see text] for stable libration points and [Formula: see text] for unstable libration points, our study has established that the triangular libration points are respectively stable and unstable for cases 1, 2, and 6 and cases 3, 4, 5, and 7. Our study has also revealed that each set of values has at least one characteristic complex root with a positive real part. Hence, the triangular libration points for the Earth–Moon system are unstable in the sense of Lyapunov. The Earth–Moon system's Poincare Surface of Section (PSS) has demonstrated that a slight change in the initial conditions, the semi-major axis, and the Eccentricity of the orbits have affected the system's behavior dramatically. Further, it is seen that a chaotic dynamical behavior of the system results into either regular or irregular orbits. |
format | Online Article Text |
id | pubmed-10017830 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2023 |
publisher | Nature Publishing Group UK |
record_format | MEDLINE/PubMed |
spelling | pubmed-100178302023-03-17 Albedo effects in the ER3BP with an oblate primary, a triaxial secondary and a potential due to belt Singh, Jagadish Richard, Tyokyaa K. Sci Rep Article We have examined the effects of Albedo in the Elliptic Restricted Three-Body Problem (ER3BP) with an oblate primary, a triaxial secondary, and potential due to belt for the Earth–Moon system. We have found that as the perturbed parameters increases, the possible boundary regions of the primary come closer to one other, allowing particles to travel from one region to the next freely and possibly merge the permissible regions. Our study has revealed that the formation of triangular libration points depends on the Albedo effects, semi-major axis, the Eccentricity of the orbits, triaxiality, and the potential due to the belt. As the parameters mentioned above increase, the triangular positions [Formula: see text] and [Formula: see text] move towards the center of origin in cases 1, 2, 3, and 4 and away from the center of the origin in cases 5, 6, and 7. Considering the range of a stable and unstable libration point for the problem under study given as [Formula: see text] for stable libration points and [Formula: see text] for unstable libration points, our study has established that the triangular libration points are respectively stable and unstable for cases 1, 2, and 6 and cases 3, 4, 5, and 7. Our study has also revealed that each set of values has at least one characteristic complex root with a positive real part. Hence, the triangular libration points for the Earth–Moon system are unstable in the sense of Lyapunov. The Earth–Moon system's Poincare Surface of Section (PSS) has demonstrated that a slight change in the initial conditions, the semi-major axis, and the Eccentricity of the orbits have affected the system's behavior dramatically. Further, it is seen that a chaotic dynamical behavior of the system results into either regular or irregular orbits. Nature Publishing Group UK 2023-03-15 /pmc/articles/PMC10017830/ /pubmed/36922508 http://dx.doi.org/10.1038/s41598-023-30671-3 Text en © The Author(s) 2023 https://creativecommons.org/licenses/by/4.0/Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/ (https://creativecommons.org/licenses/by/4.0/) . |
spellingShingle | Article Singh, Jagadish Richard, Tyokyaa K. Albedo effects in the ER3BP with an oblate primary, a triaxial secondary and a potential due to belt |
title | Albedo effects in the ER3BP with an oblate primary, a triaxial secondary and a potential due to belt |
title_full | Albedo effects in the ER3BP with an oblate primary, a triaxial secondary and a potential due to belt |
title_fullStr | Albedo effects in the ER3BP with an oblate primary, a triaxial secondary and a potential due to belt |
title_full_unstemmed | Albedo effects in the ER3BP with an oblate primary, a triaxial secondary and a potential due to belt |
title_short | Albedo effects in the ER3BP with an oblate primary, a triaxial secondary and a potential due to belt |
title_sort | albedo effects in the er3bp with an oblate primary, a triaxial secondary and a potential due to belt |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10017830/ https://www.ncbi.nlm.nih.gov/pubmed/36922508 http://dx.doi.org/10.1038/s41598-023-30671-3 |
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