Third-Body Perturbation Using a Single Averaged Model: Application in Nonsingular Variables

The Lagrange's planetary equations written in terms of the classical orbital elements have the disadvantage of singularities in eccentricity and inclination. These singularities are due to the mathematical model used and do not have physical reasons. In this paper, we studied the thir...

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Main Authors: Carlos Renato Huaura Solórzano, Antonio Fernando Bertachini de Almeida Prado
Format: Article
Language:English
Published: Hindawi Limited 2007-01-01
Series:Mathematical Problems in Engineering
Online Access:http://dx.doi.org/10.1155/2007/40475
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spelling doaj-324344f494094049aa5d16498f1af0e52020-11-24T23:04:18ZengHindawi LimitedMathematical Problems in Engineering1024-123X1563-51472007-01-01200710.1155/2007/4047540475Third-Body Perturbation Using a Single Averaged Model: Application in Nonsingular VariablesCarlos Renato Huaura Solórzano0Antonio Fernando Bertachini de Almeida Prado1National Institute for Space Research (INPE), São José Dos Campos, SP 12227-010, BrazilNational Institute for Space Research (INPE), São José Dos Campos, SP 12227-010, BrazilThe Lagrange's planetary equations written in terms of the classical orbital elements have the disadvantage of singularities in eccentricity and inclination. These singularities are due to the mathematical model used and do not have physical reasons. In this paper, we studied the third-body perturbation using a single averaged model in nonsingular variables. The goal is to develop a semianalytical study of the perturbation caused in a spacecraft by a third body using a single averaged model to eliminate short-period terms caused by the motion of the spacecraft. This is valid if no resonance occurs with the moon or the sun. Several plots show the time histories of the Keplerian elements of equatorial and circular orbits, which are the situations with singularities. In this paper, the expansions are limited only to second order in eccentricity and for the ratio of the semimajor axis of the perturbing and perturbed bodies and to the fourth order for the inclination.http://dx.doi.org/10.1155/2007/40475
collection DOAJ
language English
format Article
sources DOAJ
author Carlos Renato Huaura Solórzano
Antonio Fernando Bertachini de Almeida Prado
spellingShingle Carlos Renato Huaura Solórzano
Antonio Fernando Bertachini de Almeida Prado
Third-Body Perturbation Using a Single Averaged Model: Application in Nonsingular Variables
Mathematical Problems in Engineering
author_facet Carlos Renato Huaura Solórzano
Antonio Fernando Bertachini de Almeida Prado
author_sort Carlos Renato Huaura Solórzano
title Third-Body Perturbation Using a Single Averaged Model: Application in Nonsingular Variables
title_short Third-Body Perturbation Using a Single Averaged Model: Application in Nonsingular Variables
title_full Third-Body Perturbation Using a Single Averaged Model: Application in Nonsingular Variables
title_fullStr Third-Body Perturbation Using a Single Averaged Model: Application in Nonsingular Variables
title_full_unstemmed Third-Body Perturbation Using a Single Averaged Model: Application in Nonsingular Variables
title_sort third-body perturbation using a single averaged model: application in nonsingular variables
publisher Hindawi Limited
series Mathematical Problems in Engineering
issn 1024-123X
1563-5147
publishDate 2007-01-01
description The Lagrange's planetary equations written in terms of the classical orbital elements have the disadvantage of singularities in eccentricity and inclination. These singularities are due to the mathematical model used and do not have physical reasons. In this paper, we studied the third-body perturbation using a single averaged model in nonsingular variables. The goal is to develop a semianalytical study of the perturbation caused in a spacecraft by a third body using a single averaged model to eliminate short-period terms caused by the motion of the spacecraft. This is valid if no resonance occurs with the moon or the sun. Several plots show the time histories of the Keplerian elements of equatorial and circular orbits, which are the situations with singularities. In this paper, the expansions are limited only to second order in eccentricity and for the ratio of the semimajor axis of the perturbing and perturbed bodies and to the fourth order for the inclination.
url http://dx.doi.org/10.1155/2007/40475
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AT antoniofernandobertachinidealmeidaprado thirdbodyperturbationusingasingleaveragedmodelapplicationinnonsingularvariables
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