Method for special perturbations
A method for computing special perturbations has been devised. At the present time we have only considered the case with three co-planar bodies. Only one differential equation is to be solved. The radius vector r is the dependent variable. The time has been taken as independent variable. The true an...
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Formato: | Articulo Comunicacion |
Lenguaje: | Inglés |
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1963
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Acceso en línea: | http://sedici.unlp.edu.ar/handle/10915/91811 |
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I19-R120-10915-918112024-07-04T18:52:32Z http://sedici.unlp.edu.ar/handle/10915/91811 Method for special perturbations Altavista, Carlos Alberto 1963 2020-03-26T10:44:06Z en Ciencias Astronómicas special perturbations A method for computing special perturbations has been devised. At the present time we have only considered the case with three co-planar bodies. Only one differential equation is to be solved. The radius vector r is the dependent variable. The time has been taken as independent variable. The true anomaly ν is the remaining quantity to be disturbed. The corresponding set of equations algebraic ones. The whole process is an iterative one. Special attention is to be paid for determining the most favorable cases for the applications. Asociación Argentina de Astronomía Articulo Comunicacion http://creativecommons.org/licenses/by-nc-sa/4.0/ Creative Commons Attribution-NonCommercial-ShareAlike 4.0 International (CC BY-NC-SA 4.0) application/pdf 94-94 |
institution |
Universidad Nacional de La Plata |
institution_str |
I-19 |
repository_str |
R-120 |
collection |
SEDICI (UNLP) |
language |
Inglés |
topic |
Ciencias Astronómicas special perturbations |
spellingShingle |
Ciencias Astronómicas special perturbations Altavista, Carlos Alberto Method for special perturbations |
topic_facet |
Ciencias Astronómicas special perturbations |
description |
A method for computing special perturbations has been devised. At the present time we have only considered the case with three co-planar bodies. Only one differential equation is to be solved. The radius vector r is the dependent variable. The time has been taken as independent variable. The true anomaly ν is the remaining quantity to be disturbed. The corresponding set of equations algebraic ones. The whole process is an iterative one. Special attention is to be paid for determining the most favorable cases for the applications. |
format |
Articulo Comunicacion |
author |
Altavista, Carlos Alberto |
author_facet |
Altavista, Carlos Alberto |
author_sort |
Altavista, Carlos Alberto |
title |
Method for special perturbations |
title_short |
Method for special perturbations |
title_full |
Method for special perturbations |
title_fullStr |
Method for special perturbations |
title_full_unstemmed |
Method for special perturbations |
title_sort |
method for special perturbations |
publishDate |
1963 |
url |
http://sedici.unlp.edu.ar/handle/10915/91811 |
work_keys_str_mv |
AT altavistacarlosalberto methodforspecialperturbations |
_version_ |
1807220485212078080 |