Modeling tails and bridges in galaxy interactions with the restricted three body problem

Galaxy interaction is a common feature in our universe but the dynamics behind it is still not fully understood. More data is becoming available lately and every time it is more precise. However, we need mathematical and physical models to understand this new data. In this work we model the interact...

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Detalhes bibliográficos
Autor: García Gutierrez, Albert
Tipo de documento: dissertação
Data de publicação:2021
País:España
Recursos:Universitat Politècnica de Catalunya (UPC)
Repositório:UPCommons. Portal del coneixement obert de la UPC
Idioma:inglês
OAI Identifier:oai:upcommons.upc.edu:2117/336300
Acesso em linha:https://hdl.handle.net/2117/336300
Access Level:Acceso aberto
Palavra-chave:Numerical analysis
Dynamical systems
Galaxy interaction
Galactic dynamics
Restricted three body problem
Numerical methods
Anàlisi numèrica
Classificació AMS::65 Numerical analysis::65P Numerical problems in dynamical systems
Àrees temàtiques de la UPC::Matemàtiques i estadística::Anàlisi numèrica
Descrição
Resumo:Galaxy interaction is a common feature in our universe but the dynamics behind it is still not fully understood. More data is becoming available lately and every time it is more precise. However, we need mathematical and physical models to understand this new data. In this work we model the interaction between two galaxies with the parabolic restricted three body problem. In a first step, we simulate the effects of the interaction in a disk galaxy doing several particle simulations, obtaining results close to reality. Secondly, with the help of the C-criterion classification we try to understand the relation between the radius of the disks and the formation of galactic structures such as tails and bridges. Finally we use the invariant objects in the circular restricted three body problem in order to understand the dynamics of our simulations. In fact, we are able to explain the formation of tails with the invariant manifolds of Lyapunov orbits around L1.