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Symmetric Constellations of Satellites Moving Around a Central Body of Large Mass
We consider a ( 1 + N ) -body problem in which one particle has mass m 0 ≫ 1 and the remaining N have unitary mass. We can assume that the body with larger mass (central body) is at rest at the origin, coinciding with the center of mass of the N bodies with smaller masses (satellites). The interacti...
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Published in: | Journal of dynamics and differential equations 2023-06, Vol.35 (2), p.1511-1559 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites |
Online Access: | Get full text |
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Summary: | We consider a
(
1
+
N
)
-body problem in which one particle has mass
m
0
≫
1
and the remaining
N
have unitary mass. We can assume that the body with larger mass (central body) is at rest at the origin, coinciding with the center of mass of the
N
bodies with smaller masses (satellites). The interaction force between two particles is defined through a potential of the form
U
∼
1
r
α
,
where
α
∈
[
1
,
2
)
and
r
is the distance between the particles. Imposing symmetry and topological constraints, we search for periodic orbits of this system by variational methods. Moreover, we use
Γ
-convergence theory to study the asymptotic behaviour of these orbits, as the mass of the central body increases. It turns out that the Lagrangian action functional
Γ
-converges to the action functional of a Kepler problem, defined on a suitable set of loops. In some cases, minimizers of the
Γ
-limit problem can be easily found, and they are useful to understand the motion of the satellites for large values of
m
0
. We discuss some examples, where the symmetry is defined by an action of the groups
Z
4
,
Z
2
×
Z
2
and the rotation groups of Platonic polyhedra on the set of loops. |
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ISSN: | 1040-7294 1572-9222 |
DOI: | 10.1007/s10884-021-10083-5 |