The circular restricted 4-body problem with three equal primaries in the collinear central configuration of the 3-body problem

2021 ◽  
Vol 133 (11-12) ◽  
Author(s):  
Jaume Llibre ◽  
Daniel Paşca ◽  
Claudià Valls
Author(s):  
Małgorzata Moczurad ◽  
Piotr Zgliczyński

Abstract We give a computer-assisted proof of the full listing of central configuration for n-body problem for Newtonian potential on the plane for $$n=5,6,7$$ n = 5 , 6 , 7 with equal masses. We show all these central configurations have a reflective symmetry with respect to some line. For $$n=8,9,10$$ n = 8 , 9 , 10 , we establish the existence of central configurations without any reflectional symmetry.


Author(s):  
Alain Albouy ◽  
Yanning Fu ◽  
Shanzhong Sun

We study the relationship between the masses and the geometric properties of central configurations. We prove that, in the planar four-body problem, a convex central configuration is symmetric with respect to one diagonal if and only if the masses of the two particles on the other diagonal are equal. If these two masses are unequal, then the less massive one is closer to the former diagonal. Finally, we extend these results to the case of non-planar central configurations of five particles.


Nonlinearity ◽  
2019 ◽  
Vol 33 (1) ◽  
pp. 388-407
Author(s):  
Antonio Carlos Fernandes ◽  
Luis Fernando Mello ◽  
Claudio Vidal

2020 ◽  
Vol 132 (11-12) ◽  
Author(s):  
Małgorzata Moczurad ◽  
Piotr Zgliczyński

AbstractWe present a computer assisted proof of the full listing of central configurations for spatial n-body problem for $$n=5$$ n = 5 and 6, with equal masses. For each central configuration, we give a full list of its Euclidean symmetries. For all masses sufficiently close to the equal masses case, we give an exact count of configurations in the planar case for $$n=4,5,6,7$$ n = 4 , 5 , 6 , 7 and in the spatial case for $$n=4,5,6$$ n = 4 , 5 , 6 .


1996 ◽  
Vol 16 (5) ◽  
pp. 1059-1070 ◽  
Author(s):  
Christopher K. McCord

AbstractFor all masses, there are at least n − 2, O2-orbits of non-collinear planar central configurations. In particular, this estimate is valid even if the potential function is not a Morse function. If the potential function is a Morse function, then an improved lower bound, of the order of n! ln(n + 1/3)/2, can be given.


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