2004
DOI: 10.1142/s021827180400492x
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Restricted Problem of Three Bodies With Newtonian + Yukawa Potential

Abstract: Trajectories of the third body in the Restricted Problem of Three Bodies including a Yukawa term to the Newtonian gravitational potential are analyzed. It is shown that this modified gravitational potential changes some important aspects of the Restricted Problem of Three Bodies. Depending of coupling constant α, motions obtained in the pure Newtonian case are qualitatively different when Yukawa term is included. Depending of coupling parameters α, the nature of dynamics change from regular to chaotic (α<0)… Show more

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Cited by 9 publications
(6 citation statements)
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“…The equations of motion of the infinitesimal mass in a barycentric synodic coordinate system ðx, yÞ and dimensionless variables are [18]:…”
Section: Equations Of Motionmentioning
confidence: 99%
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“…The equations of motion of the infinitesimal mass in a barycentric synodic coordinate system ðx, yÞ and dimensionless variables are [18]:…”
Section: Equations Of Motionmentioning
confidence: 99%
“…where V N ðrÞ is the Newtonian potential between the two bodies M and m, V Y ðrÞ is the Yukawa correction to the Newtonian potential, r is the distance between m and M, G is the Newtonian gravitational constant, α ∈ ð−1, 1Þ is the coupling constant of the Yukawa force to the Gravitational force, and λ ∈ ð0,∞Þ is the range of the Yukawa force [18]. Therefore, the corresponding force between M and m can be expressed as…”
Section: Introductionmentioning
confidence: 99%
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“…Te restricted three-body problem under the consideration of Yukawa correction is studied by Kokubun [3]. Te main aim of this research was to study the efect of modifed potential on the important aspects of restricted three-body problem.…”
Section: Introductionmentioning
confidence: 99%
“…where V N (r) is the Newtonian potential between the two bodies m and M, V Y (r) is the Yukawa correction to the Newtonian potential, r is the distance between m and M, G is the Newtonian gravitational constant, α ϵ (− 1, 1) is the coupling constant of the Yukawa force to the Gravitational force, and λ ϵ (0, ∞) is the range of the Yukawa force [14]. Terefore, the corresponding force between m and M can be expressed as…”
Section: Introductionmentioning
confidence: 99%