2009
DOI: 10.1007/s10509-009-0047-1
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Linearization of the Hamiltonian in the generalized photogravitational Chermnykh’s problem

Abstract: Linearization of the Hamiltonian is being performed in the generalized photogravitational Chermnykh's problem. The normal form of the second order part of the Hamiltonian have been found. The effect of radiation pressure, gravitational potential from the belt have been examined analytically and numerically

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Cited by 7 publications
(6 citation statements)
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“…In a rotating reference frame the coordinates of m 1 and m 2 are (−µ, 0) and (1 − µ, 0) respectively. We consider the model proposed by Miyamoto and Nagai (1975), and equations of motion are given as in Kushvah (2008) and Kushvah (2009a):…”
Section: Trajectory Of Lmentioning
confidence: 99%
See 1 more Smart Citation
“…In a rotating reference frame the coordinates of m 1 and m 2 are (−µ, 0) and (1 − µ, 0) respectively. We consider the model proposed by Miyamoto and Nagai (1975), and equations of motion are given as in Kushvah (2008) and Kushvah (2009a):…”
Section: Trajectory Of Lmentioning
confidence: 99%
“…In present paper our aim is to obtain trajectories of L 4 and is to estimate the rate of deviation for initially closely related trajectories in the modified restricted three body problem model(as in Kushvah (2008Kushvah ( , 2009a) with radiation from Sun, oblateness of the second primary(massive body) and influence of the belt. It is supposed that the primary bodies and a belt are moving in a circular orbits about the common center of mass of both primaries.…”
Section: Introductionmentioning
confidence: 99%
“…The coordinates of m 1 , m 2 are (−μ, 0), (1 − μ, 0) respectively. In the above mentioned reference system and Miyamoto and Nagai (1975) model, the equations of motion of the infinitesimal mass particle in the xy-plane formulated as (please see Kushvah 2008Kushvah , 2009a):…”
Section: Location Of the Lagrangian Pointsmentioning
confidence: 99%
“…Indeed, the restricted three-body problem has been a useful model in many fields, such as the evolution of binary stars (Eggleton 1983) and orbital calculations of planetary systems (Mikkola et al 1994;Namouni 1999). Moreover, modifications of the restricted three-body problem were employed to model various problems related to planetary systems (Chermnykh 1987;Papadakis 2004Papadakis , 2005aPapadakis , 2005bPerdios, Kalantonis & Douskos 2008;Kushvah 2008aKushvah , 2008bKushvah , 2009Kushvah , 2011aKushvah , 2011bDouskos 2011;Kushvah, Kishor & Dolas 2012;Kishor & Kushvah 2013;Douskos et al 2012;Douskos 2015).…”
Section: Introductionmentioning
confidence: 99%