2010
DOI: 10.1088/1751-8113/43/10/105203
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Bifurcation diagrams involving the linear integral of Yehia

Abstract: In the general case the Hamiltonian system with three degrees of freedom describing the motion of a rigid body in two constant forces does not admit any symmetry groups. Yehia (1986 Mech. Res. Commun. 13 169-72) found conditions under which the equations of motion of the Kowalevski-type top have an integral linear in angular velocities in addition to the energy integral. Later it was noticed that such an integral exists for the same force field for any dynamically symmetric top with the center of force applic… Show more

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Cited by 6 publications
(8 citation statements)
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References 12 publications
(23 reference statements)
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“…Finding the set of critical points using (16) requires searching for the simultaneous zeros of one or more functions of four variables. For example, applying condition (16d), which is expressed using exterior differential forms, results in a set of six functions to be zeroed.…”
Section: Critical Points and The Bifurcation Diagrammentioning
confidence: 99%
See 1 more Smart Citation
“…Finding the set of critical points using (16) requires searching for the simultaneous zeros of one or more functions of four variables. For example, applying condition (16d), which is expressed using exterior differential forms, results in a set of six functions to be zeroed.…”
Section: Critical Points and The Bifurcation Diagrammentioning
confidence: 99%
“…The techniques described here do not require the use of action-angle coordinates, and are sufficiently general to be applied to future machine designs [12] described by an autonomous Hamiltonian, in which a second invariant is analytically known. Related techniques have recently had a major impact in molecular spectroscopy [13][14][15], and have been applied to a number of systems of physical interest [16,17].…”
Section: Introductionmentioning
confidence: 99%
“…Suppose that passing to the quotient space we identify the whole subgroup fg t g to one point. Then we obtain the fiber bundle of SOð3Þ over the two-dimensional sphere, but this bundle is not locally trivial [27,28]. Therefore, such symmetry is called a singular symmetry.…”
Section: Equations and Integralsmentioning
confidence: 99%
“…Классический случай Кова-левской изучен в [4], [5], [6]. Случай Яхья и его обобщения рассматривались в [7]. Глобальный подход к классификации интегрируемых систем на двумерной сфере, порожденных задачами динамики твердого тела с осесимметричным потенциалом, реализован в работах [8], [9], [10].…”
Section: § 1 введениеunclassified