2013
DOI: 10.1007/s11232-013-0087-0
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Phase topology of one irreducible integrable problem in the dynamics of a rigid body

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Cited by 10 publications
(19 citation statements)
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“…In the following sections we point out the equations of three invariant manifolds generalizing the Appelrot classes for the Hamilton function (2.13). Two of them exist only for the top with λ = 0 and correspond to the bifurcation surfaces found in [28], the third one exists for arbitrary values of λ and generalizes the cases shown in the works [18,19,17].…”
Section: The Appelrot Classesmentioning
confidence: 55%
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“…In the following sections we point out the equations of three invariant manifolds generalizing the Appelrot classes for the Hamilton function (2.13). Two of them exist only for the top with λ = 0 and correspond to the bifurcation surfaces found in [28], the third one exists for arbitrary values of λ and generalizes the cases shown in the works [18,19,17].…”
Section: The Appelrot Classesmentioning
confidence: 55%
“…P.E. Ryabov in [28] started the topological analysis of the GTFG system. First of all, he obtains the explicit formulas of the commutating integrals K and G generalizing K Y and G RS , thus expressing in terms of these integrals the coefficients of the algebraic curve associated with the Lax representation:…”
Section: Preliminariesmentioning
confidence: 99%
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“…For the Hamiltonian function (2), we represent the additional integrals K and G as functions of two deformation parameters ε 1 and ε 2 [4]:…”
Section: Intrtoductionmentioning
confidence: 99%
“…Remark 4. We note that, generally speaking, the authors of [19] presented a more general case of the Kovalevskaya top in which the equations of motion possess an additional integral of degree 2 and 4 in momenta (the explicit form of the integral is presented in [18]).…”
Section: The Kovalevskaya Casementioning
confidence: 99%