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In the phase space of the integrable Hamiltonian system with three degrees of freedom used to describe the motion of a Kowalevski-type top in a double constant force field, we point out the four-dimensional invariant manifold. It is shown…

Exactly Solvable and Integrable Systems · Physics 2008-03-07 Mikhail P. Kharlamov , Alexander Y. Savushkin

The problem of motion of the Kovalevskaya top in a double force field is investigated (the integrable case of A.G. Reyman and M.A. Semenov-Tian-Shansky without a gyrostatic momentum). It is a completely integrable Hamiltonian system with…

Exactly Solvable and Integrable Systems · Physics 2014-08-04 P. E. Ryabov , M. P. Kharlamov

The article presents a compact review of the analytical results (2002-2009) in the study of the system describing the motion of a top in two constant fields. The Liouville integrability of this system under certain condition of the…

Dynamical Systems · Mathematics 2012-11-26 Mikhail P. Kharlamov , Alexander Y. Savushkin

In the problem of motion of the Kowalevski top in a double force field the 4-dimensional invariant submanifold of the phase space was pointed out by M.P.Kharlamov (Mekh. Tverd. Tela, 32, 2002). We show that the equations of motion on this…

Exactly Solvable and Integrable Systems · Physics 2008-03-07 Mikhail P. Kharlamov , Alexander Y. Savushkin

The Kowalevski top in two constant fields is known as the unique profound example of an integrable Hamiltonian system with three degrees of freedom not reducible to a family of systems in fewer dimensions. As the first approach to…

Exactly Solvable and Integrable Systems · Physics 2008-03-07 Mikhail P. Kharlamov

We discuss the polynomial bi-Hamiltonian structures for the Kowalevski top in special case of zero square integral. An explicit procedure to find variables of separation and separation relations is considered in detail.

Exactly Solvable and Integrable Systems · Physics 2011-09-06 A V Tsiganov

We fulfill the rough topological analysis of the problem of the motion of the Kovalevskaya top in a double field. This problem is described by a completely integrable system with three degrees of freedom not reducible to a family of systems…

Exactly Solvable and Integrable Systems · Physics 2014-12-05 Mikhail P. Kharlamov , Pavel E. Ryabov

The structure of integral manifolds in the Kovalevskaya problem of the motion of a heavy rigid body about a fixed point is considered. An analytic description of a bifurcation set is obtained, and bifurcation diagrams are constructed. The…

Exactly Solvable and Integrable Systems · Physics 2013-12-30 Mikhail P. Kharlamov

In the paper, we consider a completely integrable Hamiltonian system with three degrees of freedom found by V.V.Sokolov and A.V.Tsiganov. This system is known as the generalized two-field gyrostat. For the case of only gyroscopic forces…

Exactly Solvable and Integrable Systems · Physics 2015-06-19 Pavel E. Ryabov

We consider the analogue of the 4th Appelrot class of motions of the Kowalevski top for the case of two constant force fields. The trajectories of this family fill the four-dimensional surface O^4 in the six-dimensional phase space. The…

Exactly Solvable and Integrable Systems · Physics 2008-03-10 Mikhail P. Kharlamov

The case of motion of a generalized two-field gyrostat found by V.V.Sokolov and A.V.Tsiganov is known as a Liouville integrable Hamiltonian system with three degrees of freedom. We find a set of points at which the momentum map has rank 1.…

Exactly Solvable and Integrable Systems · Physics 2016-01-01 Pavel Ryabov , Sergei Sokolov , Irina Kharlamova

A Hamiltonian formulation of generic many-particle systems with space-dependent balanced loss and gain coefficients is presented. It is shown that the balancing of loss and gain necessarily occurs in a pair-wise fashion. Further, using a…

Mathematical Physics · Physics 2019-08-30 Debdeep Sinha , Pijush K. Ghosh

The phase topology of the integrable Hamiltonian system on $e(3)$ found by V.V.Sokolov (2001) and generalizing the Kowalevski case is investigated. The generalization contains, along with a homogeneous potential force field, gyroscopic…

Exactly Solvable and Integrable Systems · Physics 2015-07-10 Pavel E. Ryabov , Alexander Y. Savushkin

Constrained Hamiltonian systems are investigated by using the Hamilton-Jacobi method. Integration of a set of equations of motion and the action function is discussed. It is shown that we have two types of integrable systems: a) ${\it…

High Energy Physics - Theory · Physics 2009-11-10 Sami I. Muslih

In the problem of motion of the Kowalevski top on two constant fields (the A.G.Reyman - M.A.Semenov-Tian-Shansky case) the type of all critical points of the momentum map is calculated.

Exactly Solvable and Integrable Systems · Physics 2010-12-21 P. E. Ryabov , M. P. Kharlamov

The contributions of Sophya Kowalewski to the integrability theory of the equations for the heavy top extend to a larger class of Hamiltonian systems on Lie groups; this paper explains these extensions, and along the way reveals further…

Symplectic Geometry · Mathematics 2009-09-25 Velimir Jurdjevic

The paper concludes the cycle of investigations on the bifurcation diagrams of the system with three degrees of freedom which describes the motion of an axially symmetric top with the Kowalevski conditions in a double force field. The…

Exactly Solvable and Integrable Systems · Physics 2014-12-15 Mikhail P. Kharlamov

The article continues the author's publication in [Mech. Tverd. Tela, No. 35, 2005 and No. 38, 2008], in which we investigate the integrable dynamical system induced on one four-dimensional submanifold of the phase space of the problem of a…

Exactly Solvable and Integrable Systems · Physics 2013-09-30 Mikhail P. Kharlamov

Consider a rigid body having a fixed point in a superposition of two constant force fields (for example, gravitational and magnetic). Introducing the condition of Kowalevski type, O.I.Bogoyavlensky (1984) has found the first integral…

Exactly Solvable and Integrable Systems · Physics 2008-03-10 Mikhail P. Kharlamov

The constants of motion of the following systems are deduced: a relativistic particle with linear dissipation, a no-relativistic particle with a time explicitly depending force, a no-relativistic particle with a constant force and time…

Classical Physics · Physics 2011-08-19 G. López , L. A. Barrera , Y. Garibo , H. Hernández , J. C. Salazar , C. A. Vargas
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