The motion of an auto:aomous mechanical system with one degree of freedom subject to small time-periodic perturbations and small dissipative forces in the vicinity of a stable position of equilibrium of the system is considered. It is assumed that resonance occurs in forced vibrations when the ratio
Resonant periodic motions of Hamiltonian systems with one degree of freedom when the Hamiltonian is degenerate
β Scribed by O.V. Kholostova
- Publisher
- Elsevier Science
- Year
- 2006
- Tongue
- English
- Weight
- 360 KB
- Volume
- 70
- Category
- Article
- ISSN
- 0021-8928
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β¦ Synopsis
The motions of a non-autonomous Hamiltonian system with one degree of freedom which is periodic in time and where the Hamiltonian contains a small parameter is considered. The origin of coordinates of the phase space is the equilibrium position of the unperturbed or complete system, which is stable in the linear approximation. It is assumed that there is degeneracy in the unperturbed Hamiltonian when account is taken of terms no higher than the fourth degree (the frequency of the small linear oscillations depends on the amplitude) and, in this case, one of the resonances of up to the fourth order inclusive is realized in the system. Model Hamiltonians are constructed for each case of resonance and a qualitative investigation of the motions of the model system is carried out. Using PoincarΓ©'s theory of periodic motions and KAM-theory, a rigorous solution is given of the problem of the existence, bifurcations and stability of the periodic motions of the initial system, which are analytic with respect to fractional powers of the small parameter. The resonant periodic motions (in the case of the degeneracy being considered) of a spherical pendulum with an oscillating suspension point are investigated as an application.
π SIMILAR VOLUMES
The problem of the orbital stability of periodic motions, produced from an equilibrium position of an autonomous Hamiltonian system with two degrees of freedom is considered. The Hamiltonian function is assumed to be analytic and alternating in a certain neighbourhood of the equilibrium position, th