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IssuesArchive of Issues2009-3pp.366-371

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S. A. Agafonov, "On the stability of a circular system subjected to nonlinear dissipative forces," Mech. Solids. 44 (3), 366-371 (2009)
Year 2009 Volume 44 Number 3 Pages 366-371
DOI 10.3103/S0025654409030054
Title On the stability of a circular system subjected to nonlinear dissipative forces
Author(s) S. A. Agafonov (Bauman Moscow State Technical University, 2-ya Baumanskaya 5, Moscow, 105005 Russia)
Abstract A circular system is a mechanical system subjected to potential forces and positional nonconservative forces (circular forces). The latter linearly depend on the coordinates and are characterized by a skew-symmetric matrix. The influence of linear dissipative forces on the stability of a circular system is ambiguous: on the one hand, they can stabilize a stable circular system (making it asymptotically stable); on the other hand, they can destabilize it [1-4]. The action of linear dissipative forces on a circular system results in the so-called destabilization paradox: the stability threshold decreases by a finite value.

A detailed survey of this phenomenon can be found in [5]. The destabilization effect is also preserved under the action of nonlinear dissipative forces. The influence of these forces on the stability of the Ziegler pendulum with a tracking force was studied in [6]. It was shown that the critical value of the tracking force decreases by a finite value. A similar effect was discovered in the analysis of a continual system in [7].

In the present paper, we study how nonlinear dissipative forces affect the stability of the equilibrium of a circular mechanical system with two degrees of freedom. The stability problem is solved without any references to specific mechanical systems. The results are used to analyze the stability of a gimbal gyro with allowance for dry friction in the rotor bearings.
References
1.  S.A. Agafonov, "To the Stability of Nonconservative Systems," Izv. Akad. Nauk SSSR. Mekh. Tverd. Tela, No. 1, 47-51 (1986) [Mech. Solids (Engl. Transl.) 21 (1), 46-50 (1986)].
2.  D.R. Merkin, Introduction to Theory of Stability of Motion (Nauka, Moscow, 1971) [in Russian].
3.  O.N. Kirillov and A.P. Seyranian, "Stabilization and Destabilization of a Circulatory System by Small Velocity-Dependent Forces," J. Sound Vibr. 283 (3-5), 781-800 (2005).
4.  O.N. Kirillov, "A Theory of the Destabilization Paradox in Non-Conservative Systems," Acta Mech. 174 (3-4), 145-166 (2005).
5.  A.P. Seyranian, "Destabilization Paradox in Nonconservative Systems," Uspekhi Mekh. 13 (2), 89-124 (1990).
6.  P. Hagedorn, "On the Destabilizing Effect of Non-Linear Damping in Nonconservative Systems with Follower Forces," Int. J. Nonlin. Mech. 5 (2), 341-358 (1970).
7.  S.A. Agafonov and D.V. Georgievskii, "Dynamic Stability of a Beam That has Nonlinear Internal Viscosity and is Subjected to a Follower Force," Dokl. Ross. Akad. Nauk 396 (3), 339-342 (2004) [Dokl. Phys. (Engl. Transl.) 49 (5), 332-335 (2004)].
8.  G.V. Kamenkov, Selected Works, Vol. 1: \Motion Stability. Oscillations. Aerodynamics (Nauka, Moscow, 1971) [in Russian].
9.  L.G. Khazin and E.E. Shnol, Stability of Critical Equilibrium States (Center of Biological Studies, Pushchino, 1985) [in Russian].
10.  V.Ph. Zhuravlev, "Nutational Self-Oscillation of a Free Gyroscope," Izv. Akad. Nauk. Mekh. Tverd. Tela, No. 6, 13-16 (1992) [Mech. Solids (Engl. Transl.) 27 (6), 11-14 (1992)].
Received 07 July 2005
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