Lyapunov-Kozlov method for singular cases

Lyapunov's first method,extended by Kozlov to nonlinear mechanical systems,is applied to study the instability of the equilibrium position of a mechanical system moving in the field of conservative and dissipative forces.The cases with a tensor of inertia or a matrix of coefficients of the Rayleigh...

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Bibliographic Details
Published in:Applied mathematics and mechanics Vol. 32; no. 9; pp. 1207 - 1220
Main Authors: Covic, V, Djuric, D, Veskovic, M, Obradovic, A
Format: Journal Article
Language:English
Published: Heidelberg Shanghai University Press 01-09-2011
Faculty of Mechanical Engineering, University of Belgrade,Kraljice Marije 16, Belgrade 11000, Serbia%Faculty of Mechanical Engineering, University of Kragujevac,Dositejeva 19, Kraljevo 36000, Serbia
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Summary:Lyapunov's first method,extended by Kozlov to nonlinear mechanical systems,is applied to study the instability of the equilibrium position of a mechanical system moving in the field of conservative and dissipative forces.The cases with a tensor of inertia or a matrix of coefficients of the Rayleigh dissipative function are analyzed singularly in the equilibrium position.This fact renders the impossible application of Lyapunov's approach in the analysis of the stability because,in the equilibrium position,the conditions of the existence and uniqueness of the solutions to the differential equations of motion are not fulfilled.It is shown that Kozlov's generalization of Lyapunov's first method can also be applied in the mentioned cases on the conditions that,besides the known algebraic expression,more are fulfilled.Three theorems on the instability of the equilibrium position are formulated.The results are illustrated by an example.
Bibliography:Lyapunov's first method,extended by Kozlov to nonlinear mechanical systems,is applied to study the instability of the equilibrium position of a mechanical system moving in the field of conservative and dissipative forces.The cases with a tensor of inertia or a matrix of coefficients of the Rayleigh dissipative function are analyzed singularly in the equilibrium position.This fact renders the impossible application of Lyapunov's approach in the analysis of the stability because,in the equilibrium position,the conditions of the existence and uniqueness of the solutions to the differential equations of motion are not fulfilled.It is shown that Kozlov's generalization of Lyapunov's first method can also be applied in the mentioned cases on the conditions that,besides the known algebraic expression,more are fulfilled.Three theorems on the instability of the equilibrium position are formulated.The results are illustrated by an example.
instability; singular case; asymptotic motion; potential; dissipative force
31-1650/O1
ObjectType-Article-2
SourceType-Scholarly Journals-1
ObjectType-Feature-1
content type line 23
ISSN:0253-4827
1573-2754
DOI:10.1007/s10483-011-1494-6